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NSR database version of April 11, 2024.

Search: Author = T.Mart

Found 53 matches.

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2023MA55      Eur.Phys.J. A 59, 286 (2023)

M.Mai, J.Hergenrather, M.Doring, T.Mart, U.-G.Meissner, D.Ronchen, R.Workman, Julich–Bonn–Washington Collaboration

Inclusion of KΛ electroproduction data in a coupled channel analysis

doi: 10.1140/epja/s10050-023-01188-0
Citations: PlumX Metrics


2019MA66      Phys.Rev. C 100, 035207 (2019)

T.Mart, J.Kristiano, S.Clymton

Pure spin-3/2 representation with consistent interactions

doi: 10.1103/PhysRevC.100.035207
Citations: PlumX Metrics


2017KR10      Phys.Rev. C 96, 052201 (2017)

J.Kristiano, S.Clymton, T.Mart

Pure spin-3/2 propagator for use in particle and nuclear physics

doi: 10.1103/PhysRevC.96.052201
Citations: PlumX Metrics


2017MA21      Phys.Rev. C 95, 045205 (2017)

T.Mart, S.Sakinah

Multipoles model for K+Λ photoproduction on the nucleon reexamined

NUCLEAR REACTIONS 1H(γ, K+Λ), E=1.5-2.7 GeV; analyzed total σ(E), differential σ(θ, E), polarization of the recoiled Λ, photon and target asymmetries, beam-recoil double polarization; deduced nucleon resonance parameters by fitting the calculated observables to about 7400 experimental data points, including the new CLAS 2016 data.

doi: 10.1103/PhysRevC.95.045205
Citations: PlumX Metrics


2017SU14      Phys.Rev. C 95, 045806 (2017)

Suparti, A.Sulaksono, T.Mart

Influence of the nucleon radius on the properties of slowly rotating neutron stars

doi: 10.1103/PhysRevC.95.045806
Citations: PlumX Metrics


2016MA21      Phys.Rev. C 93, 039802 (2016)

T.Mart, A.Sulaksono

Reply to "Comment on 'Nonidentical protons'"

doi: 10.1103/PhysRevC.93.039802
Citations: PlumX Metrics


2014MA94      Phys.Rev. C 90, 065202 (2014)

T.Mart

Electromagnetic production of KΣ on the nucleon near threshold

doi: 10.1103/PhysRevC.90.065202
Citations: PlumX Metrics


2013MA11      Phys.Rev. C 87, 025807 (2013)

T.Mart, A.Sulaksono

Nonidentical protons

doi: 10.1103/PhysRevC.87.025807
Citations: PlumX Metrics


2013MA31      Phys.Rev. C 87, 042201 (2013)

T.Mart

Coupling strength of the N*(1535)s11 to the K+Λ channel

doi: 10.1103/PhysRevC.87.042201
Citations: PlumX Metrics


2013MA78      Few-Body Systems 54, 1729 (2013)

T.Mart, N.Nurhadiansyah

Are Hyperon Resonances Required in the Elementary K+Λ Photoproduction?

NUCLEAR REACTIONS 1H(γ, K+), E=2 GeV; analyzed available data; deduced form factors, σ(θ), σ, hyperon resonances.

doi: 10.1007/s00601-012-0497-9
Citations: PlumX Metrics


2013MA85      Phys.Rev. C 88, 059802 (2013)

T.Mart, A.Sulaksono

Reply to "Comment on 'Nonidentical protons'"

doi: 10.1103/PhysRevC.88.059802
Citations: PlumX Metrics


2012MA34      Phys.Rev. C 86, 022201 (2012)

T.Mart, M.J.Kholili

Origin of the second peak in the cross section of K+Λ photoproduction

doi: 10.1103/PhysRevC.86.022201
Citations: PlumX Metrics


2011MA26      Phys.Rev. C 83, 048203 (2011)

T.Mart

Photo- and electroproduction of K0Λ near threshold and effects of the K0 electromagnetic form factor

doi: 10.1103/PhysRevC.83.048203
Citations: PlumX Metrics


2011VA07      Ann.Phys.(New York) 326, 1085 (2011)

