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79 results on '"Total Cross-sections"'

1. Reaction rate of p14N→15Oγ capture to all bound states in potential cluster model.

Author: Dubovichenko, Sergey, Burkova, Nataliya, Dzhazairov-Kakhramanov, Albert, and Beysenov, Bekmurza
Subjects: *BOUND states, *EXCITED states, *SCATTERING (Physics), *NUCLEAR astrophysics, *ATOMIC nucleus, *INTRAMOLECULAR proton transfer reactions
Abstract: Review of calculation results for astrophysical S -factor of the 1 4 N (p , γ) 1 5 O capture reaction in the p 1 4 N channel of 1 5 O was presented. It was carried out in the frame of the modified potential cluster model (MPCM) taking into account resonances in the 1 5 O spectrum up to 3.2 MeV at energy of incident protons varying of 30 keV to 5 MeV. It is possible to describe experimental data for the astrophysical S -factors of the radiative proton capture on 1 4 N to five excited states of 1 5 O at excitation energies of 5.18 MeV to 6.86 MeV, only under assumption, that all five resonances are D scattering waves. Quality new physical interpretation of the capture mechanism is discussed in this channel to the ground state of 1 5 O. We assumed that the ground state of 1 5 O is determined by the p 1 4 N ∗ channel with excited 1 4 N ∗ cluster, which immediately allowed us to correctly describe order of values of the experimental S -factor for capture to this state. Taking into account these results, the total S -factor of the proton capture on 1 4 N and the reaction rates to the ground and five excited states of 1 5 O were determined at temperatures of 0.01 T 9 to 10 T 9 . The parametrization of the total reaction rate with a simple form is performed, which allows as to obtain χ 2 equal to 0.06 with 5% errors of the calculated rate. [ABSTRACT FROM AUTHOR]
Published: 2020
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2. Total Cross Sections for Electron and Positron Scattering on Molecules: In Search of the Dispersion Relation

Author: Fabio Carelli, Kamil Fedus, and Grzegorz Karwasz
Subjects: electron scattering, positron scattering, total cross-sections, dispersion relation, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract: More than one hundred years of experimental and theoretical investigations of electron scattering in gases delivered cross-sections in a wide energy range, from few meV to keV. An analogy in optics, characterizing different materials, comes under the name of the dispersion relation, i.e., of the dependence of the refraction index on the light wavelength. The dispersion relation for electron (and positron) scattering was hypothesized in the 1970s, but without clear results. Here, we review experimental, theoretical, and semi-empirical cross-sections for N2, CO2, CH4, and CF4 in search of any hint for such a relation—unfortunately, without satisfactory conclusions.
Published: 2021
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3. Soft pomerons and the forward LHC data.

Author: Broilo, M., Luna, E.G.S., and Menon, M.J.
Subjects: *LARGE Hadron Collider, *POMERONS, *REGGE trajectories, *DISPERSION (Atmospheric chemistry), *HYPOTHETICAL composite particles, *PARTICLES (Nuclear physics)
Abstract: Recent data from LHC13 by the TOTEM Collaboration on σ t o t and ρ have indicated disagreement with all the Pomeron model predictions by the COMPETE Collaboration (2002). On the other hand, as recently demonstrated by Martynov and Nicolescu (MN), the new σ t o t datum and the unexpected decrease in the ρ value are well described by the maximal Odderon dominance at the highest energies. Here, we discuss the applicability of Pomeron dominance through fits to the most complete set of forward data from pp and p ¯ p scattering. We consider an analytic parameterization for σ t o t ( s ) consisting of non-degenerated Regge trajectories for even and odd amplitudes (as in the MN analysis) and two Pomeron components associated with double and triple poles in the complex angular momentum plane. The ρ parameter is analytically determined by means of dispersion relations. We carry out fits to pp and p ¯ p data on σ t o t and ρ in the interval 5 GeV–13 TeV (as in the MN analysis). Two novel aspects of our analysis are: (1) the dataset comprises all the accelerator data below 7 TeV and we consider three independent ensembles by adding: either only the TOTEM data (as in the MN analysis), or only the ATLAS data, or both sets; (2) in the data reductions to each ensemble, uncertainty regions are evaluated through error propagation from the fit parameters, with 90% CL. We argument that, within the uncertainties, this analytic model corresponding to soft Pomeron dominance, does not seem to be excluded by the complete set of experimental data presently available. [ABSTRACT FROM AUTHOR]
Published: 2018
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4. Leading components in forward elastic hadron scattering: Derivative dispersion relations and asymptotic uniqueness.

Author: Fagundes, D. A., Menon, M. J., and Silva, P. V. R. G.
Subjects: *HADRON-hadron scattering, *UNIQUENESS (Mathematics), *MATHEMATICAL bounds, *DISPERSION relations, *GOODNESS-of-fit tests
Abstract: Forward amplitude analyses constitute an important approach in the investigation of the energy dependence of the total hadronic cross-section and the parameter. The standard picture indicates for a leading log-squared dependence at the highest c.m. energies, in accordance with the Froissart-Lukaszuk-Martin bound and as predicted by the COMPETE Collaboration in 2002. Beyond this log-squared (L2) leading dependence, other amplitude analyses have considered a log-raised-to-gamma form , with as a real free fit parameter. In this case, analytic connections with can be obtained either through dispersion relations (derivative forms), or asymptotic uniqueness (Phragmén-Lindelöff theorems). In this work, we present a detailed discussion on the similarities and mainly the differences between the Derivative Dispersion Relation (DDR) and Asymptotic Uniqueness (AU) approaches and results, with focus on the and L2 leading terms. We also develop new Regge-Gribov fits with updated dataset on and from and scattering, including all available data in the region 5 GeV-8 TeV. The recent tension between the TOTEM and ATLAS results at 7 TeV and mainly at 8 TeV is discussed and considered in the data reductions. Our main conclusions are the following: (1) all fit results present agreement with the experimental data analyzed and the goodness-of-fit is slightly better in case of the DDR approach; (2) by considering only the TOTEM data at the LHC region, the fits with L indicate (AU approach) and (DDR approach); (3) by including the ATLAS data the fits provide (AU) and (DDR); (4) in the formal and practical contexts, the DDR approach is more adequate for the energy interval investigated than the AU approach. A pedagogical and detailed review on the analytic results for and from the Regge-Gribov, DDR and AU approaches is presented. Formal and practical aspects related to forward amplitude analyses are also critically discussed. [ABSTRACT FROM AUTHOR]
Published: 2017
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5. Bounds on the rise of total cross section from LHC7 and LHC8 data.

Author: Fagundes, D.A., Menon, M.J., and Silva, P.V.R.G.
Subjects: *PROTON-proton interactions, *HADRON interactions, *ASYMPTOTIC freedom, *MEASUREMENT uncertainty (Statistics), *EXTREMAL problems (Mathematics)
Abstract: Recent measurements of the proton–proton total cross section σ t o t at 7 and 8 TeV by the TOTEM and ATLAS Collaborations are characterized by some discrepant values: the TOTEM data suggest a rise of the cross section with the energy faster than the ATLAS data. Attempting to quantify these different behaviors, we develop new analytical fits to σ t o t and ρ data from pp and p ¯ p scattering in the energy region 5 GeV–8 TeV. The dataset comprises all the accelerator data below 7 TeV and we consider three ensembles by adding: either only the TOTEM data (T), or only the ATLAS data (A), or both sets (T + A). For the purposes, we use our previous RRPL γ parametrization for σ t o t ( s ) , consisting of two Reggeons (RR), one critical Pomeron (P) and a leading log-raised-to-gamma (L γ ) contribution (with γ as a free fit parameter), analytically connected to ρ ( s ) through singly-subtracted derivative dispersion relations and energy scale fixed at the physical threshold. The data reductions with ensembles T and A present good agreement with the experimental data analyzed and cannot be distinguished on statistical grounds. The quality of the fit is not as good with ensemble T + A. The fit results provide γ ∼ 2.3 ± 0.1 (T), 2.0 ± 0.1 (A), 2.2 ± 0.2 ( T + A ), with χ 2 / DOF ∼ 1.07 (T), 1.09 (A), 1.14 (T + A), suggesting extrema bounds for γ given by 1.9 and 2.4. Fits with γ = 2 (fixed) are also developed and discussed. [ABSTRACT FROM AUTHOR]
Published: 2017
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6. Exploring central opacity and asymptotic scenarios in elastic hadron scattering.

Author: Fagundes, D.A., Menon, M.J., and Silva, P.V.R.G.
Subjects: *HADRONS, *OPACITY (Optics), *QUANTUM chromodynamics, *PHENOMENOLOGICAL theory (Physics), *NUCLEAR cross sections, *PARAMETERIZATION, SCATTERING
Abstract: In the absence of a global description of the experimental data on elastic and soft diffractive scattering from the first principles of QCD, model-independent analyses may provide useful phenomenological insights for the development of the theory in the soft sector. With that in mind, we present an empirical study on the energy dependence of the ratio X between the elastic and total cross sections; a quantity related to the evolution of the hadronic central opacity. The dataset comprises all the experimental information available on proton–proton and antiproton–proton scattering in the c.m. energy interval 5 GeV–8 TeV. Generalizing previous works, we discuss four model-independent analytical parameterizations for X , consisting of sigmoid functions composed with elementary functions of the energy and three distinct asymptotic scenarios: either the standard black disk limit or scenarios above or below that limit. Our two main conclusions are the following: (1) although consistent with the experimental data, the black disk does not represent an unique solution; (2) the data reductions favor a semi-transparent scenario, with asymptotic average value for the ratio X ¯ = 0.30 ± 0.12 . In this case, within the uncertainty, the asymptotic regime may already be reached around 1000 TeV. We present a comparative study of the two scenarios, including predictions for the inelastic channel (diffraction dissociation) and the ratio associated with the total cross-section and the elastic slope. Details on the selection of our empirical ansatz for X and physical aspects related to a change of curvature in this quantity at 80–100 GeV, indicating the beginning of a saturation effect, are also presented and discussed. [ABSTRACT FROM AUTHOR]
Published: 2016
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7. The neutron microscopic optical potential based on skyrme interaction.

Author: Xu, Yong-Li, Guo, Hai-Rui, Han, Yin-Lu, and Shen, Qing-Biao
Subjects: *NEUTRONS, *SKYRME model, *GREEN'S functions, *NUCLEAR matter, *ELASTIC scattering, *NUCLEAR structure
Abstract: The neutron microscopic optical potential (MOP) based on Skyrme interaction has been achieved by the Green function method in the nuclear matter, and given by the local density approximation (LDA) for finite nuclei. The total cross-sections, nonelastic cross-sections, elastic scattering angular distributions and analyzing powers are predicted for some light nuclei and actinide nuclei below 100MeV by the obtained neutron MOP with the Skyrme interaction SkC. These data are also predicted for targets in the mass range of which are too deformed and have rich nuclear structure properties. All of the theoretical results give reasonable agreements with the corresponding experimental data. [ABSTRACT FROM AUTHOR]
Published: 2016
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8. AN UPDATED ANALYSIS ON THE RISE OF THE HADRONIC TOTAL CROSS-SECTION AT THE LHC ENERGY REGION.

Author: MENON, M. J. and SILVA, P. V. R. G.
Subjects: *HADRONS, *NUCLEAR cross sections, *LARGE Hadron Collider, *ELASTIC scattering, *PROTON-proton interactions, *PROTON scattering, *DATA analysis
Abstract: A forward amplitude analysis on p̅p and elastic scattering above 5 GeV is presented. The dataset includes the recent high-precision TOTEM measurements of the pp total and elastic (integrated) cross-sections at 7 TeV and 8 TeV. Following previous works, the leading high-energy contribution for the total cross-section (σtot) is parametrized as γ(s/sh), where γ and sh are free real fit parameters. Singly-subtracted derivative dispersion relations are used to connect σtot and the rho parameter (ρ) in an analytical way. Different fit procedures are considered, including individual fits to σtot data, global fits to σtot and ρ data, constrained and unconstrained data reductions. The results favor a rise of the σtot faster than the log-squared bound by Froissart and Martin at the LHC energy region. The parametrization for σtot is extended to fit the elastic cross-section (σel data with satisfactory results. The analysis indicates an asymptotic ratio σel/σtot consistent with 1/3 (as already obtained in a previous work). A critical discussion on the correlation, practical role and physical implications of the parameters γ and sh is presented. The discussion confronts the 2002 prediction of σtot by the COMPETE Collaboration and the recent result by the Particle Data Group (2012 edition of the Review of Particle Physics). Some conjectures on possible implications of a fast rise of the proton-proton total cross-section at the highest energies are also presented. [ABSTRACT FROM AUTHOR]
Published: 2013
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9. 209Bi(N,TOT.) CROSS-SECTIONS FOR INCIDENT NEUTRON ENERGIES 0.01-400 eV.

Author: Moinul Haque Meaze, A. K. M. and Guinyun Kim
Subjects: *NEUTRONS, *LINEAR accelerators, *ELECTRONS, *TANTALUM, *NEUTRON counters, *SCINTILLATORS, *TRANSITION metals, *FACTORIES
Abstract: The neutron induced total cross-sections of 209Bi for the energies 0.01 - 400 eV were measured with the neutron time of flight (TOF) method at the pohang neutron facility (PNF), Korea. The PNF consists of a 100 MeV electron linear accelerator (LINAC), a water cooled Tantalum (Ta) target, 12.06 m TOF path length, four position automatic sample changer controlled remotely by the CAMAC data acquisitions systems, and a 6LiZnS(Ag) inorganic scintillator as a neutron detector. The distance from the water cooled Ta target to the sample changer is 5.4 m. To reduce the gamma flash originated from the neutron target we have employed a neutron-gamma separation system based on their different pulse shape. The sample was highly pure. The size of the sample 209Bi was 100 × 100 × 0.5 mm. In order to estimate the background and also to calibrate the energy we used notch filter of Cobalt (Co), Indium (In), and Cadmium (Cd) that has a large resonance peaks within our analyzed energy region. The area of the each samples of notch filter was 100 × 100 mm, and the thickness were 0.5 mm for Co and Cd; and 0.2 mm for the In. The transmission experiments were carried out on samples in and samples out method. The present measured values were compared with the others reported values and with the latest evaluated reaction data library ENDF/B-VII.0. The present measured neutron total cross-sections are generally in good agreement with the others experimental data and the evaluated data library. [ABSTRACT FROM AUTHOR]
Published: 2010

10. NEUTRAL HIGGS BOSON PAIR-PRODUCTION AND TRILINEAR SELF-COUPLINGS IN THE MSSM AT ILC AND CLIC ENERGIES.

Author: GUTIÉRREZ-RODRÍGUEZ, A., HERNÁNDEZ-RUÍZ, M. A., and SAMPAYO, O. A.
Subjects: *CROSS-sectional method, *HIGGS bosons, *SUPERSYMMETRY, *PARTICLES (Nuclear physics), *FEYNMAN diagrams
Abstract: We study pair-production as well as the triple self-couplings of the neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) at the future International Linear e+e- Collider (ILC) and Compact Linear Collider (CLIC). The analysis is based on the reactions $e^{+}e^{-}\rightarrow b \bar b h_ih_i,\, t \bar t h_ih_i$ with hi = h, H, A. We evaluate the total cross-section for both $b\bar bh_ih_i, \, t\bar th_ih_i$ and calculate the total number of events considering the complete set of Feynman diagrams at tree-level. We vary the triple couplings κλhhh, κλHhh, κλhAA, κλHAA, κλhHH and κλHHH within the range κ = -1 and +2. The numerical computation is done for the energies expected at the ILC with a center-of-mass energy 500, 1000, 1600 GeV and a luminosity 1000 fb-1. The channels $e^{+}e^{-}\rightarrow b \bar b h_ih_i$ and $e^{+}e^{-}\rightarrow t \bar t h_ih_i$ are also discussed to a center-of-mass energy of 3 TeV and luminosities of 1000 fb-1 and 5000 fb-1. [ABSTRACT FROM AUTHOR]
Published: 2009

11. Total Cross Sections for Electron and Positron Scattering on Molecules: In Search of the Dispersion Relation.

Author: Carelli, Fabio, Fedus, Kamil, and Karwasz, Grzegorz
Subjects: ELECTRON scattering, DISPERSION relations, REFRACTIVE index, ELECTRON gas, REFRACTION (Optics), POSITRONIUM, OPTICS
Abstract: More than one hundred years of experimental and theoretical investigations of electron scattering in gases delivered cross-sections in a wide energy range, from few meV to keV. An analogy in optics, characterizing different materials, comes under the name of the dispersion relation, i.e., of the dependence of the refraction index on the light wavelength. The dispersion relation for electron (and positron) scattering was hypothesized in the 1970s, but without clear results. Here, we review experimental, theoretical, and semi-empirical cross-sections for N 2 , CO 2 , CH 4 , and CF 4 in search of any hint for such a relation—unfortunately, without satisfactory conclusions. [ABSTRACT FROM AUTHOR]
Published: 2021
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12. INELASTIC COLLISIONS OF POSITRONS WITH BERYLLIUM AND MAGNESIUM IONS.

Author: EL-BAKRY, SALAH-YASEEN
Subjects: *DEEP inelastic collisions, *POSITRONS, *BERYLLIUM, *POSITRONIUM, *MAGNESIUM ions, *CONDUCTION electrons
Abstract: The collision of positrons with beryllium and magnesium positive ions is treated for the first time as a three-channel problem with the assumption that the elastic, ground-positronium and excited-positronium formation channels are open. A one-valence-electron model for the targets, based on the Clementi–Roetti Slater basis functions, as well as an improved coupled-static approach allowing for the polarization of the excited positronium, are used for calculating the partial cross-sections of eight partial waves (corresponding to 0≤ℓ≤7, where ℓ is the total angular momentum of the scattering problem considered). The calculations are carried out, in each case, at 19 values of the incident energy lying above the excited positronium formation threshold (i.e. above 16.42 eV in e+–Be+ scattering and above 13.02 eV in e+–Mg+ scattering). The total elastic cross-sections of e+–Mg+ scattering show a peak around the ionization threshold of Mg+ (at 14.723 eV) but for e+–Be+ scattering, display a peak at 90 eV (remember that the ionization threshold of Be+ is 18.2 eV). Although the resulting total collisional positronium formation cross-sections are smaller than the elastic ones, their relatively large values should draw the attention of experimental and theoretical physicists to the field of positron–ion collisions. [ABSTRACT FROM AUTHOR]
Published: 2007
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13. PAIRS-PRODUCTION OF HIGGS IN ASSOCIATION WITH BOTTOM QUARKS PAIRS AT e+e- COLLIDERS.

