191 results on '"M.N. HARAKEH"'
Search Results
2. Accurate simultaneous lead stopping power and charge-state measurements in gases and solids: Benchmark data for basic atomic theory and nuclear applications
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S. Ishikawa, H. Geissel, S. Purushothaman, H. Weick, E. Haettner, N. Iwasa, C. Scheidenberger, A.H. Sørensen, Y.K. Tanaka, T. Abel, J. Äystö, S. Bagchi, T. Dickel, V. Drozd, B. Franczak, F. Greiner, M.N. Harakeh, N. Kalantar-Nayestanaki, B. Kindler, R. Knöbel, D. Kostyleva, S. Kraft-Bermuth, N. Kuzminchuk, E. Lamour, B. Lommel, I. Mukha, Z. Patyk, S. Pietri, G. Schaumann, and J. Zhao
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Heavy ion ,Stopping power ,Mean charge state ,Bohr-Lindhard density effect ,Physics ,QC1-999 - Abstract
We have measured for the first time simultaneously both the mean charge states and stopping powers of (35–280) MeV/u 208Pb ions in gases and solids with an accuracy of 1%. The existence at lower energies and disappearance at higher of density effects in the charge-state distribution and the corresponding stopping power are directly confirmed and comparisons with widely used theories and simulations for heavy ions demonstrate strong deviations of up to 27%. However, an unprecedented prediction power of better than 3% has been achieved for the energy loss when the measured mean charge-states are implemented in the Lindhard-Sørensen theory. Our present benchmark data contribute to an improved understanding of the basic atomic collision processes and to numerous applications in nuclear physics. Extending the GANIL data [1] to higher accuracy and energies, we can now answer at which velocities the Bohr-Lindhard density effect in stopping will vanish.
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- 2023
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3. Intruder configurations in 29Ne at the transition into the island of inversion: Detailed structure study of 28Ne
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H. Wang, M. Yasuda, Y. Kondo, T. Nakamura, J.A. Tostevin, K. Ogata, T. Otsuka, A. Poves, N. Shimizu, K. Yoshida, N.L. Achouri, H. Al Falou, L. Atar, T. Aumann, H. Baba, K. Boretzky, C. Caesar, D. Calvet, H. Chae, N. Chiga, A. Corsi, H.L. Crawford, F. Delaunay, A. Delbart, Q. Deshayes, Zs. Dombrádi, C. Douma, Z. Elekes, P. Fallon, I. Gašparić, J.-M. Gheller, J. Gibelin, A. Gillibert, M.N. Harakeh, A. Hirayama, C.R. Hoffman, M. Holl, A. Horvat, Á. Horváth, J.W. Hwang, T. Isobe, J. Kahlbow, N. Kalantar-Nayestanaki, S. Kawase, S. Kim, K. Kisamori, T. Kobayashi, D. Körper, S. Koyama, I. Kuti, V. Lapoux, S. Lindberg, F.M. Marqués, S. Masuoka, J. Mayer, K. Miki, T. Murakami, M.A. Najafi, K. Nakano, N. Nakatsuka, T. Nilsson, A. Obertelli, N.A. Orr, H. Otsu, T. Ozaki, V. Panin, S. Paschalis, A. Revel, D. Rossi, A.T. Saito, T. Saito, M. Sasano, H. Sato, Y. Satou, H. Scheit, F. Schindler, P. Schrock, M. Shikata, Y. Shimizu, H. Simon, D. Sohler, O. Sorlin, L. Stuhl, S. Takeuchi, M. Tanaka, M. Thoennessen, H. Törnqvist, Y. Togano, T. Tomai, J. Tscheuschner, J. Tsubota, T. Uesaka, Z. Yang, and K. Yoneda
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In-beam γ-ray spectroscopy ,Island of inversion ,Shell evolution ,Physics ,QC1-999 - Abstract
Detailed γ-ray spectroscopy of the exotic neon isotope 28Ne has been performed for the first time using the one-neutron removal reaction from 29Ne on a liquid hydrogen target at 240 MeV/nucleon. Based on an analysis of parallel momentum distributions, a level scheme with spin-parity assignments has been constructed for 28Ne and the negative-parity states are identified for the first time. The measured partial cross sections and momentum distributions reveal a significant intruder p-wave strength providing evidence of the breakdown of the N=20 and N=28 shell gaps. Only a weak, possible f-wave strength was observed to bound final states. Large-scale shell-model calculations with different effective interactions do not reproduce the large p-wave and small f-wave strength observed experimentally, indicating an ongoing challenge for a complete theoretical description of the transition into the island of inversion along the Ne isotopic chain.
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- 2023
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4. The decay of the 21.47-MeV stretched resonance in 13C: A precise probe of the open nuclear quantum system description
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N. Cieplicka-Oryńczak, Y. Jaganathen, B. Fornal, S. Leoni, M. Płoszajczak, M. Ciemała, S. Ziliani, M. Kmiecik, A. Maj, J. Łukasik, P. Pawłowski, B. Sowicki, B. Wasilewska, M. Ziębliński, P. Bednarczyk, C. Boiano, S. Bottoni, A. Bracco, S. Brambilla, I. Burducea, F. Camera, I. Ciepał, C. Clisu, F.C.L. Crespi, K. Dhanmeher, N. Florea, E. Gamba, J. Grębosz, M.N. Harakeh, D.A. Iancu, Ł.W. Iskra, M. Krzysiek, P. Kulessa, N. Marginean, R. Marginean, I. Matea, M. Matejska-Minda, K. Mazurek, B. Million, W. Parol, M. Sferrazza, L. Stan, and B. Włoch
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13C ,Nuclear structure ,Stretched resonance states ,Gamow Shell Model ,Physics ,QC1-999 - Abstract
The decay of the 21.47-MeV stretched resonance in 13C, arising from p3/2→d5/2 nucleon excitation coupled to maximum spin, was investigated in a (p,p′) experiment at 135 MeV proton bombarding energy, performed at the Cyclotron Centre Bronowice (CCB) at IFJ PAN in Krakow. First experimental information on the proton and neutron decay branches from this state was obtained by using coincidence measurement of protons inelastically scattered on a 13C target and γ rays from daughter nuclei, namely, 12B (proton decay) and 12C (neutron decay). The main branches lead to the Jπ=2+, first-excited state at 0.953 MeV in 12B, and to the Jπ=1+, T=1 level at 15.110 MeV in 12C. The results were compared with predictions from the Gamow Shell Model (GSM), which was used to describe the stretched resonance in terms of its energy, width, electromagnetic transition strengths and decay pattern. A very good agreement was obtained between the measured and calculated properties of the 21.47-MeV stretched resonance in 13C, demonstrating the high-quality and precision of the GSM wave function calculations, which include coupling to the resonant and non-resonant particle continuum.
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- 2022
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5. Investigating the predicted breathing-mode excitation of the Hoyle state
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K.C.W. Li, F.D. Smit, P. Adsley, R. Neveling, P. Papka, E. Nikolskii, J.W. Brümmer, L.M. Donaldson, M. Freer, M.N. Harakeh, F. Nemulodi, L. Pellegri, V. Pesudo, M. Wiedeking, E.Z. Buthelezi, V. Chudoba, S.V. Förtsch, P. Jones, M. Kamil, J.P. Mira, G.G. O'Neill, E. Sideras-Haddad, B. Singh, S. Siem, G.F. Steyn, J.A. Swartz, I.T. Usman, and J.J. van Zyl
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Nuclear structure ,Nuclear astrophysics ,Cluster models ,Nuclear reactions ,Collective levels ,Direct reactions ,Physics ,QC1-999 - Abstract
Knowledge of the low-lying monopole strength in C12—the Hoyle state in particular—is crucial for our understanding of both the astrophysically important 3α reaction and of α-particle clustering. Multiple theoretical models have predicted a breathing mode of the Hoyle State at Ex≈9 MeV, corresponding to a radial in-phase oscillation of the underlying α clusters. The C12(α,α′)C12 and C14(p,t)C12 reactions were employed to populate states in 12C in order to search for this predicted breathing mode. A self-consistent, simultaneous analysis of the inclusive spectra with R-matrix lineshapes, together with angular distributions of charged-particle decay, yielded clear evidence for excess monopole strength at Ex≈9 MeV which is highly collective. Reproduction of the experimentally observed inclusive yields using a fit, with consistent population ratios for the various broad states, required an additional source of monopole strength. The interpretation of this additional monopole resonance as the breathing-mode excitation of the Hoyle state would provide evidence supporting a D3h symmetry for the Hoyle state itself. The excess monopole strength may complicate analysis of the properties of the Hoyle state, modifying the temperature dependence of the 3α rate at T9≳2 and ultimately, the predicted nucleosynthesis in explosive stars.
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- 2022
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6. The structure of low-lying 1− states in 90,94Zr from (α,α′γ) and (p,p′γ) reactions
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F.C.L. Crespi, A. Bracco, E.G. Lanza, A. Tamii, N. Blasi, F. Camera, O. Wieland, N. Aoi, D.L. Balabanski, S. Bassauer, A.S. Brown, M.P. Carpenter, J.J. Carroll, M. Ciemała, A. Czeszumska, P.J. Davies, V. Derya, L.M. Donaldson, Y.D. Fang, H. Fujita, G. Gey, H.T. Ha, M.N. Harakeh, T. Hashimoto, N. Ichige, E. Ideguchi, A. Inoue, J. Isaak, C. Iwamoto, D.G. Jenkins, T. Klaus, N. Kobayashi, T. Koike, M. Krzysiek, M.K. Raju, M. Liu, A. Maj, L. Morris, P. von Neumann Cosel, S. Noji, H.J. Ong, S.G. Pickstone, N. Pietralla, D. Savran, J.M. Schmitt, M. Spieker, G. Steinhilber, C. Sullivan, B. Wasilewska, M. Weinert, V. Werner, Y. Yamamoto, T. Yamamoto, R.G.T. Zegers, X. Zhou, S. Zhu, and A. Zilges
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Nuclear structure ,Dipole excitation around neutron threshold ,Inelastic scattering ,Physics ,QC1-999 - Abstract
The low-lying dipole strength in the 90,94Zr nuclei was investigated via (p,p′γ) at 80 MeV and (α,α′γ) at 130 MeV. The experiments, made at RCNP, used the magnetic spectrometer Grand Raiden for the scattered particles and the array CAGRA with HPGe detectors for the γ-decay. For 94Zr these are the first data for both reactions and for 90Zr these are the first data with (p,p′γ) and the first ones at high resolution for (α,α′γ). The comparison of the present results for the two nuclei with existing (γ,γ′) data shows that both nuclear probes produce an excitation pattern different than that of the electromagnetic probes.DWBA calculations were made using form factors deduced from transition densities, based on RPA calculations, characterized by a strong neutron component at the nuclear surface. A combined analysis of the two reactions was performed for the first time to investigate the isoscalar character of the 1− states in 90,94Zr. The (p,p′γ) cross section was calculated using values for the isoscalar electric dipole energy-weighted sum rule (E1 ISEWSR) obtained from the (α,α′γ) data. The isoscalar strength for 90Zr was found to exhaust 20 ± 2.5% of the EWSR in the energy range up to 12 MeV. In case of 94Zr, a strength of 9 ± 1.1% of the EWSR was found in the range up to 8.5 MeV.Although an overall general description was obtained in the studied energy intervals, not all proton cross sections were well reproduced using the isoscalar strength from (α,α′γ). This might suggest mixing of isoscalar and isovector components and that this mixing and the degree of collectivity are not the same for all the 1− states below the particle binding energy.
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- 2021
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7. Compressional-mode resonances in the molybdenum isotopes: Emergence of softness in open-shell nuclei near A = 90
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K.B. Howard, U. Garg, M. Itoh, H. Akimune, M. Fujiwara, T. Furuno, Y.K. Gupta, M.N. Harakeh, K. Inaba, Y. Ishibashi, K. Karasudani, T. Kawabata, A. Kohda, Y. Matsuda, M. Murata, S. Nakamura, J. Okamoto, S. Ota, J. Piekarewicz, A. Sakaue, M. Şenyiğit, M. Tsumura, and Y. Yang
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Collectivity ,Giant resonance ,Nuclear incompressibility ,Softness ,Equation of state ,Physics ,QC1-999 - Abstract
“Why are the tin isotopes soft?” has remained, for the past decade, an open problem in nuclear structure physics: models which reproduce the isoscalar giant monopole resonance (ISGMR) in the “doubly-closed shell” nuclei, 90Zr and 208Pb, overestimate the ISGMR energies of the open-shell tin and cadmium nuclei, by as much as 1 MeV. In an effort to shed some light onto this problem, we present results of detailed studies of the ISGMR in the molybdenum nuclei, with the goal of elucidating where–and how–the softness manifests itself between 90Zr and the cadmium and tin isotopes. The experiment was conducted using the 94,96,98,100Mo(α,α′) reaction at Eα=386 MeV. A comparison of the results with relativistic, self-consistent Random-Phase Approximation calculations indicates that the ISGMR response begins to show softness in the molybdenum isotopes beginning with A=92.
