We complete the leading-log renormalization group scaling of the nonrelativistic (NRQCD) Lagrangian at O ( 1 / m 2 ) . The next-to-next-to-leading-log renormalization group scaling of the potential NRQCD Lagrangian (as far as the singlet is concerned) is also obtained in the situation m α s ≫ Λ QCD . As a by-product, we obtain the heavy quarkonium spectrum with the same accuracy in the situation m α 2 s ≳ Λ QCD . When Λ QCD ≪ m α 2 s , this is equivalent to obtain the whole set of O ( m α ( n + 4 ) s ln n α s ) terms in the heavy quarkonium spectrum. The implications of our results in the nonperturbative situation m α s ∼ Λ QCD are also mentioned
Rare decays of B mesons, such as B \to K^*\gamma and B\to K^{(*)}\ell^+\ell^- are loop suppressed in...
We discuss recent theoretical developments concerning the description of the production and decay of...
We review recent progress in Non-Relativistic QCD and in related Non-Relativistic Effective Field Th...
In the framework of potential NRQCD, we obtain the next-to-leading-log renormalization-group running...
In the framework of potential NRQCD, we obtain the next-to-leading-log renormalization-group running...
We discuss the matching conditions and renormalization group evolution of non-relativistic QCD. A va...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting, u...
In this talk I review the calculation of the third order corrections to the heavy quarkonium spectru...
We discuss the form and construction of general color singlet heavy particle-antiparticle pair produ...
We review some recent developments on non-relativistic effective field theories for heavy quark-anti...
We review the recent theoretical progress in heavy quarkonium spectroscopy within the boundstate the...
In the framework of potential NRQCD, we obtain the next-to-leading-log renormalization-group running...
A new derivation of the effective lagrangian for non-relativistic quantum chromodynamics and the hea...
The order 1/v contribution to the heavy quark potential is first generated at one-loop order in QCD....
The matching coefficients for the four-quark operators in NRQCD (NRQED) are calculated at one loop u...
Rare decays of B mesons, such as B \to K^*\gamma and B\to K^{(*)}\ell^+\ell^- are loop suppressed in...
We discuss recent theoretical developments concerning the description of the production and decay of...
We review recent progress in Non-Relativistic QCD and in related Non-Relativistic Effective Field Th...
In the framework of potential NRQCD, we obtain the next-to-leading-log renormalization-group running...
In the framework of potential NRQCD, we obtain the next-to-leading-log renormalization-group running...
We discuss the matching conditions and renormalization group evolution of non-relativistic QCD. A va...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting, u...
In this talk I review the calculation of the third order corrections to the heavy quarkonium spectru...
We discuss the form and construction of general color singlet heavy particle-antiparticle pair produ...
We review some recent developments on non-relativistic effective field theories for heavy quark-anti...
We review the recent theoretical progress in heavy quarkonium spectroscopy within the boundstate the...
In the framework of potential NRQCD, we obtain the next-to-leading-log renormalization-group running...
A new derivation of the effective lagrangian for non-relativistic quantum chromodynamics and the hea...
The order 1/v contribution to the heavy quark potential is first generated at one-loop order in QCD....
The matching coefficients for the four-quark operators in NRQCD (NRQED) are calculated at one loop u...
Rare decays of B mesons, such as B \to K^*\gamma and B\to K^{(*)}\ell^+\ell^- are loop suppressed in...
We discuss recent theoretical developments concerning the description of the production and decay of...
We review recent progress in Non-Relativistic QCD and in related Non-Relativistic Effective Field Th...