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Kinetic corrections to B -> X_c l nu at one loop
High Energy Physics - Phenomenology · Submitted 6 Aug 2007
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Together with a two-loop calculation of the leading-power rate and an evaluation of the one-loop corrections to the Wilson coefficient of the chromo-magnetic operator, our results will allow for a high-precision determination of |V_cb| and the b- and c-quark masses.
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The abstract, sentence by sentence
We evaluate the one-loop corrections to the Wilson coefficient of the kinetic operator in the operator product expansion of the differential B -> X_c l nu decay rate. With a moderate cut on the lepton energy, the one-loop terms change the kinetic operator contributions to spectral moments by about 20%. This amounts to a small correction for leptonic and hadronic moments, except for those which vanish at the lowest order, where the effect can be sizable. Together with a two-loop calculation of the leading-power rate and an evaluation of the one-loop corrections to the Wilson coefficient of the chromo-magnetic operator, our results will allow for a high-precision determination of |V_cb| and the b- and c-quark masses.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We evaluate the one-loop corrections to the Wilson coefficient of the kinetic operator in the operator product expansion of the differential B -> X_c l nu decay rate. | contribution 1.00 | 0.95 | 0.08 | asserted 0.99 |
| s1 | With a moderate cut on the lepton energy, the one-loop terms change the kinetic operator contributions to spectral moments by about 20%. | result 1.00 | 0.90 | 0.24 | asserted 1.00 |
| s2 | This amounts to a small correction for leptonic and hadronic moments, except for those which vanish at the lowest order, where the effect can be sizable. | interpretation 0.92 | 0.87 | 0.19 | asserted 0.94 |
| s3 | Together with a two-loop calculation of the leading-power rate and an evaluation of the one-loop corrections to the Wilson coefficient of the chromo-magnetic operator, our results will allow for a high-precision determination of |V_cb| and the b- and c-quark masses. | interpretation 0.81 | 0.68 | 0.43 | hedged possibility 0.59 |
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The paper
Original abstract
We evaluate the one-loop corrections to the Wilson coefficient of the kinetic operator in the operator product expansion of the differential B -> X_c l nu decay rate. With a moderate cut on the lepton energy, the one-loop terms change the kinetic operator contributions to spectral moments by about 20%. This amounts to a small correction for leptonic and hadronic moments, except for those which vanish at the lowest order, where the effect can be sizable. Together with a two-loop calculation of the leading-power rate and an evaluation of the one-loop corrections to the Wilson coefficient of the chromo-magnetic operator, our results will allow for a high-precision determination of |V_cb| and the b- and c-quark masses.
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References
How the literature uses it
38 arXiv papers cite this in 47 sentences
Papers citing it · 34 sentences without a confident label
Compares with it 1 paper
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We have confirmed the numerical results presented in [ref] and reproduced the RI relations given by Manohar [ref] .
Kinetic operator effects in B-> X_c l nu at O(alpha_s) · Summary · 0.97
Cites it as background 11 papers
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The relations for differential distributions and moments tend to be more intricate, see [ref] , especially in the presence of experimental cuts.
Kinetic operator effects in B-> X_c l nu at O(alpha_s) · Reparameterization Invariance relations · 0.84
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Lepton energy moments and moments of hadronic invariant mass have been extensively measured at $B$ factories and their prediction is know up to next-to-next-to leading order (NNLO) for free quarks [ref] , and next-to-leading order (NLO) at order $1/m_b^2$ [ref] .
A first glance to the kinematic moments of $B \to X_c \ell \nu$ at third order · Introduction · 0.80
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Current state-of-the-art analysis are theoretical calculations up to $O(α_s^2)$ [ref] , the mixed $O(α_s / m_b )$ [ref] and $O(1/m_b^5)$ non-perturbative corrections; the results for $1/m_b^3$ have been known [ref] for quiet some time, while the calculations of $1/m_b^4$ [ref] and $1/m_b^5$ [ref] including investigations concerning subtleties due to the heavy final state quark “intrinsic-charm” [ref] have lately been performed.
Additional Information on Heavy Quark Parameters from Charged Lepton Forward-Backward Asymmetry · Introduction · 0.83
What it cites · 44 sentences without a confident label
Contests 1 paper
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In the fit of [ref] , the corrections are underestimated to be $α_s/4πΛ_QCD^2/m_b^2∼0.0002$: the contributions we find are roughly ten times larger.
Global analysis of inclusive B decays · Results for the moments of the differential rate · contest 0.83
Uses the method or tool of 2 papers
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Using heavy-quark effective theory (HQET) [ref] , all the matrix elements necessary to second order in the expansion can be reduced to [equation] The HQET parameter $μ_π^2$ is often denoted by $-λ_1$ and is not renormalized.
Heavy Quark Symmetry · Evaluation of the kinetic corrections · 0.93
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A definition of the axial current in $d$ dimensions suitable for our purposes has been given by Larin [ref] and we adopt it for our calculation.
The renormalization of the axial anomaly in dimensional regularization · Evaluation of the kinetic corrections · 1.00
Compares with 1 paper
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As a byproduct of our analysis, we obtain the $O(α_s)$ corrections to the leading-power moments and reproduce the numerical results of [ref] .
Perturbative corrections to semileptonic b decay distributions · Introduction · 0.98
Cites as background 7 papers
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Schematically, the decay rate takes the form [ref] [equation] where $ρ=m_c^2/m_b^2$.
QCD Predictions for Lepton Spectra in Inclusive Heavy Flavour Decays · Introduction · 0.92
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Schematically, the decay rate takes the form [ref] [equation] where $ρ=m_c^2/m_b^2$.
Differential Distributions in Semileptonic Decays of the Heavy Flavors in QCD · Introduction · 0.92
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Schematically, the decay rate takes the form [ref] [equation] where $ρ=m_c^2/m_b^2$.
Inclusive Semileptonic B and Polarized Lambda_b Decays from QCD · Introduction · 0.92
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