NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = A.W.Thomas Found 249 matches. Showing 1 to 100. [Next]2023LE09 Phys.Rev. C 108, 015804 (2023) J.Leong, T.F.Motta, A.W.Thomas, P.A.M.Guichon Dense nuclear matter with phenomenological short distance repulsion
doi: 10.1103/PhysRevC.108.015804
2021AC08 Eur.Phys.J. A 57, 261 (2021) A.Accardi, A.Afanasev, I.Albayrak, S.F.Ali, M.Amaryan, J.R.M.Annand, J.Arrington, A.Asaturyan, H.Atac, H.Avakian, T.Averett, C.Ayerbe Gayoso, X.Bai, L.Barion, M.Battaglieri, V.Bellini, R.Beminiwattha, F.Benmokhtar, V.V.Berdnikov, J.C.Bernauer, V.Bertone, A.Bianconi, A.Biselli, P.Bisio, P.Blunden, M.Boer, M.Bondi, K.-T.Brinkmann, W.J.Briscoe, V.Burkert, T.Cao, A.Camsonne, R.Capobianco, L.Cardman, M.Carmignotto, M.Caudron, L.Causse, A.Celentano, P.Chatagnon, J.-P.Chen, T.Chetry, G.Ciullo, E.Cline, P.L.Cole, M.Contalbrigo, G.Costantini, A.D'Angelo, L.Darme, D.Day, M.Defurne, M.De Napoli, A.Deur, R.De Vita, N.D'Hose, S.Diehl, M.Diefenthaler, B.Dongwi, R.Dupre, H.Dutrieux, D.Dutta, M.Ehrhart, L.El Fassi, L.Elouadrhiri, R.Ent, J.Erler, I.P.Fernando, A.Filippi, D.Flay, T.Forest, E.Fuchey, S.Fucini, Y.Furletova, H.Gao, D.Gaskell, A.Gasparian, T.Gautam, F.-X.Girod, K.Gnanvo, J.Grames, G.N.Grauvogel, P.Gueye, M.Guidal, S.Habet, T.J.Hague, D.J.Hamilton, O.Hansen, D.Hasell, M.Hattawy, D.W.Higinbotham, A.Hobart, T.Horn, C.E.Hyde, H.Ibrahim, A.Ilyichev, A.Italiano, K.Joo, S.J.Joosten, V.Khachatryan, N.Kalantarians, G.Kalicy, B.Karky, D.Keller, C.Keppel, M.Kerver, M.Khandaker, A.Kim, J.Kim, P.M.King, E.Kinney, V.Klimenko, H.-S.Ko, M.Kohl, V.Kozhuharov, B.T.Kriesten, G.Krnjaic, V.Kubarovsky, T.Kutz, L.Lanza, M.Leali, P.Lenisa, N.Liyanage, Q.Liu, S.Liuti, J.Mammei, S.Mantry, D.Marchand, P.Markowitz, L.Marsicano, V.Mascagna, M.Mazouz, M.McCaughan, B.McKinnon, D.McNulty, W.Melnitchouk, A.Metz, Z.-E.Meziani, S.Migliorati, M.Mihovilovic, R.Milner, A.Mkrtchyan, H.Mkrtchyan, A.Movsisyan, H.Moutarde, M.Muhoza, C.Munoz Camacho, J.Murphy, P.Nadel-Turonski, E.Nardi, J.Nazeer, S.Niccolai, G.Niculescu, R.Novotny, J.F.Owens, M.Paolone, L.Pappalardo, R.Paremuzyan, B.Pasquini, E.Pasyuk, T.Patel, I.Pegg, C.Peng, D.Perera, M.Poelker, K.Price, A.J.R.Puckett, M.Raggi, N.Randazzo, M.N.H.Rashad, M.Rathnayake, B.Raue, P.E.Reimer, M.Rinaldi, A.Rizzo, Y.Roblin, J.Roche, O.Rondon-Aramayo, F.Sabatie, G.Salme, E.Santopinto, R.Santos Estrada, B.Sawatzky, A.Schmidt, P.Schweitzer, S.Scopetta, V.Sergeyeva, M.Shabestari, A.Shahinyan, Y.Sharabian, S.Sirca, E.S.Smith, D.Sokhan, A.Somov, N.Sparveris, M.Spata, H.Spiesberger, M.Spreafico, S.Stepanyan, P.Stoler, I.Strakovsky, R.Suleiman, M.Suresh, P.Sznajder, H.Szumila-Vance, V.Tadevosyan, A.S.Tadepalli, A.W.Thomas, M.Tiefenback, R.Trotta, M.Ungaro, P.Valente, M.Vanderhaeghen, L.Venturelli, H.Voskanyan, E.Voutier, B.Wojtsekhowski, M.H.Wood, S.Wood, J.Xie, W.Xiong, Z.Ye, M.Yurov, H.-G.Zaunick, S.Zhamkochyan, J.Zhang, S.Zhang, S.Zhao, Z.W.Zhao, X.Zheng, J.Zhou, C.Zorn An experimental program with high duty-cycle polarized and unpolarized positron beams at Jefferson Lab
doi: 10.1140/epja/s10050-021-00564-y
2021MO08 Nucl.Phys. A1009, 122157 (2021) T.F.Motta, P.A.M.Guichon, A.W.Thomas On the sound speed in hyperonic stars
doi: 10.1016/j.nuclphysa.2021.122157
2021WA22 Phys.Rev. C 103, 034606 (2021) Relativistic mean-field corrections for interactions of dark matter particles with nucleons
doi: 10.1103/PhysRevC.103.034606
2020AN18 Phys.Rev. C 102, 065801 (2020) S.Antic, J.R.Stone, J.C.Miller, K.L.Martinez, P.A.M.Guichon, A.W.Thomas Outer crust of a cold, nonaccreting neutron star within the quark-meson-coupling model NUCLEAR STRUCTURE Z=26-50, N=20-90; calculated nuclear binding energies, two-neutron drip line using the QMCπ-III mass model, and compared with experimental data. 56Fe, 62,64,66,78Ni, 80Zn, 82Ge, 84Se, 86,118,120Kr, 120,122,124Sr, 121Y, 122Zr, 124Mo, 126Ru; calculated numerical results of the equation of state (EOSs) in the outer crust of cold nonaccreting, nonrotating neutron stars, such as baryon number densities at the bottom and top of each layer, and neutron and electron chemical potentials, and properties of individual layers in the outer crust. Comparison with results from FRDM, HFB24, and NL3 mass models.
