NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = P.Blunden Found 40 matches. 2024MC01 Phys.Rev. C 109, 015503 (2024) Novel approach to the global analysis of proton form factors in elastic electron-proton scattering
doi: 10.1103/PhysRevC.109.015503
2023AH02 Phys.Rev. C 108, 055202 (2023) J.Ahmed, P.G.Blunden, W.Melnitchouk Normal single-spin asymmetries in electron-proton scattering: Two-photon exchange with intermediate-state resonances
doi: 10.1103/PhysRevC.108.055202
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
2020AH05 Phys.Rev. C 102, 045205 (2020) J.Ahmed, P.G.Blunden, W.Melnitchouk Two-photon exchange from intermediate state resonances in elastic electron-proton scattering NUCLEAR REACTIONS 1H(e, e), at Q2<5 GeV2; calculated two-photon exchange (TPE) correction due to finite width of three significant resonance intermediate states Δ(1232), N(1520) and N(1720), TPE form factors, ratio R2γ of e++p to e-+p elastic scattering cross sections, ratio of the proton electric to magnetic form factors. Dispersive approach for the two-photon exchange (TPE) correction to elastic electron-proton scattering. Comparison with experimental data from CLAS, VEPP-3 and OLYMPUS collaborations, and from other laboratories.
doi: 10.1103/PhysRevC.102.045205
2017BL08 Phys.Rev. C 95, 065209 (2017) Dispersive approach to two-photon exchange in elastic electron-proton scattering NUCLEAR REACTIONS 1H(e, e), (e+, e+), Q2=0-3 GeV2; calculated two-photon exchange (TPE) corrections, algebraically and numerically, within a dispersive approach, including contributions from nucleon and Δ intermediate states. Comparison with measurements from the CLAS, VEPP-3, and OLYMPUS experiments, and with polarization transfer observables.
doi: 10.1103/PhysRevC.95.065209
2013SI34 Phys.Rev. C 88, 065202 (2013) Q2 evolution of the electric and magnetic polarizabilities of the proton
doi: 10.1103/PhysRevC.88.065202
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
2010BL01 Phys.Rev. C 81, 018202 (2010) P.G.Blunden, W.Melnitchouk, J.A.Tjon Two-photon exchange corrections to the pion form factor
doi: 10.1103/PhysRevC.81.018202
2009TJ01 Phys.Rev. C 79, 055201 (2009) J.A.Tjon, P.G.Blunden, W.Melnitchouk Detailed analysis of two-boson exchange in parity-violating e-p scattering
doi: 10.1103/PhysRevC.79.055201
2008BL13 J.Phys.(London) G35, 115001 (2008) A connection between the high energy-scale evolution of the P- and T-odd πNN coupling constant and the strong πNN interaction
doi: 10.1088/0954-3899/35/11/115001
2007KO22 Nucl.Phys. A785, 351 (2007) P- and T-violating π N N form factor
doi: 10.1016/j.nuclphysa.2006.12.054
2007KO25 Phys.Rev. C 75, 038201 (2007) Contribution of spin 1/2 and 3/2 resonances to two-photon exchange effects in elastic electron-proton scattering NUCLEAR REACTIONS 1H(e, e), E=high; calculated two-photon exchange effects.
doi: 10.1103/PhysRevC.75.038201
2006KO33 Nucl.Phys. A778, 44 (2006) Calculation of two-photon exchange effects for Δ production in electron-proton collisions NUCLEAR REACTIONS 1H(e, X), E not given; calculated two-photon exchange correction for Δ-resonance production.
doi: 10.1016/j.nuclphysa.2006.07.038
2005BL02 Eur.Phys.J. A 24, Supplement 1, 59 (2005) P.G.Blunden, W.Melnitchouk, J.A.Tjon Two-photon exchange in elastic electron-proton scattering NUCLEAR REACTIONS 1H(e, e), (polarized e, e), E not given; calculated two-photon exchange contributions to elastic σ.
doi: 10.1140/epjad/s2005-05-010-2
2005BL24 Phys.Rev. C 72, 034612 (2005) P.G.Blunden, W.Melnitchouk, J.A.Tjon Two-photon exchange in elastic electron-nucleon scattering NUCLEAR REACTIONS 1H(e, e), (e+, e+), (polarized e, e), E=high; 1n, 3He(e, e), E=high; analyzed σ(Q2), polarization observables, two-photon exchange contributions, nucleon structure effects.