Author: Gutiérrez-Rodríguez, A., Hernández-Ruíz, M. A., and Sampayo, O. A.
Subjects: *PAIR production, *DILEPTON production, *QUARKS, *PARTICLES (Nuclear physics), *NUCLEAR physics
Abstract: In a previous paper, we studied the Higgs pair production in the standard model with the reaction $e^{+}e^{-}\rightarrow t\bar{t}HH$. Based on this, we study the Higgs pair production via $e^{+}e^{-}\rightarrow b\bar{b}HH$. We evaluate the total cross-section of $b\bar{b}HH$ and calculate the total number of events considering the complete set of Feynman diagrams at tree-level, and compare this process with the process $e^{+}e^{-}\rightarrow t\bar{t}HH$. The numerical computation is done for the energy which is expected to be available at a possible Next Linear e+e- Collider with a center-of-mass energy 800, 1000, 1600 GeV and luminosity 1000 fb-1. [ABSTRACT FROM AUTHOR]
Published: 2005

14. A GLOBAL TEST OF FACTORIZATION FOR NUCLEON–NUCLEON, γp AND γγ SCATTERING.

Author: BLOCK, MARTIN M. and KANG, KYUNGSIK
Subjects: *NUCLEON-nucleon scattering, *MESONS, *COSMIC rays, *MUONS, *PARTICLES (Nuclear physics), *IONIZING radiation
Abstract: The purpose of this paper is to show that the cross-section factorization relation σnn(s)/σγp(s) = σγp(s)/σγγ(s) is satisfied experimentally in the energy domain $8\le\sqrt s\le 2000~{\rm GeV}$, where the σ's are total cross-sections and nn denotes the even portion of the pp and $\bar pp$ total cross-section. A convenient phenomenological parametrization for a global simultaneous fit to the pp, $\bar pp$, γp and γγ total cross-section data together with the ρ-value data for pp and $\bar pp$ is provided by using real analytic amplitudes. Within experimental errors, we show that factorization is satisfied when we unfold the published γγ data which had averaged the cross-sections obtained by using the two different PHOJET and PYTHIA Monte Carlo results. Our analysis clearly favors the PHOJET results and suggests that the additive quark model, together with vector meson dominance, allows one to compute σγp(s) and σγγ(s) from σnn(s) with essentially no free parameters. The universal ρ-value predicted by our fit, i.e. ρnn = ργp = ργγ, is compared to the ρ-value obtained by a QCD-inspired analysis of $\bar pp$ and pp data, including the p-air cross-sections from cosmic rays. The ρ-values obtained from the two techniques are essentially indistinguishable in the energy region $8\le\sqrt s\le 2000~{\rm GeV}$, giving us increased confidence in our parametrization of the cross-sections needed for the factorization relation. [ABSTRACT FROM AUTHOR]
Published: 2005
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15. Theoretical investigation of the electron capture in collisions of O8+ ion with H and He atoms: Comparison between the Landau–Zener and the over-barrier models

Author: Lugosi, L. and Sarkadi, L.
Subjects: *ION-atom collisions, *ELECTRON capture
Abstract: Analytical and semi-analytical theories based on the molecular and classical treatments have been applied for electron capture processes in collisions of hydrogen and helium atoms with low energy (E=0.1,…,10 keV/amu) O8+ bare ion impact. The used Landau–Zener model (LZ), which allows to give analytical formulas for the cross-sections in our recent approach and the modified over-barrier model (OBM) [Phys. Rev. A 62 (2000) 042711] are briefly summarized. The obtained values of the LZ and OBM cross-sections are compared with experimental data and the results of other sophisticated numerical calculations. It is found that the LZ model provides much reliable cross-sections for charge transfer than the OBM model. [Copyright &y& Elsevier]
Published: 2003
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16. Using world pi(+/-)-nucleus scattering data to constrain an intranuclear cascade model

Author: S. Bhadra, V. Paolone, R. Terri, T. Feusels, C. Wret, P. de Perio, S. Bolognesi, K. Ieki, J. Calcutt, M. Yu, E. S. Pinzon Guerra, Kendall Mahn, C. Wilkinson, Y. Hayato, S. Dolan, M. O. Wascko, R. Tacik, L. Pickering, K. S. McFarland, M. J. Wilking, G. A. Fiorentini, Hiromasa Tanaka, and Science and Technology Facilities Council (STFC)
Subjects: Work (thermodynamics), Particle physics, HIGH-ENERGY, Astronomy & Astrophysics, 7. Clean energy, 01 natural sciences, Physics, Particles & Fields, 0103 physical sciences, medicine, PION ABSORPTION, NEGATIVE PIONS, CHARGE-EXCHANGE, 010306 general physics, Physics, Science & Technology, NUCLEI, CHALLENGES, 010308 nuclear & particles physics, Scattering, State (functional analysis), QUASI-ELASTIC SCATTERING, medicine.anatomical_structure, Cascade, Physical Sciences, SIMULATION, Neutrino, Variety (universal algebra), Nucleus, Energy (signal processing), TOTAL CROSS-SECTIONS, TRUE ABSORPTION
Abstract: The NEUT intranuclear cascade model is described and fit to a large body of ${\ensuremath{\pi}}^{\ifmmode\pm\else\textpm\fi{}}$ -nucleus scattering data. Methods are developed to deal with deficiencies in the available historical data, and robust uncertainty estimates are produced. The results are compared to a variety of simulation packages and the data. This work provides a method for tuning final state interaction models, which are of particular interest to neutrino experiments that operate in the few-GeV energy region, and provides results which can be used directly by the T2K and Super-Kamiokande Collaborations, for whom NEUT is the primary simulation package.
Published: 2019

17. Proton-proton forward scattering at the LHC

Author: Rocha, Mateus Broilo da, Fagundes, Daniel Almeida, Luna, Emerson Gustavo de Souza, and Menon, Marcio Jose
Subjects: Pomerons, Altas energias, Other nonperturbative calculations, Espalhamento proton proton, Hadrons, Elastic scattering, Total cross-sections
Abstract: Recently the TOTEM experiment at the LHC has released measurements at √s=13 TeV of the proton-proton total cross section, σtot, and the ratio of the real to imaginary parts of the forward elastic amplitude, ρ. Since then an intense debate on the C-parity asymptotic nature of the scattering amplitude was initiated. We examine the proton-proton and the antiproton-proton forward data above 10 GeV in the context of an eikonal QCD-based model, where nonperturbative effects are readily included via a QCD effective charge. We show that, despite an overall satisfactory description of the forward data is obtained by a model in which the scattering amplitude is dominated by only crossing-even elastic terms, there is evidence that the introduction of a crossing-odd term may improve the agreement with the measurements of ρ at √s=13 TeV. In the Regge language the dominant even(odd)-under-crossing object is the so called Pomeron (Odderon).
Published: 2019

18. Proton-proton forward scattering at the LHC

Author: Menon, Márcio José, 1952 and UNIVERSIDADE ESTADUAL DE CAMPINAS
Subjects: Energy, Colisões (Física), Espalhamento elástico, Other nonperturbative calculations, Artigo original, Energia, Collisions (Physics), Elastic scattering, Total cross-sections
Abstract: Agradecimentos: We are thankful to an anonymous referee for the important points raised on a previous version of this work. This research was partially supported by the CNPQ - CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICO (CNPq) under the grant 141496/2015-0. DAF acknowledges support by the project INCTFNA (464898/2014-5). EGSL acknowledges the financial support from the ANII-FCE-126412 project Abstract: Recently the TOTEM experiment at the LHC has released measurements root 2 = 13 TeV of the proton-proton total cross section, sigma(tot), and the ratio of the real to imaginary parts of the forward elastic amplitude, rho. Since then an intense debate on the C-parity asymptotic nature of the scattering amplitude was initiated. We examine the proton-proton and the antiproton-proton forward data above 10 GeV in the context of an eikonal QCD-based model, where nonperturbative effects are readily included via a QCD effective charge. We show that, despite an overall satisfactory description of the forward data is obtained by a model in which the scattering amplitude is dominated by only crossing-even elastic terms, there is evidence that the introduction of a crossing-odd term may improve the agreement with the measurements of rho at root 2 = 13 TeV. In the Regge language the dominant even(odd)-under-crossing object is the so called Pomeron (Odderon) CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICO - CNPQ Aberto
Published: 2019

19. Measurement of the elastic, total and single diffraction cross-sections at tevatron energies.

Author: Belforte, S.
Abstract: Results are presented for a measurement of the differential elastic cross-section dτ/d t, the single-diffraction dissociation double differential crossection dα/d M d t and the total inelastic cross-section in antiproton-proton collisions at centre-of-mass energies √ s=546 and 1800 GeV. The elastic-scattering slope is 15.28±0.58 (16.98±0.25)GeV at √ s= (1800) GeV. Using the luminosity-independent method, (1+ρ)α is measured to be 62.64±0.95 (81.83±2.29) mb at √ s=546 (1800) GeV. Assuming ρ=0.15, the elastic, total and single-diffractive cross-sections are τ=12.87±0.30, τ=61.26±0.93 and τ= 7.89±0.33 mb (τ=1970±0.85, τ=80.03±2.24 and τ=9.46±0.44 mb) at 546 (1800) GeV. [ABSTRACT FROM AUTHOR]
Published: 1994
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20. Relation between short-range correlations and intermittency.

Author: Parashar, Neeti
Abstract: Experimental data at 800 GeV has been analyzed to establish a relation between short-range correlation and the observed intermittent behaviour of pseudorapidity density fluctuations. There is good agreement between the calculated and the observed values of the normalized factorial moments. [ABSTRACT FROM AUTHOR]
Published: 1994
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21. Numerical analysis of the high-energy behaviour of the baryon-baryon scattering amplitude in a spontaneously broken gauge theory of the vector meson exchange.

Author: Rączka, P. and Pindor, M.
Abstract: Copyright of Il Nuovo Cimento: A is the property of Springer Nature and its content may not be copied or emailed to multiple sites or posted to a listserv without the copyright holder's express written permission. However, users may print, download, or email articles for individual use. This abstract may be abridged. No warranty is given about the accuracy of the copy. Users should refer to the original published version of the material for the full abstract. (Copyright applies to all Abstracts.)
Published: 1990
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22. Soft pomerons and the forward LHC data

Author: Menon, Márcio José, 1952 and UNIVERSIDADE ESTADUAL DE CAMPINAS
Subjects: Hadronic interactions, Cross sections (Nuclear physics), Seção de choque (Física nuclear), Teoria assintótica - Teoria da estimativa, Artigo original, Total cross-sections, Hadron-induced high- and super-high-energy interactions, Estimation theory - Asymptotic theory, Interações hadrônicas, Asymptotic problems and properties
Abstract: Agradecimentos: This research was partially supported by the Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) grant 141496/2015-0 and by the Fundação de Amparo à Pesquisa do Estado do Rio Grande do Sul (FAPERGS) grant 1945-2551/13-8. EGSL acknowledge the financial support from the Rede Nacional de Altas Energias (RENAFAE) Recent data from LHC13 by the TOTEM Collaboration on sigma(tot) and rho have indicated disagreement with all the Pomeron model predictions by the COMPETE Collaboration (2002). On the other hand, as recently demonstrated by Martynov and Nicolescu (MN), the new sigma(tot) datum and the unexpected decrease in the rho value are well described by the maximal Odderon dominance at the highest energies. Here, we discuss the applicability of Pomeron dominance through fits to the most complete set of forward data from pp and (p) over barp scattering. We consider an analytic parameterization for sigma(tot)(s) consisting of non-degenerated Regge trajectories for even and odd amplitudes (as in the MN analysis) and two Pomeron components associated with double and triple poles in the complex angular momentum plane. The rho parameter is analytically determined by means of dispersion relations. We carry out fits to pp and (p) over barp data on sigma(tot) and rho in the interval 5 GeV-13 TeV (as in the MN analysis). Two novel aspects of our analysis are: (1) the dataset comprises all the accelerator data below 7 TeV and we consider three independent ensembles by adding: either only the TOTEM data (as in the MN analysis), or only the ATLAS data, or both sets||(2) in the data reductions to each ensemble, uncertainty regions are evaluated through error propagation from the fit parameters, with 90% CL. We argument that, within the uncertainties, this analytic model corresponding to soft Pomeron dominance, does not seem to be excluded by the complete set of experimental data presently available. CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICO - CNPQ FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DO RIO GRANDE DO SUL - FAPERGS REDE NACIONAL DE FÍSICA DE ALTAS ENERGIAS - RENAFAE Aberto
Published: 2018

23. Soft pomerons and the forward LHC data

Author: Rocha, Mateus Broilo da, Luna, Emerson Gustavo de Souza, and Menon, Marcio Jose
Subjects: Colisões proton-proton, Pomerons, Hadron-induced high-and super-high-energy interactions, Altas energias, Aceleradores de partículas, Total cross-sections, Asymptotic problems and properties
Abstract: Recent data from LHC13 by the TOTEM Collaboration on σtotand ρhave indicated disagreement with all the Pomeron model predictions by the COMPETE Collaboration (2002). On the other hand, as recently demonstrated by Martynov and Nicolescu (MN), the new σtotdatum and the unexpected decrease in the ρvalue are well described by the maximal Odderon dominance at the highest energies. Here, we discuss the applicability of Pomeron dominance through fits to the most complete setof forward data from ppand ¯ppscattering. We consider an analytic parameterization for σtot(s)consisting of non-degenerated Regge trajectories for even and odd amplitudes (as in the MN analysis) and two Pomeron components associated with double and triple poles in the complex angular momentum plane. The ρparameter is analytically determined by means of dispersion relations. We carry out fits to ppand ¯ppdata on σtotand ρin the interval 5 GeV–13 TeV (as in the MN analysis). Two novel aspects of our analysis are: (1) the dataset comprises all the accelerator data below 7 TeV and we consider three independent ensemblesby adding: either only the TOTEM data (as in the MN analysis), or only the ATLAS data, or both sets; (2) in the data reductions to each ensemble, uncertainty regions are evaluated through error propagation from the fit parameters, with 90% CL. We argument that, within the uncertainties, this analytic model corresponding to soft Pomeron dominance, does not seem to be excluded by the completeset of experimental data presently available.
Published: 2018

24. Isoscalar single-pion production in the region of Roper and d*(2380) resonances

Author: Adlarsona, P., Augustyniak, W., Bardan, W., Bashkanov, M., Bergmann, F. S., Berlowski, M., Bhatt, H., Bondar, A., Buescher, M., Calen, H., Ciepal, I., Clement, H., Czerwinski, E., Demmich, K., Engels, R., Erven, A., Erven, W., Eyrich, W., Fedorets, P., Foehl, K., Fransson, K., Goldenbaum, F., Goswami, A., Grigoryev, K., Gullstrom, C. -O., Heijkenskjoeld, L., Hejny, V., Huesken, N., Jarczyk, L., Johansson, T., Kamys, B., Kemmerling, G., Khatri, G., Khoukaz, A., Khreptak, O., Kirillov, D. A., Kistryn, S., Kleines, H., Klos, B., Krzemien, W., Kulessa, P., Kupsc, A., Kuzmin, A., Lalwani, K., Lersch, D., Lorentz, B., Magiera, A., Maier, R., Marciniewski, P., and Marianski, B.
Subjects: Roper resonance, Single-pion production, Isoscalar part, RANGE, GEV/C, PROTON-PROTON COLLISIONS, BRANCHING RATIOS, WIDTH, SCATTERING, DECAY, Dibaryon resonance, TOTAL CROSS-SECTIONS, THRESHOLD
Abstract: Exclusive measurements of the quasi-free pn -> pp pi(-) and pp -> pp pi(0) reactions have been performed by means of pd collisions at T-p= 1.2 GeV using the WASA detector setup at COSY. Total and differential cross sections have been obtained covering the energy region T-p= 0.95-1.3 GeV (root s = 2.3-2.46 GeV), which includes the regions of triangle(1232), N*(1440) and d*(2380) resonance excitations. From these measurements the isoscalar single-pion production has been extracted, for which data existed so far only below T-p = 1 GeV. We observe a substantial increase of this cross section around 1 GeV, which can be related to the Roper resonance N*(1440), the strength of which shows up isolated from the triangle resonance in the isoscalar (N pi)(I=0) invariant-mass spectrum. No evidence for a decay of the dibaryon resonance d*(2380) into the isoscalar (NN pi)(I=0) channel is found. An upper limit of 180 mu b (90% CL.) corresponding to a branching ratio of 9% has been deduced.
Published: 2017
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25. Bounds on the rise of total cross section from LHC7 and LHC8 data

Author: Menon, Márcio José, 1952, Silva, Paulo Victor Recchia Gomes da, 1989, and UNIVERSIDADE ESTADUAL DE CAMPINAS
Subjects: Hadron-induced high and super-high-energy interactions, Cross sections (Nuclear physics), Seção de choque (Física nuclear), Artigo original, Hadrons, Total cross-sections, Hádrons, Asymptotic problems and properties
Abstract: Agradecimentos: We are thankful to David D. Chinellato for useful discussions. Research supported by FAPESP, Contract 2013/27060-3 (P.V.R.G.S.) Abstract: Recent measurements of the proton proton total cross section sigma(tot) at 7 and 8 TeV by the TOTEM and ATLAS Collaborations are characterized by some discrepant values: the TOTEM data suggest a rise of the cross section with the energy faster than the ATLAS data. Attempting to quantify these different behaviors, we develop new analytical fits to sigma(tot) and rho data from (p) over barp and pp scattering in the energy region 5 GeV-8 TeV. The dataset comprises all the accelerator data below 7 TeV and we consider three ensembles by adding: either only the TOTEM data (T), or only the ATLAS data (A), or both sets (T + A). For the purposes, we use our previous RRPL gamma parametrization for sigma(tot) (s), consisting of two Reggeons (RR), one critical Pomeron (P) and a leading log-raised-to-gamma (L gamma) contribution (with gamma as a free fit parameter), analytically connected to rho(s) through singly-subtracted derivative dispersion relations and energy scale fixed at the physical threshold. The data reductions with ensembles T and A present good agreement with the experimental data analyzed and cannot be distinguished on statistical grounds. The quality of the fit is not as good with ensemble T + A. The fit results provide gamma similar to 2.3 +/- 0.1 (T), 2.0 +/- 0.1 (A), 2.2 +/- 0.2 (T + A), with x(2)/DOF similar to 1.07 (T), 1.09 (A), 1.14 (T + A), suggesting extrema bounds for gamma given by 1.9 and 2.4. Fits with gamma = 2 (fixed) are also developed and discussed FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DE SÃO PAULO - FAPESP Aberto
Published: 2017

26. Leading components in forward elastic hadron scattering : derivative dispersion relations and asymptotic uniqueness

Author: Menon, Márcio José, 1952, Silva, Paulo Victor Recchia Gomes da, 1989, and UNIVERSIDADE ESTADUAL DE CAMPINAS
Subjects: Cross sections (Nuclear physics), Seção de choque (Física nuclear), Artigo original, Hadrons, Total cross-sections, Hadron-induced high- and super-high-energy interactions, Hádrons, Asymptotic problems and properties
Abstract: Agradecimentos: We are thankful to Professor Vladimir Ezhela (PDG, COMPAS Group,IHEP,Protvino) for useful correspondence. Work supported by SãoPaulo Research Foundation (FAPESP), Contract 2013/27060-3 (P. V. R. G. Silva) Abstract: Forward amplitude analyses constitute an important approach in the investigation of the energy dependence of the total hadronic cross-section sigma(tot) and the rho parameter. The standard picture indicates for sigma(tot) a leading log-squared dependence at the highest c.m. energies, in accordance with the Froissart-Lukaszuk-Martin bound and as predicted by the COMPETE Collaboration in 2002. Beyond this log-squared (L2) leading dependence, other amplitude analyses have considered a log-raised-to-gamma form (L gamma), with gamma as a real free fit parameter. In this case, analytic connections with rho can be obtained either through dispersion relations (derivative forms), or asymptotic uniqueness (Phragmen-Lindeloff theorems). In this work, we present a detailed discussion on the similarities and mainly the differences between the Derivative Dispersion Relation (DDR) and Asymptotic Uniqueness (AU) approaches and results, with focus on the L gamma and L2 leading terms. We also develop new Regge-Gribov fits with updated dataset on sigma(tot) and rho from pp and (p) over barp scattering, including all available data in the region 5 GeV-8 TeV. The recent tension between the TOTEM and ATLAS results at 7 TeV and mainly at 8 TeV is discussed and considered in the data reductions. Our main conclusions are the following: (1) all fit results present agreement with the experimental data analyzed and the goodness-of-fit is slightly better in case of the DDR approach; (2) by considering only the TOTEM data at the LHC region, the fits with L gamma indicate gamma similar to 2.0 +/- 0.2 (AU approach) and gamma similar to 2.3 +/- 0.1 (DDR approach); (3) by including the ATLAS data the fits provide gamma similar to 1.9 +/- 0.1 (AU) and gamma similar to 2.2 +/- 0.2 (DDR); (4) in the formal and practical contexts, the DDR approach is more adequate for the energy interval investigated than the AU approach. A pedagogical and detailed review on the analytic results for sigma(tot) and rho from the Regge-Gribov, DDR and AU approaches is presented. Formal and practical aspects related to forward amplitude analyses are also critically discussed FUNDAÇÃO DE AMPARO À PESQUISA DO ESTADO DE SÃO PAULO - FAPESP Aberto
Published: 2017