doi: 10.1103/PhysRevC.102.065801
2020BA15 Acta Phys.Pol. B51, 611 (2020) P.Baczyk, M.Konieczka, K.M.L.Martinez, S.Antic, P.A.M.Guichon, W.Satula, J.R.Stone, A.W.Thomas On Introducing Charge-Symmetry-Breaking Terms to Nuclear Energy Density Functionals
doi: 10.5506/APhysPolB.51.611
2020MA43 Phys.Rev. C 102, 034304 (2020) K.L.Martinez, A.W.Thomas, P.A.M.Guichon, J.R.Stone Tensor and pairing interactions within the quark-meson coupling energy-density functional NUCLEAR STRUCTURE Z=20, N=14-38; Z=28, N=20-50; Z=50, N=50-88; Z=82, N=96-138; calculated binding energies with and without tensor contribution, two-neutron shell gaps. 40,48Ca, 56,78Ni, 100,132Sn; calculated proton and neutron single-particle states, deformation energies, spin-orbit splittings with and without tensor contribution. 90,92,94,96,98,100,102,104,106,108,110,112Zr; calculated β2 deformation parameters and deformation energies. 254,256,254,256,258,260,262,264Fm, 254,256,258,260,262,264,266,268Rf; calculated two-neutron shell gaps. Quark-meson coupling (QMC) model (QMCπ-III-T), with the density functional which included tensor component, and pairing interaction from the QMC framework. Comparison with experimental data.
doi: 10.1103/PhysRevC.102.034304
2019MA57 Phys.Rev. C 100, 024333 (2019) K.L.Martinez, A.W.Thomas, J.R.Stone, P.A.M.Guichon Parameter optimization for the latest quark-meson coupling energy-density functional NUCLEAR STRUCTURE Z=20, 28, 50, 82; N=20, 28, 50, 82, 126; calculated binding energies, rms charge radii, and pairing gaps for 70 nuclei. Z=8-96, N=8-160; calculated binding energies, rms charge radii, and S(2n) for 739 even-even nuclei. Z=20, N=16-36; Z=28, N=26-52; Z=50, N=52-86; Z=82, N=98-142; calculated S(2n) for even-even nuclei. Z=20, A=34-58; Z=82, A=178-220; calculated isotopic shifts for even-even nuclei. 36,38,40,48Ca, 54Fe, 58,60,64Ni, 90Zr, 112,116,124Sn, 208Pb; calculated skin thicknesses. 40Ca, 78Ni, 132Sn; calculated proton and neutron single-particle states. Z=64, A=134-170; calculated B(E2) and β2 for the first 2+ states in even-even nuclei. 90Zr, 116Sn, 144Sm, 208Pb; calculated energies of giant monopole resonances (GMR). Z>96, A=232-294; calculated binding energies for superheavy nuclei. HF+BCS calculations with quark-meson-coupling (QMC) model, using QMCπ-II energy density functional. Optimization of model parameters by detailed comparisons and fittings with the experimental data. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.100.024333
2019PE15 Phys.Rev. C 100, 025206 (2019) R.J.Perry, A.Kizilersu, A.W.Thomas Model dependence of the pion form factor extracted from pion electroproduction
doi: 10.1103/PhysRevC.100.025206
2019ST10 Phys.Rev. C 100, 044302 (2019) J.R.Stone, K.Morita, P.A.M.Guichon, A.W.Thomas Physics of even-even superheavy nuclei with 96 < Z < 110 in the quark-meson-coupling model NUCLEAR STRUCTURE 244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm; calculated ground state binding energies and compared to values in AME-2016. 234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280Cm, 236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282Cf, 238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284Fm, 240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286No, 242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288Rf, 244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290Sg, 246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292Hs, 248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294Ds; calculated deformation energies and neutron pairing energies as a function of the quadrupole deformation parameter β2, S(2n), Q(α), shape coexistence in N=168-184 Sg nuclei. 40,48Ca, 56,68,78Ni, 90Zr, 100,132Sn, 146Gd, 208Pb; calculated proton and neutron single-particle energies. 244Cm, 248Cf, 252Fm, 256No, 260Rf, 264Sg, 268Hs, 272Ds; calculated neutron single-particle states. Quark-meson-coupling (QMC) model. Comparison with available experimental data from AME-2016 and databases at NNDC.
