NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = J.Carbonell Found 66 matches. 2023CA18 Eur.Phys.J. A 59, 259 (2023) J.Carbonell, G.Hupin, S.Wycech Comparison of N-bar N optical models
doi: 10.1140/epja/s10050-023-01161-x
2023LA03 Phys.Rev.Lett. 130, 102501 (2023) R.Lazauskas, E.Hiyama, J.Carbonell Low Energy Structures in Nuclear Reactions with 4n in the Final State NUCLEAR STRUCTURE 8He, 2,4NN; calculated strength and low energy four-neutron response functions with the AV18 nn interaction, low energy 4n response functions for the scaled nn MT13 potential; deduced the sharp low energy peak observed by studying the missing mass spectra of four neutrons as a consequence of dineutron-dineutron correlations.
doi: 10.1103/PhysRevLett.130.102501
2022AU03 Eur.Phys.J. A 58, 88 (2022) T.Aumann, W.Bartmann, O.Boine-Frankenheim, A.Bouvard, A.Broche, F.Butin, D.Calvet, J.Carbonell, P.Chiggiato, H.De Gersem, R.De Oliveira, T.Dobers, F.Ehm, J.Ferreira Somoza, J.Fischer, M.Fraser, E.Friedrich, A.Frotscher, M.Gomez-Ramos, J.-L.Grenard, A.Hobl, G.Hupin, A.Husson, P.Indelicato, K.Johnston, C.Klink, Y.Kubota, R.Lazauskas, S.Malbrunot-Ettenauer, N.Marsic, W.F.O Muller, S.Naimi, N.Nakatsuka, R.Necca, D.Neidherr, G.Neyens, A.Obertelli, Y.Ono, S.Pasinelli, N.Paul, E.C.Pollacco, D.Rossi, H.Scheit, M.Schlaich, A.Schmidt, L.Schweikhard, R.Seki, S.Sels, E.Siesling, T.Uesaka, M.Vilen, M.Wada, F.Wienholtz, S.Wycech, S.Zacarias PUMA, antiProton unstable matter annihilation
doi: 10.1140/epja/s10050-022-00713-x
2022HI06 Phys.Lett. B 833, 137367 (2022) E.Hiyama, R.Lazauskas, J.Carbonell 7H ground state as a 3H+4n resonance NUCLEAR STRUCTURE 3,4,5,7H, 4NN; analyzed available data; calculated S- and P-wave n-t phase shifts, resonant states, energy trajectories, eigenvalues of the 7H hamiltonian as a function of the stabilization parameter. The solution of the 5-body Schrodinger equation has been obtained by means of the variational Gaussian expansion approach and the resonance parameters.
doi: 10.1016/j.physletb.2022.137367
2022HI10 Phys.Rev. C 106, 064001 (2022) E.Hiyama, R.Lazauskas, J.Carbonell, T.Frederico Scaling of the 19B two-neutron halo properties close to unitarity NUCLEAR STRUCTURE 19B; calculated rms radii, S(2n), ground-state energy, n-17B scattering length, rms relative separation distances in the 17B+n+n system. Faddeev equation formalism in configuration space with Gaussian expansion method are used for solving three-body problem. Calculations with charge independent Bonn-A and charge dependent AV18 nn-interactions.
doi: 10.1103/PhysRevC.106.064001
2021LA14 Phys.Lett. B 820, 136573 (2021), Erratum Phys.Lett. B 841, 137936 (2023) Antiproton-deuteron hydrogenic states in optical models
doi: 10.1016/j.physletb.2021.136573
2021MA23 Eur.Phys.J. A 57, 105 (2021) The quest for light multineutron systems NUCLEAR REACTIONS 12C, 4He(π-, π+), E=165 MeV; 7Li(7Li, 10C), E<65 MeV; analyzed available data. 3,4NN; deduced miltineutron systems.
doi: 10.1140/epja/s10050-021-00417-8
2021YD01 Eur.Phys.J. A 57, 303 (2021) Protonium annihilation densities in a unitary coupled channel model
doi: 10.1140/epja/s10050-021-00609-2
2019HI05 Phys.Rev. C 100, 011603 (2019) E.Hiyama, R.Lazauskas, F.M.Marques, J.Carbonell Modeling 19B as a 17B - n - n three-body system in the unitary limit NUCLEAR STRUCTURE 19B; calculated n-17B scattering length, radial potential, ground state energy and probability amplitude of ground state using three-body (17B-n-n) system model, with the two-body subsystems 17B-n and n-n as unbound (virtual) states close to the unitary limit. Discussed link with the Efimov physics, and possibility to explain recently discovered resonant states in 20,21B.
