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NSR database version of April 24, 2024.

Search: Author = B.Blankleider

Found 25 matches.

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2021BL08      Few-Body Systems 62, 87 (2021)

B.Blankleider, S.S.Kumar, A.N.Kvinikhidze

Effect of Nucleon Dressing on Triton Binding Energy

NUCLEAR STRUCTURE 3H; calculated triton binding energy shifts due to nucleon dressing, nucleon dressing model parameters.

doi: 10.1007/s00601-021-01676-3
Citations: PlumX Metrics


2019SK01      Phys.Rev. C 99, 034001 (2019)

T.Skawronski, B.Blankleider, A.N.Kvinikhidze

Electromagnetic currents of the pion-nucleon system

doi: 10.1103/PhysRevC.99.034001
Citations: PlumX Metrics


2009KV02      Phys.Rev. C 80, 044004 (2009)

A.N.Kvinikhidze, B.Blankleider, E.Epelbaum, C.Hanhart, M.Pavon Valderrama

Gauge invariance in the presence of a cutoff

doi: 10.1103/PhysRevC.80.044004
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2007KV01      Nucl.Phys. A784, 259 (2007)

A.N.Kvinikhidze, B.Blankleider

Generalized parton distributions for dynamical equation models

doi: 10.1016/j.nuclphysa.2006.11.161
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2007KV06      Phys.Rev. C 76, 064003 (2007)

A.N.Kvinikhidze, B.Blankleider

Wilsonian renormalization group equation for nuclear current operators

doi: 10.1103/PhysRevC.76.064003
Citations: PlumX Metrics


2005KV01      Phys.Rev. C 72, 054001 (2005)

A.N.Kvinikhidze, B.Blankleider

Three-body problem at finite temperature and density

doi: 10.1103/PhysRevC.72.054001
Citations: PlumX Metrics


2002KV02      Phys.Rev. C66, 045203 (2002)

A.N.Kvinikhidze, M.C.Birse, B.Blankleider

Pionic dressing of baryons in chiral quark models

doi: 10.1103/PhysRevC.66.045203
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2000KV02      Nucl.Phys. A670, 210c (2000)

A.N.Kvinikhidze, B.Blankleider

Complete Set of Electromagnetic Corrections to the Nucleon Mass in the Nambu-Jona-Lasinio Model

doi: 10.1016/S0375-9474(00)00101-9
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1999KV01      Phys.Rev. C59, 1263 (1999)

A.N.Kvinikhidze, B.Blankleider

Unified Relativistic Description of πNN and γπNN

doi: 10.1103/PhysRevC.59.1263
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1999KV02      Phys.Rev. C60, 044003 (1999)

A.N.Kvinikhidze, B.Blankleider

Gauging of Equations Method. I. Electromagnetic Currents of Three Distinguishable Particles

doi: 10.1103/PhysRevC.60.044003
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1999KV03      Phys.Rev. C60, 044004 (1999)

A.N.Kvinikhidze, B.Blankleider

Gauging of Equations Method. II. Electromagnetic Currents of Three Identical Particles

doi: 10.1103/PhysRevC.60.044004
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1998KV01      Nucl.Phys. A631, 559c (1998)

A.N.Kvinikhidze, B.Blankleider

Gauging Hadronic Systems

doi: 10.1016/S0375-9474(98)00067-0
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1997KV01      Phys.Rev. C56, 2963 (1997)

A.N.Kvinikhidze, B.Blankleider

Gauging the Spectator Equations

doi: 10.1103/PhysRevC.56.2963
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1997KV02      Phys.Rev. C56, 2973 (1997)

A.N.Kvinikhidze, B.Blankleider

Gauging the Three-Nucleon Spectator Equation

doi: 10.1103/PhysRevC.56.2973
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1995WE05      Phys.Rev. C51, 2575 (1995)

M.Wessler, E.Boschitz, B.Brinkmoller, J.Buhler, H.Garcilazo, W.Gyles, W.List, R.Meier, S.Ritt, R.Tacik, J.A.Konter, D.Gill, S.Mango, D.Renker, B.van den Brandt, G.Wait, V.A.Efimovykh, A.I.Kovalev, A.N.Prokofiev, W.Thiel, B.Blankleider

Polarization Observables in πd(pol) Elastic Scattering: Analyzing powers τ22 and iT11 in the Forward Hemisphere

NUCLEAR REACTIONS 2H(π+, π+), E=100-294 MeV; measured analyzing powers, other observables. Polarized target, two different methods. Model comparison.

doi: 10.1103/PhysRevC.51.2575
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1994KV01      Nucl.Phys. A574, 788 (1994)

