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NSR database version of April 26, 2024.

Search: Author = A.M.Gasparyan

Found 27 matches.

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2023GA07      Phys.Rev. C 107, 034001 (2023)

A.M.Gasparyan, E.Epelbaum

"Renormalization-group-invariant effective field theory" for few-nucleon systems is cutoff dependent

doi: 10.1103/PhysRevC.107.034001
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2023GA08      Phys.Rev. C 107, 044002 (2023)

A.M.Gasparyan, E.Epelbaum

Renormalization of nuclear chiral effective field theory with nonperturbative leading-order interactions

doi: 10.1103/PhysRevC.107.044002
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2022GA08      Phys.Rev. C 105, 024001 (2022)

A.M.Gasparyan, E.Epelbaum

Nucleon-nucleon interaction in chiral effective field theory with a finite cutoff: Explicit perturbative renormalization at next-to-leading order

doi: 10.1103/PhysRevC.105.024001
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2022RI03      Phys.Rev. C 106, 025202 (2022)

N.Rijneveen, A.M.Gasparyan, H.Krebs, E.Epelbaum

Pion photoproduction in chiral perturbation theory with explicit treatment of the Δ(1232) resonance

NUCLEAR REACTIONS 1H(γ, π0p), √ sNN=1092-1214 GeV; calculated low-energy constants, s- and p-wave multipoles contributions to the pion photoproduction σ(E). Covariant chiral perturbation theory with explicit Δ(1232) degrees of freedom with errors from the truncation of the small-scale expansion estimated using Bayesian approach. Comparison with experimental data from MAMI-Mainz facility.

doi: 10.1103/PhysRevC.106.025202
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2021RI05      Phys.Rev. C 103, 045203 (2021)

J.Rijneveen, N.Rijneveen, H.Krebs, A.M.Gasparyan, E.Epelbaum

Radiative pion photoproduction in covariant chiral perturbation theory

NUCLEAR REACTIONS 1H(γ, pπ0γ), (polarized γ, pπ0γ), (γ, nπ+γ), (polarized γ, nπ+γ), E<200 MeV; calculated differential σ(E), convergence of the small-scale expansion and sensitivity to magnetic moment of Δ+, double differential σ(E, θ), polarization asymmetries. Covariant chiral perturbation theory with explicitΔ(1232) degrees of freedom, including contributions up to next-to-next-to-leading order, with errors from the truncation of the small-scale expansion estimated using Bayesian approach. Comparison with experimental data from MAMI-Mainz facility.

doi: 10.1103/PhysRevC.103.045203
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2021TH07      Phys.Rev. C 103, 035201 (2021)

M.Thurmann, E.Epelbaum, A.M.Gasparyan, H.Krebs

Nucleon polarizabilities in covariant baryon chiral perturbation theory with explicit Δ degrees of freedom

NUCLEAR STRUCTURE 1H, 1n; calculated nucleon spin-independent octupole, quadrupole dispersive, and higher dipole dispersive polarizabilities. Chiral perturbation theory, with explicit Δ(1232) degrees of freedom. Comparison with available experimental data, and with other theoretical results.

doi: 10.1103/PhysRevC.103.035201
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2020EP02      Eur.Phys.J. A 56, 152 (2020)

E.Epelbaum, A.M.Gasparyan, J.Gegelia, Ulf-G.Meissner, X.-L.Ren

How to renormalize integral equations with singular potentials in effective field theory

doi: 10.1140/epja/s10050-020-00162-4
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2019EP02      Eur.Phys.J. A 55, 56 (2019)

E.Epelbaum, A.M.Gasparyan, J.Gegelia, Ulf-G.Meissner

Reply to the Comment by Manuel Pavon Valderrama on "How (not) to renormalize integral equations with singular potentials in effective field theory"

doi: 10.1140/epja/i2019-12751-1
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2018EP01      Eur.Phys.J. A 54, 186 (2018)