doi: 10.1103/PhysRevC.100.011603
2019LA07 Phys.Lett. B 791, 335 (2019) R.Lazauskas, E.Hiyama, J.Carbonell Ab initio calculations of 5H resonant states NUCLEAR STRUCTURE 5H; calculated resonant states, J, π using the 5-body Faddeev-Yakubovsky equations in configuration space with realistic nuclear Hamiltonians.
doi: 10.1016/j.physletb.2019.02.047
2017CA16 Few-Body Systems 58, 67 (2017) J.Carbonell, R.Lazauskas, E.Hiyama, M.Kamimura On the Possible Existence of Four Neutron Resonances NUCLEAR REACTIONS 3He(n, n), E=0.03-10 MeV;3He(n, x), E not given; calculated possible tetraneutron resonance trajectory for 0+ state; deduced resonance, σ, resonance energy and width vs other parameters, higher 4n resonances, tetraneutron production response function via double charge exchange; deduced parameters.
doi: 10.1007/s00601-017-1219-0
2017LA11 Prog.Theor.Exp.Phys. 2017, 073D03 (2017) R.Lazauskas, J.Carbonell, E.Hiyama Modeling the double charge exchange response function for a tetraneutron system NUCLEAR REACTIONS 4He(8He, 8Be)4NN, E<8 MeV; analyzed available data; calculated σ, response functions, 4n resonance trajectory.
doi: 10.1093/ptep/ptx078
2017PA16 Phys.Rev. C 95, 054001 (2017) M.Pavon Valderrama, M.Sanchez Sanchez, C.-J.Yang, B.Long, J.Carbonell, U.van Kolck Power counting in peripheral partial waves: The singlet channels
doi: 10.1103/PhysRevC.95.054001
2016HI03 Phys.Rev. C 93, 044004 (2016) E.Hiyama, R.Lazauskas, J.Carbonell, M.Kamimura Possibility of generating a 4-neutron resonance with a T=3/2 isospin 3-neutron force NUCLEAR STRUCTURE 4n; calculated narrow resonant states of tetraneutron for Jπ=0+, 2+ and 2-. 4H, 4He, 4Li; calculated energies of the lowest T=1, Jπ=2- states. 3n; calculated resonance trajectories for Jπ=3/2-, 1/2- and 1/2+ states. Complex scaling method (CSM) for resonance positions and widths. Gaussian expansion method used to solve Schrodinger equation and Lagrange-mesh technique to solve Faddeev-Yakubovsky (FY) equation. Comparison with recent experimental data from RIKEN.
doi: 10.1103/PhysRevC.93.044004
2015DY02 Phys.Lett. B 744, 391 (2015) S.Dymov, T.Azaryan, Z.Bagdasarian, S.Barsov, J.Carbonell, D.Chiladze, R.Engels, R.Gebel, K.Grigoryev, M.Hartmann, A.Kacharava, A.Khoukaz, V.Komarov, P.Kulessa, A.Kulikov, V.Kurbatov, N.Lomidze, B.Lorentz, G.Macharashvili, D.Mchedlishvili, S.Merzliakov, M.Mielke, M.Mikirtychyants, S.Mikirtychyants, M.Nioradze, H.Ohm, D.Prasuhn, F.Rathmann, V.Serdyuk, H.Seyfarth, V.Shmakova, H.Stroher, M.Tabidze, S.Trusov, D.Tsirkov, Yu.Uzikov, Yu.Valdau Analysing powers and spin correlations in deuteron-proton charge exchange at 726 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=726 MeV; measured reaction products, Ep, Ip; deduced yields, analysing powers. Comparison with an impulse approximation calculation.
