NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = G.Rupak Found 31 matches. 2023YA29 Eur.Phys.J. A 59, 233 (2023) C.-J.Yang, A.Ekstrom, C.Forssen, G.Hagen, G.Rupak, U.van Kolck The importance of few-nucleon forces in chiral effective field theory NUCLEAR STRUCTURE 3H, 4He, 16O, 40Ca; calculated binding energy per nucleon with NN-only and NN+NNN interactions at leading order (LO) with coupled-cluster model of the equation of state for symmetric nuclear matter; deduced LO four-nucleon forces could play a crucial role for describing heavy-mass nuclei.
doi: 10.1140/epja/s10050-023-01149-7
2022HI04 Phys.Rev. C 106, 014601 (2022) R.Higa, P.Premarathna, G.Rupak Coupled-channels treatment of 7Be(p, γ)8B in effective field theory NUCLEAR REACTIONS 7Be(p, γ), E(cm)=0.2864-50.3 MeV; calculated S-factor, E1 and M1 contributions to the radiative capture. Halo effective field theory up to next-to-next-to-leading order (NNLO). Comparison to experimental data and previous EFT calculations. Bayesian analysis to estimate the expected theory error.
doi: 10.1103/PhysRevC.106.014601
2021HI13 Eur.Phys.J. A 57, 269 (2021) R.Higa, P.Premarathna, G.Rupak Coupled-channel treatment of 7Li(n, γ)8Li in effective field theory NUCLEAR REACTIONS 7Li(n, γ), E<1 MeV; calculated total capture σ, contributions of inelastic channels. Comparison with available data.
doi: 10.1140/epja/s10050-021-00516-6
2020PR07 Eur.Phys.J. A 56, 166 (2020) Bayesian analysis of capture reactions 3He(α, γ)7Be and 3H(α, γ)7Li
doi: 10.1140/epja/s10050-020-00113-z
2019AC09 Phys.Rev. C 100, 021001R (2019) Universal behavior of p-wave proton-proton fusion near threshold NUCLEAR REACTIONS 1H(p, X), E<110 keV; calculated p-wave contribution to the proton-proton fusion S factor and total threshold S factor using chiral effective-field theory (EFT) up to the next-to-leading order.
doi: 10.1103/PhysRevC.100.021001
2018HI09 Eur.Phys.J. A 54, 89 (2018) Radiative 3He(α, g)7Be reaction in halo effective field theory NUCLEAR REACTIONS 3He(α, γ), E not given; calculated phase shifts using halo effective field theory (EFT) (in LO and NLO); deduced parameters from simultaneous fitting published phase shift data for both reactions. 3He(α, γ)7Be, E(cm)=0-1600 keV; calculated S-factor, branching ratio.Compared to data.
doi: 10.1140/epja/i2018-12486-5
2017EL05 Phys.Rev.Lett. 119, 222505 (2017) S.Elhatisari, E.Epelbaum, H.Krebs, T.A.Lahde, D.Lee, N.Li, B.-n.Lu, U.-G.Meissner, G.Rupak Ab initio Calculations of the Isotopic Dependence of Nuclear Clustering NUCLEAR STRUCTURE 12,14,16C; calculated proton and neutron densities for the ground states, spin-up proton probability distributions.
doi: 10.1103/PhysRevLett.119.222505
2016EL02 Eur.Phys.J. A 52, 174 (2016) S.Elhatisari, D.Lee, U.-G.Meissner, G.Rupak Nucleon-deuteron scattering using the adiabatic projection method
doi: 10.1140/epja/i2016-16174-2
2016EL03 Phys.Rev.Lett. 117, 132501 (2016) S.Elhatisari, N.Li, A.Rokash, J.M.Alarcon, D.Du, N.Klein, B.-n.Lu, U.-G.Meissner, E.Epelbaum, H.Krebs, Ti.A.Lahde, De.Lee, G.Rupak Nuclear Binding Near a Quantum Phase Transition NUCLEAR STRUCTURE 3H, 3,4He, 8Be, 12C, 16O, 20Ne; calculated ground state energies; deduced a first-order transition at zero temperature from a Bose-condensed gas of alpha particles to a nuclear liquid. Leading order (LO) nuclear interactions.
doi: 10.1103/PhysRevLett.117.132501
2015EL07 Nature(London) 528, 111 (2015) S.Elhatisari, D.Lee, G.Rupak, E.Epelbaum, H.Krebs, T.A.Lahde, T.Luu, Ulf-G.Meissner Ab initio alpha-alpha scattering NUCLEAR REACTIONS 4He(α, α), (α, X), E<12 MeV; calculated phase shifts, wave functions. Comparison with experimental data, lattice Monte Carlo simulations.
doi: 10.1038/nature16067
2015LA16 Eur.Phys.J. A 51, 92 (2015) T.A.Lahde, T.Luu, D.Lee, U.-G.Meissner, E.Epelbaum, H.Krebs, G.Rupak Nuclear lattice simulations using symmetry-sign extrapolation NUCLEAR STRUCTURE 6He, 6Be, 12C; calculated two-nucleon, three-nucleon forces shift for low energy levels using PMC (Projection Monte Carlo) with LO, NLO, EMIB and 3NF.
doi: 10.1140/epja/i2015-15092-1
2014EP01 Phys.Rev.Lett. 112, 102501 (2014) E.Epelbaum, H.Krebs, T.A.Lahde, D.Lee, Ulf-G.Meissner, G.Rupak Ab Initio Calculation of the Spectrum and Structure of 16O NUCLEAR STRUCTURE 16O; calculated lowest energy even-parity states, J, π, charge radius, quadrupole moments, B(E2), M(E0). Comparison with experimental data.
