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1. Measurements of the electron-helicity asymmetry in the quasi-elastic A(e→,e′p) process

Author

T. Kolar, S.J. Paul, P. Achenbach, H. Arenhövel, A. Ashkenazi, J. Beričič, R. Böhm, D. Bosnar, T. Brecelj, E. Cline, E.O. Cohen, M.O. Distler, A. Esser, I. Friščić, R. Gilman, C. Giusti, M. Heilig, M. Hoek, D. Izraeli, S. Kegel, P. Klag, I. Korover, J. Lichtenstadt, I. Mardor, H. Merkel, D.G. Middleton, M. Mihovilovič, J. Müller, U. Müller, M. Olivenboim, E. Piasetzky, J. Pochodzalla, G. Ron, B.S. Schlimme, M. Schoth, F. Schulz, C. Sfienti, S. Širca, R. Spreckels, S. Štajner, Y. Stöttinger, S. Strauch, M. Thiel, A. Tyukin, A. Weber, and I. Yaron

Subjects
Physics, QC1-999
Abstract

We present measurements of the electron helicity asymmetry in quasi-elastic proton knockout from 2H and 12C nuclei by polarized electrons. This asymmetry depends on the fifth structure function, is antisymmetric with respect to the scattering plane, and vanishes in the absence of final-state interactions, and thus it provides a sensitive tool for their study. Our kinematics cover the full range in off-coplanarity angle ϕpq, with a polar angle θpq coverage up to about 8°. The missing energy resolution enabled us to determine the asymmetries for knock-out resulting in different states of the residual 11B system. We find that the helicity asymmetry for p-shell knockout from 12C depends on the final state of the residual system and is relatively large (up to ≈0.16), especially at low missing momentum. It is considerably smaller (up to ≈0.01) for s-shell knockout from both 12C and 2H. The data for 2H are in very good agreement with theoretical calculations, while the predictions for 12C exhibit differences with respect to the data.

Published
2022
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2. 12C(e,e'pN) measurements of short range correlations in the tensor-to-scalar interaction transition region

Author

I. Korover, J.R. Pybus, A. Schmidt, F. Hauenstein, M. Duer, O. Hen, E. Piasetzky, L.B. Weinstein, D.W. Higinbotham, S. Adhikari, K. Adhikari, M.J. Amaryan, Giovanni Angelini, H. Atac, L. Barion, M. Battaglieri, A. Beck, I. Bedlinskiy, Fatiha Benmokhtar, A. Bianconi, A.S. Biselli, S. Boiarinov, W.J. Briscoe, W.K. Brooks, D. Bulumulla, V.D. Burkert, D.S. Carman, A. Celentano, P. Chatagnon, T. Chetry, L. Clark, B. Clary, P.L. Cole, M. Contalbrigo, V. Crede, R. Cruz-Torres, A. D'Angelo, R. De Vita, M. Defurne, A. Denniston, A. Deur, S. Diehl, C. Djalali, R. Dupre, H. Egiyan, M. Ehrhart, A. El Alaoui, L. El Fassi, L. Elouadrhiri, P. Eugenio, R. Fersch, A. Filippi, T. Forest, G. Gavalian, F.X. Girod, E. Golovatch, R.W. Gothe, K.A. Griffioen, M. Guidal, K. Hafidi, H. Hakobyan, N. Harrison, M. Hattawy, T.B. Hayward, D. Heddle, K. Hicks, M. Holtrop, Y. Ilieva, D.G. Ireland, E.L. Isupov, D. Jenkins, H.S. Jo, K. Joo, S. Joosten, D. Keller, M. Khachatryan, A. Khanal, M. Khandaker, A. Kim, C.W. Kim, F.J. Klein, V. Kubarovsky, L. Lanza, M. Leali, P. Lenisa, K. Livingston, V. Lucherini, I.J.D. MacGregor, D. Marchand, N. Markov, L. Marsicano, V. Mascagna, B. McKinnon, S. Mey-Tal Beck, T. Mineeva, M. Mirazita, A. Movsisyan, C. Munoz Camacho, B. Mustapha, P. Nadel-Turonski, K. Neupane, G. Niculescu, M. Osipenko, A.I. Ostrovidov, M. Paolone, L.L. Pappalardo, R. Paremuzyan, E. Pasyuk, W. Phelps, O. Pogorelko, J.W. Price, Y. Prok, D. Protopopescu, B.A. Raue, M. Ripani, J. Ritman, A. Rizzo, G. Rosner, J. Rowley, F. Sabatié, C. Salgado, R.A. Schumacher, E.P. Segarra, Y.G. Sharabian, U. Shrestha, D. Sokhan, O. Soto, N. Sparveris, S. Stepanyan, I.I. Strakovsky, S. Strauch, J.A. Tan, N. Tyler, M. Ungaro, L. Venturelli, H. Voskanyan, E. Voutier, T. Wang, D. Watts, X. Wei, M.H. Wood, N. Zachariou, J. Zhang, Z.W. Zhao, and X. Zheng

Subjects
Physics, QC1-999
Abstract

High-momentum configurations of nucleon pairs at short-distance are probed using measurements of the 12C(e,e′p) and 12C(e,e′pN) reactions (where N is either n or p), at high-Q2 and xB>1.1. The data span a missing-momentum range of 300–1000 MeV/c and are predominantly sensitive to the transition region of the strong nuclear interaction from a Tensor to Scalar interaction. The data are well reproduced by theoretical calculations using the Generalized Contact Formalism with both chiral and phenomenological nucleon-nucleon (NN) interaction models. This agreement suggests that the measured high missing-momentum protons up to 1000 MeV/c predominantly belong to short-ranged correlated (SRC) pairs. The measured 12C(e,e′pN) / 12C(e,e′p) and 12C(e,e′pp) / 12C(e,e′pn) cross-section ratios are consistent with a decrease in the fraction of proton-neutron SRC pairs and increase in the fraction of proton-proton SRC pairs with increasing missing momentum. This confirms the transition from an isospin-dependent tensor NN interaction at ∼400 MeV/c to an isospin-independent scalar interaction at high-momentum around ∼800 MeV/c as predicted by theoretical calculation.

Published
2021
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3. Quasi-elastic polarization-transfer measurements on the deuteron in anti-parallel kinematics

Author

S. Paul, D. Izraeli, T. Brecelj, I. Yaron, P. Achenbach, H. Arenhövel, A. Ashkenazi, J. Beričič, R. Böhm, D. Bosnar, E. Cline, E.O. Cohen, L. Debenjak, M.O. Distler, A. Esser, I. Friščić, R. Gilman, M. Heilig, S. Kegel, P. Klag, Y. Kohl, T. Kolar, I. Korover, J. Lichtenstadt, I. Mardor, H. Merkel, D.G. Middleton, M. Mihovilovič, J. Müller, U. Müller, M. Olivenboim, E. Piasetzky, J. Pochodzalla, G. Ron, B.S. Schlimme, M. Schoth, F. Schulz, C. Sfienti, S. Širca, S. Štajner, S. Strauch, M. Thiel, A. Tyukin, and A. Weber

Subjects
Physics, QC1-999
Abstract

We present measurements of the polarization-transfer components in the H2(e→,e′p→) reaction, covering a previously unexplored kinematic region with large positive (anti-parallel) missing momentum, pmiss, up to 220MeV/c, and Q2=0.65 (GeV/c)2. These measurements, performed at the Mainz Microtron (MAMI), were motivated by theoretical calculations which predict small final-state interaction (FSI) effects in these kinematics, making them favorable for searching for medium modifications of bound nucleons in nuclei. We find in this kinematic region that the measured polarization-transfer components Px and Pz and their ratio agree with the theoretical calculations, which use free-proton form factors. Using this, we establish upper limits on possible medium effects that modify the bound proton's form factor ratio GE/GM at the level of a few percent. We also compare the measured polarization-transfer components and their ratio for 2H to those of a free (moving) proton. We find that the universal behavior of 2H, 4He and 12C in the double ratio (Px/Pz)A(Px/Pz)H1 is maintained in the positive missing-momentum region.

Published
2019
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4. The influence of Fermi motion on the comparison of the polarization transfer to a proton in elastic e→p and quasi-elastic e→A scattering

Author

S. Paul, T. Brecelj, H. Arenhövel, P. Achenbach, A. Ashkenazi, J. Beričič, R. Böhm, D. Bosnar, E.O. Cohen, L. Debenjak, M.O. Distler, A. Esser, I. Friščić, R. Gilman, D. Izraeli, T. Kolar, I. Korover, J. Lichtenstadt, I. Mardor, H. Merkel, D.G. Middleton, M. Mihovilovič, U. Müller, M. Olivenboim, E. Piasetzky, J. Pochodzalla, G. Ron, B.S. Schlimme, M. Schoth, F. Schulz, C. Sfienti, S. Širca, S. Štajner, S. Strauch, M. Thiel, A. Tyukin, A. Weber, and I. Yaron

Subjects
Physics, QC1-999
Abstract

A comparison between polarization-transfer to a bound proton in quasi-free kinematics by the A(e→,e′p→) knockout reaction and that in elastic scattering off a free proton can provide information on the characteristics of the bound proton. In the past the reported measurements have been compared to those of a free proton with zero initial momentum. We introduce, for the first time, expressions for the polarization-transfer components when the proton is initially in motion and compare them to the 2H data measured at the Mainz Microtron (MAMI). We show the ratios of the transverse (Px) and longitudinal (Pz) components of the polarization transfer in H2(e→,e′p→)n, to those of elastic scattering off a “moving proton”, assuming the proton's initial (Fermi-motion) momentum equals the negative missing momentum in the measured reaction. We found that the correction due to the proton motion is up to 20% at high missing momentum. However the effect on the double ratio (Px/Pz)A(Px/Pz)H1 is largely canceled out, as shown for both 2H and 12C data. This implies that the difference between the resting- and the moving-proton kinematics is not the primary cause for the deviations between quasi-elastic and elastic scattering reported previously.

Published
2019
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5. Comparison of recoil polarization in the C12(e→,e′p→) process for protons extracted from s and p shells

Author

T. Kolar, S.J. Paul, T. Brecelj, P. Achenbach, R. Böhm, D. Bosnar, E. Cline, E.O. Cohen, M.O. Distler, A. Esser, R. Gilman, C. Giusti, M. Hoek, D. Izraeli, S. Kegel, Y. Kohl, I. Korover, J. Lichtenstadt, I. Mardor, H. Merkel, M. Mihovilovič, J. Müller, U. Müller, M. Olivenboim, E. Piasetzky, J. Pochodzalla, G. Ron, B.S. Schlimme, C. Sfienti, S. Širca, R. Spreckels, S. Štajner, S. Strauch, M. Thiel, A. Weber, and I. Yaron

Subjects
Physics, QC1-999
Abstract

We present the first measurements of the double ratio of the polarization-transfer components (Px′/Pz′)p/(Px′/Pz′)s for knock-out protons from the s and p shells in C12 measured by the C12(e→,e′p→) reaction in quasi-elastic kinematics. The data are compared to theoretical predictions in the relativistic distorted-wave impulse approximation. Our results show that the differences between s- and p-shell protons, observed when compared at the same initial momentum (missing momentum), largely disappear when the comparison is done at the same proton virtuality. We observe no difference in medium modifications between protons from the s and p shells with the same virtuality in spite of the large differences in the respective nuclear densities.

Published
2020
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6. Measurements of the induced polarization in the quasi-elastic A(e,e′p→) process in non-coplanar kinematics

Author

S.J. Paul, T. Kolar, T. Brecelj, P. Achenbach, H. Arenhövel, A. Ashkenazi, J. Beričič, R. Böhm, D. Bosnar, E. Cline, E.O. Cohen, L. Debenjak, M.O. Distler, A. Esser, I. Friščić, R. Gilman, C. Giusti, M. Heilig, M. Hoek, D. Izraeli, S. Kegel, P. Klag, Y. Kohl, I. Korover, J. Lichtenstadt, I. Mardor, H. Merkel, D.G. Middleton, M. Mihovilovič, J. Müller, U. Müller, M. Olivenboim, E. Piasetzky, J. Pochodzalla, G. Ron, B.S. Schlimme, M. Schoth, F. Schulz, C. Sfienti, S. Širca, R. Spreckels, S. Štajner, S. Strauch, M. Thiel, A. Tyukin, A. Weber, and I. Yaron

Subjects
Physics, QC1-999
Abstract

We report measurements of the induced polarization P→ of protons knocked out from 2H and 12C via the A(e,e′p→) reaction. We have studied the dependence of P→ on two kinematic variables: the missing momentum pmiss and the “off-coplanarity” angle ϕpq between the scattering and reaction planes. For the full 360° range in ϕpq, both the normal (Py) and, for the first time, the transverse (Px) components of the induced polarization were measured with respect to the coordinate system associated with the scattering plane. Px vanishes in coplanar kinematics, however in non-coplanar kinematics, it is on the same scale as Py.We find that the dependence on ϕpq is sine-like for Px and cosine-like for Py. For carbon, the magnitude of the induced polarization is especially large when protons are knocked out from the p3/2 shell at very small pmiss. For the deuteron, the induced polarization is near zero at small |pmiss|, and its magnitude increases with |pmiss|. For both nuclei such behavior is reproduced qualitatively by theoretical results, driven largely by the spin-orbit part of the final-state interactions. However, for both nuclei, sizeable discrepancies exist between experiment and theory.

Published
2020
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7. Generalized contact formalism analysis of the 4He(e,e′pN) reaction

Author

J.R. Pybus, I. Korover, R. Weiss, A. Schmidt, N. Barnea, D.W. Higinbotham, E. Piasetzky, M. Strikman, L.B. Weinstein, and O. Hen

Subjects
Physics, QC1-999
Abstract

Measurements of short-range correlations in exclusive 4He(e,e′pN) reactions are analyzed using the Generalized Contact Formalism (GCF). We consider both instant-form and light-cone formulations with both the AV18 and local N2LO(1.0) nucleon-nucleon (NN) potentials. We find that kinematic distributions, such as the reconstructed pair opening angle, recoil neutron momentum distribution, and pair center of mass motion, as well as the measured missing energy, missing mass distributions, are all well reproduced by GCF calculations. The missing momentum dependence of the measured 4He(e,e′pN)/4He(e,e′p) cross-section ratios, sensitive to nature of the NN interaction at short-distacnes, are also well reproduced by GCF calculations using either interaction and formulation. This gives credence to the GCF scale-separated factorized description of the short-distance many-body nuclear wave-function.

Published
2020
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8. Components of polarization-transfer to a bound proton in a deuteron measured by quasi-elastic electron scattering

Author

D. Izraeli, I. Yaron, B.S. Schlimme, P. Achenbach, H. Arenhövel, A. Ashkenazi, J. Beričič, R. Böhm, D. Bosnar, E.O. Cohen, M.O. Distler, A. Esser, I. Friščić, R. Gilman, I. Korover, J. Lichtenstadt, I. Mardor, H. Merkel, D.G. Middleton, M. Mihovilovič, U. Müller, M. Olivenboim, E. Piasetzky, J. Pochodzalla, G. Ron, M. Schoth, F. Schulz, C. Sfienti, S. Širca, S. Štajner, S. Strauch, M. Thiel, A. Tyukin, and A. Weber

Subjects
Physics, QC1-999
Abstract

We report the first measurements of the transverse (Px and Py) and longitudinal (Pz) components of the polarization transfer to a bound proton in the deuteron via the H2(e→,e′p→) reaction, over a wide range of missing momentum. A precise determination of the electron beam polarization reduces the systematic uncertainties on the individual components to a level that enables a detailed comparison to a state-of-the-art calculation of the deuteron using free-proton electromagnetic form factors. We observe very good agreement between the measured and the calculated Px/Pz ratios, but deviations of the individual components. Our results cannot be explained by medium modified electromagnetic form factors. They point to an incomplete description of the nuclear reaction mechanism in the calculation.

Published
2018
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9. Measurement of polarization-transfer to bound protons in carbon and its virtuality dependence

Author

D. Izraeli, T. Brecelj, P. Achenbach, A. Ashkenazi, R. Böhm, E.O. Cohen, M.O. Distler, A. Esser, R. Gilman, T. Kolar, I. Korover, J. Lichtenstadt, I. Mardor, H. Merkel, M. Mihovilovič, U. Müller, M. Olivenboim, E. Piasetzky, G. Ron, B.S. Schlimme, M. Schoth, C. Sfienti, S. Širca, S. Štajner, S. Strauch, M. Thiel, A. Weber, and I. Yaron

Subjects
Physics, QC1-999
Abstract

We measured the ratio Px/Pz of the transverse to longitudinal components of polarization transferred from electrons to bound protons in C12 by the C12(e→,e′p→) process at the Mainz Microtron (MAMI). We observed consistent deviations from unity of this ratio normalized to the free-proton ratio, (Px/Pz)C12/(Px/Pz)H1, for both s- and p-shell knocked out protons, even though they are embedded in averaged local densities that differ by about a factor of two. The dependence of the double ratio on proton virtuality is similar to the one for knocked out protons from H2 and He4, suggesting a universal behavior. It further implies no dependence on average local nuclear density.

Published
2018
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10. A glimpse of gluons through deeply virtual compton scattering on the proton

Author

M. Defurne, A. Martí Jiménez-Argüello, Z. Ahmed, H. Albataineh, K. Allada, K. A. Aniol, V. Bellini, M. Benali, W. Boeglin, P. Bertin, M. Brossard, A. Camsonne, M. Canan, S. Chandavar, C. Chen, J.-P. Chen, C. W. de Jager, R. de Leo, C. Desnault, A. Deur, L. El Fassi, R. Ent, D. Flay, M. Friend, E. Fuchey, S. Frullani, F. Garibaldi, D. Gaskell, A. Giusa, O. Glamazdin, S. Golge, J. Gomez, O. Hansen, D. Higinbotham, T. Holmstrom, T. Horn, J. Huang, M. Huang, C. E. Hyde, S. Iqbal, F. Itard, H. Kang, A. Kelleher, C. Keppel, S. Koirala, I. Korover, J. J. LeRose, R. Lindgren, E. Long, M. Magne, J. Mammei, D. J. Margaziotis, P. Markowitz, M. Mazouz, F. Meddi, D. Meekins, R. Michaels, M. Mihovilovic, C. Muñoz Camacho, P. Nadel-Turonski, N. Nuruzzaman, R. Paremuzyan, A. Puckett, V. Punjabi, Y. Qiang, A. Rakhman, M. N. H. Rashad, S. Riordan, J. Roche, G. Russo, F. Sabatié, K. Saenboonruang, A. Saha, B. Sawatzky, L. Selvy, A. Shahinyan, S. Sirca, P. Solvignon, M. L. Sperduto, R. Subedi, V. Sulkosky, C. Sutera, W. A. Tobias, G. M. Urciuoli, D. Wang, B. Wojtsekhowski, H. Yao, Z. Ye, X. Zhan, J. Zhang, B. Zhao, Z. Zhao, X. Zheng, and P. Zhu

Subjects
Science
Abstract

It remains a challenge to find the structure and the distribution of the constituents of nucleons. Here the authors use a scattering method to get information about the gluons and quarks inside a proton and separate the contribution of Bethe-Heitler from the deeply virtual Compton scattering process.

Published
2017
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11. Polarization-transfer measurement to a large-virtuality bound proton in the deuteron

Author

I. Yaron, D. Izraeli, P. Achenbach, H. Arenhövel, J. Beričič, R. Böhm, D. Bosnar, E.O. Cohen, L. Debenjak, M.O. Distler, A. Esser, I. Friščić, R. Gilman, I. Korover, J. Lichtenstadt, H. Merkel, D.G. Middleton, M. Mihovilovič, U. Müller, E. Piasetzky, J. Pochodzalla, G. Ron, B.S. Schlimme, M. Schoth, F. Schulz, C. Sfienti, S. Širca, S. Strauch, M. Thiel, A. Tyukin, and A. Weber

Subjects
d(e,e'p), Electron-scattering, Physics, QC1-999
Abstract

We report the measurement of the ratio of polarization-transfer components, Px/Pz, in the H2(e→,e′p→)n reaction at low and high missing momenta, in search of differences between free and bound protons. The observed deviation of Px/Pz from that of a free proton, which is similar to that observed in 4He, indicates that the effect in nuclei is a function of the virtuality of the knock-out proton and the missing momentum direction, but not the average nuclear density. There is a general agreement between the data and calculations, which assume free proton form factors, however, the measurements are consistently about 10% higher.

