NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.Ji Found 40 matches. 2023LI40 Phys.Rev. C 108, 024002 (2023) Effective field theory with resonant P-wave interaction NUCLEAR STRUCTURE 6He; calculated binding energy. Effective field theory with momentum-dependent nonlocal potential for shallow P-wave resonances applied to neutron-α and neutron-neutron-α systems.
doi: 10.1103/PhysRevC.108.024002
2023WA06 Prog.Part.Nucl.Phys. 129, 104017 (2023) P.Wang, F.He, C.-R.Ji, W.Melnitchouk Nucleon form factors and parton distributions in nonlocal chiral effective theory
doi: 10.1016/j.ppnp.2022.104017
2021EM01 J.Phys.(London) G48, 035101 (2021) Pionless effective field theory evaluation of nuclear polarizability in muonic deuterium
doi: 10.1088/1361-6471/abcb58
2019BA24 Few-Body Systems 60, 41 (2019) The Compton Form Factors of the 4Helium Nucleus NUCLEAR STRUCTURE 4He; calculated form factors.
doi: 10.1007/s00601-019-1509-9
2019DI06 Phys.Rev. C 99, 034004 (2019) N.N.Dinur, O.J.Hernandez, S.Bacca, N.Barnea, C.Ji, S.Pastore, M.Piarulli, R.B.Wiringa Zemach moments and radii of 2, 3H and 3, 4He NUCLEAR STRUCTURE 2,3H, 3,4He; calculated Zemach electromagnetic moments, charge radii, ground-state wave-functions using various few-body methods, such as Numerov algorithm or the harmonic oscillator expansion method for A=2 nuclei, and Monte Carlo (VMC) and Green's function Monte Carlo (GFMC) methods, with hyperspherical harmonics (HH) expansions and momentum-space formulation (HH-p), and the effective interaction scheme in coordinate space (EIHH). Comparison with experimental values. Benchmarking of electromagnetic moments relevant to ongoing experimental efforts of muon-nucleus systems, and to muonic atom data measured by the CREMA collaboration at the Paul Scherrer Institute.
doi: 10.1103/PhysRevC.99.034004
2019HE18 Phys.Rev. C 100, 064315 (2019) O.J.Hernandez, C.Ji, S.Bacca, N.Barnea Probing uncertainties of nuclear structure corrections in light muonic atoms
doi: 10.1103/PhysRevC.100.064315
2018HE03 Phys.Lett. B 778, 377 (2018) O.J.Hernandez, A.Ekstrom, N.N.Dinur, C.Ji, S.Bacca, N.Barnea The deuteron-radius puzzle is alive: A new analysis of nuclear structure uncertainties NUCLEAR STRUCTURE 2H; analyzed available data; deduced discrepancy between the calculated and the corresponding experimental deuteron radii.
doi: 10.1016/j.physletb.2018.01.043
2018JI05 J.Phys.(London) G45, 093002 (2018) C.Ji, S.Bacca, N.Barnea, O.J.Hernandez, N.N.Dinur Ab initio calculation of nuclear-structure corrections in muonic atoms NUCLEAR REACTIONS 1,2,3H, 3,4He(μ, X), E not given; calculated nuclear-structure corrections to the Lamb shift energy of muonic atoms.
doi: 10.1088/1361-6471/aad3eb
2017HA22 J.Phys.(London) G44, 103002 (2017) H.-W.Hammer, C.Ji, D.R.Phillips Effective field theory description of halo nuclei NUCLEAR STRUCTURE 2H, 4,5,6He, 8,11Li, 11,14Be, 15,19,22C; calculated halo, Efimov states, matter radii, one- and two-neutron separation energies. Effective field theory (EFT).
doi: 10.1088/1361-6471/aa83db
2016JI04 Int.J.Mod.Phys. E25, 1641003 (2016) Three-body systems in physics of cold atoms and halo nuclei NUCLEAR STRUCTURE 22C; calculated two-neutron halo parameters, Efimov states.
doi: 10.1142/S0218301316410032
2015CH61 Phys.Rev. C 92, 055203 (2015) H.-M.Choi, C.-R.Ji, Z.Li, H.-Y.Ryu Variational analysis of mass spectra and decay constants for ground state pseudoscalar and vector mesons in the light-front quark model
doi: 10.1103/PhysRevC.92.055203
2015ZH05 Phys.Rev. C 91, 024001 (2015) L.Zhang, Z.-z.Ren, M.Lyu, C.Ji Investigation of 23N in a three-body model NUCLEAR STRUCTURE 22,23N; calculated binding energies, single particle levels, S(2n), neutron, proton and matter rms radii, density distribution profiles, related features of the bound and excited states using Faddeev equations in a three-body model consisting of 21N core and two valence neutrons. Evidence of Efimov physics in the drip-line nucleus 23N.
