Effect of neutron-proton mass difference on charge symmetry breaking in neutron-proton elastic scattering

1987 ◽  
Vol 36 (6) ◽  
pp. 2442-2449 ◽  
Author(s):  
M. J. Iqbal ◽  
J. Thaler ◽  
R. M. Woloshyn
2011 ◽  
Vol 26 (03n04) ◽  
pp. 592-594
Author(s):  
ARSENIY A. FILIN

We study charge symmetry breaking (CSB) in the reaction pn → dπ0. CSB manifests itself in a forward-backward asymmetry of the differential cross section measured recently at TRIUMF. A complete calculation of CSB effects at leading order in chiral perturbation theory is performed. A new leading-order operator is included. This allows us to extract the strong contribution to the neutron-proton mass difference from the analysis. The value obtained is consistent with the result of Gasser and Leutwyler based on the Cottingham sum rule and with an extraction from lattice QCD.


2009 ◽  
Vol 681 (5) ◽  
pp. 423-427 ◽  
Author(s):  
A. Filin ◽  
V. Baru ◽  
E. Epelbaum ◽  
J. Haidenbauer ◽  
C. Hanhart ◽  
...  

1987 ◽  
Vol 36 (5) ◽  
pp. 1956-1967 ◽  
Author(s):  
A. G. Williams ◽  
A. W. Thomas ◽  
G. A. Miller

1993 ◽  
Vol 562 (4) ◽  
pp. 644-658 ◽  
Author(s):  
Thomas Schäfer ◽  
Volker Koch ◽  
Gerald E. Brown

1986 ◽  
Vol 56 (24) ◽  
pp. 2567-2570 ◽  
Author(s):  
G. A. Miller ◽  
A. W. Thomas ◽  
A. G. Williams

1992 ◽  
Vol 07 (32) ◽  
pp. 3037-3043 ◽  
Author(s):  
T. GOLDMAN ◽  
J.A. HENDERSON ◽  
A.W. THOMAS

In generating a charge-symmetry breaking potential using ρ-ω mixing it is usually assumed that the mixing amplitude is constant (at the on-mass-shell value). Since the exchanged meson is actually far off-shell one must question the validity of this assumption. By constructing a simple quark model in which the mixing is generated by the u-d quark mass difference, we find that the assumption seems to be a very poor one.


1986 ◽  
Vol 36 (2) ◽  
pp. 248-252 ◽  
Author(s):  
M. Kh. Khankhasayev ◽  
F. Nichitiu ◽  
M. G. Sapozhnikov

1995 ◽  
Author(s):  
R. Abegg ◽  
A. R. Berdoz ◽  
J. Birchall ◽  
J. R. Campbell ◽  
C. A. Davis ◽  
...  

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