B.I.S.van der Ventel, T.Mart, H.-F.Lu, H.L.Yadav, G.C.Hillhouse

Electromagnetic production of hypernuclei

NUCLEAR REACTIONS 12C(e, e'K+X)12B, E<1 GeV; calculated hypernuclei production unpolorized σ(θ), σ(E, θ), radial wave functions. Particle-hole model.

doi: 10.1016/j.aop.2011.02.003
Citations: PlumX Metrics


2010AD15      Phys.Rev. C 82, 025501 (2010)

G.B.Adera, B.I.S.Van Der Ventel, D.D.van Niekerk, T.Mart

Strange-particle production via the weak interaction

doi: 10.1103/PhysRevC.82.025501
Citations: PlumX Metrics


2010MA42      Phys.Rev. C 82, 025209 (2010)

T.Mart

Electromagnetic production of kaons near threshold

doi: 10.1103/PhysRevC.82.025209
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2009MA01      Nucl.Phys. A815, 18 (2009)

T.Mart

Effects of the higher partial waves and relativistic terms on the accuracy of the calculation of the hypertriton electroproduction

NUCLEAR REACTIONS 3He(e, e'K+), E(cm)=3.5-5 GeV; calculated hypernucleus production σ(θ) using various approximations. Comparison with experimental data.

doi: 10.1016/j.nuclphysa.2008.10.009
Citations: PlumX Metrics


2008MA31      Phys.Rev. C 78, 014004 (2008)

T.Mart, B.I.S.van der Ventel

Photo- and electroproduction of the hypertriton on 3He

NUCLEAR REACTIONS 1H, 3He(e, e'K+), 3He(γ, K+); calculated σ, σ(θ). Comparison with experimental data.

doi: 10.1103/PhysRevC.78.014004
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2008MA37      Phys.Rev. C 78, 025808 (2008)

T.Mart, A.Sulaksono

Low-density instability of multicomponent matter with trapped neutrinos

doi: 10.1103/PhysRevC.78.025808
Citations: PlumX Metrics


2007BY03      Phys.Rev. C 76, 065202 (2007)

P.Bydzovsky, T.Mart

Analysis of the consistency of kaon photoproduction data with Λ in the final state

NUCLEAR REACTIONS p(γ, X)K+/Λ, E<2.6 GeV; calculated cross-sections.

doi: 10.1103/PhysRevC.76.065202
Citations: PlumX Metrics


2007HU05      Nucl.Phys. A782, 400c (2007)

P.T.P.Hutauruk, A.Sulaksono, T.Mart

Effects of the neutrino electromagnetic form factors on the neutrino and antineutrino mean free paths difference in dense matter

doi: 10.1016/j.nuclphysa.2006.10.034
Citations: PlumX Metrics


2007SU21      Phys.Rev. C 76, 041301 (2007)

A.Sulaksono, T.Mart, T.J.Burvenich, J.A.Maruhn

Instabilities of relativistic mean field models and the role of nonlinear terms

doi: 10.1103/PhysRevC.76.041301
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2006MA76      Phys.Rev. C 74, 055203 (2006)

T.Mart, A.Sulaksono

Kaon photoproduction in a multipole approach

NUCLEAR REACTIONS 1H(γ, K+X), E ≈ 1.5-2.5 GeV; analyzed hyperon production data; deduced resonance contributions.

doi: 10.1103/PhysRevC.74.055203
Citations: PlumX Metrics


2006MI21      Phys.Rev. C 74, 034002 (2006)

K.Miyagawa, T.Mart, C.Bennhold, W.Glockle

Polarization observables in exclusive kaon photoproduction on the deuteron

NUCLEAR REACTIONS 2H(γ, K+X), E=1.3 GeV; calculated σ(E, θ), polarization observables, hyperon production features.

doi: 10.1103/PhysRevC.74.034002
Citations: PlumX Metrics


2006NO07      Phys.Rev. C 74, 024323 (2006)

M.Nowakowski, N.G.Kelkar, T.Mart

Neutron structure effects in the deuteron and one neutron halos

NUCLEAR STRUCTURE 2H, 11Be; calculated binding-energy corrections arising from neutron electromagnetic form factors.

