scholarly journals Heavy quark symmetry and weak decays of thebbaryons in pentaquarks with acc¯component

2016 ◽  
Vol 94 (5) ◽  
Author(s):  
Ahmed Ali ◽  
Ishtiaq Ahmed ◽  
M. Jamil Aslam ◽  
Abdur Rehman
Pramana ◽  
1996 ◽  
Vol 47 (3) ◽  
pp. 261-261
Author(s):  
A K Giri ◽  
L Maharana ◽  
R Mohanta

1997 ◽  
Vol 12 (03) ◽  
pp. 195-204 ◽  
Author(s):  
Debrupa Chakraverty ◽  
Triptesh De ◽  
Binayak Dutta-Roy ◽  
K. S. Gupta

We calculate the decay width for [Formula: see text] in the framework of a non-relativistic quark (NRQ) model of heavy baryons where the light quarks play the role of spectators. Our calculation does not make an explicit use of the heavy quark symmetry. The branching ratio for the above process as calculated here agrees reasonably well with the experimental value.


B Decays ◽  
1994 ◽  
pp. 231-282 ◽  
Author(s):  
Nathan Isgur ◽  
Mark B. Wise

1993 ◽  
Vol 47 (3) ◽  
pp. 1007-1020 ◽  
Author(s):  
Cathy Reader ◽  
Nathan Isgur

Pramana ◽  
1996 ◽  
Vol 47 (5) ◽  
pp. 411-417 ◽  
Author(s):  
A K Giri ◽  
L Maharana ◽  
R Mohanta

2015 ◽  
Vol 30 (10) ◽  
pp. 1543005 ◽  
Author(s):  
Alexander Lenz

Kolya Uraltsev was one of the inventors of the Heavy Quark Expansion (HQE), that describes inclusive weak decays of hadrons containing heavy quarks and in particular lifetimes. Besides giving a pedagogic introduction to the subject, we review the development and the current status of the HQE, which just recently passed several non-trivial experimental tests with an unprecedented precision. In view of many new experimental results for lifetimes of heavy hadrons, we also update several theory predictions: [Formula: see text], τ(Bs)/τ(Bd) = 1.001 ±0.002, τ(Λb)/τ(Bd) = 0.935 ±0.054 and [Formula: see text]. The theoretical precision is currently strongly limited by the unknown size of the non-perturbative matrix elements of four-quark operators, which could be determined with lattice simulations.


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