${\mathit {\mathit b}}$-QUARK MASS INSPIRE search

2020

THEO

$4.049$ ${}^{+0.138}_{-0.118}$

⁴

HERA

$4.195$ $\pm0.014$

⁵

BAZAVOV

LATT

$4.186$ $\pm0.037$

⁶

PESET

THEO

$4.197$ $\pm0.022$

⁷

KIYO

2016

THEO

$4.183$ $\pm0.037$

⁸

ALBERTI

THEO

$4.203$ ${}^{+0.016}_{-0.034}$

⁹

BENEKE

THEO

$4.196$ $\pm0.023$

¹⁰

COLQUHOUN

LATT

$4.176$ $\pm0.023$

¹¹

DEHNADI

THEO

$4.21$ $\pm0.11$

¹²

BERNARDONI

LATT

$4.169$ $\pm0.002$ $\pm0.008$

¹³

THEO

$4.166$ $\pm0.043$

¹⁴

LEE

LATT

$4.247$ $\pm0.034$

¹⁵

LUCHA

THEO

$4.171$ $\pm0.009$

¹⁶

BODENSTEIN

THEO

$4.29$ $\pm0.14$

¹⁷

DIMOPOULOS

LATT

$4.18$ ${}^{+0.05}_{-0.04}$

¹⁸

LASCHKA

2011

THEO

$4.186$ $\pm0.044$ $\pm0.015$

¹⁹

BABR

$4.163$ $\pm0.016$

²⁰

CHETYRKIN

2009

THEO

$4.243$ $\pm0.049$

²¹

SCHWANDA

BELL

• • • We do not use the following data for averages, fits, limits, etc. • • •

$4.184$ $\pm0.011$

²²

THEO

$4.188$ $\pm0.008$

²³

THEO

$4.07$ $\pm0.17$

²⁴

ZEUS

$4.201$ $\pm0.043$

²⁵

AYALA

THEO

$4.236$ $\pm0.069$

²⁶

THEO

$4.213$ $\pm0.059$

²⁷

THEO

$4.235$ $\pm0.003$ $\pm0.055$

²⁸

THEO

$4.212$ $\pm0.032$

²⁹

THEO

$4.177$ $\pm0.011$

³⁰

THEO

$4.171$ $\pm0.014$

³¹

THEO

$4.164$ $\pm0.023$

³²

LATT

$4.173$ $\pm0.010$

³³

THEO

$5.26$ $\pm1.2$

³⁴

DLPH

$4.42$ $\pm0.06$ $\pm0.08$

³⁵

GUAZZINI

LATT

$4.347$ $\pm0.048$ $\pm0.08$

³⁶

DELLA-MORTE

LATT

$4.164$ $\pm0.025$

³⁷

KUHN

THEO

$4.19$ $\pm0.40$

³⁸

DLPH

$4.205$ $\pm0.058$

³⁹

BOUGHEZAL

THEO

$4.20$ $\pm0.04$

⁴⁰

BUCHMUELLER

THEO

$4.19$ $\pm0.06$

⁴¹

PINEDA

THEO

$4.4$ $\pm0.3$

⁴²

GRAY

2005

LATT

$4.22$ $\pm0.06$

⁴³

THEO

$4.17$ $\pm0.03$

⁴⁴

THEO

$4.22$ $\pm0.11$

⁴⁵

THEO

$4.25$ $\pm0.11$

⁴⁶

LATT

$4.22$ $\pm0.09$

⁴⁷

THEO

$4.19$ $\pm0.05$

⁴⁸

BORDES

THEO

$4.20$ $\pm0.09$

⁴⁹

CORCELLA

THEO

$4.33$ $\pm0.10$

⁵⁰

DEDIVITIIS

LATT

$4.24$ $\pm0.10$

⁵¹

EIDEMULLER

THEO

$4.207$ $\pm0.03$

⁵²

ERLER

THEO

$4.33$ $\pm0.06$ $\pm0.10$

⁵³

MAHMOOD

CLEO

$4.190$ $\pm0.032$

⁵⁴

BRAMBILLA

THEO

$4.346$ $\pm0.070$

⁵⁵

THEO

¹ APARISI 2022 determine ${{\mathit m}_{{{b}}}}$ at the Higgs mass, ${{\overline{\mathit m}}_{{{b}}}}({{\mathit m}_{{{H}}}}$) = $2.60$ ${}^{+0.36}_{-0.31}$ GeV from Higgs boson decay rates at the LHC, which is used to obtain ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$).

