NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = R.J.Furnstahl Found 107 matches. Showing 1 to 100. [Next]2024ZU01 Phys.Rev. C 109, 014319 (2024) L.Zurek, S.K.Bogner, R.J.Furnstahl, R.Navarro Perez, N.Schunck, A.Schwenk Optimized nuclear energy density functionals including long-range pion contributions
doi: 10.1103/PhysRevC.109.014319
2023GA12 Phys.Rev. C 107, 054001 (2023) A.J.Garcia, C .Drischler, R.J.Furnstahl, J.A.Melendez, X.Zhang Wave-function-based emulation for nucleon-nucleon scattering in momentum space NUCLEAR REACTIONS 1H(n, n), E<360 MeV; calculated phase shifts, σ(θ), σ(E), analyzing power. Scattering emulator based on the Kohn variational principle (KVP) extended to momentum space (including coupled channels) with arbitrary boundary conditions, which enable the mitigation of spurious singularities (Kohn anomalies). Simulations using semilocal momentum-space (SMS) regularized chiral potential at N4LO.
doi: 10.1103/PhysRevC.107.054001
2022CI08 J.Phys.(London) G49, 120502 (2022) V.Cirigliano, Z.Davoudi, J.Engel, R.J.Furnstahl, G.Hagen, U.Heinz, H.Hergert, M.Horoi, C.W.Johnson, A.Lovato, E.Mereghetti, W.Nazarewicz, A.Nicholson, T.Papenbrock, S.Pastore, M.Plumlee, D.R.Phillips, P.E.Shanahan, S.R.Stroberg, F.Viens, A.Walker-Loud, K.A.Wendt, S.M.Wild Towards precise and accurate calculations of neutrinoless double-beta decay RADIOACTIVITY 48Ca(2β-); calculated neutrinoless nuclear matrix elements using chiral-EFT interactions, EDF, IBM, QRPA, SM-pf, SM-sdpf, SM-MBPT, RSM, QMC+SM, IM-GCM, VS-IMSRG, CCSD, CCSD-T1.
doi: 10.1088/1361-6471/aca03e
2022HI05 Phys.Rev. C 106, 024616 (2022) M.A.Hisham, R.J.Furnstahl, A.J.Tropiano Renormalization group evolution of optical potentials: Explorations using a "toy" model
doi: 10.1103/PhysRevC.106.024616
2022MA63 Phys.Rev. C 106, 064002 (2022) P.Maris, R.Roth, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, T.Huther, H.Kamada, H.Krebs, H.Le, Ulf-G.Meissner, J.A.Melendez, A.Nogga, P.Reinert, R.Skibinski, J.P.Vary, H.Witala, T.Wolfgruber Nuclear properties with semilocal momentum-space regularized chiral interactions beyond N2LO NUCLEAR STRUCTURE 14,16,18,20,22,24,26O, 40,48Ca; calculated ground-state energies, point-proton radii. 4,6,8He, 6Li, 10Be, 10,12B, 12C; calculated ground state energies. 10,12B, 12C; calculated low-lying levels, J, π. Chiral EFT calculations with semilocal momentum-space regularized NN potentials up to fourth leading order N4LO. NUCLEAR REACTIONS 2H(n, X), E=70, 135, 200 MeV; calculated σ(E), σ(θ), vector- and tensor analyzing power. Comparison to experimental data.
doi: 10.1103/PhysRevC.106.064002
2022SE11 Phys.Rev. C 106, 044002 (2022) A.C.Semposki, R.J.Furnstahl, D.R.Phillips Interpolating between small- and large-g expansions using Bayesian model mixing
doi: 10.1103/PhysRevC.106.044002
2022TR02 Phys.Rev. C 106, 024324 (2022) A.J.Tropiano, S.K.Bogner, R.J.Furnstahl, M.A.Hisham Quasi-deuteron model at low renormalization group resolution NUCLEAR STRUCTURE 9Be, 12C, 16O, 40Ca, 56Fe, 118Sn, 208Pb; calculated ratios of the pn momentum distribution over the deuteron momentum distribution as a function of relative momentum. A=6-115; calculated average Levinger constant. Similarity renormalization group (SRG) transformations applied to several nucleon-nucleon interactions - AV18, Nijmegen II, CD-Bonn, SMS N4LO, and GT+ N2LO. Comparison to the data extracted from experimental results.