Published
2017
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12. Measurement of nuclear transparency ratios for protons and neutrons

Author

M. Duer, O. Hen, E. Piasetzky, L.B. Weinstein, A. Schmidt, I. Korover, E.O. Cohen, H. Hakobyan, S. Adhikari, G. Angelini, H. Avakian, C. Ayerbe Gayoso, L. Barion, M. Battaglieri, A. Beck, I. Bedlinskiy, A.S. Biselli, S. Boiarinov, W.J. Briscoe, W. Brooks, V.D. Burkert, F. Cao, D.S. Carman, A. Celentano, P. Chatagnon, T. Chetry, G. Ciullo, P.L. Cole, M. Contalbrigo, O. Cortes, V. Crede, R. Cruz Torres, A. D'Angelo, N. Dashyan, R. De Vita, E. De Sanctis, A. Deur, S. Diehl, C. Djalali, R. Dupre, Burcu Duran, H. Egiyan, M. Ehrhart, A. El Alaoui, L. El Fassi, P. Eugenio, A. Filippi, T.A. Forest, G.P. Gilfoyle, F.X. Girod, E. Golovatch, R.W. Gothe, K.A. Griffioen, M. Guidal, L. Guo, K. Hafidi, C. Hanretty, N. Harrison, M. Hattawy, F. Hauenstein, T.B. Hayward, D. Heddle, M. Holtrop, Y. Ilieva, D.G. Ireland, B.S. Ishkhanov, E.L. Isupov, H.S. Jo, S. Johnston, K. Joo, S. Joosten, D. Keller, G. Khachatryan, M. Khachatryan, A. Khanal, M. Khandaker, A. Kim, W. Kim, A. Klein, F.J. Klein, V. Kubarovsky, S.E. Kuhn, S.V. Kuleshov, L. Lanza, G. Laskaris, P. Lenisa, K. Livingston, I.J.D. MacGregor, D. Marchand, B. McKinnon, S. Mey-Tal Beck, T. Mineeva, M. Mirazita, V. Mokeev, R.A. Montgomery, A. Movsisyan, C. Munoz Camacho, B. Mustapha, P. Nadel-Turonski, S. Niccolai, G. Niculescu, M. Osipenko, A.I. Ostrovidov, M. Paolone, L.L. Pappalardo, R. Paremuzyan, E. Pasyuk, M. Patsyuk, D. Payette, J. Price, D. Pocanic, O. Pogorelko, Y. Prok, D. Protopopescu, B.A. Raue, M. Ripani, D. Riser, A. Rizzo, G. Rosner, P. Rossi, F. Sabatié, C. Salgado, B.A. Schmookler, R.A. Schumacher, E.P. Segarra, Y.G. Sharabian, Iu. Skorodumina, D. Sokhan, O. Soto, N. Sparveris, S. Stepanyan, S. Strauch, M. Taiuti, J.A. Tan, M. Ungaro, H. Voskanyan, E. Voutier, R. Wang, X. Wei, N. Zachariou, J. Zhang, Z.W. Zhao, and X. Zheng

Subjects
Physics, QC1-999
Abstract

This paper presents, for the first time, measurements of neutron transparency ratios for nuclei relative to C measured using the (e,e′n) reaction, spanning measured neutron momenta of 1.4 to 2.4 GeV/c. The transparency ratios were extracted in two kinematical regions, corresponding to knockout of mean-field nucleons and to the breakup of Short-Range Correlated nucleon pairs. The extracted neutron transparency ratios are consistent with each other for the two measured kinematical regions and agree with the proton transparencies extracted from new and previous (e,e′p) measurements, including those from neutron-rich nuclei such as lead. The data also agree with and confirm the Glauber approximation that is commonly used to interpret experimental data. The nuclear-mass-dependence of the extracted transparencies scales as Aα with α=−0.289±0.007, which is consistent with nuclear-surface dominance of the reactions.

Published
2019
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13. Comparing proton momentum distributions in A = 2 and 3 nuclei via 2H 3H and 3He (e,e′p) measurements

Author

R. Cruz-Torres, S. Li, F. Hauenstein, A. Schmidt, D. Nguyen, D. Abrams, H. Albataineh, S. Alsalmi, D. Androic, K. Aniol, W. Armstrong, J. Arrington, H. Atac, T. Averett, C. Ayerbe Gayoso, X. Bai, J. Bane, S. Barcus, A. Beck, V. Bellini, H. Bhatt, D. Bhetuwal, D. Biswas, D. Blyth, W. Boeglin, D. Bulumulla, A. Camsonne, J. Castellanos, J.-P. Chen, E.O. Cohen, S. Covrig, K. Craycraft, B. Dongwi, M. Duer, B. Duran, D. Dutta, E. Fuchey, C. Gal, T.N. Gautam, S. Gilad, K. Gnanvo, T. Gogami, J. Gomez, C. Gu, A. Habarakada, T. Hague, O. Hansen, M. Hattawy, O. Hen, D.W. Higinbotham, E. Hughes, C. Hyde, H. Ibrahim, S. Jian, S. Joosten, A. Karki, B. Karki, A.T. Katramatou, C. Keppel, M. Khachatryan, V. Khachatryan, A. Khanal, D. King, P. King, I. Korover, T. Kutz, N. Lashley-Colthirst, G. Laskaris, W. Li, H. Liu, N. Liyanage, D. Lonardoni, R. Machleidt, L.E. Marcucci, P. Markowitz, R.E. McClellan, D. Meekins, S. Mey-Tal Beck, Z.-E. Meziani, R. Michaels, M. Mihovilovič, V. Nelyubin, N. Nuruzzaman, M. Nycz, R. Obrecht, M. Olson, L. Ou, V. Owen, B. Pandey, V. Pandey, A. Papadopoulou, S. Park, M. Patsyuk, S. Paul, G.G. Petratos, E. Piasetzky, R. Pomatsalyuk, S. Premathilake, A.J.R. Puckett, V. Punjabi, R. Ransome, M.N.H. Rashad, P.E. Reimer, S. Riordan, J. Roche, F. Sammarruca, N. Santiesteban, B. Sawatzky, E.P. Segarra, B. Schmookler, A. Shahinyan, S. Širca, N. Sparveris, T. Su, R. Suleiman, H. Szumila-Vance, A.S. Tadepalli, L. Tang, W. Tireman, F. Tortorici, G. Urciuoli, M. Viviani, L.B. Weinstein, B. Wojtsekhowski, S. Wood, Z.H. Ye, Z.Y. Ye, and J. Zhang

Subjects
Physics, QC1-999
Abstract

We report the first measurement of the (e,e′p) reaction cross-section ratios for Helium-3 (He3), Tritium (H3), and Deuterium (d). The measurement covered a missing momentum range of 40≤pmiss≤550MeV/c, at large momentum transfer (〈Q2〉≈1.9 (GeV/c)2) and xB>1, which minimized contributions from non quasi-elastic (QE) reaction mechanisms. The data is compared with plane-wave impulse approximation (PWIA) calculations using realistic spectral functions and momentum distributions. The measured and PWIA-calculated cross-section ratios for He3/d and H3/d extend to just above the typical nucleon Fermi-momentum (kF≈250 MeV/c) and differ from each other by ∼20%, while for He3/H3 they agree within the measurement accuracy of about 3%. At momenta above kF, the measured He3/H3 ratios differ from the calculation by 20%−50%. Final state interaction (FSI) calculations using the generalized Eikonal Approximation indicate that FSI should change the He3/H3 cross-section ratio for this measurement by less than 5%. If these calculations are correct, then the differences at large missing momenta between the He3/H3 experimental and calculated ratios could be due to the underlying NN interaction, and thus could provide new constraints on the previously loosely-constrained short-distance parts of the NN interaction.

Published
2019
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14. Electroexcitation of the Δ+(1232) at low momentum transfer

Author

A. Blomberg, D. Anez, N. Sparveris, A.J. Sarty, M. Paolone, S. Gilad, D. Higinbotham, Z. Ahmed, H. Albataineh, K. Allada, B. Anderson, K. Aniol, J. Annand, J. Arrington, T. Averett, H. Baghdasaryan, X. Bai, A. Beck, S. Beck, V. Bellini, F. Benmokhtar, W. Boeglin, C.M. Camacho, A. Camsonne, C. Chen, J.P. Chen, K. Chirapatpimol, E. Cisbani, M. Dalton, W. Deconinck, M. Defurne, R. De Leo, D. Flay, N. Fomin, M. Friend, S. Frullani, E. Fuchey, F. Garibaldi, R. Gilman, C. Gu, D. Hamilton, C. Hanretty, O. Hansen, M. Hashemi Shabestari, O. Hen, T. Holmstrom, M. Huang, S. Iqbal, N. Kalantarians, H. Kang, A. Kelleher, M. Khandaker, I. Korover, J. Leckey, J. LeRose, R. Lindgren, E. Long, J. Mammei, D.J. Margaziotis, A. Martí Jimenez-Arguello, D. Meekins, Z.E. Meziani, M. Mihovilovic, N. Muangma, B. Norum, Nuruzzaman, K. Pan, S. Phillips, E. Piasetzky, A. Polychronopoulou, I. Pomerantz, M. Posik, V. Punjabi, X. Qian, A. Rakhman, P.E. Reimer, S. Riordan, G. Ron, A. Saha, E. Schulte, L. Selvy, R. Shneor, S. Sirca, J. Sjoegren, R. Subedi, V. Sulkosky, W. Tireman, D. Wang, J. Watson, B. Wojtsekhowski, W. Yan, I. Yaron, Z. Ye, X. Zhan, J. Zhang, Y. Zhang, B. Zhao, Z. Zhao, X. Zheng, and P. Zhu

Subjects
CMR, Pion electroproduction, Nucleon deformation, Physics, QC1-999
Abstract

We report on new p(e,e′p)π∘ measurements at the Δ+(1232) resonance at the low momentum transfer region, where the mesonic cloud dynamics is predicted to be dominant and rapidly changing, offering a test bed for chiral effective field theory calculations. The new data explore the Q2 dependence of the resonant quadrupole amplitudes and for the first time indicate that the Electric and the Coulomb quadrupole amplitudes converge as Q2→0. The measurements of the Coulomb quadrupole amplitude have been extended to the lowest momentum transfer ever reached, and suggest that more than half of its magnitude is attributed to the mesonic cloud in this region. The new data disagree with predictions of constituent quark models and are in reasonable agreement with dynamical calculations that include pion cloud effects, chiral effective field theory and lattice calculations. The measurements indicate that improvement is required to the theoretical calculations and provide valuable input that will allow their refinements.

Published
2016
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15. Probing the Repulsive Core of the Nucleon-Nucleon Interaction via the 4He(e,e'pN) Triple-Coincidence Reaction

Author

Muangma, I. Korover N., Hen, O., Shneor, R., Sulkosky, V., Kelleher, A., Gilad, S., Higinbotham, D. W., Watson, E. Piasetzky J., Wood, S., Rakhman, Abdurahim, Aguilera, P., Ahmed, Z., Albataineh, H., Allada, K., Anderson, B., Anez, D., Aniol, K., Annand, J., Armstrong, W., Arrington, J., Averett, T., Badman, T., Baghdasaryan, H., Bai, X., Beck, A., Beck, S., Bellini, V., Benmokhtar, F., Bertozzi, W., Bittner, J., Boeglin, W., Camsonne, A., Chen, C., Chen, J. -P., Chirapatpimol, K., Cisbani, E., Dalton, M. M., Daniel, A., Day, D., de Jager, C. W., De Leo, R., Deconinck, W., Defurne, M., Flay, D., Fomin, N., Friend, M., Frullani, S., Fuchey, E., Garibaldi, F., Gaskell, D., Gilman, R., Glamazdin, O., Gu, C., Gueye, P., Hamilton, D., Hanretty, C., Hansen, O., Shabestari, M. Hashemi, Holmstrom, T., Huang, M., Iqbal, S., Jin, G., Kalantarians, N., Kang, H., Khandaker, M., LeRose, J., Leckey, J., Lindgren, R., Long, E., Mammei, J., Margaziotis, D. J., Markowitz, P., Jimenez-Arguello, A. Marti, Meekins, D., Meziani, Z., Michaels, R., Mihovilovic, M., Monaghan, P., Camacho, C. Munoz, Norum, B., Nuruzzaman, Pan, K., Phillips, S., Pomerantz, I., Posik, M., Punjabi, V., Qian, X., Qiang, Y., Qiu, X., Reimer, P. E., Riordan, S., Ron, G., Rondon-Aramayo, O., Saha, A., Schulte, E., Selvy, L., Shahinyan, A., Sirca, S., Sjoegren, J., Slifer, K., Solvignon, P., Sparveris, N., Subedi, R., Tireman, W., Wang, D., Weinstein, L. B., Wojtsekhowski, B., Yan, W., Yaron, I., Ye, Z., Zhan, X., Zhang, J., Zhang, Y., Zhao, B., Zhao, Z., Zheng, X., Zhu, P., and Zielinski, R.

Subjects
Nuclear Experiment
Abstract

We studied simultaneously the 4He(e,e'p), 4He(e,e'pp), and 4He(e,e'pn) reactions at Q^2=2 [GeV/c]2 and x_B>1, for a (e,e'p) missing-momentum range of 400 to 830 MeV/c. The knocked-out proton was detected in coincidence with a proton or neutron recoiling almost back to back to the missing momentum, leaving the residual A=2 system at low excitation energy. These data were used to identify two-nucleon short-range correlated pairs and to deduce their isospin structure as a function of missing momentum in a region where the nucleon-nucleon force is expected to change from predominantly tensor to repulsive. Neutron-proton pairs dominate the high-momentum tail of the nucleon momentum distributions, but their abundance is reduced as the nucleon momentum increases beyond ~500 MeV/c. The extracted fraction of proton-proton pairs is small and almost independent of the missing momentum in the range we studied. Our data are compared with ab-initio calculations of two-nucleon momentum distributions in 4He., Comment: 6 pages, 2 figures

Published
2014
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16. Proton spin structure and generalized polarizabilities in the strong quantum chromodynamics regime

Author

D. Ruth, R. Zielinski, C. Gu, M. Allada, T. Badman, M. Huang, J. Liu, P. Zhu, K. Allada, J. Zhang, A. Camsonne, J.-P. Chen, K. Slifer, K. Aniol, J. Annand, J. Arrington, T. Averett, H. Baghdasaryan, V. Bellini, W. Boeglin, J. Brock, C. Carlin, C. Chen, E. Cisbani, D. Crabb, A. Daniel, D. Day, R. Duve, L. El Fassi, M. Friedman, E. Fuchey, H. Gao, R. Gilman, S. Glamazdin, P. Gueye, M. Hafez, Y. Han, O. Hansen, M. Hashemi Shabestari, O. Hen, D. Higinbotham, T. Horn, S. Iqbal, E. Jensen, H. Kang, C. D. Keith, A. Kelleher, D. Keller, H. Khanal, I. Korover, G. Kumbartzki, W. Li, J. Lichtenstadt, R. Lindgren, E. Long, S. Malace, P. Markowitz, J. Maxwell, D. M. Meekins, Z. E. Meziani, C. McLean, R. Michaels, M. Mihovilovič, N. Muangma, C. Munoz Camacho, J. Musson, K. Myers, Y. Oh, M. Pannunzio Carmignotto, C. Perdrisat, S. Phillips, E. Piasetzky, J. Pierce, V. Punjabi, Y. Qiang, P. E. Reimer, Y. Roblin, G. Ron, O. Rondon, G. Russo, K. Saenboonruang, B. Sawatzky, A. Shahinyan, R. Shneor, S. Širca, J. Sjoegren, P. Solvignon-Slifer, N. Sparveris, V. Sulkosky, F. Wesselmann, W. Yan, H. Yang, H. Yao, Z. Ye, M. Yurov, Y. Zhang, Y. X. Zhao, and X. Zheng

Subjects
General Physics and Astronomy
Published
2022

17. Detector requirements and simulation results for the EIC exclusive, diffractive and tagging physics program using the ECCE detector concept

Author

A. Bylinkin, C.T. Dean, S. Fegan, D. Gangadharan, K. Gates, S.J.D. Kay, I. Korover, W.B. Li, X. Li, R. Montgomery, D. Nguyen, G. Penman, J.R. Pybus, N. Santiesteban, S. Shimizu, R. Trotta, A. Usman, M.D. Baker, J. Frantz, D.I. Glazier, D.W. Higinbotham, T. Horn, J. Huang, G.M. Huber, R. Reed, J. Roche, A. Schmidt, P. Steinberg, J. Stevens, Y. Goto, C. Munoz Camacho, M. Murray, Z. Papandreou, W. Zha, J.K. Adkins, Y. Akiba, A. Albataineh, M. Amaryan, I.C. Arsene, C. Ayerbe Gayoso, J. Bae, X. Bai, M. Bashkanov, R. Bellwied, F. Benmokhtar, V. Berdnikov, J.C. Bernauer, F. Bock, W. Boeglin, M. Borysova, E. Brash, P. Brindza, W.J. Briscoe, M. Brooks, S. Bueltmann, M.H.S. Bukhari, R. Capobianco, W.-C. Chang, Y. Cheon, K. Chen, K.-F. Chen, K.-Y. Cheng, M. Chiu, T. Chujo, Z. Citron, E. Cline, E. Cohen, T. Cormier, Y. Corrales Morales, C. Cotton, J. Crafts, C. Crawford, S. Creekmore, C. Cuevas, J. Cunningham, G. David, M. Demarteau, S. Diehl, N. Doshita, R. Dupré, J.M. Durham, R. Dzhygadlo, R. Ehlers, L. El Fassi, A. Emmert, R. Ent, C. Fanelli, R. Fatemi, M. Finger, M. Friedman, I. Friscic, S. Gardner, F. Geurts, R. Gilman, E. Glimos, N. Grau, S.V. Greene, A.Q. Guo, L. Guo, S.K. Ha, J. Haggerty, T. Hayward, X. He, O. Hen, M. Hoballah, A. Hoghmrtsyan, P.-h.J. Hsu, A. Hutson, K.Y. Hwang, C.E. Hyde, M. Inaba, T. Iwata, H.S. Jo, K. Joo, N. Kalantarians, G. Kalicy, K. Kawade, A. Kim, B. Kim, C. Kim, M. Kim, Y. Kim, E. Kistenev, V. Klimenko, S.H. Ko, W. Korsch, G. Krintiras, S. Kuhn, C.-M. Kuo, T. Kutz, J. Lajoie, D. Lawrence, S. Lebedev, H. Lee, J.S.H. Lee, S.W. Lee, Y.-J. Lee, W. Li, Y.T. Liang, S. Lim, C.-h. Lin, D.X. Lin, K. Liu, M.X. Liu, K. Livingston, N. Liyanage, W.J. Llope, C. Loizides, E. Long, R.-S. Lu, Z. Lu, W. Lynch, S. Mantry, D. Marchand, M. Marcisovsky, C. Markert, P. Markowitz, H. Marukyan, P. McGaughey, M. Mihovilovic, R.G. Milner, A. Milov, Y. Miyachi, A. Mkrtchyan, P. Monaghan, D. Morrison, A. Movsisyan, H. Mkrtchyan, K. Nagai, J. Nagle, I. Nakagawa, C. Nattrass, S. Niccolai, R. Nouicer, G. Nukazuka, M. Nycz, V.A. Okorokov, S. Orešić, J.D. Osborn, C. O’Shaughnessy, S. Paganis, S.F. Pate, M. Patel, C. Paus, M.G. Perdekamp, D.V. Perepelitsa, H. Periera da Costa, K. Peters, W. Phelps, E. Piasetzky, C. Pinkenburg, I. Prochazka, T. Protzman, M.L. Purschke, J. Putschke, R. Rajput-Ghoshal, J. Rasson, B. Raue, K.F. Read, K. Røed, J. Reinhold, E.L. Renner, J. Richards, C. Riedl, T. Rinn, G.M. Roland, G. Ron, M. Rosati, C. Royon, J. Ryu, S. Salur, R. Santos, M. Sarsour, J. Schambach, N. Schmidt, C. Schwarz, J. Schwiening, R. Seidl, A. Sickles, P. Simmerling, S. Sirca, D. Sharma, Z. Shi, T.-A. Shibata, C.-W. Shih, U. Shrestha, K. Slifer, K. Smith, D. Sokhan, R. Soltz, W. Sondheim, J. Song, I.I. Strakovsky, P. Stepanov, J. Strube, P. Sun, X. Sun, K. Suresh, V. Tadevosyan, W.-C. Tang, S. Tapia Araya, S. Tarafdar, L. Teodorescu, D. Thomas, A. Timmins, L. Tomasek, N. Trotta, T.S. Tveter, E. Umaka, H.W. van Hecke, C. Van Hulse, J. Velkovska, E. Voutier, P.K. Wang, Q. Wang, Y. Wang, D.P. Watts, N. Wickramaarachchi, L. Weinstein, M. Williams, C.-P. Wong, L. Wood, M.H. Wood, C. Woody, B. Wyslouch, Z. Xiao, Y. Yamazaki, Y. Yang, Z. Ye, H.D. Yoo, M. Yurov, N. Zachariou, W.A. Zajc, J.-L. Zhang, J.-X. Zhang, Y. Zhang, Y.-X. Zhao, X. Zheng, P. Zhuang, HEP, INSPIRE, Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), and Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay

Subjects
Nuclear and High Energy Physics, Physics - Instrumentation and Detectors, detector: performance, [PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex], nucleon: structure, diffraction, FOS: Physical sciences, tagging, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], ion: beam, Diffractive, exclusive, EIC, Tagging, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], Nuclear Experiment (nucl-ex), electron–ion collider, Instrumentation, Nuclear Experiment, detector: design, quark gluon, nucleus, Electron Ion Collider, Instrumentation and Detectors (physics.ins-det), experimental equipment, [PHYS.PHYS.PHYS-INS-DET] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], diffractive, Exclusive, vertex: primary, ECCE, technology: proposed
Abstract

The version of this article on this repository is an arXiv preprint (arXiv:2208.14575v2 [physics.ins-det] Mon, 6 Mar 2023 19:46:42 UTC (39,794 KB)) submitted to Elsevier and is not the final, peer reviewed, corrected article. It is made available under a Creative Commons (CC BY 4.0) Attribution License. This article presents a collection of simulation studies using the ECCE detector concept in the context of the EIC's exclusive, diffractive, and tagging physics program, which aims to further explore the rich quark–gluon structure of nucleons and nuclei. To successfully execute the program, ECCE proposed to utilize the detector system close to the beamline to ensure exclusivity and tag ion beam/fragments for a particular reaction of interest. Preliminary studies confirm the proposed technology and design satisfy the requirements. The projected physics impact results are based on the projected detector performance from the simulation at 10 or 100 fb−1 of integrated luminosity. Additionally, insights related to a potential second EIC detector are documented, which could serve as a guidepost for future development. Office of Nuclear Physics in the Office of Science in the Department of Energy, the National Science Foundation, USA, the Los Alamos National Laboratory Directed Research and Development (LDRD), USA 20200022DR, the Natural Sciences and Engineering Research Council of Canada (NSERC), and the UK Research and Innovation Science and Technology Facilities Council; This research used resources from the Compute and Data Environment for Science (CADES) at the Oak Ridge National Laboratory, which is supported by the Office of Science of the U.S. Department of Energy under Contract No. DE-AC05-00OR22725; Brookhaven National Lab and the Thomas Jefferson National Accelerator Facility which are operated under contracts DE-SC0012704 and DE-AC05-06OR23177 respectively.