² HATTON 2021 determine ${{\overline{\mathit m}}_{{{b}}}}$(3 GeV) = $4.513$ $\pm0.026$ GeV using a lattice QCD + quenched QED simulation using the HISQ action and including ${{\mathit n}_{{{f}}}}$ = 2+1+1 flavors of sea quarks, by combining their ${{\overline{\mathit m}}_{{{b}}}}/{{\overline{\mathit m}}_{{{c}}}}$ and ${{\overline{\mathit m}}_{{{c}}}}$ determinations.

³ NARISON 2020 determines the quark mass using QCD Laplace sum rules from the ${{\mathit B}_{{{c}}}}$ mass, combined with previous determinations of the QCD condensates and ${\mathit {\mathit c}}$ and ${\mathit {\mathit b}}$ masses.

⁴ ABRAMOWICZ 2018 determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) = $4.049$ ${}^{+0.104}_{-0.109}{}^{+0.090}_{-0.032}{}^{+0.001}_{-0.031}$ from the production of ${\mathit {\mathit b}}$ quarks in ${{\mathit e}}{{\mathit p}}$ collisions at HERA using combined H1 and ZEUS data. The experimental/fitting errors, and those from modeling and parameterization have been combined in quadrature.

⁵ BAZAVOV 2018 determine the ${\mathit {\mathit b}}$ mass using a lattice computation with staggered fermions and five active quark flavors.

⁶ PESET 2018 determine ${{\overline{\mathit m}}_{{{c}}}}({{\overline{\mathit m}}_{{{c}}}}$) and ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) using an N3LO calculation of the ${{\mathit \eta}_{{{c}}}}$, ${{\mathit \eta}_{{{b}}}}$ and ${{\mathit B}_{{{c}}}}$ masses.

⁷ KIYO 2016 determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) from the ${{\mathit \Upsilon}{(1S)}}$ mass at order ${{\mathit \alpha}_{{{s}}}^{3}}$ (N3LO).

⁸ ALBERTI 2015 determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) from fits to inclusive ${{\mathit B}}$ $\rightarrow$ ${{\mathit X}_{{{c}}}}{{\mathit e}}{{\overline{\mathit \nu}}}$ decay. They also find ${{\mathit m}}{}^{{\mathrm {kin}}}_{b}$(1 GeV) = $4.553$ $\pm0.020$ GeV.

⁹ BENEKE 2015 determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) using sum rules for ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons at order N3LO including finite ${\mathit m}_{{{\mathit c}}}$ effects. They find ${{\mathit m}}{}^{{\mathrm {PS}}}_{b}$(2 GeV) = $4.532$ ${}^{+0.013}_{-0.039}$ GeV, and ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) = $4.193$ ${}^{+0.022}_{-0.035}$ GeV. The value quoted is obtained using the four-loop conversion given in BENEKE 2016.

¹⁰ COLQUHOUN 2015 determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) from moments of the vector current correlator computed with a lattice simulation using the NRQCD action.

¹¹ DEHNADI 2015 determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) using sum rules for ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons at order ${{\mathit \alpha}_{{{s}}}^{3}}$ (N3LO), and fitting to both experimental data and lattice results.

¹² BERNARDONI 2014 determine ${{\mathit m}_{{{b}}}}$ from ${{\mathit n}_{{{f}}}}$ = 2 lattice calculations using heavy quark effective theory non-perturbatively renormalized and matched to QCD at 1/$\mathit m$ order.

¹³ PENIN 2014 determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) = $4.169$ $\pm0.008$ $\pm0.002$ $\pm0.002$ using an estimate of the order ${{\mathit \alpha}_{{{s}}}^{3}}{\mathit {\mathit b}}$-quark vacuum polarization function in the threshold region, including finite ${\mathit m}_{{{\mathit c}}}$ effects. The errors of $\pm0.008$ from theoretical uncertainties, and $\pm0.002$ from ${{\mathit \alpha}_{{{s}}}}$ have been combined in quadrature.