doi: 10.1103/PhysRevC.72.034612
2005BL29 Phys.Rev. C 72, 057601 (2005) Proton radii and two-photon exchange NUCLEAR REACTIONS 1H(e, e), E=160 MeV; calculated two-photon exchange contribution, effect on proton radius determination.
doi: 10.1103/PhysRevC.72.057601
2005KO35 Phys.Rev.Lett. 95, 172503 (2005) S.Kondratyuk, P.G.Blunden, W.Melnitchouk, J.A.Tjon Δ Resonance Contribution to Two-Photon Exchange in Electron-Proton Scattering NUCLEAR REACTIONS 1H(e, e), E=high; calculated Δ resonance contribution to two-photon exchange.
doi: 10.1103/PhysRevLett.95.172503
2003BL09 Phys.Rev.Lett. 91, 142304 (2003) P.G.Blunden, W.Melnitchouk, J.A.Tjon Two-Photon Exchange and Elastic Electron-Proton Scattering NUCLEAR REACTIONS 1H(e, e), E not given; analyzed σ, form factors; deduced two-photon exchange correction.
doi: 10.1103/PhysRevLett.91.142304
2000BL04 Phys.Rev. C61, 025206 (2000) P.G.Blunden, M.Burkardt, G.A.Miller Light Front Nuclear Physics: Toy models, static sources, and tilted light front coordinates
doi: 10.1103/PhysRevC.61.025206
1999BL09 Phys.Rev. C59, R2998 (1999) P.G.Blunden, M.Burkardt, G.A.Miller Rotational Invariance in Nuclear Light-Front Mean Field Theory NUCLEAR STRUCTURE 40Ca; calculated single-particle levels, nucleon, meson momentum distributions. Light-front mean field theory.
doi: 10.1103/PhysRevC.59.R2998
1999BL20 Phys.Rev. C60, 055211 (1999) P.G.Blunden, M.Burkardt, G.A.Miller Light-Front Nuclear Physics: Mean field theory for finite nuclei NUCLEAR STRUCTURE 16O, 40Ca, 80Zr; calculated nucleon, meson momentum distributions. Light-front approach.
doi: 10.1103/PhysRevC.60.055211
1996BL09 Phys.Rev. C54, 359 (1996) Quark-Meson Coupling Model for Finite Nuclei NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb; calculated binding energy per nucleon, rms charge radii. Quark meson coupling model.
doi: 10.1103/PhysRevC.54.359
1993AD08 Phys.Rev. C48, 1438 (1993) J.P.Adams, P.G.Blunden, B.Castel, Y.Okuhara Role of Nuclear Structure in the Spin-Isopin Nuclear Response Problem NUCLEAR STRUCTURE 40Ca; calculated spin-longitudinal to spin-transverse response functions ratio; deduced structure effects role in discrepancy with data. Hartree-Fock based RPA approach.
doi: 10.1103/PhysRevC.48.1438
1992BL03 Nucl.Phys. A536, 697 (1992) The Isoscalar Electromagnetic Current Operator and the Nucleon-Nucleon Interaction NUCLEAR STRUCTURE 2H; calculated structure function, magnetic form factor. Exchange currents.
doi: 10.1016/0375-9474(92)90119-5
1991BL14 Nucl.Phys. A531, 461 (1991) One-Pion Exchange Currents in the QHD Formalism NUCLEAR STRUCTURE 39K, 17O, 41Ca, 209Bi; calculated μ, elastic magnetic form factor. 15N; calculated transition current density, μ. Relativistic many-body problem, one-pion exchange currents.
doi: 10.1016/0375-9474(91)90736-P
1990BL09 Phys.Lett. 240B, 6 (1990) Elastic Magnetic Electron Scattering and Vacuum Polarization NUCLEAR REACTIONS 15N, 209Bi(e, e), E not given; calculated magnetic form factor. Relativistic model.
doi: 10.1016/0370-2693(90)90399-Q
1989BL02 Phys.Lett. 219B, 151 (1989) The Effect of Meson Exchange Currents in a Relativistic Model of Quasielastic (e, e') NUCLEAR REACTIONS 40Ca(e, e'), E not given; calculated transverse response function. Relativistic model, meson exchange effects, quasielastic process.
doi: 10.1016/0370-2693(89)90366-3
1989BL07 Phys.Rev. C40, 1541 (1989) P.G.Blunden, W.R.Greenberg, E.L.Lomon New Comparisons of the Coupled-Channel Model with Elastic Deuteron Form Factors NUCLEAR STRUCTURE 2H; calculated electric, magnetic structure function. Coupled-channels model.