Published
2023

18. ECCE sensitivity studies for single hadron transverse single spin asymmetry measurements

Author

R. Seidl, A. Vladimirov, D. Pitonyak, A. Prokudin, J.K. Adkins, Y. Akiba, A. Albataineh, M. Amaryan, I.C. Arsene, C. Ayerbe Gayoso, J. Bae, X. Bai, M.D. Baker, M. Bashkanov, R. Bellwied, F. Benmokhtar, V. Berdnikov, J.C. Bernauer, F. Bock, W. Boeglin, M. Borysova, E. Brash, P. Brindza, W.J. Briscoe, M. Brooks, S. Bueltmann, M.H.S. Bukhari, A. Bylinkin, R. Capobianco, W.-C. Chang, Y. Cheon, K. Chen, K.-F. Chen, K.-Y. Cheng, M. Chiu, T. Chujo, Z. Citron, E. Cline, E. Cohen, T. Cormier, Y. Corrales Morales, C. Cotton, J. Crafts, C. Crawford, S. Creekmore, C. Cuevas, J. Cunningham, G. David, C.T. Dean, M. Demarteau, S. Diehl, N. Doshita, R. Dupré, J.M. Durham, R. Dzhygadlo, R. Ehlers, L. El Fassi, A. Emmert, R. Ent, C. Fanelli, R. Fatemi, S. Fegan, M. Finger, J. Frantz, M. Friedman, I. Friscic, D. Gangadharan, S. Gardner, K. Gates, F. Geurts, R. Gilman, D. Glazier, E. Glimos, Y. Goto, N. Grau, S.V. Greene, A.Q. Guo, L. Guo, S.K. Ha, J. Haggerty, T. Hayward, X. He, O. Hen, D.W. Higinbotham, M. Hoballah, T. Horn, A. Hoghmrtsyan, P.-h.J. Hsu, J. Huang, G. Huber, A. Hutson, K.Y. Hwang, C.E. Hyde, M. Inaba, T. Iwata, H.S. Jo, K. Joo, N. Kalantarians, G. Kalicy, K. Kawade, S.J.D. Kay, A. Kim, B. Kim, C. Kim, M. Kim, Y. Kim, E. Kistenev, V. Klimenko, S.H. Ko, I. Korover, W. Korsch, G. Krintiras, S. Kuhn, C.-M. Kuo, T. Kutz, J. Lajoie, D. Lawrence, S. Lebedev, H. Lee, J.S.H. Lee, S.W. Lee, Y.-J. Lee, W. Li, W.B. Li, X. Li, Y.T. Liang, S. Lim, C.-H. Lin, D.X. Lin, K. Liu, M.X. Liu, K. Livingston, N. Liyanage, W.J. Llope, C. Loizides, E. Long, R.-S. Lu, Z. Lu, W. Lynch, S. Mantry, D. Marchand, M. Marcisovsky, C. Markert, P. Markowitz, H. Marukyan, P. McGaughey, M. Mihovilovic, R.G. Milner, A. Milov, Y. Miyachi, A. Mkrtchyan, P. Monaghan, R. Montgomery, D. Morrison, A. Movsisyan, H. Mkrtchyan, C. Munoz Camacho, M. Murray, K. Nagai, J. Nagle, I. Nakagawa, C. Nattrass, D. Nguyen, S. Niccolai, R. Nouicer, G. Nukazuka, M. Nycz, V.A. Okorokov, S. Orešić, J.D. Osborn, C. O’Shaughnessy, S. Paganis, Z. Papandreou, S.F. Pate, M. Patel, C. Paus, G. Penman, M.G. Perdekamp, D.V. Perepelitsa, H. Periera da Costa, K. Peters, W. Phelps, E. Piasetzky, C. Pinkenburg, I. Prochazka, T. Protzman, M.L. Purschke, J. Putschke, J.R. Pybus, R. Rajput-Ghoshal, J. Rasson, B. Raue, K.F. Read, K. Røed, R. Reed, J. Reinhold, E.L. Renner, J. Richards, C. Riedl, T. Rinn, J. Roche, G.M. Roland, G. Ron, M. Rosati, C. Royon, J. Ryu, S. Salur, N. Santiesteban, R. Santos, M. Sarsour, J. Schambach, A. Schmidt, N. Schmidt, C. Schwarz, J. Schwiening, A. Sickles, P. Simmerling, S. Sirca, D. Sharma, Z. Shi, T.-A. Shibata, C.-W. Shih, S. Shimizu, U. Shrestha, K. Slifer, K. Smith, D. Sokhan, R. Soltz, W. Sondheim, J. Song, I.I. Strakovsky, P. Steinberg, P. Stepanov, J. Stevens, J. Strube, P. Sun, X. Sun, K. Suresh, V. Tadevosyan, W.-C. Tang, S. Tapia Araya, S. Tarafdar, L. Teodorescu, D. Thomas, A. Timmins, L. Tomasek, N. Trotta, R. Trotta, T.S. Tveter, E. Umaka, A. Usman, H.W. van Hecke, C. Van Hulse, J. Velkovska, E. Voutier, P.K. Wang, Q. Wang, Y. Wang, D.P. Watts, N. Wickramaarachchi, L. Weinstein, M. Williams, C.-P. Wong, L. Wood, M.H. Wood, C. Woody, B. Wyslouch, Z. Xiao, Y. Yamazaki, Y. Yang, Z. Ye, H.D. Yoo, M. Yurov, N. Zachariou, W.A. Zajc, W. Zha, J.-L. Zhang, J.-X. Zhang, Y. Zhang, Y.-X. Zhao, X. Zheng, P. Zhuang, Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), and Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay

Subjects
transverse spin dependent distribution and fragmentation functions, Nuclear and High Energy Physics, FOS: Physical sciences, lepton: scattering, transverse momentum dependence, hadron: transverse momentum, fragmentation function, x-dependence, High Energy Physics - Experiment, Sivers function, semi-inclusive DIS, High Energy Physics - Experiment (hep-ex), [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], parton, Collins, Instrumentation, transversity, spin: transverse, flavor, deep inelastic scattering: semi-inclusive reaction, positron p: deep inelastic scattering, nucleon: spin: transverse, sensitivity, Transverse spin dependent distribution and fragmentation functions, error: statistical, kinematics, ECCE detector feasibility studies, charge: tensor, numerical calculations: Monte Carlo, Semi-inclusive DIS, spin: asymmetry
Abstract

We performed feasibility studies for various single transverse spin measurements that are related to the Sivers effect, transversity and the tensor charge, and the Collins fragmentation function. The processes studied include semi-inclusive deep inelastic scattering (SIDIS) where single hadrons (pions and kaons) were detected in addition to the scattered DIS lepton. The data were obtained in {\sc pythia}6 and {\sc geant}4 simulated e+p collisions at 18 GeV on 275 GeV, 18 on 100, 10 on 100, and 5 on 41 that use the ECCE detector configuration. Typical DIS kinematics were selected, most notably $Q^2 > 1 $ GeV$^2$, and cover the $x$ range from $10^{-4}$ to $1$. The single spin asymmetries were extracted as a function of $x$ and $Q^2$, as well as the semi-inclusive variables $z$, and $P_T$. They are obtained in azimuthal moments in combinations of the azimuthal angles of the hadron transverse momentum and transverse spin of the nucleon relative to the lepton scattering plane. The initially unpolarized MonteCarlo was re-weighted in the true kinematic variables, hadron types and parton flavors based on global fits of fixed target SIDIS experiments and $e^+e^-$ annihilation data. The expected statistical precision of such measurements is extrapolated to 10 fb$^{-1}$ and potential systematic uncertainties are approximated given the deviations between true and reconstructed yields. The impact on the knowledge of the Sivers functions, transversity and tensor charges, and the Collins function has then been evaluated in the same phenomenological extractions as in the Yellow Report. The impact is found to be comparable to that obtained with the parameterized Yellow Report detector and shows that the ECCE detector configuration can fulfill the physics goals on these quantities., 22 pages, 22 figures, to be submitted to joint ECCE proposal NIM-A volume

Published
2023

19. Search for e→τ charged lepton flavor violation at the EIC with the ECCE detector

Author

J.-L. Zhang, S. Mantry, J.K. Adkins, Y. Akiba, A. Albataineh, M. Amaryan, I.C. Arsene, C. Ayerbe Gayoso, J. Bae, X. Bai, M.D. Baker, M. Bashkanov, R. Bellwied, F. Benmokhtar, V. Berdnikov, J.C. Bernauer, F. Bock, W. Boeglin, M. Borysova, E. Brash, P. Brindza, W.J. Briscoe, M. Brooks, S. Bueltmann, M.H.S. Bukhari, A. Bylinkin, R. Capobianco, W.-C. Chang, Y. Cheon, K. Chen, K.-F. Chen, K.-Y. Cheng, M. Chiu, T. Chujo, Z. Citron, E. Cline, E. Cohen, T. Cormier, Y. Corrales Morales, C. Cotton, J. Crafts, C. Crawford, S. Creekmore, C. Cuevas, J. Cunningham, G. David, C.T. Dean, M. Demarteau, S. Diehl, N. Doshita, R. Dupré, J.M. Durham, R. Dzhygadlo, R. Ehlers, L. El Fassi, A. Emmert, R. Ent, C. Fanelli, R. Fatemi, S. Fegan, M. Finger, J. Frantz, M. Friedman, I. Friscic, D. Gangadharan, S. Gardner, K. Gates, F. Geurts, R. Gilman, D. Glazier, E. Glimos, Y. Goto, N. Grau, S.V. Greene, A.Q. Guo, L. Guo, S.K. Ha, J. Haggerty, T. Hayward, X. He, O. Hen, D.W. Higinbotham, M. Hoballah, T. Horn, A. Hoghmrtsyan, P.-h.J. Hsu, J. Huang, G. Huber, A. Hutson, K.Y. Hwang, C.E. Hyde, M. Inaba, T. Iwata, H.S. Jo, K. Joo, N. Kalantarians, G. Kalicy, K. Kawade, S.J.D. Kay, A. Kim, B. Kim, C. Kim, M. Kim, Y. Kim, E. Kistenev, V. Klimenko, S.H. Ko, I. Korover, W. Korsch, G. Krintiras, S. Kuhn, C.-M. Kuo, T. Kutz, J. Lajoie, D. Lawrence, S. Lebedev, H. Lee, J.S.H. Lee, S.W. Lee, Y.-J. Lee, W. Li, W.B. Li, X. Li, Y.T. Liang, S. Lim, C.-H. Lin, D.X. Lin, K. Liu, M.X. Liu, K. Livingston, N. Liyanage, W.J. Llope, C. Loizides, E. Long, R.-S. Lu, Z. Lu, W. Lynch, D. Marchand, M. Marcisovsky, C. Markert, P. Markowitz, H. Marukyan, P. McGaughey, M. Mihovilovic, R.G. Milner, A. Milov, Y. Miyachi, A. Mkrtchyan, H. Mkrtchyan, P. Monaghan, R. Montgomery, D. Morrison, A. Movsisyan, C. Munoz Camacho, M. Murray, K. Nagai, J. Nagle, I. Nakagawa, C. Nattrass, D. Nguyen, S. Niccolai, R. Nouicer, G. Nukazuka, M. Nycz, V.A. Okorokov, S. Orešić, J.D. Osborn, C. O’Shaughnessy, S. Paganis, Z. Papandreou, S.F. Pate, M. Patel, C. Paus, G. Penman, M.G. Perdekamp, D.V. Perepelitsa, H. Periera da Costa, K. Peters, W. Phelps, E. Piasetzky, C. Pinkenburg, I. Prochazka, T. Protzman, M.L. Purschke, J. Putschke, J.R. Pybus, R. Rajput-Ghoshal, J. Rasson, B. Raue, K.F. Read, K. Røed, R. Reed, J. Reinhold, E.L. Renner, J. Richards, C. Riedl, T. Rinn, J. Roche, G.M. Roland, G. Ron, M. Rosati, C. Royon, J. Ryu, S. Salur, N. Santiesteban, R. Santos, M. Sarsour, J. Schambach, A. Schmidt, N. Schmidt, C. Schwarz, J. Schwiening, R. Seidl, A. Sickles, P. Simmerling, S. Sirca, D. Sharma, Z. Shi, T.-A. Shibata, C.-W. Shih, S. Shimizu, U. Shrestha, K. Slifer, K. Smith, D. Sokhan, R. Soltz, W. Sondheim, J. Song, I.I. Strakovsky, P. Steinberg, P. Stepanov, J. Stevens, J. Strube, P. Sun, X. Sun, K. Suresh, V. Tadevosyan, W.-C. Tang, S. Tapia Araya, S. Tarafdar, L. Teodorescu, D. Thomas, A. Timmins, L. Tomasek, N. Trotta, R. Trotta, T.S. Tveter, E. Umaka, A. Usman, H.W. van Hecke, C. Van Hulse, J. Velkovska, E. Voutier, P.K. Wang, Q. Wang, Y. Wang, D.P. Watts, N. Wickramaarachchi, L. Weinstein, M. Williams, C.-P. Wong, L. Wood, M.H. Wood, C. Woody, B. Wyslouch, Z. Xiao, Y. Yamazaki, Y. Yang, Z. Ye, H.D. Yoo, M. Yurov, N. Zachariou, W.A. Zajc, W. Zha, J.-X. Zhang, Y. Zhang, Y.-X. Zhao, X. Zheng, and P. Zhuang

Subjects
Nuclear and High Energy Physics, Instrumentation
Published
2023

20. Exclusive J/ψ detection and physics with ECCE

Author

X. Li, J.K. Adkins, Y. Akiba, A. Albataineh, M. Amaryan, I.C. Arsene, C. Ayerbe Gayoso, J. Bae, X. Bai, M.D. Baker, M. Bashkanov, R. Bellwied, F. Benmokhtar, V. Berdnikov, J.C. Bernauer, F. Bock, W. Boeglin, M. Borysova, E. Brash, P. Brindza, W.J. Briscoe, M. Brooks, S. Bueltmann, M.H.S. Bukhari, A. Bylinkin, R. Capobianco, W.-C. Chang, Y. Cheon, K. Chen, K.-F. Chen, K.-Y. Cheng, M. Chiu, T. Chujo, Z. Citron, E. Cline, E. Cohen, T. Cormier, Y. Corrales Morales, C. Cotton, J. Crafts, C. Crawford, S. Creekmore, C. Cuevas, J. Cunningham, G. David, C.T. Dean, M. Demarteau, S. Diehl, N. Doshita, R. Dupré, J.M. Durham, R. Dzhygadlo, R. Ehlers, L. El Fassi, A. Emmert, R. Ent, C. Fanelli, R. Fatemi, S. Fegan, M. Finger, J. Frantz, M. Friedman, I. Friscic, D. Gangadharan, S. Gardner, K. Gates, F. Geurts, R. Gilman, D. Glazier, E. Glimos, Y. Goto, N. Grau, S.V. Greene, A.Q. Guo, L. Guo, S.K. Ha, J. Haggerty, T. Hayward, X. He, O. Hen, D.W. Higinbotham, M. Hoballah, T. Horn, A. Hoghmrtsyan, P.-h.J. Hsu, J. Huang, G. Huber, A. Hutson, K.Y. Hwang, C.E. Hyde, M. Inaba, T. Iwata, H.S. Jo, K. Joo, N. Kalantarians, G. Kalicy, K. Kawade, S.J.D. Kay, A. Kim, B. Kim, C. Kim, M. Kim, Y. Kim, E. Kistenev, V. Klimenko, S.H. Ko, I. Korover, W. Korsch, G. Krintiras, S. Kuhn, C.-M. Kuo, T. Kutz, J. Lajoie, D. Lawrence, S. Lebedev, H. Lee, J.S.H. Lee, S.W. Lee, Y.-J. Lee, W. Li, W.B. Li, Y.T. Liang, S. Lim, C.-H. Lin, D.X. Lin, K. Liu, M.X. Liu, K. Livingston, N. Liyanage, W.J. Llope, C. Loizides, E. Long, R.-S. Lu, Z. Lu, W. Lynch, S. Mantry, D. Marchand, M. Marcisovsky, C. Markert, P. Markowitz, H. Marukyan, P. McGaughey, M. Mihovilovic, R.G. Milner, A. Milov, Y. Miyachi, A. Mkrtchyan, P. Monaghan, R. Montgomery, D. Morrison, A. Movsisyan, H. Mkrtchyan, C. Munoz Camacho, M. Murray, K. Nagai, J. Nagle, I. Nakagawa, C. Nattrass, D. Nguyen, S. Niccolai, R. Nouicer, G. Nukazuka, M. Nycz, V.A. Okorokov, S. Orešić, J.D. Osborn, C. O’Shaughnessy, S. Paganis, Z. Papandreou, S.F. Pate, M. Patel, C. Paus, G. Penman, M.G. Perdekamp, D.V. Perepelitsa, H. Periera da Costa, K. Peters, W. Phelps, E. Piasetzky, C. Pinkenburg, I. Prochazka, T. Protzman, M.L. Purschke, J. Putschke, J.R. Pybus, R. Rajput-Ghoshal, J. Rasson, B. Raue, K.F. Read, K. Røed, R. Reed, J. Reinhold, E.L. Renner, J. Richards, C. Riedl, T. Rinn, J. Roche, G.M. Roland, G. Ron, M. Rosati, C. Royon, J. Ryu, S. Salur, N. Santiesteban, R. Santos, M. Sarsour, J. Schambach, A. Schmidt, N. Schmidt, C. Schwarz, J. Schwiening, R. Seidl, A. Sickles, P. Simmerling, S. Sirca, D. Sharma, Z. Shi, T.-A. Shibata, C.-W. Shih, S. Shimizu, U. Shrestha, K. Slifer, K. Smith, D. Sokhan, R. Soltz, W. Sondheim, J. Song, I.I. Strakovsky, P. Steinberg, P. Stepanov, J. Stevens, J. Strube, P. Sun, X. Sun, K. Suresh, V. Tadevosyan, W.-C. Tang, S. Tapia Araya, S. Tarafdar, L. Teodorescu, D. Thomas, A. Timmins, L. Tomasek, N. Trotta, R. Trotta, T.S. Tveter, E. Umaka, A. Usman, H.W. van Hecke, C. Van Hulse, J. Velkovska, E. Voutier, P.K. Wang, Q. Wang, Y. Wang, D.P. Watts, N. Wickramaarachchi, L. Weinstein, M. Williams, C.-P. Wong, L. Wood, M.H. Wood, C. Woody, B. Wyslouch, Z. Xiao, Y. Yamazaki, Y. Yang, Z. Ye, H.D. Yoo, M. Yurov, N. Zachariou, W.A. Zajc, W. Zha, J.-L. Zhang, J.-X. Zhang, Y. Zhang, Y.-X. Zhao, X. Zheng, P. Zhuang, Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), and Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay

Subjects
Nuclear and High Energy Physics, Physics - Instrumentation and Detectors, Quarkonia, design, electron nucleon, Near threshold, EIC, pomeron, threshold, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], colliding beams, structure, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], Nuclear Experiment, Instrumentation, detector, exchange, nucleus, Electron Ion Collider, nucleon, gluon, statistics, Exclusive, mass, production, ECCE, quarkonium, performance, photoproduction
Abstract

Exclusive heavy quarkonium photoproduction is one of the most popular processes in EIC, which has a large cross section and a simple final state. Due to the gluonic nature of the exchange Pomeron, this process can be related to the gluon distributions in the nucleus. The momentum transfer dependence of this process is sensitive to the interaction sites, which provides a powerful tool to probe the spatial distribution of gluons in the nucleus. Recently the problem of the origin of hadron mass has received lots of attention in determining the anomaly contribution $M_{a}$. The trace anomaly is sensitive to the gluon condensate, and exclusive production of quarkonia such as J/$\psi$ and $\Upsilon$ can serve as a sensitive probe to constrain it. In this paper, we present the performance of the ECCE detector for exclusive J/$\psi$ detection and the capability of this process to investigate the above physics opportunities with ECCE., Comment: 11 pages, 14 figures, 1 table

Published
2023

21. AI-assisted Optimization of the ECCE Tracking System at the Electron Ion Collider

Author

C. Fanelli, Z. Papandreou, K. Suresh, J.K. Adkins, Y. Akiba, A. Albataineh, M. Amaryan, I.C. Arsene, C. Ayerbe Gayoso, J. Bae, X. Bai, M.D. Baker, M. Bashkanov, R. Bellwied, F. Benmokhtar, V. Berdnikov, J.C. Bernauer, F. Bock, W. Boeglin, M. Borysova, E. Brash, P. Brindza, W.J. Briscoe, M. Brooks, S. Bueltmann, M.H.S. Bukhari, A. Bylinkin, R. Capobianco, W.-C. Chang, Y. Cheon, K. Chen, K.-F. Chen, K.-Y. Cheng, M. Chiu, T. Chujo, Z. Citron, E. Cline, E. Cohen, T. Cormier, Y. Corrales Morales, C. Cotton, J. Crafts, C. Crawford, S. Creekmore, C. Cuevas, J. Cunningham, G. David, C.T. Dean, M. Demarteau, S. Diehl, N. Doshita, R. Dupré, J.M. Durham, R. Dzhygadlo, R. Ehlers, L. El Fassi, A. Emmert, R. Ent, R. Fatemi, S. Fegan, M. Finger, J. Frantz, M. Friedman, I. Friscic, D. Gangadharan, S. Gardner, K. Gates, F. Geurts, R. Gilman, D. Glazier, E. Glimos, Y. Goto, N. Grau, S.V. Greene, A.Q. Guo, L. Guo, S.K. Ha, J. Haggerty, T. Hayward, X. He, O. Hen, D.W. Higinbotham, M. Hoballah, T. Horn, A. Hoghmrtsyan, P.-h.J. Hsu, J. Huang, G. Huber, A. Hutson, K.Y. Hwang, C.E. Hyde, M. Inaba, T. Iwata, H.S. Jo, K. Joo, N. Kalantarians, G. Kalicy, K. Kawade, S.J.D. Kay, A. Kim, B. Kim, C. Kim, M. Kim, Y. Kim, E. Kistenev, V. Klimenko, S.H. Ko, I. Korover, W. Korsch, G. Krintiras, S. Kuhn, C.-M. Kuo, T. Kutz, J. Lajoie, D. Lawrence, S. Lebedev, H. Lee, J.S.H. Lee, S.W. Lee, Y.-J. Lee, W. Li, W.B. Li, X. Li, Y.T. Liang, S. Lim, C.-H. Lin, D.X. Lin, K. Liu, M.X. Liu, K. Livingston, N. Liyanage, W.J. Llope, C. Loizides, E. Long, R.-S. Lu, Z. Lu, W. Lynch, S. Mantry, D. Marchand, M. Marcisovsky, C. Markert, P. Markowitz, H. Marukyan, P. McGaughey, M. Mihovilovic, R.G. Milner, A. Milov, Y. Miyachi, A. Mkrtchyan, P. Monaghan, R. Montgomery, D. Morrison, A. Movsisyan, H. Mkrtchyan, C. Munoz Camacho, M. Murray, K. Nagai, J. Nagle, I. Nakagawa, C. Nattrass, D. Nguyen, S. Niccolai, R. Nouicer, G. Nukazuka, M. Nycz, V.A. Okorokov, S. Orešić, J.D. Osborn, C. O’Shaughnessy, S. Paganis, S.F. Pate, M. Patel, C. Paus, G. Penman, M.G. Perdekamp, D.V. Perepelitsa, H. Periera da Costa, K. Peters, W. Phelps, E. Piasetzky, C. Pinkenburg, I. Prochazka, T. Protzman, M.L. Purschke, J. Putschke, J.R. Pybus, R. Rajput-Ghoshal, J. Rasson, B. Raue, K.F. Read, K. Røed, R. Reed, J. Reinhold, E.L. Renner, J. Richards, C. Riedl, T. Rinn, J. Roche, G.M. Roland, G. Ron, M. Rosati, C. Royon, J. Ryu, S. Salur, N. Santiesteban, R. Santos, M. Sarsour, J. Schambach, A. Schmidt, N. Schmidt, C. Schwarz, J. Schwiening, R. Seidl, A. Sickles, P. Simmerling, S. Sirca, D. Sharma, Z. Shi, T.-A. Shibata, C.-W. Shih, S. Shimizu, U. Shrestha, K. Slifer, K. Smith, D. Sokhan, R. Soltz, W. Sondheim, J. Song, I.I. Strakovsky, P. Steinberg, P. Stepanov, J. Stevens, J. Strube, P. Sun, X. Sun, V. Tadevosyan, W.-C. Tang, S. Tapia Araya, S. Tarafdar, L. Teodorescu, D. Thomas, A. Timmins, L. Tomasek, N. Trotta, R. Trotta, T.S. Tveter, E. Umaka, A. Usman, H.W. van Hecke, C. Van Hulse, J. Velkovska, E. Voutier, P.K. Wang, Q. Wang, Y. Wang, D.P. Watts, N. Wickramaarachchi, L. Weinstein, M. Williams, C.-P. Wong, L. Wood, M.H. Wood, C. Woody, B. Wyslouch, Z. Xiao, Y. Yamazaki, Y. Yang, Z. Ye, H.D. Yoo, M. Yurov, N. Zachariou, W.A. Zajc, W. Zha, J.-L. Zhang, J.-X. Zhang, Y. Zhang, Y.-X. Zhao, X. Zheng, P. Zhuang, HEP, INSPIRE, Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), and Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay

Subjects
FOS: Computer and information sciences, Nuclear and High Energy Physics, Computer Science - Machine Learning, Physics - Instrumentation and Detectors, [PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex], [PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex], FOS: Physical sciences, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], [INFO] Computer Science [cs], Machine Learning (cs.LG), High Energy Physics - Experiment, Brookhaven Lab, High Energy Physics - Experiment (hep-ex), [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], [INFO]Computer Science [cs], tracking detector, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], evolutionary algorithms, Nuclear Experiment (nucl-ex), numerical calculations, Instrumentation, Nuclear Experiment, detector: design, Bayesian optimization, Instrumentation and Detectors (physics.ins-det), tracking, Computational Physics (physics.comp-ph), artificial intelligence, electron nucleus: colliding beams, [PHYS.PHYS.PHYS-INS-DET] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], ECCE, Physics - Computational Physics, electron ion collider, performance
Abstract

The Electron-Ion Collider (EIC) is a cutting-edge accelerator facility that will study the nature of the "glue" that binds the building blocks of the visible matter in the universe. The proposed experiment will be realized at Brookhaven National Laboratory in approximately 10 years from now, with detector design and R&D currently ongoing. Notably, EIC is one of the first large-scale facilities to leverage Artificial Intelligence (AI) already starting from the design and R&D phases. The EIC Comprehensive Chromodynamics Experiment (ECCE) is a consortium that proposed a detector design based on a 1.5T solenoid. The EIC detector proposal review concluded that the ECCE design will serve as the reference design for an EIC detector. Herein we describe a comprehensive optimization of the ECCE tracker using AI. The work required a complex parametrization of the simulated detector system. Our approach dealt with an optimization problem in a multidimensional design space driven by multiple objectives that encode the detector performance, while satisfying several mechanical constraints. We describe our strategy and show results obtained for the ECCE tracking system. The AI-assisted design is agnostic to the simulation framework and can be extended to other sub-detectors or to a system of sub-detectors to further optimize the performance of the EIC detector., 16 pages, 18 figures, 2 appendices, 3 tables

Published
2022

22. Scientific Computing Plan for the ECCE Detector at the Electron Ion Collider

Author

J.C. Bernauer, C.T. Dean, C. Fanelli, J. Huang, K. Kauder, D. Lawrence, J.D. Osborn, C. Paus, J.K. Adkins, Y. Akiba, A. Albataineh, M. Amaryan, I.C. Arsene, C. Ayerbe Gayoso, J. Bae, X. Bai, M.D. Baker, M. Bashkanov, R. Bellwied, F. Benmokhtar, V. Berdnikov, F. Bock, W. Boeglin, M. Borysova, E. Brash, P. Brindza, W.J. Briscoe, M. Brooks, S. Bueltmann, M.H.S. Bukhari, A. Bylinkin, R. Capobianco, W.-C. Chang, Y. Cheon, K. Chen, K.-F. Chen, K.-Y. Cheng, M. Chiu, T. Chujo, Z. Citron, E. Cline, E. Cohen, T. Cormier, Y. Corrales Morales, C. Cotton, J. Crafts, C. Crawford, S. Creekmore, C. Cuevas, J. Cunningham, G. David, M. Demarteau, S. Diehl, N. Doshita, R. Dupré, J.M. Durham, R. Dzhygadlo, R. Ehlers, L. El Fassi, A. Emmert, R. Ent, R. Fatemi, S. Fegan, M. Finger, J. Frantz, M. Friedman, I. Friscic, D. Gangadharan, S. Gardner, K. Gates, F. Geurts, R. Gilman, D. Glazier, E. Glimos, Y. Goto, N. Grau, S.V. Greene, A.Q. Guo, L. Guo, S.K. Ha, J. Haggerty, T. Hayward, X. He, O. Hen, D.W. Higinbotham, M. Hoballah, T. Horn, A. Hoghmrtsyan, P.-h.J. Hsu, G. Huber, A. Hutson, K.Y. Hwang, C. Hyde, M. Inaba, T. Iwata, H.S. Jo, K. Joo, N. Kalantarians, G. Kalicy, K. Kawade, S.J.D. Kay, A. Kim, B. Kim, C. Kim, M. Kim, Y. Kim, E. Kistenev, V. Klimenko, S.H. Ko, I. Korover, W. Korsch, G. Krintiras, S. Kuhn, C.-M. Kuo, T. Kutz, J. Lajoie, S. Lebedev, H. Lee, J.S.H. Lee, S.W. Lee, Y.-J. Lee, W. Li, X. Li, Y.T. Liang, S. Lim, C.-h. Lin, D.X. Lin, K. Liu, M.X. Liu, K. Livingston, N. Liyanage, W.J. Llope, C. Loizides, E. Long, R.-S. Lu, Z. Lu, W. Lynch, D. Marchand, M. Marcisovsky, P. Markowitz, H. Marukyan, P. McGaughey, M. Mihovilovic, R.G. Milner, A. Milov, Y. Miyachi, A. Mkrtchyan, P. Monaghan, R. Montgomery, D. Morrison, A. Movsisyan, H. Mkrtchyan, C. Munoz Camacho, M. Murray, K. Nagai, J. Nagle, I. Nakagawa, C. Nattrass, D. Nguyen, S. Niccolai, R. Nouicer, G. Nukazuka, M. Nycz, V.A. Okorokov, S. Orešić, C. O’Shaughnessy, S. Paganis, Z. Papandreou, S.F. Pate, M. Patel, G. Penman, M.G. Perdekamp, D.V. Perepelitsa, H. Periera da Costa, K. Peters, W. Phelps, E. Piasetzky, C. Pinkenburg, I. Prochazka, T. Protzman, M.L. Purschke, J. Putschke, J.R. Pybus, R. Rajput-Ghoshal, J. Rasson, B. Raue, K. Read, K. Røed, R. Reed, J. Reinhold, E.L. Renner, J. Richards, C. Riedl, T. Rinn, J. Roche, G.M. Roland, G. Ron, M. Rosati, C. Royon, J. Ryu, S. Salur, N. Santiesteban, R. Santos, M. Sarsour, J. Schambach, A. Schmidt, N. Schmidt, C. Schwarz, J. Schwiening, R. Seidl, A. Sickles, P. Simmerling, S. Sirca, D. Sharma, Z. Shi, T.-A. Shibata, C.-W. Shih, S. Shimizu, U. Shrestha, K. Slifer, K. Smith, D. Sokhan, R. Soltz, W. Sondheim, J. Song, I.I. Strakovsky, P. Steinberg, P. Stepanov, J. Stevens, J. Strube, P. Sun, X. Sun, K. Suresh, V. Tadevosyan, W.-C. Tang, S. Tapia Araya, S. Tarafdar, L. Teodorescu, A. Timmins, L. Tomasek, N. Trotta, R. Trotta, T.S. Tveter, E. Umaka, A. Usman, H.W. van Hecke, C. Van Hulse, J. Velkovska, E. Voutier, P.K. Wang, Q. Wang, Y. Wang, D.P. Watts, N. Wickramaarachchi, L. Weinstein, M. Williams, C.-P. Wong, L. Wood, M.H. Wood, C. Woody, B. Wyslouch, Z. Xiao, Y. Yamazaki, Y. Yang, Z. Ye, H.D. Yoo, M. Yurov, N. Zachariou, W.A. Zajc, J. Zhang, Y. Zhang, Y.X. Zhao, X. Zheng, P. Zhuang, Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), and Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay

Subjects
Nuclear and High Energy Physics, Physics - Instrumentation and Detectors, data acquisition, FOS: Physical sciences, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], programming, computer: network, High Energy Physics - Experiment, Brookhaven Lab, High Energy Physics - Experiment (hep-ex), data compilation, quantum chromodynamics, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], [INFO]Computer Science [cs], [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], Nuclear Experiment (nucl-ex), numerical calculations, Instrumentation, Nuclear Experiment, activity report, track data analysis, Instrumentation and Detectors (physics.ins-det), Computational Physics (physics.comp-ph), artificial intelligence, calibration, detector: proposed, electron nucleus: colliding beams, federated computing, data management, Physics - Computational Physics, electron ion collider, Jefferson Lab
Abstract

This is the arXiv pre-print which has not been peer reviewed. It is made available under a Creative Commons (CC BY) Attribution Lciense. The corrected version of record is available at: https://doi.org/10.1016/j.nima.2022.167859. Cite as: arXiv:2205.08607 [physics.ins-det] (or arXiv:2205.08607v1 [physics.ins-det] for this version) https://doi.org/10.48550/arXiv.2205.08607 Focus to learn more Journal reference: NIMA 1047, 167859 (2023) Related DOI: https://doi.org/10.1016/j.nima.2022.167859 Focus to learn more Submission history From: Joseph Osborn [view email] [v1] Tue, 17 May 2022 19:53:56 UTC (29,605 KB) Copyright © 2022 The Author(s). The Electron Ion Collider (EIC) is the next generation of precision QCD facility to be built at Brookhaven National Laboratory in conjunction with Thomas Jefferson National Laboratory. There are a significant number of software and computing challenges that need to be overcome at the EIC. During the EIC detector proposal development period, the ECCE consortium began identifying and addressing these challenges in the process of producing a complete detector proposal based upon detailed detector and physics simulations. In this document, the software and computing efforts to produce this proposal are discussed; furthermore, the computing and software model and resources required for the future of ECCE are described. Office of Nuclear Physics in the Office of Science in the Department of Energy, USA; National Science Foundation, USA; Los Alamos National Laboratory Laboratory Directed Research and Development (LDRD), USA 20200022DR.

Published
2022

23. Measurement of the Nucleon F_{2}^{n}/F_{2}^{p} Structure Function Ratio by the Jefferson Lab MARATHON Tritium/Helium-3 Deep Inelastic Scattering Experiment

Author

D, Abrams, H, Albataineh, B S, Aljawrneh, S, Alsalmi, D, Androic, K, Aniol, W, Armstrong, J, Arrington, H, Atac, T, Averett, C Ayerbe, Gayoso, X, Bai, J, Bane, S, Barcus, A, Beck, V, Bellini, H, Bhatt, D, Bhetuwal, D, Biswas, D, Blyth, W, Boeglin, D, Bulumulla, J, Butler, A, Camsonne, M, Carmignotto, J, Castellanos, J-P, Chen, E O, Cohen, S, Covrig, K, Craycraft, R, Cruz-Torres, B, Dongwi, B, Duran, D, Dutta, E, Fuchey, C, Gal, T N, Gautam, S, Gilad, K, Gnanvo, T, Gogami, J, Gomez, C, Gu, A, Habarakada, T, Hague, J-O, Hansen, M, Hattawy, F, Hauenstein, D W, Higinbotham, R J, Holt, E W, Hughes, C, Hyde, H, Ibrahim, S, Jian, S, Joosten, A, Karki, B, Karki, A T, Katramatou, C, Keith, C, Keppel, M, Khachatryan, V, Khachatryan, A, Khanal, A, Kievsky, D, King, P M, King, I, Korover, S A, Kulagin, K S, Kumar, T, Kutz, N, Lashley-Colthirst, S, Li, W, Li, H, Liu, S, Liuti, N, Liyanage, P, Markowitz, R E, McClellan, D, Meekins, S Mey-Tal, Beck, Z-E, Meziani, R, Michaels, M, Mihovilovic, V, Nelyubin, D, Nguyen, Nuruzzaman, M, Nycz, R, Obrecht, M, Olson, V F, Owen, E, Pace, B, Pandey, V, Pandey, M, Paolone, A, Papadopoulou, S, Park, S, Paul, G G, Petratos, R, Petti, E, Piasetzky, R, Pomatsalyuk, S, Premathilake, A J R, Puckett, V, Punjabi, R D, Ransome, M N H, Rashad, P E, Reimer, S, Riordan, J, Roche, G, Salmè, N, Santiesteban, B, Sawatzky, S, Scopetta, A, Schmidt, B, Schmookler, J, Segal, E P, Segarra, A, Shahinyan, S, Širca, N, Sparveris, T, Su, R, Suleiman, H, Szumila-Vance, A S, Tadepalli, L, Tang, W, Tireman, F, Tortorici, G M, Urciuoli, B, Wojtsekhowski, S, Wood, Z H, Ye, Z Y, Ye, and J, Zhang

Abstract

The ratio of the nucleon F_{2} structure functions, F_{2}^{n}/F_{2}^{p}, is determined by the MARATHON experiment from measurements of deep inelastic scattering of electrons from ^{3}H and ^{3}He nuclei. The experiment was performed in the Hall A Facility of Jefferson Lab using two high-resolution spectrometers for electron detection, and a cryogenic target system which included a low-activity tritium cell. The data analysis used a novel technique exploiting the mirror symmetry of the two nuclei, which essentially eliminates many theoretical uncertainties in the extraction of the ratio. The results, which cover the Bjorken scaling variable range 0.19x0.83, represent a significant improvement compared to previous SLAC and Jefferson Lab measurements for the ratio. They are compared to recent theoretical calculations and empirical determinations of the F_{2}^{n}/F_{2}^{p} ratio.

