Development of spin-polarized slow positron beam using a 68Ge–68Ga positron source

Author(s):  
Masaki Maekawa ◽  
Yuki Fukaya ◽  
Atsushi Yabuuchi ◽  
Izumi Mochizuki ◽  
Atsuo Kawasuso
1997 ◽  
Vol 255-257 ◽  
pp. 799-801
Author(s):  
T. Nozaki ◽  
Yoshiko Itoh ◽  
Z.L. Peng ◽  
Yasuo Ito ◽  
N. Nakanishi ◽  
...  

2000 ◽  
Vol 58 (5-6) ◽  
pp. 759-762 ◽  
Author(s):  
J.H Kim ◽  
F Saito ◽  
Y Nagashima ◽  
T Kurihara ◽  
A Goto ◽  
...  

1999 ◽  
Vol 149 (1-4) ◽  
pp. 30-33 ◽  
Author(s):  
Ichiro Fujiwara ◽  
Yoshiko Itoh ◽  
Ren Iwata ◽  
Fuminori Saito ◽  
Akira Goto

1997 ◽  
Vol 116 ◽  
pp. 168-176 ◽  
Author(s):  
Terunobu Nakajyo ◽  
Mutsumi Tashiro ◽  
Tomoya Koizumi ◽  
Ikuzo Kanazawa ◽  
Fumio Komori ◽  
...  

1998 ◽  
Vol 5 (3) ◽  
pp. 360-362 ◽  
Author(s):  
A. Ando ◽  
S. Daté ◽  
M. G. Fedurin ◽  
M. Hara ◽  
H. Kamitsubo ◽  
...  

A low-energy positron beam is a unique probe of materials. In high-energy electron and positron storage rings it is possible to generate intense synchrotron radiation with a photon energy of 1–3 MeV by installing a high-field (8–10 T) superconducting wiggler. High-energy photons are converted to low-energy positrons by using a suitable target–moderator system. For an 8 GeV electron storage ring at a beam current of 100 mA, final yields are estimated to be about 108–1010 slow-e+ s−1 or larger depending on the moderation efficiency, with the size of the positron source 101–102 cm2. In the present work a wiggler magnetic system of 10 T is proposed. The main parameters of the superconducting wiggler are presented.


Author(s):  
Raed Alsulami ◽  
Mubarak Albarqi ◽  
Safwan Jaradat ◽  
Shoaib Usman ◽  
Joseph Graham

1999 ◽  
Vol 149 (1-4) ◽  
pp. 175-180 ◽  
Author(s):  
J.W. Taylor ◽  
A.S. Saleh ◽  
P.C. Rice-Evans ◽  
A.P. Knights ◽  
C. Jeynes

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