Near-threshold incoherent pion photoproduction on the deuteron with final-state interaction effects

2019 ◽  
Vol 411 ◽  
pp. 167990 ◽  
Author(s):  
E.M. Darwish ◽  
M.M. Almarashi ◽  
E.M. Mahrous ◽  
M.A. Hassanain ◽  
M. Saleh Yousef
Keyword(s):  
Final State Interaction ◽  
Interaction Effects ◽  
Pion Photoproduction ◽  
State Interaction ◽  
Final State ◽  
Near Threshold

Final state interaction effects in the B + → D + K 0 decay

JETP Letters ◽  
2014 ◽  
Vol 100 (5) ◽  
pp. 285-294
Author(s):  
H. Mehraban ◽  
M. Borhani ◽  
A. Asadi
Keyword(s):  
Final State Interaction ◽  
Interaction Effects ◽  
State Interaction ◽  
Final State

Final state interaction effects in B 0 → J/ψπ 0 decay

2014 ◽  
Vol 77 (12) ◽  
pp. 1483-1490
Author(s):  
Hossein Mehraban ◽  
Amin Asadi
Keyword(s):  
Final State Interaction ◽  
Interaction Effects ◽  
State Interaction ◽  
Final State

scholarly journals The hidden charm decay of and final state interaction effects

2007 ◽  
Vol 645 (2-3) ◽  
pp. 185-188 ◽  
Author(s):  
Xiang Liu ◽  
Bo Zhang ◽  
Shi-Lin Zhu
Keyword(s):  
Final State Interaction ◽  
Interaction Effects ◽  
State Interaction ◽  
Final State ◽  
Charm Decay

scholarly journals STUDY OF THE η-7Be INTERACTION NEAR THRESHOLD IN p-6Li FUSION

2009 ◽  
Vol 18 (05n06) ◽  
pp. 1383-1388
Author(s):  
N. J. UPADHYAY ◽  
N. G. KELKAR ◽  
K. P. KHEMCHANDANI ◽  
B. K. JAIN
Keyword(s):  
Wave Function ◽  
Final State Interaction ◽  
Radial Wave Function ◽  
State Interaction ◽  
Nuclear Medium ◽  
Final State ◽  
Radial Wave ◽  
Near Threshold

We present a calculation for η production in the p-6Li fusion near threshold including the η-7Be final state interaction (FSI). We consider the 6Li and 7Be nuclei as α-d and α-3He clusters respectively. The calculations are done for the lowest states of 7 Be with [Formula: see text] resulting from the L = 1 radial wave function. The η-7Be interaction is incorporated through the η-7BeT–matrix, constructed from the medium modified matrices for the η-3He and η-α systems. These medium modified matrices are obtained by solving few body equations, where the scattering in nuclear medium is taken into account.

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