doi: 10.1103/PhysRevC.106.024324
2022ZH32 Phys.Rev. C 105, 064004 (2022) Fast emulation of quantum three-body scattering
doi: 10.1103/PhysRevC.105.064004
2021FU10 Few-Body Systems 62, 72 (2021) R.J.Furnstahl, H.-W.Hammer, A.Schwenk Nuclear Structure at the Crossroads
doi: 10.1007/s00601-021-01658-5
2021MA32 Phys.Rev. C 103, 054001 (2021) P.Maris, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, T.Huther, H.Kamada, H.Krebs, Ulf-G.Meissner, J.A.Melendez, A.Nogga, P.Reinert, R.Roth, R.Skibinski, V.Soloviov, K.Topolnicki, J.P.Vary, Yu.Volkotrub, H.Witala, T.Wolfgruber, for the LENPIC Collaboration Light nuclei with semilocal momentum-space regularized chiral interactions up to third order NUCLEAR STRUCTURE 3H, 3,4,6,8He, 6,7,8,9Li, 8,10Be, 10,11,12,13B, 12,13,14C, 14,15N, 16O; calculated energies of ground and excited states, S(2n) for 6He and 6Li, α+d breakup up for 6Li, and 3α breakup for 12C, energies, wave functions and radii for 3H, 3,4He. Semilocal momentum-space (SMS) regularized two- and three-nucleon forces up to third chiral order (N2LO), with the two low-energy constants entering the three-body force determined from the triton binding energy and the differential cross-section minimum in elastic nucleon-deuteron scattering. Comparison with experimental data. NUCLEAR REACTIONS 1H(polarized d, d), E=70, 140, 200, 270 MeV; 2H(p, d), (polarized p, d), E=65 MeV; calculated analyzing powers Ay(θ) and differential cross sections for elastic scattering using semilocal momentum-space (SMS) regularized two- and three-nucleon forces up to third chiral order (N2LO) three-nucleon force (3NF). Comparison with experimental data.
doi: 10.1103/PhysRevC.103.054001
2021ME07 Eur.Phys.J. A 57, 81 (2021) J.A.Melendez, R.J.Furnstahl, H.W.Griesshammer, J.A.McGovern, D.R.Phillips, M.T.Pratola Designing optimal experiments: an application to proton Compton scattering
doi: 10.1140/epja/s10050-021-00382-2
2021PH05 J.Phys.(London) G48, 072001 (2021) D.R.Phillips, R.J.Furnstahl, U.Heinz, T.Maiti, W.Nazarewicz, F.M.Nunes, M.Plumlee, M.T.Pratola, S.Pratt, F.G.Viens, S.M.Wild Get on the BAND Wagon: a Bayesian framework for quantifying model uncertainties in nuclear dynamics NUCLEAR REACTIONS 208Pb(p, p), E=30 MeV; calculated σ. Comparison with available data.
doi: 10.1088/1361-6471/abf1df
2021TR08 Phys.Rev. C 104, 034311 (2021) A.J.Tropiano, S.K.Bogner, R.J.Furnstahl Short-range correlation physics at low renormalization group resolution NUCLEAR STRUCTURE 12C, 16O, 40,48Ca, 56Fe, 208Pb; calculated proton momentum distributions for 12C, 16O, 40Ca, pp+pn/nn+np pair and pp/pn+np ratios for momentum transfer q=1.5-4.0 fm-1, percentage contributions from s-waves and selected p-waves to proton momentum distributions, short-range correlation (SRC) scaling factors and compared with experimental values. High renormalization group (RG)-resolution SRC physics incorporated at low resolution by unitary RG evolution, with weakly-correlated wave functions and simple evolved operators. Relevance to the analysis of knockout reactions such as (e, e'p) knockout reaction experiments at NIKHEF and other electron scattering facilities.
doi: 10.1103/PhysRevC.104.034311
2021WE14 Phys.Rev. C 104, 064001 (2021) S.Wesolowski, I.Svensson, A.Ekstrom, C.Forssen, R.J.Furnstahl, J.A.Melendez, D.R.Phillips Rigorous constraints on three-nucleon forces in chiral effective field theory from fast and accurate calculations of few-body observables NUCLEAR STRUCTURE 3H, 4He; calculated binding energies, rms point-proton radius of 4He, T1/2 of 3H β decay in the LO, NLO, and NNLO orders using three-nucleon force (3NF) of chiral effective field theory (χEFT), and compared with experimental values; evaluated Bayesian statistical methods for effective field theories of nuclei by using eigenvector continuation (EC) emulator.
doi: 10.1103/PhysRevC.104.064001
2021ZU01 Phys.Rev. C 103, 014325 (2021) L.Zurek, E.A.Coello Perez, S.K.Bogner, R.J.Furnstahl, A.Schwenk Comparing different density-matrix expansions for long-range pion exchange NUCLEAR STRUCTURE 16O, 48Ca, 132Sn; calculated normalized density-matrix square for 132Sn, isoscalar density distributions, and ratios of the DME-approximated and exact exchange energy contributions for Yukawa interaction for 16O, 48Ca, 132Sn, scalar-isoscalar and scalar-isovector exchange-energy integrands for Yukawa interaction in 132Sn. Density-matrix expansion (DME) with two-body scalar terms to embed long-range pion interactions into a Skyrme energy density functional.
