Energy and Mass Dependence of Low-Energy Pion Single Charge Exchange to the Isobaric Analog State

1985 ◽  
Vol 55 (18) ◽  
pp. 1862-1865 ◽  
Author(s):  
F. Irom ◽  
M. J. Leitch ◽  
H. W. Baer ◽  
J. D. Bowman ◽  
M. D. Cooper ◽  
...  
1987 ◽  
Vol 36 (4) ◽  
pp. 1453-1458 ◽  
Author(s):  
F. Irom ◽  
H. W. Baer ◽  
A. G. Bergmann ◽  
J. D. Bowman ◽  
P. Heusi ◽  
...  

1987 ◽  
Vol 35 (4) ◽  
pp. 1382-1387 ◽  
Author(s):  
J. N. Knudson ◽  
J. R. Comfort ◽  
R. A. Gianelli ◽  
B. G. Ritchie ◽  
D. Rothenberger ◽  
...  

1992 ◽  
Vol 46 (6) ◽  
pp. 2259-2263 ◽  
Author(s):  
J. M. O’Donnell ◽  
H. T. Fortune ◽  
J. D. Silk ◽  
S. Mordechai ◽  
C. L. Morris ◽  
...  

1980 ◽  
Vol 45 (12) ◽  
pp. 982-986 ◽  
Author(s):  
Helmut W. Baer ◽  
J. D. Bowman ◽  
M. D. Cooper ◽  
F. H. Cverna ◽  
C. M. Hoffman ◽  
...  

1987 ◽  
Author(s):  
H. W. Baer ◽  
A. G. Bergmann ◽  
J. D. Bowman ◽  
F. Irom ◽  
M. J. Leitch ◽  
...  

2018 ◽  
Vol 178 ◽  
pp. 05001
Author(s):  
Yoshitaka Fujita ◽  
Hirohiko Fujita ◽  
Yusuke Tanumura

Nuclei have spin- and isospin-degrees of freedom. Therefore, Gamow-Teller (GT) transitions caused by the στ operator (spin-isospin operator) are unique tools for the studies of nuclear structure as well as nuclear interactions. They can be studied in β decays as well as charge-exchange (CE) reactions. Similarly, M1 γ decays are mainly caused by the στ operator. Combined studies of these transitions caused by Weak, Strong, and Electro-Magnetic interactions provide us a deeper understanding of nuclear spin-isospin-type transitions. We first compare the strengths of analogous GT and M1 transitions in the A = 27, Tz = ±½ mirror nuclei 27Al and 27Si. The comparison is extended to the Tz = ±1, 0 nuclei. The strength of GT transition from the ground state (g.s.) of 42Ca to the 0.611 MeV first Jπ = 1+ state in 42Sc is compared with that of the analogous M1 transition from the 0.611 MeV state to the T = 1, 0+ g.s. (isobaric analog state: IAS) in 42Sc. The 0.611 MeV state has the property of Low-energy Super GT (LeSGT) state, because it carries the main part of the GT strength of all available transitions from the g.s. of 42Ca (and 42Ti) to the Jπ = 1+ GT states in 42Sc.


2019 ◽  
Vol 223 ◽  
pp. 01053
Author(s):  
Hiroyuki Sagawa

We study the sum rules of double Gamow-Teller (DGT) excitations through double spin-isospin operator (σt­)2 In general, 2+states in the granddaughter nuclei have dominant transition strength in DGT excitations and 0+states are weak, except in T = 1 mother nuclei in which 0+strength is competitive with 2+strength. A possibility to extract the unit cross section for the DGT transition strength is pointed out in the (#x03C3;t­)2 excitation of double isobaric analog state (DIAS) in T = 1 nuclei.


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