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- 2020
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8. Multi-messenger investigation of the Pygmy Dipole Resonance in 140Ce
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D. Savran, V. Derya, S. Bagchi, J. Endres, M.N. Harakeh, J. Isaak, N. Kalantar-Nayestanaki, E.G. Lanza, B. Löher, A. Najafi, S. Pascu, S.G. Pickstone, N. Pietralla, V.Yu. Ponomarev, C. Rigollet, C. Romig, M. Spieker, A. Vitturi, and A. Zilges
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Physics ,QC1-999 - Abstract
We report on the first (p,p′γ) experiments at Ep=80 MeV to investigate the Pygmy Dipole Resonance (PDR) in the semi-magic nucleus 140Ce. This experiment is the latest in a series of experiments to investigate the PDR with different complementary probes to provide a multi-messenger data set on the properties of the PDR in 140Ce. In addition, calculations within the Quasi-particle Phonon Model (QPM) have been performed. Cross sections have been calculated for proton- as well as α-scattering reactions based on the transition densities obtained from the QPM, not only at the RPA level, but including the full model space of up to 3p–3h configurations. This allows for the first time to compare the calculations to the experimental results on an absolute scale for single excitations. Agreement between QPM and experiment is observed, which proves the high accuracy of the calculated transition densities for individual PDR states. Keywords: Pygmy Dipole Resonance, E1 strength, Direct reactions, Collective levels, Quasi-particle Phonon Model
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- 2018
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9. Halo-induced large enhancement of soft dipole excitation of 11Li observed via proton inelastic scattering
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J. Tanaka, R. Kanungo, M. Alcorta, N. Aoi, H. Bidaman, C. Burbadge, G. Christian, S. Cruz, B. Davids, A. Diaz Varela, J. Even, G. Hackman, M.N. Harakeh, J. Henderson, S. Ishimoto, S. Kaur, M. Keefe, R. Krücken, K.G. Leach, J. Lighthall, E. Padilla Rodal, J.S. Randhawa, P. Ruotsalainen, A. Sanetullaev, J.K. Smith, O. Workman, and I. Tanihata
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11Li ,Neutron halo ,Soft-dipole resonance ,Proton inelastic scattering ,Isoscalar E1 ,Physics ,QC1-999 - Abstract
Proton inelastic scattering off a neutron halo nucleus, 11Li, has been studied in inverse kinematics at the IRIS facility at TRIUMF. The aim was to establish a soft dipole resonance and to obtain its dipole strength. Using a high quality 66 MeV 11Li beam, a strongly populated excited state in 11Li was observed at Ex=0.80±0.02 MeV with a width of Γ=1.15±0.06 MeV. A DWBA (distorted-wave Born approximation) analysis of the measured differential cross section with isoscalar macroscopic form factors leads us to conclude that this observed state is excited in an electric dipole (E1) transition. Under the assumption of isoscalar E1 transitions, the strength is evaluated to be extremely large amounting to 30∼296 Weisskopf units, exhausting 2.2%∼21% of the isoscalar E1 energy-weighted sum rule (EWSR) value. The large observed strength originates from the halo and is consistent with the simple di-neutron model of 11Li halo.
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- 2017
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10. Isovector excitations in 100Nb and their decays by neutron emission studied via the Mo100(t,He3+n) reaction at 115 MeV/u
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K. Miki, R.G.T. Zegers, Sam M. Austin, D. Bazin, B.A. Brown, A.C. Dombos, R.K. Grzywacz, M.N. Harakeh, E. Kwan, S.N. Liddick, S. Lipschutz, E. Litvinova, M. Madurga, M.T. Mustonen, W.J. Ong, S.V. Paulauskas, G. Perdikakis, J. Pereira, W.A. Peters, C. Robin, M. Scott, A. Spyrou, C. Sullivan, and R. Titus
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Spin–isospin excitations ,Neutron decay ,Charge-exchange reaction ,Missing mass spectroscopy ,Physics ,QC1-999 - Abstract
Spin–isospin excitations in Nb100 were studied via the Mo100(t,He3) charge-exchange reaction at 115 MeV/u with the goal to constrain theoretical models used to describe the isovector spin response of nuclei. The experiment was performed with a secondary beam of tritons, and 3He particles were analyzed in the S800 magnetic spectrometer. Decay by neutron emission from excited states in Nb100 was observed by using plastic and liquid scintillator arrays. Differential cross sections were analyzed and monopole excitations were revealed by using a multipole decomposition analysis. The Gamow–Teller transition strength observed at low excitation energies, which is important for estimating the electron-capture rate in astrophysical scenarios, was strongly fragmented and reduced compared to single-particle and spherical mean-field models. The consideration of deformation in the theoretical estimates was found to be important to better describe the fragmentation and strengths. A strong excitation of the isovector spin giant monopole resonance was observed, and well reproduced by the mean-field models. Its presence makes the extraction of Gamow–Teller strengths at high excitation energies difficult. The branches for statistical and direct decay by neutron emission were identified in the spectra. The upper limit for the branching ratio by direct decay (integrated over all observed excitations) was determined to be 20±6%. Even though the statistical uncertainties in the neutron-coincident data were too large to perform detailed studies of the decay by neutron emission from individual states and resonances, the experiment demonstrates the feasibility of the method.
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- 2017
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11. Compression-mode resonances in the calcium isotopes and implications for the asymmetry term in nuclear incompressibility
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K.B. Howard, U. Garg, M. Itoh, H. Akimune, S. Bagchi, T. Doi, Y. Fujikawa, M. Fujiwara, T. Furuno, M.N. Harakeh, Y. Hijikata, K. Inaba, S. Ishida, N. Kalantar-Nayestanaki, T. Kawabata, S. Kawashima, K. Kitamura, N. Kobayashi, Y. Matsuda, A. Nakagawa, S. Nakamura, K. Nosaka, S. Okamoto, S. Ota, S. Weyhmiller, and Z. Yang
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Physics ,QC1-999 - Abstract
Recent data on isoscalar giant monopole resonance (ISGMR) in the calcium isotopes 40,44,48Ca have suggested that Kτ, the asymmetry term in the nuclear incompressibility, has a positive value. A value of Kτ>0 is entirely incompatible with present theoretical frameworks and, if correct, would have far-reaching implications on our understanding of myriad nuclear and astrophysical phenomena. This paper presents results of an independent ISGMR measurement with the 40,42,44,48Ca(α,α′) reaction at Eα=386 MeV. These results conclusively discount the possibility of a positive value for Kτ, and are consistent with the previously-obtained values for this quantity. Keywords: Collectivity, Giant resonance, Nuclear incompressibility, Equation of state
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- 2020
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12. First measurement of isoscalar giant resonances in a stored-beam experiment
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J.C. Zamora, T. Aumann, S. Bagchi, S. Bönig, M. Csatlós, I. Dillmann, C. Dimopoulou, P. Egelhof, V. Eremin, T. Furuno, H. Geissel, R. Gernhäuser, M.N. Harakeh, A.-L. Hartig, S. Ilieva, N. Kalantar-Nayestanaki, O. Kiselev, H. Kollmus, C. Kozhuharov, A. Krasznahorkay, Th. Kröll, M. Kuilman, S. Litvinov, Yu.A. Litvinov, M. Mahjour-Shafiei, M. Mutterer, D. Nagae, M.A. Najafi, C. Nociforo, F. Nolden, U. Popp, C. Rigollet, S. Roy, C. Scheidenberger, M. von Schmid, M. Steck, B. Streicher, L. Stuhl, M. Thürauf, T. Uesaka, H. Weick, J.S. Winfield, D. Winters, P.J. Woods, T. Yamaguchi, K. Yue, and J. Zenihiro
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Physics ,QC1-999 - Abstract
A new technique developed for measuring nuclear reactions at low momentum transfer with stored beams in inverse kinematics was successfully used to study isoscalar giant resonances. The experiment was carried out at the experimental heavy-ion storage ring (ESR) at the GSI facility using a stored 58Ni beam at 100 MeV/u and an internal helium gas-jet target. In these measurements, inelastically scattered α-recoils at very forward center-of-mass angles (θcm≤1.5°) were detected with a dedicated setup, including ultra-high vacuum compatible detectors. Experimental results indicate a dominant contribution of the isoscalar giant monopole resonance at this very forward angular range. It was found that the monopole contribution exhausts 79−11+12% of the energy-weighted sum rule (EWSR), which agrees with measurements performed in normal kinematics. This opens up the opportunity to investigate the giant resonances in a large domain of unstable and exotic nuclei in the near future. It is a fundamental milestone towards new nuclear reaction studies with stored ion beams. Keywords: Storage ring, Inverse kinematics, Isoscalar giant resonances
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- 2016
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13. Are there nuclear structure effects on the isoscalar giant monopole resonance and nuclear incompressibility near A∼90?
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Y.K. Gupta, U. Garg, K.B. Howard, J.T. Matta, M. Şenyiğit, M. Itoh, S. Ando, T. Aoki, A. Uchiyama, S. Adachi, M. Fujiwara, C. Iwamoto, A. Tamii, H. Akimune, C. Kadono, Y. Matsuda, T. Nakahara, T. Furuno, T. Kawabata, M. Tsumura, M.N. Harakeh, and N. Kalantar-Nayestanaki
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Physics ,QC1-999 - Abstract
“Background-free” spectra of inelastic α-particle scattering have been measured at a beam energy of 385 MeV in 90,92Zr and 92Mo at extremely forward angles, including 0°. The ISGMR strength distributions for the three nuclei coincide with each other, establishing clearly that nuclear incompressibility is not influenced by nuclear shell structure near A∼90 as was claimed in recent measurements.
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- 2016
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14. The pygmy quadrupole resonance and neutron-skin modes in 124Sn
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M. Spieker, N. Tsoneva, V. Derya, J. Endres, D. Savran, M.N. Harakeh, S. Harissopulos, R.-D. Herzberg, A. Lagoyannis, H. Lenske, N. Pietralla, L. Popescu, M. Scheck, F. Schlüter, K. Sonnabend, V.I. Stoica, H.J. Wörtche, and A. Zilges
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Atomic nuclei ,Collective quadrupole excitations ,Pygmy quadrupole resonance ,124Sn ,Physics ,QC1-999 - Abstract
We present an extensive experimental study of the recently predicted pygmy quadrupole resonance (PQR) in Sn isotopes, where complementary probes were used. In this study, (α,α′γ) and (γ,γ′) experiments were performed on 124Sn. In both reactions, Jπ=2+ states below an excitation energy of 5 MeV were populated. The E2 strength integrated over the full transition densities could be extracted from the (γ,γ′) experiment, while the (α,α′γ) experiment at the chosen kinematics strongly favors the excitation of surface modes because of the strong α-particle absorption in the nuclear interior. The excitation of such modes is in accordance with the quadrupole-type oscillation of the neutron skin predicted by a microscopic approach based on self-consistent density functional theory and the quasiparticle-phonon model (QPM). The newly determined γ-decay branching ratios hint at a non-statistical character of the E2 strength, as it has also been recently pointed out for the case of the pygmy dipole resonance (PDR). This allows us to distinguish between PQR-type and multiphonon excitations and, consequently, supports the recent first experimental indications of a PQR in 124Sn.
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- 2016
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15. Observation of isoscalar multipole strengths in exotic doubly-magic 56Ni in inelastic α scattering in inverse kinematics
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S. Bagchi, J. Gibelin, M.N. Harakeh, N. Kalantar-Nayestanaki, N.L. Achouri, H. Akimune, B. Bastin, K. Boretzky, H. Bouzomita, M. Caamaño, L. Càceres, S. Damoy, F. Delaunay, B. Fernández-Domínguez, M. Fujiwara, U. Garg, G.F. Grinyer, O. Kamalou, E. Khan, A. Krasznahorkay, G. Lhoutellier, J.F. Libin, S. Lukyanov, K. Mazurek, M.A. Najafi, J. Pancin, Y. Penionzhkevich, L. Perrot, R. Raabe, C. Rigollet, T. Roger, S. Sambi, H. Savajols, M. Senoville, C. Stodel, L. Suen, J.C. Thomas, M. Vandebrouck, and J. Van de Walle
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Physics ,QC1-999 - Abstract
The Isoscalar Giant Monopole Resonance (ISGMR) and the Isoscalar Giant Dipole Resonance (ISGDR) compression modes have been studied in the doubly-magic unstable nucleus 56Ni. They were measured by inelastic α-particle scattering in inverse kinematics at 50 MeV/u with the MAYA active target at the GANIL facility. The centroid of the ISGMR has been obtained at Ex=19.1±0.5 MeV. Evidence for the low-lying part of the ISGDR has been found at Ex=17.4±0.7 MeV. The strength distribution for the dipole mode shows similarity with the prediction from the Hartree–Fock (HF) based random-phase approximation (RPA) [1]. These measurements confirm inelastic α-particle scattering as a suitable probe for exciting the ISGMR and the ISGDR modes in radioactive isotopes in inverse kinematics.
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- 2015
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16. Splitting of ISGMR strength in the light-mass nucleus 24Mg due to ground-state deformation
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Y.K. Gupta, U. Garg, J.T. Matta, D. Patel, T. Peach, J. Hoffman, K. Yoshida, M. Itoh, M. Fujiwara, K. Hara, H. Hashimoto, K. Nakanishi, M. Yosoi, H. Sakaguchi, S. Terashima, S. Kishi, T. Murakami, M. Uchida, Y. Yasuda, H. Akimune, T. Kawabata, and M.N. Harakeh
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Physics ,QC1-999 - Abstract
The isoscalar giant monopole resonance (ISGMR) strength distribution in 24Mg has been determined from background-free inelastic scattering of 386-MeV α particles at extreme forward angles, including 0∘. The ISGMR strength distribution has been observed for the first time to have a two-peak structure in a light-mass nucleus. This splitting of ISGMR strength is explained well by microscopic theory in terms of the prolate deformation of the ground state of 24Mg.
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- 2015
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17. Corrigendum to 'Splitting of ISGMR strength in the light-mass nucleus 24Mg due to ground-state deformation' [Phys. Lett. B 748 (2015) 343–346]
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Y.K. Gupta, U. Garg, J.T. Matta, D. Patel, T. Peach, J. Hoffman, K. Yoshida, M. Itoh, M. Fujiwara, K. Hara, H. Hashimoto, K. Nakanishi, M. Yosoi, H. Sakaguchi, S. Terashima, S. Kishi, T. Murakami, M. Uchida, Y. Yasuda, H. Akimune, T. Kawabata, and M.N. Harakeh
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Physics ,QC1-999 - Published
- 2015
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18. M4 Resonances in Light Nuclei Studied at CCB
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N. Cieplicka-Oryńczak, B. Fornal, M. Ciemała, M. Kmiecik, A. Maj, J. Łukasik, P. Pawłowski, B. Sowicki, B. Wasilewska, M. Ziębliński, P. Bednarczyk, I. Ciepał, K. Dhanmeher, J. Grębosz, Ł.W. Iskra, M. Krzysiek, M. Matejska-Minda, K. Mazurek, W. Parol, B. Włoch, C. Boiano, S. Brambilla, B. Million, Y. Jaganathen, M. Płoszajczak, I. Burducea, C. Clisu, N. Florea, D.A. Iancu, N. Marginean, R. Marginean, L. Stan, M.N. Harakeh, P. Kulessa, I. Matea, M. Sferrazza, Grand Accélérateur National d'Ions Lourds (GANIL), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), and Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)
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[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th] ,General Physics and Astronomy - Abstract
International audience; M4 resonances in light nuclei result from the p3/2 → d5/2 stretched excitations. Their configurations should be relatively simple, which makes them good benchmarks for the theoretical calculations taking into account the role of continuum couplings. The first experimental studies aiming at tracing the decay of the M4 stretched resonance in 13C, located at 21.47 MeV, were undertaken at the Cyclotron Centre Bronowice at the Institute of Nuclear Physics Polish Academy of Sciences in Kraków, Poland (IFJ PAN). They provided information on the proton and neutron decay channels of this resonance to 12B and 12C daughter nuclei, respectively. These experimental results were then compared with the theoretical calculations based on the Gamow Shell Model approach, in terms of energy, width, and in particular, the decay pattern. Furthermore, the studies of the next cases, namely, 14N and 16O, where several M4 resonances appear at around 20 MeV, have been recently performed at CCB. The new experimental findings will serve as a testing ground for future calculations describing the heavier nuclei in this important region of the nuclear chart.
