Lattice calculation of meson form factors for semi-leptonic decays

1989 ◽  
Vol 9 ◽  
pp. 186-192 ◽  
Author(s):  
Claude Bernard ◽  
Aida El-Khadra ◽  
Amarjit Soni
1991 ◽  
Vol 527 ◽  
pp. 531-534 ◽  
Author(s):  
Terrence Draper ◽  
Keh-Fei Liu ◽  
D.B. Leinweber ◽  
R.M. Woloshyn

2021 ◽  
Vol 104 (7) ◽  
Author(s):  
Gen Wang ◽  
Jian Liang ◽  
Terrence Draper ◽  
Keh-Fei Liu ◽  
Yi-Bo Yang ◽  
...  

2021 ◽  
Vol 81 (12) ◽  
Author(s):  
Zhi-Peng Xing ◽  
Zhen-Xing Zhao

AbstractA comprehensive study of $$b\rightarrow c$$ b → c weak decays of doubly heavy baryons is presented in this paper. The transition form factors as well as the pole residues of the initial and final states are respectively obtained by investigating the three-point and two-point correlation functions in QCD sum rules. Contributions from up to dimension-6 operators are respectively considered for the two-point and three-point correlation functions. The obtained form factors are then applied to a phenomenological analysis of semi-leptonic decays.


Author(s):  
Hong-Wei Ke ◽  
Fang Lu ◽  
Xiao-Hai Liu ◽  
Xue-Qian Li

Abstract In this work we study the weak decays of $$\Xi _{cc}\rightarrow \Xi _c$$Ξcc→Ξc and $$\Xi _{cc}\rightarrow \Xi '_c$$Ξcc→Ξc′ in the light-front quark model. Generally, a naive, but reasonable conjecture suggests that the cc subsystem in $$\Xi _{cc}$$Ξcc ( us pair in $$\Xi ^{(')}_c$$Ξc(′)) stands as a diquark with definite spin and color assignments. During the concerned processes, the diquark of the initial state is not a spectator, namely must be broken. A Racah transformation would decompose the original (cc)q into a combination of c(cq) components. Thus we may deal with the decaying c quark alone while keeping the (cq) subsystem as a spectator. With the re-arrangement of the inner structure we calculate the form factors numerically and then obtain the rates of semi-leptonic decays and non-leptonic decays, which will be measured in the future.


1962 ◽  
Vol 8 (7) ◽  
pp. 295-297 ◽  
Author(s):  
J. M. Dobbs ◽  
K. Lande ◽  
A. K. Mann ◽  
K. Reibel ◽  
F. J. Sciulli ◽  
...  
Keyword(s):  

2014 ◽  
Vol 562 ◽  
pp. 012009 ◽  
Author(s):  
K U Can ◽  
G Erkol ◽  
B Isildak ◽  
M Oka ◽  
T T Takahashi

2017 ◽  
Vol 32 (08) ◽  
pp. 1750043 ◽  
Author(s):  
E. Di Salvo ◽  
Z. J. Ajaltouni

We propose two different and complementary observables for singling out possible signals of physics beyond the Standard Model (SM) in the semi-leptonic decays [Formula: see text], both with the [Formula: see text] lepton and with a light lepton. The two observables are the partial decay width and a T-odd asymmetry, whose respective sensitivities to scalar and/or pseudo-scalar coupling are calculated as functions of the parameters characterizing new physics (NP). Two different form factors are used. Three particular cases are discussed and analyzed in detail.


1991 ◽  
Vol 20 ◽  
pp. 467-471 ◽  
Author(s):  
Keh-Fei Liu ◽  
Ji-Min Wu ◽  
Shao-Jing Dong ◽  
Walter Wilcox

Experimental results on strange particle leptonic decays are summarized and compared with predictions based on the Δ S = + Δ Q , |Δ I | = ½ and Δ S ǂ 2 rules, CP invariance and electron-muon universality. Recent (and still preliminary) results on K 0 1.2 → π ± + e ∓ + v , K + → π + + π ± + e ∓ + v and Ʃ ± → N + ( μ or e ) ± + v are compatible with little (< 10%) or no violation of the Δ S = + Δ Q rule. Three-body leptonic decay rates of K + and K 0 disagree by about two standard deviations with the |Δ I = ½ rule prediction, but the agreement is restored if ca . 10% |Δ I | = 3/2 admixture is allowed. No Δ S = 2, ≡ - → N + e - + v or ≡ 0 → p + e - + v decays have been observed to the level of ca . 1% of the normal decays. All the data are in good agreement with time reversal or CP invariance and with the assumptions that the lepton pair is coupled locally and that electrons and muons behave identically apart from effects of their mass difference. † The branching ratios for the various hyperon leptonic decays and the observed V-A form for A β decay are explained qualitatively by the theory of Cabibbo, for example, but the data are not yet precise enough for a sharp test of the theory. New data on K + → π 0 + ( e or μ ) + + v spectra, branching ratios and muon polarization indicate that the interaction is of the vector form with approximately constant form factors and that the form factor ratio f - / f + is of order 1 or compatible with 0, as in the case of K 0 2 → π ± + e ∓ + v .


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