References quoted in the XUNDL dataset: 62CR 9BE(65MN,62CRG):XUNDL-5

4 references found.

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2010GA06

Phys.Rev. C 81, 051304 (2010)

A.Gade, R.V.F.Janssens, T.Baugher, D.Bazin, B.A.Brown, M.P.Carpenter, C.J.Chiara, A.N.Deacon, S.J.Freeman, G.F.Grinyer, C.R.Hoffman, B.P.Kay, F.G.Kondev, T.Lauritsen, S.McDaniel, K.Meierbachtol, A.Ratkiewicz, S.R.Stroberg, K.A.Walsh, D.Weisshaar, R.Winkler, S.Zhu

Collectivity at N = 40 in neutron-rich ⁶⁴Cr

NUCLEAR REACTIONS ⁹Be(⁶²Fe, ⁶²Fe'), E=73.0 MeV/nucleon [⁶²Fe secondary beam from primary reaction ⁹Be(⁷⁶Ge, X), E=130 MeV/nucleon], ⁹Be(⁶⁴Fe, ⁶⁴Fe'), E=67.5 MeV/nucleon [⁶⁴Fe secondary beam from primary reaction ⁹Be(⁷⁶Ge, X), E=130 MeV/nucleon], ⁹Be(⁶⁶Fe, ⁶⁶Fe'), E=82.6 MeV/nucleon [⁶⁶Fe secondary beam from primary reaction ⁹Be(⁷⁶Ge, X), E=130 MeV/nucleon], ⁹Be(⁶⁰Cr, ⁶⁰Cr'), E=80.6 MeV/nucleon [⁶⁰Cr secondary beam from primary reaction ⁹Be(⁷⁶Ge, X), E=130 MeV/nucleon], ⁹Be(⁶²Cr, ⁶²Cr'), E=74.6 MeV/nucleon [⁶²Cr secondary beam from primary reaction ⁹Be(⁷⁶Ge, X), E=130 MeV/nucleon], ⁹Be(⁶⁴Cr, ⁶⁴Cr'), E=87.0 MeV/nucleon [⁶⁴Cr secondary beam from primary reaction ⁹Be(⁷⁶Ge, X), E=130 MeV/nucleon]; measured Eγ, Iγ, (particle)γ-coin, σ. ^62,64,66Fe, ^60,62,64Cr; deduced levels, J, π. Comparison with large-scale shell-model calculations in different model spaces. ⁹Be(⁷⁶Ge, X)⁶²Fe/⁶⁴Fe/⁶⁶Fe/⁶⁰Cr/⁶²Cr/⁶⁴Cr/⁶⁵Mn/⁶⁶Mn/⁶⁷Fe/⁶⁹Co, E=130 MeV/nucleon; measured yields of secondary ion beams.

doi: 10.1103/PhysRevC.81.051304

2012BA31

Phys.Rev. C 86, 011305 (2012), Erratum Phys.Rev. C 86, 049902 (2012)

T.Baugher, A.Gade, R.V.F.Janssens, S.M.Lenzi, D.Bazin, B.A.Brown, M.P.Carpenter, A.N.Deacon, S.J.Freeman, T.Glasmacher, G.F.Grinyer, F.G.Kondev, S.McDaniel, A.Poves, A.Ratkiewicz, E.A.McCutchan, D.K.Sharp, I.Stefanescu, K.A.Walsh, D.Weisshaar, S.Zhu

Intermediate-energy Coulomb excitation of ^{58, 60, 62}Cr: The onset of collectivity toward N=40

NUCLEAR REACTIONS ¹⁹⁷Au(⁵⁸Cr, ⁵⁸Cr'), E=81.1 MeV/nucleon; ¹⁹⁷Au(⁶⁰Cr, ⁶⁰Cr'), E=81.7 MeV/nucleon; ²⁰⁹Bi(⁶²Cr, ⁶²Cr'), E=79.0 MeV/nucleon; measured scattered projectile spectra, energy loss, time-of-flight, Eγ, Iγ, (particle)γ-coin using SeGA array at NSCL facility, integrated cross section, GEANT-4 simulations. Intermediate Coulomb excitation using secondary Cr beams from ⁹Be(⁷⁶Ge, X), E=130 MeV/nucleon primary reaction. ^58,60,62Cr, ¹⁹⁷Au; deduced levels, B(E2) of first 2+ state in Cr nuclei and a level in ¹⁹⁷Au, ratio of neutron and proton transition matrix elements M_n/M_p. ⁶²Cr; measured half-life of first 2+ state by Doppler shift and line-shape method. Systematics of energies and B(E2) values of first 2+ states in even-even N=22-40 Ni, Fe and Cr isotopes. Comparison with shell model calculations in the fpgd space using the state-of-the-art LNPS effective interaction.