doi: 10.1103/PhysRevC.100.044302
2018HU06 Phys.Rev. C 97, 055210 (2018) P.T.P.Hutauruk, W.Bentz, I.C.Cloet, A.W.Thomas Charge symmetry breaking effects in pion and kaon structure
doi: 10.1103/PhysRevC.97.055210
2017CO11 Phys.Rev. C 96, 035201 (2017) J.J.Cobos-Martinez, K.Tsushima, G.Krein, A.W.Thomas Φ-meson-nucleus bound states
doi: 10.1103/PhysRevC.96.035201
2016CL02 Phys.Rev.Lett. 116, 032701 (2016) I.C.Cloet, W.Bentz, A.W.Thomas Relativistic and Nuclear Medium Effects on the Coulomb Sum Rule
doi: 10.1103/PhysRevLett.116.032701
2016HU15 Phys.Rev. C 94, 035201 (2016) P.T.P.Hutauruk, I.C.Cloet, A.W.Thomas Flavor dependence of the pion and kaon form factors and parton distribution functions
doi: 10.1103/PhysRevC.94.035201
2016LI22 Phys.Rev. C 93, 045203 (2016) H.Li, P.Wang, D.B.Leinweber, A.W.Thomas Spin of the proton in chiral effective field theory NUCLEAR STRUCTURE 1H; calculated proton spin structure, total quark spin contribution, singlet axial charge. Predictions of the meson-cloud model.
doi: 10.1103/PhysRevC.93.045203
2016ST07 Phys.Rev.Lett. 116, 092501 (2016) J.R.Stone, P.A.M.Guichon, P.G.Reinhard, A.W.Thomas Finite Nuclei in the Quark-Meson Coupling Model NUCLEAR STRUCTURE 270Db, 264,255Hs, 260,262Sg, 256,258Rf, 254,256No, 246,248,250,252,254,256Fm; calculated ground-state binding energies, deformation parameters. Effective quark-meson coupling (QMC) energy density functional (EDF), comparison with available data.
doi: 10.1103/PhysRevLett.116.092501
2016VE05 J.Phys.(London) G43, 115002 (2016) J.D.Vergados, F.T.Avignone, III, M.Kortelainen, P.Pirinen, P.C.Srivastava, J.Suhonen, A.W.Thomas Inelastic WIMP-nucleus scattering to the first excited state in 125Te NUCLEAR STRUCTURE 125Te; calculated energy levels, J, π, B(E2), B(M1). Comparison with available data.
doi: 10.1088/0954-3899/43/11/115002
2016WH01 Phys.Rev. C 93, 035807 (2016) D.L.Whittenbury, H.H.Matevosyan, A.W.Thomas Hybrid stars using the quark-meson coupling and proper-time Nambu-Jona-Lasinio models
doi: 10.1103/PhysRevC.93.035807
2015CA13 Phys.Rev. C 92, 015212 (2015) M.E.Carrillo-Serrano, W.Bentz, I.C.Cloet, A.W.Thomas ρ meson form factors in a confining Nambu-Jona-Lasinio model
doi: 10.1103/PhysRevC.92.015212
2015TH02 Phys.Rev. C 91, 015209 (2015) A.W.Thomas, X.G.Wang, R.D.Young Electromagnetic contribution to the proton-neutron mass splitting NUCLEAR STRUCTURE 1H, 1n; calculated electromagnetic contribution to proton-neutron mass splitting by combining RBC lattice simulations and modified Cottingham sum rule of Walker-Loud, Carlson and Miller, estimate of isovector nucleon magnetic polarizability as a function of pion mass. Relevance to accurate estimate of contribution to proton-neutron mass difference from difference of the masses of the up and down quarks. Comparison with experimental value.