27. Proton-proton forward scattering at the LHC.

Author: Broilo, M., Fagundes, D.A., Luna, E.G.S., and Menon, M.J.
Subjects: *DOMINANT language, *ELASTIC scattering
Abstract: Recently the TOTEM experiment at the LHC has released measurements at s = 13 TeV of the proton-proton total cross section, σ t o t , and the ratio of the real to imaginary parts of the forward elastic amplitude, ρ. Since then an intense debate on the C -parity asymptotic nature of the scattering amplitude was initiated. We examine the proton-proton and the antiproton-proton forward data above 10 GeV in the context of an eikonal QCD-based model, where nonperturbative effects are readily included via a QCD effective charge. We show that, despite an overall satisfactory description of the forward data is obtained by a model in which the scattering amplitude is dominated by only crossing-even elastic terms, there is evidence that the introduction of a crossing-odd term may improve the agreement with the measurements of ρ at s = 13 TeV. In the Regge language the dominant even(odd)-under-crossing object is the so called Pomeron (Odderon). [ABSTRACT FROM AUTHOR]
Published: 2019
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28. Midrapidity antiproton-to-proton ratio in pp collisions at $\sqrt{s} = 0.9$ and $7$~TeV measured by the ALICE experiment

Author: Universidade Estadual de Campinas
Subjects: Scattering, String Model, Total Cross-sections, Physics, Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431 [VDP], High Energy Physics::Experiment, Collisions, Antinucleon-nucleon, Nuclear Experiment, Particle Physics - Experiment, Energies, Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP], High Energy Physics - Experiment
Abstract: The ratio of the yields of antiprotons to protons in pp collisions has been measured by the ALICE experiment at $\sqrt{s} = 0.9$ and $7$~TeV during the initial running periods of the Large Hadron Collider(LHC). The measurement covers the transverse momentum interval $0.45 < p_{\rm{t}} < 1.05$~GeV/$c$ and rapidity $|y| < 0.5$. The ratio is measured to be $R_{|y| < 0.5} = 0.957 \pm 0.006 (stat.) \pm 0.014 (syst.)$ at $0.9$~TeV and $R_{|y| < 0.5} = 0.991 \pm 0.005 (stat.) \pm 0.014 (syst.)$ at $7$~TeV and it is independent of both rapidity and transverse momentum. The results are consistent with the conventional model of baryon-number transport and set stringent limits on any additional contributions to baryon-number transfer over very large rapidity intervals in pp collisions. The ratio of the yields of antiprotons to protons in pp collisions has been measured by the ALICE experiment at $\sqrt{s} = 0.9$ and $7$ TeV during the initial running periods of the Large Hadron Collider(LHC). The measurement covers the transverse momentum interval $0.45 < p_{\rm{t}} < 1.05$ GeV/$c$ and rapidity $|y| < 0.5$. The ratio is measured to be $R_{|y| < 0.5} = 0.957 \pm 0.006 (stat.) \pm 0.014 (syst.)$ at $0.9$ TeV and $R_{|y| < 0.5} = 0.991 \pm 0.005 (stat.) \pm 0.014 (syst.)$ at $7$ TeV and it is independent of both rapidity and transverse momentum. The results are consistent with the conventional model of baryon-number transport and set stringent limits on any additional contributions to baryon-number transfer over very large rapidity intervals in pp collisions.
Published: 2016

29. Electron-Capture Cross Sections of Ground-State O2+ Recoil Ions in Slow Collisions with H2 and O2

Author: Asad T. Hasan and Tom J. Gray
Subjects: Thermonuclear fusion, Electron capture, Nanotechnology, Measure (mathematics), Catalysis, Full Research Paper, Ion, Inorganic Chemistry, lcsh:Chemistry, Recoil, Single electron-capture, Physical and Theoretical Chemistry, Molecular Biology, lcsh:QH301-705.5, Spectroscopy, Physics, Range (particle radiation), Organic Chemistry, total cross-sections, Charge (physics), General Medicine, Computer Science Applications, lcsh:Biology (General), lcsh:QD1-999, Atomic physics, Ground state
Abstract: We report the measured total charge-transfer (electron-capture) cross sections for the ground state + O 2 (X 2 Π g ) ions with H 2 and O 2 molecular gases in the collision energy range between 0.50 and 2 keV. The time-of-flight technique has been used to measure the fast neutral products from + O 2 charge transfer reactions. The analyzed process has cross sections that continue to increase slowly, as a function of incident energy. Measured cross sections for + O 2 + H 2, O 2 systems are compared with previously available experimental and theoretical results in the literature. Keywords: Single electron-capture; total cross-sections 1. Introduction A detailed understanding of charge-transfer processes of the type A q+ + B AE A (q-1)+ (n,l) + B + (n,l`) has been the goal of many experimental studies [1-4]. These processes have become extremely important in many research areas such as plasma fusion [5], astrophysics and atmospheric science [6,7], atomic physics [8] and the design of controlled thermonuclear fusion devices [9]. At low
Published: 2007

30. Measurements of neutrino oscillation in appearance and disappearance channels by the T2K experiment with 6.6 x 10(20) protons on target

Author: T2K Collaboration, Abe, Kou, Cervera Villanueva, Anselmo, Escudero Sánchez, Lorena, Izmaylov, A., Sorel, Michel, Stamoulis, Panagiotis, Ministerio de Economía y Competitividad (España), Ministry of Education, Culture, Sports, Science and Technology (Japan), Natural Sciences and Engineering Research Council of Canada, Centre National de la Recherche Scientifique (France), and Royal Society (UK)
Subjects: Pion absorption, Quasi-elastic scattering, Super-kamiokande detector, Total cross-sections
Abstract: 111 pages.- 45 figures, We report on measurements of neutrino oscillation using data from the T2K long-baseline neutrino experiment collected between 2010 and 2013. In an analysis of muon neutrino disappearance alone, we find the following estimates and 68% confidence intervals for the two possible mass hierarchies: normal hierarchy: sin(2)theta(23) = 0.514(-0.055)(+0.056) and Delta m(32)(2) = (2.51 +/- 0.10) x 10(-3) eV(2)/c(4) and inverted hierarchy: sin(2)theta(23) = 0.511 +/- 0.055 and Delta m(13)(2) = (2.48 +/- 0.10) x 10(-3) eV(2)/c(4). The analysis accounts for multinucleon mechanisms in neutrino interactions which were found to introduce negligible bias. We describe our first analyses that combine measurements of muon neutrino disappearance and electron neutrino appearance to estimate four oscillation parameters, vertical bar Delta m(2)vertical bar, sin(2)theta(23), sin(2)theta(13,) delta(CP), and the mass hierarchy. Frequentist and Bayesian intervals are presented for combinations of these parameters, with and without including recent reactor measurements. At 90% confidence level and including reactor measurements, we exclude the region delta(CP) = [0.15; 0.83]pi for normal hierarchy and delta(CP) = [-0.08; 1.09]pi for inverted hierarchy. The T2K and reactor data weakly favor the normal hierarchy with a Bayes factor of 2.2. The most probable values and 68% one-dimensional credible intervals for the other oscillation parameters, when reactor data are included, are sin(2)theta(23) = 0.528(-0.055)(+0.038) and vertical bar Delta m(32)(2)vertical bar = (2.51 +/- 0.11) x 10(-3) eV(2)/c(4)., We thank the J-PARC staff for superb accelerator performance and the CERN NA61/SHINE Collaboration for providing valuable particle production data. We acknowledge the support of MEXT, Japan; NSERC, NRC, and CFI, Canada; CEA and CNRS/IN2P3, France; DFG, Germany; INFN, Italy; National Science Centre (NCN), Poland; RSF, RFBR and MES, Russia; MINECO and ERDF funds, Spain; SNSF and SER, Switzerland; STFC, UK; and the U.S. Deparment of Energy, USA. We also thank CERN for the UA1/NOMAD magnet, DESY for the HERA-B magnet mover system, NII for SINET4, the WestGrid and SciNet consortia in Compute Canada, GridPP, UK, and the Emerald High Performance Computing facility in the Centre for Innovation, UK. In addition, participation of individual researchers and institutions has been further supported by funds from ERC (FP7), EU; JSPS, Japan; Royal Society, UK; and DOE Early Career program, USA.
Published: 2015

31. Measurements of neutrino oscillation in appearance and disappearance channels by the T2K experiment with 6.6E20 protons on target

Author: T2K Collaboration, Abe, K., Adam, J., Aihara, H., Akiri, T., Andreopoulos, C., Aoki, S., Ariga, A., Assylbekov, S., Autiero, D., Barbi, M., Barker, G. J., Barr, G., Bartet-Friburg, P., Bass, M., Batkiewicz, M., Bay, F., Berardi, V., Berger, B. E., Berkman, S., Bhadra, S., Blaszczyk, F. d. M., Blondel, A., Bolognesi, S., Bordoni, S., Boyd, S. B., Brailsford, D., Bravar, A., Bronner, C., Buchanan, N., Calland, R. G., Rodr��guez, J. Caravaca, Cartwright, S. L., Castillo, R., Catanesi, M. G., Cervera, A., Cherdack, D., Chikuma, N., Christodoulou, G., Clifton, A., Coleman, J., Coleman, S. J., Collazuol, G., Connolly, K., Cremonesi, L., Dabrowska, A., Danko, I., Das, R., Davis, S., de Perio, P., De Rosa, G., Dealtry, T., Dennis, S. R., Densham, C., Dewhurst, D., Di Lodovico, F., Di Luise, S., Dolan, S., Drapier, O., Duboyski, T., Duffy, K., Dumarchez, J., Dytman, S., Dziewiecki, M., Emery-Schrenk, S., Ereditato, A., Escudero, L., Feusels, T., Finch, A. J., Fiorentini, G. A., Friend, M., Fujii, Y., Fukuda, Y., Furmanski, A. P., Galymov, V., Garcia, A., Giffin, S., Giganti, C., Gilje, K., Goeldi, D., Golan, T., Gonin, M., Grant, N., Gudin, D., Hadley, D. R., Haegel, L., Haesler, A., Haigh, M. D., Hamilton, P., Hansen, D., Hara, T., Hartz, M., Hasegawa, T., Hastings, N. C., Hayashino, T., Hayato, Y., Hearty, C., Helmer, R. L., Hierholzer, M., Hignight, J., Hillairet, A., Himmel, A., Hiraki, T., Hirota, S., Holeczek, J., Horikawa, S., Hosomi, F., Huang, K., Ichikawa, A. K., Ieki, K., Ieva, M., Ikeda, M., Imber, J., Insler, J., Irvine, T. J., Ishida, T., Ishii, T., Iwai, E., Iwamoto, K., Iyogi, K., Izmaylov, A., Jacob, A., Jamieson, B., Jiang, M., Johnson, S., Jo, J. H., Jonsson, P., Jung, C. K., Kabirnezhad, M., Kaboth, A. C., Kajita, T., Kakuno, H., Kameda, J., Kanazawa, Y., Karlen, D., Karpikov, I., Katori, T., Kearns, E., Khabibullin, M., Khotjantsev, A., Kielczewska, D., Kikawa, T., Kilinski, A., Kim, J., King, S., Kisiel, J., Kitching, P., Kobayashi, T., Koch, L., Koga, T., Kolaceke, A., Konaka, A., Kormos, L. L., Korzenev, A., Koshio, Y., Kropp, W., Kubo, H., Kudenko, Y., Kurjata, R., Kutter, T., Lagoda, J., Lamont, I., Larkin, E., Laveder, M., Lawe, M., Lazos, M., Lindner, T., Lister, C., Litchfield, R. P., Longhin, A., Lopez, J. P., Ludovici, L., Magaletti, L., Mahn, K., Malek, M., Manly, S., Marino, A. D., Marteau, J., Martin, J. F., Martins, P., Martynenko, S., Maruyama, T., Matveev, V., Mavrokoridis, K., Mazzucato, E., McCarthy, M., McCauley, N., McFarland, K. S., McGrew, C., Mefodiev, A., Metelko, C., Mezzetto, M., Mijakowski, P., Miller, C. A., Minamino, A., Mineev, O., Missert, A., Miura, M., Moriyama, S., Mueller, Th. A., Murakami, A., Murdoch, M., Murphy, S., Myslik, J., Nakadaira, T., Nakahata, M., Nakamura, K. G., Nakamura, K., Nakayama, S., Nakaya, T., Nakayoshi, K., Nantais, C., Nielsen, C., Nirkko, M., Nishikawa, K., Nishimura, Y., Nowak, J., O'Keeffe, H. M., Ohta, R., Okumura, K., Okusawa, T., Oryszczak, W., Oser, S. M., Ovsyannikova, T., Owen, R. A., Oyama, Y., Palladino, V., Palomino, J. L., Paolone, V., Payne, D., Perevozchikov, O., Perkin, J. D., Petrov, Y., Pickard, L., Guerra, E. S. Pinzon, Pistillo, C., Plonski, P., Poplawska, E., Popov, B., Posiadala-Zezula, M., Poutissou, J. -M., Poutissou, R., Przewlocki, P., Quilain, B., Radicioni, E., Ratoff, P. N., Ravonel, M., Rayner, M. A. M., Redij, A., Reeves, M., Reinherz-Aronis, E., Riccio, C., Rodrigues, P. A., Rojas, P., Rondio, E., Roth, S., Rubbia, A., Ruterbories, D., Rychter, A., Sacco, R., Sakashita, K., S��nchez, F., Sato, F., Scantamburlo, E., Scholberg, K., Schoppmann, S., Schwehr, J., Scott, M., Seiya, Y., Sekiguchi, T., Sekiya, H., Sgalaberna, D., Shah, R., Shaker, F., Shaw, D., Shiozawa, M., Short, S., Shustrov, Y., Sinclair, P., Smith, B., Smy, M., Sobczyk, J. T., Sobel, H., Sorel, M., Southwell, L., Stamoulis, P., Steinmann, J., Still, B., Suda, Y., Suzuki, A., Suzuki, K., Suzuki, S. Y., Suzuki, Y., Tacik, R., Tada, M., Takahashi, S., Takeda, A., Takeuchi, Y., Tanaka, H. K., Tanaka, H. A., Tanaka, M. M., Terhorst, D., Terri, R., Thompson, L. F., Thorley, A., Tobayama, S., Toki, W., Tomura, T., Totsuka, Y., Touramanis, C., Tsukamoto, T., Tzanov, M., Uchida, Y., Vacheret, A., Vagins, M., Vasseur, G., Wachala, T., Wakamatsu, K., Walter, C. W., Wark, D., Warzycha, W., Wascko, M. O., Weber, A., Wendell, R., Wilkes, R. J., Wilking, M. J., Wilkinson, C., Williamson, Z., Wilson, J. R., Wilson, R. J., Wongjirad, T., Yamada, Y., Yamamoto, K., Yanagisawa, C., Yano, T., Yen, S., Yershov, N., Yokoyama, M., Yoshida, K., Yuan, T., Yu, M., Zalewska, A., Zalipska, J., Zambelli, L., Zaremba, K., Ziembicki, M., Zimmerman, E. D., Zito, M., ��muda, J., Science and Technology Facilities Council (STFC), Institut de Physique Nucléaire de Lyon (IPNL), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Nucléaire et de Hautes Énergies (LPNHE), Université Pierre et Marie Curie - Paris 6 (UPMC)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS), Département de Physique des Particules (ex SPP) (DPhP), 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, Laboratoire Leprince-Ringuet (LLR), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), T2K, Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Centre National de la Recherche Scientifique (CNRS)-Université Paris Diderot - Paris 7 (UPD7)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Pierre et Marie Curie - Paris 6 (UPMC), Département de Physique des Particules (ex SPP) (DPP), and Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)
Subjects: Science & Technology, NUCLEI, hep-ex, Physics, MODELS, FOS: Physical sciences, Astronomy & Astrophysics, QUASI-ELASTIC SCATTERING, Nuclear & Particles Physics, High Energy Physics - Experiment, Physics, Particles & Fields, High Energy Physics - Experiment (hep-ex), PI(+), Physical Sciences, SIMULATION, 0201 Astronomical and Space Sciences, 0202 Atomic, Molecular, Nuclear, Particle and Plasma Physics, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], PION ABSORPTION, SYMMETRIES, CHARGE-EXCHANGE, 0206 Quantum Physics, TOTAL CROSS-SECTIONS, TRUE ABSORPTION
Abstract: We report on measurements of neutrino oscillation using data from the T2K long-baseline neutrino experiment collected between 2010 and 2013. In an analysis of muon neutrino disappearance alone, we find the following estimates and 68% confidence intervals for the two possible mass hierarchies: Normal Hierarchy: $\sin^2\theta_{23}=0.514^{+0.055}_{-0.056}$ and $\Delta m^2_{32}=(2.51\pm0.10)\times 10^{-3}$ eV$^2$/c$^4$ Inverted Hierarchy: $\sin^2\theta_{23}=0.511\pm0.055$ and $\Delta m^2_{13}=(2.48\pm0.10)\times 10^{-3}$ eV$^2$/c$^4$ The analysis accounts for multi-nucleon mechanisms in neutrino interactions which were found to introduce negligible bias. We describe our first analyses that combine measurements of muon neutrino disappearance and electron neutrino appearance to estimate four oscillation parameters and the mass hierarchy. Frequentist and Bayesian intervals are presented for combinations of these parameters, with and without including recent reactor measurements. At 90% confidence level and including reactor measurements, we exclude the region: $\delta_{CP}=[0.15,0.83]\pi$ for normal hierarchy and $\delta_{CP}=[-0.08,1.09]\pi$ for inverted hierarchy. The T2K and reactor data weakly favor the normal hierarchy with a Bayes Factor of 2.2. The most probable values and 68% 1D credible intervals for the other oscillation parameters, when reactor data are included, are: $\sin^2\theta_{23}=0.528^{+0.055}_{-0.038}$ and $|\Delta m^2_{32}|=(2.51\pm0.11)\times 10^{-3}$ eV$^2$/c$^4$., Comment: 111 pages, 45 figures, submitted to Physical Review D. Minor revisions to text following referee comments
Published: 2015
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32. Measurement of the Semileptonic CP Asymmetry in B-0-(B)over-bar(0) Mixing

Subjects: DEUTERONS, PROTONS, PBAR, DECAY, TOTAL CROSS-SECTIONS
Abstract: The semileptonic CP asymmetry in B-0-(B) over bar (0) mixing, a(s1)(d), is measured in proton-proton collision data, corresponding to an integrated luminosity of 3.0 fb(-1), recorded by the LHCb experiment. Semileptonic B-0 decays are reconstructed in the inclusive final states D-mu(+) and D*(-)mu(+), where the D- meson decays into the K+pi(-)pi(-) final state and the D*(-) meson into the (D) over bar (0)(-> K+pi(-))pi(-) final state. The asymmetry between the numbers of D-(*()-)mu(+) and D-(*()+)mu(-) decays is measured as a function of the decay time of the B-0 mesons. The CP asymmetry is measured to be a(s1)(d) = (-0.02 +/- 0.19 +/- 0.30)%, where the first uncertainty is statistical and the second systematic. This is the most precise measurement of a(s1)(d) to date and is consistent with the prediction from the standard model.
Published: 2015
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33. Measurement of the Semileptonic CP Asymmetry in B-0-(B)over-bar(0) Mixing

Author: Aaij, R., Adeva, B., Adinolfi, M., Affolder, A., Ajaltouni, Z., Akar, S., Albrecht, J., Alessio, F., Alexander, M., Ali, S., Alkhazov, G., Cartelle, P. Alvarez, Alves, A. A., Amato, S., Amerio, S., Amhis, Y., An, L., Anderlini, L., Anderson, J., Andreassen, R., Andreotti, M., Andrews, J. E., Appleby, R. B., Gutierrez, O. Aquines, Archilli, F., Artamonov, A., Artuso, M., Aslanides, E., Auriemma, G., Baalouch, M., Bachmann, S., Back, J. J., Badalov, A., Baesso, C., Baldini, W., Barlow, R. J., Barschel, C., Barsuk, S., Barter, W., Batozskaya, V., Battista, V., Bay, A., Beaucourt, L., Beddow, J., Bedeschi, F., Bediaga, I., Belogurov, S., Onderwater, C. J. G., Pellegrino, A., Wilschut, H. W., and Precision Frontier
Subjects: DEUTERONS, High Energy Physics::Phenomenology, PROTONS, High Energy Physics::Experiment, PBAR, DECAY, TOTAL CROSS-SECTIONS
Abstract: The semileptonic CP asymmetry in B-0-(B) over bar (0) mixing, a(s1)(d), is measured in proton-proton collision data, corresponding to an integrated luminosity of 3.0 fb(-1), recorded by the LHCb experiment. Semileptonic B-0 decays are reconstructed in the inclusive final states D-mu(+) and D*(-)mu(+), where the D- meson decays into the K+pi(-)pi(-) final state and the D*(-) meson into the (D) over bar (0)(-> K+pi(-))pi(-) final state. The asymmetry between the numbers of D-(*()-)mu(+) and D-(*()+)mu(-) decays is measured as a function of the decay time of the B-0 mesons. The CP asymmetry is measured to be a(s1)(d) = (-0.02 +/- 0.19 +/- 0.30)%, where the first uncertainty is statistical and the second systematic. This is the most precise measurement of a(s1)(d) to date and is consistent with the prediction from the standard model.
Published: 2015