E.Epelbaum, A.M.Gasparyan, J.Gegelia, Ulf-G.Meissner

How (not) to renormalize integral equations with singular potentials in effective field theory

doi: 10.1140/epja/i2018-12632-1
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2018KR02      Phys.Rev. C 98, 014003 (2018)

H.Krebs, A.M.Gasparyan, E.Epelbaum

Three-nucleon force in chiral effective field theory with explicit Δ(1232) degrees of freedom: Longest-range contributions at fourth order

doi: 10.1103/PhysRevC.98.014003
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2017SI25      Phys.Rev. C 96, 055205 (2017)

D.Siemens, V.Bernard, E.Epelbaum, A.M.Gasparyan, H.Krebs, Ulf-G.Meissner

Elastic and inelastic pion-nucleon scattering to fourth order in chiral perturbation theory

NUCLEAR REACTIONS 1H(π-, π0π0), (π-, π+π-), (π-, π0π-), (π+, π+π+), (π-, π+π0), Tπ<0.4 GeV; calculated pion-nucleon total cross sections, σ(θ, E), low-energy constants (LECs); deduced contributions of the Δ(1232) resonance. Chiral perturbation theory using heavy-baryon approach and covariant formulation, with extended on-mass-shell (EOMS) scheme. Comparison with experimental data.

doi: 10.1103/PhysRevC.96.055205
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2015EP01      Eur.Phys.J. A 51, 26 (2015)

E.Epelbaum, A.M.Gasparyan, H.Krebs, C.Schat

Three-nucleon force at large distances: Insights from chiral effective field theory and the large-Nc expansion

doi: 10.1140/epja/i2015-15026-y
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2015EP03      Eur.Phys.J. A 51, 71 (2015)

E.Epelbaum, A.M.Gasparyan, J.Gegelia, H.Krebs

1S0 nucleon-nucleon scattering in the modified Weinberg approach

doi: 10.1140/epja/i2015-15071-6
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2014EP02      Eur.Phys.J. A 50, 51 (2014)

E.Epelbaum, A.M.Gasparyan, J.Gegelia, M.R.Schindler

Deuteron electromagnetic form factors in a renormalizable formulation of chiral effective field theory

NUCLEAR STRUCTURE 2H; calculated Coulomb, magnetic and quadrupole form factors using renormalizable chiral effective field theory.

doi: 10.1140/epja/i2014-14051-8
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2014EP04      Few-Body Systems 55, 967 (2014)

E.Epelbaum, A.M.Gasparyan, J.Gegelia, M.R.Schindler

Renormalizable Chiral EFT for NN Scattering

doi: 10.1007/s00601-013-0763-5
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2013GA39      Eur.Phys.J. A 49, 115 (2013)

A.M.Gasparyan, M.F.M.Lutz, E.Epelbaum

Two-nucleon scattering: Merging chiral effective field theory with dispersion relations

doi: 10.1140/epja/i2013-13115-7
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2012GA03      Phys.Rev. C 85, 015204 (2012)

A.M.Gasparyan, J.Haidenbauer, C.Hanhart

Scattering lengths of strangeness S= -2 baryon-baryon interactions

doi: 10.1103/PhysRevC.85.015204
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2011GA41      Nucl.Phys. A866, 79 (2011)

A.M.Gasparyan, M.F.M.Lutz, B.Pasquini

Compton scattering from chiral dynamics with unitarity and causality

NUCLEAR REACTIONS 1H(γ, γ'), E=0-0.35 GeV; calculated beam asymmetry, beam asymmetry(θ) for polarized, unpolarized target.

doi: 10.1016/j.nuclphysa.2011.07.005
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2004HA62      Fizika(Zagreb) B 13, 37 (2004)

J.Haidenbauer, V.Baru, A.M.Gasparyan, C.Hanhart, J.Speth

Eta meson production in NN collisions

NUCLEAR REACTIONS 1H(p, pX), (n, nX), E ≈ threshold; calculated η meson production σ, invariant mass spectra. Comparisons with data.