doi: 10.1103/PhysRevC.103.014325
2020DR04 Phys.Rev.Lett. 125, 202702 (2020) C.Drischler, R.J.Furnstahl, J.A.Melendez, D.R.Phillips How Well Do We Know the Neutron-Matter Equation of State at the Densities Inside Neutron Stars? A Bayesian Approach with Correlated Uncertainties
doi: 10.1103/PhysRevLett.125.202702
2020DR05 Phys.Rev. C 102, 054315 (2020) C.Drischler, J.A.Melendez, R.J.Furnstahl, D.R.Phillips Quantifying uncertainties and correlations in the nuclear-matter equation of state
doi: 10.1103/PhysRevC.102.054315
2020FU01 Eur.Phys.J. A 56, 85 (2020) Turning the nuclear energy density functional method into a proper effective field theory: reflections
doi: 10.1140/epja/s10050-020-00095-y
2020TR02 Phys.Rev. C 102, 034005 (2020) A.J.Tropiano, S.K.Bogner, R.J.Furnstahl Operator evolution from the similarity renormalization group and the Magnus expansion
doi: 10.1103/PhysRevC.102.034005
2020ZH30 Phys.Rev.Lett. 125, 112503 (2020) X.Zhang, S.R.Stroberg, P.Navratil, C.Gwak, J.A.Melendez, R.J.Furnstahl, J.D.Holt Ab Initio Calculations of Low-Energy Nuclear Scattering Using Confining Potential Traps NUCLEAR REACTIONS 4He, 24O(n, n), E<3.5 MeV; calculated phase shifts and error bands.
doi: 10.1103/PhysRevLett.125.112503
2019ME05 Phys.Rev. C 100, 044001 (2019) J.A.Melendez, R.J.Furnstahl, D.R.Phillips, M.T.Pratola, S.Wesolowski Quantifying correlated truncation errors in effective field theory
doi: 10.1103/PhysRevC.100.044001
2019WE07 J.Phys.(London) G46, 045102 (2019) S.Wesolowski, R.J.Furnstahl, J.A.Melendez, D.R.Phillips Exploring Bayesian parameter estimation for chiral effective field theory using nucleon-nucleon phase shifts
doi: 10.1088/1361-6471/aaf5fc
2018BI08 Phys.Rev. C 98, 014002 (2018) S.Binder, A.Calci, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, T.Huther, H.Kamada, H.Krebs, P.Maris, Ulf-G.Meissner, A.Nogga, R.Roth, R.Skibinski, K.Topolnicki, J.P.Vary, K.Vobig, H.Witala, at the LENPIC Collaboration Few-nucleon and many-nucleon systems with semilocal coordinate-space regularized chiral nucleon-nucleon forces NUCLEAR REACTIONS 2H(n, n), E=5, 10, 14.1 MeV; 2H(n, 2np), E=13, 65 MeV; calculated differential σ(θ), Ay analyzing powers, nucleon and deuteron vector analyzing powers, phase shifts, polarization-transfer coefficient, breakup cross sections, and pd analyzing powers. NUCLEAR STRUCTURE 3H, 3,4He, 6Li; calculated binding energies, ground-state energies of 4He and 6Li, proton rms radii. 3H, 4,6,8He, 6,7,8,9Li, 8,9Be, 10B, 16,24O, 40,48Ca; calculated ground state energies. 3H, 3He, 6,7,8,9Li, 7,9Be, 8,9,10B, 9C; calculated magnetic dipole moments. 16,24O, 40,48Ca; calculated charge radii. Faddeev-Yakubovsky equations, with no-core configuration interaction approach, coupled-cluster (CC) theory, and in-medium similarity renormalization group (IM-SRG)methods with SCS chiral nucleon-nucleon (NN) potentials. Comparison with experimental values, and with other theoretical predictions.
doi: 10.1103/PhysRevC.98.014002
2018NA11 Phys.Rev. C 97, 054304 (2018) R.Navarro-Perez, N.Schunck, A.Dyhdalo, R.J.Furnstahl, S.K.Bogner Microscopically based energy density functionals for nuclei using the density matrix expansion. II. Full optimization and validation ATOMIC MASSES N=10-160; calculated binding energies of even-even nuclei, and compared with measured values from AME-2016. NUCLEAR STRUCTURE N=10-160; calculated proton radii using the UNEDF2 and NLOΔ+3N functionals, and compared with experimental data. 208Pb; calculated neutron single particle levels using energy density functions (EDFs) from NN and 3N forces with and without Δ excitation. 240Pu; calculated deformation potential energy surface, excitation energy of the fission isomer, and height of the first and second fission barriers using LO, NLO, N2LO, N2LO+3N, NLOΔ, NLOΔ+3N, N2LOΔ, and N2LOΔ+3N energy density functionals, and compared with experimental values.