34. Measurements of neutrino oscillation in appearance and disappearance channels by the T2K experiment with 6.6 x 10(20) protons on target

Author: Ministerio de Economía y Competitividad (España), Ministry of Education, Culture, Sports, Science and Technology (Japan), Natural Sciences and Engineering Research Council of Canada, Centre National de la Recherche Scientifique (France), Royal Society (UK), T2K Collaboration, Abe, Kou, Cervera Villanueva, Anselmo, Escudero Sánchez, Lorena, Izmaylov, A., Sorel, Michel, Stamoulis, Panagiotis, Ministerio de Economía y Competitividad (España), Ministry of Education, Culture, Sports, Science and Technology (Japan), Natural Sciences and Engineering Research Council of Canada, Centre National de la Recherche Scientifique (France), Royal Society (UK), T2K Collaboration, Abe, Kou, Cervera Villanueva, Anselmo, Escudero Sánchez, Lorena, Izmaylov, A., Sorel, Michel, and Stamoulis, Panagiotis
Abstract: We report on measurements of neutrino oscillation using data from the T2K long-baseline neutrino experiment collected between 2010 and 2013. In an analysis of muon neutrino disappearance alone, we find the following estimates and 68% confidence intervals for the two possible mass hierarchies: normal hierarchy: sin(2)theta(23) = 0.514(-0.055)(+0.056) and Delta m(32)(2) = (2.51 +/- 0.10) x 10(-3) eV(2)/c(4) and inverted hierarchy: sin(2)theta(23) = 0.511 +/- 0.055 and Delta m(13)(2) = (2.48 +/- 0.10) x 10(-3) eV(2)/c(4). The analysis accounts for multinucleon mechanisms in neutrino interactions which were found to introduce negligible bias. We describe our first analyses that combine measurements of muon neutrino disappearance and electron neutrino appearance to estimate four oscillation parameters, vertical bar Delta m(2)vertical bar, sin(2)theta(23), sin(2)theta(13,) delta(CP), and the mass hierarchy. Frequentist and Bayesian intervals are presented for combinations of these parameters, with and without including recent reactor measurements. At 90% confidence level and including reactor measurements, we exclude the region delta(CP) = [0.15; 0.83]pi for normal hierarchy and delta(CP) = [-0.08; 1.09]pi for inverted hierarchy. The T2K and reactor data weakly favor the normal hierarchy with a Bayes factor of 2.2. The most probable values and 68% one-dimensional credible intervals for the other oscillation parameters, when reactor data are included, are sin(2)theta(23) = 0.528(-0.055)(+0.038) and vertical bar Delta m(32)(2)vertical bar = (2.51 +/- 0.11) x 10(-3) eV(2)/c(4).
Published: 2015

35. Neutron total cross-sections and resonance parameters of Mo and Ta

Author: Moinul Haque Meaze, A. K. M., Devan, K., Lee, Y. S., Oh, Y. D., Kim, G. N., and Son, D.
Published: 2007
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36. Theoretical expectations for σtot at the large hadron collider

Author: Godbole, Rohini M., Grau, Agnes, Hegde, Rohit, Pancheri, Giulia, and Srivastava, Yogi
Published: 2006
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37. Ionization and excitation of some atomic targets and metal oxides by electron impact

Author: Joshipura, K. N., Vaishnav, B. G., and Limbachiya, C. G.
Published: 2006
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38. Simulation of charge-state distribution of ions scattered on crystals

Subjects: SOLIDS, ATOM COLLISIONS, HYDROGEN, charge exchange, COMPUTATION, channeling, surface structure, ANGULAR-DEPENDENCE, ion-atom collisions, PROTONS, ELECTRON-CAPTURE, HIGH-ENERGY COLLISIONS, TOTAL CROSS-SECTIONS, NISI2(111) SURFACE
Published: 1997

39. Centrality dependence of $\pi$, K, p production in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV

Author: Abelev, Betty, Ahammed, Zubayer, Blau, Dmitry, Blume, Christoph, Boccioli, Marco, Boettger, Stefan, Bogdanov, Alexey, Boggild, Hans, Bogolyubsky, Mikhail, Boldizsar, Laszlo, Bombara, Marek, Book, Julian, Ahmad, Nazeer, Borel, Herve, Borissov, Alexander, Bossu, Francesco, Botje, Michiel, Botta, Elena, Braidot, Ermes, Braun-Munzinger, Peter, Bregant, Marco, Breitner, Timo Gunther, Broker, Theo Alexander, Ahmad, Arshad, Browning, Tyler Allen, Broz, Michal, Brun, Rene, Bruna, Elena, Bruno, Giuseppe Eugenio, Budnikov, Dmitry, Buesching, Henner, Bufalino, Stefania, Buncic, Predrag, Busch, Oliver, Ahn, Sul-Ah, Buthelezi, Edith Zinhle, Caffarri, Davide, Cai, Xu, Caines, Helen Louise, Calvo Villar, Ernesto, Camerini, Paolo, Canoa Roman, Veronica, Cara Romeo, Giovanni, Carena, Francesco, Carena, Wisla, Ahn, Sang Un, Carlin Filho, Nelson, Carminati, Federico, Casanova Diaz, Amaya Ofelia, Castillo Castellanos, Javier Ernesto, Castillo Hernandez, Juan Francisco, Casula, Ester Anna Rita, Catanescu, Vasile, Cavicchioli, Costanza, Ceballos Sanchez, Cesar, Cepila, Jan, Ajaz, Muhammad, Cerello, Piergiorgio, Chang, Beomsu, Chapeland, Sylvain, Charvet, Jean-Luc Fernand, Chattopadhyay, Sukalyan, Chattopadhyay, Subhasis, Cherney, Michael Gerard, Cheshkov, Cvetan, Cheynis, Brigitte, Chibante Barroso, Vasco Miguel, Akindinov, Alexander, Chinellato, David, Chochula, Peter, Chojnacki, Marek, Choudhury, Subikash, Christakoglou, Panagiotis, Christensen, Christian Holm, Christiansen, Peter, Chujo, Tatsuya, Chung, Suh-Urk, Cicalo, Corrado, Aleksandrov, Dmitry, Cifarelli, Luisa, Cindolo, Federico, Cleymans, Jean Willy Andre, Colamaria, Fabio, Colella, Domenico, Collu, Alberto, Conesa Balbastre, Gustavo, Conesa del Valle, Zaida, Connors, Megan Elizabeth, Contin, Giacomo, Alessandro, Bruno, Contreras, Jesus Guillermo, Cormier, Thomas Michael, Corrales Morales, Yasser, Cortese, Pietro, Cortes Maldonado, Ismael, Cosentino, Mauro Rogerio, Costa, Filippo, Cotallo, Manuel Enrique, Crescio, Elisabetta, Crochet, Philippe, Alici, Andrea, Cruz Alaniz, Emilia, Cruz Albino, Rigoberto, Cuautle, Eleazar, Cunqueiro, Leticia, Dainese, Andrea, Danu, Andrea, Das, Kushal, Das, Indranil, Das, Supriya, Das, Debasish, Adam, Jaroslav, Alkin, Anton, Dash, Sadhana, Dash, Ajay Kumar, De, Sudipan, de Barros, Gabriel, De Caro, Annalisa, de Cataldo, Giacinto, de Cuveland, Jan, De Falco, Alessandro, De Gruttola, Daniele, Delagrange, Hugues, Almaraz Avina, Erick Jonathan, Deloff, Andrzej, De Marco, Nora, Denes, Ervin, De Pasquale, Salvatore, Deppman, Airton, D'Erasmo, Ginevra, de Rooij, Raoul Stefan, Diaz Corchero, Miguel Angel, Di Bari, Domenico, Dietel, Thomas, Alme, Johan, Di Giglio, Carmelo, Di Liberto, Sergio, Di Mauro, Antonio, Di Nezza, Pasquale, Divia, Roberto, Djuvsland, Oeystein, Dobrin, Alexandru Florin, Dobrowolski, Tadeusz Antoni, Donigus, Benjamin, Dordic, Olja, Alt, Torsten, Driga, Olga, Dubey, Anand Kumar, Dubla, Andrea, Ducroux, Laurent, Dupieux, Pascal, Dutta Majumdar, AK, Elia, Domenico, Emschermann, David Philip, Engel, Heiko, Erazmus, Barbara, Altini, Valerio, Erdal, Hege Austrheim, Espagnon, Bruno, Estienne, Magali Danielle, Esumi, Shinichi, Evans, David, Eyyubova, Gyulnara, Fabris, Daniela, Faivre, Julien, Falchieri, Davide, Fantoni, Alessandra, Altinpinar, Sedat, Fasel, Markus, Fearick, Roger Worsley, Fehlker, Dominik, Feldkamp, Linus, Felea, Daniel, Feliciello, Alessandro, Fenton-Olsen, Bo, Feofilov, Grigory, Fernandez Tellez, Arturo, Ferretti, Alessandro, Altsybeev, Igor, Festanti, Andrea, Figiel, Jan, Figueredo, Marcel, Filchagin, Sergey, Finogeev, Dmitry, Fionda, Fiorella, Fiore, Enrichetta Maria, Floratos, Emmanuel, Floris, Michele, Foertsch, Siegfried Valentin, Andrei, Cristian, Foka, Panagiota, Fokin, Sergey, Fragiacomo, Enrico, Francescon, Andrea, Frankenfeld, Ulrich Michael, Fuchs, Ulrich, Furget, Christophe, Fusco Girard, Mario, Gaardhoje, Jens Joergen, Gagliardi, Martino, Andronic, Anton, Gago, Alberto, Gallio, Mauro, Gangadharan, Dhevan Raja, Ganoti, Paraskevi, Garabatos, Jose, Garcia-Solis, Edmundo, Gargiulo, Corrado, Garishvili, Irakli, Gerhard, Jochen, Germain, Marie, Anguelov, Venelin, Geuna, Claudio, Gheata, Andrei George, Gheata, Mihaela, Ghidini, Bruno, Ghosh, Premomoy, Gianotti, Paola, Girard, Martin Robert, Giubellino, Paolo, Gladysz-Dziadus, Ewa, Glassel, Peter, Adamova, Dagmar, Anielski, Jonas, Gomez, Ramon, Gonzalez Ferreiro, Elena, Gonzalez-Trueba, Laura Helena, Gonzalez-Zamora, Pedro, Gorbunov, Sergey, Goswami, Ankita, Gotovac, Sven, Graczykowski, Lukasz Kamil, Grajcarek, Robert, Grelli, Alessandro, Anson, Christopher Daniel, Grigoras, Alina Gabriela, Grigoras, Costin, Grigoriev, Vladislav, Grigoryan, Smbat, Grigoryan, Ara, Grinyov, Boris, Grion, Nevio, Gros, Philippe, Grosse-Oetringhaus, Jan Fiete, Grossiord, Jean-Yves, Anticic, Tome, Grosso, Raffaele, Guber, Fedor, Guernane, Rachid, Guerzoni, Barbara, Guilbaud, Maxime Rene Joseph, Gulbrandsen, Kristjan Herlache, Gulkanyan, Hrant, Gunji, Taku, Gupta, Ramni, Gupta, Anik, Antinori, Federico, Haake, Rudiger, Haaland, Oystein Senneset, Hadjidakis, Cynthia Marie, Haiduc, Maria, Hamagaki, Hideki, Hamar, Gergoe, Han, Byounghee, Hanratty, Luke David, Hansen, Alexander, Harmanova, Zuzana, Antonioli, Pietro, Harris, John William, Hartig, Matthias, Harton, Austin, Hatzifotiadou, Despoina, Hayashi, Shinichi, Hayrapetyan, Arsen, Heckel, Stefan Thomas, Heide, Markus Ansgar, Helstrup, Haavard, Herghelegiu, Andrei Ionut, Aphecetche, Laurent Bernard, Herrera Corral, Gerardo Antonio, Herrmann, Norbert, Hess, Benjamin Andreas, Hetland, Kristin Fanebust, Hicks, Bernard, Hippolyte, Boris, Hori, Yasuto, Hristov, Peter Zahariev, Hrivnacova, Ivana, Huang, Meidana, Appelshauser, Harald, Humanic, Thomas, Hwang, Dae Sung, Ichou, Raphaelle, Ilkaev, Radiy, Ilkiv, Iryna, Inaba, Motoi, Incani, Elisa, Innocenti, Gian Michele, Innocenti, Pier Giorgio, Ippolitov, Mikhail, Arbor, Nicolas, Irfan, Muhammad, Ivan, Cristian George, Ivanov, Marian, Ivanov, Andrey, Ivanov, Vladimir, Ivanytskyi, Oleksii, Jacholkowski, Adam Wlodzimierz, Jacobs, Peter, Jang, Haeng Jin, Janik, Malgorzata Anna, Arcelli, Silvia, Janik, Rudolf, Jayarathna, Sandun, Jena, Satyajit, Jha, Deeptanshu Manu, Jimenez Bustamante, Raul Tonatiuh, Jones, Peter Graham, Jung, Hyung Taik, Jusko, Anton, Kaidalov, Alexei, Kalcher, Sebastian, Arend, Andreas, Kalinak, Peter, Kalliokoski, Tuomo Esa Aukusti, Kalweit, Alexander Philipp, Kang, Ju Hwan, Kaplin, Vladimir, Karasu Uysal, Ayben, Karavichev, Oleg, Karavicheva, Tatiana, Karpechev, Evgeny, Kazantsev, Andrey, Adare, Andrew Marshall, Armesto, Nestor, Kebschull, Udo Wolfgang, Keidel, Ralf, Khan, Mohisin Mohammed, Khan, Kamal Hussain, Khan, Palash, Khan, Shuaib Ahmad, Khanzadeev, Alexei, Kharlov, Yury, Kileng, Bjarte, Kim, Taesoo, Arnaldi, Roberta, Kim, Jin Sook, Kim, Dong Jo, Kim, Se Yong, Kim, Minwoo, Kim, Beomkyu, Kim, Mimae, Kim, Do Won, Kim, Jonghyun, Kirsch, Stefan, Kisel, Ivan, Aronsson, Tomas Robert, Kiselev, Sergey, Kisiel, Adam Ryszard, Klay, Jennifer Lynn, Klein, Jochen, Klein-Bosing, Christian, Kliemant, Michael, Kluge, Alexander, Knichel, Michael Linus, Knospe, Anders Garritt, Kohler, Markus, Arsene, Ionut Cristian, Kollegger, Thorsten, Kolojvari, Anatoly, Kompaniets, Mikhail, Kondratiev, Valery, Kondratyeva, Natalia, Konevskih, Artem, Kovalenko, Vladimir, Kowalski, Marek, Kox, Serge, Koyithatta Meethaleveedu, Greeshma, Arslandok, Mesut, Kral, Jiri, Kralik, Ivan, Kramer, Frederick, Kravcakova, Adela, Krawutschke, Tobias, Krelina, Michal, Kretz, Matthias, Krivda, Marian, Krizek, Filip, Krus, Miroslav, Asryan, Andzhey, Kryshen, Evgeny, Krzewicki, Mikolaj, Kucheriaev, Yury, Kugathasan, Thanushan, Kuhn, Christian Claude, Kuijer, Paul, Kulakov, Igor, Kumar, Jitendra, Kurashvili, Podist, Kurepin, A, Augustinus, Andre, Kurepin, AB, Kuryakin, Alexey, Kushpil, Svetlana, Kushpil, Vasily, Kvaerno, Henning, Kweon, Min Jung, Kwon, Youngil, Ladron de Guevara, Pedro, Lakomov, Igor, Langoy, Rune, Averbeck, Ralf Peter, La Pointe, Sarah Louise, Lara, Camilo Ernesto, Lardeux, Antoine Xavier, La Rocca, Paola, Lea, Ramona, Lechman, Mateusz, Lee, Ki Sang, Lee, Graham Richard, Lee, Sung Chul, Legrand, Iosif, Awes, Terry, Lehnert, Joerg Walter, Lemmon, Roy Crawford, Lenhardt, Matthieu Laurent, Lenti, Vito, Leon, Hermes, Leon