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- 2022
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19. Search for in-band transitions in the candidate superdeformed band in 28Si
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R. G. T. Zegers, Johann Isaak, A. Bracco, B. Wasilewska, S. Zhu, T. H. Hoang, X. H. Zhou, J. J. Carroll, S. Adachi, C. Sullivan, M. P. Carpenter, M. Kumar Raju, Atsushi Tamii, L. Morris, Y. D. Fang, J. Schmitt, Shumpei Noji, N. Ichige, P. J. Davies, D. G. Jenkins, Eiji Ideguchi, G. Gey, Deniz Savran, Nobumichi Kobayashi, P. Adsley, S. Courtin, G. Fruet, Hooi Jin Ong, P. von Neumann-Cosel, A. S. Brown, Takeshi Koike, D. Montanari, A. Inoue, Nori Aoi, Hisanori Fujita, M.N. Harakeh, C. Iwamoto, V. Werner, Yasuo Yamamoto, M. L. Liu, M. Weinert, F. C. L. Crespi, Université de Strasbourg (UNISTRA), Institut Pluridisciplinaire Hubert Curien (IPHC), and Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université de Strasbourg (UNISTRA)-Centre National de la Recherche Scientifique (CNRS)
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Physics ,[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th] ,010308 nuclear & particles physics ,0103 physical sciences ,Astrophysics ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,010306 general physics ,01 natural sciences - Abstract
International audience; Background: Superdeformed (SD) bands are suggested by theory around Ca40 and in lighter alpha-conjugate nuclei such as Mg24, Si28, and S32. Such predictions originate from a number of theoretical models including mean-field models and antisymmetrized molecular dynamics (AMD) calculations. While SD bands have been identified in Ca40 and its near neighbors, evidence of their existence in the lighter, midshell nuclei is circumstantial at best. The key evidence of superdeformation would be the observation of transitions with high B(E2) transition strengths connecting states in a rotational sequence. This is challenging information to obtain since the bands lie at a high excitation energy and competition from out-of-band decay is dominant.Purpose: The purpose of the present study is to establish a new methodology to circumvent the difficulties in identifying and quantifying in-band transitions through directly populating candidate states in the SD band in Si28 through inelastic alpha scattering, selecting such states with a spectrometer, and measuring their gamma-ray decay with a large array of high-purity germanium detectors, allowing direct access to electromagnetic transition strengths.Methods: Excited states in Si28 were populated in the Si28(α,α′) reaction using a 130-MeV He4 beam from the K140 AVF cyclotron at the Research Center for Nuclear Physics. Outgoing alpha particles were analyzed using the Grand Raiden spectrometer positioned at an angle of 9.1∘ to favor the population of states with J≈4. Coincident gamma rays were detected with the CAGRA array of 12 HPGe clover detectors augmented by a set of four large LaBr3 detectors.Results: Data analysis showed that it was possible to identify additional low-energy transitions in competition with high-energy decays from excited states in Si28 in the vicinity of 10 MeV. However, while the candidate 4+ SD state at 10.944 MeV was populated, a 1148-keV transition to the candidate 2+ SD state at 9.796 MeV was not observed, and only an upper limit for its transition strength of B(E2)<43 W.u. could be established. This contradicts AMD predictions of ≈200 W.u. for such a transition.Conclusion: The present study strongly rejects the hypothesis that the candidate set of states identified in Si28 represents an SD band, which demonstrates the potential of the methodology devised here.
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- 2021
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20. Study of spin-isospin responses of radioactive nuclei with the background-reduced neutron spectrometer, PANDORA
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N. Fukuda, Takashi Nakamura, H. Sakai, Yohei Shimizu, J. Gibelin, Makoto Yasuda, Tomotsugu Wakasa, M. Nishimura, J. Gao, Masashige Matsumoto, S. Franchoo, H. Miki, H. Kasahara, T. Harada, Masaki Sasano, D. Tudor, Toshio Kobayashi, T. Isobe, G. G. Kiss, Tomohiro Uesaka, Yasuhiro Togano, Susumu Shimoura, Atsumi Saito, N. Zhang, I. C. Stefanescu, E. Takada, Zoltán Halász, L. Trache, Yuya Kubota, D. Kim, T. Shimada, Shoko Koyama, Y. Fujino, Juzo Zenihiro, Z. Korkulu, D. Inomoto, Zaihong Yang, H. Sato, H. N. Liu, A. Spiridon, M. Miwa, H. Suzuki, L. Stuhl, V. Panin, H. Baba, Yosuke Kondo, S. Park, K. Yoneda, T. Motobayashi, Y. L. Sun, T. Tomai, I. S. Hahn, Kentaro Yako, X. Sun, A. Kurihara, M.N. Harakeh, Y. Hirai, D. S. Ahn, A. I. Chilug, Hideaki Otsu, Hiroki Yamada, Shin'ichiro Michimasa, K. Yoshida, 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), Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Département de Physique Nucléaire (ex SPhN) (DPHN), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Research unit Nuclear & Hadron Physics, 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), and Normandie Université (NU)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)
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Nuclear and High Energy Physics ,Nuclear Theory ,n) reactions ,Inverse-kinematics (p, n) reactions ,01 natural sciences ,Low-energy neutron detector ,Inverse-kinematics [formula omitted] reactions ,Nuclear physics ,0103 physical sciences ,Figure-of-Merit (FoM) ,Neutron detection ,Neutron ,010306 general physics ,Spin (physics) ,Nuclear Experiment ,Instrumentation ,Gamow-Teller transition ,DETECTOR ,Real-time pulse-shape discrimination ,Physics ,[PHYS]Physics [physics] ,Spin-isospin response ,Spectrometer ,010308 nuclear & particles physics ,Figure-of-Merit (RIM) ,Detector ,PULSE-SHAPE DISCRIMINATION ,PLASTIC SCINTILLATOR ,Inverse-kinematics (p ,Isospin ,Ground state ,Beam (structure) - Abstract
The status of a project to measure spin-isospin responses of neutron drip-line nuclei using a new low-energy neutron detector, PANDORA (Particle Analyzer Neutron Detector Of Real-time Acquisition), is reported. The performance of PANDORA was characterized by the 6He(p,n)6Li reaction in inverse kinematics at the HIMAC facility in Chiba. Observation of the strong transition to the ground state in 6Li is discussed. Preliminary results of 11Li(p,n)11Be and 14Be(p,n)14B experiments in inverse kinematics at RI Beam Factory (RIBF) of RIKEN Nishina Center are also presented including the exotic decay channel of 11Be→9Li + d. Details of the experimental setup based on PANDORA and the SAMURAI large-acceptance magnetic spectrometer, as well as the combined data-acquisition system are described. The neutron-gamma discrimination capability of PANDORA was evaluated, Figure-of-Merit (FoM) values higher than those found in the literature for similar materials were derived from experimental data.
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- 2020
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21. Decay of the 'stretched' M4 resonance in 13C
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D.A. Iancu, P. Kulessa, L. Stan, Y. Jaganathen, S. Bottoni, A. Maj, N. Marginean, Michele Sferrazza, S. Brambilla, P. Pawłowski, S. Ziliani, A. Bracco, M. Kmiecik, J. Łukasik, Ł. W. Iskra, B. Fornal, K. Mazurek, I. Burducea, S. Leoni, C. Boiano, R. Marginean, N. Florea, C. Clisu, F. Camera, B. Sowicki, M. Płoszajczak, M.N. Harakeh, N. Cieplicka-Oryńczak, M. Krzysiek, M. Ciemala, M. Zieblinski, J. Grebosz, B. Wasilewska, M. Matejska-Minda, Grand Accélérateur National d'Ions Lourds (GANIL), Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), and Research unit Nuclear & Hadron Physics
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Physics ,[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th] ,Proton ,Nuclear Theory ,Continuum (design consultancy) ,Cyclotron ,SHELL model ,General Physics and Astronomy ,Resonance (particle physics) ,Coincidence ,law.invention ,Nuclear physics ,law ,Neutron ,Nuclear Experiment - Abstract
International audience; “Stretched” states are examples of the simplest nuclear excitations in the continuum, thus offering an excellent testing ground for various theoretical approaches. The decay of the stretched single-particle state in 13C, located at 21.47 MeV, was investigated in an experiment performed recently at the Cyclotron Centre Bronowice (CCB) at IFJ PAN in Kraków. First experimental information on the proton and neutron decay channels of this resonance was obtained by employing coincidence measurement of protons inelastically scattered on the 13C target and γ rays from daughter nuclei. The new experimental findings will be used for testing predictions obtained by the Gamow Shell Model calculations.
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- 2020
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22. Spectroscopy of neutron-rich nitrogen isotopes with Agata+Paris+Vamos
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S. Ziliani, M. Ciemała, F.C.L. Crespi, S. Leoni, B. Fornal, A. Maj, P. Bednarczyk, G. Benzoni, A. Bracco, C. Boiano, S. Bottoni, S. Brambilla, M. Bast, M. Beckers, T. Braunroth, F. Camera, N. Cieplicka-Oryńczak, E. Clément, S. Coelli, O. Dorvaux, S. Erturk, G. de France, C. Fransen, A. Goldkuhle, J. Grębosz, M.N. Harakeh, Ł.W. Iskra, B. Jacquot, A. Karpov, M. Kicińska-Habior, Y. Kim, M. Kmiecik, A. Lemasson, S.M. Lenzi, M. Lewitowicz, H. Li, I. Matea, K. Mazurek, C. Michelagnoli, M. Matejska-Minda, B. Million, C. Müller-Gatermann, V. Nanal, P. Napiorkowski, D.R. Napoli, R. Palit, M. Rejmund, Ch. Schmitt, M. Stanoiu, I. Stefan, E. Vardaci, B. Wasilewska, O. Wieland, M. Ziębliński, M. Zielińska, Ziliani, S., Ciemała, M., Crespi, F. C. L., Leoni, S., Fornal, B., Maj, A., Bednarczyk, P., Benzoni, G., Bracco, A., Boiano, C., Bottoni, S., Brambilla, S., Bast, M., Beckers, M., Braunroth, T., Camera, F., Cieplicka-Orynczak, N., Clément, E., Coelli, S., Dorvaux, O., Erturk, S., de France, G., Fransen, C., Goldkuhle, A., Grebosz, J., Harakeh, M. N., Iskra, Ł. W., Jacquot, B., Karpov, A., Kicinska-Habior, M., Kim, Y., Kmiecik, M., Lemasson, A., Lenzi, S. M., Lewitowicz, M., Li, H., Matea, I., Mazurek, K., Michelagnoli, C., Matejska-Minda, M., Million, B., Müller-Gatermann, C., Nanal, V., Napiorkowski, P., Napoli, D. R., Palit, R., Rejmund, M., Schmitt, Ch., Stanoiu, M., Stefan, I., Vardaci, E., Wasilewska, B., Wieland, O., Zieblinski, M., Zielinska, M., Grand Accélérateur National d'Ions Lourds (GANIL), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg (UNISTRA)-Université de Haute-Alsace (UHA) Mulhouse - Colmar (Université de Haute-Alsace (UHA))-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-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 Laue-Langevin (ILL), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université de Strasbourg (UNISTRA)-Centre National de la Recherche Scientifique (CNRS), 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), ILL, and Research unit Nuclear & Hadron Physics
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Physics ,education.field_of_study ,Spectrometer ,010308 nuclear & particles physics ,Astrophysics::High Energy Astrophysical Phenomena ,Population ,Gamma ray ,General Physics and Astronomy ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,01 natural sciences ,Nuclear physics ,Excited state ,0103 physical sciences ,Neutron ,AGATA ,010306 general physics ,Spectroscopy ,education ,Beam (structure) - Abstract
Excited states of 17N, 18N and 19N were investigated through the measurement of gamma rays, following their population via deep-inelastic reactions induced by an 18O beam (7 MeV/u) on a thick 181Ta target. The experimental setup comprised the AGATA+PARIS detection system, coupled to the VAMOS++ magnetic spectrometer. In the 17N nucleus, the analysis of gamma-ray transitions de-exciting two states around 4-5 MeV clearly pointed to discrepancies with the lifetime values reported in literature. Three new gamma rays were observed in 18N at the energies of 1662.3 (3) keV, 2073.4 (8) keV and 2300.9 (8) keV, and hints for other two new transitions around 1566 keV and 1720 keV were found. In addition, a new transition with energy of 2489.7 (8) keV was observed in 19N.