doi: 10.1103/PhysRevC.74.024323
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2006SA39      Phys.Rev. C 74, 044004 (2006)

A.Salam, K.Miyagawa, T.Mart, C.Bennhold, W.Glockle

K0 photoproduction on the deuteron and the extraction of the elementary amplitude

NUCLEAR REACTIONS 2H(γ, K0X), E=1.1 GeV; calculated hyperon production associated σ(E, θ), final state interaction effects.

doi: 10.1103/PhysRevC.74.044004
Citations: PlumX Metrics


2006SU03      Phys.Rev. C 73, 025803 (2006)

A.Sulaksono, C.K.Williams, P.T.P.Hutauruk, T.Mart

Effect of neutrino electromagnetic form factors on the neutrino cross section in dense matter

doi: 10.1103/PhysRevC.73.025803
Citations: PlumX Metrics


2006SU17      Phys.Rev. C 74, 045806 (2006)

A.Sulaksono, T.Mart

Low density instability in relativistic mean field models

doi: 10.1103/PhysRevC.74.045806
Citations: PlumX Metrics


2005LA12      Eur.Phys.J. A 24, 275 (2005)

R.Lawall, J.Barth, C.Bennhold, K.-H.Glander, S.Goers, J.Hannappel, N.Jopen, F.Klein, E.Klempt, T.Mart, D.Menze, M.Ostrick, E.Paul, I.Schulday, W.J.Schwille, F.W.Wieland, C.Wu

Measurement of the reaction γp → K0+ at photon energies up to 2.6 GeV

NUCLEAR REACTIONS 1H(γ, Σ+K0), E=0.9-2.6 GeV; measured σ, σ(θ), polarization. Tagged photons. Comparison with model predictions.

doi: 10.1140/epja/i2005-10002-x
Citations: PlumX Metrics


2005MA07      Phys.Rev. C 71, 022202 (2005)

T.Mart

Photoproduction of the Θ+ pentaquark in Feynman and Regge theories

NUCLEAR REACTIONS 1H(γ, X), E=1.7-16 GeV; calculated pentaquark production σ, σ(θ). Comparison of isobar and Regge models.

doi: 10.1103/PhysRevC.71.022202
Citations: PlumX Metrics


2005SU05      Phys.Rev. C 71, 034312 (2005)

A.Sulaksono, T.Mart, C.Bahri

Nilsson parameters κ and μ in relativistic mean field models

NUCLEAR STRUCTURE 208Pb, 132Sn, 40Ca; calculated single-particle energies, spin-orbit splitting, Nilsson parameters; deduced role of effective mass. Relativistic mean-field models, comparison with data.

doi: 10.1103/PhysRevC.71.034312
Citations: PlumX Metrics


2005SU26      Phys.Rev. C 72, 065801 (2005)

A.Sulaksono, P.T.P.Hutauruk, T.Mart

Isovector-channel role of relativistic mean field models in the neutrino mean free path

doi: 10.1103/PhysRevC.72.065801
Citations: PlumX Metrics


2004HU22      Phys.Rev. C 70, 068801 (2004)

P.T.P.Hutauruk, C.K.Williams, A.Sulaksono, T.Mart

Neutron fraction and neutrino mean free path predictions in relativistic mean field models

doi: 10.1103/PhysRevC.70.068801
Citations: PlumX Metrics


2003MI35      Mod.Phys.Lett. A 18, 290 (2003)

K.Miyagawa, T.Mart, C.Bennhold, W.Glockle

Electromagnetic K+ production on light nuclei with beam and hyperon recoil polarizations

NUCLEAR REACTIONS 2H(γ, K+X), E=1.3 GeV; 2H(e, e'K+X), E=3.2 GeV; calculated σ(E, θ), hyperon recoil polarization, final state interaction effects.

doi: 10.1142/S0217732303010363
Citations: PlumX Metrics


2003MO08      Phys.Rev. C 67, 055205 (2003)