doi: 10.1103/PhysRevC.91.015209
2014CA44 Phys.Rev. C 90, 064316 (2014) M.E.Carrillo-Serrano, I.C.Cloet, A.W.Thomas SU(3)-flavor breaking in octet baryon masses and axial couplings
doi: 10.1103/PhysRevC.90.064316
2014CL03 Phys.Rev. C 90, 045202 (2014) I.C.Cloet, W.Bentz, A.W.Thomas Role of diquark correlations and the pion cloud in nucleon elastic form factors
doi: 10.1103/PhysRevC.90.045202
2014ER05 Phys.Rev. C 90, 065205 (2014) F.B.Erben, P.E.Shanahan, A.W.Thomas, R.D.Young Dispersive estimate of the electromagnetic charge symmetry violation in the octet baryon masses
doi: 10.1103/PhysRevC.90.065205
2014WH01 Phys.Rev. C 89, 065801 (2014) D.L.Whittenbury, J.D.Carroll, A.W.Thomas, K.Tsushima, J.R.Stone Quark-meson coupling model, nuclear matter constraints, and neutron star properties
doi: 10.1103/PhysRevC.89.065801
2014WU09 Phys.Rev. C 90, 055206 (2014) J.-J.Wu, T.-S.H.Lee, A.W.Thomas, R.D.Young Finite-volume Hamiltonian method for coupled-channels interactions in lattice QCD
doi: 10.1103/PhysRevC.90.055206
2014YO04 Int.J.Mod.Phys. E23, 1461010 (2014) R.D.Young, P.E.Shanahan, A.W.Thomas Progress in resolving charge symmetry violation in nucleon structure
doi: 10.1142/S0218301314610102
2013CA02 Phys.Rev. C 87, 015801 (2013) M.E.Carrillo-Serrano, I.C.Cloet, K.Tsushima, A.W.Thomas, I.R.Afnan Variations of nuclear binding with quark masses NUCLEAR STRUCTURE 7Li, 12C, 16O; calculated single-particle energies versus quark masses. 2,3H, 7Li, 12C, 16O; calculated variation of binding energy, and the 1S0 antibound pole position versus quark mass. Quark-meson coupling (QMD) and one boson-exchange (OBE) models. 7Li; calculated abundance using Big Bang nucleosynthesis computer code of Kawano.
doi: 10.1103/PhysRevC.87.015801
2013CH31 Nucl.Phys. A913, 116 (2013) R.Chatterjee, R.Shyam, K.Tsushima, A.W.Thomas Structure and Coulomb dissociation of 23O within the quark-meson coupling model NUCLEAR REACTIONS Pb(23O, n22O), E=422 MeV/nucleon; calculated Coulomb dissociation σ(E), longitudinal momentum distribution using QMC (quark-meson coupling) model. Compared with available data. NUCLEAR STRUCTURE 23N, 23O, 31Ne, 35Mg, 37Na, 45S, 49Ar; calculated valence neutron separation energy, 23O density distribution, neutron, proton radii using QMC (quark-meson coupling) model. Compared with available data.
doi: 10.1016/j.nuclphysa.2013.06.004
2013RA01 J.Phys.(London) G40, 015102 (2013) G.Ramalho, K.Tsushima, A.W.Thomas Octet baryon electromagnetic form factors in nuclear medium
doi: 10.1088/0954-3899/40/1/015102
2013SH32 Phys.Rev. C 88, 025209 (2013) R.Shyam, O.Scholten, A.W.Thomas Production of the H dibaryon via the (K-, K+) reaction on a 12C target
doi: 10.1103/PhysRevC.88.025209
2012BL11 Phys.Rev.Lett. 109, 262301 (2012) P.G.Blunden, W.Melnitchouk, A.W.Thomas γZ Box Corrections to Weak Charges of Heavy Nuclei in Atomic Parity Violation
doi: 10.1103/PhysRevLett.109.262301
2012CL02 Phys.Rev.Lett. 109, 182301 (2012) I.C.Cloet, W.Bentz, A.W.Thomas Parity-Violating Deep Inelastic Scattering and the Flavor Dependence of the EMC Effect
doi: 10.1103/PhysRevLett.109.182301
2012MI25 Phys.Rev. C 86, 065201 (2012) G.A.Miller, A.W.Thomas, J.D.Carroll Nuclear quasielastic electron scattering limits nucleon off-mass shell properties
doi: 10.1103/PhysRevC.86.065201
2012SH11 Nucl.Phys. A881, 255 (2012) R.Shyam, K.Tsushima, A.W.Thomas Production of cascade hypernuclei via the (K-, K+) reaction within a quark-meson coupling model NUCLEAR REACTIONS 1H(K-, K+)Ξ-, E at 1-4 GeV/c;12C, 28Si(K-, K+), E at 0.5-2 GeV/c; calculated Ξ-, bound hypernuclei 12ΞBe, 28ΞMg hypernuclei production σ, σ(θ) using covariant effective Lagrangian model including Λ and Σ resonance intermediate states. Compared with data.