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- 2020
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23. Investigation of the isoscalar response of Mg24 to Li6 scattering
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Shumpei Noji, G. Gey, Y. Yamamoto, L. Batail, S. Zhu, R. Titus, Eiji Ideguchi, P. von Neumann-Cosel, A. Inoue, J. C. Zamora, Hooi Jin Ong, J. Schmitt, Johann Isaak, M. P. Carpenter, Nori Aoi, T. H. Hoang, U. Garg, J. J. Carroll, V. Werner, X. K. Zhou, M. L. Liu, Takeshi Koike, Nobuyuki Kobayashi, C. Kacir, C. J. Guess, D. Bazin, Hisanori Fujita, R. G. T. Zegers, Chihiro Iwamoto, Sophie Péru, N. Ichige, C. Sullivan, Atsushi Tamii, S. Lipschutz, E. Hudson, J. Pereira, M.N. Harakeh, M. Kumar Raju, and Y. D. Fang
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Physics ,010308 nuclear & particles physics ,Scattering ,Isoscalar ,Nuclear Theory ,Resonance ,Inelastic scattering ,01 natural sciences ,Molecular physics ,0103 physical sciences ,Quadrupole ,010306 general physics ,Random phase approximation ,Ground state ,Multipole expansion - Abstract
Background: Mg 24 is a strongly deformed nucleus in the ground state. Deformation effects can be observed in the structure of the isoscalar giant monopole and quadrupole resonances. Mg 24 is also a nucleus that is well known to present different types of cluster-oscillation modes. Both giant resonances and cluster states are strongly populated by isoscalar transitions. Purpose: To extract the E 0 , E 1 , and E 2 transition strengths via Li 6 scattering. The Li 6 probe is a powerful tool for investigating the isoscalar nuclear response with a very favorable ratio of resonance-to-continuum background. Method: Double-differential cross sections of Li 6 inelastic scattering, at the beam energy of 100 MeV/u, were measured in the excitation-energy range 10 – 40 MeV and scattering angles 0 − 3 ∘ . A multipole-decomposition analysis was performed for extracting the isoscalar E 0 , E 1 , and E 2 strength distributions. Results: The extracted multipole strengths were compared with predictions from consistent quasiparticle random phase approximation calculations. The theoretical predictions are in fair agreement with the experimental data. The E 0 strength was also compared with results from antisymmetrized molecular dynamics calculations found in the literature. A few peaks in the experimental data might be associated with clustering in Mg 24 . Conclusions: Ground-state deformation effects were observed in the isoscalar giant monopole resonance (ISGMR) and isoscalar giant quadrupole resonance (ISGQR) distributions. The ISGMR strength is split in two peaks around 19 and 28 MeV. The ISGQR exhibits a pronounced peak at 20 MeV with a broadening at the low-energy region, similar to predictions from microscopic calculations. Signatures of excitation of cluster states were observed in the E 0 response. Further studies including particle-decay measurements will be required to confirm the nature of the observed peaks.
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- 2021
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24. The structure of low-lying 1− states in 90,94Zr from (α,α′γ) and (p,p′γ) reactions
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Miao Liu, T. Hashimoto, J.M. Schmitt, X. K. Zhou, O. Wieland, C. Iwamoto, Norbert Pietralla, B. Wasilewska, S. Zhu, A. Czeszumska, Johann Isaak, T. Klaus, C. Sullivan, A. Inoue, M.K. Raju, Y.D. Fang, Nobuyuki Kobayashi, F. Camera, Yoshihisa Yamamoto, Shumpei Noji, V. Werner, A. Maj, G. Gey, D. G. Jenkins, Hooi Jin Ong, M. Krzysiek, F. C. L. Crespi, Andreas Zilges, M. Ciemała, L. Morris, R. G. T. Zegers, Takeshi Koike, T. Yamamoto, M. P. Carpenter, G. Steinhilber, D. L. Balabanski, A. Bracco, S. Bassauer, V. Derya, Nori Aoi, J. J. Carroll, E.G. Lanza, M. Spieker, A. S. Brown, N. Ichige, Deniz Savran, H. Fujita, S. G. Pickstone, N. Blasi, P. J. Davies, P. von Neumann Cosel, M.N. Harakeh, H.T. Ha, Atsushi Tamii, M. Weinert, L. M. Donaldson, Eiji Ideguchi, and Research unit Nuclear & Hadron Physics
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Physics ,Nuclear and High Energy Physics ,Range (particle radiation) ,Inelastic scattering ,Isovector ,Proton ,010308 nuclear & particles physics ,Isoscalar ,Binding energy ,01 natural sciences ,Dipole excitation around neutron threshold ,lcsh:QC1-999 ,Dipole ,0103 physical sciences ,Neutron ,Sum rule in quantum mechanics ,Nuclear structure ,Atomic physics ,010306 general physics ,lcsh:Physics - Abstract
The low-lying dipole strength in the 90,94Zr nuclei was investigated via (p,p′γ) at 80 MeV and (α,α′γ) at 130 MeV. The experiments, made at RCNP, used the magnetic spectrometer Grand Raiden for the scattered particles and the array CAGRA with HPGe detectors for the γ-decay. For 94Zr these are the first data for both reactions and for 90Zr these are the first data with (p,p′γ) and the first ones at high resolution for (α,α′γ). The comparison of the present results for the two nuclei with existing (γ,γ′) data shows that both nuclear probes produce an excitation pattern different than that of the electromagnetic probes. DWBA calculations were made using form factors deduced from transition densities, based on RPA calculations, characterized by a strong neutron component at the nuclear surface. A combined analysis of the two reactions was performed for the first time to investigate the isoscalar character of the 1− states in 90,94Zr. The (p,p′γ) cross section was calculated using values for the isoscalar electric dipole energy-weighted sum rule (E1 ISEWSR) obtained from the (α,α′γ) data. The isoscalar strength for 90Zr was found to exhaust 20 ± 2.5% of the EWSR in the energy range up to 12 MeV. In case of 94Zr, a strength of 9 ± 1.1% of the EWSR was found in the range up to 8.5 MeV. Although an overall general description was obtained in the studied energy intervals, not all proton cross sections were well reproduced using the isoscalar strength from (α,α′γ). This might suggest mixing of isoscalar and isovector components and that this mixing and the degree of collectivity are not the same for all the 1− states below the particle binding energy.
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- 2021
25. Experimental Study of $^{4}n$ by Directly Detecting the Decay Neutrons
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Atsumi Saito, Yohei Shimizu, H. Törnqvist, B. Monteagudo, T. Isobe, M. Caamaño, H. Scheit, S. Kiyotake, J. Tscheuschner, M. L. Cortés, F. M. Marqués, N. Fukuda, N. A. Orr, J. M. Gheller, A. Gillibert, A. Matta, K. Yoneda, L. Stuhl, Z. Elekes, I. Kuti, V. Wagner, M. Miwa, Z. Halász, A. Obertelli, S. Kim, A. Revel, L. Zanetti, N. L. Achouri, S. Takeuchi, F. Dufter, C. A. Douma, S. Masuoka, Stefanos Paschalis, R. Gernhäuser, S. Chen, Nobuyuki Chiga, S. Storck, T. Shimada, M.N. Harakeh, P. Koseoglou, T. Harada, B. Yang, M. Matsumoto, H. Takeda, D. S. Ahn, Yuya Kubota, H. Yamada, Yasuhiro Togano, A. Hirayama, Y. Yasuda, T. Fujino, D. M. Rossi, Nasser Kalantar-Nayestanaki, J. Tanaka, M. Böhmer, N. Inabe, Didier Beaumel, S. Park, Thomas Aumann, H. Baba, Tomohiro Uesaka, F. Schindler, J. Feng, Zaihong Yang, I. Murray, Julien Gibelin, K. Boretzky, S. W. Huang, B. Fernández-Domínguez, S. Reichert, Takashi Nakamura, Yu-xin Liu, K. Wimmer, Yukie Maeda, L. Yang, H. Sato, E. Tronchin, P. Doornenbal, Dmytro Symochko, D. Cortina, J. Kahlbow, S. Shimoura, H. Suzuki, Hideaki Otsu, M. Potlog, P. J. Li, J. Mayer, H. Miki, Masaki Sasano, Toshio Kobayashi, Z. Ge, D. Kim, Juzo Zenihiro, T. Tomai, I. Stefan, M. Parlog, H. Simon, V. Panin, Igor Gašparić, C. Lehr, Yosuke Kondo, C. Lenain, U. Forsberg, Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-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), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Grand Accélérateur National d'Ions Lourds (GANIL), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Normandie Université (NU)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), 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), Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Research unit Nuclear & Hadron Physics, and Nuclear Energy
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Nuclear structure and force ,tetraneutron ,direct reactions ,radioactive beams ,Physics ,Nuclear physics ,010308 nuclear & particles physics ,0103 physical sciences ,Tetraneutron ,Neutron ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,010306 general physics ,01 natural sciences ,Atomic and Molecular Physics, and Optics ,3. Good health - Abstract
The tetraneutron has attracted the attention of nuclear physicists during the past decades, but there is still no unambiguous confirmation of its existence or non-existence. A new experiment based on $$^{8}$$ He(p, 2p) $$^{7}$$ H{t+ $$^{4}n$$ } reaction, with direct detection of the four neutrons, has been carried out at RIBF, which can hopefully help to draw a definite conclusion on the tetraneutron system.
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- 2021
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26. Search for η'-mesic nuclei using (p,d) reaction with FRS/Super-FRS at GSI/FAIR
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R. Kanungo, Oleksandr Rundel, Haruhiko Outa, Isao Tanihata, C. Scheidenberger, C. Guo, N. Kuzminchuk, N. Ikeno, S. Purushothaman, E. Haettner, M.N. Harakeh, S. Terashima, Frank Goldenbaum, H. Fujioka, Timo Dickel, R. Knöbel, J. Zhao, Yasumoto Tanaka, James Ritman, Birgit Kindler, Bao-Hua Sun, J. L. Rodriguez-Sanchez, Ryugo S. Hayano, Satoru Hirenzaki, Hideko Nagahiro, I. G. Mukha, W. R. Plass, Peter Strmen, Magdalena Skurzok, Christine Hornung, T.R. Saito, Hiroyuki Ekawa, M. Takechi, Y. Igarashi, Branislav Sitar, Helmut Weick, V. Metag, V. Drozd, Nasser Kalantar-Nayestanaki, Y. Ma, S. Bagchi, M. Iwasaki, N. Kurz, Daisuke Jido, Hans Geissel, S. Minami, D. Kostyleva, Bettina Lommel, R. Ruber, Imrich Szarka, C. Rappold, Herbert A. Simon, K. Itahashi, R. Sekiya, M. Nakagawa, V. Serdyuk, S. Pietri, J. Benlliure, Tomofumi Nagae, A. Prochazka, Paweł Moskal, Hooi Jin Ong, S.Y. Matsumoto, A. Yamamoto, Energy and Sustainability Research Institute Groni, and Research unit Nuclear & Hadron Physics
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Physics ,History ,Proton ,Detector ,Nuclear Theory ,Coincidence ,Computer Science Applications ,Education ,Event selection ,Nuclear physics ,Subatomär fysik ,Deuterium ,Subatomic Physics ,ddc:530 ,High Energy Physics::Experiment ,Spectroscopy ,Nuclear Experiment ,Beam (structure) - Abstract
Journal of physics / Conference series 1643, 012181 (2020). doi:10.1088/1742-6596/1643/1/012181, Published by IOP Publ., Bristol
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- 2020
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27. Signature of a possible $\alpha $-cluster state in $N=Z$ doubly-magic $^{56}$Ni
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L. Perrot, S. M. Lukyanov, U. Garg, L. Caceres, B. Bastin, A. Krasznahorkay, M. A. Najafi, J. F. Libin, S. Damoy, Marine Vandebrouck, Franck Delaunay, Catherine Rigollet, L. Suen, M. Caamaño, Julien Gibelin, K. Boretzky, J. Van de Walle, Nasser Kalantar-Nayestanaki, Hidetoshi Akimune, H. Bouzomita, G. Lhoutellier, C. Stodel, J. Pancin, Riccardo Raabe, S. Bagchi, O. Kamalou, H. Savajols, M.N. Harakeh, T. Roger, B. Fernández-Domínguez, Y. E. Penionzhkevich, M. Sénoville, N. L. Achouri, K. Mazurek, G. F. Grinyer, E. Khan, S. Sambi, J. C. Thomas, M. Fujiwara, Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Grand Accélérateur National d'Ions Lourds (GANIL), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), 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), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Normandie Université (NU)-Centre National de la Recherche Scientifique (CNRS)-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)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), 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)
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Nuclear and High Energy Physics ,Hadron ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,01 natural sciences ,Physics, Particles & Fields ,0103 physical sciences ,medicine ,Incident energy ,Nuclear fusion ,ddc:530 ,Multiplicity (chemistry) ,Nuclear Experiment ,010306 general physics ,ComputingMilieux_MISCELLANEOUS ,Physics ,Science & Technology ,010308 nuclear & particles physics ,Cluster state ,Physics, Nuclear ,medicine.anatomical_structure ,Physical Sciences ,Atomic physics ,α particles ,Nucleus ,Excitation - Abstract
An inelastic $\alpha$-scattering experiment on the unstable $N=Z$, doubly-magic $^{56}$Ni nucleus was performed in inverse kinematics at an incident energy of 50 A.MeV at GANIL. High multiplicity for $\alpha$-particle emission was observed within the limited phase-space of the experimental setup. This observation cannot be explained by means of the statistical-decay model. The ideal classical gas model at $kT$ = 0.4 MeV reproduces fairly well the experimental momentum distribution and the observed multiplicity of $\alpha$ particles corresponds to an excitation energy around 96 MeV. The method of distributed $m\alpha$-decay ensembles is in agreement with the experimental results if we assume that the $\alpha$-gas state in $^{56}$Ni exists at around $113^{+15}_{-17}$ MeV. These results suggest that there may exist an exotic state consisting of many $\alpha$ particles at the excitation energy of $113^{+15}_{-17}$ MeV., Comment: Accepted for publication in the European Physical Journal A
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- 2020
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28. Reexamination of isoscalar giant resonances in C12 and Nb93 through Li6 scattering
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J. C. Zamora, J. Schmitt, C. J. Guess, V. Werner, Shumpei Noji, G. Gey, Nobuyuki Kobayashi, Y. Yamamoto, S. Zhu, T. H. Hoang, I. Deloncle, L. Batail, R. Titus, D. Bazin, S. Péru, R. G. T. Zegers, X. K. Zhou, J. Pereira, E. Hudson, C. Kacir, U. Garg, Takeshi Koike, C. Sullivan, M. P. Carpenter, Atsushi Tamii, Nori Aoi, S. Lipschutz, Eiji Ideguchi, Hisanori Fujita, Hooi Jin Ong, M.N. Harakeh, A. Inoue, Johann Isaak, Chihiro Iwamoto, M. L. Liu, Y. D. Fang, J. J. Carroll, M. Kumar Raju, N. Ichige, and P. von Neumann-Cosel
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Mass number ,Physics ,010308 nuclear & particles physics ,Scattering ,Isoscalar ,Magnetic monopole ,Nuclear structure ,Resonance ,01 natural sciences ,Excited state ,0103 physical sciences ,Sum rule in quantum mechanics ,Atomic physics ,Nuclear Experiment ,010306 general physics - Abstract
Inelastic ${}^{6}$Li scattering at 100 MeV/u on ${}^{12}$C and ${}^{93}$Nb have been measured with the high-resolution magnetic spectrometer Grand Raiden. The magnetic-rigidity settings of the spectrometer covered excitation energies from 10 to 40 MeV and scattering angles in the range $0^\circ < \theta_{\text{lab.}}< 2^\circ$. The isoscalar giant monopole resonance was selectively excited in the present data. Measurements free of instrumental background and the very favorable resonance-to-continuum ratio of ${}^{6}$Li scattering allowed for precise determination of the $E0$ strengths in ${}^{12}$C and ${}^{93}$Nb. It was found that the monopole strength in ${}^{12}$C exhausts $52 \pm 3^\text{(stat.)} \pm 8 ^\text{(sys.)}$\% of the energy-weighted sum rule (EWSR), which is considerably higher than results from previous $\alpha$-scattering experiments. The monopole strength in ${}^{93}$Nb exhausts $92 \pm 4^\text{(stat.)} \pm 10 ^\text{(sys.)}$\% of the EWSR, and it is consistent with measurements of nuclei with mass number of $A\approx90$. Such comparison indicates that the isoscalar giant monopole resonance distributions in these nuclei are very similar, and no influence due to nuclear structure was observed.
