NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = S.Bogner Found 55 matches. 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
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
2022YA19 Phys.Rev. C 106, 014315 (2022) J.M.Yao, I.Ginnett, A.Belley, T.Miyagi, R.Wirth, S.Bogner, J.Engel, H.Hergert, J.D.Holt, S.R.Stroberg Ab initio studies of the double-Gamow-Teller transition and its correlation with neutrinoless double-β decay RADIOACTIVITY 6,8He, 10Be, 14C, 18,22O, 22Ne, 26,28Mg, 30Si, 34S, 38Ar, 42,44,48,56Ca, 50Cr, 46,52Ti(2β-); A=6-76(2β-); calculated nuclear matrix elements (NMEs) for ground-state-to-ground-state double Gamow-Teller transitions (DGT) and Gamow Teller (GT) 0νββ decay, transition densities of parent nuclei, correlation between the transition densities and NMEs of DGT transitions. Ab initio many body methods by importance-truncated no-core shell model (IT-NCSM) with GXPF1A interaction, valence-space in-medium similarity renormalization group method (VSIMSRG) with EM1.8/2.0 interaction, and in-medium generator coordinate method (IM-GCM). 6He, 10Be, 14C, 18O, 22Ne, 26Mg, 30Si, 34S, 38Ar, 42,44Ca, 46Ti, 50Cr; 2β- decay mode forbidden for these nuclei due to negative Q values, however, on query, authors mentioned that these nuclei were included for NMEs for 0νββ decays as these involved the same decay operators that determine the allowed decay rates, thus helpful to benchmark many-body approaches for the nuclear matrix elements of neutrinoless double beta decay.
doi: 10.1103/PhysRevC.106.014315
2021LE13 Phys.Rev.Lett. 127, 062501 (2021) D.Lee, S.Bogner, B.A.Brown, S.Elhatisari, E.Epelbaum, H.Hergert, M.Hjorth-Jensen, H.Krebs, N.Li, B.-N.Lu, U.-G.Meissner Hidden Spin-Isospin Exchange Symmetry
doi: 10.1103/PhysRevLett.127.062501
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
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
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
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
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
2017PA09 Phys.Rev. C 95, 044304 (2017) N.M.Parzuchowski, T.D.Morris, S.K.Bogner Ab initio excited states from the in-medium similarity renormalization group NUCLEAR STRUCTURE 16,22O; calculated low-lying levels using ab initio approach within the in-medium similarity renormalization group (IMSRG) framework, and Tamm-Dancoff approximation (TDA) with equations-of-motion (EOM) techniques.
doi: 10.1103/PhysRevC.95.044304
2017PA26 Phys.Rev. C 96, 034324 (2017) N.M.Parzuchowski, S.R.Stroberg, P.Navratil, H.Hergert, S.K.Bogner Ab initio electromagnetic observables with the in-medium similarity renormalization group NUCLEAR STRUCTURE 14C; calculated energies of the ground state and first 2+ state, B(E2) for the first 2+ state. 2H; calculated energy, magnetic dipole moment, electric quadrupole moment and charge radius of the ground state. 6Li; calculated energies of ground-state and first 3+ state, quadrupole moments, B(M1), B(E2). 6He, 14C, 22O, 32S, 48Ca, 56,60Ni; calculated energies and B(E2) of first 2+ states. 14N; calculated energy and B(M1) of the first excited 0+ state. 32S, 32Cl; calculated energies, B(M1) and magnetic-dipole moments of first 1+ states. 16O, 40Ca; calculated energies and B(E3) of first 3- states. 14C, 22O, 32S; calculated E2 and M1 transition matrix elements. Equations-of-motion in-medium similarity renormalization group (EOM-IMSRG), and valence-space VS-IMSRG methods. Comparison with available experimental values, and theoretical calculations from no-core shell-model.