doi: 10.1016/j.physletb.2015.04.019
2015MA16 Phys.Rev. C 91, 034602 (2015) D.Mancusi, A.Boudard, J.Carbonell, J.Cugnon, J.-C.David, S.Leray Improving the description of proton-induced one-nucleon removal in intranuclear-cascade models NUCLEAR REACTIONS 40Ca(p, 39Ca), (p, 39K), E=500-1000 MeV; 208Pb(p, 207Pb), (p, 207Tl), E=500-1000 MeV; calculated one-proton- and one-neutron-removal cross sections, mass distribution of the residues, isotopic distributions of Z=76-83 residues, double-differential cross sections for the production of neutrons. INCL/ABLA07, Isabel/ABLA07, CEM03.03 and Geant4s Bertini model, INCL/GEMINI++ calculations. Comparison with experimental data. NUCLEAR STRUCTURE 208Pb; calculated proton kinetic-energy and space densities, space-kinetic-energy density contours, proton and neutron densities using initial conditions of the standard intranuclear-cascade models (INCL).
doi: 10.1103/PhysRevC.91.034602
2014BA37 Few-Body Systems 55, 683 (2014) B.L.G.Bakker, J.Carbonell, C.Elster, E.Epelbaum, N.Kalantar-Nayestanaki, J.-M.Richard Panel Session on the Future of Few-Body Physics
doi: 10.1007/s00601-014-0821-7
2014CA33 Few-Body Systems 55, 687 (2014) Transition Electromagnetic Form Factor in the Minkowski Space Bethe-Salpeter Approach
doi: 10.1007/s00601-013-0770-6
2013MC08 Eur.Phys.J. A 49, 49 (2013) D.Mchedlishvili, S.Barsov, J.Carbonell, D.Chiladze, S.Dymov, A.Dzyuba, R.Engels, R.Gebel, V.Glagolev, K.Grigoryev, P.Goslawski, M.Hartmann, A.Kacharava, V.Kamerdzhiev, I.Keshelashvili, A.Khoukaz, V.Komarov, P.Kulessa, A.Kulikov, A.Lehrach, N.Lomidze, B.Lorentz, G.Macharashvili, R.Maier, S.Merzliakov, M.Mielke, M.Mikirtychyants, S.Mikirtychyants, M.Nioradze, H.Ohm, M.Papenbrock, D.Prasuhn, F.Rathmann, V.Serdyuk, H.Seyfarth, H.J.Stein, E.Steffens, H.Stockhorst, H.Stroher, M.Tabidze, S.Trusov, Yu.Uzikov, Yu.Valdau, C.Wilkin The neutron-proton charge-exchange amplitudes measured in the dp → ppn reaction
doi: 10.1140/epja/i2013-13049-0
2013MC12 Phys.Lett. B 726, 145 (2013) D.Mchedlishvili, S.Barsov, J.Carbonell, D.Chiladze, S.Dymov, A.Dzyuba, R.Engels, R.Gebel, V.Glagolev, K.Grigoryev, P.Goslawski, M.Hartmann, O.Imambekov, A.Kacharava, V.Kamerdzhiev, I.Keshelashvili, A.Khoukaz, V.Komarov, P.Kulessa, A.Kulikov, A.Lehrach, N.Lomidze, B.Lorentz, G.Macharashvili, R.Maier, S.Merzliakov, M.Mielke, M.Mikirtychyants, S.Mikirtychyants, M.Nioradze, H.Ohm, M.Papenbrock, D.Prasuhn, F.Rathmann, V.Serdyuk, H.Seyfarth, H.J.Stein, E.Steffens, H.Stockhorst, H.Stroher, M.Tabidze, S.Trusov, Yu.Uzikov, Yu.Valdau, C.Wilkin Excitation of the Δ(1232) isobar in deuteron charge exchange on hydrogen at 1.6, 1.8, and 2.3 GeV NUCLEAR REACTIONS 1H(polarized d, n), E=1.6, 1.8, 2.3 GeV; measured reaction products; deduced σ(E), analysing powers. Comparison with calculations.