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- 2020
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29. Extending the Southern Shore of the Island of Inversion to F28
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J. Mayer, Noritsugu Nakatsuka, Michael Thoennessen, A. Gillibert, Ákos Horváth, Q. Deshayes, Yosuke Kondo, J. Tscheuschner, Nasser Kalantar-Nayestanaki, J. M. Gheller, István Kuti, M. Shikata, Thomas Aumann, C. Caesar, J. Tsubota, A. Revel, N. L. Achouri, W. He, Z. Elekes, Calem Hoffman, Shoichiro Kawase, Heiko Scheit, J. Kahlbow, Masahiro Yasuda, H. Simon, H. Sato, K. Yoneda, A. Horvat, K. Nakano, Igor Gašparić, T. Ozaki, H. Chae, J. A. Tostevin, L. Stuhl, K. Miki, F. de Oliveira Santos, H. L. Crawford, D. Calvet, Stefanos Paschalis, S. Masuoka, T. Isobe, A. Obertelli, Tomoki Saito, Momoko Tanaka, N. A. Orr, Shoko Koyama, Nobuyuki Chiga, L. Atar, Y. Satou, P. Fallon, Atsumi Saito, Zsolt Dombrádi, H. Törnqvist, Jongwon Hwang, A. Corsi, Julien Gibelin, K. Boretzky, A. Delbart, D. M. Rossi, H. Baba, Masaki Sasano, D. Sohler, V. Lapoux, M. A. Najafi, S. K. Kim, A. Hirayama, H. Al Falou, K. Kisamori, T. Tomai, V. Panin, P. Schrock, Takashi Nakamura, Yasuhiro Togano, M.N. Harakeh, M. Holl, Zaihong Yang, F. Nowacki, T. Kobayashi, Cenxi Yuan, D. Körper, Tomohiro Uesaka, Thomas Nilsson, C. A. Douma, Simon Lindberg, Hideaki Otsu, O. Sorlin, T. Murakami, Yohei Shimizu, Fabia Schindler, Franck Delaunay, F. M. Marqués, and Satoshi Takeuchi
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Physics ,Proton ,Island of inversion ,General Physics and Astronomy ,01 natural sciences ,Spectral line ,Momentum ,0103 physical sciences ,Neutron ,Atomic physics ,010306 general physics ,Nucleon ,Spectroscopy ,Ground state - Abstract
Detailed spectroscopy of the neutron-unbound nucleus 28 F has been performed for the first time following proton/neutron removal from 29 Ne / 29 F beams at energies around 230 MeV / nucleon . The invariant-mass spectra were reconstructed for both the 27 F ( * ) + n and 26 F ( * ) + 2 n coincidences and revealed a series of well-defined resonances. A near-threshold state was observed in both reactions and is identified as the 28 F ground state, with S n ( 28 F ) = − 199 ( 6 ) keV , while analysis of the 2 n decay channel allowed a considerably improved S n ( 27 F ) = 1620 ( 60 ) keV to be deduced. Comparison with shell-model predictions and eikonal-model reaction calculations have allowed spin-parity assignments to be proposed for some of the lower-lying levels of 28 F . Importantly, in the case of the ground state, the reconstructed 27 F + n momentum distribution following neutron removal from 29 F indicates that it arises mainly from the 1 p 3 / 2 neutron intruder configuration. This demonstrates that the island of inversion around N = 20 includes 28 F , and most probably 29 F , and suggests that 28 O is not doubly magic.
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- 2020
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30. Gamow–Teller strength distributions of $${^{116} \text {Sb}}$$ and $${^{122} \text {Sb}}$$ using the $${(^{3} \text {He}, t)}$$ charge-exchange reaction
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Manuela Cavallaro, P. Puppe, G. Gey, M. Alanssari, Atsushi Tamii, Yifei Niu, Francesco Cappuzzello, R. G. T. Zegers, V. Werner, M. Fujiwara, K. Heguri, M. Holl, C. A. Douma, Kichiji Hatanaka, C. Agodi, Hidetoshi Akimune, A. Inoue, M.N. Harakeh, D. Frekers, Hisanori Fujita, Diana Carbone, F. Hattori, Gianluca Colò, H. Ejiri, Kai Zuber, P. Ries, F Diel, Y. Fujita, and Nasser Kalantar-Nayestanaki
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Scattering ,Hadron ,Resonance ,Sum rule in quantum mechanics ,Coupling (probability) ,Charge exchange - Abstract
The Gamow–Teller strength distributions of $${^{116} \text {Sb}}$$116Sb and $${^{122} \text {Sb}}$$122Sb were measured with the $${^{116,122} \text {Sn} (^{3} \text {He},t) ^{116,122} \text {Sb}}$$116,122Sn(3He,t)116,122Sb charge-exchange reactions at $${140 \ \text {MeV/u}}$$140MeV/u. The measurements were carried out at the Research Center for Nuclear Physics (RCNP) at Osaka University in Osaka, Japan using the Grand Raiden spectrometer. The data were analysed by Multipole-Decomposition Analysis (MDA). The Gamow–Teller strengths summed up to $${28 \ \text {MeV}}$$28MeV are $${(38 \pm 7) \%}$$(38±7)% and $${(48 \pm 6) \%}$$(48±6)% of the Ikeda sum rule for $${^{116} \text {Sb}}$$116Sb and $${^{122} \text {Sb}}$$122Sb, respectively, if the quasi-free scattering (QFS) contribution is not subtracted. These percentages are $${(29 \pm 7) \%}$$(29±7)% and $${(35 \pm 5) \%}$$(35±5)%, respectively, if the QFS contribution is maximally subtracted. These results were compared to those from previous measurements of the same isotopes, to recent measurements of $${^{150} \text {Pm}}$$150Pm, and to a Quasi-particle Random-Phase Approximation (QRPA) calculation with Quasi-Particle Vibration Coupling (QPVC). The data suggest that the true QFS contribution is small for $${^{116} \text {Sb}}$$116Sb, but are inconclusive about whether the QFS contribution is small or significant for $${^{122} \text {Sb}}$$122Sb. Therefore, these data may provide an interesting test for the general quenching phenomenon of the Gamow–Teller Resonance (GTR). However, more research to reveal the nature of the QFS contribution is still needed on both the experimental and the theoretical side.
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- 2020
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31. Fragmentation of Single-Particle Strength around the Doubly Magic Nucleus Sn132 and the Position of the 0f5/2 Proton-Hole State in In131
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Hiroyoshi Sakurai, J. Tscheuschner, Yosuke Kondo, A. Bracco, D. Semmler, S. Nishimura, T. Motobayashi, Ryo Taniuchi, N. Imai, Kazuo Ieki, A. Jungclaus, Ismael Martel, F. Camera, P. Schrock, Heiko Scheit, Juzo Zenihiro, Andreas Zilges, V. Derya, D. S. Ahn, K. Boretzky, Yasuhiro Togano, R. Avigo, M.N. Harakeh, D. Symochko, Hiroyuki Takeda, T. Kubo, Shoko Koyama, D. M. Rossi, M. Shikata, H. Baba, Agnese Giaz, Haik Simon, T. Ozaki, J. L. Rodriguez-Sanchez, P. Doornenbal, David Steppenbeck, Atsumi Saito, I. Syndikus, C. Caesar, M. Heil, Si-Ge Chen, J. A. Tostevin, J. Tsubota, Nagao Kobayashi, Deniz Savran, Yoshiaki Shiga, U. Garg, Marina Petri, N. Nakatsuka, Masafumi Matsushita, Toshiyuki Sumikama, Naohito Inabe, Victor Vaquero, Takashi Nakamura, B. Million, J. Endres, Satoshi Takeuchi, A. Horvat, Y. Shimizu, E. V. Litvinova, K. Yoneda, H. Suzuki, O. Wieland, Rene Reifarth, Hideaki Otsu, H. Wang, Fabia Schindler, Shuichi Ota, Nasser Kalantar-Nayestanaki, M. Nishimura, Thomas Aumann, and N. Fukuda
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Physics ,medicine.anatomical_structure ,Fragmentation (mass spectrometry) ,Astrophysics::High Energy Astrophysical Phenomena ,Excited state ,0103 physical sciences ,Magic (programming) ,medicine ,General Physics and Astronomy ,Atomic physics ,010306 general physics ,01 natural sciences ,Nucleus - Abstract
Spectroscopic factors of neutron-hole and proton-hole states in 131Sn and 131In, respectively, were measured using one-nucleon removal reactions from doubly magic 132Sn at relativistic energies. For 131In, a 2910(50)-keV γ ray was observed for the first time and tentatively assigned to a decay from a 5=2− state at 3275(50) keV to the known 1=2− level at 365 keV. The spectroscopic factors determined for this new excited state and three other single-hole states provide first evidence for a strong fragmentation of singlehole strength in 131Sn and 131In. The experimental results are compared to theoretical calculations based on the relativistic particle-vibration coupling
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32. Spin-dipole nuclear matrix element for the double beta decay of 76Ge by the (3He, t) charge-exchange reaction
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C. Agodi, F Diel, Francesco Cappuzzello, C. A. Douma, M. Holl, M. Fujiwara, Manuela Cavallaro, Daniele Carbone, Yifei Niu, H. Ejiri, Hidetoshi Akimune, Nasser Kalantar-Nayestanaki, G. Gey, Kichiji Hatanaka, Kai Zuber, Atsushi Tamii, A. Inoue, Hisanori Fujita, P. Puppe, F. Hattori, M. Alanssari, K. Heguri, V. Werner, M.N. Harakeh, D. Frekers, P. Ries, Gianluca Colò, Y. Fujita, and Research unit Nuclear & Hadron Physics
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Physics ,Nuclear and High Energy Physics ,Dipole ,Double beta decay ,double beta decay of Ge-76 ,charge-exchange reaction ,Atomic physics ,quenching of axial-vector coupling g(A) ,Nuclear matrix ,Spin (physics) ,Charge exchange ,spin-dipole matrix element - Abstract
Nuclear matrix elements (NMEs) for double beta decays (DBDs) are crucial for studying the neutrino mass and other neutrino properties beyond the standard electro-weak model by measuring neutrino-less DBDs. The spin-dipole (SD) J π = 2- NME is one of the major components associated with the DBD NME. The SD NME for 76Ge was derived for the first time by using the 74,76 Ge (3He, t) at RCNP Osaka. The obtained SD NME for the 76Ge → 76As ground-state transition is in natural units. This is smaller by a coefficient around k ≈ 0.2 with respect to the quasi-particle model NME. The impact of the reduced (quenched) SD NME on DBD neutrino studies is discussed.
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- 2020
33. Experimental study of 4 n with 8He(p,2p) reaction
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M. Böhmer, Masaki Sasano, S. Reichert, Naohito Inabe, S. Chen, T. Shimada, M. Matsumoto, Susumu Shimoura, I. Stefan, J. Kahlbow, N. Kalantar-Nayestanaki, T. Harada, D. Symochko, István Kuti, S. W. Huang, D. Cortina, Tomohiro Uesaka, Z. Ge, N. L. Achouri, Yosuke Kondo, Hiroyuki Takeda, K. Yoneda, B. Fernández-Domínguez, U. Forsberg, Z. Elekes, Roman Gernhäuser, Y. Yasuda, H. Suzuki, Yohei Shimizu, D. Beaumel, D. Kim, C. A. Douma, Yukie Maeda, A. Hirayama, J. M. Gheller, Heiko Scheit, F. Dufter, T. Elidiano, Yasuhiro Togano, M. L. Cortés, M. Potlog, Nobuyuki Chiga, P. J. Li, Juzo Zenihiro, B. Yang, T. Isobe, M. Caamaño, Thomas Aumann, H. T. Törnqvsit, A. Gillibert, D. S. Ahn, F. Schindler, M.N. Harakeh, J. Feng, J. Tscheuschner, S. Kim, Atsumi Saito, L. Zanetti, P. Koseoglou, V. Wagner, M. Parlog, B. M. Godoy, N. Orr, Takashi Nakamura, Yu-xin Liu, J. Mayer, A. Obertelli, Yuya Kubota, Hideaki Otsu, S. Storck, S. Masuoka, K. Boretzky, Kathrin Wimmer, H. Miki, T. Tomai, F. M. Marqués, V. Panin, P. Doornenbal, Stefanos Paschalis, L. Yang, Satoshi Takeuchi, M. A. Knösel, Igor Gašparić, T. Kobayashi, C. Lehr, H. Yang, C. Lenain, M. Miwa, Z. Halász, A. Revel, H. Sato, T. Fujino, D. M. Rossi, H. Baba, S. Park, I. Murray, L. Stuhl, H. Yamada, J. Gibelin, J. Tanaka, Naoki Fukuda, RIKEN Nishina Center for Accelerator-Based Science, German Research Foundation, Federal Ministry of Education and Research (Germany), Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-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), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Grand Accélérateur National d'Ions Lourds (GANIL), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Normandie Université (NU)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), 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), and Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)
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Physics ,Paper ,History ,010308 nuclear & particles physics ,tetraneutron ,nuclear force ,proton knock-out ,radioactive beams ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,01 natural sciences ,Computer Science Applications ,Education ,ddc ,Nuclear physics ,0103 physical sciences ,Tetraneutron ,Neutron ,ddc:530 ,010306 general physics - Abstract
7 pags., 3 figs. -- 27th International Nuclear Physics Conference (INPC2019), The tetraneutron has attracted the attention of nuclear physicists during the past decades, but there is still no unambiguous confirmation of its existence or nonexistence. A new experiment based on 8 He(p,2p)7H{t+4n} reaction, with direct detection of the four neutrons, has been carried out at RIBF, which can hopefully help to draw a definite conclusion on the tetraneutron system., We acknowledge the support of the RIBF accelerator staff and the BigRIPS team for providing the high-quality beam. Z. H. Yang acknowledges the financial support from the Foreign Postdoctoral Researcher program of RIKEN. T. Aumann acknowledges the support by DFG via SFB 1245. P. Koseoglou acknowledges the support from BMBF (NUSTAR.DA grant No.05P 15RDFN1).