doi: 10.1103/PhysRevLett.112.102501
2013PI12 Eur.Phys.J. A 49, 151 (2013) Adiabatic projection method for scattering and reactions on the lattice
doi: 10.1140/epja/i2013-13151-3
2013RU09 Phys.Rev.Lett. 111, 032502 (2013) Radiative Capture Reactions in Lattice Effective Field Theory
doi: 10.1103/PhysRevLett.111.032502
2013RU15 Phys.Rev. C 88, 065801 (2013) r-mode instability in quark stars with a crystalline crust
doi: 10.1103/PhysRevC.88.065801
2012FE02 Eur.Phys.J. A 48, 24 (2012) Leading E1 and M1 contributions to radiative neutron capture on lithium-7
doi: 10.1140/epja/i2012-12024-7
2012RU05 Phys.Rev. C 86, 044608 (2012) G.Rupak, L.Fernando, A.Vaghani Radiative neutron capture on carbon-14 in effective field theory NUCLEAR REACTIONS 14C(n, γ)15C, E(cm)<2 MeV; calculated B(E1) strength. Model-independent formalism of halo effective field theory. Resonant and nonresonant interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.044608
2011RU09 Phys.Rev.Lett. 106, 222501 (2011) Model-Independent Calculation of Radiative Neutron Capture on Lithium-7 NUCLEAR REACTIONS 7Li(n, γ), E not given; calculated σ. Phenomenological potentials in the single-particle approximation.
doi: 10.1103/PhysRevLett.106.222501
2010RU11 Phys.Rev. C 82, 055806 (2010) Constraining phases of quark matter with studies of r-mode damping in compact stars
doi: 10.1103/PhysRevC.82.055806
2009RU02 Nucl.Phys. A816, 52 (2009) Density functional theory for non-relativistic fermions in the unitarity limit
doi: 10.1016/j.nuclphysa.2008.11.004
2005BE22 Phys.Rev. D 71, 054015 (2005) P.F.Bedaque, H.W.Griesshammer, G.Rupak A nucleon in a tiny box
doi: 10.1103/PhysRevD.71.054015
2005RE03 Phys.Rev. C 71, 025201 (2005) Phase structure of two-flavor quark matter: Heterogeneous superconductors
doi: 10.1103/PhysRevC.71.025201
2003BE08 Nucl.Phys. A714, 589 (2003) P.E.Bedaque, G.Rupak, H.W.Griesshammer, H.-W.Hammer Low energy expansion in the three body system to all orders and the triton channel NUCLEAR REACTIONS 2H(n, n), E not given; calculated phase shifts, three-body force effects.
doi: 10.1016/S0375-9474(02)01402-1
2003BE63 Phys.Rev. C 68, 065802 (2003) P.F.Bedaque, G.Rupak, M.J.Savage Goldstone bosons in the 3P2 superfluid phase of neutron matter and neutrino emission
doi: 10.1103/PhysRevC.68.065802
2003RU03 Nucl.Phys. A717, 73 (2003) Quartet S-wave p-d scattering in EFT NUCLEAR REACTIONS 2H(p, p), E(cm)=20-100 MeV; calculated phase shifts. Pionless effective field theory, power counting, comparison with data.
doi: 10.1016/S0375-9474(03)00638-9
2002GR07 Phys.Lett. 529B, 57 (2002) Nucleon Polarisabilities from Compton Scattering on the Deuteron NUCLEAR REACTIONS 2H(γ, γ), E=20-50 MeV; calculated, analyzed σ(θ); deduced nucleon polarizabilities.
doi: 10.1016/S0370-2693(02)01238-8
2000PH01 Phys.Lett. 473B, 209 (2000) D.R.Phillips, G.Rupak, M.J.Savage Improving the Convergence of NN Effective Field Theory NUCLEAR STRUCTURE 2H; calculated radius, quadrupole moment. Low-energy effective field theory.
doi: 10.1016/S0370-2693(99)01496-3
2000RU07 Nucl.Phys. A678, 405 (2000) Precision Calculation of np → dγ Cross Section for Big-Bang Nucleosynthesis NUCLEAR REACTIONS 1H(n, γ), E(cm) < 1 MeV; 2H(γ, n), E=2-10 MeV; calculated σ. Effective field theory. Applications to big-bang nucleosynthesis discussed.
doi: 10.1016/S0375-9474(00)00323-7
1999CH21 Nucl.Phys. A653, 386 (1999) J.-W.Chen, G.Rupak, M.J.Savage Nucleon-Nucleon Effective Field Theory without Pions NUCLEAR REACTIONS 1H(n, γ), E=low; calculated σ, effective range parameters. Effective field theory without pions. NUCLEAR STRUCTURE 2H; calculated form factors. Effective field theory without pions.
doi: 10.1016/S0375-9474(99)00298-5
1999CH31 Phys.Lett. 464B, 1 (1999) Isoscalar M1 and E2 Amplitudes in np → dγ NUCLEAR REACTIONS 1H(n, γ), E=low; calculated isoscaler M1 and E2 amplitudes. NUCLEAR STRUCTURE 2H; calculated quadrupole form factor.
doi: 10.1016/S0370-2693(99)01007-2
1999RU08 Phys.Rev. C60, 054004 (1999) Next-to-Next-to-Leading-Order Calculation of Two-Nucleon Scattering in an Effective Field Theory
doi: 10.1103/PhysRevC.60.054004
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