doi: 10.1016/j.nuclphysa.2012.01.025
2011BA10 Phys.Rev. C 83, 038202 (2011) Gluon polarization in the proton
doi: 10.1103/PhysRevC.83.038202
2011SH29 Phys.Rev. C 84, 042201 (2011) R.Shyam, O.Scholten, A.W.Thomas Production of a cascade hyperon in the K--proton interaction
doi: 10.1103/PhysRevC.84.042201
2011TS06 Phys.Rev. C 83, 065208 (2011) K.Tsushima, D.H.Lu, G.Krein, A.W.Thomas J/ψ-nuclear bound states
doi: 10.1103/PhysRevC.83.065208
2010AR06 Nucl.Phys. A840, 97 (2010) W.Armour, C.R.Allton, D.B.Leinweber, A.W.Thomas, R.D.Young An analysis of the nucleon spectrum from lattice partially-quenched QCD
doi: 10.1016/j.nuclphysa.2010.03.012
2010TH05 Nucl.Phys. A844, 19c (2010) Symmetries and the search for physics beyond the standard model
doi: 10.1016/j.nuclphysa.2010.05.008
2010TS03 Int.J.Mod.Phys. E19, 2546 (2010) K.Tsushima, P.A.M.Guichon, R.Shyam, A.W.Thomas Binding of hypernuclei, and photoproduction of Λ-hypernuclei in the latest quark-meson coupling model NUCLEAR STRUCTURE 16,17O, 40,41,49Ca, 89Y, 91Zr, 208,209Pb; calculated hypernuclei single-particle energies. Quark-meson coupling model, comparison with experimental data.
doi: 10.1142/S021830131001706X
2010YO09 Nucl.Phys. A844, 266c (2010) Recent results on nucleon sigma terms in lattice QCD
doi: 10.1016/j.nuclphysa.2010.05.048
2009CA12 Phys.Rev. C 79, 045810 (2009) J.D.Carroll, D.B.Leinweber, A.G.Williams, A.W.Thomas Phase transition from quark-meson coupling hyperonic matter to deconfined quark matter
doi: 10.1103/PhysRevC.79.045810
2009CL04 Phys.Rev.Lett. 102, 252301 (2009) I.C.Cloet, W.Bentz, A.W.Thomas Isovector EMC Effect and the NuTeV Anomaly
doi: 10.1103/PhysRevLett.102.252301
2009GU13 Phys.Rev. C 79, 055205 (2009) V.Guzey, A.W.Thomas, K.Tsushima Medium modifications of the bound nucleon generalized parton distributions and the quark contribution to the spin sum rule
doi: 10.1103/PhysRevC.79.055205
2009SI29 Eur.Phys.J. A 41, 71 (2009) A.Sibirtsev, J.Haidenbauer, S.Krewald, U.-G.Meissner, A.W.Thomas Neutral pion photoproduction at high energies
doi: 10.1140/epja/i2009-10771-0
2009WA12 Phys.Rev. C 79, 065202 (2009) P.Wang, D.B.Leinweber, A.W.Thomas, R.D.Young Strange magnetic form factor of the proton at Q2 = 0.23 GeV2
doi: 10.1103/PhysRevC.79.065202
2008GU18 Nucl.Phys. A814, 66 (2008) P.A.M.Guichon, A.W.Thomas, K.Tsushima Binding of hypernuclei in the latest quark-meson coupling model NUCLEAR STRUCTURE 17O, 41,49Ca, 91Zr, 209Pb; calculated hypernuclei binding energies using quark-meson coupling model. Comparison with data.
doi: 10.1016/j.nuclphysa.2008.10.001
2008TH04 Nucl.Phys. A805, 271c (2008) WG.9: The IUPAP Working Group on International Cooperation in Nuclear Physics
doi: 10.1016/j.nuclphysa.2008.02.256
2007MA32 Phys.Rev. C 75, 045201 (2007) H.H.Matevosyan, A.W.Thomas, P.C.Tandy Quark-gluon vertex dressing and meson masses beyond ladder-rainbow truncation
doi: 10.1103/PhysRevC.75.045201
2007RI13 Nucl.Phys. A792, 341 (2007) J.Rikovska Stone, P.A.M.Guichon, H.H.Matevosyan, A.W.Thomas Cold uniform matter and neutron stars in the quark-meson-coupling model
doi: 10.1016/j.nuclphysa.2007.05.011
2007SA01 Prog.Part.Nucl.Phys. 58, 1 (2007) K.Saito, K.Tsushima, A.W.Thomas Nucleon and hadron structure changes in the nuclear medium and the impact on observables
doi: 10.10106/j.ppnp.2005.07.003
2007SI03 Eur.Phys.J. A 31, 221 (2007) A.Sibirtsev, J.Haidenbauer, S.Krewald, U.-G.Meissner, A.W.Thomas K(K-bar) photoproduction from protons NUCLEAR REACTIONS 1H(γ, K+K-), E=1.8-3.8 GeV; analyzed data; deduced contribution from Drell mechanism, possible hyperon resonance, other reaction mechanism features.