doi: 10.1016/j.physletb.2013.08.018
2013MO41 Ann.Nucl.Energy 54, 167 (2013) B.Morillon, R.Lazauskas, J.Carbonell Influence of the ab initio n-d cross sections in the critical heavy-water benchmarks
doi: 10.1016/j.anucene.2012.06.032
2011DE19 Eur.Phys.J. A 47, 57 (2011) F.de Soto, J.C.Angles d'Auriac, J.Carbonell The nuclear Yukawa model on a lattice
doi: 10.1140/epja/i2011-11057-8
2011LA15 Phys.Rev. C 84, 034002 (2011) Application of the complex-scaling method to few-body scattering
doi: 10.1103/PhysRevC.84.034002
2011VI06 Phys.Rev. C 84, 054010 (2011) M.Viviani, A.Deltuva, R.Lazauskas, J.Carbonell, A.C.Fonseca, A.Kievsky, L.E.Marcucci, S.Rosati Benchmark calculation of n-3H and p-3He scattering NUCLEAR REACTIONS 3He(p, p), E=2.25, 4.05, 5.54 MeV; 3H(n, n), E=1.0, 2.0, 3.5, 6.0 MeV; analyzed phase shifts, mixing parameters, total cross sections, differential σ(θ), neutron and triton analyzing powers using AGS, HS, and FY methods with I-N3LO, Argonne v18, CD Bonn interactions for four-nucleon problem.
doi: 10.1103/PhysRevC.84.054010
2010CA32 Eur.Phys.J. A 46, 387 (2010) Solving the Bethe-Salpeter equation for two fermions in Minkowski space
doi: 10.1140/epja/i2010-11055-4
2009CA04 Eur.Phys.J. A 39, 53 (2009) J.Carbonell, V.A.Karmanov, M.Mangin-Brinet Electromagnetic form factor via Bethe-Salpeter amplitude in Minkowski space
doi: 10.1140/epja/i2008-10690-6
2009CH31 Eur.Phys.J. A 40, 23 (2009) D.Chiladze, J.Carbonell, S.Dymov, A.Dzyuba, V.Glagolev, M.Hartmann, A.Kacharava, I.Keshelashvili, A.Khoukaz, V.Komarov, P.Kulessa, A.Kulikov, N.Lomidze, G.Macharashvili, Y.Maeda, D.Mchedlishvili, T.Mersmann, S.Merzliakov, M.Mielke, S.Mikirtychyants, M.Nekipelov, M.Nioradze, H.Ohm, F.Rathmann, H.Stroher, M.Tabidze, S.Trusov, Yu.Uzikov, Yu.Valdau, C.Wilkin The dp → ppn reaction as a method to study neutron-proton charge-exchange amplitudes
doi: 10.1140/epja/i2008-10731-2
2007DE03 Nucl.Phys. B(Proc.Supp.) S164, 252 (2007) F.de Soto, J.Carbonell, C.Roiesnel, Ph.Boucaud, J.P.Leroy, O.Pene Nuclear models on a lattice
doi: 10.1016/j.nuclphysbps.2006.11.086
2007DE22 Eur.Phys.J. A 31, 777 (2007) F.De Soto, J.Carbonell, C.Roiesnel, Ph.Boucaud, J.P.Leroy, O.Pene Yukawa model on a lattice: Two-body states
doi: 10.1140/epja/i2007-10005-7
2007DE44 Nucl.Phys. A790, 410c (2007) F.De Soto, J.Carbonell, C.Roiesnel, Ph.Boucaud, J.P.Leroy, O.Pene Two body scattering length of Yukawa model on a lattice
doi: 10.1016/j.nuclphysa.2007.03.141
2007HA21 Phys.Rev.Lett. 99, 022506 (2007) K.Hagino, H.Sagawa, J.Carbonell, P.Schuck Coexistence of BCS- and BEC-Like Pair Structures in Halo Nuclei
doi: 10.1103/PhysRevLett.99.022506
2007KA43 Nucl.Phys. A790, 598c (2007) V.A.Karmanov, J.Carbonell, M.Mangin-Brinet Bethe-Salpeter equation with cross-ladder kernel in Minkowski and Euclidean spaces
doi: 10.1016/j.nuclphysa.2007.03.101
2006CA11 Eur.Phys.J. A 27, 11 (2006) Cross-ladder effects in Bethe-Salpeter and light-front equations
doi: 10.1140/epja/i2005-10194-y
2006CH23 Phys.Lett. B 637, 170 (2006) D.Chiladze, J.Carbonell, S.Dymov, V.Glagolev, M.Hartmann, V.Hejny, A.Kacharava, I.Keshelashvili, A.Khoukaz, H.R.Koch, V.Komarov, P.Kulessa, A.Kulikov, G.Macharashvili, Y.Maeda, T.Mersmann, S.Merzliakov, S.Mikirtytchiants, A.Mussgiller, M.Nioradze, H.Ohm, F.Rathmann, R.Schleichert, H.J.Stein, H.Stroher, Yu.Uzikov, S.Yaschenko, C.Wilkin Vector and tensor analysing powers in deuteron-proton breakup reactions at intermediate energies NUCLEAR REACTIONS 1H(polarized d, np), (polarized d, 2p), E at 2.4 GeV/c; measured vector and tensor analyzing powers. Comparison with impulse approximation calculations.