doi: 10.1103/PhysRevC.40.1541
1988BL10 Phys.Rev. C38, 1861 (1988) Random Phase Approximation for Light Nuclei Based on Fully Relativistic Hartree-Fock Calculations NUCLEAR STRUCTURE 12C, 16O, 40Ca; calculated levels. RPA.
doi: 10.1103/PhysRevC.38.1861
1987BL05 Nucl.Phys. A464, 525 (1987) A Consistent Treatment of Nuclear Currents for Scalar and Vector Fields NUCLEAR STRUCTURE A=15, 17, 39, 41; calculated isoscalar magnetic moments. Scalar, vector field model.
doi: 10.1016/0375-9474(87)90365-4
1987BL20 Phys.Lett. 196B, 295 (1987) Relativistic Hartree-Fock Calculations for Finite Nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated charge, matter densities, binding energy, rms charge radii. Relativistic Hartree-Fock.
doi: 10.1016/0370-2693(87)90734-9
1987BL22 Phys.Lett. 198B, 14 (1987) Contribution of Charge Symmetry Breaking Forces to Energy differences in Mirror Nuclei NUCLEAR REACTIONS 1H(p, p), 1n(n, n), E=low; calculated scattering length differences, charge symmetry breaking potentials. NUCLEAR STRUCTURE A=11-41; calculated odd mirror nuclei energy, differences. Charge symmetry breaking potentials.
doi: 10.1016/0370-2693(87)90148-1
1987SI19 Phys.Rev. C36, 2479 (1987) W.P.Sitarski, P.G.Blunden, E.L.Lomon Deuteron Properties of the Coupled Nucleon and Isobar Channels Model NUCLEAR STRUCTURE 2H; calculated magnetic, elastic monopole, quadrupole form factors. Coupled nucleon, isobar channels models.
doi: 10.1103/PhysRevC.36.2479
1985BL03 Phys.Rev. C31, 674 (1985) Anomalous M3 Moment in 39K as a Test of Nuclear Structure NUCLEAR STRUCTURE 43K; calculated quadrupole, M3 moments. Meson exchange, core polarization, isobar excitation.
doi: 10.1103/PhysRevC.31.674
1985BL15 Nucl.Phys. A440, 647 (1985) Quenching of Magnetic Transitions as an Angular Momentum Effect NUCLEAR STRUCTURE A=4-80; analyzed multipole quenching; deduced isobar-hole, nucleon-hole polarizations role multipole dependence.
doi: 10.1016/0375-9474(85)90399-9
1985BL20 Nucl.Phys. A445, 742 (1985) The Magnetic Form Factors of 15N, 17O and 39K NUCLEAR STRUCTURE 15N, 17O, 39K; calculated μ, magnetic form factors.
doi: 10.1016/0375-9474(85)90570-6
1985BL21 Phys.Lett. 164B, 258 (1985) Transverse-Inelastic Form Factor of the First Excited State in 39K NUCLEAR STRUCTURE 39K; calculated M1, E2 transition densities. Second-order core polarization, meson exchange current corrections. NUCLEAR REACTIONS 39K(e, e'), E not given; calculated transverse form factor. Second-order core polarization, meson exchange currents.
doi: 10.1016/0370-2693(85)90321-1
1984BL03 Phys.Lett. 135B, 367 (1984) The Importance of Meson Exchange Currents, Isobars and Core Polarisation on the Magnetic Form Factor of 17O NUCLEAR REACTIONS 17O(e, e'), E not given; calculated magnetic form factor; deduced meson exchange, isobar, core polarization effects relative magnitude. Perturbation approach.
doi: 10.1016/0370-2693(84)90295-8
1983BL06 Z.Phys. A312, 247 (1983) Quenched Magnetic Transitions from High Spin States in Light Nuclei NUCLEAR STRUCTURE 28Si, 24Mg; calculated isoscalar, isovector M6 transition strength quenching factors; deduced isoscalar, isovector transition density structure difference role. Shell model, Landau-Migdal, boson exchange interactions.
doi: 10.1007/BF01412167
1982CA06 Phys.Rev. C25, 2148 (1982) Role of Isobar-Hole Excitations in the Quenching of the 40K(β-)40Ca Transition RADIOACTIVITY 40K; calculated β-decay rate; deduced nuclear, isobar excitation quenching effects. Shell model, isobar-hole excitations.
doi: 10.1103/PhysRevC.25.2148
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