doi: 10.1103/PhysRevC.97.054304
2018ZH57 Phys.Rev. C 98, 064306 (2018) Y.N.Zhang, S.K.Bogner, R.J.Furnstahl Incorporating Brueckner-Hartree-Fock correlations in energy density functionals
doi: 10.1103/PhysRevC.98.064306
2017DY02 Phys.Rev. C 95, 054314 (2017) A.Dyhdalo, S.K.Bogner, R.J.Furnstahl Applying the density matrix expansion with coordinate-space chiral interactions
doi: 10.1103/PhysRevC.95.054314
2017DY04 Phys.Rev. C 96, 054005 (2017) A.Dyhdalo, S.K.Bogner, R.J.Furnstahl Estimates and power counting in uniform nuclear matter with softened interactions
doi: 10.1103/PhysRevC.96.054005
2017HO24 Phys.Rev. C 96, 054002 (2017) J.Hoppe, C.Drischler, R.J.Furnstahl, K.Hebeler, A.Schwenk Weinberg eigenvalues for chiral nucleon-nucleon interactions
doi: 10.1103/PhysRevC.96.054002
2017ME09 Phys.Rev. C 96, 024003 (2017) J.A.Melendez, S.Wesolowski, R.J.Furnstahl Bayesian truncation errors in chiral effective field theory: Nucleon-nucleon observables
doi: 10.1103/PhysRevC.96.024003
2017MO39 Phys.Rev. C 96, 054004 (2017) S.N.More, S.K.Bogner, R.J.Furnstahl Scale dependence of deuteron electrodisintegration NUCLEAR STRUCTURE 2H; calculated initial deuteron wave function, current operator, and the final-state interactions (FSIs) and their combinations at different scales using similarity renormalization group (SRG) for each component of deuteron electro-disintegration for example in 2H(e, e'p)n. Relevance to scale dependence in nuclear knock-out reactions.
doi: 10.1103/PhysRevC.96.054004
2016BI06 Phys.Rev. C 93, 044002 (2016) S.Binder, A.Calci, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, H.Kamada, H.Krebs, J.Langhammer, S.Liebig, P.Maris, Ulf-G.Meissner, D.Minossi, A.Nogga, H.Potter, R.Roth, R.Skibinski, K.Topolnicki, J.P.Vary, H.Witala, for the LENPIC Collaboration Few-nucleon systems with state-of-the-art chiral nucleon-nucleon forces NUCLEAR STRUCTURE 3H, 4He, 6Li; calculated energies of ground-state and lowest two states, point-proton radius using improved NN chiral potentials LO, NLO, N2LO, N3LO and N4LO. Comparison with experimental data. NUCLEAR REACTIONS 3H, 4He, 6Li(d, X), (polarized d, d), E=10, 70, 135, 200 MeV; total σ(E), differential cross section and tensor analyzing powers for elastic scattering based on NN chiral potentials LO, NLO, N2LO, N3LO and N4LO. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.044002
2016DY01 Phys.Rev. C 94, 034001 (2016) A.Dyhdalo, R.J.Furnstahl, K.Hebeler, I.Tews Regulator artifacts in uniform matter for chiral interactions
doi: 10.1103/PhysRevC.94.034001
2015FU10 Phys.Rev. C 92, 024005 (2015) R.J.Furnstahl, N.Klco, D.R.Phillips, S.Wesolowski Quantifying truncation errors in effective field theory
doi: 10.1103/PhysRevC.92.024005
2015MO26 Phys.Rev. C 92, 064002 (2015) S.N.More, S.Konig, R.J.Furnstahl, K.Hebeler Deuteron electrodisintegration with unitarily evolved potentials NUCLEAR REACTIONS 2H(e, X), E not given; calculated momentum distributions for various potentials. Electrodisintegration of deuteron. Similarity renormalization-group (SRG) method for investigation of RG evolution of structure and reaction components. Unitary transformation matrices.
doi: 10.1103/PhysRevC.92.064002
2014DA03 Phys.Rev. C 89, 014001 (2014) B.Dainton, R.J.Furnstahl, R.J.Perry Universality in similarity renormalization group evolved potential matrix elements and T-matrix equivalence
doi: 10.1103/PhysRevC.89.014001
2014FU03 Phys.Rev. C 89, 044301 (2014) R.J.Furnstahl, S.N.More, T.Papenbrock Systematic expansion for infrared oscillator basis extrapolations
doi: 10.1103/PhysRevC.89.044301
2014KO46 Phys.Rev. C 90, 064007 (2014) S.Konig, S.K.Bogner, R.J.Furnstahl, S.N.More, T.Papenbrock Ultraviolet extrapolations in finite oscillator bases NUCLEAR STRUCTURE 2H; calculated relative error in the deuteron energy, computed in harmonic-oscillator bases for a wide range of oscillator parameters, infrared (IR) and ultraviolet (UV) corrections and extrapolations in finite oscillator, comparison of UV extrapolations for a deuteron state bases for different potentials.