doi: 10.1016/j.physletb.2006.04.031
2006KA10 Eur.Phys.J. A 27, 1 (2006) Solving Bethe-Salpeter equation in Minkowski space
doi: 10.1140/epja/i2005-10193-0
2005LA06 Phys.Rev. C 71, 034004 (2005) R.Lazauskas, J.Carbonell, A.C.Fonseca, M.Viviani, A.Kievsky, S.Rosati Low energy n-3H scattering: A novel testground for nuclear interactions NUCLEAR REACTIONS 3H(n, n), E(cm)=0.1-5 MeV; calculated phase shifts, total σ. Three methods compared.
doi: 10.1103/PhysRevC.71.034004
2005LA11 Phys.Rev. C 71, 044004 (2005) Three-neutron resonance trajectories for realistic interaction models NUCLEAR STRUCTURE 3n; calculated resonance trajectories.
doi: 10.1103/PhysRevC.71.044004
2005LA27 Phys.Rev. C 72, 034003 (2005) Is a physically observable tetraneutron resonance compatible with realistic nuclear interactions? NUCLEAR STRUCTURE 4n; calculated resonance energies; deduced no observable state. Faddeev-Yakubovski equations, realistic interactions, complex scaling and analytical continuation in the coupling constant.
doi: 10.1103/PhysRevC.72.034003
2004LA16 Few-Body Systems 34, 105 (2004) Ab-Initio Calculations of Four-Nucleon Elastic Scattering NUCLEAR REACTIONS 3H(n, n), E(cm)=2.625 MeV; 3He(p, p), E(cm)=4.1325 MeV; calculated σ(θ). 3H(n, n), E < 10 MeV; calculated total σ. 3He(p, p), E(cm) < 0.6 MeV; calculated σ(E, θ=120°). Faddeev-Yakubovski equations, comparison with data.
doi: 10.1007/s00601-004-0049-z
2004LA22 Phys.Rev. C 70, 044002 (2004) Testing nonlocal nucleon-nucleon interactions in four-nucleon systems NUCLEAR STRUCTURE 3H, 3,4He; calculated binding energies, radii, partial wave contributions. 4He calculated continuum states features. Fadeev-Yakubovski equations, nonlocal nucleon-nucleon interaction models. NUCLEAR REACTIONS 3H(n, X), E=0.1-10 MeV; calculated scattering lengths, phase shifts, total σ. Fadeev-Yakubovski equations, nonlocal nucleon-nucleon interaction models.
doi: 10.1103/PhysRevC.70.044002
2003CA08 Phys.Rev. C 67, 037001 (2003) Three-boson relativistic bound states with zero-range two-body interaction
doi: 10.1103/PhysRevC.67.037001
2003MA74 Phys.Rev. C 68, 055203 (2003) M.Mangin-Brinet, J.Carbonell, V.A.Karmanov Two-fermion relativistic bound states in light-front dynamics
doi: 10.1103/PhysRevC.68.055203
2001CA18 Nucl.Phys. A684, 218c (2001) The Continuum Spectrum of the 4N System: Results and challenges NUCLEAR REACTIONS 3H(n, n), E ≈ 0-6 MeV; calculated σ, σ(θ); 3H(p, p), E(cm) ≈ 50-500 keV; calculated σ(θ=120°); deduced continuum states features.
