Constraints on higher-order perturbative corrections in b → u semileptonic decays from residual renormalization-scale dependence

The constraint of a progressive decrease in residual renormalization scale dependence with increasing loop order is developed as a method for obtaining bounds on unknown higher-order perturbative corrections to renormalization-group-invariant quantities. This technique is applied to the inclusive semileptonic process b → ull− (explicitly known to two-loop order) in order to obtain bounds on the three- and four-loop perturbative contributions that are not accessible via the renormalization group. Combining this technique with the principle of minimal sensitivity, we obtain an estimate for the perturbative contributions to Γ(b → ull−) that incorporates theoretical uncertainty from as-yet-undetermined higher-order QCD corrections.

[1]  F. Chishtie,et al.  Three Loop Estimate of the Inclusive Semileptonic b → c Decay Rate , 2001, hep-ph/0109061.

[2]  D. Broadhurst,et al.  Renormalons and multi-loop estimates in scalar correlators, Higgs decay and quark-mass sum rules. , 2000, hep-ph/0007152.

[3]  K. Melnikov,et al.  The three-loop relation between the and the pole quark masses , 1999, hep-ph/9912391.

[4]  F. Chishtie,et al.  Estimate of the three loop perturbative contribution to inclusive semileptonic b ---> u decays , 1999, hep-ph/9910551.

[5]  M. Steinhauser,et al.  Short distance mass of a heavy quark at order $\alpha_s^3$ , 1999, hep-ph/9907509.

[6]  T. V. Ritbergen The second order QCD contribution to the semileptonic b -> u decay rate , 1999, hep-ph/9903226.

[7]  F. Chishtie,et al.  Asymptotic Padé-approximant methods and QCD current correlation functions , 1998, hep-ph/9812498.

[8]  F. Chishtie,et al.  Pade-Improvement of QCD Running Coupling Constants, Running Masses, Higgs Decay Rates, and Scalar Channel Sum Rules , 1998, hep-ph/9806324.

[9]  A. Hoang Bottom Quark Mass from Upsilon Mesons , 1998, hep-ph/9803454.

[10]  M. Karliner,et al.  Asymptotic Pade approximant predictions: Up to five loops in QCD and SQCD , 1997, hep-ph/9710302.

[11]  B. Kniehl,et al.  Decoupling relations to O(a s 3) and their connection to low-energy theorems , 1997, hep-ph/9708255.

[12]  J.A.M. Vermaseren,et al.  The 4-loop quark mass anomalous dimension and the invariant quark mass , 1997, hep-ph/9703284.

[13]  T. V. Ritbergen,et al.  The four-loop β-function in quantum chromodynamics , 1997, hep-ph/9701390.

[14]  M. Karliner,et al.  A Prediction for the 4-Loop \beta Function , 1996, hep-ph/9612202.

[15]  Hayes,et al.  Review of Particle Physics. , 1996, Physical review. D, Particles and fields.

[16]  Ball,et al.  Resummation of running coupling effects in semileptonic B meson decays and extraction of ||Vcb|| , 1995, Physical review. D, Particles and fields.

[17]  M. Beneke,et al.  Naive nonabelianization and resummation of fermion bubble chains , 1994, hep-ph/9411229.

[18]  G. Grunberg Renormalization-scheme-invariant QCD and QED: The method of effective charges , 1984 .

[19]  P. Stevenson Optimized Perturbation Theory , 1981 .

[20]  P. Stevenson Resolution of the renormalisation-scheme ambiguity in perturbative QCD , 1981 .

[21]  G. Grunberg Renormalization group improved perturbative QCD , 1980 .