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NSR database version of May 24, 2024.

Search: Author = P.Blunden

Found 41 matches.

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2024AF01      Eur.Phys.J. A 60, 91 (2024)

A.Afanasev, J.C.Bernauer, P.Blunden, J.Blumlein, E.W.Cline, J.M.Friedrich, F.Hagelstein, T.Husek, M.Kohl, F.Myhrer, G.Paz, S.Schadmand, A.Schmidt, V.Sharkovska, A.Signer, O.Tomalak, E.Tomasi-Gustafsson, Y.Ulrich, M.Vanderhaeghen

Radiative corrections: from medium to high energy experiments

doi: 10.1140/epja/s10050-024-01281-y
Citations: PlumX Metrics


2024MC01      Phys.Rev. C 109, 015503 (2024)

C.McRae, P.G.Blunden

Novel approach to the global analysis of proton form factors in elastic electron-proton scattering

doi: 10.1103/PhysRevC.109.015503
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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 R 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
Citations: PlumX Metrics


2017BL08      Phys.Rev. C 95, 065209 (2017)

P.G.Blunden, W.Melnitchouk

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
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2013SI34      Phys.Rev. C 88, 065202 (2013)

A.Sibirtsev, P.G.Blunden

Q2 evolution of the electric and magnetic polarizabilities of the proton

doi: 10.1103/PhysRevC.88.065202
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2008BL13      J.Phys.(London) G35, 115001 (2008)

P.G.Blunden, S.Kondratyuk

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
Citations: PlumX Metrics


2007KO22      Nucl.Phys. A785, 351 (2007)

S.Kondratyuk, P.G.Blunden

P- and T-violating π N N form factor

doi: 10.1016/j.nuclphysa.2006.12.054
Citations: PlumX Metrics


2007KO25      Phys.Rev. C 75, 038201 (2007)

S.Kondratyuk, P.G.Blunden

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
Citations: PlumX Metrics


2006KO33      Nucl.Phys. A778, 44 (2006)

S.Kondratyuk, P.G.Blunden

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2005BL29      Phys.Rev. C 72, 057601 (2005)

P.G.Blunden, I.Sick

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
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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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1996BL09      Phys.Rev. C54, 359 (1996)

P.G.Blunden, G.A.Miller

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
Citations: PlumX Metrics


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
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1992BL03      Nucl.Phys. A536, 697 (1992)

P.G.Blunden, D.O.Riska

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
Citations: PlumX Metrics


1991BL14      Nucl.Phys. A531, 461 (1991)

P.G.Blunden, E.J.Kim

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
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1990BL09      Phys.Lett. 240B, 6 (1990)

P.G.Blunden, C.J.Horowitz

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
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1989BL02      Phys.Lett. 219B, 151 (1989)

P.G.Blunden, M.N.Butler

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
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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
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1988BL10      Phys.Rev. C38, 1861 (1988)

P.G.Blunden, P.McCorquodale

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
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1987BL05      Nucl.Phys. A464, 525 (1987)

P.G.Blunden

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
Citations: PlumX Metrics


1987BL20      Phys.Lett. 196B, 295 (1987)

P.G.Blunden, M.J.Iqbal

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
Citations: PlumX Metrics


1987BL22      Phys.Lett. 198B, 14 (1987)

P.G.Blunden, M.J.Iqbal

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
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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
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1985BL03      Phys.Rev. C31, 674 (1985)

P.Blunden, B.Castel

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
Citations: PlumX Metrics


1985BL15      Nucl.Phys. A440, 647 (1985)

P.Blunden, B.Castel, H.Toki

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
Citations: PlumX Metrics


1985BL20      Nucl.Phys. A445, 742 (1985)

P.G.Blunden, B.Castel

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
Citations: PlumX Metrics


1985BL21      Phys.Lett. 164B, 258 (1985)

P.G.Blunden

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
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1984BL03      Phys.Lett. 135B, 367 (1984)

P.G.Blunden, B.Castel

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
Citations: PlumX Metrics


1983BL06      Z.Phys. A312, 247 (1983)

P.Blunden, B.Castel, H.Toki

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
Citations: PlumX Metrics


1982CA06      Phys.Rev. C25, 2148 (1982)

B.Castel, H.Toki, P.Blunden

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
Citations: PlumX Metrics


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Note: The following list of authors and aliases matches the search parameter P.Blunden: , P.D.BLUNDEN, P.G.BLUNDEN