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- 2020
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34. Erratum: Precision evaluation of the Ga71(νe,e−) solar neutrino capture rate from the ( He3,t ) charge-exchange reaction [Phys. Rev. C 91 , 034608 (2015)]
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V. N. Gavrin, C. Iwamoto, Hidetoshi Akimune, Atsushi Tamii, M. Alanssari, M. Fujiwara, B. T. Cleveland, M.N. Harakeh, Takatoshi Suzuki, D. Frekers, H. Okamura, A. Okamoto, Kichiji Hatanaka, A. Lennarz, Y. Fujita, H. Ejiri, M. Holl, Hisanori Fujita, T. Adachi, and B. A. Brown
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Nuclear physics ,Physics ,Solar neutrino ,Charge exchange - Published
- 2019
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35. Measurement of the $\gamma$ Decay from the Energy Region of the Pygmy Dipole States Excited in the $^{208}$Pb$(p,p'\gamma )$ Reaction at CCB
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M. Matejska-Minda, Piotr Pawłowski, P. J. Napiorkowski, A. Bracco, M. Zieblinski, J. Grebosz, Y. Sobolev, B. Wasilewska, M. Kmiecik, S. Brambilla, P. Bednarczyk, F. C. L. Crespi, N. Cieplicka-Oryńczak, M. Krzysiek, M. Ciemala, J. Łukasik, K. Mazurek, A. Maj, K. Guguła, Izabela Ciepał, M. Lewitowicz, Ch. Schmitt, M.N. Harakeh, B. Sowicki, B. Fornal, M. Jeżabek, M. Kicińska-Habior, P. Kulessa, Grand Accélérateur National d'Ions Lourds (GANIL), Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut Pluridisciplinaire Hubert Curien (IPHC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université de Strasbourg (UNISTRA)-Centre National de la Recherche Scientifique (CNRS), Research unit Nuclear & Hadron Physics, Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), and Université de Strasbourg (UNISTRA)-Université de Haute-Alsace (UHA) Mulhouse - Colmar (Université de Haute-Alsace (UHA))-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
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Physics ,010308 nuclear & particles physics ,Cyclotron ,Nuclear structure ,Gamma ray ,General Physics and Astronomy ,Scintillator ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,01 natural sciences ,7. Clean energy ,Spectral line ,law.invention ,Nuclear physics ,Dipole ,law ,Excited state ,0103 physical sciences ,Nuclear Experiment - Abstract
International audience; For a few years, the medical cyclotron Proteus C-235 at the Cyclotron Centre Bronowice in Kraków, Poland has been regularly used for nuclear structure experiments. One of the ongoing studies is focused on the γ decay of collective states populated in (p, p0γ) reactions. In a recent experiment, γ decays of excited states in the energy region of the Pygmy Dipole States in 208Pb have been observed. Good efficiency and energy resolution provided by the PARIS clusters and LaBr3:Ce scintillators facilitate a comparison of the obtained energy spectra with previous measurements of pygmy states in this nucleus.
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- 2019
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36. SPECTROSCOPY OF NEUTRON-RICH C, O, N AND F ISOTOPES WITH THE AGATA plus PARIS plus VAMOS SETUP AT GANIL
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S. Ziliani, M. Ciemała, F. Crespi, S. Leoni, B. Fornal, A. Maj, P. Bednarczyk, G. Benzoni, A. Bracco, C. Boiano, S. Bottoni, S. Brambilla, M. Bast, M. Beckers, T. Braunroth, F. Camera, N. Cieplicka-Oryńczak, E. Clément, O. Dorvaux, S. Erturk, G. De France, A. Goldkuhle, J. Grębosz, M.N. Harakeh, Ł.W. Iskra, B. Jacquot, M. Kicińska-Habior, Y. Kim, M. Kmiecik, A. Lemasson, H. Li, I. Matea, K. Mazurek, C. Michelagnoli, B. Million, C. Müller-Gatermann, P. Napiorkowski, V. Nanal, M. Matejska-Minda, M. Rejmund, Ch. Schmitt, M. Stanoiu, I. Stefan, B. Wasilewska, M. Ziębliński, Fornal, Bogdan -- 0000-0002-1142-8067, Ciemala, Michal -- 0000-0001-5328-720X, [Ziliani, S. -- Crespi, F. -- Leoni, S. -- Bracco, A. -- Bottoni, S. -- Camera, F.] Univ Milan, Milan, Italy -- [Ziliani, S. -- Crespi, F. -- Leoni, S. -- Benzoni, G. -- Bracco, A. -- Boiano, C. -- Bottoni, S. -- Brambilla, S. -- Camera, F. -- Million, B.] INFN, Sez Milano, Milan, Italy -- [Ciemala, M. -- Fornal, B. -- Maj, A. -- Bednarczyk, P. -- Cieplicka-Orynczak, N. -- Grebosz, J. -- Iskra, L. W. -- Kmiecik, M. -- Mazurek, K. -- Wasilewska, B.] Polish Acad Sci, Inst Nucl Phys, Krakow, Poland -- [Bast, M. -- Beckers, M. -- Braunroth, T. -- Goldkuhle, A. -- Mueller-Gatermann, C.] IKP Cologne, Cologne, Germany -- [Clement, E. -- De France, G. -- Jacquot, B. -- Kim, Y. -- Lemasson, A. -- Li, H. -- Rejmund, M.] CEA, DSAM, GANIL, Caen, France -- [Clement, E. -- De France, G. -- Jacquot, B. -- Kim, Y. -- Lemasson, A. -- Li, H. -- Rejmund, M.] CNRS, IN2P3, Caen, France -- [Dorvaux, O. -- Schmitt, Ch] CNRS, IN2P3, IPHC UMR 7178, Strasbourg, France -- [Erturk, S.] Nigde Univ, Nigde, Turkey -- [Harakeh, M. N.] KVI Ctr Adv Radiat Technol, Groningen, Netherlands -- [Kicinska-Habior, M. -- Matea, I -- Stefan, I] Warsaw Univ, Fac Phys, Warsaw, Poland -- [Kicinska-Habior, M. -- Matea, I -- Stefan, I] IPN, Orsay Lab, Orsay, France -- [Michelagnoli, C.] ILL Grenoble, Grenoble, France -- [Napiorkowski, P. -- Matejska-Minda, M.] Univ Warsaw, Heavy Ion Lab, Warsaw, Poland -- [Nanal, V] Dept Nucl & Atom Phys, Mumbai, Maharashtra, India -- [Stanoiu, M.] IFIN HH, Bucharest, Romania -- [Zieblinski, M.] CEA, DRF, IRFU, Ctr CEA Saclay, Saclay, France, Grand Accélérateur National d'Ions Lourds (GANIL), Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut Pluridisciplinaire Hubert Curien (IPHC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université de Strasbourg (UNISTRA)-Centre National de la Recherche Scientifique (CNRS), 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 Laue-Langevin (ILL), ILL, Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Université de Strasbourg (UNISTRA)-Centre National de la Recherche Scientifique (CNRS), 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), 0-Belirlenecek, and Université de Strasbourg (UNISTRA)-Université de Haute-Alsace (UHA) Mulhouse - Colmar (Université de Haute-Alsace (UHA))-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
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Physics ,Isotope ,Spectrometer ,010308 nuclear & particles physics ,General Physics and Astronomy ,Context (language use) ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,7. Clean energy ,01 natural sciences ,0-Belirlenecek ,Nuclear physics ,Nuclear interaction ,Ab initio quantum chemistry methods ,0103 physical sciences ,Neutron ,AGATA ,Spectroscopy ,Nuclear Experiment - Abstract
Zakopane Conference on Nuclear Physics - Extremes of the Nuclear Landscape -- AUG 26-SEP 02, 2018 -- Zakopane, POLAND, WOS: 000463866500052, Recent ab initio calculations pointed out the importance of the three-body terms of the nuclear interaction, in the description of the structure of n-rich systems. The state lifetimes in light n-rich carbon and oxygen nuclei have been predicted to be sensitive to the three-body terms and, in this context, an experiment, aiming at the measurement of these lifetimes, was performed in GANIL in July 2017 with the AGATA and PARIS arrays coupled to the VAMOS++ magnetic spectrometer. Details on the AGATA preliminary data analysis are presented., National Science Centre, Poland (NCN) [2013/08/M/ST2/00257, 2014/14/M/ST2/00738, 2016/22/M/ST2/00269], This work was supported by the National Science Centre, Poland (NCN) under contracts No. 2013/08/M/ST2/00257, 2014/14/M/ST2/00738 and 2016/22/M/ST2/00269.
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- 2019
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37. Nuclear Breakup and Coulomb Dissociation of $^{9}$C Nucleus Studied at RIBF RIKEN
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Livius Trache, H. Baba, M.N. Harakeh, H. N. Liu, H. Takeda, F. M. Marques, Zoltán Halász, T. Isobe, H. Murakami, H. Otsu, J. Zenihiro, D. H. Kim, M. Sasano, S. Y. Park, Z. Yang, I. C. Stefanescu, D. Tudor, T. Motobayashi, Masahiro Yasuda, A. E. Spiridon, A. N. Petrovici, Y. L. Sun, Takashi Nakamura, Naoki Fukuda, Y. Kubota, K. Yoneda, Masanori Nishimura, Y. Shimizu, T. Uesaka, Yasuhiro Togano, P. J. Li, A. Kurihara, K. Y. Chae, H. Suzuki, D. S. Ahn, A. I. Chilug, T. Kobayashi, J. Gibelin, Shuichi Ota, I. S. Hahn, L. Stuhl, F. Carstoiu, N. T. Zhang, Z. Elekes, Antti Saastamoinen, H. Sato, G. G. Kiss, T. Harada, V. Panin, Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), and Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
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Physics ,Hydrogen ,Explosive material ,010308 nuclear & particles physics ,chemistry.chemical_element ,Inverse ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,Breakup ,01 natural sciences ,7. Clean energy ,Dissociation (chemistry) ,Nuclear physics ,chemistry ,0103 physical sciences ,Radiative transfer ,Coulomb ,010306 general physics ,[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph] ,Mass gap - Abstract
International audience; The 9C breakup was studied during the SAMURAI29R1 experiment through inclusive and exclusive measurements at energies around 160 AMeV for 9C, in order to evaluate the astrophysical S18 factor for the inverse process 8B(p,γ)9C at energies in the region of astrophysical interest. The radiative proton capture on 8B is important in the hot pp chains, in explosive Hydrogen burning (ppIV and rapI), at temperatures between 0.05 < T9 < 1 K, as possible alternative paths across the A = 8 mass gap. Another goal of this experiment was a detailed study of the breakup reaction mechanism. During the experiment the nuclear breakup process was studied using a natural C target with 425 µm thickness and the Coulomb dissociation by using a natural Pb target with 150 µm thickness. The reaction products were tracked simultaneously using a system of position sensitive Si detectors and in total 1024 output channels were read out by using new dual gain preamplifiers (DGP) specially designed for the experiments of the HI-p collaboration. The SAMURAI29R1 experiment was carried out during the SAMURAI 18Oxygen 2018 Spring campaign and it is part of the HI-p collaboration together with another three experiments. Performances of the setup used and first results of the analysis are presented.
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- 2018
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38. Determination of Lifetimes of Excited States in Neutron-rich $^{20}$O Isotope from Experiment with the AGATA+PARIS+VAMOS Setup
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M. Ciemała, S. Ziliani, F. Crespi, S. Leoni, B. Fornal, A. Maj, P. Bednarczyk, G. Benzoni, A. Bracco, C. Boiano, S. Bottoni, S. Brambilla, M. Bast, M. Beckers, T. Braunroth, F. Camera, N. Cieplicka-Oryńczak, E. Clément, O. Dorvaux, S. Ertürk, G. De France, A. Goldkuhle, J. Grębosz, M.N. Harakeh, Ł.W. Iskra, B. Jacquot, A. Karpov, M. Kicińska-Habior, Y. Kim, M. Kmiecik, A. Lemasson, H. Li, I. Matea, K. Mazurek, C. Michelagnoli, B. Millon, C. Müller-Gatermann, P. Napiorkowski, V. Nanal, M. Matejska-Minda, M. Rejmund, B. Sowicki, Ch. Schmitt, M. Stanoiu, I. Stefan, B. Wasilewska, M. Zielińska, M. Ziębliński, Grand Accélérateur National d'Ions Lourds (GANIL), Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut Pluridisciplinaire Hubert Curien (IPHC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université de Strasbourg (UNISTRA)-Centre National de la Recherche Scientifique (CNRS), 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 Laue-Langevin (ILL), ILL, Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Université de Strasbourg (UNISTRA)-Université de Haute-Alsace (UHA) Mulhouse - Colmar (Université de Haute-Alsace (UHA))-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), 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 Université de Strasbourg (UNISTRA)-Centre National de la Recherche Scientifique (CNRS)
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Physics ,Isotope ,010308 nuclear & particles physics ,Nuclear Theory ,General Physics and Astronomy ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,01 natural sciences ,7. Clean energy ,Nuclear physics ,Excited state ,0103 physical sciences ,AGATA ,Neutron ,Nuclear Experiment - Abstract
International audience; An experiment aiming at measuring lifetimes of the second 2+ excited states in neutron-rich C and O isotopes was recently performed at the GANIL laboratory, in France. In these nuclei, recent ab initio calculations provide a detailed description of the nuclear excited states, predicting a strong sensitivity of the electromagnetic transition probabilities to the details of the nucleon–nucleon interactions, especially in connection with the role played by the three-body (NNN) forces. Thus, the measurement of 2 + states lifetimes in this region will be a stringent test of the importance of including the NNN forces in describing the electromagnetic properties of selected nuclear states. This contribution reports on the status of the experimental analysis for the case of lifetimes in 20O.