R.M.Mohring, D.Abbott, A.Ahmidouch, Ts.A.Amatuni, P.Ambrozewicz, T.Angelescu, C.S.Armstrong, J.Arrington, K.Assamagan, S.Avery, K.Bailey, K.Beard, S.Beedoe, E.J.Beise, H.Breuer, R.Carlini, J.Cha, C.C.Chang, N.Chant, E.Cisbani, G.Collins, W.Cummings, S.Danagoulian, R.De Leo, F.Duncan, J.Dunne, D.Dutta, T.Eden, R.Ent, L.Eyraud, L.Ewell, M.Finn, T.Fortune, V.Frolov, S.Frullani, C.Furget, F.Garibaldi, D.Gaskell, D.F.Geesaman, P.Gueye, K.K.Gustafsson, J.-O.Hansen, M.Harvey, W.Hinton, E.Hungerford, M.Iodice, C.Jackson, C.Keppel, W.Kim, K.Kino, D.Koltenuk, S.Kox, L.Kramer, T.Leone, A.Lung, D.Mack, R.Madey, M.Maeda, S.Majewski, P.Markowitz, T.Mart, C.J.Martoff, D.Meekins, A.Mihul, J.Mitchell, H.Mkrtchyan, S.Mtingwa, I.Niculescu, R.Perrino, D.Potterveld, J.W.Price, B.A.Raue, J.-S.Real, J.Reinhold, P.Roos, T.Saito, G.Savage, R.Sawafta, R.Segel, S.Stepanyan, P.Stoler, V.Tadevosian, L.Tang, L.Teodorescu, T.Terasawa, H.Tsubota, G.M.Urciuoli, J.Volmer, W.Vulcan, T.P.Welch, R.Williams S.Wood, C.Yan, B.Zeidman

Separation of the longitudinal and transverse cross sections in the 1H(e, e'K+)Λ and 1H(e, e'K+0 reactions

NUCLEAR REACTIONS 1H(e, e'K+X), E=2.4-4 GeV; measured Λ and Σ0 hyperon production transverse and longitudinal σ, missing mass spectra. Comparison with previous results.

doi: 10.1103/PhysRevC.67.055205
Citations: PlumX Metrics


2001BA92      Nucl.Phys. A691, 374c (2001)

J.Barth, C.Bennhold, W.Braun, J.Ernst, K.H.Glander, S.Goers, J.Hannappel, N.Jopen, H.Kalinowsky, F.Klein, E.Klempt, A.Kozela, R.Lawall, J.Link, T.Mart, D.Menze, W.Neuerburg, M.Ostrick, E.Paul, H.van Pee, I.Schulday, W.-J.Schwille, J.Smyrski, U.Thoma, R.Wedemeyer, B.Wiegers, F.W.Wieland, J.Wisskirchen

New Results on η and η' Photoproduction with SAPHIR at ELSA

NUCLEAR REACTIONS 1H(γ, X), E=0.7-2.6 GeV; measured η and η' meson production σ, σ(θ).

doi: 10.1016/S0375-9474(01)01059-4
Citations: PlumX Metrics


2001HA22      Nucl.Phys. A684, 475c (2001)

H.Haberzettl, C.Bennhold, T.Mart

Gauge-Invariant Description of Photo- and Electroproduction of Mesons with Extended Nucleons Applied to Kaon Production

NUCLEAR REACTIONS 1H(γ, K+), (e, e'K+), E=high; calculated hyperon production associated σ(θ). Gauge-invariant approach, off-shell form factors discussed. Comparisons with data.

doi: 10.1016/S0375-9474(01)00510-3
Citations: PlumX Metrics


2001LE40      Nucl.Phys. A695, 237 (2001)

F.X.Lee, T.Mart, C.Bennhold, H.Haberzettl, L.E.Wright

Quasifree Kaon Photoproduction on Nuclei

NUCLEAR REACTIONS 1n, 1H(γ, K+), (γ, K0), E=1.6-2.2 GeV; calculated hyperon production σ, σ(θ), asymmetry, recoil polarization. 12C(γ, K+X), (γ, K0X), E=1.4 GeV; calculated hyperon production σ(θ), Ay(θ), final-state interaction effects.

