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NSR database version of May 20, 2024.

Search: Author = M.Kruse

Found 10 matches.

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2019KR15      Eur.Phys.J. A 55, 225 (2019)

M.K.G.Kruse, W.E.Ormand, C.W.Johnson

No-core shell model calculations of the photonuclear cross section of 10B

doi: 10.1140/epja/i2019-12905-1
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2018VO02      Phys.Rev. C 97, 034314 (2018)

M.Vorabbi, A.Calci, P.Navratil, M.K.G.Kruse, S.Quaglioni, G.Hupin

Structure of the exotic 9He nucleus from the no-core shell model with continuum

NUCLEAR STRUCTURE 9He; calculated n+8He continuum by ab initio no-core shell model with continuum (NCSMC) formalism and chiral nucleon-nucleon interactions at N4LO; deduced unbound character of 9He, and two resonant states, J, π. Comparison with structure of 10Li and 11B. 4,6,8He; calculated ground-state energies by NCSM using the SRG-evolved N4LO nucleon-nucleon potential. Comparison with available experimental data.

doi: 10.1103/PhysRevC.97.034314
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2013KR03      Phys.Rev. C 87, 044301 (2013)

M.K.G.Kruse, E.D.Jurgenson, P.Navratil, B.R.Barrett, W.E.Ormand

Extrapolation uncertainties in the importance-truncated no-core shell model

NUCLEAR STRUCTURE 6Li; calculated distribution of ground-state energies, and other parameters. Importance-truncated no-core shell model (IT-NCSM), and NCSM calculations.

doi: 10.1103/PhysRevC.87.044301
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2012CO20      Phys.Rev. C 86, 054002 (2012)

S.A.Coon, M.I.Avetian, M.K.G.Kruse, U.van Kolck, P.Maris, J.P.Vary

Convergence properties of ab initio calculations of light nuclei in a harmonic oscillator basis

NUCLEAR STRUCTURE 2,3H, 4,6He; calculated ground-state energy of light nuclei as function of momentum using shell model with the bare and soft NN interactions Idaho N3LO and JISP16.

doi: 10.1103/PhysRevC.86.054002
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2011BA53      J.Phys.:Conf.Ser. 312, 092016 (2011)

B.Barrett, M.Kruse, A.Lisetskiy, P.Navratil, I.Stetcu, J.Vary

Ab initio shell model with a core: Extending the No Core Shell Model to heavier nuclei

NUCLEAR STRUCTURE 7Li; calculated ground state energy. 8,9,10He; calculated levels, J, π. 6Li; calculated quadrupole moment. SSM (standard shell model), NCSM (No Core Shell Model).

doi: 10.1088/1742-6596/312/9/092016
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2009LI31      Phys.Rev. C 80, 024315 (2009)

A.F.Lisetskiy, M.K.G.Kruse, B.R.Barrett, P.Navratil, I.Stetcu, J.P.Vary

Effective operators from exact many-body renormalization

NUCLEAR STRUCTURE 6Li; calculated levels, J, π, reduced two-body matrix elements, E2 reduced matrix elements and quadrupole moments using ab initio no-core shell model (NCSM) approach. 7,9Li; calculated absolute quadrupole moments and E2 transition matrix elements. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.024315
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2008LI44      Phys.Rev. C 78, 044302 (2008)

A.F.Lisetskiy, B.R.Barrett, M.K.G.Kruse, P.Navratil, I.Stetcu, J.P.Vary

Ab-initio shell model with a core

NUCLEAR STRUCTURE 6,7Li, 8,9,10He; calculated excitation energies, J, π. Ab-initio no-core shell model calculations.

doi: 10.1103/PhysRevC.78.044302
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2005KR17      Eur.Phys.J. A 25, 339 (2005)

M.K.G.Kruse, H.G.Miller, A.R.Plastino, A.Plastino, S.Fujita

Landau-Ginzburg method applied to finite fermion systems: Pairing in nuclei

NUCLEAR STRUCTURE 20Ne, 48Ca, 88Sr, 208Pb; calculated specific heat vs temperature, pairing phase transition features. Landau-Ginzburg method.

doi: 10.1140/epja/i2005-10133-0
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1990BA31      Nucl.Phys. A515, 493 (1990)

A.M.Baxter, A.P.Byrne, G.D.Dracoulis, R.A.Bark, F.Riess, A.E.Stuchbery, M.C.Kruse, A.R.Poletti

Spectroscopy of High-Spin States of 206Po

NUCLEAR REACTIONS 198Pt(13C, 5n), E=70-80 MeV; measured γγ(t), (13C)γ(t), Eγ, Iγ, Iγ(E), Iγ(θ), I(ce). 206Po deduced levels, J, π, T1/2, B(λ), ICC. Enriched targets, Ge, Si(Li) detectors, pulsed beam. Empirical shell model calculations.

doi: 10.1016/0375-9474(90)90595-D
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1989DR02      Nucl.Phys. A493, 145 (1989)

G.D.Dracoulis, F.Riess, A.E.Stuchbery, R.A.Bark, S.L.Gupta, A.M.Baxter, M.Kruse

Properties of (15/2)- States in 215Ra and 217Th; Evaluation of the (15/2)- to (9/2)+ E3 strength in N = 127 isotones

NUCLEAR REACTIONS 208Pb(12C, 5n), E=80 MeV; 206Pb(13C, 4n), E=78 MeV; 204Pb(16O, 3n), E=84 MeV; measured Eγ, Iγ(t), I(ce)(t). 215Ra, 217Th deduced levels, ICC, T1/2, B(E3). Enriched targets, pulsed beams, Ge, Si(Li), Compton suppressed detector. Model comparison.

NUCLEAR STRUCTURE 209Pb, 211Po, 213Rn, 215Ra, 217Th; calculated levels, B(E3). Particle-octupole vibration coupling.

doi: 10.1016/0375-9474(89)90537-X
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Note: The following list of authors and aliases matches the search parameter M.Kruse: , M.C.KRUSE, M.K.KRUSE