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Related papers: The $\Upsilon$ and $\Upsilon^{\prime}$ Leptonic Wi…

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As tests of QCD in the bottomonium system, we give the most accurate results to date for the ground-state hyperfine splitting and the $\Upsilon$ leptonic width from full lattice QCD. These quantities are both accurately known from…

High Energy Physics - Lattice · Physics 2021-11-12 C. T. H. Davies , D. Hatton , J. Koponen , G. P. Lepage , A. T. Lytle

We calculate the mass difference between the $\Upsilon$ and $\eta_b$ and the $\Upsilon$ leptonic width from lattice QCD using the Highly Improved Staggered Quark formalism for the $b$ quark and including $u$, $d$, $s$ and $c$ quarks in the…

High Energy Physics - Lattice · Physics 2021-03-31 D. Hatton , C. T. H. Davies , J. Koponen , G. P. Lepage , A. T. Lytle

The HPQCD collaboration has used radiatively-improved NonRelativistic QCD (NRQCD) for $b$ quarks in bottomonium to determine the decay rate of $\Upsilon$ and $\Upsilon^\prime$ mesons to leptons in lattice QCD. Using time-moments of vector…

High Energy Physics - Lattice · Physics 2015-11-06 Brian Colquhoun , Christine T. H. Davies , Rachel J. Dowdall , Jonna Koponen , G. Peter Lepage , Andrew T. Lytle

We present a calculation of the hindered M$1$ $\Upsilon(2S) \to \eta_b(1S) \gamma$ decay rate using lattice non-relativistic QCD. The calculation includes spin-dependent relativistic corrections to the NRQCD action through…

High Energy Physics - Lattice · Physics 2015-11-11 Ciaran Hughes , Rachel J. Dowdall , Christine T. H. Davies , Ronald R. Horgan , Georg von Hippel , Matthew Wingate

We present the complete next-to-next-to-next-to-leading order short-distance and bound-state QCD correction to the leptonic decay rate Gamma(Upsilon(1S)->l+l-) of the lowest-lying spin-1 bottomonium state. The perturbative QCD prediction is…

High Energy Physics - Phenomenology · Physics 2014-04-24 Martin Beneke , Yuichiro Kiyo , Peter Marquard , Alexander Penin , Jan Piclum , Dirk Seidel , Matthias Steinhauser

Recent results from lattice QCD simulations provide a realistic picture, based upon first principles, of~$\Upsilon$ physics. We combine these results with the experimentally measured mass of the $\Upsilon$~meson to obtain an accurate and…

High Energy Physics - Lattice · Physics 2009-10-22 C. T. H. Davies , K. Hornbostel , A. Langnau , G. P. Lepage , A. Lidsey , C. J. Morningstar , J. Shigemitsu , J. Sloan

We calculate the J/{\psi} mass, leptonic width and radiative decay rate to \gamma \eta_c from lattice QCD including u, d and s quarks in the sea for the first time. We use the Highly Improved Staggered Quark formalism and nonperturbatively…

High Energy Physics - Lattice · Physics 2013-05-30 G. C. Donald , C. T. H. Davies , R. J. Dowdall , E. Follana , K. Hornbostel , J. Koponen , G. P. Lepage , C. McNeile

We give results for the Upsilon spectrum from lattice QCD using an improved version of the NRQCD action for b quarks which includes radiative corrections to kinetic terms at O(v^4) in the velocity expansion. We also include for the first…

We show results for the Upsilon spectrum calculated in lattice QCD including for the first time vacuum polarization effects for light u and d quarks as well as s quarks. We use gluon field configurations generated by the MILC collaboration.…

High Energy Physics - Lattice · Physics 2008-11-26 A. Gray , I. Allison , C. T. H. Davies , E. Gulez , G. P. Lepage , J. Shigemitsu , M. Wingate

The spectrum of the Upsilon system is investigated using the Nonrelativistic Lattice QCD approach to heavy quarks and ignoring light quark vacuum polarization. We find good agreement with experiment for the Upsilon(1S), Upsilon(2S),…