doi: 10.1016/S0375-9474(01)01098-3
Citations: PlumX Metrics


2001MA36      Nucl.Phys. A684, 502c (2001)

T.Mart, S.Sumowidagdo, D.Kusno, C.Bennhold, H.Haberzettl

Kaon Photoproduction on the Nucleon: Overview of some applications

doi: 10.1016/S0375-9474(01)00477-8
Citations: PlumX Metrics


2001MI31      Nucl.Phys. A691, 64c (2001)

K.Miyagawa, H.Yamamura, T.Mart, C.Bennhold, H.Haberzettl, W.Glockle

Electromagnetic K+ Production on the Deuteron with Hyperon Recoil Polarization

NUCLEAR REACTIONS 2H(γ, K+), E=1.3 GeV; 2H(e, e'K+), E=3.2 GeV; calculated σ(E), σ(θ), hyperon polarization.

doi: 10.1016/S0375-9474(01)01008-9
Citations: PlumX Metrics


2000MA02      Phys.Rev. C61, 012201 (2000)

T.Mart, C.Bennhold

Evidence for a Missing Nucleon Resonance in Kaon Photoproduction

NUCLEAR REACTIONS 1H(γ, K+X), E(cm)=1.6-2.2 GeV; analyzed hyperon production associated σ, σ(θ), asymmetry; deduced possible resonance.

doi: 10.1103/PhysRevC.61.012201
Citations: PlumX Metrics


2000MA64      Phys.Rev. C62, 038201 (2000)

T.Mart

Role of P13(1720) in KΣ Photoproduction

NUCLEAR REACTIONS 1n, 1H(γ, K+), (γ, K0), E=1.7-2.2 GeV; calculated Σ hyperon production σ, σ(θ); deduced role of P13(1720) resonance. Comparisons with data.

doi: 10.1103/PhysRevC.62.038201
Citations: PlumX Metrics


2000YA01      Phys.Rev. C61, 014001 (2000)

H.Yamamura, K.Miyagawa, T.Mart, C.Bennhold, H.Haberzettl, W.Glockle

Inclusive K+ and Exclusive K+Y Photoproduction on the Deuteron: Λ- and Σ-Threshold Phenomena

NUCLEAR REACTIONS 2H(γ, K+X), E=high; calculated hyperon production associated σ, σ(θ); deduced final state interaction effects.

doi: 10.1103/PhysRevC.61.014001
Citations: PlumX Metrics


1999SU11      Phys.Rev. C60, 028201 (1999)

S.Sumowidagdo, T.Mart

Kaon Photoproduction on the Nucleon: Contributions of kaon-hyperon final states to the magnetic moment of the nucleon

NUCLEAR REACTIONS 1n, 1H(γ, K0), (γ, K+), E=1-2.2 GeV; calculated hyperon production associated total σ; deduced kaon-hyperon final states contribution to nucleon magnetic moments. Comparisons with data.

doi: 10.1103/PhysRevC.60.028201
Citations: PlumX Metrics


1998BE59      Nucl.Phys. A639, 209c (1998)

C.Bennhold, S.Goers, J.Barth, W.Braun, R.Burgwinkel, J.Ernst, K.H.Glander, J.Hannappel, N.Jopen, H.Kalinowsky, U.Kirch, F.Klein, F.J.Klein, E.Klempt, A.Kozela, R.Lawall, Z.Li, J.Link, T.Mart, D.Menze, W.Neuerburg, M.Paganetti, E.Paul, H.van Pee, R.Plotzke, M.Schumacher, W.J.Schwille, F.Smend, J.Smyrski, H.-N.Tran, M.Q.Tran, F.Wehnes, B.Wiegers, F.W.Wieland, J.Wisskirchen

K0+ Photoproduction with SAPHIR

NUCLEAR REACTIONS 1H(γ, K0), E=1.0-1.6 GeV; measured hyperon production σ(θ), σ. Model comparisons.

doi: 10.1016/S0375-9474(98)00275-9
Citations: PlumX Metrics


1998BE60      Nucl.Phys. A639, 227c (1998)