doi: 10.1016/S0375-9474(01)00417-1
2001CA52 Nucl.Phys. A692, 11c (2001) Selected Topics on Low Energy Antiproton Physics
doi: 10.1016/S0375-9474(01)01154-X
2001KA24 Nucl.Phys. A684, 366c (2001) V.A.Karmanov, J.Carbonell, M.Mangin-Brinet Relativistic Wave Functions and Energies for Nonzero Angular Momentum States in Light-Front Dynamics
doi: 10.1016/S0375-9474(01)00387-6
2001MA61 Nucl.Phys. A689, 463c (2001) Bound States of Two Scalar Particles in Light-Front Dynamics
doi: 10.1016/S0375-9474(01)00879-X
2001VO14 Nucl.Phys. A689, 529c (2001) Antihydrogen-Hydrogen Annihilation at Sub-Kelvin Temperatures NUCLEAR REACTIONS 1,2H(p-bar, X), E=low; calculated annihilation σ. Coupled-channels approach.
doi: 10.1016/S0375-9474(01)00897-1
2000CA12 Nucl.Phys. A663-664, 361c (2000) Deuteron Electromagnetic Form Factors in the Light-Front Dynamics NUCLEAR STRUCTURE 2H; calculated form factors. Comparisons with data.
doi: 10.1016/S0375-9474(99)00617-X
1999CA38 Eur.Phys.J. A 6, 9 (1999) Deuteron Electromagnetic Form Factors in the Light-Front Dynamics NUCLEAR STRUCTURE 2H; calculated electromagnetic form factors, structure functions; deduced influence of nucleon form factors. Relativistic nucleon-meson dynamics.
doi: 10.1007/s100500050311
1999CI02 Phys.Lett. 447B, 199 (1999) F.Ciesielski, J.Carbonell, C.Gignoux Low Energy n + t Scattering and the NN Forces NUCLEAR REACTIONS 3H(n, n), E < 10 MeV; calculated σ, phase shifts. Faddeev-Yakubovsky equations, several interactions compared. Comparison with data.
doi: 10.1016/S0370-2693(98)01501-9
1998CI01 Nucl.Phys. A631, 653c (1998) F.Ciesielski, J.Carbonell, C.Gignoux Scattering States in the Four Nucleons System NUCLEAR REACTIONS 3H(n, n), E < 10 MeV; calculated σ, partial waves contributions. Fadeev-Yakubowski equations.
doi: 10.1016/S0375-9474(98)00085-2
1998CI04 Phys.Rev. C58, 58 (1998) Solutions of the Faddeev-Yakubovsky Equations for the Four Nucleon Scattering States NUCLEAR REACTIONS 3H(n, n), E < 10 MeV; calculated σ. 3H(p, p), (p, n), (p, d), E not given; calculated S-matrix elements. Fadeev-Yakubovsky equations.
doi: 10.1103/PhysRevC.58.58
1998VO06 Phys.Rev. A57, 4335 (1998) Antiproton-Hydrogen Annihilation at Subkelvin Temperatures NUCLEAR REACTIONS 1H(p-bar, X), E at rest; calculated annihilation σ. ATOMIC PHYSICS 1H(p-bar, X), E at rest; calculated protonium formation σ.
doi: 10.1103/PhysRevA.57.4335
1998VO14 Hyperfine Interactions 115, 143 (1998) Antiproton-Hydrogen and Antihydrogen-Hydrogen Annihilation at Sub-Kelvin Temperatures NUCLEAR REACTIONS 1H(p-bar, X), E=low; calculated annihilation σ; deduced role of metastable states. Coupled-channels approach.
doi: 10.1023/A:1012604923540
1997CA22 Phys.Lett. 397B, 345 (1997) J.Carbonell, K.V.Protasov, A.Zenoni (p-bar)p Low Energy Parameters from Annihilation Cross Section Data NUCLEAR REACTIONS 1H(p-bar, X), E at 43.6-174.4 MeV/c; analyzed total annihilation σ; deduced spin-averaged scattering amplitude parameters.
doi: 10.1016/S0370-2693(97)00190-1
1996CA20 Z.Phys. A355, 87 (1996) Annihilation of Slow Antiprotons in Flight and in Traps NUCLEAR REACTIONS 1H(p-bar, X), E=low; analyzed annihilation σ. Coulomb interaction included.
doi: 10.1007/s002180050082
1995CA03 Nucl.Phys. A581, 625 (1995) Relativistic Deuteron Wave Function in the Light-Front Dynamics NUCLEAR STRUCTURE 2H; calculated relativistic wave functions. Light front dynamics.