doi: 10.1103/PhysRevC.96.034324
2017ST03 Phys.Rev.Lett. 118, 032502 (2017) S.R.Stroberg, A.Calci, H.Hergert, J.D.Holt, S.K.Bogner, R.Roth, A.Schwenk Nucleus-Dependent Valence-Space Approach to Nuclear Structure NUCLEAR STRUCTURE 16,18,22O, 10B, 22Na, 46V, C, N, O, Na, Ca, Ni; calculated ground-state energies, J, π, the extension of ab initio nuclear structure calculations.
doi: 10.1103/PhysRevLett.118.032502
2016ST12 Phys.Rev. C 93, 051301 (2016) S.R.Stroberg, H.Hergert, J.D.Holt, S.K.Bogner, A.Schwenk Ground and excited states of doubly open-shell nuclei from ab initio valence-space Hamiltonians NUCLEAR STRUCTURE 19,23,25,26F, 20,22,24,25,26Ne, 24Mg; calculated levels, J, π, yrast states from ab initio in-medium similarity renormalization group (IM-SRG) Hamiltonians based on NN+3N-induced and NN+3N-full Hamiltonians. Comparison with experimental data, and with phenomenological USDB predictions. 17,18,19,20,21,22,23,24,25,26,27,28,29F, 18,19,20,21,22,23,24,25,26,27,28,29,30Ne; calculated ground-state energies from the A-dependent IM-SRG valence-space Hamiltonian. Comparison with AME-2012 values, and the phenomenological USDB interaction.
doi: 10.1103/PhysRevC.93.051301
2015CA09 Phys.Rev. C 92, 014327 (2015) L.Caceres, A.Lepailleur, O.Sorlin, M.Stanoiu, D.Sohler, Zs.Dombradi, S.K.Bogner, B.A.Brown, H.Hergert, J.D.Holt, A.Schwenk, F.Azaiez, B.Bastin, C.Borcea, R.Borcea, C.Bourgeois, Z.Elekes, Zs.Fulop, S.Grevy, L.Gaudefroy, G.F.Grinyer, D.Guillemaud-Mueller, F.Ibrahim, A.Kerek, A.Krasznahorkay, M.Lewitowicz, S.M.Lukyanov, J.Mrazek, F.Negoita, F.de Oliveira, Yu.-E.Penionzhkevich, Zs.Podolyak, M.G.Porquet, F.Rotaru, P.Roussel-Chomaz, M.G.Saint-Laurent, H.Savajols, G.Sletten, J.C.Thomas, J.Timar, C.Timis, Zs.Vajta Nuclear structure studies of 24F NUCLEAR REACTIONS 9Be(36S, X)24O/26F/27Ne/28Ne/29Na/30Na, E=77.6 MeV/nucleon; measured energy loss, TOF, yields using LISE achromatic spectrometer at GANIL facility. C(27Na, 24F), E=54-65 MeV/nucleon, [secondary cocktail beam of 25,26Ne, 27,28Na, 29,30Mg from C(36S, X), E=77.6 MeV/nucleon primary reaction, and separated using ALPHA and SPEG spectrometers]; measured Eγ, Iγ, (particle)γ-, γγ-coin using Chateau de Cristal array. 24F; deduced levels, J, π, branching ratios, configurations. Comparison with shell-model calculations using USDA and USDB interactions, and ab initio shell-model calculations, using interactions derived from chiral NN+3N forces by means of IM-SRG. RADIOACTIVITY 24O(β-), (β-n)[from Be(36S, X), E=77.6 MeV/nucleon using LISE spectrometer at GANIL]; measured Eγ, Iγ, Eβ, βγ-, γγ-coin, (24O)β-correlations, half-life of 24O isotope from (24O)γ-correlated decay curve, β-delayed neutron emission probability Pn using four segmented Ge clover detectors of EXOGAM array for γ rays and DSSSDs for particles. 24F; deduced levels, J, π, branching ratios, β feedings, logft. Comparison with shell-model calculations.