doi: 10.1140/epja/i2006-10216-4
2007SI31 Eur.Phys.J. A 34, 49 (2007) A.Sibirtsev, J.Haidenbauer, S.Krewald, T.-S.H.Lee, U.-G.Meissner, A.W.Thomas Regge approach to charged pion photoproduction at invariant energies above 2 GeV
doi: 10..1140/epja/i2007-10482-6
2007TH03 Nucl.Phys. A782, 1c (2007) Recent Developments Concerning the Role of Strangeness in the Nucleon
doi: 10.1016/j.nuclphysa.2006.10.042
2007TH11 Nucl.Phys. A787, 396c (2007) Origin of the Nuclear Equation of State at the Quark Level NUCLEAR STRUCTURE 16O, 40,48Ca, 208Pb; calculated spin-orbit splitting, proton and neutron densities. Quark-meson coupling model, comparison with Skyrme models and data.
doi: 10.1016/j.nuclphysa.2006.12.061
2007TH12 Nucl.Phys. A790, 173c (2007) Progress in the calculation and experimental determination of the strangeness contributions to nucleon form factors NUCLEAR STRUCTURE 1n, 1H; calculated μ, strangeness electromagnetic form factors. Full lattice QCD calculations. Comparison with data.
doi: 10.1016/j.nuclphysa.2007.03.154
2007TS05 Eur.Phys.J. A 31, 626 (2007) K.Tsushima, K.Saito, A.W.Thomas, A.Valcarce Nucleon sigma term and quark condensate in nuclear matter
doi: 10.1140/epja/i2006-10179-4
2007WA13 Phys.Rev. C 75, 045202 (2007) P.Wang, A.W.Thomas, A.G.Williams Phase transition from hadronic matter to quark matter
doi: 10.1103/PhysRevC.75.045202
2007WA14 Phys.Rev. D 75, 073012 (2007) P.Wang, D.B.Leinweber, A.W.Thomas, R.D.Young Chiral extrapolation of nucleon magnetic form factors NUCLEAR STRUCTURE 1n, 1H; calculated nucleon magnetic form factors using chiral extrapolation of lattice QCD results.
doi: 10.1103/PhysRevD.75.073012
2006BA18 Phys.Lett. B 634, 368 (2006) η bound states in nuclei: a probe of flavour-singlet dynamics
doi: 10.1016/j.physletb.2006.01.071
2006CL07 Phys.Lett. B 642, 210 (2006) I.C.Cloet, W.Bentz, A.W.Thomas EMC and polarized EMC effects in nuclei NUCLEAR STRUCTURE 7Li, 11B, 15N, 27Al; calculated quark distributions, structure functions. Covariant quark-diquark model, polarized EMC effect introduced.
doi: 10.1016/j.physletb.2006.08.076
2006GU11 Nucl.Phys. A772, 1 (2006) P.A.M.Guichon, H.H.Matevosyan, N.Sandulescu, A.W.Thomas Physical origin of density dependent forces of Skyrme type within the quark meson coupling model NUCLEAR STRUCTURE 16O, 40,48Ca, 208Pb; calculated binding energies, radii, proton and neutron densities. Ni, Zr; calculated two-neutron drip line. 42Si, 60Ge; calculated two-neutron separation energy, shell quenching features. Quark-meson coupling model, comparison with Skyrme models, astrophysical implications discussed.
doi: 10.1016/j.nuclphysa.2006.04.002
2006LA02 Phys.Lett. B 632, 495 (2006) The phases of isospin-asymmetric matter in the two-flavor NJL model
doi: 10.1016/j.physletb.2005.11.025
2006LA05 J.Phys.(London) G32, 667 (2006) Nucleons, nuclear matter and quark matter: a unified NJL approach
doi: 10.1088/0954-3899/32/5/006
2006LE26 Phys.Rev.Lett. 97, 022001 (2006) D.B.Leinweber, S.Boinepalli, A.W.Thomas, P.Wang, A.G.Williams, R.D.Young, J.M.Zanotti, J.B.Zhang Strange Electric Form Factor of the Proton NUCLEAR STRUCTURE 1H; calculated strange electric charge radius, form factor.
doi: 10.1103/PhysRevLett.97.022001
2006SI28 Eur.Phys.J. A 29, 209 (2006) A.Sibirtsev, H.-W.Hammer, U.-G.Meissner, A.W.Thomas φ-meson photoproduction from nuclei
doi: 10.1140/epja/i2006-10070-4
2006YO06 Phys.Rev.Lett. 97, 102002 (2006) R.D.Young, J.Roche, R.D.Carlini, A.W.Thomas Extracting Nucleon Strange and Anapole Form Factors from World Data NUCLEAR STRUCTURE 1n, 1H; analyzed electron scattering data; deduced strange and anapole form factors.
doi: 10.1103/PhysRevLett.97.102002
2005CL05 Phys.Lett. B 621, 246 (2005) I.C.Cloet, W.Bentz, A.W.Thomas Nucleon quark distributions in a covariant quark-diquark model NUCLEAR STRUCTURE 1n, 1H; calculated quark light-cone momentum distributions, structure functions. Covariant quark-diquark model.