Published
2022

24. Revealing the short-range structure of the mirror nuclei

Author

S, Li, R, Cruz-Torres, N, Santiesteban, Z H, Ye, D, Abrams, S, Alsalmi, D, Androic, K, Aniol, J, Arrington, T, Averett, C Ayerbe, Gayoso, J, Bane, S, Barcus, J, Barrow, A, Beck, V, Bellini, H, Bhatt, D, Bhetuwal, D, Biswas, D, Bulumulla, A, Camsonne, J, Castellanos, J, Chen, J-P, Chen, D, Chrisman, M E, Christy, C, Clarke, S, Covrig, K, Craycraft, D, Day, D, Dutta, E, Fuchey, C, Gal, F, Garibaldi, T N, Gautam, T, Gogami, J, Gomez, P, Guèye, A, Habarakada, T J, Hague, J O, Hansen, F, Hauenstein, W, Henry, D W, Higinbotham, R J, Holt, C, Hyde, T, Itabashi, M, Kaneta, A, Karki, A T, Katramatou, C E, Keppel, M, Khachatryan, V, Khachatryan, P M, King, I, Korover, L, Kurbany, T, Kutz, N, Lashley-Colthirst, W B, Li, H, Liu, N, Liyanage, E, Long, J, Mammei, P, Markowitz, R E, McClellan, F, Meddi, D, Meekins, S Mey-Tal, Beck, R, Michaels, M, Mihovilovič, A, Moyer, S, Nagao, V, Nelyubin, D, Nguyen, M, Nycz, M, Olson, L, Ou, V, Owen, C, Palatchi, B, Pandey, A, Papadopoulou, S, Park, S, Paul, T, Petkovic, R, Pomatsalyuk, S, Premathilake, V, Punjabi, R D, Ransome, P E, Reimer, J, Reinhold, S, Riordan, J, Roche, V M, Rodriguez, A, Schmidt, B, Schmookler, E P, Segarra, A, Shahinyan, K, Slifer, P, Solvignon, S, Širca, T, Su, R, Suleiman, H, Szumila-Vance, L, Tang, Y, Tian, W, Tireman, F, Tortorici, Y, Toyama, K, Uehara, G M, Urciuoli, D, Votaw, J, Williamson, B, Wojtsekhowski, S, Wood, J, Zhang, and X, Zheng

Abstract

When protons and neutrons (nucleons) are bound into atomic nuclei, they are close enough to feel significant attraction, or repulsion, from the strong, short-distance part of the nucleon-nucleon interaction. These strong interactions lead to hard collisions between nucleons, generating pairs of highly energetic nucleons referred to as short-range correlations (SRCs). SRCs are an important but relatively poorly understood part of nuclear structure

Published
2021

25. Searching for New Physics with DarkLight at the ARIEL Electron-Linac

Author

E Cline, R Corliss, J C Bernauer, R Alarcon, R Baartman, S Benson, J Bessuille, D Ciarniello, A Christopher, A Colon, W Deconinck, K Dehmelt, A Deshpande, J Dilling, D H Dongwi, P Fisher, T Gautam, M Gericke, D Hasell, M Hasinoff, E Ihloff, R Johnston, R Kanungo, J Kelsey, O Kester, M Kohl, I Korover, R Laxdal, S Lee, X Li, C Ma, A Mahon, J W Martin, R Milner, M Moore, P Moran, J Nazeer, K Pachal, T Patel, T Planche, M Rathnayake, M Suresh, C Vidal, Y Wang, and S Yen

Subjects
History, Computer Science Applications, Education
Abstract

The search for a dark photon holds considerable interest in the physics community. Such a force carrier would begin to illuminate the dark sector. Many experiments have searched for such a particle, but so far it has proven elusive. In recent years the concept of a low mass dark photon has gained popularity in the physics community. Of particular recent interest is the 8Be and 4He anomaly, which could be explained by a new fifth force carrier with a mass of 17 MeV/c 2. The proposed Darklight experiment would search for this potential low mass force carrier at ARIEL in the 10-20 MeV/c 2 e+e− invariant mass range. This proceeding will focus on the experimental design and physics case of the Darklight experiment.

Published
2022

26. The influence of Fermi motion on the comparison of the polarization transfer to a proton in elastic e→p and quasi-elastic e→A scattering

Author

T. Brecelj, F. Schulz, U. Müller, A. Tyukin, Michaela Thiel, Concettina Sfienti, Anselm Esser, D. G. Middleton, J. Beričič, Guy Ron, Hartmuth Arenhövel, Ronald Gilman, J. Pochodzalla, Harald Merkel, M. Olivenboim, S. Strauch, B. S. Schlimme, M. Mihovilovič, R. Böhm, D. Izraeli, Israel Mardor, S. Širca, S. Štajner, Ivica Friščić, A. Weber, L. Debenjak, J. Lichtenstadt, I. Yaron, E. Piasetzky, M. Schoth, Patrick Achenbach, M. O. Distler, I. Korover, Adi Ashkenazi, S.J. Paul, D. Bosnar, T. Kolar, and Eliahu Cohen

Subjects
Physics, Elastic scattering, Nuclear and High Energy Physics, 010308 nuclear & particles physics, Scattering, Initial momentum, Nuclear Theory, Kinematics, Polarization (waves), 01 natural sciences, 7. Clean energy, Transverse plane, 0103 physical sciences, Physics::Accelerator Physics, Atomic physics, Nuclear Experiment, 010306 general physics, Microtron, Fermi Gamma-ray Space Telescope
Abstract

A comparison between polarization-transfer to a bound proton in quasi-free kinematics by the A ( e → , e ′ p → ) knockout reaction and that in elastic scattering off a free proton can provide information on the characteristics of the bound proton. In the past the reported measurements have been compared to those of a free proton with zero initial momentum. We introduce, for the first time, expressions for the polarization-transfer components when the proton is initially in motion and compare them to the 2H data measured at the Mainz Microtron (MAMI). We show the ratios of the transverse ( P x ) and longitudinal ( P z ) components of the polarization transfer in H 2 ( e → , e ′ p → ) n , to those of elastic scattering off a “moving proton”, assuming the proton's initial (Fermi-motion) momentum equals the negative missing momentum in the measured reaction. We found that the correction due to the proton motion is up to 20% at high missing momentum. However the effect on the double ratio ( P x / P z ) A ( P x / P z ) H 1 is largely canceled out, as shown for both 2H and 12C data. This implies that the difference between the resting- and the moving-proton kinematics is not the primary cause for the deviations between quasi-elastic and elastic scattering reported previously.

Published
2019

27. Energy and momentum dependence of nuclear short-range correlations - Spectral function, exclusive scattering experiments and the contact formalism

Author

Or Hen, Nir Barnea, Ronen Weiss, I. Korover, and E. Piasetzky

Subjects
Physics, Nuclear and High Energy Physics, Nuclear Theory, Proton, 010308 nuclear & particles physics, Scattering, FOS: Physical sciences, Experimental data, Energy–momentum relation, Kinematics, Computer Science::Digital Libraries, 01 natural sciences, lcsh:QC1-999, Nuclear Theory (nucl-th), Maxima and minima, 0103 physical sciences, Nuclear Experiment (nucl-ex), Atomic physics, Nuclear Experiment, 010306 general physics, Wave function, Electron scattering, lcsh:Physics
Abstract

Results of electron-induced one- and two-nucleon hard knockout reactions, A(e,e′p) and A(e,e′pN), in kinematics sensitive to nuclear short-range correlations, are studied using the nuclear contact formalism. A relation between the spectral function and the nuclear contacts is derived and used to analyze the dependence of the data on the initial energy and momentum of the knocked-out proton. The ratio between the number of emitted proton-proton pairs and proton-neutron pairs is shown to depend predominantly on a single ratio of contacts. This ratio is expected to present deep minima in the initial energy and momentum plane, associated with the node in the proton-proton wave function.The formalism is applied to analyze data from recent $^{4}$He and $^{12}$C electron-scattering experiments performed at Jefferson laboratory. Different nucleon-nucleon potentials were used to assess the model-dependence of the results. For the ratio of proton-proton to proton-neutron pairs in $^{4}$He, a fair agreement with the experimental data is obtained using the two potentials, whereas for the ratio of proton-proton pairs to the total knocked-out protons in $^{12}$C, some of the features of the theory are not seen in the experimental data. Several possible explanations for this disagreement are discussed. It is also observed that the spectral function at specific domains of the momentum-energy plane is sensitive to the nucleon-nucleon interaction. Based on this sensitivity, it might be possible to constrain the short range part of the nuclear potential using such experimental data.

Published
2019

28. Unperturbed inverse kinematics nucleon knockout measurements with a carbon beam

Author

S. Morozov, T. Atovullaev, O. Gavrischuk, I. Rufanov, D. M. Rossi, I. Slepnev, V. Tcholakov, V. Zhezher, Yu. Potrebenikov, E.P. Segarra, A. Timoshenko, A. Taranenko, A. Corsi, A. Shutov, D. Blaschke, A. Terletsky, G. Musulmanbekov, A. Kuznetsov, A. Vishnevsky, Herbert A. Simon, V. Vasendina, E. Piasetzky, V. Lenivenko, R. Kattabekov, D. Sakulin, A. Dmitriev, S. Lobastov, P. Dulov, Yu. Ivanova, O. Warmusz, N. Topilin, V. Rogov, M. Duer, P. Senger, V. Spaskov, D. Suvarieva, A. Morozov, Alexander Schmidt, N. Lashmanov, Kh. U. Abraamyan, I. Slepov, K. Gertsenberger, N. Zamiatin, D. Baranov, M. Strikhanov, V. Yurevich, K. Boretzky, V. Babkin, V. Samsonov, G. Agakishiev, N. Karpushkin, D. Bogoslovsky, V. Kekelidze, D. Peresunko, Y.-G. Ma, I. Filippov, A. Ciszewski, A. Ivashkin, D. Egorov, B. Topko, A. Zinchenko, M. Patsyuk, V. Shumikhin, V. Plotnikov, O. Petukhov, S. Bazylev, V. Shutov, Carlos A. Bertulani, M. Buryakov, A. Fediunin, V. Tikhomirov, E. Litvinenko, A. Makankin, I. Korover, D. Blau, S. Khabarov, Yu. Kiryushin, S. Piyadin, A. Stavinskiy, V. Kolesnikov, D. Finogeev, A. Kovalenko, M. Golubeva, M. Kapishin, A. Chebotov, D. Nikitin, A. Dryablov, J. Tanaka, Oleg B. Tarasov, Igor Gašparić, S. Kakurin, Or Hen, J. Kahlbow, F. Guber, Yu. Kopylov, O. Teryaev, V. Wagner, I. Selyuzhenkov, A. Malakhov, O. Streltsova, A. Kolozhvari, V. Burtsev, P. Alekseev, M. Rumyantsev, H. Törnqvist, E. Zherebtsova, S. Sedykh, P. Rukoyatkin, I. Gabdrakhmanov, A. Bolozdynya, A. Kugler, M. Shitenkov, N. Barbashina, N. Zhigareva, A. Izvestnyy, Yu. Kovalev, S. Kuklin, K. Roslon, N. Tarasov, O. Rogachevsky, A. Galavanov, S. Merts, Thomas Aumann, B. Dabrowska, V. Palchik, L. Kovachev, E. Atkin, R. Nagdasev, A. Maksymchyuk, V. Golovatyuk, N. Sukhov, J. Chen, G. Laskaris, E. Zubarev, V. Slepnev, T. Aushev, A. Sorin, B. Löher, S. Sergeev, V. Panin, V. Karjavin, A. Sheremeteva, E. Kulish, V. Sosnovtsev, G. Pokatashkin, G. Johansson, S. Buzin, K. Filippov, E. Streletskaya, M. Peryt, I. Mardor, Yu.P. Petukhov, V. Tarasov, H. Scheit, M. Zuev, P. Batyuk, V. Balandin, A. Shchipunov, I. Yaron, E. Ladygin, Song Zhang, D. Dabrowski, R. Cruz-Torres, A. Beck, T. Starecki, N. Voytishin, I. Tyapkin, A. Kisiel, and S. Afanasiev

Subjects
Physics, Hydrogen, Isotope, Scattering, Nuclear Theory, General Physics and Astronomy, chemistry.chemical_element, nuclear structure, experiments with inverse kinematics, quasi-free scattering, short-range correlations, 01 natural sciences, 010305 fluids & plasmas, Ion, Nuclear physics, chemistry, 0103 physical sciences, Particle, Facility for Antiproton and Ion Research, 010306 general physics, Nucleon, Wave function, Nuclear Experiment
Abstract

Particle knockout scattering experiments1,2 are fundamental for mapping the structure of atomic nuclei2–6, but their interpretation is often complicated by initial- and final-state interactions of the incoming and scattered particles1,2,7–9. Such interactions lead to reduction in the scattered particle flux and distort their kinematics. Here we overcome this limitation by measuring the quasi-free scattering of 48 GeV c–1 12C ions from hydrogen. The distribution of single protons is studied by detecting two protons at large angles in coincidence with an intact 11B nucleus. The 11B detection suppresses the otherwise large distortions of reconstructed single-proton distributions induced by initial- and final-state interactions. By further detecting residual 10B and 10Be nuclei, we also identified short-range correlated nucleon–nucleon pairs9–13 and provide direct experimental evidence for separation of the pair wavefunction from that of the residual many-body nuclear system9,14. All measured reactions are well described by theoretical calculations that include no distortions from the initial- and final-state interactions. Our results showcase the ability to study the short-distance structure of short-lived radioactive nuclei at the forthcoming Facility for Antiproton and Ion Research (FAIR)15 and Facility for Rare Isotope Beams (FRIB)16 facilities, which is relevant for understanding the structure and properties of nuclei far from stability and the formation of visible matter in the Universe. Initial- and final-state interactions distort the kinematics in particle knockout scattering experiments, complicating their interpretation. These effects are suppressed by detecting 11B nuclei in quasi-free scattering of 12C ions from hydrogen.

Published
2021

29. Generalized contact formalism analysis of the 4He(e,e′pN) reaction

Author

Mark Strikman, Douglas Higinbotham, Nir Barnea, E. Piasetzky, Axel Schmidt, I. Korover, Or Hen, Ronen Weiss, J.R. Pybus, and Larry Weinstein

Subjects
Physics, Nuclear and High Energy Physics, Missing energy, Nuclear Theory, 010308 nuclear & particles physics, FOS: Physical sciences, Kinematics, 01 natural sciences, lcsh:QC1-999, Nuclear Theory (nucl-th), Formalism (philosophy of mathematics), Recoil, 0103 physical sciences, Neutron, Nuclear Experiment (nucl-ex), 010306 general physics, Nuclear theory, Nuclear Experiment, lcsh:Physics, Mathematical physics
Abstract

Measurements of short-range correlations in exclusive $^4$He$(e,e'pN)$ reactions are analyzed using the Generalized Contact Formalism (GCF). We consider both instant-form and light-cone formulations with both the AV18 and local N2LO(1.0) nucleon-nucleon ($NN$) potentials. We find that kinematic distributions, such as the reconstructed pair opening angle, recoil neutron momentum distribution, and pair center of mass motion, as well as the measured missing energy, missing mass distributions, are all well reproduced by GCF calculations. The missing momentum dependence of the measured $^4$He$(e,e'pN)$ / $^4$He$(e,e'p)$ cross-section ratios, sensitive to nature of the $NN$ interaction at short-distacnes, are also well reproduced by GCF calculations using either interaction and formulation. This gives credence to the GCF scale-separated factorized description of the short-distance many-body nuclear wave-function., Comment: Accepted for publication in Physics Letters B. 8 pages, 4 figures and online supplementary materials

Published
2020

30. Probing Few-Body Nuclear Dynamics via H3 and He3 (e,e′p)pn Cross-Section Measurements

Author

M. Mihovilovic, Bogdan Wojtsekhowski, Darko Androić, D. Blyth, R. I. Pomatsalyuk, R. Obrecht, Andrew Puckett, Toshiyuki Gogami, Shalev Gilad, H. F. Ibrahim, B. Karki, Dipangkar Dutta, J. Castellanos, N. Santiesteban, Afroditi Papadopoulou, Pete Markowitz, M. Duer, Misak Sargsian, J. Arrington, M. Khachatryan, K. A. Aniol, S. Alsalmi, Nikolaos Sparveris, W. Tireman, Henryk Witała, Z. E. Meziani, J. P. Chen, Siyu Jian, T. Gautam, A. Karki, P. E. Reimer, H. Bhatt, I. Korover, R. Cruz-Torres, Nilanga Liyanage, C. Ayerbe Gayoso, V. Bellini, M. N. H. Rashad, G. M. Urciuoli, S. Covrig, Elliot Hughes, Z. Ye, S. Mey-Tal Beck, B. Schmookler, L. Ou, Weidong Li, J. Gomez, Simon Širca, B. Pandey, H. Albataineh, S. Barcus, S. Premathilake, E. Piasetzky, Ronald Ransome, D. Nguyen, Or Hen, Vladimir Nelyubin, Shanfeng Li, A. Beck, A. Camsonne, E. Fuchey, A. S. Tadepalli, Jacek Golak, P. M. King, T. Averett, D. G. Meekins, A. T. Katramatou, A. Shahinyan, Alexander Schmidt, N. Nuruzzaman, C. E. Hyde, R. E. McClellan, T. Kutz, Larry Weinstein, F. Hauenstein, Sylvester Joosten, S. A. Wood, G. Laskaris, W. U. Boeglin, D. Bulumulla, D. Biswas, F. Tortorici, Olfred Hansen, J. Roche, G. G. Petratos, L. Tang, Fatiha Benmokhtar, H. Atac, R. Skibiński, Kondo Gnanvo, Aditya R. Khanal, M. Nycz, D. Abrams, Cynthia Keppel, X. Bai, S. Park, H. Szumila-Vance, B. Duran, E.P. Segarra, S. Riordan, V. Khachatryan, V. A. Punjabi, C. Gu, Vishvas Pandey, T. Hague, D. King, M. Hattawy, D. Bhetuwal, Eliahu Cohen, R. Michaels, Hongjun Liu, M. Olson, M. Patsyuk, Kacper Topolnicki, B. Sawatzky, N. Lashley-Colthirst, Jiawen Zhang, Whitney Armstrong, S. Paul, T. Su, B. Dongwi, Hiroyuki Kamada, Douglas Higinbotham, V. Owen, J. Bane, C. Gal, A. Habarakada, Riad Suleiman, and K. Craycraft

Subjects
Physics, Scattering, Isoscalar, Nuclear Theory, Momentum transfer, General Physics and Astronomy, Few-body systems, 01 natural sciences, Nuclear physics, Cover (topology), 0103 physical sciences, Nuclear force, Nuclear Experiment, 010306 general physics, Ground state, Nucleon
Abstract

We report the first measurement of the (e,e^{'}p) three-body breakup reaction cross sections in helium-3 (^{3}He) and tritium (^{3}H) at large momentum transfer [⟨Q^{2}⟩≈1.9 (GeV/c)^{2}] and x_{B}>1 kinematics, where the cross section should be sensitive to quasielastic (QE) scattering from single nucleons. The data cover missing momenta 40≤p_{miss}≤500 MeV/c that, in the QE limit with no rescattering, equals the initial momentum of the probed nucleon. The measured cross sections are compared with state-of-the-art ab initio calculations. Overall good agreement, within ±20%, is observed between data and calculations for the full p_{miss} range for ^{3}H and for 100≤p_{miss}≤350 MeV/c for ^{3}He. Including the effects of rescattering of the outgoing nucleon improves agreement with the data at p_{miss}>250 MeV/c and suggests contributions from charge-exchange (SCX) rescattering. The isoscalar sum of ^{3}He plus ^{3}H, which is largely insensitive to SCX, is described by calculations to within the accuracy of the data over the entire p_{miss} range. This validates current models of the ground state of the three-nucleon system up to very high initial nucleon momenta of 500 MeV/c.