A.N.Kvinikhidze, B.Blankleider

Covariant Three-Body Equations in φ3 Field Theory

doi: 10.1016/0375-9474(94)90959-8
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1990AL21      Phys.Rev. C42, 517 (1990)

C.Alexandrou, B.Blankleider

Effects of Short Range ΔN Interaction on Observables of the πNN System

NUCLEAR REACTIONS 2H(π, π), E=140-256 MeV; calculated σ(θ), iT11(θ). 1H(p, π+), (polarized p, π+), E=567-800 MeV; calculated σ(θ), analyzing power vs θ; deduced nucleon-isobar interaction role. Polarized, unpolarized targets.

doi: 10.1103/PhysRevC.42.517
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1990NO01      Phys.Rev. C41, 213 (1990)

S.Nozawa, T.-S.H.Lee, B.Blankleider

Neutral Pion Photoproduction on the Nucleon Near Threshold

NUCLEAR REACTIONS 1H(γ, π0), E=145-160 MeV; calculated σ(E); deduced final state interaction role. Dynamical model.

doi: 10.1103/PhysRevC.41.213
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1990NO03      Nucl.Phys. A508, 355c (1990)

S.Nozawa, T.-S.H.Lee, B.Blankleider

Neutral Pion Photoproduction of the Nucleon Near Threshold

NUCLEAR REACTIONS 1H(γ, π0), (γ, π+), (γ, π-), E at threshold; calculated amplitudes; deduced π0 production mechanism. Dynamical model.

doi: 10.1016/0375-9474(90)90497-A
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1990NO05      Nucl.Phys. A513, 459 (1990)

S.Nozawa, B.Blankleider, T.-S.H.Lee

A Dynamical Model of Pion Photoproduction on the Nucleon

NUCLEAR REACTIONS 1n(γ, π-), 1H(γ, π+), (γ, π0), E=180-450 MeV; calculated σ(θ), recoil nucleon asymmetries. Dynamical model.

doi: 10.1016/0375-9474(90)90395-3
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1987BL03      Nucl.Phys. A463, 77c (1987)

B.Blankleider

Few Body Physics at SIN

NUCLEAR REACTIONS 2H(π, π), E=100-400 MeV; compiled, analyzed σ(E, θ), tensor polarization; 2H(π+, π+p), E=294 MeV; compiled, analyzed σ(Ep, θp, θπ); 3He(π+, γ), (π-, γ), E=120 MeV; compiled, analyzed σ(θ).

doi: 10.1016/0375-9474(87)90649-X
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1985BL08      Phys.Rev. C31, 1380 (1985)

B.Blankleider, I.R.Afnan

Relatioship between Partial Wave Amplitudes and Polarization Observables in pp → dπ+ and πd → πd

NUCLEAR REACTIONS 1H(polarized p, π+), E=567, 383, 800 MeV; calculated σ(θ), polarization transfer, correlation observables vs θ; deduced relation to partial wave amplitudes. Orthogonal function expansion.

doi: 10.1103/PhysRevC.31.1380
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1984BL02      Phys.Rev. C29, 538 (1984)

B.Blankleider, R.M.Woloshyn

Quasi-Elastic Scattering of Polarized Electrons on Polarized 3He

NUCLEAR REACTIONS 3He(e, e'), E=0.2488, 0.3984, 0.5, 7.26 GeV; calculated σ(θ, E(e')). 3He(polarized e, e'), E=0.25-2.75 GeV; calculated σ(θ, E(e')), asymmetry vs E. Polarized target, longitudinal beam polarization, impulse approximation.

doi: 10.1103/PhysRevC.29.538
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1981BL12      Phys.Rev. C24, 1572 (1981)

B.Blankleider, I.R.Afnan

Unified Theory of NN → πd, πd → πd, and NN → NN Reactions

NUCLEAR REACTIONS 2H(π+, d), E=25-250 MeV; calculated σ(total, E); 1H(p, π+), E=382.9-799.3 MeV; calculated σ(θ); 2H(π+, π+), E=47.7 MeV; calculated σ(θ); 2H(π+, π+), E=50-350 MeV; calculated σ(total, E); 2H(π+, π+), E=140, 256 MeV; calculated iT11(θ, d), T20(θ, d). Nucleon-nucleon phase shift input, unified theory.

doi: 10.1103/PhysRevC.24.1572
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1980AF01      Phys.Lett. 93B, 367 (1980)

I.R.Afnan, B.Blankleider

The Effect of Absorption on Low Energy π-d Scattering

NUCLEAR REACTIONS 2H(π+, π+), (π+, p), E=47.7 MeV; calculated σ(θ); deduced absorption effects. 1H(p, p), E=380, 425 MeV; calculated phase shifts. Faddeev equations, channel coupling effects.

doi: 10.1016/0370-2693(80)90344-5
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