doi: 10.1016/j.physletb.2005.06.065
2005CL06 Phys.Rev.Lett. 95, 052302 (2005) I.C.Cloet, W.Bentz, A.W.Thomas Spin-Dependent Structure Functions in Nuclear Matter and the Polarized EMC Effect
doi: 10.1103/PhysRevLett.95.052302
2005LE08 Eur.Phys.J. A 24, Supplement 2, 79 (2005) D.B.Leinweber, S.Boinepalli, A.W.Thomas, A.G.Williams, R.D.Young, J.B.Zhang, J.M.Zanotti Systematic uncertainties in the precise determination of the strangeness magnetic moment of the nucleon NUCLEAR STRUCTURE 1n, 1H; analyzed μ, strangeness magnetic moment.
doi: 10.1140/epjad/s2005-04-017-y
2005LE22 Phys.Rev.Lett. 94, 212001 (2005) D.B.Leinweber, S.Boinepalli, I.C.Cloet, A.W.Thomas, A.G.Williams, R.D.Young, J.M.Zanotti, J.B.Zhang Precise Determination of the Strangeness Magnetic Moment of the Nucleon NUCLEAR MOMENTS 1H; calculated strange magnetic moment. Comparison with data.
doi: 10.1103/PhysRevLett.94.212001
2005LE24 Nucl.Phys. A755, 59c (2005) D.B.Leinweber, A.W.Thomas, R.D.Young Extrapolation of lattice QCD results beyond the power-counting regime
doi: 10.1016/j.nuclphysa.2005.03.024
2005LO10 J.Phys.(London) G31, 1151 (2005) Implications of current constraints on parton charge symmetry
doi: 10.1088/0954-3899/31/11/003
2005MA33 Phys.Rev. C 71, 055204 (2005) H.H.Matevosyan, G.A.Miller, A.W.Thomas Comparison of nucleon form factors from lattice QCD against the light front cloudy bag model and extrapolation to the physical mass regime
doi: 10.1103/PhysRevC.71.055204
2005MA78 Nucl.Phys. A760, 319 (2005) T.Maruyama, T.Muto, T.Tatsumi, K.Tsushima, A.W.Thomas Kaon condensation and lambda-nucleon loop in the relativistic mean-field approach
doi: 10.1016/j.nuclphysa.2005.06.008
2005MB08 Phys.Rev. C 72, 065204 (2005) H.H.Matevosyan, A.W.Thomas, G.A.Miller Study of lattice QCD form factors using the extended Gari-Krumpelmann model NUCLEAR STRUCTURE 1H; calculated electromagnetic form factors, quark mass dependence. Vector meson dominance model.
doi: 10.1103/PhysRevC.72.065204
2005SA68 Eur.Phys.J. A 26, 159 (2005) K.Saito, H.Kouno, K.Tsushima, A.W.Thomas Two-scale scalar mesons in nuclei NUCLEAR STRUCTURE 40Ca; calculated single-particle energies, charge and neutron density distributions. Chiral invariant model based on linear σ model.
doi: 10.1140/epja/i2005-10170-7
2005WA03 Nucl.Phys. A748, 226 (2005) P.Wang, D.B.Leinweber, A.W.Thomas, A.G.Williams Liquid-gas phase transition and Coulomb instability of asymmetric nuclear systems
doi: 10.1016/j.nuclphysa.2004.10.012
2005WA32 Phys.Rev. C 72, 045801 (2005) P.Wang, S.Lawley, D.B.Leinweber, A.W.Thomas, A.G.Williams Neutron stars and strange stars in the chiral SU(3) quark mean field model
doi: 10.1103/PhysRevC.72.045801
2005YO02 Phys.Rev. D 71, 014001 (2005) R.D.Young, D.B.Leinweber, A.W.Thomas Leading quenching effects in the proton magnetic moment NUCLEAR MOMENTS 1n, 1H; calculated magnetic moments, quenching effects. Quenched chiral effective field theory.
doi: 10.1103/PhysRevD.71.014001
2004AS03 Eur.Phys.J. A 19, Supplement 1, 9 (2004) J.D.Ashley, D.B.Leinweber, A.W.Thomas, R.D.Young Nucleon electromagnetic form factors from lattice QCD NUCLEAR STRUCTURE 1n, 1H; calculated electromagnetic form factors. Lattice QCD, comparison with data.
doi: 10.1140/epjad/s2004-03-002-4
2004GU16 Phys.Rev.Lett. 93, 132502 (2004) Quark Structure and Nuclear Effective Forces
doi: 10.1103/PhysRevLett.93.132502
2004LE18 Nucl.Phys. A737, 177 (2004) D.B.Leinweber, A.W.Thomas, A.G.Williams, R.D.Young, J.M.Zanotti, J.B.Zhang Observing Chiral Nonanalytic Behavior with FLIC Fermions
doi: 10.1016/j.nuclphysa.2004.03.060
2004LE20 Phys.Rev.Lett. 92, 242002 (2004) D.B.Leinweber, A.W.Thomas, R.D.Young Physical Nucleon Properties from Lattice QCD NUCLEAR STRUCTURE A=1; calculated nucleon mass. Lattice QCD.