Published
2020

31. Laser Calibration System for Time of Flight Scintillator Arrays

Author

A. Hrnjic, S. May-Tal Beck, A. Denniston, E. Piasetzky, Or Hen, J.R. Pybus, M. Olivenboim, T. Kutz, A. Beck, R. Cruz-Torres, I. Korover, Larry Weinstein, F. Hauenstein, A. Nambrath, P. Toledo, E.P. Segarra, and Alexander Schmidt

Subjects
Physics, Nuclear and High Energy Physics, Physics - Instrumentation and Detectors, 010308 nuclear & particles physics, business.industry, Physics::Instrumentation and Detectors, Detector, FOS: Physical sciences, Instrumentation and Detectors (physics.ins-det), Scintillator, Laser, 01 natural sciences, law.invention, Time of flight, Optics, law, 0103 physical sciences, Calibration, Neutron detection, Nuclear Experiment (nucl-ex), 010306 general physics, business, Nuclear Experiment, Instrumentation
Abstract

A laser calibration system was developed for monitoring and calibrating time of flight (TOF) scintillating detector arrays. The system includes setups for both small- and large-scale scintillator arrays. Following test-bench characterization, the laser system was recently commissioned in experimental Hall B at the Thomas Jefferson National Accelerator Facility for use on the new Backward Angle Neutron Detector (BAND) scintillator array. The system successfully provided time walk corrections, absolute time calibration, and TOF drift correction for the scintillators in BAND. This showcases the general applicability of the system for use on high-precision TOF detectors., 11 pages, 11 figures

Published
2020

32. Polarization transfer to bound protons measured by quasi-elastic electron scattering on $^{12}$C

Author

S. Strauch, T. Kolar, Eli Piasetzky, Concettina Sfienti, T. Brecelj, J. Lichtenstadt, I. Yaron, S.J. Paul, Simon Širca, Adi Ashkenazi, Carlotta Giusti, M. Mihovilovic, S. Štajner, M. Schoth, Anselm Esser, I. Korover, B. S. Schlimme, F. Schulz, Guy Ron, Michaela Thiel, P. Achenbach, D. Izraeli, M. O. Distler, E.O. Cohen, U. Müller, R. Böhm, Israel Mardor, Ronald Gilman, Harald Merkel, Adrian Weber, and M. Olivenboim

Subjects
Physics, Proton, 010308 nuclear & particles physics, Nuclear Theory, FOS: Physical sciences, Polarization (waves), 01 natural sciences, Transverse plane, 0103 physical sciences, Atomic physics, Nuclear Experiment (nucl-ex), 010306 general physics, Nuclear Experiment, Electron scattering
Abstract

We report the measurements of the transverse ($P'x$) and longitudinal ($P'z$) components of the polarization transfer to a bound proton in carbon via the quasi-free $^{12}{\rm C}(\vec e,e'\vec p)$ reaction, over a wide range of missing momenta. We determine these polarization-transfers separately for protons knocked out from the $s$- and $p$-shells. The electron-beam polarization was measured to determine the individual components with systematic uncertainties which allow a detailed comparison with theoretical calculations.

Published
2020

33. The CLAS12 Backward Angle Neutron Detector (BAND)

Author

A. I. Ostrovidov, A. Denniston, A. Nambrath, Eliahu Cohen, A. Hrnjic, P. Eugenio, I. Vega, I. Korover, Alexander Schmidt, M. Ungerer, H. Hakobyan, R. Cruz-Torres, T. Hartlove, F. Hauenstein, Larry Weinstein, J.R. Pybus, E.P. Segarra, M. Duer, Or Hen, T. Kutz, C. Fogler, A. Beck, J. Barlow, William Brooks, K. Price, E. Piasetzky, E. Barriga, S. May-Tal Beck, and Massachusetts Institute of Technology. Laboratory for Nuclear Science

Subjects
Physics, Nuclear and High Energy Physics, Physics - Instrumentation and Detectors, business.industry, Detector, FOS: Physical sciences, Cosmic ray, Instrumentation and Detectors (physics.ins-det), Scintillator, Charged particle, Momentum, Time of flight, Optics, Neutron detection, Neutron, Nuclear Experiment (nucl-ex), business, Instrumentation, Nuclear Experiment
Abstract

The Backward Angle Neutron Detector (BAND) of CLAS12 detects neutrons emitted at backward angles of $155^\circ$ to $175^\circ$, with momenta between $200$ and $600$ MeV/c. It is positioned 3 meters upstream of the target, consists of $18$ rows and $5$ layers of $7.2$ cm by $7.2$ cm scintillator bars, and read out on both ends by PMTs to measure time and energy deposition in the scintillator layers. Between the target and BAND there is a 2 cm thick lead wall followed by a 2 cm veto layer to suppress gammas and reject charged particles. This paper discusses the component-selection tests and the detector assembly. Timing calibrations (including offsets and time-walk) were performed using a novel pulsed-laser calibration system, resulting in time resolutions better than $250$ ps (150 ps) for energy depositions above 2 MeVee (5 MeVee). Cosmic rays and a variety of radioactive sources were used to calibration the energy response of the detector. Scintillator bar attenuation lengths were measured. The time resolution results in a neutron momentum reconstruction resolution, $\delta p/p < 1.5$\% for neutron momentum $200\le p\le 600$ MeV/c. Final performance of the BAND with CLAS12 is shown, including electron-neutral particle timing spectra and a discussion of the off-time neutral contamination as a function of energy deposition threshold., Comment: 17 pages, 25 figures, 3 tables. Accepted for publication in NIM-A

Published
2020
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34. Probing few-body nuclear dynamics via ^{3}H and ^{3}He (e, {e}'p)pn cross-section measurements

Author

R, Cruz-Torres, D, Nguyen, F, Hauenstein, A, Schmidt, S, Li, D, Abrams, H, Albataineh, S, Alsalmi, D, Androic, K, Aniol, W, Armstrong, J, Arrington, H, Atac, T, Averett, C, Ayerbe Gayoso, X, Bai, J, Bane, S, Barcus, A, Beck, V, Bellini, F, Benmokhtar, H, Bhatt, D, Bhetuwal, D, Biswas, D, Blyth, W, Boeglin, D, Bulumulla, A, Camsonne, J, Castellanos, J-P, Chen, E O, Cohen, S, Covrig, K, Craycraft, B, Dongwi, M, Duer, B, Duran, D, Dutta, E, Fuchey, C, Gal, T N, Gautam, S, Gilad, K, Gnanvo, T, Gogami, J, Golak, J, Gomez, C, Gu, A, Habarakada, T, Hague, O, Hansen, M, Hattawy, O, Hen, D W, Higinbotham, E, Hughes, C, Hyde, H, Ibrahim, S, Jian, S, Joosten, H, Kamada, A, Karki, B, Karki, A T, Katramatou, C, Keppel, M, Khachatryan, V, Khachatryan, A, Khanal, D, King, P, King, I, Korover, T, Kutz, N, Lashley-Colthirst, G, Laskaris, W, Li, H, Liu, N, Liyanage, P, Markowitz, R E, McClellan, D, Meekins, S, Mey-Tal Beck, Z-E, Meziani, R, Michaels, M, Mihovilovič, V, Nelyubin, N, Nuruzzaman, M, Nycz, R, Obrecht, M, Olson, L, Ou, V, Owen, B, Pandey, V, Pandey, A, Papadopoulou, S, Park, M, Patsyuk, S, Paul, G G, Petratos, E, Piasetzky, R, Pomatsalyuk, S, Premathilake, A J R, Puckett, V, Punjabi, R, Ransome, M N H, Rashad, P E, Reimer, S, Riordan, J, Roche, M, Sargsian, N, Santiesteban, B, Sawatzky, E P, Segarra, B, Schmookler, A, Shahinyan, S, Širca, R, Skibiński, N, Sparveris, T, Su, R, Suleiman, H, Szumila-Vance, A S, Tadepalli, L, Tang, W, Tireman, K, Topolnicki, F, Tortorici, G, Urciuoli, L B, Weinstein, H, Witała, B, Wojtsekhowski, S, Wood, Z H, Ye, Z Y, Ye, and J, Zhang

Abstract

We report the first measurement of the (e,e^{'}p) three-body breakup reaction cross sections in helium-3 (^{3}He) and tritium (^{3}H) at large momentum transfer [⟨Q^{2}⟩≈1.9 (GeV/c)^{2}] and x_{B}1 kinematics, where the cross section should be sensitive to quasielastic (QE) scattering from single nucleons. The data cover missing momenta 40≤p_{miss}≤500 MeV/c that, in the QE limit with no rescattering, equals the initial momentum of the probed nucleon. The measured cross sections are compared with state-of-the-art ab initio calculations. Overall good agreement, within ±20%, is observed between data and calculations for the full p_{miss} range for ^{3}H and for 100≤p_{miss}≤350 MeV/c for ^{3}He. Including the effects of rescattering of the outgoing nucleon improves agreement with the data at p_{miss}250 MeV/c and suggests contributions from charge-exchange (SCX) rescattering. The isoscalar sum of ^{3}He plus ^{3}H, which is largely insensitive to SCX, is described by calculations to within the accuracy of the data over the entire p_{miss} range. This validates current models of the ground state of the three-nucleon system up to very high initial nucleon momenta of 500 MeV/c.

Published
2020

35. Deeply virtual Compton scattering off the neutron

Author

M. Benali, C. Desnault, M. Mazouz, Z. Ahmed, H. Albataineh, K. Allada, K. A. Aniol, V. Bellini, W. Boeglin, P. Bertin, M. Brossard, A. Camsonne, M. Canan, S. Chandavar, C. Chen, J.-P. Chen, M. Defurne, C. W. de Jager, R. de Leo, A. Deur, L. El Fassi, R. Ent, D. Flay, M. Friend, E. Fuchey, S. Frullani, F. Garibaldi, D. Gaskell, A. Giusa, O. Glamazdin, S. Golge, J. Gomez, O. Hansen, D. Higinbotham, T. Holmstrom, T. Horn, J. Huang, M. Huang, G. M. Huber, C. E. Hyde, S. Iqbal, F. Itard, Ho. Kang, Hy. Kang, A. Kelleher, C. Keppel, S. Koirala, I. Korover, J. J. LeRose, R. Lindgren, E. Long, M. Magne, J. Mammei, D. J. Margaziotis, P. Markowitz, A. Martí Jiménez-Argüello, F. Meddi, D. Meekins, R. Michaels, M. Mihovilovic, N. Muangma, C. Muñoz Camacho, P. Nadel-Turonski, N. Nuruzzaman, R. Paremuzyan, R. Pomatsalyuk, A. Puckett, V. Punjabi, Y. Qiang, A. Rakhman, M. N. H. Rashad, S. Riordan, J. Roche, G. Russo, F. Sabatié, K. Saenboonruang, A. Saha, B. Sawatzky, L. Selvy, A. Shahinyan, S. Sirca, P. Solvignon, M. L. Sperduto, R. Subedi, V. Sulkosky, C. Sutera, W. A. Tobias, G. M. Urciuoli, D. Wang, B. Wojtsekhowski, H. Yao, Z. Ye, L. Zana, X. Zhan, J. Zhang, B. Zhao, Z. Zhao, X. Zheng, P. Zhu, Laboratoire de Physique de Clermont (LPC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Clermont Auvergne (UCA), Institut de Physique Nucléaire d'Orsay (IPNO), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), and Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Clermont Auvergne (UCA)-Centre National de la Recherche Scientifique (CNRS)

Subjects
quark: flavor, Astrophysics::High Energy Astrophysical Phenomena, High Energy Physics::Lattice, High Energy Physics::Phenomenology, Nuclear Theory, n: structure function, nucleon, FOS: Physical sciences, General Physics and Astronomy, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], 01 natural sciences, High Energy Physics - Experiment, 010305 fluids & plasmas, High Energy Physics - Phenomenology, High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology (hep-ph), deeply virtual Compton scattering, 0103 physical sciences, photon: scattering, High Energy Physics::Experiment, Nuclear Experiment (nucl-ex), 010306 general physics, Nuclear Experiment
Abstract

The three-dimensional structure of nucleons (protons and neutrons) is embedded in so-called generalized parton distributions, which are accessible from deeply virtual Compton scattering. In this process, a high energy electron is scattered off a nucleon by exchanging a virtual photon. Then, a highly-energetic real photon is emitted from one of the quarks inside the nucleon, which carries information on the quark's transverse position and longitudinal momentum. By measuring the cross-section of deeply virtual Compton scattering, Compton form factors related to the generalized parton distributions can be extracted. Here, we report the observation of unpolarized deeply virtual Compton scattering off a deuterium target. From the measured photon-electroproduction cross-sections, we have extracted the cross-section of a quasi-free neutron and a coherent deuteron. Due to the approximate isospin symmetry of quantum chromodynamics, we can determine the contributions from the different quark flavours to the helicity-conserved Compton form factors by combining our measurements with previous ones probing the proton's internal structure. These results advance our understanding of the description of the nucleon structure, which is important to solve the proton spin puzzle.

Published
2020

36. Novel observation of isospin structure of short-range correlations in calcium isotopes

Author

V. Bellini, A. Daniel, R. Shneor, Juliette Mammei, Simon Širca, Chunhui Chen, Shalev Gilad, F. Garibaldi, J. Leckey, K. A. Aniol, C. Hanretty, Nadia Fomin, S. K. Phillips, M. Hashemi Shabestari, Guy Ron, Z. E. Meziani, T. Averett, A. Shahinyan, S. Iqbal, Kalyan Allada, N. Muangma, R. Subedi, A. Saha, Wouter Deconinck, Ishay Pomerantz, M. Mihovilovic, I. Korover, X. Zhan, D. Anez, P. Aguilera, D. J. Margaziotis, J.-O. Hansen, Ping Zhu, Yujie Qiang, S. A. Wood, E. Cisbani, R. A. Lindgren, J. J. LeRose, P. E. Reimer, Z. Ye, B. E. Norum, V. A. Punjabi, M. Friend, Fatiha Benmokhtar, Karl Slifer, E. Fuchey, John Arrington, V. Sulkosky, Donal Day, Nikolaos Sparveris, Y. Zhang, D. Wang, S. Beck, E. Long, M. Posik, Jie Zhang, X. Bai, Xin Qian, D. Flay, A. Kelleher, M. M. Dalton, S. Riordan, J. W. Watson, D. G. Meekins, N. Kalantarians, Bogdan Wojtsekhowski, Paul Gueye, Nuruzzaman, S. Frullani, D. Nguyen, G. Jin, R. Zielinski, X. Zheng, Brian P. Anderson, R. Michaels, Shanfeng Li, Alexandre Camsonne, A. Beck, B. Zhao, C. Munoz Camacho, H. Kang, D. Gaskell, Douglas Higinbotham, M. Defurne, J. R. M. Annand, K. Pan, Abdurahim Rakhman, E. Piasetzky, M. Huang, P. Solvignon, C. Gu, I. Yaron, H. Al-Bataineh, S. Glamazdin, Larry Weinstein, Ronald Gilman, L. Selvy, Pete Markowitz, J. P. Chen, H. Baghdasaryan, K. Chirapatpimol, Z. Ahmed, X. Qiu, O. Rondon-Aramayo, Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Commissariat à l'énergie atomique et aux énergies alternatives (CEA), Laboratoire de Physique de Clermont (LPC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Clermont Auvergne (UCA), Jefferson Lab Hall A, and Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11)

Subjects
Triple coincidence, Physics, 010308 nuclear & particles physics, Nuclear Theory, FOS: Physical sciences, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], 01 natural sciences, 3. Good health, Isotopes of calcium, Isospin, 0103 physical sciences, Nuclear Experiment (nucl-ex), Nucleon-Nucleon Interaction, 010306 general physics, Nucleon, Nuclear Experiment, Few-Body Systems, Range (computer programming), Mathematical physics
Abstract

Short Range Correlations (SRCs) have been identified as being responsible for the high momentum tail of the nucleon momentum distribution, n(k). Hard, short-range interactions of nucleon pairs generate the high momentum tail and imprint a universal character on n(k) for all nuclei at large momentum. Triple coincidence experiments have shown a strong dominance of np pairs, but these measurements involve large final state interactions. This paper presents the results from Jefferson Lab experiment E08014 which measured inclusive electron scattering cross-section from Ca isotopes. By comparing the inclusive cross section from 48Ca to 40Ca in a kinematic region dominated by SRCs we provide a new way to study the isospin structure of SRCs., Comment: 7 pages, 3 figures

Published
2020
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37. Measurements of the electron-helicity asymmetry in the quasi-elastic A(e→,e′p) process

Author

Concettina Sfienti, D. Bosnar, Anselm Esser, I. Korover, Guy Ron, P. Klag, T. Kolar, M. Hoek, M. Heilig, Adi Ashkenazi, A. Tyukin, T. Brecelj, Patrick Achenbach, M. Schoth, Michaela Thiel, D. Izraeli, F. Schulz, M. Mihovilovič, R. Spreckels, S. Strauch, R. Böhm, Israel Mardor, J. Beričič, J. Müller, U. Müller, S. Kegel, A. Weber, J. Pochodzalla, D. G. Middleton, Carlotta Giusti, M. Olivenboim, Y. Stöttinger, B. S. Schlimme, E. Piasetzky, Hartmuth Arenhövel, E. Cline, S.J. Paul, M. O. Distler, S. Širca, Ivica Friščić, S. Štajner, Ronald Gilman, J. Lichtenstadt, Eliahu Cohen, I. Yaron, and Harald Merkel

Subjects
Physics, Nuclear and High Energy Physics, Missing energy, Proton, 010308 nuclear & particles physics, Scattering, Antisymmetric relation, media_common.quotation_subject, Electron, 01 natural sciences, Helicity, Asymmetry, 3. Good health, Momentum, 0103 physical sciences, Atomic physics, 010306 general physics, media_common
Abstract

We present measurements of the electron helicity asymmetry in quasi-elastic proton knockout from 2H and 12C nuclei by polarized electrons. This asymmetry depends on the fifth structure function, is antisymmetric with respect to the scattering plane, and vanishes in the absence of final-state interactions, and thus it provides a sensitive tool for their study. Our kinematics cover the full range in off-coplanarity angle ϕ p q , with a polar angle θ p q coverage up to about 8°. The missing energy resolution enabled us to determine the asymmetries for knock-out resulting in different states of the residual 11B system. We find that the helicity asymmetry for p-shell knockout from 12C depends on the final state of the residual system and is relatively large (up to ≈0.16), especially at low missing momentum. It is considerably smaller (up to ≈0.01) for s-shell knockout from both 12C and 2H. The data for 2H are in very good agreement with theoretical calculations, while the predictions for 12C exhibit differences with respect to the data.