Monzon, Ildefonso, Leon Vargas, Hermes, Levai, Peter, Li, Shuang, Lien, Jorgen, Aysto, Juha Heikki, Lietava, Roman, Lindal, Svein, Lindenstruth, Volker, Lippmann, Christian, Lisa, Michael Annan, Ljunggren, Hans Martin, Lodato, Davide Francesco, Loenne, Per-Ivar, Loggins, Vera, Loginov, Vitaly, Aggarwal, Madan, Azmi, Mohd Danish, Lohner, Daniel, Loizides, Constantinos, Loo, Kai Krister, Lopez, Xavier Bernard, Lopez Torres, Ernesto, Lovhoiden, Gunnar, Lu, Xianguo, Luettig, Philipp, Lunardon, Marcello, Luo, Jiebin, Bach, Matthias Jakob, Luparello, Grazia, Luzzi, Cinzia, Ma, Rongrong, Ma, Ke, Madagodahettige-Don, Dilan Minthaka, Maevskaya, Alla, Mager, Magnus, Mahapatra, Durga Prasad, Maire, Antonin, Malaev, Mikhail, Badala, Angela, Maldonado Cervantes, Ivonne Alicia, Malinina, Ludmila, Mal'Kevich, Dmitry, Malzacher, Peter, Mamonov, Alexander, Manceau, Loic Henri Antoine, Mangotra, Lalit Kumar, Manko, Vladislav, Manso, Franck, Manukyan, Narine, Baek, Yong Wook, Manzari, Vito, Mao, Yaxian, Marchisone, Massimiliano, Mares, Jiri, Margagliotti, Giacomo Vito, Margotti, Anselmo, Marin, Ana Maria, Markert, Christina, Marquard, Marco, Martashvili, Irakli, Bailhache, Raphaelle Marie, Martin, Nicole Alice, Martinengo, Paolo, Martinez, Mario Ivan, Martinez Davalos, Arnulfo, Martinez Garcia, Gines, Martynov, Yevgen, Mas, Alexis Jean-Michel, Masciocchi, Silvia, Masera, Massimo, Masoni, Alberto, Bala, Renu, Massacrier, Laure Marie, Mastroserio, Annalisa, Matyja, Adam Tomasz, Mayer, Christoph, Mazer, Joel, Mazzoni, Alessandra Maria, Meddi, Franco, Menchaca-Rocha, Arturo Alejandro, Mercado Perez, Jorge, Meres, Michal, Baldisseri, Alberto, Miake, Yasuo, Mikhaylov, Konstantin, Milano, Leonardo, Milosevic, Jovan, Mischke, Andre, Mishra, Aditya Nath, Miskowiec, Dariusz, Mitu, Ciprian Mihai, Mizuno, Sanshiro, Mlynarz, Jocelyn, Baltasar Dos Santos Pedrosa, Fernando, Mohanty, Bedangadas, Molnar, Levente, Montano Zetina, Luis Manuel, Monteno, Marco, Montes, Esther, Moon, Taebong, Morando, Maurizio, Moreira De Godoy, Denise Aparecida, Moretto, Sandra, Morreale, Astrid, Ban, Jaroslav, Morsch, Andreas, Muccifora, Valeria, Mudnic, Eugen, Muhuri, Sanjib, Mukherjee, Maitreyee, Muller, Hans, Munhoz, Marcelo, Murray, Sean, Musa, Luciano, Musinsky, Jan, Baral, Rama Chandra, Nandi, Basanta Kumar, Nania, Rosario, Nappi, Eugenio, Nattrass, Christine, Nayak, Tapan Kumar, Nazarenko, Sergey, Nedosekin, Alexander, Nicassio, Maria, Niculescu, Mihai, Nielsen, Borge Svane, Aglieri Rinella, Gianluca, Barbera, Roberto, Niida, Takafumi, Nikolaev, Sergey, Nikolic, Vedran, Nikulin, Sergey, Nikulin, Vladimir, Nilsen, Bjorn Steven, Nilsson, Mads Stormo, Noferini, Francesco, Nomokonov, Petr, Nooren, Gerardus, Barile, Francesco, Nyanin, Alexandre, Nyatha, Anitha, Nygaard, Casper, Nystrand, Joakim Ingemar, Ochirov, Alexander, Oeschler, Helmut Oskar, Oh, Sun Kun, Oh, Saehanseul, Oleniacz, Janusz, Oliveira Da Silva, Antonio Carlos, Barnafoldi, Gergely Gabor, Oppedisano, Chiara, Ortiz Velasquez, Antonio, Oskarsson, Anders Nils Erik, Ostrowski, Piotr Krystian, Otwinowski, Jacek Tomasz, Oyama, Ken, Ozawa, Kyoichiro, Pachmayer, Yvonne Chiara, Pachr, Milos, Padilla, Fatima, Barnby, Lee Stuart, Pagano, Paola, Paic, Guy, Painke, Florian, Pajares, Carlos, Pal, Susanta Kumar, Palaha, Arvinder Singh, Palmeri, Armando, Papikyan, Vardanush, Pappalardo, Giuseppe, Park, Woo Jin, Barret, Valerie, Passfeld, Annika, Patalakha, Dmitri Ivanovich, Paticchio, Vincenzo, Paul, Biswarup, Pavlinov, Alexei, Pawlak, Tomasz Jan, Peitzmann, Thomas, Pereira Da Costa, Hugo Denis Antonio, Pereira De Oliveira Filho, Elienos, Peresunko, Dmitri, Bartke, Jerzy Gustaw, Perez Lara, Carlos Eugenio, Perrino, Davide, Peryt, Wiktor Stanislaw, Pesci, Alessandro, Peskov, Vladimir, Pestov, Yury, Petracek, Vojtech, Petran, Michal, Petris, Mariana, Petrov, Plamen Rumenov, Basile, Maurizio, Petrovici, Mihai, Petta, Catia, Piano, Stefano, Pikna, Miroslav, Pillot, Philippe, Pinazza, Ombretta, Pinsky, Lawrence, Pitz, Nora, Piyarathna, Danthasinghe, Planinic, Mirko, Bastid, Nicole, Ploskon, Mateusz Andrzej, Pluta, Jan Marian, Pocheptsov, Timur, Pochybova, Sona, Podesta Lerma, Pedro Luis Manuel, Poghosyan, Martin, Polak, Karel, Polichtchouk, Boris, Poljak, Nikola, Pop, Amalia, Basu, Sumit, Porteboeuf-Houssais, Sarah, Pospisil, Vladimir, Potukuchi, Baba, Prasad, Sidharth Kumar, Preghenella, Roberto, Prino, Francesco, Pruneau, Claude Andre, Pshenichnov, Igor, Puddu, Giovanna, Punin, Valery, Bathen, Bastian, Putis, Marian, Putschke, Jorn Henning, Qvigstad, Henrik, Rachevski, Alexandre, Rademakers, Alphonse, Raiha, Tomi Samuli, Rak, Jan, Rakotozafindrabe, Andry Malala, Ramello, Luciano, Ramirez Reyes, Abdiel, Agnello, Michelangelo, Batigne, Guillaume, Raniwala, Sudhir, Raniwala, Rashmi, Rasanen, Sami Sakari, Rascanu, Bogdan Theodor, Rathee, Deepika, Read, Kenneth Francis, Real, Jean-Sebastien, Redlich, Krzysztof, Reed, Rosi Jan, Rehman, Attiq Ur, Batyunya, Boris, Reichelt, Patrick, Reicher, Martijn, Renfordt, Rainer Arno Ernst, Reolon, Anna Rita, Reshetin, Andrey, Rettig, Felix Vincenz, Revol, Jean-Pierre, Reygers, Klaus Johannes, Riccati, Lodovico, Ricci, Renato Angelo, Baumann, Christoph Heinrich, Richert, Tuva, Richter, Matthias Rudolph, Riedler, Petra, Riegler, Werner, Riggi, Francesco, Rodriguez Cahuantzi, Mario, Rodriguez Manso, Alis, Roed, Ketil, Rogochaya, Elena, Rohr, David, Bearden, Ian Gardner, Rohrich, Dieter, Romita, Rosa, Ronchetti, Federico, Rosnet, Philippe, Rossegger, Stefan, Rossi, Andrea, Roy, Christelle Sophie, Roy, Pradip Kumar, Rubio Montero, Antonio Juan, Rui, Rinaldo, Beck, Hans, Russo, Riccardo, Ryabinkin, Evgeny, Rybicki, Andrzej, Sadovsky, Sergey, Safarik, Karel, Sahoo, Raghunath, Sahu, Pradip Kumar, Saini, Jogender, Sakaguchi, Hiroaki, Sakai, Shingo, Behera, Nirbhay Kumar, Sakata, Dosatsu, Salgado, Carlos Albert, Salzwedel, Jai, Sambyal, Sanjeev Singh, Samsonov, Vladimir, Sanchez Castro, Xitzel, Sandor, Ladislav, Sandoval, Andres, Sano, Masato, Santagati, Gianluca, Belikov, Iouri, Santoro, Romualdo, Sarkamo, Juho Jaako, Scapparone, Eugenio, Scarlassara, Fernando, Scharenberg, Rolf Paul, Schiaua, Claudiu Cornel, Schicker, Rainer Martin, Schmidt, Hans Rudolf, Schmidt, Christian Joachim, Schuchmann, Simone, Bellini, Francesca, Schukraft, Jurgen, Schuster, Tim, Schutz, Yves Roland, Schwarz, Kilian Eberhard, Schweda, Kai Oliver, Scioli, Gilda, Scomparin, Enrico, Scott, Rebecca, Scott, Patrick Aaron, Segato, Gianfranco, Bellwied, Rene, Selyuzhenkov, Ilya, Senyukov, Serhiy, Seo, Jeewon, Serci, Sergio, Serradilla, Eulogio, Sevcenco, Adrian, Shabetai, Alexandre, Shabratova, Galina, Shahoyan, Ruben, Sharma, Satish, Belmont-Moreno, Ernesto, Sharma, Natasha, Sharma, Rohni, Shigaki, Kenta, Shtejer, Katherin, Sibiriak, Yury, Sicking, Eva, Siddhanta, Sabyasachi, Siemiarczuk, Teodor, Silvermyr, David Olle Rickard, Silvestre, Catherine, Agocs, Andras Gabor, Bencedi, Gyula, Simatovic, Goran, Simonetti, Giuseppe, Singaraju, Rama Narayana, Singh, Ranbir, Singha, Subhash, Singhal, Vikas, Sinha, Tinku, Sinha, Bikash, Sitar, Branislav, Sitta, Mario, Beole, Stefania, Skaali, Bernhard, Skjerdal, Kyrre, Smakal, Radek, Smirnov, Nikolai, Snellings, Raimond, Sogaard, Carsten, Soltz, Ron Ariel, Son, Hyungsuk, Song, Jihye, Song, Myunggeun, Berceanu, Ionela, Soos, Csaba, Soramel, Francesca, Sputowska, Iwona, Spyropoulou-Stassinaki, Martha, Srivastava, Brijesh Kumar, Stachel, Johanna, Stan, Ionel, Stefanek, Grzegorz, Steinpreis, Matthew, Stenlund, Evert Anders, Bercuci, Alexandru, Steyn, Gideon Francois, Stiller, Johannes Hendrik, Stocco, Diego, Stolpovskiy, Mikhail, Strmen, Peter, Suaide, Alexandre Alarcon do Passo, Subieta Vasquez, Martin Alfonso, Sugitate, Toru, Suire, Christophe Pierre, Sultanov, Rishat, Berdnikov, Yaroslav, Sumbera, Michal, Susa, Tatjana, Symons, Timothy, Szanto de Toledo, Alejandro, Szarka, Imrich, Szczepankiewicz, Adam, Szymanski, Maciej, Takahashi, Jun, Tangaro, Marco-Antonio, Tapia Takaki, Daniel Jesus, Berenyi, Daniel, Tarantola Peloni, Attilio, Tarazona Martinez, Alfonso, Tauro, Arturo, Tejeda Munoz, Guillermo, Telesca, Adriana, Ter-Minasyan, Astkhik, Terrevoli, Cristina, Thader, Jochen Mathias, Thomas, Deepa, Tieulent, Raphael Noel, Bergognon, Anais Annick Erica, Timmins, Anthony, Tlusty, David, Toia, Alberica, Torii, Hisayuki, Toscano, Luca, Trubnikov, Victor, Truesdale, David Christopher, Trzaska, Wladyslaw Henryk, Tsuji, Tomoya, Tumkin, Alexandr, Berzano, Dario, Turrisi, Rosario, Tveter, Trine Spedstad, Ulery, Jason Glyndwr, Ullaland, Kjetil, Ulrich, Jochen, Uras, Antonio, Urciuoli, Guido Marie, Usai, Gianluca, Vajzer, Michal, Vala, Martin, Betev, Latchezar, Valencia Palomo, Lizardo, Vande Vyvre, Pierre, van Leeuwen, Marco, Vannucci, Luigi, Vargas, Aurora Diozcora, Varma, Raghava, Vasileiou, Maria, Vasiliev, Andrey, Vechernin, Vladimir, Veldhoen, Misha, Bhasin, Anju, Venaruzzo, Massimo, Vercellin, Ermanno, Vergara, Sergio, Vernet, Renaud, Verweij, Marta, Vickovic, Linda, Viesti, Giuseppe, Viinikainen, Jussi, Vilakazi, Zabulon, Villalobos Baillie, Orlando, Agostinelli, Andrea, Bhati, Ashok Kumar, Vinogradov, Leonid, Vinogradov, Yury, Vinogradov, Alexander, Virgili, Tiziano, Viyogi, Yogendra, Vodopianov, Alexander, Volkl, Martin Andreas, Voloshin, Sergey, Voloshin, Kirill, Volpe, Giacomo, Bhom, Jihyun, von Haller, Barthelemy, Vorobyev, Ivan, Vranic, Danilo, Vrlakova, Janka, Vulpescu, Bogdan, Vyushin, Alexey, Wagner, Vladimir, Wagner, Boris, Wan, Renzhuo, Wang, Yaping, Bianchi, Livio, Wang, Mengliang, Wang, Dong, Wang, Yifei, Watanabe, Kengo, Weber, Michael, Wessels, Johannes, Westerhoff, Uwe, Wiechula, Jens, Wikne, Jon, Wilde, Martin Rudolf, Bianchi, Nicola, Wilk, Alexander, Wilk, Grzegorz Andrzej, Williams, Crispin, Windelband, Bernd Stefan, Xaplanteris Karampatsos, Leonidas, Yaldo, Chris G, Yamaguchi, Yorito, Yang, Hongyan, Yang, Shiming, Yasnopolsky, Stanislav, Bielcik, Jaroslav, Yi, JunGyu, Yin, Zhongbao, Yoo, In-Kwon, Yoon, Jongik, Yu, Weilin, Yuan, Xianbao, Yushmanov, Igor, Zaccolo, Valentina, Zach, Cenek, Zampolli, Chiara, Bielcikova, Jana, Zaporozhets, Sergey, Zarochentsev, Andrey, Zavada, Petr, Zaviyalov, Nikolai, Zbroszczyk, Hanna Paulina, Zelnicek, Pierre, Zgura, Sorin Ion, Zhalov, Mikhail, Zhang, Xiaoming, Zhang, Haitao, Bilandzic, Ante, Zhou, You, Zhou, Fengchu, Zhou, Daicui, Zhu, Jianlin, Zhu, Jianhui, Zhu, Xiangrong, Zhu, Hongsheng, Zichichi, Antonino, Zimmermann, Alice, Zinovjev, Gennady, Bjelogrlic, Sandro, Zoccarato, Yannick Denis, Zynovyev, Mykhaylo, Zyzak, Maksym, Blanco, Francesco, Blanco, F, and Universidade Estadual de Campinas
Subjects: Chemical Freeze-out, Quark-gluon Plasma, Collaboration, High Energy Physics - Experiment, Subatomär fysik, Heavy-ion Collisions, Qcd Phase-transition, Total Cross-sections, Models, centrality dependence, MESON PRODUCTION, Subatomic Physics, Perspective, Nuclear Experiment, Hadron-production, Particle Physics - Experiment, Nucleus-nucleus Collisions
Abstract: In this paper measurements are presented of $\pi^\pm, K^\pm$, p and $\bar p$ production at mid-rapidity (|y| < 0.5), in Pb–Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV as a function of centrality. The measurement covers the transverse momentum ($p_T$) range from 100, 200, 300 MeV/c up to 3, 3, 4.6 GeV/c, for $\pi$, K, and p respectively. The measured $p_T$ distributions and yields are compared to expectations based on hydrodynamic, thermal and recombination models. The spectral shapes of central collisions show a stronger radial flow than measured at lower energies, which can be described in hydrodynamic models. In peripheral collisions, the $p_T$ distributions are not well reproduced by hydrodynamic models. Ratios of integrated particle yields are found to be nearly independent of centrality. The yield of protons normalized to pions is a factor ~ 1.5 lower than the expectation from thermal models. In this paper measurements are presented of π±, K±, p, and p¯ production at midrapidity (|y
Published: 2013

