Subleading Isgur-Wise Function of $\Lambda_b\to\Lambda_{c1}$ using QCD sum rules
Phys.Lett. B552 (2003) 185-197 Subleading Isgur-Wise form factor $\tau(v\cdot v')$ at ${\cal O}(1/m_Q)$ for $\Lambda_b\to\Lambda_{c1}^{1/2,3/2}$ weak transition is calculated by using the QCD sum rules in the framework of the heavy quark effective theory (HQET), where $\Lambda^{1/2}_{c1}$ and $...
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Main Authors | , |
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Format | Journal Article |
Language | English |
Published |
07.10.2002
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Subjects | |
Online Access | Get full text |
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Summary: | Phys.Lett. B552 (2003) 185-197 Subleading Isgur-Wise form factor $\tau(v\cdot v')$ at ${\cal O}(1/m_Q)$ for
$\Lambda_b\to\Lambda_{c1}^{1/2,3/2}$ weak transition is calculated by using the
QCD sum rules in the framework of the heavy quark effective theory (HQET),
where $\Lambda^{1/2}_{c1}$ and $\Lambda^{3/2}_{c1}$ are the orbitally excited
charmed baryon doublet with $J^P=(1^-/2,3^-/2)$. We consider the subleading
contributions from the weak current matching in the HQET. The interpolating
currents with transverse covariant derivative are adopted for
$\Lambda^{1/2}_{c1}$ and $\Lambda^{3/2}_{c1}$ in the analysis. The slope
parameter $\rho^2$ in linear approximation of $\tau$ is obtained to be
$\rho^2=2.76$ and the interception to be $\tau(1)=-1.27$ GeV. |
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DOI: | 10.48550/arxiv.hep-ph/0210097 |