doi: 10.1103/PhysRevC.90.064007
2013BO19 Comput.Phys.Commun. 184, 085101 (2013) S.Bogner, A.Bulgac, J.Carlson, J.Engel, G.Fann, R.J.Furnstahl, S.Gandolfi, G.Hagen, M.Horoi, C.Johnson, M.Kortelainen, E.Lusk, P.Maris, H.Nam, P.Navratil, W.Nazarewicz, E.Ng, G.P.A.Nobre, E.Ormand, T.Papenbrock, J.Pei, S.C.Pieper, S.Quaglioni, K.J.Roche, J.Sarich, N.Schunck, M.Sosonkina, J.Terasaki, I.Thompson, J.P.Vary, S.M.Wild Computational nuclear quantum many-body problem: The UNEDF project NUCLEAR REACTIONS 3He(d, p), 7Be(p, γ), E<1MeV; 172Yb, 188Os, 238U(γ, X), E<24 MeV; calculated σ. Comparison with experimental data. NUCLEAR STRUCTURE 100Zr; calculated quadrupole deformation parameter, radii, neutron separation energy.
doi: 10.1016/j.cpc.2013.05.020
2013HE06 Phys.Rev. C 87, 031302 (2013) Neutron matter based on consistently evolved chiral three-nucleon interactions
doi: 10.1103/PhysRevC.87.031302
2013JU01 Phys.Rev. C 87, 054312 (2013) E.D.Jurgenson, P.Maris, R.J.Furnstahl, P.Navratil, W.E.Ormand, J.P.Vary Structure of p-shell nuclei using three-nucleon interactions evolved with the similarity renormalization group NUCLEAR STRUCTURE 3H, 4He, 7Li, 8Be, 10B, 12C; calculated ground-state and low-lying levels, J, π. 7Li, 7Be, 10B; calculated magnetic dipole moments of ground states and low-lying states. No-core full configuration (NCFC) and similarity renormalization group (SRG) ab initio calculations for p-shell nuclei. Assessment of convergence properties, extrapolation techniques, and dependence of energies, including four-body contributions. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.054312
2013MO11 Phys.Rev. C 87, 044326 (2013) S.N.More, A.Ekstrom, R.J.Furnstahl, G.Hagen, T.Papenbrock Universal properties of infrared oscillator basis extrapolations
doi: 10.1103/PhysRevC.87.044326
2012FU08 Phys.Rev. C 86, 031301 (2012) R.J.Furnstahl, G.Hagen, T.Papenbrock Corrections to nuclear energies and radii in finite oscillator spaces NUCLEAR STRUCTURE 6He, 16O; calculated ground-state energies, nuclear radii. Finite oscillator basis space. Halo nuclei. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.86.031301
2012WE06 Phys.Rev. C 86, 014003 (2012) K.A.Wendt, R.J.Furnstahl, S.Ramanan Local projections of low-momentum potentials
doi: 10.1103/PhysRevC.86.014003
2011BO22 Phys.Rev. C 84, 044306 (2011) S.K.Bogner, R.J.Furnstahl, H.Hergert, M.Kortelainen, P.Maris, M.Stoitsov, J.P.Vary Testing the density matrix expansion against ab initio calculations of trapped neutron drops
doi: 10.1103/PhysRevC.84.044306
2011HE06 Phys.Rev. C 83, 031301 (2011) K.Hebeler, S.K.Bogner, R.J.Furnstahl, A.Nogga, A.Schwenk Improved nuclear matter calculations from chiral low-momentum interactions
doi: 10.1103/PhysRevC.83.031301
2011JU02 Phys.Rev. C 83, 034301 (2011) E.D.Jurgenson, P.Navratil, R.J.Furnstahl Evolving nuclear many-body forces with the similarity renormalization group NUCLEAR STRUCTURE 3H, 4He, 6Li; calculated Ground state energies. 6Li; calculated levels, J, π, rms radius, quadrupole moment, B(M1), B(E2). Similarity Renormalization Group method. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.034301
2011LI46 Phys.Rev. C 84, 054002 (2011) W.Li, E.R.Anderson, R.J.Furnstahl Similarity renormalization group with novel generators
doi: 10.1103/PhysRevC.84.054002
2011WE03 Phys.Rev. C 83, 034005 (2011) K.A.Wendt, R.J.Furnstahl, R.J.Perry Decoupling of spurious deeply bound states with the similarity renormalization group
doi: 10.1103/PhysRevC.83.034005
2010AN14 Phys.Rev. C 82, 054001 (2010) E.R.Anderson, S.K.Bogner, R.J.Furnstahl, R.J.Perry Operator evolution via the similarity renormalization group: The deuteron
doi: 10.1103/PhysRevC.82.054001
2010KO22 Phys.Rev. C 82, 011304 (2010) M.Kortelainen, R.J.Furnstahl, W.Nazarewicz, M.V.Stoitsov Natural units for nuclear energy density functional theory
doi: 10.1103/PhysRevC.82.011304
2010ST12 Phys.Rev. C 82, 054307 (2010) M.Stoitsov, M.Kortelainen, S.K.Bogner, T.Duguet, R.J.Furnstahl, B.Gebremariam, N.Schunck Microscopically based energy density functionals for nuclei using the density matrix expansion: Implementation and pre-optimization NUCLEAR STRUCTURE 40Ca, 208Pb; calculated kinetic energies for neutrons and protons, surface, volume and total energies, single-particle neutron and proton energies. 54,56,58,60,62,64,66Ni, 68Ni, 70,72,74,76,78,80,82,84,86,88,90,92Ni; calculated two-neutron separation energies, neutron rms radii, and average neutron pairing gaps. 100Zr; calculated deformation energy. 40,42,44,46,48Ca; calculated proton rms radii. Energy density functionals SLy4' and density matrix expansion (DME) in LO, NLO and N2LO.