doi: 10.1103/PhysRevC.92.014327
2015MO19 Phys.Rev. C 92, 034331 (2015) T.D.Morris, N.M.Parzuchowski, S.K.Bogner Magnus expansion and in-medium similarity renormalization group NUCLEAR STRUCTURE 16O; calculated energy of the ground-state of 16O and that of homogeneous electron gas (HEG) using an improved variant of the in-medium similarity renormalization group (IM-SRG) based on the Magnus expansion and a first-order Euler method. Substantial memory savings and modest computational speedups.
doi: 10.1103/PhysRevC.92.034331
2014BO25 Phys.Rev.Lett. 113, 142501 (2014) S.K.Bogner, H.Hergert, J.D.Holt, A.Schwenk, S.Binder, A.Calci, J.Langhammer, R.Roth Nonperturbative Shell-Model Interactions from the In-Medium Similarity Renormalization Group NUCLEAR STRUCTURE 21,22,23,24,25,26O; calculated energy levels, J, π. Comparison with experimental data.
doi: 10.1103/PhysRevLett.113.142501
2014HE23 Phys.Rev. C 90, 041302 (2014) H.Hergert, S.K.Bogner, T.D.Morris, S.Binder, A.Calci, J.Langhammer, R.Roth Ab initio multireference in-medium similarity renormalization group calculations of even calcium and nickel isotopes NUCLEAR STRUCTURE 34,36,38,40,42,44,46,48,50,52,54,56,58,60,62Ca, 48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86,88,90Ni; calculated ground state energies, and S(2n) using multireference in-medium similarity renormalization group based on NN+3N nucleon interactions from chiral effective field theory. Comparison with other calculations and experimental results.
doi: 10.1103/PhysRevC.90.041302
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
2014SH22 Phys.Rev. C 90, 024324 (2014) A.M.Shirokov, A.G.Negoita, J.P.Vary, S.K.Bogner, A.I.Mazur, E.A.Mazur, D.Gogny Properties of nuclear matter within the JISP16 NN interaction
doi: 10.1103/PhysRevC.90.024324
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
2013HE07 Phys.Rev. C 87, 034307 (2013) H.Hergert, S.K.Bogner, S.Binder, A.Calci, J.Langhammer, R.Roth, A.Schwenk In-medium similarity renormalization group with chiral two- plus three-nucleon interactions NUCLEAR STRUCTURE 4He, 16,24O, 40,48Ca, 48,56Ni; calculated ground states energies, and binding energies using the in-medium similarity renormalization group (IM-SRG), based on chiral two- plus three-nucleon interactions. Comparison with coupled cluster calculations, truncated no-core shell model, and with experimental data.
doi: 10.1103/PhysRevC.87.034307
2012BO18 Phys.Rev. C 86, 064304 (2012) High-momentum tails from low-momentum effective theories
doi: 10.1103/PhysRevC.86.064304
2012TS02 Phys.Rev. C 85, 061304 (2012) K.Tsukiyama, S.K.Bogner, A.Schwenk In-medium similarity renormalization group for open-shell nuclei NUCLEAR STRUCTURE 6Li, 18O; calculated level energies using the in-medium similarity renormalization group (IM-SRG) approach. Comparison with experimental data, and other theoretical studies.
doi: 10.1103/PhysRevC.85.061304
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
2011GE02 Nucl.Phys. A851, 17 (2011) B.Gebremariam, S.K.Bogner, T.Duguet Microscopically-constrained Fock energy density functionals from chiral effective field theory. I. Two-nucleon interactions
doi: 10.1016/j.nuclphysa.2010.12.009
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
2011TS05 Phys.Rev.Lett. 106, 222502 (2011) K.Tsukiyama, S.K.Bogner, A.Schwenk In-Medium Similarity Renormalization Group For Nuclei NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated ground-state energies, two-body matrix elements. Ab initio calculations.
doi: 10.1103/PhysRevLett.106.222502
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
2010GE02 Phys.Rev. C 82, 014305 (2010) B.Gebremariam, T.Duguet, S.K.Bogner Improved density matrix expansion for spin-unsaturated nuclei NUCLEAR STRUCTURE 46,64,80Cr, 102,114,132Sn, 180,198,214Pb; calculated quadrupole anisotropy. Z=24, A=44-82; Z=50, A=100-132; Z=82, A=176-214; calculated energy density expansions for even-even nuclei. Nuclear energy density functionals.