doi: 10.1103/PhysRevC.86.011305

2015BR10

Phys.Rev. C 92, 034306 (2015)

T.Braunroth, A.Dewald, H.Iwasaki, S.M.Lenzi, M.Albers, V.M.Bader, T.Baugher, T.Baumann, D.Bazin, J.S.Berryman, C.Fransen, A.Gade, T.Ginter, A.Gottardo, M.Hackstein, J.Jolie, A.Lemasson, J.Litzinger, S.Lunardi, T.Marchi, V.Modamio, C.Morse, D.R.Napoli, A.Nichols, F.Recchia, S.R.Stroberg, R.Wadsworth, D.Weisshaar, K.Whitmore, K.Wimmer

Reduced transition strengths of low-lying yrast states in chromium isotopes in the vicinity of N=40

NUCLEAR REACTIONS ⁹Be(⁵⁹Mn, ⁵⁸Cr), E=92.1 MeV/nucleon; ⁹Be(⁶¹Mn, ⁶⁰Cr), E=91.9 MeV/nucleon; ⁹Be(⁶³Mn, ⁶²Cr), E=98 MeV/nucleon, [secondary ^59,61,63Mn beams from ⁹Be(⁸²Se, X), E=140 MeV/nucleon primary reaction using A1900 separator at NSCL-MSU]; measured Eγ, Iγ, beam-like recoil particle spectra and yields, (particle)γ-coin, level half-lives by recoil-distance Doppler-shift (RDDS) method using S800 spectrograph and SeGA array. ^58,60,62Cr; deduced levels, J, π, B(E2), intrinsic quadrupole moments Q₀ and deformation parameter β₂. Comparison with calculations using shell-model with LNPS interactions, realistic shell-model, and IBM-2. Systematics of energies and B(E2) for first 2+ states in N=22-52, Ti, Cr, Fe, Ni, Se and Kr nuclei. Systematics of ratios of energies and B(E2) values for first 2+, 4+ and 6+ states in ^{52,54,56,58,60,62}Cr, and E(5) limit.

doi: 10.1103/PhysRevC.92.034306

2021GA02

Phys.Rev. C 103, 014314 (2021)

A.Gade, R.V.F.Janssens, D.Bazin, P.Farris, A.M.Hill, S.M.Lenzi, J.Li, D.Little, B.Longfellow, F.Nowacki, A.Poves, D.Rhodes, J.A.Tostevin, D.Weisshaar

In-beam γ-ray spectroscopy of ^{62, 64}Cr

NUCLEAR REACTIONS ⁹Be(⁶⁵Mn, ⁶²Cr), (⁶⁵Mn, ⁶⁴Cr), (⁶⁶Fe, ⁶²Cr), (⁶⁶Fe, ⁶⁴Cr), (⁶⁸Co, ⁶²Cr), (⁶⁸Co, ⁶⁴Cr), E=90-95 MeV/nucleon, [secondary beams of ⁶⁵Mn, ⁶⁶Fe, ⁶⁸Co from ⁹Be(⁸²Se, X), E=140 MeV/nucleon primary reaction followed by separation of fragments using A1900 separator at NSCL-MSU Coupled Cyclotron Facility]; measured projectile-like reaction residues, Eγ, Iγ, (particle)γ-, and γγ-coin using GRETINA array for γ detection, and S800 ionization chamber with two plastic timing scintillators for detection of ⁶²Cr and ⁶⁴Cr particles analyzed through time-of-flight and energy loss. ^62,64Cr; deduced levels, J, π. Comparison with shell-model calculations using LNPS interaction.

NUCLEAR STRUCTURE ^62,64Cr; calculated levels, J, π, B(E2) using shell-model calculations with Lenzi-Nowacki-Poves-Sieja (LNPS) interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.103.014314