doi: 10.1103/PhysRevC.82.054307
2009BO05 Eur.Phys.J. A 39, 219 (2009) S.K.Bogner, R.J.Furnstahl, L.Platter Density matrix expansion for low-momentum interactions
doi: 10.1140/epja/i2008-10695-1
2009JU01 Nucl.Phys. A818, 152 (2009) Similarity renormalization group evolution of many-body forces in a one-dimensional model NUCLEAR STRUCTURE A=2, 3, 4; calculated ground state energies with a no-core shell model.
doi: 10.1016/j.nuclphysa.2008.12.007
2009JU03 Phys.Rev.Lett. 103, 082501 (2009) E.D.Jurgenson, P.Navratil, R.J.Furnstahl Evolution of Nuclear Many-Body Forces with the Similarity Renormalization Group NUCLEAR STRUCTURE 3H, 4He; calculated ground-state and binding energies. Similarity renormalization group, NNN potential.
doi: 10.1103/PhysRevLett.103.082501
2008AN02 Phys.Rev. C 77, 037001 (2008) E.Anderson, S.K.Bogner, R.J.Furnstahl, E.D.Jurgenson, R.J.Perry, A.Schwenk Block diagonalization using similarity renormalization group flow equations
doi: 10.1103/PhysRevC.77.037001
2008BO07 Nucl.Phys. A801, 21 (2008) S.K.Bogner, R.J.Furnstahl, P.Maris, R.J.Perry, A.Schwenk, J.P.Vary Convergence in the no-core shell model with low-momentum two-nucleon interactions NUCLEAR STRUCTURE 2,3H, 4,6He, 6,7Li; calculated ground/excited state energies with no core shell model using similarity renormalization group interactions.
doi: 10.1016/j.nuclphysa.2007.12.008
2008JU05 Phys.Rev. C 78, 014003 (2008) E.D.Jurgenson, S.K.Bogner, R.J.Furnstahl, R.J.Perry Decoupling in the similarity renormalization group for nucleon-nucleon forces NUCLEAR STRUCTURE 2H; calculated rms radius. 4He, 6Li; calculated ground state energies. No-core shell model.
doi: 10.1103/PhysRevC.78.014003
2007BO03 Nucl.Phys. A784, 79 (2007) S.K.Bogner, R.J.Furnstahl, S.Ramanan, A.Schwenk Low-momentum interactions with smooth cutoffs NUCLEAR STRUCTURE 2,3H; calculated binding energies, radii, wave functions. Low-momentum interactions with smooth cutoffs.
doi: 10.1016/j.nuclphysa.2006.11.123
2007BO20 Phys.Rev. C 75, 061001 (2007) S.K.Bogner, R.J.Furnstahl, R.J.Perry Similarity renormalization group for nucleon-nucleon interactions
doi: 10.1103/PhysRevC.75.061001
2007BO36 Phys.Lett. B 649, 488 (2007) S.K.Bogner, R.J.Furnstahl, R.J.Perry, A.Schwenk Are low-energy nuclear observables sensitive to high-energy phase shifts? NUCLEAR STRUCTURE 2H; calculated binding energies, wave functions, phase shifts. Low-momentum interactions with smooth cutoffs. Similarity renormalization group.
doi: 10.1016/j.physletb.2007.04.048
2007RA29 Nucl.Phys. A797, 81 (2007) S.Ramanan, S.K.Bogner, R.J.Furnstahl Weinberg eigenvalues and pairing with low-momentum potentials
doi: 10.1016/j.nuclphysa.2007.10.005
2006BO03 Phys.Lett. B 632, 501 (2006) Variational calculations of nuclei with low-momentum potentials NUCLEAR STRUCTURE 2,3H; calculated wave functions. Low-momentum potentials.
doi: 10.1016/j.physletb.2005.10.094
2006BO19 Nucl.Phys. A773, 203 (2006) S.K.Bogner, R.J.Furnstahl, S.Ramanan, A.Schwenk Convergence of the Born series with low-momentum interactions
doi: 10.1016/j.nuclphysa.2006.05.004
2005BH01 Nucl.Phys. A747, 268 (2005) A.Bhattacharyya, R.J.Furnstahl The kinetic energy density in Kohn-Sham density functional theory
doi: 10.1016/j.nuclphysa.2004.10.008
2005BH03 Phys.Lett. B 607, 259 (2005) A.Bhattacharyya, R.J.Furnstahl Single-particle properties from Khon-Sham Green's Functions
doi: 10.1016/j.physletb.2004.12.056
2005BO48 Nucl.Phys. A763, 59 (2005) S.K.Bogner, A.Schwenk, R.J.Furnstahl, A.Nogga Is nuclear matter perturbative with low-momentum interactions?