C.Bennhold, F.X.Lee, T.Mart, L.E.Wright

Kaon Electromagnetic Production on Nuclei

NUCLEAR REACTIONS 12C(γ, K+X)11B, E=1.4 GeV; calculated hyperon production σ(θ); deduced reaction mechanism features. Quasifree kinematics.

doi: 10.1016/S0375-9474(98)00278-4
Citations: PlumX Metrics


1998HA32      Phys.Rev. C58, R40 (1998)

H.Haberzettl, C.Bennhold, T.Mart, T.Feuster

Gauge-Invariant Tree-Level Photoproduction Amplitudes with Form Factors

doi: 10.1103/PhysRevC.58.R40
Citations: PlumX Metrics


1998MA20      Nucl.Phys. A631, 765c (1998)

T.Mart, D.Kusno, C.Bennhold, L.Tiator, D.Drechsel

Photoproduction of the Hypertriton

NUCLEAR REACTIONS 3He(γ, X), E=1500-2200 MeV; calculated kaon production σ(θ); deduced hypertriton production features. Fadeev equations.

doi: 10.1016/S0375-9474(98)00106-7
Citations: PlumX Metrics


1998MA57      Nucl.Phys. A639, 237c (1998)

T.Mart, C.Bennhold

Kaon and Hyperon Form Factors in Kaon Electroproduction on the Nucleon

NUCLEAR REACTIONS 1n, 1H(e, e'K0), 1H(e, e'K+), E not given; calculated hyperon production associated response functions.

doi: 10.1016/S0375-9474(98)00279-6
Citations: PlumX Metrics


1998MA59      Nucl.Phys. A640, 235 (1998)

T.Mart, L.Tiator, D.Drechsel, C.Bennhold

Electromagnetic Production of the Hypertriton

NUCLEAR REACTIONS 3He(γ, K+), E=1500-2200 MeV; calculated hypernucleus production σ(θ); deduced Fermi motion effects, other reaction mechanism features. Impulse approximation.

doi: 10.1016/S0375-9474(98)00441-2
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1998TR06      Phys.Lett. 445B, 20 (1998)

M.Q.Tran, J.Barth, C.Bennhold, M.Bockhorst, W.Braun, A.Budzanowski, G.Burbach, R.Burgwinkel, J.Ernst, K.H.Glander, S.Goers, B.Guse, K.-M.Haas, J.Hannappel, K.Heinloth, K.Honscheid, T.Jahnen, N.Jopen, H.Jungst, H.Kalinowsky, U.Kirch, F.J.Klein, F.Klein, E.Klempt, D.Kostrewa, A.Kozela, R.Lawall, L.Lindemann, J.Link, J.Manns, T.Mart, D.Menze, H.Merkel, R.Merkel, W.Neuerburg, M.Paganetti, E.Paul, R.Plotzke, U.Schenk, J.Scholmann, I.Schulday, M.Schumacher, P.Schutz, W.J.Schwille, F.Smend, J.Smyrski, W.Speth, H.N.Tran, H.van Pee, W.Vogel, R.Wedemeyer, F.Wehnes, B.Wiegers, F.W.Wieland, J.Wisskirchen, A.Wolf, and the SAPHIR Collaboration

Measurement of γp → K+ Λ and γp → K+Σ0 at Photon Energies up to 2 GeV

NUCLEAR REACTIONS 1H(γ, K+X), E=0.8-2 GeV; measured Λ, Σ0 hyperon production σ(θ), σ, polarizations. Tagged photons.

doi: 10.1016/S0370-2693(98)01393-8
Citations: PlumX Metrics


1996MA83      Acta Phys.Pol. B27, 3167 (1996)

T.Mart, C.Bennhold, L.Alfieri

Electromagnetic Production of Kaons on the Nucleon


1995MA09      Phys.Rev. C51, R1074 (1995)

T.Mart, C.Bennhold, C.E.Hyde-Wright

Constraints on Coupling Constants Through Charge Σ Photoproduction

NUCLEAR REACTIONS 1n, 1H(γ, X), E=1-2 GeV; analyzed Σ+, Σ- production σ(E) data; deduced Born coupling constants. Phenomenological models.

doi: 10.1103/PhysRevC.51.R1074
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