Published
2022

38. 12C(e,e'pN) measurements of short range correlations in the tensor-to-scalar interaction transition region

Author

M. J. Amaryan, P. Lenisa, Jie Zhang, A. Beck, L. Marsicano, T. B. Hayward, U. Shrestha, Larry Weinstein, S. Strauch, Maxime Defurne, K. A. Griffioen, D. P. Watts, Friedrich Klein, R. Paremuzyan, Brian Raue, O. Pogorelko, J. Rowley, A. I. Ostrovidov, R. A. Schumacher, F. X. Girod, M. Duer, A. Denniston, E. Golovatch, R. Dupre, Nicholas M. Harrison, R. De Vita, I. I. Strakovsky, P. Eugenio, A. Deur, W. K. Brooks, A. Filippi, D. Sokhan, B. A. Clary, D. Protopopescu, Volker D. Burkert, A. S. Biselli, L. Lanza, M. Khandaker, N. Tyler, C. Djalali, E. Voutier, Michael Paolone, Y. G. Sharabian, X. Zheng, H. Atac, J. A. Tan, Y. Prok, D. S. Carman, I. Bedlinskiy, W. Phelps, V. Lucherini, M. Battaglieri, A. El Alaoui, Y. Ilieva, E. L. Isupov, Nicholas Zachariou, X. Wei, S. Mey-Tal Beck, S. Boiarinov, Hovanes Egiyan, F. Hauenstein, C. Munoz Camacho, J. W. Price, Taofeng Wang, Fatiha Benmokhtar, M. Khachatryan, Nikolaos Sparveris, N. Markov, A. Movsisyan, R. Cruz-Torres, T. A. Forest, O. Soto, D. Heddle, M. Ungaro, K. P. Adhikari, Douglas Higinbotham, Latifa Elouadrhiri, D. Marchand, P. Nadel-Turonski, S. Adhikari, B. McKinnon, M. Ripani, A. Kim, S. Stepanyan, I. Korover, M. Hattawy, M. Guidal, B. Mustapha, Z. W. Zhao, T. Mineeva, Or Hen, H. Hakobyan, M. Mirazita, J. Ritman, L. Barion, J.R. Pybus, M. Holtrop, S. Diehl, R. G. Fersch, C. Salgado, K. Joo, Luciano Pappalardo, T. Chetry, E.P. Segarra, H. S. Jo, D. G. Jenkins, M. Leali, Eugene Pasyuk, P. L. Cole, M. Ehrhart, G. Rosner, P. Chatagnon, A. D'Angelo, L. El Fassi, V. P. Kubarovsky, L. Venturelli, Krishna Neupane, C. W. Kim, H. Voskanyan, W. J. Briscoe, Dustin Keller, E. Piasetzky, D. Bulumulla, Michael Wood, K. Hafidi, Aditya R. Khanal, Andrea Bianconi, G. Niculescu, Alexander Schmidt, G. Gavalian, M. Osipenko, I. J. D. MacGregor, F. Sabatié, D. G. Ireland, V. Crede, M. Contalbrigo, Laura Clark, G. Angelini, K. Hicks, A. Celentano, R. W. Gothe, Alessandro Rizzo, V. Mascagna, S. Joosten, K. Livingston, Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), and The Clas Collaboration

Subjects
Nuclear and High Energy Physics, Nuclear Theory, dependence, CLAS, dynamics, isospin, energy, system, Astronomy & Astrophysics, Physics, QC1-999, Scalar (mathematics), FOS: Physical sciences, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], Astrophysics, 01 natural sciences, Nuclear Theory (nucl-th), Momentum, High Energy Physics - Phenomenology (hep-ph), 0103 physical sciences, ddc:530, Tensor, Nuclear Experiment (nucl-ex), Nuclear Experiment, 010306 general physics, Nuclear theory, [PHYS]Physics [physics], Range (particle radiation), 010308 nuclear & particles physics, Settore FIS/04, Nuclear interaction, High Energy Physics - Phenomenology, Astronomy &amp, Atomic physics, Nucleon
Abstract

High-momentum configurations of nucleon pairs at short-distance are probed using measurements of the $^{12}$C$(e,e'p)$ and $^{12}$C$(e,e'pN)$ reactions (where $N$ is either $n$ or $p$), at high-$Q^2$ and $x_B>1.1$. The data span a missing-momentum range of 300--1000 MeV/c and are predominantly sensitive to the transition region of the strong nuclear interaction from a Tensor to Scalar interaction. The data are well reproduced by theoretical calculations using the Generalized Contact Formalism with both chiral and phenomenological nucleon-nucleon ($NN$) interaction models. This agreement suggests that the measured high missing-momentum protons up to $1000$ MeV/c predominantly belong to short-ranged correlated (SRC) pairs. The measured $^{12}$C$(e,e'pN)$ / $^{12}$C$(e,e'p)$ and $^{12}$C$(e,e'pp)$ / $^{12}$C$(e,e'pn)$ cross-section ratios are consistent with a decrease in the fraction of proton-neutron SRC pairs and increase in the fraction of proton-proton SRC pairs with increasing missing momentum. This confirms the transition from an isospin-dependent tensor $NN$ interaction at $\sim 400$ MeV/c to an isospin-independent scalar interaction at high-momentum around $\sim 800$ MeV/c as predicted by theoretical calculation., Accepted for publication in Physics Letters B. 7 pages, 3 figures, and online supplementary materials

Published
2021

39. Polarization-transfer measurement to a large-virtuality bound proton in the deuteron

Author

J. Lichtenstadt, I. Yaron, Anselm Esser, Guy Ron, A. Weber, J. Pochodzalla, J. Beričič, A. Tyukin, M. Schoth, R. Böhm, F. Schulz, Hartmuth Arenhövel, E. Piasetzky, B. S. Schlimme, P. Achenbach, Damir Bosnar, L. Debenjak, M. Mihovilovic, Concettina Sfienti, U. Müller, D. G. Middleton, Ronald Gilman, Harald Merkel, S. Strauch, D. Izraeli, S. Širca, Ivica Friščić, Michaela Thiel, M. O. Distler, E.O. Cohen, and I. Korover

Subjects
Physics, Nuclear and High Energy Physics, Proton, 010308 nuclear & particles physics, Nuclear Theory, FOS: Physical sciences, Polarization (waves), 01 natural sciences, NATURAL SCIENCES. Physics, lcsh:QC1-999, Nuclear physics, PRIRODNE ZNANOSTI. Fizika, Deuterium, 0103 physical sciences, d(e, e’p), Electron-scattering, Physics::Accelerator Physics, Nuclear Experiment (nucl-ex), 010306 general physics, Nuclear Experiment, d(e,e'p), Electron scattering, Nuclear density, lcsh:Physics
Abstract

Possible differences between free and bound protons may be observed in the ratio of polarization-transfer components, $P'_x/P'_z$. We report the measurement of $P'_x/P'_z$, in the $^2\textrm{H}(\vec{e},e^{\prime}\vec{p})n$ reaction at low and high missing momenta. Observed increasing deviation of $P'_x/P'_z$ from that of a free proton as a function of the virtuality, similar to that observed in \hefour, indicates that the effect in nuclei is due to the virtuality of the knock-out proton and not due to the average nuclear density. The measured differences from calculations assuming free-proton form factors ($\sim10\%$), may indicate in-medium modifications., 4 figures

Published
2017

40. Phase diagrams of binary alloys under pressure

Author

Eyal Yahel, R. Hevroni, Guy Makov, Yaron Greenberg, I. Korover, and Moran Emuna

Subjects
010302 applied physics, Materials science, Composition dependence, Mechanical Engineering, Alloy, Binary alloy, Metals and Alloys, Thermodynamics, Binary number, 02 engineering and technology, engineering.material, Pressure dependence, 021001 nanoscience & nanotechnology, 01 natural sciences, Mechanics of Materials, 0103 physical sciences, Materials Chemistry, engineering, 0210 nano-technology, Ambient pressure, Phase diagram, Eutectic system
Abstract

The phase diagrams of binary alloys are known to vary with pressure. Within the framework of solution-type models, the variation is controlled by the pressure dependence of the elemental end members, which is relatively well known, and that of the excess interaction, which is unknown. We develop an exact thermodynamic relationship for the pressure dependence of the excess interaction in an alloy solution and relate it to the composition dependence of the density and sound velocity measured at ambient pressure. The effect of composition on the sound velocity and density was studied for the isomorphous binary alloy Bi Sb and the eutectic systems Bi Sn and Pb Sn, and the pressure dependence of the excess interaction was evaluated. On the basis of these results, the pressure dependence of these binary alloy phase diagrams was calculated and found to agree well with the experimental data in the literature.

Published
2016

41. Comparing proton momentum distributions in A = 2 and 3 nuclei via 2H 3H and 3He (e,e′p) measurements

Author

Z. Ye, B. Schmookler, J. P. Chen, G. M. Urciuoli, Diego Lonardoni, P. M. King, Hongbang Liu, R. Michaels, D. King, M. Olson, Darko Androić, S. Covrig, Toshiyuki Gogami, Pete Markowitz, S. Paul, Weidong Li, M. Viviani, Whitney Armstrong, P. E. Reimer, Larry Weinstein, T. Su, M. Patsyuk, H. Atac, B. Dongwi, Or Hen, N. Santiesteban, B. Sawatzky, T. Kutz, V. Bellini, R. I. Pomatsalyuk, H. Bhatt, I. Korover, S. A. Wood, R. Obrecht, S. Riordan, V. Pandey, E. Fuchey, Shanfeng Li, A. Beck, M. Hattawy, John Arrington, S. Mey-Tal Beck, Andrew Puckett, D. Bulumulla, Bogdan Wojtsekhowski, Aditya R. Khanal, F. Hauenstein, Simon Širca, A. Shahinyan, M. N. H. Rashad, Axel Schmidt, Cynthia Keppel, M. Khachatryan, J. Gomez, N. Lashley-Colthirst, D. Blyth, J. Castellanos, Ruprecht Machleidt, R. Suleiman, H. Albataineh, D. Bhetuwal, V. Khachatryan, Kondo Gnanvo, Eliahu Cohen, F. Tortorici, J. Roche, V. A. Punjabi, N. Nuruzzaman, S. Alsalmi, M. Nycz, H. Szumila-Vance, B. Duran, G. G. Petratos, Z. E. Meziani, C. Gal, Vladimir Nelyubin, G. Laskaris, L. Tang, W. Tireman, M. Mihovilovic, A. Karki, Ronald Ransome, D. G. Meekins, A. T. Katramatou, Olfred Hansen, W. U. Boeglin, Nilanga Liyanage, D. Biswas, C. Ayerbe Gayoso, Jiawen Zhang, S. Premathilake, D. Nguyen, X. Bai, E.P. Segarra, Siyu Jian, Elliot Hughes, R. Cruz-Torres, Douglas Higinbotham, L. Ou, S. Barcus, V. Owen, J. Bane, A. S. Tadepalli, R. E. McClellan, A. Habarakada, Sylvester Joosten, K. Craycraft, H. F. Ibrahim, B. Karki, Dipangkar Dutta, Laura Elisa Marcucci, M. Duer, T. Gautam, B. Pandey, Shalev Gilad, A. Papadopoulou, K. A. Aniol, A. Camsonne, D. Abrams, S. Park, F. Sammarruca, N. Sparveris, E. Piasetzky, C. Gu, T. Hague, T. Averett, and C. E. Hyde

Subjects
production [pi], Nuclear and High Energy Physics, data analysis method, Photon, Nuclear Theory, interference, FOS: Physical sciences, Electron, Impulse (physics), Inelastic scattering, 01 natural sciences, xperimental results | Jefferson Lab | electron p: scattering | parity: violation | inelastic scattering | structure function | interference | photon | Z0 | pi: production | spin: asymmetry | data analysis method, Nuclear Theory (nucl-th), structure function, 0103 physical sciences, Z0, Nuclear Experiment (nucl-ex), 010306 general physics, Nuclear Experiment, Physics, 010308 nuclear & particles physics, Momentum transfer, photon, inelastic scattering, scattering [electron p], Eikonal approximation, NATURAL SCIENCES. Physics, lcsh:QC1-999, PRIRODNE ZNANOSTI. Fizika, Deuterium, xperimental results, High Energy Physics::Experiment, violation [parity], Atomic physics, Nucleon, asymmetry [spin], lcsh:Physics, Jefferson Lab
Abstract

We report the first measurement of the $(e,e'p)$ reaction cross-section ratios for Helium-3 ($^3$He), Tritium ($^3$H), and Deuterium ($d$). The measurement covered a missing momentum range of $40 \le p_{miss} \le 550$ MeV$/c$, at large momentum transfer ($\langle Q^2 \rangle \approx 1.9$ (GeV$/c$)$^2$) and $x_B>1$, which minimized contributions from non quasi-elastic (QE) reaction mechanisms. The data is compared with plane-wave impulse approximation (PWIA) calculations using realistic spectral functions and momentum distributions. The measured and PWIA-calculated cross-section ratios for $^3$He$/d$ and $^3$H$/d$ extend to just above the typical nucleon Fermi-momentum ($k_F \approx 250$ MeV$/c$) and differ from each other by $\sim 20\%$, while for $^3$He/$^3$H they agree within the measurement accuracy of about 3\%. At momenta above $k_F$, the measured $^3$He/$^3$H ratios differ from the calculation by $20\% - 50\%$. Final state interaction (FSI) calculations using the generalized Eikonal Approximation indicate that FSI should change the $^3$He/$^3$H cross-section ratio for this measurement by less than 5\%. If these calculations are correct, then the differences at large missing momenta between the $^3$He/$^3$H experimental and calculated ratios could be due to the underlying $NN$ interaction, and thus could provide new constraints on the previously loosely-constrained short-distance parts of the $NN$ interaction., 8 pages, 3 figures (4 panels)

Published
2019

42. Quasi-elastic polarization-transfer measurements on the deuteron in anti-parallel kinematics

Author

I. Korover, Concettina Sfienti, B. S. Schlimme, E. Cline, E. Piasetzky, Eliahu Cohen, A. Weber, M. Heilig, Anselm Esser, M. O. Distler, J. Müller, T. Kolar, M. Schoth, Guy Ron, S. Širca, Ivica Friščić, D. Bosnar, F. Schulz, J. Lichtenstadt, U. Müller, I. Yaron, T. Brecelj, S. Strauch, S. Štajner, Michaela Thiel, R. Böhm, Israel Mardor, Ronald Gilman, J. Beričič, Adi Ashkenazi, Harald Merkel, L. Debenjak, M. Mihovilovič, S.J. Paul, S. Kegel, J. Pochodzalla, M. Olivenboim, P. Klag, Y. Kohl, D. G. Middleton, A. Tyukin, D. Izraeli, Patrick Achenbach, and Hartmuth Arenhövel

Subjects
Physics, Nuclear and High Energy Physics, 010308 nuclear & particles physics, Nuclear Theory, FOS: Physical sciences, Kinematics, Polarization (waves), 01 natural sciences, lcsh:QC1-999, NATURAL SCIENCES. Physics, PRIRODNE ZNANOSTI. Fizika, Parallel kinematics, Nuclear physics, Deuterium, 0103 physical sciences, ddc:530, Nuclear Experiment (nucl-ex), 010306 general physics, Nucleon, Nuclear Experiment, GeneralLiterature_REFERENCE(e.g.,dictionaries,encyclopedias,glossaries), Microtron, lcsh:Physics, polarization-transfer, deuteron, anti-parallel kinematics
Abstract

We present measurements of the polarization-transfer components in the H2(e→,e′p→) reaction, covering a previously unexplored kinematic region with large positive (anti-parallel) missing momentum, pmiss, up to 220MeV/c, and Q2=0.65 (GeV/c)2. These measurements, performed at the Mainz Microtron (MAMI), were motivated by theoretical calculations which predict small final-state interaction (FSI) effects in these kinematics, making them favorable for searching for medium modifications of bound nucleons in nuclei. We find in this kinematic region that the measured polarization-transfer components Px and Pz and their ratio agree with the theoretical calculations, which use free-proton form factors. Using this, we establish upper limits on possible medium effects that modify the bound proton's form factor ratio GE/GM at the level of a few percent. We also compare the measured polarization-transfer components and their ratio for $^{2}$H to those of a free (moving) proton. We find that the universal behavior of $^{2}$H, $^{4}$He and $^{12}$C in the double ratio (Px/Pz)A(Px/Pz)H1 is maintained in the positive missing-momentum region.

Published
2019

43. Direct Observation of Proton-Neutron Short-Range Correlation Dominance in Heavy Nuclei

Author

W. Phelps, T. B. Hayward, Or Hen, Rong Wang, Friedrich Klein, P. Eugenio, M. Taiuti, M. L. Kabir, Andrea Celentano, X. Wei, J.R. Pybus, L. Guo, A. Beck, S. Niccolai, Laura Clark, A. I. Ostrovidov, G. Rosner, M. Contalbrigo, A. Denniston, D. G. Ireland, C. Hanretty, A. Hrnjic, G. Niculescu, K. A. Griffioen, G. Ciullo, G. Angelini, P. Rossi, D. S. Carman, Volker D. Burkert, A. S. Biselli, R. Cruz Torres, K. Livingston, A. Rizzo, M. Duer, Michael Paolone, N. Markov, H. S. Jo, Iu. Skorodumina, A. Movsisyan, S. Diehl, Y. Prok, E. L. Isupov, B. McKinnon, N. Tyler, M. Osipenko, R. W. Gothe, M. Khandaker, Michael Wood, J. A. Tan, V. Crede, Y. Ilieva, K. Joo, E. De Sanctis, F. Cao, B. Duran, I. Korover, R. A. Montgomery, K. Hicks, D. Heddle, I. Bedlinskiy, S. Stepanyan, H. Voskanyan, F. Hauenstein, R. A. Schumacher, M. Battaglieri, Chaden Djalali, F. X. Girod, B. Mustapha, E. Pasyuk, N. Dashyan, H. Hakobyan, A. D'Angelo, F. Sabatié, M. Holtrop, M. Mirazita, I. J. D. MacGregor, Eliahu Cohen, K. Park, A. El Alaoui, P. Nadel-Turonski, H. Egiyan, T. A. Forest, W. Kim, B. S. Ishkhanov, David M. Keller, E.P. Segarra, L. El Fassi, Aditya R. Khanal, Nicholas Zachariou, S. E. Kuhn, Eli Piasetzky, M. Ripani, S. Strauch, V. P. Kubarovsky, Taya Chetry, M. Hattawy, Nir Barnea, Axel Schmidt, J. Zhang, D. Protopopescu, P. L. Cole, Z. W. Zhao, E. Voutier, Y. G. Sharabian, A. Deur, W. K. Brooks, S. Adhikari, E. Golovatch, R. Dupre, Ronen Weiss, K. Hafidi, L. Lanza, M. Khachatryan, C. Munoz Camacho, Nikolaos Sparveris, M. Patsyuk, R. Paremuzyan, Nicholas M. Harrison, Gerard Gilfoyle, D. Sokhan, A. Filippi, K. L. Giovanetti, Larry Weinstein, X. Zheng, R. De Vita, S. Mey-Tal Beck, B. Schmookler, D. Marchand, M. Ungaro, G. Laskaris, S. Boiarinov, O. Pogorelko, O. Cortes, Victor Mokeev, P. Lenisa, Institut de Physique Nucléaire d'Orsay (IPNO), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, CLAS, and Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)

Subjects
Triple coincidence, Nuclear Theory, [PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th], General Physics and Astronomy, Socio-culturale, FOS: Physical sciences, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], 01 natural sciences, Nuclear matter in neutron stars, Correlation, Nuclear Theory (nucl-th), 0103 physical sciences, Neutron, Nuclear Experiment (nucl-ex), 010306 general physics, Nuclear Experiment, Nuclear theory, Asymmetric nuclear matter,Lepton induced nuclear reactions, Nuclear matter in neutron stars, Nucleon distribution, Nucleon-nucleon interactions, Nuclear Physics, Physics, Settore FIS/04, Direct observation, Formalism (philosophy of mathematics), Lepton induced nuclear reactions, Nucleon-nucleon interactions, Nucleon distribution, Atomic physics, Nucleon, Asymmetric nuclear matter
Abstract

We measured the triple coincidence A(e,e'np) and A(e,e'pp) reactions on carbon, aluminum, iron, and lead targets at Q2 > 1.5 (GeV/c)2, xB > 1.1 and missing momentum > 400 MeV/c. This was the first direct measurement of both proton-proton (pp) and neutron-proton (np) short-range correlated (SRC) pair knockout from heavy asymmetric nuclei. For all measured nuclei, the average proton-proton (pp) to neutron-proton (np) reduced cross-section ratio is about 6%, in agreement with previous indirect measurements. Correcting for Single-Charge Exchange effects decreased the SRC pairs ratio to ~ 3%, which is lower than previous results. Comparisons to theoretical Generalized Contact Formalism (GCF) cross-section calculations show good agreement using both phenomenological and chiral nucleon-nucleon potentials, favoring a lower pp to np pair ratio. The ability of the GCF calculation to describe the experimental data using either phenomenological or chiral potentials suggests possible reduction of scale- and scheme-dependence in cross section ratios. Our results also support the high-resolution description of high-momentum states being predominantly due to nucleons in SRC pairs., Accepted for publication in PRL. 9 pages, 3 figures, 3 tables and supplementary materials

Published
2019

44. Measurements of the induced polarization in the quasi-elastic A(e,e′p→) process in non-coplanar kinematics

Author

Concettina Sfienti, M. Heilig, S. Strauch, M. Hoek, T. Brecelj, Ronald Gilman, T. Kolar, J. Müller, Harald Merkel, S. Širca, Patrick Achenbach, Ivica Friščić, U. Müller, D. Izraeli, S. Kegel, J. Pochodzalla, R. Spreckels, Anselm Esser, Michaela Thiel, L. Debenjak, J. Beričič, D. G. Middleton, J. Lichtenstadt, Guy Ron, D. Bosnar, Adi Ashkenazi, I. Yaron, M. Olivenboim, S. Štajner, M. Schoth, I. Korover, A. Weber, Hartmuth Arenhövel, Carlotta Giusti, B. S. Schlimme, E. Cline, F. Schulz, M. O. Distler, M. Mihovilovič, Eliahu Cohen, E. Piasetzky, R. Böhm, Israel Mardor, S.J. Paul, P. Klag, Y. Kohl, and A. Tyukin

Subjects
Physics, Nuclear and High Energy Physics, 010308 nuclear & particles physics, Plane (geometry), Scattering, Shell (structure), 7. Clean energy, 01 natural sciences, Induced polarization, p-process, Momentum, Transverse plane, Deuterium, 0103 physical sciences, Atomic physics, 010306 general physics
Abstract

We report measurements of the induced polarization P → of protons knocked out from 2H and 12C via the A ( e , e ′ p → ) reaction. We have studied the dependence of P → on two kinematic variables: the missing momentum p miss and the “off-coplanarity” angle ϕ p q between the scattering and reaction planes. For the full 360° range in ϕ p q , both the normal ( P y ) and, for the first time, the transverse ( P x ) components of the induced polarization were measured with respect to the coordinate system associated with the scattering plane. P x vanishes in coplanar kinematics, however in non-coplanar kinematics, it is on the same scale as P y . We find that the dependence on ϕ p q is sine-like for P x and cosine-like for P y . For carbon, the magnitude of the induced polarization is especially large when protons are knocked out from the p 3 / 2 shell at very small p miss . For the deuteron, the induced polarization is near zero at small | p miss | , and its magnitude increases with | p miss | . For both nuclei such behavior is reproduced qualitatively by theoretical results, driven largely by the spin-orbit part of the final-state interactions. However, for both nuclei, sizeable discrepancies exist between experiment and theory.

