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Related papers: Bottom Quark Mass Determination from low-n Sum Rul…

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I report here on the (first) direct extraction of the running charm quark mass m_c(\nu) from the D-meson sum rules, and on the implications of this result for the estimate of the leptonic decay constants f_{D_s}. The outputs:…

High Energy Physics - Phenomenology · Physics 2009-10-31 Stephan Narison

We present an update of neutral Higgs boson decays into bottom quark pairs in the minimal supersymmetric extension of the Standard Model. In particular the resummation of potentially large higher-order corrections due to the soft SUSY…

High Energy Physics - Phenomenology · Physics 2009-11-10 Jaume Guasch , Petra Häfliger , Michael Spira

Considering nonforward scattering amplitude off the heavy quark in the Small Velocity limit two exact superconvergent sum rules are derived. The first sum rule leads to the lower bound \rho^2 > 3/4 for the slope of the Isgur-Wise function.…

High Energy Physics - Phenomenology · Physics 2009-10-31 Nikolai Uraltsev

I extract the strange-quark mass using a $\tau$-like decay sum rule for the $\phi$-meson, and some other sum rules involving its difference with the vector component of the hadronic $\tau$-decay. As a conservative estimate, one obtains to…

High Energy Physics - Phenomenology · Physics 2008-11-26 Stephan Narison

We summarize recently improved results for the pseudoscalar [1,2] and vector [3] meson decay constants and their ratios from QCD spectral sum rules where N2LO + estimate of the N3LO PT and power corrections up to d< 6 dimensions have been…

High Energy Physics - Phenomenology · Physics 2015-12-01 Stephan Narison

We propose a new method to extract the light quark mass ratio $m_u/m_d$ using the $\Upsilon(4S)\to h_b\pi^0(\eta)$ bottomonia transitions. The decay amplitudes are dominated by the light quark mass differences, and the corrections from…

High Energy Physics - Phenomenology · Physics 2010-10-18 Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner

In this work, the charm quark mass is obtained from a QCD sum rule analysis of the charmonium system. In our investigation we include results from non-relativistic QCD at next-to-next-to-leading order. Using the pole mass scheme, we obtain…

High Energy Physics - Phenomenology · Physics 2009-10-31 Markus Eidemuller , Matthias Jamin

The upper bond on the branching ratio for $b\to s\gamma$ decays implies a stringent lower bound on the mass of the pseudoscalar Higgs boson of the MSSM if sparticles are heavy. This leads to an upper bound on the expected event rate in…

High Energy Physics - Phenomenology · Physics 2016-09-01 M. Drees

In hadronic decays of Z bosons recorded with the OPAL detector at LEP, events containing b quarks were selected using the long lifetime of b flavoured hadrons. Comparing the 3-jet rate in b events with that in d,u,s and c quark events, a…

High Energy Physics - Experiment · Physics 2010-05-28 The OPAL collaboration , G. Abbiendi

We use QCD spectral sum rules (QSSR) and the factorization properties of molecule currents to estimate the masses and couplings of the $\bar D^*D$ and $\bar B^*B~(1^{++})$ molecules at N2LO of PT QCD. We include in the OPE the contributions…

High Energy Physics - Phenomenology · Physics 2014-10-01 F. Fanomezana , S. Narison , A. Rabemananjara

Present experiments in pursuit of the mass difference in the Bs-Bs(bar) system have put a lower bound on this quantity of $\Delta M_s > 14.9 ps^{-1}$ (at 95% C.L.). The same experiments also yield a local minimum in the log-likelihood…

High Energy Physics - Phenomenology · Physics 2009-01-07 A. Ali , D. London

We re-examine the use of sum rules in the extraction of light quark masses and discuss a number of potential problems with existing analyses. The most important issue is that of the overall normalization of the hadronic spectral functions…

High Energy Physics - Phenomenology · Physics 2009-09-25 Tanmoy Bhattacharya , Rajan Gupta , Kim Maltman

The value of $\alpha_s(m_Z)=0.106\pm 0.005$ is obtained in a scheme of sum rules for the leptonic constants of the vector $nS$-levels in the heavy $(\bar b b)$-quarkonium.

High Energy Physics - Phenomenology · Physics 2007-05-23 V. V. Kiselev

In these proceedings we discuss the relation between the kinetic and the on-shell schemes for the bottom and the charm quarks and present the methods for the calculation of the mass relation to higher orders in perturbative QCD. The bottom…

High Energy Physics - Phenomenology · Physics 2021-10-26 Matteo Fael

Precision tests of the CKM mechanism and searches for new physics in the flavour sector require dedicated QCD calculations of decay widths and spectra. Significant progress has been achieved in recent years in computing inclusive B decay…

High Energy Physics - Phenomenology · Physics 2008-06-30 Einan Gardi

The strange quark mass is determined from a QCD Finite Energy Sum Rule (FESR) optimized to reduce considerably the systematic uncertainties arising from the hadronic resonance sector, as well as from the poor convergence of the pseudoscalar…

High Energy Physics - Phenomenology · Physics 2013-06-28 Sebastian Bodenstein , Cesareo A. Dominguez , Karl Schilcher

Diquarks with $J^{P}=0^{\pm}$, $1^{\pm}$ containing a heavy (charm or bottom) quark and a light quark are investigated using QCD Laplace sum rules. Masses are determined using appropriately constructed gauge invariant correlation functions,…

High Energy Physics - Phenomenology · Physics 2013-06-17 R. T. Kleiv , T. G. Steele , Ailin Zhang , Ian Blokland

In this paper, we reanalyze the $I=0$ scalar channel with the improved Monte-Carlo based QCD sum rules, which combines the rigorous H\"older-inequality-determined sum rule window and a two Breit-Wigner type resonances parametrization for…

High Energy Physics - Phenomenology · Physics 2017-08-09 Jia-Min Yuan , Zhu-Feng Zhang , T. G. Steele , Hong-Ying Jin , Zhuo-Ran Huang

In the framework of the MSSM the non-universal boundary conditions of soft SUSY breaking parameters are considered. Taking as input the top, bottom and Z-boson masses, the values of the gauge couplings at the EW scale and the infrared…

High Energy Physics - Phenomenology · Physics 2011-01-27 S. Codoban , M. Jurcisin , D. Kazakov

The charm quark's mass is determined from Monte Carlo calculations of the $\bar{c}c$ spectrum. The main sources of uncertainty are perturbation theory (for conversion to $\MSbar$), the continuum-limit extrapolation, Monte Carlo statistics,…

High Energy Physics - Lattice · Physics 2008-11-26 Andreas S. Kronfeld
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