doi: 10.1016/0375-9474(94)00430-U
1995CA19 Nucl.Phys. A589, 713 (1995) Relativistic Wave Function of the np System in the J(π) = 0+ Continuous Spectrum State
doi: 10.1016/0375-9474(95)00129-O
1994DA37 Nuovo Cim. 107A, 2409 (1994) O.D.Dalkarov, J.Carbonell, K.V.Protasov Baryon-Antibaryon States: Spectra, production, decay NUCLEAR REACTIONS 1H(n-bar, n-bar), E at ≤ 300 MeV/c; calculated σ vs momentum. 1H(p-bar, X), E ≈ threshold; calculated σ for (lambda-bar)(lambda) production.
doi: 10.1007/BF02734009
1993KO24 Nucl.Phys. A556, 621 (1993) S.Kox, J.Carbonell, C.Furget, T.Motobayashi, C.Perrin, C.Wilkin, J.Arvieux, J.P.Bocquet, A.Boudard, G.Gaillard, M.Garcon, L.Ghedira, G.Guillaume, F.Merchez, D.Rebreyend, J.Yonnet Cross Section and Deuteron Analysing Powers of the 1H(d, 2p)n Reaction at 200 and 350 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=200, 350 MeV; measured missing mass spectra, σ(θ) vs momentum transfer squared, analyzing powers; deduced figures of merit. Comparison with impulse approximation model.
doi: 10.1016/0375-9474(93)90473-B
1992CA27 J.Phys.(London) G18, 1863 (1992) The Determination of Strong p(bar)p Scattering Length from Protonium Level Shifts NUCLEAR REACTIONS 1H(p-bar, p-bar), E=low; calculated scattering lengths, protonium level shifts, widths. Coulomb corrections, spin-averaging.
doi: 10.1088/0954-3899/18/11/019
1991CA15 Nucl.Phys. A529, 653 (1991) J.Carbonell, M.B.Barbaro, C.Wilkin Deuteron Analysing Powers in the Charge Exchange Reaction d(pol)p → (pp)n NUCLEAR REACTIONS 1H(polarized d, 2p), E=200 MeV; calculated differential σ, analyzing power. Impulse approximation.
doi: 10.1016/0375-9474(91)90590-3
1991KO27 Phys.Lett. 266B, 264 (1991) S.Kox, C.Perrin, J.Arvieux, J.P.Bocquet, A.Boudard, J.Carbonell, G.Gaillard, M.Garcon, L.Ghedira, G.Guillaume, F.Merchez, T.Motobayashi, D.Rebreyend, C.Wilkin, J.Yonnet The 1H(d, 2p)n Reaction as Basis for a Deuteron Tensor Polarimeter at Intermediate Energies NUCLEAR REACTIONS 1H(polarized d, 2p), E=350 MeV; measured σ(θ) vs q2, tensor analyzing power vs momentum transfer. Deuteron tensor polarimeter. Impulse approximation.
doi: 10.1016/0370-2693(91)91037-V
1990DA21 Yad.Fiz. 52, 1670 (1990); Sov.J.Nucl.Phys. 52, 1052 (1990) O.D.Dalkarov, J.Carbonell, K.V.Protasov The Coupled-Channels Model for Describing the Low-Energy Nucleon-Antinucleon Interaction NUCLEAR REACTIONS 1H(p-bar, p-bar), E at 100-300 MeV/c; calculated σ(E). Coupled-channels model.
1989MO22 Phys.Lett. 233B, 69 (1989) T.Motobayashi, C.Perrin, J.Carbonell, C.Wilkin, S.Kox, F.Merchez, Nguyen Van Sen, D.Rebreyend, G.Guillaume, J.Arvieux, J.Yonnet, B.Bonin, A.Boudard, M.Garcon, J.Guillot, G.Gaillard Measurements of Tensor Analyzing Powers in the 1H(d, 2p)n Reaction at 200 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=200 MeV; measured differential σ, vector, tensor analyzing power vs momentum.
doi: 10.1016/0370-2693(89)90617-5
1985CA04 J.Phys.(London) G11, 325 (1985) J.Carbonell, F.Brut, R.Arvieu, J.Touchard Classical Properties and Semiclassical Quantisation of a Spherical Nuclear Potential NUCLEAR STRUCTURE A=16-208; calculated semi-classical, quantum mechanical single particle energies. 16O, 208Pb; calculated single particle level, resonance energies.
doi: 10.1088/0305-4616/11/3/011
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