Published
2020

45. Comparison of recoil polarization in the C12(e→,e′p→) process for protons extracted from s and p shells

Author

M. Olivenboim, T. Kolar, R. Böhm, Israel Mardor, Michaela Thiel, M. Mihovilovič, J. Müller, M. Hoek, M. O. Distler, Concettina Sfienti, U. Müller, D. Bosnar, J. Lichtenstadt, I. Yaron, I. Korover, S. Širca, E. Piasetzky, Eliahu Cohen, Patrick Achenbach, Carlotta Giusti, B. S. Schlimme, S. Strauch, E. Cline, R. Spreckels, Y. Kohl, Anselm Esser, Guy Ron, A. Weber, T. Brecelj, D. Izraeli, S.J. Paul, Ronald Gilman, Harald Merkel, S. Štajner, S. Kegel, and J. Pochodzalla

Subjects
Physics, Nuclear and High Energy Physics, Proton, 010308 nuclear & particles physics, Initial momentum, Nuclear Theory, Impulse (physics), Polarization (waves), 01 natural sciences, p-process, Recoil, 0103 physical sciences, Atomic physics, Nuclear Experiment, 010306 general physics
Abstract

We present the first measurements of the double ratio of the polarization-transfer components ( P x ′ / P z ′ ) p / ( P x ′ / P z ′ ) s for knock-out protons from the s and p shells in C 12 measured by the C 12 ( e → , e ′ p → ) reaction in quasi-elastic kinematics. The data are compared to theoretical predictions in the relativistic distorted-wave impulse approximation. Our results show that the differences between s- and p-shell protons, observed when compared at the same initial momentum (missing momentum), largely disappear when the comparison is done at the same proton virtuality. We observe no difference in medium modifications between protons from the s and p shells with the same virtuality in spite of the large differences in the respective nuclear densities.

Published
2020

46. Electroexcitation of the Δ+(1232) at low momentum transfer

Author

V. Bellini, C.M. Camacho, E. Schulte, H. Albataineh, J. W. Watson, M. Huang, M. Hashemi Shabestari, J. Sjoegren, C. Gu, Simon Širca, F. Garibaldi, I. Yaron, L. Selvy, M. Khandaker, V. A. Punjabi, T. Holmstrom, E. Fuchey, B. D. Anderson, M. Defurne, W. Tireman, D. J. Margaziotis, R. A. Lindgren, Or Hen, J. P. Chen, I. Korover, E. Piasetzky, Z. E. Meziani, A. Blomberg, H. Baghdasaryan, Olfred Hansen, K. Chirapatpimol, J. R. M. Annand, Juliette Mammei, A. Polychronopoulou, Salvatore Frullani, M. Posik, N. Muangma, X. Zhan, S. K. Phillips, John Arrington, X. Bai, J. Leckey, D. Flay, Nikos Sparveris, Ping Zhu, B. Zhao, Guy Ron, David Hamilton, W. B. Yan, A. Kelleher, X. Zheng, N. Kalantarians, R. Shneor, S. Riordan, Abdurahim Rakhman, A. Saha, Kalyan Allada, Vincent Sulkosky, Z. W. Zhao, Z. Ye, E. Long, Xin Qian, R. Subedi, D. G. Meekins, Bogdan Wojtsekhowski, B. E. Norum, J. LeRose, R. De Leo, M. Mihovilovič, A. Martí Jiménez-Argüello, E. Cisbani, S. Iqbal, M. M. Dalton, W. U. Boeglin, Chunhui Chen, H. Kang, A. Camsonne, Nuruzzaman, Michael Paolone, C. Hanretty, D. Anez, N. Fomin, Shalev Gilad, K. A. Aniol, T. Averett, Wouter Deconinck, Ishay Pomerantz, Z. Ahmed, A. J. Sarty, Fatiha Benmokhtar, D. Wang, S. Beck, Ronald Gilman, Douglas Higinbotham, K. Pan, Yiyang Zhang, A. Beck, Jie Zhang, M. Friend, P. E. Reimer, Institut de Physique Nucléaire d'Orsay (IPNO), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Ecole Centrale Paris, Laboratoire de Physique Corpusculaire - Clermont-Ferrand (LPC), Université Blaise Pascal - Clermont-Ferrand 2 (UBP)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), and Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)

Subjects
Angular momentum, Nuclear and High Energy Physics, High Energy Physics::Lattice, Nuclear Theory, Constituent quark, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], Nucleon deformation, 01 natural sciences, 7. Clean energy, Atomic, Nuclear physics, Pion, Particle and Plasma Physics, 0103 physical sciences, Coulomb, Effective field theory, Nuclear, CMR, 010306 general physics, Nuclear Experiment, Mathematical Physics, Physics, 010308 nuclear & particles physics, Momentum transfer, Pion electroproduction, Molecular, Nuclear & Particles Physics, lcsh:QC1-999, Quantum electrodynamics, Quadrupole, Nucleon, Astronomical and Space Sciences, lcsh:Physics
Abstract

International audience; We report on new p(e,e′p)π∘p(e,e′p)π∘ measurements at the Δ+(1232)Δ+(1232) resonance at the low momentum transfer region, where the mesonic cloud dynamics is predicted to be dominant and rapidly changing, offering a test bed for chiral effective field theory calculations. The new data explore the Q2Q2 dependence of the resonant quadrupole amplitudes and for the first time indicate that the Electric and the Coulomb quadrupole amplitudes converge as Q2→0Q2→0. The measurements of the Coulomb quadrupole amplitude have been extended to the lowest momentum transfer ever reached, and suggest that more than half of its magnitude is attributed to the mesonic cloud in this region. The new data disagree with predictions of constituent quark models and are in reasonable agreement with dynamical calculations that include pion cloud effects, chiral effective field theory and lattice calculations. The measurements indicate that improvement is required to the theoretical calculations and provide valuable input that will allow their refinements.

Published
2016

47. Center of Mass Motion of Short-Range Correlated Nucleon Pairs studied via the A(e,e′pp) Reaction

Author

D. Protopopescu, Z. W. Zhao, E. Voutier, M. Duer, D. Marchand, X. Wei, Dustin Keller, P. Eugenio, I. J. D. MacGregor, G. Ciullo, M. Taiuti, C. Djalali, J. A. Tan, W. Kim, Y. Prok, F. Sabatié, L. Lanza, J. P. Ball, D. S. Carman, G. Niculescu, M. L. Kabir, P. Lenisa, S. Strauch, Michael Wood, K. Hafidi, B. A. Clary, K. Livingston, D. G. Jenkins, S. Niccolai, A. Movsisyan, Jie Zhang, Michael Paolone, D. Heddle, A. Celentano, R. W. Gothe, N. Dashyan, Maxime Defurne, H. Avakian, S. E. Kuhn, Friedrich Klein, M. Contalbrigo, A. Beck, Hovanes Egiyan, C. Munoz Camacho, M. Osipenko, M. Ungaro, Eli Piasetzky, H. Voskanyan, R. Fersch, Or Hen, Z. Akbar, L. Barion, R. De Vita, P. Nadel-Turonski, V. Crede, Alessandro Rizzo, Eliahu Cohen, E. Golovatch, R. Dupre, W. J. Briscoe, E. Pasyuk, A. El Alaoui, R. A. Montgomery, R. Paremuzyan, V. Mokeev, M. Battaglieri, M. Ripani, F. Hauenstein, B. S. Ishkhanov, Nicholas M. Harrison, Nicholas Zachariou, Rong Wang, D. Sokhan, Alexander Schmidt, D. P. Watts, S. Adhikari, K. Hicks, B. McKinnon, E. De Sanctis, S. Mey-Tal Beck, A. Kim, V. P. Kubarovsky, Y. G. Sharabian, D. Riser, A. I. Ostrovidov, A. Filippi, P. Rossi, X. Zheng, M. Ehrhart, O. Pogorelko, M. Mirazita, A. Deur, D. G. Ireland, I. Bedlinskiy, M. Khachatryan, M. Khandaker, Nikolaos Sparveris, Volker D. Burkert, A. S. Biselli, M. J. Amaryan, Sandra K. Johnston, K. L. Giovanetti, Larry Weinstein, B. Schmookler, C. A. Meyer, P. Chatagnon, G. V. Fedotov, F. Cao, I. Korover, B. Mustapha, M. Holtrop, Taya Chetry, G. Charles, E. L. Isupov, S. Boiarinov, R. Cruz Torres, H. Hakobyan, S. Diehl, F. X. Girod, J. W. Price, R. A. Schumacher, S. Stepanyan, Avraham Klein, H. S. Jo, A. D'Angelo, L. El Fassi, G. Khachatryan, G. Rosner, Y. Ghandilyan, and K. A. Griffioen

Subjects
Physics, Range (particle radiation), 010308 nuclear & particles physics, Nuclear Theory, General Physics and Astronomy, 01 natural sciences, 7. Clean energy, Momentum, medicine.anatomical_structure, Quantum state, 0103 physical sciences, medicine, Nuclear force, Center of mass, Atomic physics, Nuclear Experiment, 010306 general physics, Nucleon, Nucleus, Fermi Gamma-ray Space Telescope
Abstract

Short-range correlated (SRC) nucleon pairs are a vital part of the nucleus, accounting for almost all nucleons with momentum greater than the Fermi momentum (k_{F}). A fundamental characteristic of SRC pairs is having large relative momenta as compared to k_{F}, and smaller center of mass (c.m.) which indicates a small separation distance between the nucleons in the pair. Determining the c.m. momentum distribution of SRC pairs is essential for understanding their formation process. We report here on the extraction of the c.m. motion of proton-proton (pp) SRC pairs in carbon and, for the first time in heavier and ansymetric nuclei: aluminum, iron, and lead, from measurements of the A(e,e^{'}pp) reaction. We find that the pair c.m. motion for these nuclei can be described by a three-dimensional Gaussian with a narrow width ranging from 140 to 170 MeV/c, approximately consistent with the sum of two mean-field nucleon momenta. Comparison with calculations appears to show that the SRC pairs are formed from mean-field nucleons in specific quantum states.

Published
2018

48. Modified structure of protons and neutrons in correlated pairs

Author

R. A. Schumacher, S. E. Kuhn, J. W. Price, G. Ciullo, J. P. Ball, J. Zhang, D. Protopopescu, D. S. Carman, E. Voutier, A. Rizzo, Y. G. Sharabian, M. J. Amaryan, M. Bashkanov, C. E. Hyde, L. El Fassi, T. A. Forest, B. McKinnon, B. S. Ishkhanov, Taya Chetry, Avraham Klein, E. Golovatch, K. Livingston, H. Avakian, H. S. Jo, Or Hen, R. Dupre, Chaden Djalali, L. Barion, F. Hauenstein, T. Mineeva, M. Mirazita, R. De Vita, P. Eugenio, Y. Prok, H. Voskanyan, Avi Ashkenazi, Alexander Schmidt, A. Filippi, K. A. Griffioen, A. D'Angelo, Sergey Kuleshov, P. Lenisa, S. Stepanyan, M. L. Kabir, Latifa Elouadrhiri, M. Osipenko, S. Mey Tal Beck, Larry Weinstein, Y. Ilieva, E.P. Segarra, I. Bedlinskiy, T. B. Hayward, G. V. Fedotov, F. X. Girod, Martin Wood, B. Mustapha, A. Deur, Eli Piasetzky, Friedrich Klein, I. J. D. MacGregor, X. Zheng, E. De Sanctis, I. Balossino, S. Strauch, R. G. Fersch, G. Laskaris, A. Beck, P. L. Cole, W. K. Brooks, S. Adhikari, M. Khandaker, Eliahu Cohen, M. Duer, E. L. Isupov, Mark Strikman, K. Hicks, I. Korover, K. Park, M. Guidal, E. Pasyuk, N. Dashyan, M. Khachatryan, Shalev Gilad, G. Charles, Nicholas Zachariou, X. Wei, Nikolaos Sparveris, S. Joosten, M. Ripani, M. Holtrop, L. Guo, V. P. Kubarovsky, Michael Paolone, D. Riser, L. Lanza, Z. W. Zhao, H. Egiyan, M. Taiuti, C. Munoz Camacho, S. Niccolai, S. Boiarinov, A. I. Ostrovidov, C. Hanretty, F. Sabatié, D. G. Ireland, Douglas Higinbotham, M. Patsyuk, R. Paremuzyan, M. Battaglieri, David M. Keller, Volker D. Burkert, Nicholas M. Harrison, A. S. Biselli, Gerard Gilfoyle, D. Sokhan, D. P. Watts, K. Hafidi, W. Kim, K. Joo, R. Cruz-Torres, M. Ungaro, S. Diehl, C. Salgado, Andrea Celentano, N. Markov, R. W. Gothe, S. Johnston, B. Schmookler, O. Pogorelko, Victor Mokeev, V. Crede, R. A. Montgomery, H. Hakobyan, G. Khachatryan, W. J. Briscoe, P. Rossi, G. Rosner, I. u. Skorodumina, J. A. Tan, A. Kim, G. Gavalian, Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Institut de Physique Nucléaire d'Orsay (IPNO), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), CLAS, and Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11)

Subjects
Quark, Nuclear Theory, Proton, nuclear physics: effect, nucleon: pair, EMC effect, Socio-culturale, FOS: Physical sciences, correlation: short-range, 01 natural sciences, symmetry breaking, Settore FIS/04 - Fisica Nucleare e Subnucleare, Nuclear physics, quark, Nuclear Theory (nucl-th), Experimental nuclear physics, Theoretical nuclear physics, High Energy Physics - Phenomenology (hep-ph), CLAS, 0103 physical sciences, quantum chromodynamics, Neutron, structure, Experimental nuclear physics, Nuclear Experiment (nucl-ex), 010306 general physics, Nuclear Experiment, quark gluon, Physics, Multidisciplinary, nucleon nucleon: correlation, 010308 nuclear & particles physics, precision measurement, High Energy Physics::Phenomenology, gluon, 3. Good health, Gluon, High Energy Physics - Phenomenology, Theoretical nuclear physics, [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph], Quark–gluon plasma, Atomic nucleus, Nucleon, experimental results
Abstract

The atomic nucleus is made of protons and neutrons (nucleons), that are themselves composed of quarks and gluons. Understanding how the quark-gluon structure of a nucleon bound in an atomic nucleus is modified by the surrounding nucleons is an outstanding challenge. Although evidence for such modification, known as the EMC effect, was first observed over 35 years ago, there is still no generally accepted explanation of its cause. Recent observations suggest that the EMC effect is related to close-proximity Short Range Correlated (SRC) nucleon pairs in nuclei. Here we report the first simultaneous, high-precision, measurements of the EMC effect and SRC abundances. We show that the EMC data can be explained by a universal modification of the structure of nucleons in neutron-proton (np) SRC pairs and present the first data-driven extraction of this universal modification function. This implies that, in heavier nuclei with many more neutrons than protons, each proton is more likely than each neutron to belong to an SRC pair and hence to have its quark structure distorted., Comment: Published in Nature. Total: 21 pages, 9 figures, 10 tables. Main text: 7 pages, 4 figures. Methods section: 1 page. Extended Data: 1 figure, 3 table. Supplementary Materials: 11 pages, 4 figures, 7 tables

Published
2018

49. Components of polarization-transfer to a bound proton in a deuteron measured by quasi-elastic electron scattering

Author

Concettina Sfienti, S. Širca, Damir Bosnar, Ivica Friščić, A. Tyukin, E. Piasetzky, Michaela Thiel, U. Müller, Adi Ashkenazi, J. Pochodzalla, D. Izraeli, Patrick Achenbach, A. Weber, Hartmuth Arenhövel, J. Lichtenstadt, I. Yaron, B. S. Schlimme, R. Böhm, I. Korover, D. G. Middleton, Israel Mardor, S. Štajner, Anselm Esser, Guy Ron, M. Mihovilovič, M. O. Distler, E.O. Cohen, M. Olivenboim, J. Beričič, F. Schulz, S. Strauch, Ronald Gilman, Harald Merkel, and M. Schoth

Subjects
Physics, Nuclear reaction, Nuclear and High Energy Physics, Proton, 010308 nuclear & particles physics, Scattering, Hadron, Nuclear Theory, FOS: Physical sciences, Electron, Polarization (waves), 7. Clean energy, 01 natural sciences, lcsh:QC1-999, Deuterium, 0103 physical sciences, polarization-transfer, deutron, Atomic physics, Nuclear Experiment (nucl-ex), 010306 general physics, Nucleon, Nuclear Experiment, lcsh:Physics
Abstract

We report the first measurements of the transverse (Px and Py) and longitudinal (Pz) components of the polarization transfer to a bound proton in the deuteron via the H2(e→,e′p→) reaction, over a wide range of missing momentum. A precise determination of the electron beam polarization reduces the systematic uncertainties on the individual components to a level that enables a detailed comparison to a state-of-the-art calculation of the deuteron using free-proton electromagnetic form factors. We observe very good agreement between the measured and the calculated Px/Pz ratios, but deviations of the individual components. Our results cannot be explained by medium modified electromagnetic form factors. They point to an incomplete description of the nuclear reaction mechanism in the calculation.

Published
2018

50. Search for three-nucleon short-range correlations in light nuclei

Author

L. Selvy, P. E. Reimer, M. Hashemi Shabestari, Wouter Deconinck, T. Averett, Karl Slifer, M. M. Dalton, H. Baghdasaryan, S. Riordan, Z. Ahmed, X. Qiu, S. Glamazdin, O. Rondon-Aramayo, X. Zhan, S. A. Wood, M. Posik, X. Bai, Yujie Qiang, N. Kalantarians, Zein-Eddine Meziani, E. Piasetzky, Larry Weinstein, P. Solvignon, Nuruzzaman, Z. Ye, B. E. Norum, Kalyan Allada, Nikolaos Sparveris, Ishay Pomerantz, N. Fomin, J. R. M. Annand, A. Kelleher, Shalev Gilad, J. Arrington, Abdurahim Rakhman, D. Wang, S. Beck, Ronald Gilman, K. A. Aniol, J. O. Hansen, B. Zhao, J. W. Watson, Juliette Mammei, Arijit Saha, M. Huang, E. Fuchey, Paul Gueye, Chunhui Chen, C. Gu, Douglas Higinbotham, I. Korover, Bogdan Wojtsekhowski, R. Michaels, H. Kang, Fatiha Benmokhtar, R. Shneor, A. Shahinyan, C. Munoz Camacho, M. Defurne, A. Camsonne, K. Chirapatpimol, I. Yaron, G. Jin, S. Iqbal, X. Zheng, Xin Qian, R. Subedi, D. J. Margaziotis, K. Pan, Pete Markowitz, D. G. Meekins, H. Albataineh, Vincent Sulkosky, B. D. Anderson, J. LeRose, Yiyang Zhang, A. Beck, P. Aguilera, A. Daniel, R. A. Lindgren, Donal Day, D. Gaskell, Guy Ron, D. Nguyen, D. Flay, C. Hanretty, N. Muangma, S. K. Phillips, M. Friend, M. Mihovilovic, Jie Zhang, E. Cisbani, Jian-Ping Chen, S. Frullani, J. Leckey, R. Zielinski, V. A. Punjabi, D. Anez, E. Long, Ping Zhu, V. Bellini, Simon Širca, F. Garibaldi, Institut de Physique Nucléaire d'Orsay (IPNO), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Commissariat à l'énergie atomique et aux énergies alternatives (CEA), Laboratoire de Physique de Clermont (LPC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Clermont Auvergne (UCA), Hall A, Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), and Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Clermont Auvergne [2017-2020] (UCA [2017-2020])-Centre National de la Recherche Scientifique (CNRS)

Subjects
Physics, Light nucleus, Nuclear and High Energy Physics, 010308 nuclear & particles physics, FOS: Physical sciences, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], 01 natural sciences, 3. Good health, Combinatorics, 0103 physical sciences, Nuclear Experiment (nucl-ex), 010306 general physics, Nucleon, Nuclear Experiment, Range (computer programming)
Abstract

We present new data probing short-range correlations (SRCs) in nuclei through the measurement of electron scattering off high-momentum nucleons in nuclei. The inclusive 4He/3He cross section ratio is observed to be both x and Q2 independent for 1.5 < x < 2, confirming the dominance of two- nucleon (2N) short-range correlations (SRCs). For x > 2, our data do not support a previous claim of three-nucleon (3N) correlation dominance. While contributions beyond those from stationary 2N- SRCs are observed, our data show that isolating 3N-SRCs is more complicated than for 2N-SRCs., 6 pages, 2 figures, new experimental results from JLab E08-014

Published
2018

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