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- 2018
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39. Study of the $^9$C breakup through NP1412-SAMURAI29R1 experiment
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H. Takeda, T. Motobayashi, Livius Trache, Julien Gibelin, S. Park, T. Isobe, G. Kiss, D. Tudor, K. Yoneda, A. I. Chilug, Hideaki Otsu, Shinsuke Ota, H. Baba, F. M. Marques, A. Kurihara, M.N. Harakeh, H. Sato, N. Zhang, H. Suzuki, Naoki Fukuda, Masahiro Yasuda, Z. Elekes, Yuya Kubota, D. S. Ahn, I. C. Stefanescu, H. N. Liu, T. Harada, Zaihong Yang, L. Stuhl, J. Zenihiro, D. Kim, Masaki Sasano, I. S. Hahn, Antti Saastamoinen, H. Murakami, Toshio Kobayashi, Tomohiro Uesaka, P. J. Li, Y. Shimizu, Yasuhiro Togano, Y. L. Sun, T. Nakamura, V. Panin, K. Y. Chae, Z. Halasz, A. Spiridon, 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
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Physics ,Proton–proton chain reaction ,Proton ,010308 nuclear & particles physics ,Monte Carlo method ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,Breakup ,7. Clean energy ,01 natural sciences ,Nuclear physics ,Reaction rate ,Nucleosynthesis ,0103 physical sciences ,Coulomb ,Radiative transfer ,010306 general physics ,Nuclear Experiment - Abstract
International audience; The 9C breakup reaction was investigated in order to obtain information about the inverse reaction: 8B(p,γ)9C at astro-physical energies within the NP1412SAMURAI29R1 experiment. The 8B(p,γ)9C reaction gives a possible path to the hot pp chain pp-IV at high temperatures and away from it toward a rapid alpha-process rap-I at high temperatures and densities and therefore is important in understanding nucleosynthesis in super-massive hot stars in the early universe, including possible bypass of the 3α-process. For this experiment it was proposed to use a combination of nuclear and Coulomb dissociation measurements (on a light target Be or C and on a heavy target Pb, respectively) at energy of 160 A MeV to extract structure information, which will allow to evaluate the radiative proton capture cross section at low energies and from there the reaction rate. The current work is focused on the development of Monte Carlo simulations for Coulomb breakup mechanism of 9C as well as on the Geant4 simulations of the resulting particle trajectories through the experimental setup, including passage of the particles through the magnetic field of the SAMURAI spectrometer.
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- 2018
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40. Observation of isoscalar multipole strengths in exotic doubly-magic 56Ni in inelastic α scattering in inverse kinematics
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N.L. Achouri, Marine Vandebrouck, S. Damoy, Elias Khan, H. Bouzomita, M. Fujiwara, K. Mazurek, L. Caceres, J. F. Libin, J. Van de Walle, M. Caamaño, U. Garg, S. M. Lukyanov, H. Savajols, A. Krasznahorkay, J. Pancin, K. Boretzky, B. Bastin, S. Bagchi, G. F. Grinyer, G. Lhoutellier, C. Stodel, Riccardo Raabe, L. Suen, J. Gibelin, Nasser Kalantar-Nayestanaki, Catherine Rigollet, Hidetoshi Akimune, S. Sambi, J. C. Thomas, O. Kamalou, L. Perrot, M. A. Najafi, T. Roger, M. Senoville, F. Delaunay, B. Fernández-Domínguez, Y. E. Penionzhkevich, M.N. Harakeh, Universidade de Santiago de Compostela. Departamento de Física de Partículas, KVI-CART, University of Groningen, University of Groningen [Groningen], Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Grand Accélérateur National d'Ions Lourds (GANIL), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Universidade de Santiago de Compostela [Spain] (USC ), 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), Institute for Nuclear Research [Budapest] (ATOMKI), Hungarian Academy of Sciences (MTA), Flerov Laboratory of Nuclear Reactions [Dubna] (FLNR), Joint Institute for Nuclear Research (JINR), Instituut voor Kern-en Stralingsfysica (IKS), Catholic University of Leuven - Katholieke Universiteit Leuven (KU Leuven), GANILEXP, Normandie Université (NU)-Centre National de la Recherche Scientifique (CNRS)-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)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), 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), and Research unit Nuclear & Hadron Physics
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Nuclear and High Energy Physics ,Isoscalar ,ACTIVE TARGET ,Nuclear Theory ,Magnetic monopole ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,Resonance (particle physics) ,NUCLEAR INCOMPRESSIBILITY ,Nuclear physics ,ENERGY ,ddc:530 ,Nuclear Experiment ,Physics ,Inverse kinematics ,Isotope ,Scattering ,BEAMS ,lcsh:QC1-999 ,3. Good health ,Dipole ,ISOTOPES ,DIPOLE RESONANCE ,Atomic physics ,Multipole expansion ,MATTER ,lcsh:Physics - Abstract
The Isoscalar Giant Monopole Resonance (ISGMR) and the Isoscalar Giant Dipole Resonance (ISGDR) compression modes have been studied in the doubly-magic unstable nucleus 56Ni. They were measured by inelastic α-particle scattering in inverse kinematics at 50MeV/u with the MAYA active target at the GANIL facility. The centroid of the ISGMR has been obtained at Ex=19.1 ±0.5MeV. Evidence for the low-lying part of the ISGDR has been found at Ex=17.4 ±0.7MeV. The strength distribution for the dipole mode shows similarity with the prediction from the Hartree–Fock (HF) based random-phase approximation (RPA)[1]. These measurements confirm inelastic α-particle scattering as a suitable probe for exciting the ISGMR and the ISGDR modes in radioactive isotopes in inverse kinematics This work was supported by the European Commission within the Seventh Framework Programme through IA-ENSAR (contract No. RII3-CT-2010-262010) and GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany, and the United States National Science Foundation (Grants Number PHY-1068192 and PHY-1419765) SI
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- 2015
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41. Missing-mass spectroscopy of the C12(p,d) reaction near the η′ -meson production threshold
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R. Knöbel, J. Zhao, Hans Geissel, Yasumoto Tanaka, Daisuke Jido, V. Metag, J. S. Winfield, H. Yamakami, J. Gellanki, C. Scheidenberger, M. Takechi, Y. Igarashi, Hooi Jin Ong, Imrich Szarka, C. Rappold, Yassid Ayyad, C. Guo, M. Iwasaki, Peter Strmen, Christine Hornung, Ryugo S. Hayano, K. Itahashi, R. Kanungo, Isao Tanihata, M.N. Harakeh, S. Terashima, Moritz P. Reiter, J. L. Rodriguez-Sanchez, N. Ikeno, E. Haettner, E. Widmann, Satoru Hirenzaki, E. Gutz, T. Nishi, X. Xu, Yuni N. Watanabe, S. Friedrich, K.-T. Brinkmann, Helmut Weick, Herbert A. Simon, Nasser Kalantar-Nayestanaki, I. G. Mukha, Y. Higashi, Bao-Hua Sun, Hideko Nagahiro, Ken Suzuki, Branislav Sitar, N. Kurz, J. Benlliure, Mariana Nanova, S. Pietri, Tomofumi Nagae, A. Prochazka, and Hiroyuki Fujioka
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Physics ,010308 nuclear & particles physics ,Nuclear Theory ,Momentum transfer ,Eta meson ,Mass spectrometry ,01 natural sciences ,Particle identification ,Spectral line ,Nuclear physics ,Deuterium ,0103 physical sciences ,Bound state ,Atomic physics ,Nuclear Experiment ,010306 general physics ,Spectroscopy - Abstract
Excitation-energy spectra of $^{11}\mathrm{C}$ nuclei near the ${\ensuremath{\eta}}^{\ensuremath{'}}$-meson production threshold have been measured by missing-mass spectroscopy using the $^{12}\mathrm{C}(p,d)$ reaction. A carbon target has been irradiated with a 2.5 GeV proton beam supplied by the synchrotron SIS-18 at GSI to produce ${\ensuremath{\eta}}^{\ensuremath{'}}$-meson bound states in $^{11}\mathrm{C}$ nuclei. Deuterons emitted at ${0}^{\ensuremath{\circ}}$ in the reaction have been momentum analyzed by the fragment separator (FRS), used as a high-resolution spectrometer. No distinct structure due to the formation of ${\ensuremath{\eta}}^{\ensuremath{'}}$-mesic states is observed although a high statistical sensitivity is achieved in the experimental spectra. Upper limits on the formation cross sections of ${\ensuremath{\eta}}^{\ensuremath{'}}$-mesic states are determined, and thereby a constraint imposed on the ${\ensuremath{\eta}}^{\ensuremath{'}}$-nucleus interaction is discussed.
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- 2018
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42. Nuclear-matter radius studies from Ni58(α,α) experiments at the GSI Experimental Storage Ring with the EXL facility
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Hans Geissel, Tatsuya Furuno, Santosh Roy, C. Dimopoulou, U. Popp, J. S. Winfield, Takayuki Yamaguchi, Iris Dillmann, F. Nolden, M. Csatlós, Yu. A. Litvinov, Peter Egelhof, M. Kuilman, M.N. Harakeh, D. Nagae, B. Streicher, P. J. Woods, Th. Kroell, M. Steck, H. Kollmus, S. Boenig, L. Stuhl, O. Kiselev, M. A. Najafi, Juzo Zenihiro, M. Thuerauf, Tomohiro Uesaka, C. Scheidenberger, C. Nociforo, Nasser Kalantar-Nayestanaki, Thomas Aumann, K. Yue, A.-L. Hartig, Catherine Rigollet, S. Ilieva, C. Kozhuharov, Helmut Weick, M. Mahjour-Shafiei, S. Bagchi, J. C. Zamora, Danyal Winters, V. K. Eremin, Sergey Litvinov, A. Krasznahorkay, M. von Schmid, Manfred Mutterer, and Roman Gernhaeuser
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Nuclear reaction ,Physics ,Elastic scattering ,010308 nuclear & particles physics ,chemistry.chemical_element ,Radius ,Nuclear matter ,01 natural sciences ,Eikonal approximation ,Ion ,Nuclear physics ,chemistry ,0103 physical sciences ,010306 general physics ,Helium ,Storage ring - Abstract
A novel method for measuring nuclear reactions in inverse kinematics with stored ion beams was successfully used to extract the nuclear-matter radius of $^{58}\mathrm{Ni}$. The experiment was performed at the experimental heavy-ion storage ring at the GSI facility using a stored $^{58}\mathrm{Ni}$ beam at energies of 100 and 150 MeV/u and an internal helium gas-jet target. Elastically scattered $\ensuremath{\alpha}$-recoils at low momentum transfers were measured with an in-ring detector system compatible with ultrahigh vacuum. Experimental angular distributions were fitted using density-dependent optical model potentials within the eikonal approximation. This permitted the extraction of the point-matter root-mean-square radius of $^{58}\mathrm{Ni}$ with an average value of 3.70(7) fm. Results from this work are in good agreement with several experiments performed in the past in normal kinematics. This pioneering experiment demonstrates a major breakthrough towards future investigations with far-from-stability stored beams using the present technique.
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- 2017
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43. Cluster Structure of $^9$Be by Scattering of Deuterons
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V. Burjan, J. Mrazek, V. Kroha, Wladyslaw Henryk Trzaska, D. Verney, K. Mendibayev, Š. Piskoř, M. A. Naumenko, I. Stefan, I. Siváček, D. Etasse, T. Zholdyvayev, N. K. Skobelev, V. Glagolev, M.N. Harakeh, Yu. E. Penionzhkevich, S. M. Lukyanov, A. S. Denikin, Kairat Kuterbekov, Laboratoire de physique corpusculaire de Caen (LPCC), Université de Caen Normandie (UNICAEN), Normandie Université (NU)-Normandie Université (NU)-École Nationale Supérieure d'Ingénieurs de Caen (ENSICAEN), Normandie Université (NU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-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), Laboratoire de physique corpusculaire de Caen ( LPCC ), Université de Caen Normandie ( UNICAEN ), Normandie Université ( NU ) -Normandie Université ( NU ) -Ecole Nationale Supérieure d'Ingénieurs de Caen ( ENSICAEN ), Normandie Université ( NU ) -Institut National de Physique Nucléaire et de Physique des Particules du CNRS ( IN2P3 ) -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 ), Normandie Université (NU)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), 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)
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Physics ,History ,rakenne ,010308 nuclear & particles physics ,Scattering ,Structure (category theory) ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,01 natural sciences ,Molecular physics ,Computer Science Applications ,Education ,klusterit ,Deuterium ,0103 physical sciences ,Cluster (physics) ,sironta ,structure ,[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex] ,010306 general physics - Abstract
International audience; Angular distributions of protons, deuterons, tritons and alpha particles emitted in the reaction 2H+9Be at Elab=19.5 MeV were measured with an aim to shed light on the internal cluster structure of 9Be and to study possible cluster transfer of 5He. The analyses suggest a significant contribution of five-nucleon transfer in the reaction channel 9Be(d,4He)7Li.