doi: 10.1103/PhysRevLett.92.242002
2004MI19 Nucl.Phys. A735, 482 (2004) H.Mineo, W.Bentz, N.Ishii, A.W.Thomas, K.Yazaki Quark distributions in nuclear matter and the EMC effect
doi: 10.1016/j.nuclphysa.2004.02.011
2004ST17 Phys.Lett. B 595, 237 (2004) F.M.Steffens, A.W.Thomas, K.Tsushima Quark distributions in a medium
doi: 10.1016/j.physletb.2004.06.042
2004TH10 Ann.Phys.(Leipzig) 13, 731 (2004) New insight into nuclear structure from QCD
doi: 10.1002/andp.200410115
2004TH14 Prog.Theor.Phys.(Kyoto), Suppl. 156, 124 (2004) A.W.Thomas, P.A.M.Guichon, D.B.Leinweber, R.D.Young Towards a Connection between Nuclear Structure and QCD
doi: 10.1143/PTPS.156.124
2004WA30 Nucl.Phys. A744, 273 (2004) P.Wang, D.B.Leinweber, A.W.Thomas, A.G.Williams New treatment of the chiral SU(3) quark mean field model NUCLEAR STRUCTURE 16O, 208Pb; calculated charge density distributions, single-particle energy levels. 4,5,6He, 7,8,9Li, 7,8,9,10Be, 10,11,12B, 15N, 40Ca, 51V, 89Y; calculated hypernucleus binding energies. Chiral SU(3) quark mean field model.
doi: 10.1016/j.nuclphysa.2004.08.015
2004WA32 Phys.Rev. C 70, 055204 (2004) P.Wang, D.B.Leinweber, A.W.Thomas, A.G.Williams Liquid-gas phase transition in nuclear matter including strangeness
doi: 10.1103/PhysRevC.70.055204
2003AF04 Phys.Rev. C 68, 035201 (2003) I.R.Afnan, F.Bissey, J.Gomez, A.T.Katramatou, S.Liuti, W.Melnitchouk, G.G.Petratos, A.W.Thomas Deep inelastic scattering from A = 3 nuclei and the neutron structure function NUCLEAR REACTIONS 3H, 3He(e, e'X), E=high; analyzed structure functions, EMC effect; deduced ratio of neutron to proton structure functions.
doi: 10.1103/PhysRevC.68.035201
2003BE33 Nucl.Phys. A720, 95 (2003) W.Bentz, T.Horikawa, N.Ishii, A.W.Thomas Phase transition from nuclear matter to color superconducting quark matter
doi: 10.1016/S0375-9474(03)00635-3
2003BE65 Prog.Theor.Phys.(Kyoto), Suppl. 151, 176 (2003) W.Bentz, T.Horikawa, N.Ishii, A.W.Thomas Description of Nucleons, Nuclear Matter and Quark Matter in an Effective Quark Theory
doi: 10.1143/PTPS.151.176
2003DE36 Eur.Phys.J. A 18, 269 (2003) W.Detmold, W.Melnitchouk, A.W.Thomas Moments of isovector quark distributions in lattice QCD
doi: 10.1140/epja/i2002-10214-6
2003LE29 Eur.Phys.J. A 18, 247 (2003) D.B.Leinweber, J.N.Hedditch, W.Melnitchouk, A.W.Thomas, A.G.Williams, R.D.Young, J.M.Zanotti, J.B.Zhang FLIC fermions and hadron phenomenology
doi: 10.1140/epja/i2002-10209-3
2003ME04 Phys.Rev. C 67, 038201 (2003) Nuclear shadowing at low Q2 NUCLEAR STRUCTURE C, Sn; calculated relative structure function vs Q2, role of vector meson dominance in nuclear shadowing. Comparison with data.
doi: 10.1103/PhysRevC.67.038201
2003MI36 Mod.Phys.Lett. A 18, 384 (2003) H.Mineo, W.Bentz, A.W.Thomas, N.Ishii, K.Yazaki Structure function in nuclear matter in the NJL model
doi: 10.1142/S0217732303010533
2003TH09 Nucl.Phys. A721, 915c (2003) A.W.Thomas, J.D.Ashley, W.Detmold, D.B.Leinweber, W.Melnitchouk, R.D.Young Progress in the Calculation of Nucleon Form Factors and Parton Distribution Functions
doi: 10.1016/S0375-9474(03)01242-9
2003TH13 Eur.Phys.J. A 18, 241 (2003) A.W.Thomas, D.B.Leinweber, R.D.Young Recent developments in quark nuclear physics
doi: 10.1140/epja/i2002-10208-4
2003YA09 Phys.Rev. C 68, 048201 (2003) U.T.Yakhshiev, A.W.Thomas, F.C.Khanna Meson-nucleon vertex form factors a finite temperature using a soft pion form factor
doi: 10.1103/PhysRevC.68.048201
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