doi: 10.1016/j.nuclphysa.2005.08.024
2005FU08 J.Phys.(London) G31, S1357 (2005) Density functional theory: methods and problems
doi: 10.1088/0954-3899/31/8/014
2004FU09 Nucl.Phys. A737, 215 (2004) Three-Body Interactions in Many-Body Effective Field Theory
doi: 10.1016/j.nuclphysa.2004.03.079
2003PU04 Nucl.Phys. A723, 145 (2003) S.J.Puglia, A.Bhattacharyya, R.J.Furnstahl Density functional theory for a confined Fermi system with short-range interaction
doi: 10.1016/S0375-9474(03)01161-8
2002FU06 Phys.Lett. 531B, 203 (2002) Are Occupation Numbers Observable ?
doi: 10.1016/S0370-2693(01)01504-0
2002FU08 Nucl.Phys. A706, 85 (2002) Neutron Radii in Mean-Field Models NUCLEAR STRUCTURE 208Pb; calculated neutron radius, skin thickness vs several mean-field model parameters.
doi: 10.1016/S0375-9474(02)00867-9
2001FU08 Nucl.Phys. A689, 846 (2001) R.J.Furnstahl, H.-W.Hammer, N.Tirfessa Field Redefinitions at Finite Density
doi: 10.1016/S0375-9474(00)00687-4
2000FU02 Nucl.Phys. A663-664, 513c (2000) Effective Field Theory and Nuclear Mean-Field Models
doi: 10.1016/S0375-9474(99)00644-2
2000FU03 Nucl.Phys. A671, 396 (2000) R.J.Furnstahl, J.V.Steele, N.Tirfessa Perturbative Effective Field Theory at Finite Density
doi: 10.1016/S0375-9474(99)00824-6
2000FU04 Nucl.Phys. A671, 447 (2000) Parameter Counting in Relativistic Mean-Field Models NUCLEAR STRUCTURE 16O, 208Pb; calculated energy contributions from relativistic mean field model terms; deduced parameter constraints, related features.
doi: 10.1016/S0375-9474(99)00839-8
2000FU07 Nucl.Phys. A673, 298 (2000) Large Lorentz Scalar and Vector Potentials in Nuclei
doi: 10.1016/S0375-9474(00)00146-9
2000HA49 Nucl.Phys. A678, 277 (2000) Effective Field Theory for Dilute Fermi Systems
doi: 10.1016/S0375-9474(00)00325-0
2000ST15 Nucl.Phys. A663-664, 999c (2000) Describing Nuclear Matter with Effective Field Theories
doi: 10.1016/S0375-9474(99)00753-8
1999ST02 Nucl.Phys. A645, 439 (1999) Removing Pions from Two-Nucleon Effective Field Theory
doi: 10.1016/S0375-9474(98)00619-8
1998CL04 Phys.Lett. 427B, 231 (1998); Erratum Phys.Lett. 486B, 272 (2000) B.C.Clark, R.J.Furnstahl, L.Kurth Kerr, J.Rusnak, S.Hama Pion-Nucleus Scattering at Medium Energies with Densities from Chiral Effective Field Theories NUCLEAR REACTIONS 208Pb(π+, π+), (π-, π-), E at 790 MeV/c; calculated σ(θ). Relativistic point-coupling models, mean-field meson models. Comparison with data.
doi: 10.1016/S0370-2693(98)00352-9
1998FU04 Nucl.Phys. A632, 607 (1998) R.J.Furnstahl, J.J.Rusnak, B.D.Serot The Nuclear Spin-Orbit Force in Chiral Effective Field Theories NUCLEAR STRUCTURE 16O, 40Ca, 208Pb; analyzed spin-orbit splitting; deduced role of tensor couplings of vector mesons.
doi: 10.1016/S0375-9474(98)00004-9
1998ST11 Nucl.Phys. A637, 46 (1998) Regularization Methods for Nucleon-Nucleon Effective Field Theory
doi: 10.1016/S0375-9474(98)00219-X
1997FU03 Nucl.Phys. A615, 441 (1997); Erratum Nucl.Phys. A640, 505 (1998) R.J.Furnstahl, B.D.Serot, H.-B.Tang A Chiral Effective Lagrangian for Nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 88Sr, 208Pb; calculated binding energies, charge densities, form factors. Quantum chromodynamics approach, chiral effective hadronic lagrangian.
