Ratio of pion-nucleus reaction cross sections and the neutron density distribution for lead

1972 ◽  
Vol 41 (5) ◽  
pp. 577-580 ◽  
Author(s):  
B.W. Allardyce ◽  
C.J. Batty ◽  
D.J. Baugh ◽  
E. Friedman ◽  
G. Heymann ◽  
...  
1999 ◽  
Vol 656 (2) ◽  
pp. 209-228 ◽  
Author(s):  
M. Fukuda ◽  
M. Mihara ◽  
T. Fukao ◽  
S. Fukuda ◽  
M. Ishihara ◽  
...  

2010 ◽  
Vol 25 (21n23) ◽  
pp. 2014-2015
Author(s):  
D. NISHIMURA ◽  
M. FUKUDA ◽  
M. TAKECHI ◽  
M. MIHARA ◽  
J. KOMURASAKI ◽  
...  

Reaction cross sections for 11 Be and 8 B on proton targets at 40A - 120A MeV have been measured by the transmission method. With these data, we can discuss the proton- and neutron- density distributions at the nuclear surface independently in principle using the Glauber theory. Our experimental results support that the constituent of halo in 11 Be is neutron dominantly and that of 8 B is proton dominantly.


2001 ◽  
Vol 10 (02) ◽  
pp. 99-105 ◽  
Author(s):  
I. AHMAD ◽  
J. H. MADANI

Theoretical study of α total reaction cross-sections for 50 Ti , 52 Cr , 54,58 Fe , and 58,64 Ni nuclei at 100 MeV is presented. Working within the framework of Coulomb modified Glauber model, we calculate α reaction cross-sections in terms of the phenomenological N-α amplitude using the semi-phenomenological nucleon density distribution proposed by Gambhir and Patil [Z. Phys.A324 (1986) 9]. We find that the semi-phenomenological density reproduces the observed behaviour of the reaction cross-sections for the isotopes and isotones quite satisfactorily.


2007 ◽  
Author(s):  
M. Fukuda ◽  
M. Takechi ◽  
M. Mihara ◽  
R. Matsumiya ◽  
K. Matsuta ◽  
...  

2005 ◽  
Vol 25 (S1) ◽  
pp. 217-219 ◽  
Author(s):  
M. Takechi ◽  
M. Fukuda ◽  
M. Mihara ◽  
T. Chinda ◽  
T. Matsumasa ◽  
...  

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