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- 2017
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44. Search for η′ Mesic Nuclei in GSI/FAIR
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Yasumoto Tanaka, Y. Higashi, E. Widmann, H. Fujioka, Christine Hornung, M. Takechi, Y. Igarashi, I. G. Mukha, Ken Suzuki, Yuni N. Watanabe, N. Ikeno, Satoru Hirenzaki, Peter Strmen, S. Pietri, K.-T. Brinkmann, S. Friedrich, C. Guo, Hans Geissel, Moritz P. Reiter, Nasser Kalantar-Nayestanaki, E. Haettner, Isao Tanihata, M. Iwasaki, T. Nishi, Helmut Weick, J. Zhao, A. Prochazka, X. Xu, E. Gutz, Hooi Jin Ong, J. Benlliure, Tomofumi Nagae, J. Gellanki, Ryugo S. Hayano, V. Metag, J. S. Winfield, H. Yamakami, C. Scheidenberger, R. Knoebel, R. Kanungo, Mariana Nanova, Daisuke Jido, Bao-Hua Sun, Hideko Nagahiro, K. Itahashi, Yassid Ayyad, M.N. Harakeh, S. Terashima, Branislav Sitar, Imrich Szarka, C. Rappold, N. Kurz, Herbert A. Simon, and J. L. Rodriguez-Sanchez
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Physics ,Nuclear physics ,Meson ,chemistry ,chemistry.chemical_element ,Anomaly (physics) ,Nuclear matter ,Carbon - Published
- 2017
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45. Observation of the Isovector Giant Monopole Resonance via the Si28(Be10,B*10[1.74 MeV]) Reaction at 100 AMeV
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Sam M. Austin, C. M. Campbell, Shumpei Noji, C. Morse, C. Loelius, U. Garg, M. Bowry, S. Lipschutz, B. A. Brown, Remco Zegers, C. Sullivan, D. Weisshaar, E. Lunderberg, T. Redpath, C. Robin, Yoshiko Sasamoto, E. Kwan, M.N. Harakeh, Hideyuki Sakai, C. Langer, Masaki Sasano, G. Perdikakis, S. Gales, Elena Litvinova, M. Scott, J. A. Tostevin, Daniel Bazin, Alexandra Gade, Tomohiro Uesaka, and R.M. Almus
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Physics ,Isovector ,010308 nuclear & particles physics ,Nuclear Theory ,Cyclotron ,Magnetic monopole ,General Physics and Astronomy ,Resonance ,Nuclear matter ,01 natural sciences ,7. Clean energy ,law.invention ,Nuclear physics ,Dipole ,law ,0103 physical sciences ,Atomic physics ,Born approximation ,Nuclear Experiment ,010306 general physics ,Excitation - Abstract
The (10Be,10B [1.74 MeV]) charge-exchange reaction at 100 AMeV is presented as a new probe for isolating the isovector (ΔT = 1) non-spin-transfer (ΔS = 0) response of nuclei, with 28Si being the rst nucleus studied. By using a secondary 10Be beam produced by fast fragmentation of 18O nuclei at the NSCL Coupled Cyclotron Facility, applying the dispersion-matching technique with the S800 magnetic spectrometer to determine the excitation energy in 28Al, and performing high- resolution -ray tracking with the Gamma-Ray Energy Tracking Array (GRETINA) to identify the 1022-keV ray associated with the decay from the 1.74-MeV T = 1 isobaric analog state in 10B, a ΔS = 0 excitation-energy spectrum in 28Al was extracted. Monopole and dipole contributions were determined through a multipole-decomposition analysis, and the isovector giant dipole (IVGDR) and monopole (IVGMR) resonances were identi ed. The results show that this probe is a powerful tool for studying the elusive IVGMR, which is of interest for performing stringent tests of modern density functional theories at high excitation energies and for constraining the bulk properties of nuclei and nuclear matter. The extracted distributions were compared with theoretical calculations based on the normal-modes formalism and the proton-neutron relativistic time-blocking approximation. Calculated cross sections based on these strengths underestimate the data by about a factor of two, which likely indicates de ciencies in the reaction calculations based on the distorted wave Born approximation.
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- 2017
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46. Spectroscopy of $\eta ^{\prime }$-mesic Nuclei with WASA at GSI/FAIR
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M. Iwasaki, H. Fujioka, Hans Geissel, Satoru Hirenzaki, C. Guo, R. Knöbel, E. Haettner, V. Metag, Christine Hornung, Imrich Szarka, C. Rappold, J. Benlliure, Frank Goldenbaum, Timo Dickel, Yasumoto Tanaka, R. Ruber, James Ritman, Tomofumi Nagae, K. Itahashi, Paweł Moskal, J. L. Rodriguez-Sanchez, J. Zhao, Oleksandr Rundel, S. Pietri, Y. Igarashi, N. Kuzminchuk, Hooi Jin Ong, A. Yamamoto, N. Ikeno, Helmut Weick, Bao-Hua Sun, V. Serdyuk, V. Drozd, Y. Ma, S.Y. Matsumoto, Hideko Nagahiro, M. Takechi, Herbert A. Simon, Bettina Lommel, S. Minami, R. Kanungo, Nasser Kalantar-Nayestanaki, Isao Tanihata, A. Prochazka, Daisuke Jido, M. Nakagawa, Magdalena Skurzok, T.R. Saito, Branislav Sitar, Ryugo S. Hayano, W. R. Plass, N. Kurz, R. Sekiya, Birgit Kindler, Haruhiko Outa, M.N. Harakeh, S. Terashima, I. G. Mukha, S. Purushothaman, C. Scheidenberger, S. Bagchi, D. Kostyleva, Peter Strmen, and Hiroyuki Ekawa
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Physics ,Proton ,Meson ,010308 nuclear & particles physics ,Detector ,General Physics and Astronomy ,01 natural sciences ,Prime (order theory) ,Nuclear physics ,Deuterium ,0103 physical sciences ,ddc:530 ,010306 general physics ,Spectroscopy ,Beam (structure) - Abstract
Acta physica Polonica / B Particle physics and field theory, nuclear physics, theory of relativity 51(1), 39 (2020). doi:10.5506/APhysPolB.51.39, Published by Inst. of Physics, Jagellonian Univ., Cracow
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- 2020
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47. Penning-trap Q-value determination of the Ga71(ν,e−)Ge71 reaction using threshold charge breeding of on-line produced isotopes
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J. R. Crespo López-Urrutia, M. Luichtl, F. Jang, B.E. Schultz, Jens Dilling, T. Brunner, P. P. J. Delheij, M.C. Simon, E. Mané, Aaron Gallant, S. Ettenauer, A. Grossheim, H. Ejiri, D. Robertson, J.C. Bale, A. Teigelhöfer, Maxime Brodeur, U. Chowdhury, A. Chaudhuri, A. Lennarz, Corina Andreoiu, J. Lassen, T. Ma, M.N. Harakeh, D. Frekers, A.A. Kwiatkowski, V. N. Gavrin, T.D. Macdonald, and Vanessa V. Simon
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Physics ,Nuclear and High Energy Physics ,010308 nuclear & particles physics ,Q value ,Nuclear structure ,Penning trap ,7. Clean energy ,01 natural sciences ,Ionization ,Excited state ,0103 physical sciences ,Isobar ,Ion trap ,GALLEX ,Atomic physics ,010306 general physics - Abstract
We present a first direct Q -value measurement of the Ga 71 ( ν , e − ) Ge 71 reaction using the TITAN mass-measurement facility at ISAC/TRIUMF. The measurements were performed in a Penning trap on neon-like 71 Ga 21+ and 71 Ge 22+ using isobar separation of the on-line produced mother and daughter nuclei through threshold charge breeding in an electron-beam ion trap. In addition, isoionic samples of 71 Ga 21+ and 71 Ge 21+ were stored concurrently in the Penning trap and provided a separate Q -value measurement. Both independent measurements result in a combined Q -value of 233.5 ± 1.2 keV , which is in agreement with the previously accepted Q -value for the ν cross-section calculations. Together with a recent measurement of the ν -response from the excited states in 71 Ge, we conclude that there are no further uncertainties in the nuclear structure, which could remove the persistent discrepancy between the SAGE and GALLEX calibration measurements performed with neutrinos from reactor-produced 51 Cr and 37 Ar sources and the theoretical expectation.
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- 2013
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48. Measurement of Excitation Spectra in the C12(p,d) Reaction near the η′ Emission Threshold
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Helmut Weick, Y. Higashi, H. Fujioka, Satoru Hirenzaki, J. Zhao, A. Prochazka, E. Widmann, Ken Suzuki, S. Friedrich, Nasser Kalantar-Nayestanaki, R. Knöbel, X. Xu, S. Pietri, Herbert A. Simon, V. Metag, J. Gellanki, K. Itahashi, Imrich Szarka, C. Rappold, Christine Hornung, J. S. Winfield, Isao Tanihata, Rituparna Kanungo, E. Haettner, Daisuke Jido, M.N. Harakeh, Satoru Terashima, Moritz P. Reiter, J. L. Rodriguez-Sanchez, Mariana Nanova, Yasumoto Tanaka, M. Iwasaki, H. Yamakami, T. Nishi, Bao-Hua Sun, Hideko Nagahiro, Yassid Ayyad, E. Gutz, I. G. Mukha, Hooi Jin Ong, Tomofumi Nagae, Yuni N. Watanabe, N. Ikeno, K.-T. Brinkmann, Y. Igarashi, Maya Takechi, Hans Geissel, Branislav Sitar, N. Kurz, C. Guo, Ryugo S. Hayano, C. Scheidenberger, J. Benlliure, and Peter Strmen
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Physics ,Spectrometer ,Proton ,010308 nuclear & particles physics ,Nuclear Theory ,General Physics and Astronomy ,chemistry.chemical_element ,01 natural sciences ,Spectral line ,Synchrotron ,law.invention ,chemistry ,Deuterium ,law ,0103 physical sciences ,Bound state ,Atomic physics ,Nuclear Experiment ,010306 general physics ,Carbon ,Beam (structure) - Abstract
Excitation spectra of ^{11}C are measured in the ^{12}C(p,d) reaction near the η^{'} emission threshold. A proton beam extracted from the synchrotron SIS-18 at GSI with an incident energy of 2.5 GeV impinges on a carbon target. The momenta of deuterons emitted at 0° are precisely measured with the fragment separator (FRS) operated as a spectrometer. In contrast to theoretical predictions on the possible existence of deeply bound η^{'}-mesic states in carbon nuclei, no distinct structures are observed associated with the formation of bound states. The spectra are analyzed to set stringent constraints on the formation cross section and on the hitherto barely known η^{'}-nucleus interaction.
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- 2016
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49. Are There Nuclear Structure Effects on the Isoscalar Giant Monopole Resonance and Nuclear Incompressibility near A~90?
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M. Fujiwara, Yohei Matsuda, S. Ando, Takahiro Kawabata, Nasser Kalantar-Nayestanaki, Masatoshi Itoh, T. Nakahara, C. Iwamoto, J. T. Matta, S. Adachi, A. Uchiyama, U. Garg, K. B. Howard, Tatsuya Furuno, Y. K. Gupta, Hidetoshi Akimune, M. Tsumura, Atsushi Tamii, Takatoshi Aoki, C. Kadono, M. Şenyiğit, M.N. Harakeh, and Research unit Nuclear & Hadron Physics
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Nuclear and High Energy Physics ,Isoscalar ,Nuclear Theory ,Magnetic monopole ,FOS: Physical sciences ,01 natural sciences ,7. Clean energy ,Resonance (particle physics) ,Spectral line ,COUPLED-CHANNELS CALCULATIONS ,Nuclear physics ,DEFORMATION ,0103 physical sciences ,STRENGTH ,SCATTERING ,Nuclear Experiment (nucl-ex) ,010306 general physics ,Nuclear Experiment ,Physics ,010308 nuclear & particles physics ,Scattering ,Nuclear structure ,CONSTRAINTS ,SYMMETRY ENERGY ,lcsh:QC1-999 ,STATE ,DIPOLE RESONANCE ,PB-208 ,Atomic physics ,Beam energy ,MATTER ,lcsh:Physics - Abstract
"Background-free" spectra of inelastic $\alpha$-particle scattering have been measured at a beam energy of 385 MeV in $^{90, 92}$Zr and $^{92}$Mo at extremely forward angles, including 0$^{\circ}$. The ISGMR strength distributions for the three nuclei coincide with each other, establishing clearly that nuclear incompressibility is not influenced by nuclear shell structure near $A\sim$90 as was claimed in recent measurements., Comment: 5 pages, 4 figures; accepted for publication in Phys. Lett. B
- Published
- 2016
50. Experimental program of the Super-FRS Collaboration at FAIR and developments of related instrumentation
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T. Grahn, Hooi Jin Ong, S. Purushothaman, K. Itahashi, A. S. Fomichev, Peter Egelhof, Juha Äystö, Isao Tanihata, Ari Jokinen, A. Bracco, J. Benlliure, M. Pfützner, A. Prochazka, M.N. Harakeh, I. G. Mukha, T. Saito, S. Pietri, Wolfgang R. Plaß, C. Nociforo, V. Zamfir, K.-H. Behr, M. Winkler, Livius Trache, Satoru Terashima, Herbert A. Simon, L. V. Grigorenko, Nasser Kalantar-Nayestanaki, Hiroshi Toki, Sydney Gales, Helmut Weick, Christoph Scheidenberger, S. Heinz, G. Münzenberg, Horst Lenske, Ryugo S. Hayano, R. Kanungo, H. Geissel, J. S. Winfield, and Helsinki Institute of Physics
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Nuclear and High Energy Physics ,Meson ,Neutron emission ,COHERENT EXCITATION ,Projectile fragments ,01 natural sciences ,114 Physical sciences ,law.invention ,Nuclear physics ,ENERGY ,law ,0103 physical sciences ,SCATTERING ,SPECTROMETER ,FACILITY ,010306 general physics ,Spectroscopy ,Nuclear Experiment ,Instrumentation ,Physics ,ta114 ,Isotope ,Spectrometer ,NUCLEI ,010308 nuclear & particles physics ,Scattering ,Detector ,Magnetic spectrometer ,PERFORMANCE ,INVERSE KINEMATICS ,PRODUCTS ,STATES ,Achromatic lens ,Experiments - Abstract
The physics program at the super-conducting fragment separator (Super-FRS) at FAIR, being operated in a multiple-stage, high-resolution spectrometer mode, is discussed. The Super-FRS will produce, separate and transport radioactive beams at high energies up to 1.5 AGeV, and it can be also used as a stand-alone experimental device together with ancillary detectors. Various combinations of the magnetic sections of the Super-FRS can be operated in dispersive, achromatic or dispersion-matched spectrometer ion-optical modes, which allow measurements of momentum distributions of secondary-reaction products with high resolution and precision. A number of unique experiments in atomic, nuclear and hadron physics are suggested with the Super-FRS as a stand-alone device, in particular searches for new isotopes, studies of hyper-nuclei, delta-resonances in exotic nuclei and spectroscopy of atoms characterized by bound mesons. Rare decay modes like multiple-proton or neutron emission and the nuclear tensor force observed in high momentum regime can be also addressed. The in-flight radioactivity measurements as well as fusion, transfer and deep-inelastic reaction mechanisms with the slowed-down and energy-bunched fragment beams are proposed for the high-resolution and energy buncher modes at the Super-FRS. (C) 2016 Elsevier B.V. All rights reserved.
- Published
- 2016
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