doi: 10.1016/S0375-9474(96)00472-1
1997FU05 Nucl.Phys. A618, 446 (1997) R.J.Furnstahl, B.D.Serot, H.-B.Tang Vacuum Nucleon Loops and Naturalness
doi: 10.1016/S0375-9474(97)00062-6
1997FU09 Phys.Rev. C56, 2875 (1997) Skyrme Energy Functional and Naturalness
doi: 10.1103/PhysRevC.56.2875
1997RU09 Nucl.Phys. A627, 495 (1997) Relativistic Point-Coupling Models as Effective Theories of Nuclei
doi: 10.1016/S0375-9474(97)00598-8
1996FU02 Nucl.Phys. A598, 539 (1996) R.J.Furnstahl, B.D.Serot, H.-B.Tang Analysis of Chiral Mean-Field Models for Nuclei NUCLEAR STRUCTURE 208Pb; calculated charge density, form factors. Chiral mean-field models.
doi: 10.1016/0375-9474(95)00488-2
1996FU19 Phys.Lett. 387B, 253 (1996) R.J.Furnstahl, X.Jin, D.B.Leinweber New QCD Sum Rules for Nucleons in Nuclear Matter
doi: 10.1016/0370-2693(96)01043-X
1995FU06 Phys.Rev. C52, 1368 (1995) R.J.Furnstahl, J.-B.Tang, B.D.Serot Vacuum Contributions in a Chiral Effective Lagrangian for Nuclei NUCLEAR STRUCTURE 16O, 40Ca, 208Pb; calculated rms charge radii, charge density, binding energy systematics. Relativistic hadronic model.
doi: 10.1103/PhysRevC.52.1368
1995JI07 Nucl.Phys. A585, 333c (1995) X.Jin, R.J.Furnstahl, M.Nielsen QCD Sum Rules for Hyperons in Nuclear Matter
doi: 10.1016/0375-9474(94)00593-C
1995RU08 Z.Phys. A352, 345 (1995) Two-Point Fermion Correlation Functions at Finite Density
doi: 10.1007/BF01289507
1994FU07 Phys.Rev. C50, 1735 (1994) Spectral Asymmetries in Nucleon Sum Rules at Finite Density
doi: 10.1103/PhysRevC.50.1735
1994JI01 Phys.Rev. C49, 1190 (1994) QCD Sum Rule for (Lambda) Hyperons in Nuclear Matter
doi: 10.1103/PhysRevC.49.1190
1993FU03 Phys.Rev. C47, 2338 (1993) Finite Nuclei in Relativistic Models with a Light Chiral Scalar Meson NUCLEAR STRUCTURE 40Ca, 208Pb; calculated charge density. 208Pb; calculated proton single-particle spectrum. Different mean field models, light chiral scalar meson.
doi: 10.1103/PhysRevC.47.2338
1993FU04 Phys.Rev. C47, 2812 (1993) Effective Interaction for Inelastic Proton Scattering Based on the Relativistic Impulse Approximation NUCLEAR REACTIONS 40Ca(polarized p, p), E=300 MeV; analyzed σ(θ), polarization, spin rotation parameter vs θ. Relativistic impulse approximation, density dependent effective interaction.
doi: 10.1103/PhysRevC.47.2812
1993FU08 Phys.Lett. 316B, 12 (1993) Finite Nuclei in a Relativistic Model with Broken Chiral and Scale Invariance NUCLEAR STRUCTURE 208Pb; calculated charge density, proton single particle spectra. Relativistic hadronic model, broken chiral, scale invariances.
doi: 10.1016/0370-2693(93)90649-3
1991CO02 Phys.Rev. C43, 357 (1991) T.D.Cohen, R.J.Furnstahl, M.K.Banerjee In-Medium Proton-Neutron Mass Difference and the Systematics of the Nolen-Schiffer Anomaly NUCLEAR STRUCTURE 17,15O, 17F, 39K, 39,41Ca, 41Sc; analyzed Nolen-Schiffer anomaly; deduced in-medium n-p mass difference role.
doi: 10.1103/PhysRevC.43.357
1991FU04 Phys.Rev. C44, 895 (1991) Charge Density Differences Near 208Pb in Relativistic Models NUCLEAR STRUCTURE 206Pb, 205Tl, 204Hg; calculated charge density differences, σ ratios. Relativistic mean field models.
doi: 10.1103/PhysRevC.44.895
1990DA14 Phys.Rev. C42, 2009 (1990) Relativistic Spectral Random-Phase Approximation in Finite Nuclei NUCLEAR STRUCTURE 16O; calculated levels, transition charge to current density ratios, form factors. Relativistic spectral RPA. NUCLEAR REACTIONS 12C, 16O, 40Ca(e, e'), E not given; calculated longitudinal, transverse form factors. Relativistic spectral RPA.
doi: 10.1103/PhysRevC.42.2009
1990FU04 Phys.Rev. C41, 1792 (1990) Vacuum Polarization Currents in Finite Nuclei NUCLEAR STRUCTURE A=15, 17, 39, 41; calculated isoscalar magnetic moment. 15N, 209Bi; calculated magnetic form factor.
doi: 10.1103/PhysRevC.41.1792
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