scholarly journals Final-state phases in doubly Cabibbo-suppressed charmed meson nonleptonic decays

2002 ◽  
Vol 65 (5) ◽  
Author(s):  
Cheng-Wei Chiang ◽  
Jonathan L. Rosner
1995 ◽  
Vol 359 (3-4) ◽  
pp. 403-410 ◽  
Author(s):  
P.L. Frabetti ◽  
H.W.K. Cheung ◽  
J.P. Cumalat ◽  
C. Dallapiccola ◽  
J.F. Ginkel ◽  
...  

2003 ◽  
Vol 67 (1) ◽  
Author(s):  
Cheng-Wei Chiang ◽  
Zumin Luo ◽  
Jonathan L. Rosner

2003 ◽  
Vol 40 (5) ◽  
pp. 563-572 ◽  
Author(s):  
Chen Shao-Long ◽  
Guo Xin-Heng ◽  
Li Xue-Qian ◽  
Wang Guo-Li

1980 ◽  
Vol 90 (4) ◽  
pp. 431-435 ◽  
Author(s):  
N. Deshpande ◽  
M. Gronau ◽  
D. Sutherland

1996 ◽  
Vol 379 (1-4) ◽  
pp. 249-256 ◽  
Author(s):  
F Buccella ◽  
M Lusignoli ◽  
A Pugliese

1993 ◽  
Vol 08 (22) ◽  
pp. 2079-2086 ◽  
Author(s):  
ASHOK DAS ◽  
VISHNU S. MATHUR

We investigate the nonleptonic decay of charmed meson into two pseudoscalar mesons using the vector-dominance model, and compare the results with those obtained from the factorization model. In particular, we discuss the role of the annihilation diagrams in the two models.


2021 ◽  
Vol 81 (4) ◽  
Author(s):  
Natsumi Ikeno ◽  
Melahat Bayar ◽  
Eulogio Oset

AbstractWe study the $$D^+ \rightarrow \pi ^+ \eta \eta $$ D + → π + η η and $$D^+ \rightarrow \pi ^+ \pi ^0 \eta $$ D + → π + π 0 η reactions, which are single Cabibbo suppressed and can proceed both through internal and external emission. The primary mechanisms at quark level are considered, followed by hadronization to produce three mesons in the $$D^+$$ D + decay, and after that the final state interaction of these mesons leads to the production of the $$a_0(980)$$ a 0 ( 980 ) resonance, seen in the $$\pi ^+ \eta $$ π + η , $$\pi ^0 \eta $$ π 0 η mass distributions. The theory has three unknown parameters to determine the shape of the distributions and the ratio between the $$D^+ \rightarrow \pi ^+ \eta \eta $$ D + → π + η η and $$D^+ \rightarrow \pi ^+ \pi ^0 \eta $$ D + → π + π 0 η rates. This ratio restricts much the sets of parameters but there is still much freedom leading to different shapes in the mass distributions. We call for a measurement of these mass distributions that will settle the reaction mechanism, while at the same time provide relevant information on the way that the $$a_0(980)$$ a 0 ( 980 ) resonance is produced in the reactions.


1998 ◽  
Vol 13 (19) ◽  
pp. 3361-3384 ◽  
Author(s):  
GUSTAV KRAMER ◽  
CAI-DIAN LÜ

Nonleptonic decays of B mesons into two mesons or meson resonances are studied on the basis of two versions of simple pole dominance models involving scalar, vector, pseudoscalar and axial vector poles. The results are compared with those obtained from the usual factorization model and are used to obtain information on strong coupling constants between the B meson and one light or one charmed meson, respectively. These coupling constants are compared to results from various QCD sum rule calculations.


2001 ◽  
Vol 500 (3-4) ◽  
pp. 247-253 ◽  
Author(s):  
Michael Gronau ◽  
Jonathan L. Rosner

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