scholarly journals Perturbative corrections to heavy quark-diquark symmetry predictions for doubly heavy baryon hyperfine splittings

2019 ◽  
Vol 100 (7) ◽  
Author(s):  
Thomas Mehen ◽  
Abhishek Mohapatra
1996 ◽  
Vol 11 (18) ◽  
pp. 1523-1528 ◽  
Author(s):  
X.-H. GUO ◽  
T. MUTA

As heavy baryon ΛQ (Q=b or c) consists of a heavy quark and a scalar light diquark, we establish the Bethe-Salpeter (B-S) equation for ΛQ in the heavy quark limit. With the reasonable kernel we solve the B-S equation numerically and calculate the Isgur-Wise function as Λb→Λc.


1997 ◽  
Vol 403 (3-4) ◽  
pp. 323-328 ◽  
Author(s):  
Hooman Davoudiasl ◽  
Adam K. Leibovich

1996 ◽  
Vol 371 (1-2) ◽  
pp. 99-104 ◽  
Author(s):  
Yuan-ben Dai ◽  
Chao-shang Huang ◽  
Chun Liu ◽  
Cai-dian Lü

2005 ◽  
Vol 20 (10) ◽  
pp. 2099-2117 ◽  
Author(s):  
NIKOLAI URALTSEV

We have calculated the perturbative corrections to all the structure functions in the semileptonic decays of a heavy quark. Assuming an arbitrary gluon mass as a technical tool allowed to obtain in parallel all the BLM corrections. We report the basic applications, viz. perturbative corrections to the hadronic mass and energy moments with full dependence on the charge lepton energy cut. In the adopted scheme with the OPE momentum scale separation around 1 GeV the perturbative corrections to [Formula: see text] are small and practically independent of E cut ; the BLM corrections are small, too. The corrections to the second mass squared moment show some decrease with E cut consistent with the effect of the Darwin operator, within the previously estimated theoretical uncertainty. Perturbative corrections in the pole-type schemes appear significant and vary with Eℓ, decreasing the moments at higher cuts. The hardness of hadronic moments is quantitatively illustrated for different cuts on Eℓ.


2021 ◽  
Vol 81 (7) ◽  
Author(s):  
Feng Feng ◽  
Yu Jia ◽  
Wen-Long Sang

AbstractWithin NRQCD factorization framework, in this work we compute, at the lowest order in velocity expansion, the next-to-leading-order (NLO) perturbative corrections to the short-distance coefficients associated with heavy quark fragmentation into the $${}^1S_0^{(1,8)}$$ 1 S 0 ( 1 , 8 ) components of a heavy quarkonium. Starting from the Collins and Soper’s operator definition of the quark fragmentation function, we apply the sector decomposition method to facilitate the numerical manipulation. It is found that the NLO QCD corrections have a significant impact.


1981 ◽  
Vol 24 (11) ◽  
pp. 3003-3006 ◽  
Author(s):  
W. Buchmüller ◽  
Yee Jack Ng ◽  
S. -H. H. Tye

1998 ◽  
Vol 13 (07) ◽  
pp. 1091-1113 ◽  
Author(s):  
DIETMAR EBERT ◽  
THORSTEN FELDMANN ◽  
CHRISTIANE KETTNER ◽  
HUGO REINHARDT

We describe heavy baryons as bound states of a quark and a diquark. For this purpose we derive the Faddeev equation for baryons containing a single heavy quark from a Nambu–Jona–Lasinio type of model which is appropriately extended to include also heavy quarks. The latter are treated in the heavy mass limit. The heavy baryon Faddeev equation is then solved using a static approximation for the exchanged quark.


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