doi: 10.1103/PhysRevC.91.024001
2014DI06 Phys.Rev. C 89, 064317 (2014) N.N.Dinur, N.Barnea, C.Ji, S.Bacca Efficient method for evaluating energy-dependent sum rules NUCLEAR STRUCTURE 4He; calculated energy-dependent sum rule (EDSR) for unretarded E1 response. Comparison with other methods. Lorentz integral transform method and the Lanczos algorithm. Use in electroweak reactions.
doi: 10.1103/PhysRevC.89.064317
2014JI11 Few-Body Systems 55, 917 (2014) C.Ji, N.N.Dinur, S.Bacca, N.Barnea Nuclear Polarization Effects in Muonic Atoms
doi: 10.1007/s00601-014-0809-3
2014JI12 Phys.Rev. C 90, 044004 (2014) 6He nucleus in halo effective field theory NUCLEAR STRUCTURE 6He; calculated S(2n), two-body amplitudes, properties of the ground state of Borromean halo nucleus 6He described as nnα three-body system in the framework of Halo effective field theory (EFT) built on cluster degrees of freedom. Faddeev formulation. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.044004
2013AC02 Phys.Lett. B 723, 196 (2013) Implications of a matter-radius measurement for the structure of Carbon-22 NUCLEAR STRUCTURE 20,21,22C; calculated binding energies, excited Efimov states, rms matter radius of s-wave Borromean halo nuclei. Comparison with available data.
doi: 10.1016/j.physletb.2013.04.055
2011CH15 Nucl.Phys. A856, 95 (2011) Light-front dynamic analysis of transition form factors in the process of P → V ell ν ell
doi: 10.1016/j.nuclphysa.2011.03.001
2007BA59 Nucl.Phys. A790, 573c (2007) B.L.G.Bakker, J.K.Boomsma, C.-R.Ji Singularities in the light-front Yukawa model
doi: 10.1016/j.nuclphysa.2007.03.097
2007JI11 Nucl.Phys. A790, 583c (2007) C.-R.Ji, B.L.G.Bakker, H.-M.Choi New developments in treacherous points of light-front dynamics
doi: 10.1016/j.nuclphysa.2007.03.099
2006HO06 Phys.Rev. C 73, 054901 (2006) Light-front wavefunction dependence of quark recombination NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated particles invariant transverse momentum spectra, yield ratios, nuclear modification factors. Quark recombination model.
doi: 10.1103/PhysRevC.73.054901
2006TH03 Phys.Rev. D 73, 054023 (2006) Real and virtual nucleon Compton scattering in the perturbative limit NUCLEAR REACTIONS 1H(γ, γ), E=high; calculated real and virtual Compton scattering σ(θ). Perturbative QCD.
doi: 10.1103/PhysRevD.73.054023
2006YU02 J.Phys.(London) G32, 387 (2006) Possibility of determining the parity of the pentaquark Θ+ from photoproduction near threshold NUCLEAR REACTIONS 1n(γ, K-X), E=1.5-3 GeV; 1H(γ, K0X), E=1.5-4 GeV; calculated pentaquark production σ, σ(θ), polarization observables; deduced parity dependence features.
doi: 10.1088/0954-3899/32/3/012
2005TH07 Few-Body Systems 36, 237 (2005) Nucleon Compton Scattering in the Perturbative Limit NUCLEAR REACTIONS 1H(γ, γ), E not given; calculated σ, phase for real and virtual photons.
doi: 10.1007/s00601-004-0107-6
2004JI04 Nucl.Phys. A737, 255 (2004) Perspectives of light-front dynamics in few-body systems
doi: 10.1016/j.nuclphysa.2004.03.086
2004YU08 Phys.Rev. C 70, 045205 (2004) Investigating the parity of the exotic Θ+ baryon from kaon photoproduction NUCLEAR REACTIONS 1n(γ, K-X), E=1.5-4 GeV; 1H(γ, K0X), E=1.5-4 GeV; calculated pentaquark production associated σ, σ(θ), dependence on parity.
doi: 10.1103/PhysRevC.70.045205
2002JI02 Nucl.Phys. A699, 344c (2002) Exploring Timelike Exclusive Processes in the Light-Front Approach
doi: 10.1016/S0375-9474(01)01517-2
2001BR37 Phys.Rev. C64, 055204 (2001) S.J.Brodsky, J.R.Hiller, C.-R.Ji, G.A.Miller Perturbative QCD and Factorization of Coherent Pion Photoproduction on the Deuteron NUCLEAR REACTIONS 2H(γ, π0), E < 40 GeV; calculated photoproduction amplitude. Perturbative QCD, factorization of amplitude, comparison with data.