2003BA14      Phys.Rev. C 67, 024002 (2003)

V.Baru, A.M.Gasparyan, J.Haidenbauer, C.Hanhart, A.E.Kudryavtsev, J.Speth

Production of η mesons in nucleon-nucleon collisions

NUCLEAR REACTIONS 1H(p, pX), (n, nX), (n, dX), E ≈ threshold; calculated η production σ. Microscopic calculation, comparisons with data.

doi: 10.1103/PhysRevC.67.024002
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2003BA95      Nucl.Phys. A721, 727c (2003)

V.Baru, A.M.Gasparyan, J.Haidenbauer, C.Hanhart, A.E.Kudryavtsev, J.Speth

Production of η mesons in nucleon-nucleon collisions

NUCLEAR REACTIONS 1n, 1H(p, pX), 1n(p, dX), E ≈ threshold; calculated η meson production σ. Comparisons with data.

doi: 10.1016/S0375-9474(03)01167-9
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2003GA35      Phys.Rev. C 68, 045207 (2003)

A.M.Gasparyan, J.Haidenbauer, C.Hanhart, J.Speth

Pion-nucleon scattering in a meson-exchange model

NUCLEAR REACTIONS 1n, 1H(π, π), E(cm)=1.1-1.9 GeV; calculated phase shifts, inelasticities. 1H(π-, nX), E(cm)=1400-1900 MeV; calculated η meson production σ, σ(θ). Meson exchange model, comparisons with data.

doi: 10.1103/PhysRevC.68.045207
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2003GA44      Eur.Phys.J. A 18, 305 (2003)

A.M.Gasparyan, V.Yu.Grishina, L.A.Kondratyuk, W.Cassing

Exclusive and semi-inclusive strangeness and charm production in πN and NN reactions

NUCLEAR REACTIONS 1H(π-, X), (p, pX), E=high; calculated kaon and hyperon production σ; deduced reaction mechanism features. Quark-gluon strings model, comparisons with data.

doi: 10.1140/epja/i2002-10222-6
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2001BA38      Yad.Fiz. 64, No 3, 633 (2001); Phys.Atomic Nuclei 64, 579 (2001)

V.V.Baru, A.M.Gasparian, J.Haidenbauer, A.E.Kudryavtsev, J.Speth

On the Migdal-Watson Approach to FSI Effects in Meson Production in NN Collisions

NUCLEAR REACTIONS 1H(p, pX), E ≈ threshold; calculated meson production associated final state interaction form factors. Migdal-Watson approach.

doi: 10.1134/1.1358484
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2001GA30      Nucl.Phys. A684, 397c (2001)

A.M.Gasparian, J.Haidenbauer, C.Hanhart, L.Kondratyuk, J.Speth

Near Threshold Λ and Σ Production in pp Collisions

NUCLEAR REACTIONS 1H(p, K+X), E ≈ threshold; calculated Λ and Σ hyperon production σ. Comparison with data.

doi: 10.1016/S0375-9474(01)00407-9
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2000BA92      Acta Phys.Pol. B31, 2127 (2000)

V.Baru, A.M.Gasparian, J.Haidenbauer, A.E.Kudryavtsev, J.Speth

FSI Effects in Meson Production in NN Collisions


2000GA21      Phys.Lett. 480B, 273 (2000)

A.M.Gasparian, J.Haidenbauer, C.Hanhart, L.Kondratyuk, J.Speth

The Reactions pp → pΛK+ and pp → pΣ0K+ Near Their Thresholds

NUCLEAR REACTIONS 1H(p, K+X), E ≈ threshold; calculated hyperon associated production σ; deduced reaction mechanism features. Comparisons with data.

doi: 10.1016/S0370-2693(00)00412-3
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Note: The following list of authors and aliases matches the search parameter A.M.Gasparyan: A.M.GASPARIAN, A.M.GASPARYAN