doi: 10.1103/PhysRevC.82.014305
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
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
2008DE04 Phys.Rev. C 77, 024002 (2008) A.Deltuva, A.C.Fonseca, S.K.Bogner Low-momentum interactions in three- and four-nucleon scattering NUCLEAR REACTIONS 2H(n, n), E=13 MeV; calculated binding energy, σ(θ), analyzing power. 3H(n, n), E=3.5 MeV; calculated cross sections, neutron analyzing power.
doi: 10.1103/PhysRevC.77.024002
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
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
2005HO29 Phys.Rev. C 72, 041304 (2005) J.D.Holt, J.W.Holt, T.T.S.Kuo, G.E.Brown, S.K.Bogner Low momentum shell model effective interactions with all-order core polarizations NUCLEAR STRUCTURE 18O, 18F; calculated levels, J, π. All-order summation of core-polarization diagrams.
doi: 10.1103/PhysRevC.72.041304
2004HO05 Nucl.Phys. A733, 153 (2004) J.D.Holt, T.T.Kuo, G.E.Brown, S.K.Bogner Counter terms for low momentum nucleon-nucleon interactions
doi: 10.1016/j.nuclphysa.2003.12.004
2004LU15 Phys.Rev. C 70, 014316 (2004) T.C.Luu, S.Bogner, W.C.Haxton, P.Navratil Effective interactions for the three-body problem NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, contributions from three-body effective interactions.
doi: 10.1103/PhysRevC.70.014316
2004NO19 Phys.Rev. C 70, 061002 (2004) A.Nogga, S.K.Bogner, A.Schwenk Low-momentum interaction in few-nucleon systems NUCLEAR STRUCTURE 3H, 3,4He; calculated binding energies, three-nucleon force effects, related features. Low-momentum interactions.
doi: 10.1103/PhysRevC.70.061002
2003BO28 Phys.Rep. 386, 1 (2003) S.K.Bogner, T.T.S.Kuo, A.Schwenk Model-independent low momentum nucleon interaction from phase shift equivalence
doi: 10.1016/j.physrep.2003.07.001
2003BO37 Phys.Lett. B 576, 265 (2003) S.K.Bogner, T.T.S.Kuo, A.Schwenk, D.R.Entem, R.Machleidt Towards a model-independent low momentum nucleon-nucleon interactions
doi: 10.1016/j.physletb.2003.10.012
2002BO18 Phys.Rev. C65, 051301 (2002) S.Bogner, T.T.S.Kuo, L.Coraggio, A.Covello, N.Itaco Low Momentum Nucleon-Nucleon Potential and Shell Model Effective Interactions NUCLEAR STRUCTURE 18O, 134Te, 135I; calculated levels, J, π. Shell model, renormalization group - effective field theory approach. Comparison with data.
doi: 10.1103/PhysRevC.65.051301
2002KU22 Nucl.Phys. A704, 107c (2002) T.T.S.Kuo, S.Bogner, L.Coraggio A New Theory of Shell-Model Effective Interactions NUCLEAR STRUCTURE 18O; calculated levels, J, π. Folded-diagram method.
doi: 10.1016/S0375-9474(02)00771-6
2002KU42 Prog.Theor.Phys.(Kyoto), Suppl. 146, 159 (2002) Low Momentum Nucleon-Nucleon Interaction and Halo Nuclei NUCLEAR STRUCTURE 6He; calculated energy levels. Low momentum nucleon-nucleon interaction, comparison with data.
doi: 10.1143/PTPS.146.159
2001BO13 Nucl.Phys. A684, 432c (2001) S.Bogner, T.T.S.Kuo, L.Coraggio Low Momentum Nucleon-Nucleon Potentials with Half-on-Shell T-Matrix Equivalence
doi: 10.1016/S0375-9474(01)00449-3
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