High Energy Physics - Lattice · Physics 2011-01-27 C. T. H. Davies , K. Hornbostel , A. Langnau , G. P. Lepage , A. Lidsey , J. Shigemitsu , J. Sloan

We describe a recent lattice-QCD calculation of the leptonic decay constants of heavy-light pseudoscalar mesons containing charm and bottom quarks and of the masses of the up, down, strange, charm, and bottom quarks. Results for these…

We give the first accurate results for $B$ and $B_s$ meson masses from lattice QCD including the effect of $u$, $d$ and $s$ sea quarks, and we improve an earlier value for the $B_c$ meson mass. By using the Highly Improved Staggered Quark…

We extend the picture of $B$-meson decay constants obtained in lattice QCD beyond those of the $B$, $B_s$ and $B_c$ to give the first full lattice QCD results for the $B^*$, $B^*_s$ and $B^*_c$. We use improved NonRelativistic QCD for the…

High Energy Physics - Lattice · Physics 2015-07-01 B. Colquhoun , C. T. H. Davies , R. J. Dowdall , J. Kettle , J. Koponen , G. P. Lepage , A. T. Lytle

We calculate the decay rate for $\eta_b \to \gamma \gamma$ in lattice QCD for the first time, providing a precise prediction for the Belle II experiment. Our calculation includes $u$, $d$, $s$ and $c$ quarks in the sea, using gluon field…

High Energy Physics - Lattice · Physics 2025-12-19 Brian Colquhoun , Christine T. H. Davies , G. Peter Lepage

Theoretical predictions for B decay rates are rewritten in terms of the Upsilon(1S) meson mass instead of the b quark mass, using a modified perturbation expansion. The theoretical consistency of this expansion is shown both at low and high…

High Energy Physics - Phenomenology · Physics 2009-10-31 Andre H. Hoang , Zoltan Ligeti , Aneesh V. Manohar

We present the results of our lattice QCD computation of the hadronic matrix elements relevant to the $h_{c}\to \eta_{c}\gamma$ and $h_{b}\to \eta_{b}\gamma$ decays by using the gauge configurations produced by the Extended Twisted Mass…

High Energy Physics - Lattice · Physics 2025-04-24 D. Bečirević , R. Di Palma , R. Frezzotti , G. Gagliardi , V. Lubicz , F. Sanfilippo , N. Tantalo

We include two loop, relativistic one loop and second order relativistic tree level corrections, plus leading nonperturbative contributions, to obtain a calculation of the lower states in the heavy quarkonium spectrum correct up to, and…

High Energy Physics - Phenomenology · Physics 2011-01-27 A. Pineda , F. J. Yndurain

We discuss \(B_c\) mass (1S state) and decay constant \(f_{B_c}\) calculated by lattice non-relativistic quantum chromodynamcs(NRQCD) method. In leading order of \(v^2\), we found that \(M_{B_c} = 6.33(2)\) GeV and \(f_{B_c} = 395(2)\) MeV…

High Energy Physics - Lattice · Physics 2007-05-23 Seyong Kim

The leading electromagnetic (e.m.) and strong isospin-breaking corrections to the $\pi^+ \to \mu^+ \nu[\gamma]$ and $K^+ \to \mu^+ \nu[\gamma]$ leptonic decay rates are evaluated for the first time on the lattice. The results are obtained…

High Energy Physics - Lattice · Physics 2019-10-25 M. Di Carlo , D. Giusti , V. Lubicz , G. Martinelli , C. T. Sachrajda , F. Sanfilippo , S. Simula , N. Tantalo

We update our previous determination of both the decay constant and the mass of the $D_s$ meson using the Highly Improved Staggered Quark formalism. We include additional results at two finer values of the lattice spacing along with…

High Energy Physics - Lattice · Physics 2010-12-24 C. T. H. Davies , C. McNeile , E. Follana , G. P. Lepage , H. Na , J. Shigemitsu
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