40. Centrality dependence of pi, K, and p production in Pb-Pb collisions at root s(NN)=2.76 TeV

Author: Abelev, B., Adam, J., Adamova, D., Adare, A. M., Aggarwal, M. M., Rinella, G., Agnello, Michelangelo, Agocs, A. G., Agostinelli, A., Ahammed, Z., Ahmad, N., Ahmad, A., Ahn, S. A., Ahn, S. U., Aimo, Ilaria, Ajaz, M., Akindinov, A., Aleksandrov, D., Alessandro, B., Alici, A., Alkin, A., Avina, E., Alme, J., Alt, T., Altini, V., Altinpinar, S., Altsybeev, I., Andrei, C., Andronic, A., Aguelov, V., Anielski, J., Anson, C., Antičić, T., Antinori, F., Antonioli, P., and Bufalino, Stefania
Subjects: NUCLEUS-NUCLEUS COLLISIONS, HEAVY-ION COLLISIONS, QCD PHASE-TRANSITION, QUARK-GLUON PLASMA, TOTAL CROSS-SECTIONS, CHEMICAL FREEZE-OUT, HADRON-PRODUCTION
Published: 2013

41. Centrality dependence of pi, K, and p production in Pb-Pb collisions at root s(NN)=2.76 TeV

Author: ABELEV, B, ADAM, J, ADAMOVA, D, ADARE, AM, AGGARWAL, MM, RINELLA, GA, AGNELLO, M, AGOCS, AG, AGOSTINELLI, A, AHAMMED, Z, AHMAD, N, MASOODI, AA, AHN, SA, AHN, SU, AJAZ, M, AKINDINOV, A, ALEKSANDROV, D, ALESSANDRO, B, ALICI, A, ALKIN, A, AVINA, EA, ALME, J, ALT, T, ALTINI, V, ALTINPINAR, S, ALTSYBEEV, I, ANDREI, C, ANDRONIC, A, ANGUELOV, V, ANIELSKI, J, ANSON, C, ANTICIC, T, ANTINORI, F, ANTONIOLI, P, APHECETCHE, L, APPELSHAUSER, H, ARBOR, N, ARCELLI, S, AREND, A, ARMESTO, N, ARNALDI, R, ARONSSON, T, ARSENE, IC, ARSLANDOK, M, ASRYAN, A, AUGUSTINUS, A, AVERBECK, R, AWES, TC, AYSTO, J, AZMI, MD, BACH, M, BADALA, A, BAEK, YW, BAILHACHE, R, BALA, R, BALDISSERI, A, PEDROSA, FBD, BAN, J, BARAL, RC, BARBERA, R, BARILE, F, BARNAFOLDI, GG, BARNBY, LS, BARRET, V, BARTKE, J, BASILE, M, BASTID, N, BASU, S, BATHEN, B, BATIGNE, G, BATYUNYA, B, BAUMANN, C, BEARDEN, IG, BECK, H, BEHERA, NK, BELIKOV, I, BELLINI, F, BELLWIED, R, BELMONT-MORENO, E, BENCEDI, G, BEOLE, S, BERCEANU, I, BERCUCI, A, BERDNIKOV, Y, BERENYI, D, BERGOGNON, AAE, BERZANO, D, BETEV, L, BHASIN, A, BHATI, AK, BHOM, J, BIANCHI, L, BIANCHI, N, BIELCIK, J, BIELCIKOVA, J, BILANDZIC, A, BJELOGRLIC, S, BLANCO, F, BLAU, D, BLUME, C, BOCCIOLI, M, BOTTGER, S, BOGDANOV, A, BOGGILD, H, BOGOLYUBSKY, M, BOLDIZSAR, L, BOMBARA, M, BOOK, J, BOREL, H, BORISSOV, A, BOSSU, F, BOTJE, M, BOTTA, E, BRAIDOT, E, BRAUN-MUNZINGER, P, BREGANT, M, BREITNER, T, BROKER, TA, BROWNING, TA, BROZ, M, BRUN, R, BRUNA, E, BRUNO, GE, BUDNIKOV, D, BUESCHING, H, BUFALINO, S, BUNCIC, P, BUSCH, O, BUTHELEZI, Z, CAFFARRI, D, CAI, X, CAINES, H, VILLAR, EC, CAMERINI, P, ROMAN, VC, ROMEO, GC, CARENA, F, CARENA, W, CARLIN, N, CARMINATI, F, DIAZ, AC, CASTELLANOS, JC, HERNANDEZ, JFC, CASULA, EAR, CATANESCU, V, CAVICCHIOLI, C, SANCHEZ, CC, CEPILA, J, CERELLO, P, CHANG, B, CHAPELAND, S, CHARVET, JL, CHATTOPADHYAY, S, CHERNEY, M, CHESHKOV, C, CHEYNIS, B, BARROSO, VC, CHINELLATO, DD, CHOCHULA, P, CHOJNACKI, M, CHOUDHURY, S, CHRISTAKOGLOU, P, CHRISTENSEN, CH, CHRISTIANSEN, P, CHUJO, T, CHUNG, SU, CICALO, C, CIFARELLI, L, CINDOLO, F, CLEYMANS, J, COLAMARIA, F, COLELLA, D, COLLU, A, BALBASTRE, GC, DEL VALLE, ZC, CONNORS, ME, CONTIN, G, CONTRERAS, JG, CORMIER, M, MORALES, YC, CORTESE, P, MALDONADO, IC, COSENTINO, MR, COSTA, F, COTALLO, ME, CRESCIO, E, CROCHET, P, ALANIZ, EC, ALBINO, RC, CUAUTLE, E, CUNQUEIRO, L, DAINESE, A, DANU, A, DAS, K, DAS, I, DAS, S, DAS, D, DASH, S, DASH, A, DE, S, DE BARROS, GOV, DE CARO, A, DE CATALDO, G, DE CUVELAND, J, DE FALCO, A, DE GRUTTOLA, D, DELAGRANGE, H, DE MARCO, N, DENES, E, DE PASQUALE, S, DEPPMAN, A, ERASMO, GD, DE ROOIJ, R, CORCHERO, MAD, DI BARI, D, DIETEL, T, DI GIGLIO, C, DI LIBERTO, S, DI MAURO, A, DI NEZZA, P, DIVIA, R, DJUVSLAND, O, DOBRIN, A, DOBROWOLSKI, T, DONIGUS, B, DORDIC, O, DRIGA, O, DUBEY, AK, DUBLA, A, DUCROUX, L, DUPIEUX, P, MAJUMDAR, AKD, ELIA, D, EMSCHERMANN, D, ENGEL, H, ERAZMUS, B, ERDAL, HA, ESPAGNON, B, ESTIENNE, M, ESUMI, S, EVANS, D, EYYUBOVA, G, FABRIS, D, FAIVRE, J, FALCHIERI, D, FANTONI, A, FASEL, M, FEARICK, R, FEHLKER, D, FELDKAMP, L, FELEA, D, FELICIELLO, A, FENTON-OLSEN, B, FEOFILOV, G, TELLEZ, AF, FERRETTI, A, FESTANTI, A, FIGIEL, J, FIGUEREDO, MAS, FILCHAGIN, S, FINOGEEV, D, FIONDA, FM, FIORE, EM, FLORATOS, E, FLORIS, M, FOERTSCH, S, FOKA, P, FOKIN, S, FRAGIACOMO, E, FRANCESCON, A, FRANKENFELD, U, FUCHS, U, FURGET, C, GIRARD, MF, GAARDHOJE, JJ, GAGLIARDI, M, GAGO, A, GALLIO, M, GANGADHARAN, DR, GANOTI, P, GARABATOS, C, GARCIA-SOLIS, E, GARGIULO, C, GARISHVILI, I, GERHARD, J, GERMAIN, M, GEUNA, C, GHEATA, A, GHEATA, M, GHIDINI, B, GHOSH, P, GIANOTTI, P, GIRARD, MR, GIUBELLINO, P, GLADYSZ-DZIADUS, E, GLASSEL, P, GOMEZ, R, FERREIRO, EG, GONZALEZ-TRUEBA, LH, GONZALEZ-ZAMORA, P, GORBUNOV, S, GOSWAMI, A, GOTOVAC, S, GRACZYKOWSKI, LK, GRAJCAREK, R, GRELLI, A, GRIGORAS, A, GRIGORAS, C, GRIGORIEV, V, GRIGORYAN, S, GRIGORYAN, A, GRINYOV, B, GRION, N, GROS, P, GROSSE-OETRINGHAUS, JF, GROSSIORD, JY, GROSSO, R, GUBER, F, GUERNANE, R, GUERZONI, B, GUILBAUD, M, 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PETRACEK, V, PETRAN, M, PETRIS, M, PETROV, P, PETROVICI, M, PETTA, C, PIANO, S, PIKNA, M, PILLOT, P, PINAZZA, O, PINSKY, L, PITZ, N, PIYARATHNA, DB, PLANINIC, M, PLOSKON, M, PLUTA, J, POCHEPTSOV, T, POCHYBOVA, S, PODESTA-LERMA, PLM, POGHOSYAN, MG, POLAK, K, POLICHTCHOUK, B, POLJAK, N, POP, A, PORTEBOEUF-HOUSSAIS, S, POSPISIL, V, POTUKUCHI, B, PRASAD, SK, PREGHENELLA, R, PRINO, F, PRUNEAU, CA, PSHENICHNOV, I, PUDDU, G, PUNIN, V, PUTIS, M, PUTSCHKE, J, QVIGSTAD, H, RACHEVSKI, A, RADEMAKERS, A, RAIHA, TS, RAK, J, RAKOTOZAFINDRABE, A, RAMELLO, L, REYES, AR, RANIWALA, S, RANIWALA, R, RASANEN, SS, RASCANU, BT, RATHEE, D, READ, KF, REAL, JS, REDLICH, K, REED, RJ, REHMAN, A, REICHELT, P, REICHER, M, RENFORDT, R, REOLON, AR, RESHETIN, A, RETTIG, F, REVOL, JP, REYGERS, K, RICCATI, L, RICCI, RA, RICHERT, T, RICHTER, M, RIEDLER, P, RIEGLER, W, RIGGI, F, CAHUANTZI, MR, MANSO, AR, ROED, K, ROGOCHAYA, E, ROHR, D, ROHRICH, D, ROMITA, R, RONCHETTI, F, ROSNET, P, ROSSEGGER, S, ROSSI, A, ROY, C, ROY, P, MONTERO, AJR, RUI, R, RUSSO, R, RYABINKIN, E, RYBICKI, A, SADOVSKY, S, SAFARIK, K, SAHOO, R, SAHU, PK, SAINI, J, SAKAGUCHI, H, SAKAI, S, SAKATA, D, SALGADO, CA, SALZWEDEL, J, SAMBYAL, S, SAMSONOV, V, CASTRO, XS, SANDOR, L, SANDOVAL, A, SANO, M, SANTAGATI, G, SANTORO, R, SARKAMO, J, SCAPPARONE, E, SCARLASSARA, F, SCHARENBERG, RP, SCHIAUA, C, SCHICKER, R, SCHMIDT, HR, SCHMIDT, C, SCHUCHMANN, S, SCHUKRAFT, J, SCHUSTER, T, SCHUTZ, Y, SCHWARZ, K, SCHWEDA, K, SCIOLI, G, SCOMPARIN, E, SCOTT, R, SCOTT, PA, SEGATO, G, SELYUZHENKOV, I, SENYUKOV, S, SEO, J, SERCI, S, SERRADILLA, E, SEVCENCO, A, SHABETAI, A, SHABRATOVA, G, SHAHOYAN, R, SHARMA, S, SHARMA, N, ROHNI, S, SHIGAKI, K, SHTEJER, K, SIBIRIAK, Y, SICKING, E, SIDDHANTA, S, SIEMIARCZUK, T, SILVERMYR, D, SILVESTRE, C, SIMATOVIC, G, SIMONETTI, G, SINGARAJU, R, SINGH, R, SINGHA, S, SINGHAL, V, SINHA, T, SINHA, BC, SITAR, B, SITTA, M, SKAALI, TB, SKJERDAL, K, SMAKAL, R, SMIRNOV, N, SNELLINGS, RJM, SOGAARD, C, SOLTZ, R, SON, H, SONG, J, SONG, M, 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BAILLIE, OV, VINOGRADOV, L, VINOGRADOV, Y, VINOGRADOV, A, VIRGILI, T, VIYOGI, YP, VODOPYANOV, A, VOELKL, MA, VOLOSHIN, S, VOLOSHIN, K, VOLPE, G, VON HALLER, B, VOROBYEV, I, VRANIC, D, VRLAKOVA, J, VULPESCU, B, VYUSHIN, A, WAGNER, V, WAGNER, B, WAN, R, WANG, Y, WANG, M, WANG, D, WATANABE, K, WEBER, M, WESSELS, JP, WESTERHOFF, U, WIECHULA, J, WIKNE, J, WILDE, M, WILK, A, WILK, G, WILLIAMS, MCS, WINDELBAND, B, KARAMPATSOS, LX, YALDO, CG, YAMAGUCHI, Y, YANG, H, YANG, S, YASNOPOLSKIY, S, YI, J, YIN, Z, YOO, IK, YOON, J, YU, W, YUAN, X, YUSHMANOV, I, ZACCOLO, V, ZACH, C, ZAMPOLLI, C, ZAPOROZHETS, S, ZAROCHENTSEV, A, ZAVADA, P, ZAVIYALOV, N, ZBROSZCZYK, H, ZELNICEK, P, ZGURA, IS, ZHALOV, M, ZHANG, X, ZHANG, H, ZHOU, Y, ZHOU, F, ZHOU, D, ZHU, J, ZHU, X, ZHU, H, ZICHICHI, A, ZIMMERMANN, A, ZINOVJEV, G, ZOCCARATO, Y, ZYNOVYEV, M, and ZYZAK, M
Subjects: Nucleus-Nucleus Collisions, Models, Chemical Freeze-Out, Perspective, Subatomic Physics, Quark-Gluon Plasma, Heavy-Ion Collisions, Hadron-Production, Nuclear Experiment, Total Cross-Sections, Collaboration, Qcd Phase-Transition
Abstract: In this paper measurements are presented of pi(+/-), K-+/-, p, and (p) over bar production at midrapidity (vertical bar y vertical bar < 0.5), in Pb-Pb collisions at root s(NN) = 2.76 TeV as a function of centrality. The measurement covers the transverse-momentum (p(T)) range from 100, 200, and 300 MeV/c up to 3, 3, and 4.6 GeV/c for pi, K, and p, respectively. The measured p(T) distributions and yields are compared to expectations based on hydrodynamic, thermal and recombination models. The spectral shapes of central collisions show a stronger radial flow than measured at lower energies, which can be described in hydrodynamic models. In peripheral collisions, the p(T) distributions are not well reproduced by hydrodynamic models. Ratios of integrated particle yields are found to be nearly independent of centrality. The yield of protons normalized to pions is a factor similar to 1.5 lower than the expectation from thermal models.
Published: 2013

42. Isospin decomposition of the basic double-pionic fusion in the region of the ABC effect

Author: P. Wüstner, M. Mikirtychiants, Magdalena Skurzok, H. Ströher, K. Grigoryev, Pawel Marciniewski, Tord Johansson, V. Serdyuk, Jerzy Smyrski, A. Magiera, S. Sawant, H. Stockhorst, Frank Goldenbaum, M. Żurek, G. Sterzenbach, L. Jarczyk, C.-O. Gullström, James Ritman, Markus Büscher, M. Krapp, A. Pricking, W. Erven, B. Mariański, P. Adlarson, T. Skorodko, G. J. Wagner, A. Khoukaz, Alexander Schmidt, H. P. Morsch, X. Yuan, D. Lersch, H. Ohm, F. S. Bergmann, W. Eyrich, P. Goslawski, Magnus Wolke, R. Stassen, E. Doroshkevich, Günter Kemmerling, T. Tolba, P. Żuprański, Wojciech Krzemien, C. Zheng, A. Trzciński, A. Jany, Jozef Zlomanczuk, F. Hauenstein, K. Föhl, C. F. Redmer, Tomasz Bednarski, L. Yurev, V. Hejny, J. Stepaniak, P. Pluciński, Marcin Zieliński, K. Demmich, P. Podkopał, Lena Heijkenskjöld, M. Hodana, T. Sefzick, W. Węglorz, A. Pyszniak, W. Augustyniak, Hans Calén, K. Pysz, P. Fedorets, D. Pszczel, R. Maier, Ferdous Khan, B. Kłos, H. Bhatt, B. Lorentz, Kjell Fransson, Aleksandra Wrońska, E. Perez del Rio, L. Li, A. Goswami, F. Hinterberger, P. Wurm, M. Berłowski, P. Kulessa, Paweł Moskal, E. Stephan, S. Schadmand, Akira Yamamoto, A. Kupść, M. Bashkanov, N. Shah, K. Lalwani, R. Varma, I. Ozerianska, Benedykt R. Jany, H. Clement, Basanta Kumar Nandi, Bo Höistad, Zbigniew Rudy, R. Siudak, J. Klaja, Eryk Czerwiński, Szymon Niedźwiecki, Harald Kleines, P. Vlasov, W. Zipper, W. Bardan, D. Coderre, V. Sopov, R. Engels, D. Prasuhn, Ankhi Roy, St. Kistryn, M. Siemaszko, J. Zabierowski, Antoni Szczurek, and B. Kamys
Subjects: Nuclear reaction, Nuclear and High Energy Physics, Particle physics, fusion, +deuteron+2pi%22">p nucleon --> deuteron 2pi, Meson, Gev-C, two-pion [mass spectrum], Nuclear Theory, Hadron, isovector, FOS: Physical sciences, Elementary particle, Juelich COSY PS, 01 natural sciences, High Energy Physics - Experiment, Nuclear physics, High Energy Physics - Experiment (hep-ex), Pion, ABC effect and resonance structure, isoscalar, 0103 physical sciences, Pi, Nuclear fusion, Collisions, ddc:530, Meson Production, Nuclear Experiment (nucl-ex), WASA, Nuclear Experiment, 010306 general physics, Physics, 010308 nuclear & particles physics, Double Pion Production, mass enhancement, Pp, energy dependence [channel cross section], Total Cross-Sections, isospin decomposition, p n, Abc Effect And Resonance Structure, double pion production, Isospin, fusion [p p], pair production [pi], Lsospin Decomposition, experimental results
Abstract: Exclusive and kinematically complete high-statistics measurements of the basic double-pionic fusion reactions $pn\rightarrow d\pi ^{0}\pi ^{0}, pn\rightarrow d\pi ^{+}\pi ^{-}$ and $pp\rightarrow d\pi ^{+}\pi ^{0}$ have been carried out simultaneously over the energy region of the ABC effect using the WASA detector setup at COSY. Whereas the isoscalar reaction part given by the $d\pi ^{0}\pi ^{0}$ channel exhibits the ABC effect, i.e. a low-mass enhancement in the $\pi \pi$ - invariant mass distribution, as well as the associated resonance structure in the total cross section, the isovector part given by the $d\pi ^{+}\pi ^{-}$ channel shows a smooth behavior consistent with the conventional t -channel $\Delta \Delta$ process. The $d\pi^{+}\pi ^{-}$ data are very well reproduced by combining the data for isovector and isoscalar contributions, if the kinematical consequences of the isospin violation due to different masses for charged and neutral pions are taken into account.
Published: 2013
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43. Centrality dependence of π, K, and p production in Pb-Pb collisions at sqrt[s_{NN}]=2.76 TeV