doi: 10.1103/PhysRevC.64.055204
2001CH05 Nucl.Phys. A679, 735 (2001) Exploring the Time-Like Region for the Elastic Form Factor in the Light-Front Quantization
doi: 10.1016/S0375-9474(00)00376-6
1999JI05 Fizika(Zagreb) B8, 321 (1999) Meson Electroweak Form Factors in the Light-Cone Approach
1998CO08 Nucl.Phys. A631, 640c (1998) S.R.Cotanch, A.P.Szczepaniak, E.S.Swanson, C.-R.Ji QCD Hamiltonian Approach for the Glueball Spectrum
doi: 10.1016/S0375-9474(98)00082-7
1998JI07 Phys.Rev. C58, 1205 (1998) C.-R.Ji, R.Kaminski, L.Lesniak, A.Szczepaniak, R.Williams Coupled Channel Analysis of S-Wave ππ and K(K-bar) Photoproduction
doi: 10.1103/PhysRevC.58.1205
1997CH15 Nucl.Phys. A618, 291 (1997) Light-Cone Quark Model Predictions for Radiative Meson Decays
doi: 10.1016/S0375-9474(97)00052-3
1995SZ06 Phys.Rev. C52, 2738 (1995) A.Szczepaniak, C.-R.Ji, S.R.Cotanch Nucleon Structure in a Relativistic Quark Model NUCLEAR STRUCTURE 1H, 1n; calculated electric, magnetic form factors, structure function ratio. Relativistic quark model, comparison to baryons.
doi: 10.1103/PhysRevC.52.2738
1993CO12 Phys.Scr. 48, 217 (1993) S.R.Cotanch, R.A.Williams, C.-R.Ji Kaon Electromagnetic Production and Radiative Capture Near Hyperon Thresholds NUCLEAR REACTIONS 1H(γ, X), E=1.25-2.5 GeV; calculated K+ electromagnetic production near hyperon thresholds. Real, virtual photons, covariant perturbation theory.
doi: 10.1088/0031-8949/48/2/019
1993WI11 Phys.Rev. C48, 1318 (1993) R.A.Williams, C.-R.Ji, S.R.Cotanch Kinematically Accessible Vector Meson Resonance Enhancements in p(K-, e+e-) (Lambda), Σ0, (Lambda)(1405) NUCLEAR REACTIONS 1H(K-, X), E not given; calculated two-body virtual photon radiative capture σ vs momentum transfer squared; deduced kinematically accessible vector meson resonance enhancements features, (K-, e+e-)Y, Y=lambda, Σ0 production.
doi: 10.1103/PhysRevC.48.1318
1992WI11 Phys.Rev. C46, 1617 (1992) R.A.Williams, C.-R.Ji, S.R.Cotanch Hyperon Electroproduction in a Crossing and Duality Constrained Model NUCLEAR REACTIONS 1H(γ, K+X), E < 2.5 GeV; calculated σ(θ) vs E. Hyperon electroproduction, crossing, duality constrained model.
doi: 10.1103/PhysRevC.46.1617
1991WI01 Phys.Rev. C43, 452 (1991) R.A.Williams, C.-R.Ji, S.R.Cotanch Crossing and Duality Consistent Study of Lambda, Σ0, and Lambda(1405) Production by Kaon Photoproduction and Radiative Capture NUCLEAR REACTIONS 1H(γ, K+X), E=1.1-1.7 GeV; calculated σ(θ) vs E. 1H(K-, γX), E at 0.1-0.6 GeV/c; calculated σ(θ). Crossing, duality consistent model, Lambda, other particle production.
doi: 10.1103/PhysRevC.43.452
1990CO39 J.Phys.(Paris), Colloq.C-6, 491 (1990) S.R.Cotanch, R.A.Williams, C.-R.Ji The Importance of Polarization in Kaon Photoproduction and Radiative Capture NUCLEAR REACTIONS 1H(K-, γX), E at 0.1-0.6 GeV/c; 1H(γ, K+X), E ≈ 0.9-1.4 GeV; calculated σ(θ) for hyperon production.
1988JI03 Phys.Rev. C38, 2691 (1988) Crossing Constraints for Hyperon Reactions NUCLEAR REACTIONS 1H(K-, K-), (K+, K+), (p-bar, K-), (γ, K+), E < 3 GeV/c; calculated σ(θ).
doi: 10.1103/PhysRevC.38.2691
1986BR08 Phys.Rev. D33, 2653 (1986) Factorization Property of the Deuteron NUCLEAR STRUCTURE 2H; calculated wave function cluster decomposition, reduced form factor. Field theoretic model, quark exchange.
doi: 10.1103/PhysRevD.33.2653
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