References quoted in the XUNDL dataset: 57CU NI(64ZN,X):T1/2:XUNDL-4

5 references found.

Clicking on a keynumber will list datasets that reference the given article.


1984SH28

Phys.Rev. C30, 2111 (1984)

T.Shinozuka, M.Fujioka, H.Miyatake, M.Yoshii, H.Hama, T.Kamiya

Observation of the Decay of a New Isotope 57Cu and Its Mirror Transition

NUCLEAR REACTIONS 58Ni(p, 2n), E=23-34 MeV; measured Eγ, Iγ, β-spectra; deduced evidence for 57Cu.

RADIOACTIVITY 57Cu(β+) [from 58Ni(p, 2n), E=23-34 MeV]; measured Eγ, Iγ, Eβ, Iβ, T1/2, β end-point energy; deduced log ft. 57Ni levels deduced Gamow-Teller transition matrix element.

doi: 10.1103/PhysRevC.30.2111


1987HAZN

Contrib.Proc. 5th Int.Conf.Nuclei Far from Stability, Rosseau Lake, Canada, J11 (1987)

H.Hama, T.Shinozuka, M.Fujioka, M.Yoshii, K.Taguchi, T.Ishimatsu

Half-Life Measurements of T(z) = (-1/2) Nuclei and the Gamow-Teller Matrix Elements in the f7/2p3/2-Shell Region

RADIOACTIVITY 45V, 47Cr, 59Mn, 51Fe, 55Ni, 57Cu; measured β-decay T1/2; deduced log ft, Gamow-Teller matrix elements. Note: 59Mn may be typo, see 1988HaZB.


1996SE01

Phys.Rev. C53, 96 (1996)

D.R.Semon, M.C.Allen, H.Dejbakhsh, C.A.Gagliardi, S.E.Hale, J.Jiang, L.Trache, R.E.Tribble, S.J.Yennello, H.M.Xu, X.G.Zhou, B.A.Brown

l-Forbidden Gamow-Teller β Decay of 57Cu

RADIOACTIVITY 57Cu(β+) [from 1H(58Ni, 57Cu), E=29-31 MeV/nucleon]; measured βγ-coin, Eγ, Iγ, T1/2. 57Ni levels deduced l-forbidden, superallowed Gamow-Teller transition features, absolute branching ratio. Shell model comparison.

NUCLEAR STRUCTURE 29P, 29Si, 57Cu, 57Ni; calculated B(λ), B(GT). Shell model.

doi: 10.1103/PhysRevC.53.96


2002LO13

Phys.Rev. C66, 025803 (2002)

M.J.Lopez Jimenez, B.Blank, M.Chartier, S.Czajkowski, P.Dessagne, G.de France, J.Giovinazzo, D.Karamanis, M.Lewitowicz, V.Maslov, C.Miehe, P.H.Regan, M.Stanoiu, M.Wiescher

Half-life measurements of proton-rich 78Kr fragments

RADIOACTIVITY 53,54Co, 54,55Ni, 56,57Cu, 57,58,59Zn, 60,61,62Ga, 61,62,63Ge, 64,65,66As, 66,67Se, 70Br, 71Kr(β+), (EC) [from 78Kr fragmentation]; measured T1/2. Astrophysical implications discussed. Comparison with previous results.

doi: 10.1103/PhysRevC.66.025803


2017KU12

Eur.Phys.J. A 53, 134 (2017)

L.Kucuk, S.E.A.Orrigo, A.Montaner-Piza, B.Rubio, Y.Fujita, W.Gelletly, B.Blank, Y.Oktem, T.Adachi, A.Algora, P.Ascher, R.B.Cakirli, G.de France, H.Fujita, E.Ganioglu, J.Giovinazzo, S.Grevy, F.M.Marques, F.Molina, F.de Oliveira Santos, L.Perrot, R.Raabe, P.C.Srivastava, G.Susoy, A.Tamii, J.C.Thomas

Half-life determination of Tz = -1 and Tz = -1/2 proton-rich nuclei and the β decay of 58Zn

NUCLEAR REACTIONS Ni(64Zn, x), E=79 MeV/nucleon; measured fragments of Tz=-1 and =-1/2 (together 16 isotopes), subsequent charged particle decays using two DSSSD and four Ge detectors, β-delayed Eγ, Iγ. 58Zn[Tz=-1]; deduced decay scheme, absolute Fermi and Gamow-Teller β-transition strength B(F), B(GT), T1/2. 50Fe, 52Co, 56Cu, 60Ga, 62Ge[Tz=-1]; deduced T1/2. 47Cr, 49Mn, 51Fe, 55Ni, 57Cu, 59Zn, 61Ga, 63Ge[Tz=-1/2]; deduced T1/2. Here, T1/2 deduced using correlation time and the results compared with published ones.

doi: 10.1140/epja/i2017-12327-1