Author: Abelev, B., Adam, J., Adamová, D., Adare, A. M., Aggarwal, M. M., Aglieri Rinella, G., Agnello, M., Agocs, A. G., Agostinelli, A., Ahammed, Z., Ahmad, N., Ahmad Masoodi, A., Ahn, S. A., Ahn, S. U., Ajaz, M., Akindinov, A., Aleksandrov, D., Alessandro, B., Alici, A., Alkin, A., Almaráz Aviña, E., Alme, J., Alt, T., Altini, V., Altinpinar, S., Altsybeev, I., Andrei, C., Andronic, A., Anguelov, V., Anielski, J., Anson, C., Antičić, T., Antinori, F., Antonioli, P., Aphecetche, L., Appelshäuser, H., Arbor, N., Arcelli, S., Arend, A., Armesto, N., Arnaldi, R., Aronsson, T., Arsene, I. C., Arslandok, M., Asryan, A., Augustinus, A., Averbeck, R., Awes, T. C., Äystö, J., Azmi, M. D., Bach, M., Badalà, A., Baek, Y. W., Bailhache, R., Bala, R., Baldisseri, A., Baltasar Dos Santos Pedrosa, F., Bán, J., Baral, R. C., Barbera, R., Barile, F., Barnaföldi, G. G., Barnby, L. S., Barret, V., Bartke, J., Basile, M., Bastid, N., Basu, S., Bathen, B., Batigne, G., Batyunya, B., Baumann, C., Bearden, I. G., Beck, H., Behera, N. K., Belikov, I., Bellini, F., Bellwied, R., Belmont Moreno, E., Bencedi, G., Beole, S., Berceanu, I., Bercuci, A., Berdnikov, Y., Berenyi, D., Bergognon, A. A. E., Berzano, D., Betev, L., Bhasin, A., Bhati, A. K., Bhom, J., Bianchi, L., Bianchi, N., Bielčík, J., Bielčíková, J., Bilandzic, A., Bjelogrlic, S., Blanco, F., Blau, D., Blume, C., Boccioli, M., Böttger, S., Bogdanov, A., Bøggild, H., Bogolyubsky, M., Boldizsár, L., Bombara, M., Book, J., Borel, H., Borissov, A., Bossú, F., Botje, M., Botta, E., Braidot, E., Braun Munzinger, P., Bregant, M., Breitner, T., Broker, T. A., Browning, T. A., Broz, M., Brun, R., Bruna, E., Bruno, G. E., Budnikov, D., Buesching, H., Bufalino, S., Buncic, P., Busch, O., Buthelezi, Z., Caffarri, D., Cai, X., Caines, H., Calvo Villar, E., Camerini, Paolo, Canoa Roman, V., Cara Romeo, G., Carena, F., Carena, W., Carlin Filho, N., Carminati, F., Casanova Díaz, A., Castillo Castellanos, J., Castillo Hernandez, J. F., Casula, E. A. R., Catanescu, V., Cavicchioli, C., Ceballos Sanchez, C., Cepila, J., Cerello, P., Chang, B., Chapeland, S., Charvet, J. L., Chattopadhyay, S., Cherney, M., Cheshkov, C., Cheynis, B., Chibante Barroso, V., Chinellato, D. D., Chochula, P., Chojnacki, M., Choudhury, S., Christakoglou, P., Christensen, C. H., Christiansen, P., Chujo, T., Chung, S. U., Cicalo, C., Cifarelli, L., Cindolo, F., Cleymans, J., Colamaria, F., Colella, D., Collu, A., Conesa Balbastre, G., Conesa del Valle, Z., Connors, M. E., Contin, G., Contreras, J. G., Cormier, T. M., Corrales Morales, Y., Cortese, P., Cortés Maldonado, I., Cosentino, M. R., Costa, F., Cotallo, M. E., Crescio, E., Crochet, P., Cruz Alaniz, E., Cruz Albino, R., Cuautle, E., Cunqueiro, L., Dainese, A., Danu, A., Das, K., Das, I., Das, S., Das, D., Dash, S., Dash, A., De, S., de Barros, G. O. V., De Caro, A., de Cataldo, G., de Cuveland, J., De Falco, A., De Gruttola, D., Delagrange, H., Deloff, A., De Marco, N., Dénes, E., De Pasquale, S., Deppman, A., Erasmo, G. D., de Rooij, R., Diaz Corchero, M. A., Di Bari, D., Dietel, T., Di Giglio, C., Di Liberto, S., Di Mauro, A., Di Nezza, P., Divià, R., Djuvsland, Ø., Dobrin, A., Dobrowolski, T., Dönigus, B., Dordic, O., Driga, O., Dubey, A. K., Dubla, A., Ducroux, L., Dupieux, P., Dutta Majumdar, A. K., Elia, D., Emschermann, D., Engel, H., Erazmus, B., Erdal, H. A., Espagnon, B., Estienne, M., Esumi, S., Evans, D., Eyyubova, G., Fabris, D., Faivre, J., Falchieri, D., Fantoni, A., Fasel, M., Fearick, R., Fehlker, D., Feldkamp, L., Felea, D., Feliciello, A., Fenton Olsen, B., Feofilov, G., Fernández Téllez, A., Ferretti, A., Festanti, A., Figiel, J., Figueredo, M. A. S., Filchagin, S., Finogeev, D., Fionda, F. M., Fiore, E. M., Floratos, E., Floris, M., Foertsch, S., Foka, P., Fokin, S., Fragiacomo, Enrico, Francescon, A., Frankenfeld, U., Fuchs, U., Furget, C., Fusco Girard, M., Gaardhøje, J. J., Gagliardi, M., Gago, A., Gallio, M., Gangadharan, D. R., Ganoti, P., Garabatos, C., Garcia Solis, E., Gargiulo, C., Garishvili, I., Gerhard, J., Germain, M., Geuna, C., Gheata, A., Gheata, M., Ghidini, B., Ghosh, P., Gianotti, P., Girard, M. R., Giubellino, P., Gladysz Dziadus, E., Glässel, P., Gomez, R., Ferreiro, E. G., González Trueba, L. H., González Zamora, P., Gorbunov, S., Goswami, A., Gotovac, S., Graczykowski, L. K., Grajcarek, R., Grelli, A., Grigoras, A., Grigoras, C., Grigoriev, V., Grigoryan, S., Grigoryan, A., Grinyov, B., Grion, N., Gros, P., Grosse Oetringhaus, J. F., Grossiord, J. Y., Grosso, R., Guber, F., Guernane, R., Guerzoni, B., Guilbaud, M., Gulbrandsen, K., Gulkanyan, H., Gunji, T., Gupta, R., Gupta, A., Haake, R., Haaland, Ø., Hadjidakis, C., Haiduc, M., Hamagaki, H., Hamar, G., Han, B. H., Hanratty, L. D., Hansen, A., Harmanová Tóthová, Z., Harris, J. W., Hartig, M., Harton, A., Hatzifotiadou, D., Hayashi, S., Hayrapetyan, A., Heckel, S. T., Heide, M., Helstrup, H., Herghelegiu, A., Herrera Corral, G., Herrmann, N., Hess, B. A., Hetland, K. F., Hicks, B., Hippolyte, B., Hori, Y., Hristov, P., Hřivnáčová, I., Huang, M., Humanic, T. J., Hwang, D. S., Ichou, R., Ilkaev, R., Ilkiv, I., Inaba, M., Incani, E., Innocenti, G. M., Innocenti, P. G., Ippolitov, M., Irfan, M., Ivan, C., Ivanov, M., Ivanov, A., Ivanov, V., Ivanytskyi, O., Jachołkowski, A., Jacobs, P. M., Jang, H. J., Janik, M. A., Janik, R., Jayarathna, P. H. S. Y., Jena, S., Jha, D. M., Jimenez Bustamante, R. T., Jones, P. G., Jung, H., Jusko, A., Kaidalov, A. B., Kalcher, S., Kaliňák, P., Kalliokoski, T., Kalweit, A., Kang, J. H., Kaplin, V., Karasu Uysal, A., Karavichev, O., Karavicheva, T., Karpechev, E., Kazantsev, A., Kebschull, U., Keidel, R., Khan, M. M., Khan, K. H., Khan, P., Khan, S. A., Khanzadeev, A., Kharlov, Y., Kileng, B., Kim, T., Kim, J. S., Kim, D. J., Kim, S., Kim, M., Kim, B., Kim, D. W., Kim, J. H., Kirsch, S., Kisel, I., Kiselev, S., Kisiel, A., Klay, J. L., Klein, J., Klein Bösing, C., Kliemant, M., Kluge, A., Knichel, M. L., Knospe, A. G., Köhler, M. K., Kollegger, T., Kolojvari, A., Kompaniets, M., Kondratiev, V., Kondratyeva, N., Konevskikh, A., Kovalenko, V., Kowalski, M., Kox, S., Koyithatta Meethaleveedu, G., Kral, J., Králik, I., Kramer, F., Kravčáková, A., Krawutschke, T., Krelina, M., Kretz, M., Krivda, M., Krizek, F., Krus, M., Kryshen, E., Krzewicki, M., Kucheriaev, Y., Kugathasan, T., Kuhn, C., Kuijer, P. G., Kulakov, I., Kumar, J., Kurashvili, P., Kurepin, A., Kurepin, A. B., Kuryakin, A., Kushpil, S., Kushpil, V., Kvaerno, H., Kweon, M. J., Kwon, Y., Ladrón de Guevara, P., Lakomov, I., Langoy, R., La Pointe, S. L., Lara, C., Lardeux, A., La Rocca, P., Lea, Ramona, Lechman, M., Lee, K. S., Lee, G. R., Lee, S. C., Legrand, I., Lehnert, J., Lemmon, R. C., Lenhardt, M., Lenti, V., León, H., León Monzón, I., León Vargas, H., Lévai, P., Li, S., Lien, J., Lietava, R., Lindal, S., Lindenstruth, V., Lippmann, C., Lisa, M. A., Ljunggren, H. M., Lodato, D. F., Loenne, P. I., Loggins, V. R., Loginov, V., Lohner, D., Loizides, C., Loo, K. K., Lopez, X., López Torres, E., Løvhøiden, G., X. G., Lu, Luettig, P., Lunardon, M., Luo, J., Luparello, G., Luzzi, C., Ma, R., Ma, K., Madagodahettige Don, D. M., Maevskaya, A., Mager, M., Mahapatra, D. P., Maire, A., Malaev, M., Maldonado Cervantes, I., Malinina, L., Mal'Kevich, D., Malzacher, P., Mamonov, A., Manceau, L., Mangotra, L., Manko, V., Manso, F., Manukyan, N., Manzari, V., Mao, Y., Marchisone, M., Mareš, J., Margagliotti, Giacomo, Margotti, A., Marín, A., Markert, C., Marquard, M., Martashvili, I., Martin, N. A., Martinengo, P., Martínez, M. I., Martínez Davalos, A., Martínez García, G., Martynov, Y., Mas, A., Masciocchi, S., Masera, M., Masoni, A., Massacrier, L., Mastroserio, A., Matyja, A., Mayer, C., Mazer, J., Mazzoni, M. A., Meddi, F., Menchaca Rocha, A., Mercado Pérez, J., Meres, M., Miake, Y., Mikhaylov, K., Milano, L., Milosevic, J., Mischke, A., Mishra, A. N., Miśkowiec, D., Mitu, C., Mizuno, S., Mlynarz, J., Mohanty, B., Molnar, L., Montaño Zetina, L., Monteno, M., Montes, E., Moon, T., Morando, M., Moreira De Godoy, D. A., Moretto, S., Morreale, A., Morsch, A., Muccifora, V., Mudnic, E., Muhuri, S., Mukherjee, M., Müller, H., Munhoz, M. G., Murray, S., Musa, L., Musinsky, J., Nandi, B. K., Nania, R., Nappi, E., Nattrass, C., Nayak, T. K., Nazarenko, S., Nedosekin, A., Nicassio, M., Niculescu, M., Nielsen, B. S., Niida, T., Nikolaev, S., Nikolic, V., Nikulin, S., Nikulin, V., Nilsen, B. S., Nilsson, M. S., Noferini, F., Nomokonov, P., Nooren, G., Nyanin, A., Nyatha, A., Nygaard, C., Nystrand, J., Ochirov, A., Oeschler, H., S. K., Oh, Oh, S., Oleniacz, J., Oliveira Da Silva, A. C., Oppedisano, C., Ortiz Velasquez, A., Oskarsson, A., Ostrowski, P., Otwinowski, J., Oyama, K., Ozawa, K., Pachmayer, Y., Pachr, M., Padilla, F., Pagano, P., Paić, G., Painke, F., Pajares, C., Pal, S. K., Palaha, A., Palmeri, A., Papikyan, V., Pappalardo, G. 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B., Kalcher, S., Kaliňák, P., Kalliokoski, T., Kalweit, A., Kang, J. H., Kaplin, V., Karasu Uysal, A., Karavichev, O., Karavicheva, T., Karpechev, E., Kazantsev, A., Kebschull, U., Keidel, R., Khan, M. M., Khan, K. H., Khan, P., Khan, S. A., Khanzadeev, A., Kharlov, Y., Kileng, B., Kim, T., Kim, J. S., Kim, D. J., Kim, S., Kim, M., Kim, B., Kim, D. W., Kim, J. H., Kirsch, S., Kisel, I., Kiselev, S., Kisiel, A., Klay, J. L., Klein, J., Klein Bösing, C., Kliemant, M., Kluge, A., Knichel, M. L., Knospe, A. G., Köhler, M. K., Kollegger, T., Kolojvari, A., Kompaniets, M., Kondratiev, V., Kondratyeva, N., Konevskikh, A., Kovalenko, V., Kowalski, M., Kox, S., Koyithatta Meethaleveedu, G., Kral, J., Králik, I., Kramer, F., Kravčáková, A., Krawutschke, T., Krelina, M., Kretz, M., Krivda, M., Krizek, F., Krus, M., Kryshen, E., Krzewicki, M., Kucheriaev, Y., Kugathasan, T., Kuhn, C., Kuijer, P. G., Kulakov, I., Kumar, J., Kurashvili, P., Kurepin, A., Kurepin, A. B., Kuryakin, A., Kushpil, S., Kushpil, V., Kvaerno, H., Kweon, M. J., Kwon, Y., Ladrón de Guevara, P., Lakomov, I., Langoy, R., La Pointe, S. L., Lara, C., Lardeux, A., La Rocca, P., Lea, Ramona, Lechman, M., Lee, K. S., Lee, G. R., Lee, S. C., Legrand, I., Lehnert, J., Lemmon, R. C., Lenhardt, M., Lenti, V., León, H., León Monzón, I., León Vargas, H., Lévai, P., Li, S., Lien, J., Lietava, R., Lindal, S., Lindenstruth, V., Lippmann, C., Lisa, M. A., Ljunggren, H. M., Lodato, D. F., Loenne, P. I., Loggins, V. R., Loginov, V., Lohner, D., Loizides, C., Loo, K. K., Lopez, X., López Torres, E., Løvhøiden, G., X. G., Lu, Luettig, P., Lunardon, M., Luo, J., Luparello, G., Luzzi, C., Ma, R., Ma, K., Madagodahettige Don, D. M., Maevskaya, A., Mager, M., Mahapatra, D. 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K. Pal, A. Palaha, A. Palmeri, V. Papikyan, G. S. Pappalardo, W. J. Park, A. Passfeld, B. Pastirčák, D. I. Patalakha, V. Paticchio, B. Paul, A. Pavlinov, T. Pawlak, T. Peitzmann, H. Pereira Da Costa, E. Pereira De Oliveira Filho, D. Peresunko, C. E. Pérez Lara, D. Perrino, W. Peryt, A. Pesci, V. Peskov, Y. Pestov, V. Petráček, M. Petran, M. Petri, P. Petrov, M. Petrovici, C. Petta, S. Piano, M. Pikna, P. Pillot, O. Pinazza, L. Pinsky, N. Pitz, D. B. Piyarathna, M. Planinic, M. Płoskoń, J. Pluta, T. Pocheptsov, S. Pochybova, P. L. M. Podesta-Lerma, M. G. Poghosyan, K. Polák, B. Polichtchouk, N. Poljak, A. Pop, S. Porteboeuf-Houssai, V. Pospíšil, B. Potukuchi, S. K. Prasad, R. Preghenella, F. Prino, C. A. Pruneau, I. Pshenichnov, G. Puddu, V. Punin, M. Putiš, J. Putschke, H. Qvigstad, A. Rachevski, A. Rademaker, T. S. Räihä, J. Rak, A. Rakotozafindrabe, L. Ramello, A. Ramírez Reye, S. Raniwala, R. Raniwala, S. S. Räsänen, B. T. Rascanu, D. Rathee, K. F. Read, J. S. Real, K. Redlich, R. J. Reed, A. Rehman, P. Reichelt, M. Reicher, R. Renfordt, A. R. Reolon, A. Reshetin, F. Rettig, J.-P. Revol, K. Reyger, L. Riccati, R. A. Ricci, T. Richert, M. Richter, P. Riedler, W. Riegler, F. Riggi, M. Rodríguez Cahuantzi, A. Rodriguez Manso, K. Røed, E. Rogochaya, D. Rohr, D. Röhrich, R. Romita, F. Ronchetti, P. Rosnet, S. Rossegger, A. Rossi, C. Roy, P. Roy, A. J. Rubio Montero, R. Rui, R. Russo, E. Ryabinkin, A. Rybicki, S. Sadovsky, K. Šafařík, R. Sahoo, P. K. Sahu, J. Saini, H. Sakaguchi, S. Sakai, D. Sakata, C. A. Salgado, J. Salzwedel, S. Sambyal, V. Samsonov, X. Sanchez Castro, L. Šándor, A. Sandoval, M. Sano, G. Santagati, R. Santoro, J. Sarkamo, E. Scapparone, F. Scarlassara, R. P. Scharenberg, C. Schiaua, R. Schicker, H. R. Schmidt, C. Schmidt, S. Schuchmann, J. Schukraft, T. Schuster, Y. Schutz, K. Schwarz, K. Schweda, G. Scioli, E. Scomparin, R. Scott, P. A. Scott, G. Segato, I. Selyuzhenkov, S. Senyukov, J. Seo, S. Serci, E. Serradilla, A. Sevcenco, A. Shabetai, G. Shabratova, R. Shahoyan, S. Sharma, N. Sharma, S. Rohni, K. Shigaki, K. Shtejer, Y. Sibiriak, E. Sicking, S. Siddhanta, T. Siemiarczuk, D. Silvermyr, C. Silvestre, G. Simatovic, G. Simonetti, R. Singaraju, R. Singh, S. Singha, V. Singhal, T. Sinha, B. C. Sinha, B. Sitar, M. Sitta, T. B. Skaali, K. Skjerdal, R. Smakal, N. Smirnov, R. J. M. Snelling, C. Søgaard, R. Soltz, H. Son, J. Song, M. Song, C. Soo, F. Soramel, I. Sputowska, M. Spyropoulou-Stassinaki, B. K. Srivastava, J. Stachel, I. Stan, G. Stefanek, M. Steinprei, E. Stenlund, G. Steyn, J. H. Stiller, D. Stocco, M. Stolpovskiy, P. Strmen, A. A. P. Suaide, M. A. Subieta Vásquez, T. Sugitate, C. Suire, R. Sultanov, M. Šumbera, T. Susa, T. J. M. Symon, A. Szanto de Toledo, I. Szarka, A. Szczepankiewicz, M. Szymański, J. Takahashi, M. A. Tangaro, J. D. Tapia Takaki, A. Tarantola Peloni, A. Tarazona Martinez, A. Tauro, G. Tejeda Muñoz, A. Telesca, A. Ter Minasyan, C. Terrevoli, J. Thäder, D. Thoma, R. Tieulent, A. R. Timmin, D. Tlusty, A. Toia, H. Torii, L. Toscano, V. Trubnikov, D. Truesdale, W. H. Trzaska, T. Tsuji, A. Tumkin, R. Turrisi, T. S. Tveter, J. Ulery, K. Ullaland, J. Ulrich, A. Ura, G. M. Urciuoli, G. L. Usai, M. Vajzer, M. Vala, L. Valencia Palomo, P. Vande Vyvre, M. van Leeuwen, L. Vannucci, A. Varga, R. Varma, M. Vasileiou, A. Vasiliev, V. Vechernin, M. Veldhoen, M. Venaruzzo, E. Vercellin, S. Vergara, R. Vernet, M. Verweij, L. Vickovic, G. Viesti, J. Viinikainen, Z. Vilakazi, O. Villalobos Baillie, L. Vinogradov, Y. Vinogradov, A. Vinogradov, T. Virgili, Y. P. Viyogi, A. Vodopyanov, M. A. Völkl, S. Voloshin, K. Voloshin, G. Volpe, B. von Haller, I. Vorobyev, D. Vranic, J. Vrláková, B. Vulpescu, A. Vyushin, V. Wagner, B. Wagner, R. Wan, Y. Wang, M. Wang, D. Wang, K. Watanabe, M. Weber, J. P. Wessel, U. Westerhoff, J. Wiechula, J. Wikne, M. Wilde, A. Wilk, G. Wilk, M. C. S. William, B. Windelband, L. Xaplanteris Karampatso, C. G. Yaldo, Y. Yamaguchi, H. Yang, S. Yang, S. Yasnopolskiy, J. Yi, Z. Yin, I.-K. Yoo, J. Yoon, W. Yu, X. Yuan, I. Yushmanov, V. Zaccolo, C. Zach, C. Zampolli, S. Zaporozhet, A. Zarochentsev, P. Závada, N. Zaviyalov, H. Zbroszczyk, P. Zelnicek, I. S. Zgura, M. Zhalov, X. Zhang, H. Zhang, Y. Zhou, F. Zhou, D. Zhou, J. Zhu, X. Zhu, H. Zhu, A. Zichichi, A. Zimmermann, G. Zinovjev, Y. Zoccarato, M. Zynovyev, and M. Zyzak
Subjects: Pb-Pb collision, MESON PRODUCTION, NUCLEUS-NUCLEUS COLLISIONS, ALICE experiment, HEAVY-ION COLLISIONS, QCD PHASE-TRANSITION, HADRON-PRODUCTION, QUARK-GLUON PLASMA, CHEMICAL FREEZE-OUT, Centrality dependence, centrality dependence, Identified hadron production, TOTAL CROSS-SECTIONS, Nuclear Experiment
Abstract: In this paper measurements are presented of π±, K±, p, and p(bar) production at midrapidity (|y| < 0.5), in Pb-Pb collisions at √sNN= 2.76 TeV as a function of centrality. The measurement covers the transverse-momentum (pT ) range from 100, 200, and 300 MeV/c up to 3, 3, and 4.6 GeV/c for π, K, and p, respectively. The measured pT distributions and yields are compared to expectations based on hydrodynamic, thermal and recombination models. The spectral shapes of central collisions show a stronger radial flow than measured at lower energies, which can be described in hydrodynamic models. In peripheral collisions, the pT distributions are not well reproduced by hydrodynamic models. Ratios of integrated particle yields are found to be nearly independent of centrality. The yield of protons normalized to pions is a factor ∼1.5 lower than the expectation from thermal models.
Published: 2013

44. Total electron scattering cross-sections for carbon monoxide at low electron energies

Author: Rawat, P., Subramanian, K. P., and Kumar, Vijay
Published: 1998
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45. Resolved photon processes

Author: Godbole, R. M.
Published: 1998
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46. Total cross sections for electron scattering from well-known and exotic molecules

Author: Joshipura, K N
Published: 1998
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47. Study of exclusive one-pion and one-eta production using hadron and dielectron channels in pp reactions at kinetic beam energies of 1.25 GeV and 2.2 GeV with HADES

Author: Agakishiev, G., Alvarez-Poll, H., Bałanda, A., Bassini, R., Böhmer, M., Bokemeyer, H., Boyard, J. L., Cabanelas, Pablo, Chernenko, S., Christ, T., Destefanis, M., Dohrmann, F., Dybczak, A., Eberl, T., Fabbietti, L., Fateev, O., Finocchiaro, P., Friese, J., Fröhlich, I., Galatyuk, T., Garzón, J. A., Gernhäuser, R., Gilardi, C., Golubeva, M., González-Diaz, D., Guber, F., Gumberidze, M., Hennino, T., Holzmann, R., Ierusalimov, A., Iori, I., Ivashkin, A., Jurkovic, M., Kämpfer, B., Kanaki, K., Karavicheva, T., Koenig, I., Koenig, W., Kolb, B. W., Kotte, R., Kozuch, A., Krizek, F., Kühn, W., Kugler, A., Kurepin, A., Lang, S., Lapidus, K., Liu, T., Maier, L., Markert, J., Metag, V., Michalska, B., Morinière, E., Mousa, J., Münch, M., Müntz, C., Naumann, L., Otwinowski, J., Pachmayer, Y. C., Pechenov, V., Pechenova, O., Pérez Cavalcanti, T., Pietraszko, J., Pospisil, V., Przygoda, W., Ramstein, B., Reshetin, A., Roy-Stephan, M., Rustamov, A., Sadovsky, A., Sailer, B., Salabura, P., Sánchez, M., Schmah, A., Schwab, E., Sobolev, Y. G., Spataro, S., Spruck, B., Ströbele, H., Stroth, J., Sturm, C., Tarantola, A., Teilab, K., Tlusty, P., Toia, A., Traxler, M., Trebacz, R., Tsertos, Haralambos, Wagner, V., Wisniowski, M., Wojcik, T., Wüstenfeld, J., Yurevich, S., Zanevsky, Y., Zumbruch, P., 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), HADES, and Tsertos, Haralambos [0000-0001-5966-343X]
Subjects: Nuclear and High Energy Physics, MESON PRODUCTION, SINGLE-PION, Hadron, SIS ENERGIES, FOS: Physical sciences, Electron, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], Kinetic energy, 01 natural sciences, Nuclear physics, Pion, 0103 physical sciences, SCATTERING, ddc:530, NEAR-THRESHOLD, Nuclear Experiment (nucl-ex), 010306 general physics, Nuclear Experiment, Physics, NUCLEON-NUCLEON COLLISIONS, 010308 nuclear & particles physics, Resonance, Sigma, OF-FLIGHT SPECTROMETER, Helicity, Baryon, proton-proton collisions, High Energy Physics::Experiment, TOTAL CROSS-SECTIONS, INTERMEDIATE ENERGIES
Abstract: We present measurements of exclusive \pi^{+,0} and \eta\ production in pp reactions at 1.25 GeV and 2.2 GeV beam kinetic energy in hadron and dielectron channels. In the case of \pi^+ and \pi^0, high-statistics invariant-mass and angular distributions are obtained within the HADES acceptance as well as acceptance corrected distributions, which are compared to a resonance model. The sensitivity of the data to the yield and production angular distribution of \Delta(1232) and higher lying baryon resonances is shown, and an improved parameterization is proposed. The extracted cross sections are of special interest in the case of pp \to pp \eta, since controversial data exist at 2.0 GeV; we find \sigma =0.142 \pm 0.022 mb. Using the dielectron channels, the \pi^0 and \eta\ Dalitz decay signals are reconstructed with yields fully consistent with the hadronic channels. The electron invariant masses and acceptance corrected helicity angle distributions are found in good agreement with model predictions., Comment: 22 pages, 18 figures, to be published in EPJA
Published: 2012
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48. Pion, Kaon, and Proton Production in Central Pb-Pb Collisions at root s(NN)=2.76 TeV

