G factor of 41+ states in the N=82 isotones Xe136 and Ba138

Z. Berant; A. Wolf; John C. Hill; F. K. Wohn; R. L. Gill; H. MacH; M. Rafailovich; H. Kruse; B. H. Wildenthal; G. Peaslee; A. Aprahamian; J. Goulden; C. Chung

doi:10.1103/PhysRevC.31.570

G factor of 41+ states in the N=82 isotones Xe136 and Ba138

Z. Berant
, A. Wolf
, John C. Hill
, F. K. Wohn
, R. L. Gill
, H. MacH
, M. Rafailovich
, H. Kruse
, B. H. Wildenthal
, G. Peaslee
, A. Aprahamian
, J. Goulden
, C. Chung

Materials Science and Engineering

Ames Laboratory
Brookhaven National Laboratory
Michigan State University
Stony Brook University
Clark University
University of Oklahoma
University of Maryland, College Park

Research output: Contribution to journal › Article › peer-review

25 Scopus citations

Abstract

The g factors for the 41+ states in Xe136 and Ba138 were measured using the method of time-integral perturbed angular correlation. The levels of interest were populated by the decay of mass-separated I136 and Cs138. g factors of 0.800.15 and 0.800.14 were measured for the 41+ states in Xe136 and Ba138, respectively. The above results, along with those for the g factors in the 41+ state in Ce140 and the 61+ states in Te134 and Ba138, are well described by a shell-model calculation in which the effective elemental proton g factors are gl=1.12 and gs=4.12.

Original language	English
Pages (from-to)	570-574
Number of pages	5
Journal	Physical Review C - Nuclear Physics
Volume	31
Issue number	2
DOIs	https://doi.org/10.1103/PhysRevC.31.570
State	Published - 1985

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10.1103/PhysRevC.31.570

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title = "G factor of 41+ states in the N=82 isotones Xe136 and Ba138",

abstract = "The g factors for the 41+ states in Xe136 and Ba138 were measured using the method of time-integral perturbed angular correlation. The levels of interest were populated by the decay of mass-separated I136 and Cs138. g factors of 0.800.15 and 0.800.14 were measured for the 41+ states in Xe136 and Ba138, respectively. The above results, along with those for the g factors in the 41+ state in Ce140 and the 61+ states in Te134 and Ba138, are well described by a shell-model calculation in which the effective elemental proton g factors are gl=1.12 and gs=4.12.",

author = "Z. Berant and A. Wolf and Hill, \{John C.\} and Wohn, \{F. K.\} and Gill, \{R. L.\} and H. MacH and M. Rafailovich and H. Kruse and Wildenthal, \{B. H.\} and G. Peaslee and A. Aprahamian and J. Goulden and C. Chung",

year = "1985",

doi = "10.1103/PhysRevC.31.570",

language = "English",

volume = "31",

pages = "570--574",

journal = "Physical Review C - Nuclear Physics",

issn = "0556-2813",

number = "2",

}

TY - JOUR

T1 - G factor of 41+ states in the N=82 isotones Xe136 and Ba138

AU - Berant, Z.

AU - Wolf, A.

AU - Hill, John C.

AU - Wohn, F. K.

AU - Gill, R. L.

AU - MacH, H.

AU - Rafailovich, M.

AU - Kruse, H.

AU - Wildenthal, B. H.

AU - Peaslee, G.

AU - Aprahamian, A.

AU - Goulden, J.

AU - Chung, C.

PY - 1985

Y1 - 1985

N2 - The g factors for the 41+ states in Xe136 and Ba138 were measured using the method of time-integral perturbed angular correlation. The levels of interest were populated by the decay of mass-separated I136 and Cs138. g factors of 0.800.15 and 0.800.14 were measured for the 41+ states in Xe136 and Ba138, respectively. The above results, along with those for the g factors in the 41+ state in Ce140 and the 61+ states in Te134 and Ba138, are well described by a shell-model calculation in which the effective elemental proton g factors are gl=1.12 and gs=4.12.

AB - The g factors for the 41+ states in Xe136 and Ba138 were measured using the method of time-integral perturbed angular correlation. The levels of interest were populated by the decay of mass-separated I136 and Cs138. g factors of 0.800.15 and 0.800.14 were measured for the 41+ states in Xe136 and Ba138, respectively. The above results, along with those for the g factors in the 41+ state in Ce140 and the 61+ states in Te134 and Ba138, are well described by a shell-model calculation in which the effective elemental proton g factors are gl=1.12 and gs=4.12.

UR - https://www.scopus.com/pages/publications/4243709853

U2 - 10.1103/PhysRevC.31.570

DO - 10.1103/PhysRevC.31.570

M3 - Article

AN - SCOPUS:4243709853

SN - 0556-2813

VL - 31

SP - 570

EP - 574

JO - Physical Review C - Nuclear Physics

JF - Physical Review C - Nuclear Physics

IS - 2

ER -

G factor of 41+ states in the N=82 isotones Xe136 and Ba138

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