Javascript must be enabled to continue!
Study on $$\Xi _{cc}\rightarrow \Xi _c$$ and $$\Xi _{cc}\rightarrow \Xi '_c$$ weak decays in the light-front quark model
View through CrossRef
AbstractIn 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.
Springer Science and Business Media LLC
Title: Study on $$\Xi _{cc}\rightarrow \Xi _c$$ and $$\Xi _{cc}\rightarrow \Xi '_c$$ weak decays in the light-front quark model
Description:
AbstractIn 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.
Related Results
CP-violating observables of four-body $$B_{(s)} \rightarrow (\pi \pi )(K\bar{K})$$ decays in perturbative QCD
CP-violating observables of four-body $$B_{(s)} \rightarrow (\pi \pi )(K\bar{K})$$ decays in perturbative QCD
AbstractIn this work, we investigate six helicity amplitudes of the four-body $$B_{(s)} \rightarrow (\pi \pi )(K\bar{K})$$
...
Study of four-body decays $$B_{(s)} \rightarrow (\pi \pi )(\pi \pi )$$ in the perturbative QCD approach
Study of four-body decays $$B_{(s)} \rightarrow (\pi \pi )(\pi \pi )$$ in the perturbative QCD approach
AbstractIn this work, we make a systematical study on the four-body $$B_{(s)} \rightarrow (\pi \pi )(\pi \pi )$$
B
...
Study of the $$B^{+}\rightarrow \pi ^{+}\left( \pi ^{+}\pi ^{-}\right) $$ decay in PQCD approach
Study of the $$B^{+}\rightarrow \pi ^{+}\left( \pi ^{+}\pi ^{-}\right) $$ decay in PQCD approach
AbstractBased on the fitting results of the LHCb collaboration on the contributions of various intermediate resonances to the$$B^{+}\rightarrow \pi ^{+}\pi ^{+}\pi ^{-}$$B+→π+π+π-d...
Dark-sector physics in the search for the rare decays $$K^+\rightarrow \pi ^+ \nu {\bar{\nu }}$$ and $$K_L\rightarrow \pi ^0 \nu {\bar{\nu }}$$
Dark-sector physics in the search for the rare decays $$K^+\rightarrow \pi ^+ \nu {\bar{\nu }}$$ and $$K_L\rightarrow \pi ^0 \nu {\bar{\nu }}$$
AbstractWe compute the contribution of the decays $$K_L \rightarrow \pi ^0 Q {\bar{Q}}$$
K
L
...
Amplitude determination for $$M M \rightarrow M M$$, $$M = \pi , K$$ and cross-sections for $$\gamma \gamma \rightarrow \pi ^+ \pi ^-, \pi ^0 \pi ^0, \pi ^0 \eta $$ in a chiral model
Amplitude determination for $$M M \rightarrow M M$$, $$M = \pi , K$$ and cross-sections for $$\gamma \gamma \rightarrow \pi ^+ \pi ^-, \pi ^0 \pi ^0, \pi ^0 \eta $$ in a chiral model
Abstract
Dai and Pennington have performed a comprehensive analysis of essentially all pion and kaon pair production data from two-photon collisions below 1.5 GeV, includ...
Prospects for studies of $${D^{*0}} \rightarrow {\mu ^+}{\mu ^-}$$ and $${B^{{*0}}_{(s)}}\rightarrow {\mu ^+}{\mu ^-}$$ decays
Prospects for studies of $${D^{*0}} \rightarrow {\mu ^+}{\mu ^-}$$ and $${B^{{*0}}_{(s)}}\rightarrow {\mu ^+}{\mu ^-}$$ decays
AbstractWeak decays of the vector $${{D} ^*} ^0$$
D
...
Hadron-Quark Phase Transition in the SU(3) Local Nambu – Jona-Lasinio (NJL) Model with Vector Interaction
Hadron-Quark Phase Transition in the SU(3) Local Nambu – Jona-Lasinio (NJL) Model with Vector Interaction
We study the hadron-quark hybrid equation of state (EOS) of compact-star matter. The Nambu—Jona-Lasinio (NJL) local SU(3) model with vector-type interaction is used to de...
Masses of constituent quarks confined in open bottom hadrons
Masses of constituent quarks confined in open bottom hadrons
We apply color-spin and flavor-spin quark–quark interactions to the meson and baryon constituent quarks, and calculate constituent quark masses, as well as the coupling constants o...