Author: ABELEV, B, ADAM, J, ADAMOVA, D, ADARE, AM, AGGARWAL, MM, RINELLA, GA, AGOCS, AG, AGOSTINELLI, A, SALAZAR, SA, AHAMMED, Z, AHMAD, N, MASOODI, AA, AHN, SA, AHN, SU, AKINDINOV, A, ALEKSANDROV, D, ALESSANDRO, B, MOLINA, RA, ALICI, A, ALKIN, A, AVINA, EA, ALME, J, ALT, T, ALTINI, V, ALTINPINAR, S, ALTSYBEEV, I, ANDREI, C, ANDRONIC, A, ANGUELOV, V, ANIELSKI, J, ANSON, C, ANTICIC, T, ANTINORI, F, ANTONIOLI, P, APHECETCHE, L, APPELSHAUSER, H, ARBOR, N, ARCELLI, S, AREND, A, ARMESTO, N, ARNALDI, R, ARONSSON, T, ARSENE, IC, ARSLANDOK, M, ASRYAN, A, AUGUSTINUS, A, AVERBECK, R, AWES, TC, AYSTO, J, AZMI, MD, BACH, M, BADALA, A, BAEK, YW, BAILHACHE, R, BALA, R, FERROLI, RB, BALDISSERI, A, BALDIT, A, PEDROSA, FBD, BAN, J, BARAL, RC, BARBERA, R, BARILE, F, BARNAFOLDI, GG, BARNBY, LS, BARRET, V, BARTKE, J, BASILE, M, BASTID, N, BASU, S, BATHEN, B, BATIGNE, G, BATYUNYA, B, BAUMANN, C, BEARDEN, IG, BECK, H, BEHERA, NK, BELIKOV, I, BELLINI, F, BELLWIED, R, BELMONT-MORENO, E, BENCEDI, G, BEOLE, S, BERCEANU, I, BERCUCI, A, BERDNIKOV, Y, BERENYI, D, BERGOGNON, AAE, BERZANO, D, BETEV, L, BHASIN, A, BHATI, AK, BHOM, J, BIANCHI, L, BIANCHI, N, BIANCHIN, C, BIELCIK, J, BIELCIKOVA, J, BILANDZIC, A, BJELOGRLIC, S, BLANCO, F, BLAU, D, BLUME, C, BOCCIOLI, M, BOCK, N, BOTTGER, S, BOGDANOV, A, BOGGILD, H, BOGOLYUBSKY, M, BOLDIZSAR, L, BOMBARA, M, BOOK, J, BOREL, H, BORISSOV, A, BOSE, S, BOSSU, F, BOTJE, M, BOTTA, E, BOYER, B, BRAIDOT, E, BRAUN-MUNZINGER, P, BREGANT, M, BREITNER, T, BROWNING, TA, BROZ, M, BRUN, R, BRUNA, E, BRUNO, GE, BUDNIKOV, D, BUESCHING, H, BUFALINO, S, BUSCH, O, BUTHELEZI, Z, ORDUNA, DC, CAFFARRI, D, CAI, X, CAINES, H, VILLAR, EC, CAMERINI, P, ROMAN, VC, ROMEO, GC, CARENA, F, CARENA, W, CARLIN, N, CARMINATI, F, DIAZ, AC, CASTELLANOS, JC, HERNANDEZ, JFC, CASULA, EAR, CATANESCU, V, CAVICCHIOLI, C, SANCHEZ, CC, CEPILA, J, CERELLO, P, CHANG, B, CHAPELAND, S, CHARVET, JL, CHATTOPADHYAY, S, CHAWLA, I, CHERNEY, M, CHESHKOV, C, CHEYNIS, B, BARROSO, VC, CHINELLATO, DD, CHOCHULA, P, CHOJNACKI, M, CHOUDHURY, S, CHRISTAKOGLOU, P, CHRISTENSEN, CH, CHRISTIANSEN, P, CHUJO, T, CHUNG, SU, CICALO, C, CIFARELLI, L, CINDOLO, F, CLEYMANS, J, COCCETTI, F, COLAMARIA, F, COLELLA, D, BALBASTRE, GC, DEL VALLE, ZC, CONSTANTIN, P, CONTIN, G, CONTRERAS, JG, CORMIER, TM, MORALES, YC, CORTESE, P, MALDONADO, IC, COSENTINO, MR, COSTA, F, COTALLO, ME, CRESCIO, E, CROCHET, P, ALANIZ, EC, CUAUTLE, E, CUNQUEIRO, L, DAINESE, A, DALSGAARD, HH, DANU, A, DAS, I, DAS, D, DAS, K, DASH, S, DASH, A, DE, S, DE BARROS, GOV, DE CARO, A, DE CATALDO, G, DE CUVELAND, J, DE FALCO, A, DE GRUTTOLA, D, DELAGRANGE, H, DELOFF, A, DEMANOV, V, DE MARCO, N, DENES, E, DE PASQUALE, S, DEPPMAN, A, ERASMO, GD, DE ROOIJ, R, CORCHERO, MAD, DI BARI, D, DIETEL, T, DI GIGLIO, C, DI LIBERTO, S, DI MAURO, A, DI NEZZA, P, DIVIA, R, DJUVSLAND, O, DOBRIN, A, DOBROWOLSKI, T, DOMINGUEZ, I, DONIGUS, B, DORDIC, O, DRIGA, O, DUBEY, AK, DUBLA, A, DUCROUX, L, DUPIEUX, P, MAJUMDAR, AKD, MAJUMDAR, MRD, ELIA, D, EMSCHERMANN, D, ENGEL, H, ERAZMUS, B, ERDAL, HA, ESPAGNON, B, ESTIENNE, M, ESUMI, S, EVANS, D, EYYUBOVA, G, FABRIS, D, FAIVRE, J, FALCHIERI, D, FANTONI, A, FASEL, M, FEARICK, R, FEDUNOV, A, FEHLKER, D, FELDKAMP, L, FELEA, D, FENTON-OLSEN, B, FEOFILOV, G, TELLEZ, AF, FERRETTI, A, FERRETTI, R, FESTANTI, A, FIGIEL, J, FIGUEREDO, MAS, FILCHAGIN, S, FINOGEEV, D, FIONDA, FM, FIORE, EM, FLORIS, M, FOERTSCH, S, FOKA, P, FOKIN, S, FRAGIACOMO, E, FRANCESCON, A, FRANKENFELD, U, FUCHS, U, FURGET, C, GIRARD, MF, GAARDHOJE, JJ, GAGLIARDI, M, GAGO, A, GALLIO, M, GANGADHARAN, DR, GANOTI, P, GARABATOS, C, GARCIA-SOLIS, E, GARISHVILI, I, GERHARD, J, GERMAIN, M, GEUNA, C, GHEATA, M, GHEATA, A, GHIDINI, B, GHOSH, P, GIANOTTI, P, GIRARD, MR, GIUBELLINO, P, GLADYSZ-DZIADUS, E, GLASSEL, P, GOMEZ, R, FERREIRO, EG, GONZALEZ-TRUEBA, LH, GONZALEZ-ZAMORA, P, GORBUNOV, S, GOSWAMI, A, GOTOVAC, S, GRABSKI, V, GRACZYKOWSKI, LK, GRAJCAREK, R, GRELLI, A, GRIGORAS, C, GRIGORAS, A, GRIGORIEV, V, GRIGORYAN, S, GRIGORYAN, A, GRINYOV, B, GRION, N, GROS, P, GROSSE-OETRINGHAUS, JF, GROSSIORD, JY, GROSSO, R, GUBER, F, GUERNANE, R, GUTIERREZ, CG, GUERZONI, B, GUILBAUD, M, GULBRANDSEN, K, GUNJI, T, GUPTA, R, GUPTA, A, GUTBROD, H, HAALAND, O, HADJIDAKIS, C, HAIDUC, M, HAMAGAKI, H, HAMAR, G, HAN, BH, HANRATTY, LD, HANSEN, A, HARMANOVA-TOTHOVA, Z, HARRIS, JW, HARTIG, M, HASEGAN, D, HATZIFOTIADOU, D, HAYRAPETYAN, A, HECKEL, ST, HEIDE, M, HELSTRUP, H, HERGHELEGIU, A, CORRAL, GH, HERRMANN, N, HESS, BA, HETLAND, KF, HICKS, B, HILLE, PT, HIPPOLYTE, B, HORAGUCHI, T, HORI, Y, HRISTOV, P, HRIVNACOVA, I, HUANG, M, HUMANIC, TJ, HWANG, DS, ICHOU, R, ILKAEV, R, ILKIV, I, INABA, M, INCANI, E, INNOCENTI, GM, INNOCENTI, PG, IPPOLITOV, M, IRFAN, M, IVAN, C, IVANOV, M, IVANOV, A, IVANOV, V, IVANYTSKYI, O, JACOBS, PM, JANG, HJ, JANIK, R, JANIK, MA, JAYARATHNA, PHSY, JENA, S, JHA, DM, BUSTAMANTE, RTJ, JIRDEN, L, JONES, PG, JUNG, H, JUSKO, A, KAIDALOV, AB, KAKOYAN, V, KALCHER, S, KALINAK, P, KALLIOKOSKI, T, KALWEIT, A, KANG, JH, KAPLIN, V, UYSAL, AK, KARAVICHEV, O, KARAVICHEVA, T, KARPECHEV, E, KAZANTSEV, A, KEBSCHULL, U, KEIDEL, R, KHAN, P, KHAN, MM, KHAN, SA, KHANZADEEV, A, KHARLOV, Y, KILENG, B, KIM, M, KIM, DJ, KIM, DW, KIM, JH, KIM, JS, KIM, T, KIM, SH, KIM, S, KIM, B, KIRSCH, S, KISEL, I, KISELEV, S, KISIEL, A, KLAY, JL, KLEIN, J, KLEIN-BOSING, C, KLIEMANT, M, KLUGE, A, KNICHEL, ML, KNOSPE, AG, KOCH, K, KOHLER, MK, KOLLEGGER, T, KOLOJVARI, A, KONDRATIEV, V, KONDRATYEVA, N, KONEVSKIKH, A, KORNEEV, A, KOUR, R, KOWALSKI, M, KOX, S, MEETHALEVEEDU, GK, KRAL, J, KRALIK, I, KRAMER, F, KRAUS, I, KRAWUTSCHKE, T, KRELINA, M, KRETZ, M, KRIVDA, M, KRIZEK, F, KRUS, M, KRYSHEN, E, KRZEWICKI, M, KUCHERIAEV, Y, KUGATHASAN, T, KUHN, C, KUIJER, PG, KULAKOV, I, KUMAR, J, KURASHVILI, P, KUREPIN, AB, KUREPIN, A, KURYAKIN, A, KUSHPIL, S, KUSHPIL, V, KVAERNO, H, KWEON, MJ, KWON, Y, DE GUEVARA, PL, LAKOMOV, I, LANGOY, R, LA POINTE, SL, LARA, C, LARDEUX, A, LA ROCCA, P, LAZZERONI, C, LEA, R, LE BORNEC, Y, LECHMAN, M, LEE, KS, LEE, GR, LEE, SC, 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Y, ZYNOVYEV, M, and ZYZAK, M
Subjects: Models, Spectrum, Chemical Freeze-Out, Quark-Gluon Plasma, Finite-Temperature, Heavy-Ion Collisions, Monte-Carlo, Hadron-Production, Total Cross-Sections, Qcd Phase-Transition
Abstract: In this Letter we report the first results on pi(+/-), K-+/-, p, and (p) over bar production at midrapidity (vertical bar y vertical bar < 0.5) in central Pb-Pb collisions at root s(NN) = 2.76 TeV, measured by the ALICE experiment at the LHC. The p(T) distributions and yields are compared to previous results at root s(NN) = 200 GeV and expectations from hydrodynamic and thermal models. The spectral shapes indicate a strong increase of the radial flow velocity with root s(NN), which in hydrodynamic models is expected as a consequence of the increasing particle density. While the K/pi ratio is in line with predictions from the thermal model, the p/pi ratio is found to be lower by a factor of about 1.5. This deviation from thermal model expectations is still to be understood.
Published: 2012

49. Pion, Kaon, and Proton Production in Central Pb-Pb Collisions at √s_NN =2.76 TeV

Author: Abelev, B., Adam, J., Adamová, D., Adare, A., Aggarwal, M., Aglieri Rinella, G., Agocs, A., Agostinelli, A., Aguilar Salazar, S., Ahammed, Z., Ahmad, N., Ahmad Masoodi, A., Ahn, S., Akindinov, A., Aleksandrov, D., Alessandro, B., Alfaro Molina, R., Alici, A., Alkin, A., Almaráz Aviña, E., Alme, J., Alt, T., Altini, V., Altinpinar, S., Altsybeev, I., Andrei, C., Andronic, A., Anguelov, V., Anielski, J., Anson, C., Antičić, T., Antinori, F., Antonioli, P., Aphecetche, L., Appelshäuser, H., Arbor, N., Arcelli, S., Arend, A., Armesto, N., Arnaldi, R., Aronsson, T., Arsene, I., Arslandok, M., Asryan, A., Augustinus, A., Averbeck, R., Awes, T., Äystö, J., Azmi, M., Bach, M., Badalà, A., Baek, Y., Bailhache, R., Bala, R., Baldini Ferroli, R., Baldisseri, A., Baldit, A., Baltasar Dos Santos Pedrosa, F., Bán, J., Baral, R., Barbera, R., Barile, F., Barnaföldi, G., Barnby, L., Barret, V., Bartke, J., Basile, M., Bastid, N., Basu, S., Bathen, B., Batigne, G., Batyunya, B., Baumann, C., Bearden, I., Beck, H., Behera, N., Belikov, I., Bellini, F., Bellwied, R., Belmont Moreno, E., Bencedi, G., Beole, S., Berceanu, I., Bercuci, A., Berdnikov, Y., Berenyi, D., Bergognon, A., Berzano, D., Betev, L., Bhasin, A., Bhati, A., Bhom, J., Bianchi, L., Bianchi, N., Bianchin, C., Bielčík, J., Bielčíková, J., Bilandzic, A., Bjelogrlic, S., Blanco, F., Blau, D., Blume, C., Boccioli, M., Bock, N., Böttger, S., Bogdanov, A., Bøggild, H., Bogolyubsky, M., Boldizsár, L., Bombara, M., Book, J., Borel, H., Borissov, A., Bose, S., Bossú, F., Botje, M., Botta, E., Boyer, B., Braidot, E., Braun Munzinger, P., Bregant, Marco, Breitner, T., Browning, T., Broz, M., Brun, R., Bruna, E., Bruno, G., Budnikov, D., Buesching, H., Bufalino, S., Busch, O., Buthelezi, Z., Caballero Orduna, D., Caffarri, D., Cai, X., Caines, H., Calvo Villar, E., Camerini, Paolo, Canoa Roman, V., Cara Romeo, G., Carena, F., Carena, W., Carlin Filho, N., Carminati, F., Casanova Díaz, A., Castillo Castellanos, J., Castillo Hernandez, J., Casula, E., Catanescu, V., Cavicchioli, C., Ceballos Sanchez, C., Cepila, J., Cerello, P., Chang, B., Chapeland, S., Charvet, J., Chattopadhyay, S., Chawla, I., Cherney, M., Cheshkov, C., Cheynis, B., Chibante Barroso, V., Chinellato, D., Chochula, P., Chojnacki, M., Choudhury, S., Christakoglou, P., Christensen, C., Christiansen, P., Chujo, T., Chung, S., Cicalo, C., Cifarelli, L., Cindolo, F., Cleymans, J., Coccetti, F., Colamaria, F., Colella, D., Conesa Balbastre, G., Conesa del Valle, Z., Constantin, P., Contin, Giacomo, Contreras, J., Cormier, T., Corrales Morales, Y., Cortese, P., Cortés Maldonado, I., Cosentino, M., Costa, F., Cotallo, M., Crescio, E., Crochet, P., Cruz Alaniz, E., Cuautle, E., Cunqueiro, L., Dainese, A., Dalsgaard, H., Danu, A., Das, I., Das, D., Das, K., Dash, S., Dash, A., De, S., de Barros, G., De Caro, A., de Cataldo, G., de Cuveland, J., De Falco, A., De Gruttola, D., Delagrange, H., Deloff, A., Demanov, V., De Marco, N., Dénes, E., De Pasquale, S., Deppman, A., Erasmo, G., de Rooij, R., Diaz Corchero, M., Di Bari, D., Dietel, T., Di Giglio, C., Di Liberto, S., Di Mauro, A., Di Nezza, P., Divià, R., Djuvsland, Ø., Dobrin, A., Dobrowolski, T., Domínguez, I., Dönigus, B., Dordic, O., Driga, O., Dubey, A., Dubla, A., Ducroux, L., Dupieux, P., Dutta Majumdar, A., Dutta Majumdar, M., Elia, D., Emschermann, D., Engel, H., Erazmus, B., Erdal, H., Espagnon, B., Estienne, M., Esumi, S., Evans, D., Eyyubova, G., Fabris, D., Faivre, J., Falchieri, D., Fantoni, A., Fasel, M., Fearick, R., Fedunov, A., Fehlker, D., Feldkamp, L., Felea, D., Fenton Olsen, B., Feofilov, G., Fernández Téllez, A., Ferretti, A., Ferretti, R., Festanti, A., Figiel, J., Figueredo, M., Filchagin, S., Finogeev, D., Fionda, F., Fiore, E., Floris, M., Foertsch, S., Foka, P., Fokin, S., Fragiacomo, Enrico, Francescon, A., Frankenfeld, U., Fuchs, U., Furget, C., Fusco Girard, M., Gaardhøje, J., Gagliardi, M., Gago, A., Gallio, M., Gangadharan, D., Ganoti, P., Garabatos, C., Garcia Solis, E., Garishvili, I., Gerhard, J., Germain, M., Geuna, C., Gheata, M., Gheata, A., Ghidini, B., Ghosh, P., Gianotti, P., Girard, M., Giubellino, P., Gladysz Dziadus, E., Glässel, P., Gomez, R., Ferreiro, E., González Trueba, L., González Zamora, P., Gorbunov, S., Goswami, A., Gotovac, S., Grabski, V., Graczykowski, L., Grajcarek, R., Grelli, A., Grigoras, C., Grigoras, A., Grigoriev, V., Grigoryan, S., Grigoryan, A., Grinyov, B., Grion, N., Gros, P., Grosse Oetringhaus, J., Grossiord, J. 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K., Yoo, J., Yoon, W., Yu, X., Yuan, I., Yushmanov, Zaccolo, Valentina, C., Zach, C., Zampolli, S., Zaporozhet, A., Zarochentsev, P., Závada, N., Zaviyalov, H., Zbroszczyk, P., Zelnicek, I., Zgura, M., Zhalov, H., Zhang, X., Zhang, D., Zhou, Y., Zhou, F., Zhou, J., Zhu, X., Zhu, A., Zichichi, A., Zimmermann, G., Zinovjev, Y., Zoccarato, M., Zynovyev, and M., Zyzak
Subjects: SPECTRUM, MODELS, pion production, HEAVY-ION COLLISIONS, QCD PHASE-TRANSITION, HEAVY-ION COLLISIONS, QCD PHASE-TRANSITION, TOTAL CROSS-SECTIONS, CHEMICAL FREEZE-OUT, QUARK-GLUON PLASMA, FINITE-TEMPERATURE, HADRON-PRODUCTION, MONTE-CARLO, SPECTRUM, MODELS, HADRON-PRODUCTION, kaon production, CHEMICAL FREEZE-OUT, QUARK-GLUON PLASMA, MONTE-CARLO, FINITE-TEMPERATURE, TOTAL CROSS-SECTIONS
Abstract: In this Letter we report the first results on π±, K±, p, and p(bar) production at midrapidity (|y| < 0.5) in central Pb-Pb collisions at √s_NN = 2.76 TeV, measured by the ALICE experiment at the LHC. The pT distributions and yields are compared to previous results at √s_NN = 200 GeV and expectations from hydrodynamic and thermal models. The spectral shapes indicate a strong increase of the radial flow velocity with √s_NN, which in hydrodynamic models is expected as a consequence of the increasing particle density. While the K/π ratio is in line with predictions from the thermal model, the p/π ratio is found to be lower by a factor of about 1.5. This deviation from thermal model expectations is still to be understood.
Published: 2012

50. Cross sections and other parameters ofe − − H2O scattering (E i⩾50 eV)

Author: Joshipura, K N and Vinodkumar, Minaxi
Published: 1996
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