¹⁴ LEE 2013O determines ${\mathit m}_{{{\mathit b}}}$ using lattice calculations of the ${{\mathit \Upsilon}}$ and ${{\mathit B}_{{{s}}}}$ binding energies in NRQCD, including three light dynamical quark flavors. The quark mass shift in NRQCD is determined to order ${{\mathit \alpha}_{{{s}}}^{2}}$, with partial ${{\mathit \alpha}_{{{s}}}^{3}}$ contributions.

¹⁵ LUCHA 2013 determines ${\mathit m}_{{{\mathit b}}}$ from QCD sum rules for heavy-light currents using the lattice value for ${{\mathit f}_{{{B}}}}$ of $191.5$ $\pm7.3$ GeV.

¹⁶ BODENSTEIN 2012 determine ${\mathit m}_{{{\mathit b}}}$ using sum rules for the vector current correlator and the ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit Q}}{{\overline{\mathit Q}}}$ total cross-section.

¹⁷ DIMOPOULOS 2012 determine quark masses from a lattice computation using ${{\mathit n}_{{{f}}}}$ = 2 dynamical flavors of twisted mass fermions.

¹⁸ LASCHKA 2011 determine the ${{\mathit b}}$ mass from the charmonium spectrum. The theoretical computation uses the heavy potential to order 1/${\mathit m}_{{{\mathit Q}}}$ obtained by matching the short-distance perturbative result onto lattice QCD result at larger scales.

¹⁹ AUBERT 2010A determine the ${\mathit {\mathit b}}$- and ${\mathit {\mathit c}}$-quark masses from a fit to the inclusive decay spectra in semileptonic ${{\mathit B}}$ decays in the kinetic scheme (and convert it to the $\overline{\rm{}MS}$ scheme).

²⁰ CHETYRKIN 2009 determine ${\mathit m}_{{{\mathit c}}}$ and ${\mathit m}_{{{\mathit b}}}$ from the ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit Q}}{{\overline{\mathit Q}}}$ cross-section and sum rules, using an order ${{\mathit \alpha}_{{{s}}}^{3}}$ (N3LO) computation of the heavy quark vacuum polarization.

²¹ SCHWANDA 2008 measure moments of the inclusive photon spectrum in ${{\mathit B}}$ $\rightarrow$ ${{\mathit X}_{{{s}}}}{{\mathit \gamma}}$ decay to determine ${{\mathit m}_{{{b}}}^{1S}}$. We have converted this to $\overline{\rm{}MS}$ scheme.

²² NARISON 2018A determines ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) as a function of ${{\mathit \alpha}_{{{s}}}}$ using QCD exponential sum rules and their ratios evaluated at the optimal scale $\mu $ = 9.5 GeV at N2LO-N3LO of perturbative QCD and including condensates up to dimension $6 - 8$ in the (axial-)vector and (pseudo-)scalar bottomonium channels.

²³ NARISON 2018B determines ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) using QCD vector moment sum rules and their ratios at N2LO-N3LO of perturbative QCD and including condensates up to dimension 8.

²⁴ ABRAMOWICZ 2014A determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) = $4.07$ $\pm0.14$ ${}^{+0.01}_{-0.07}{}^{+0.05}_{-0.00}{}^{+0.08}_{-0.05}$ from the production of ${\mathit {\mathit b}}$ quarks in ${{\mathit e}}{{\mathit p}}$ collisions at HERA. The errors due to fitting, modeling, PDF parameterization, and theoretical QCD uncertainties due to the values of ${{\mathit \alpha}_{{{s}}}}$, ${{\mathit m}_{{{c}}}}$, and the renormalization scale $\mu $ have been combined in quadrature.

²⁵ AYALA 2014A determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) from the ${{\mathit \Upsilon}{(1S)}}$ mass computed to N3LO order in perturbation theory using a renormalon subtracted scheme.

²⁶ NARISON 2013 determines ${\mathit m}_{{{\mathit b}}}$ using QCD spectral sum rules to order ${{\mathit \alpha}_{{{s}}}^{2}}$ (NNLO) and including condensates up to dimension 6.

²⁷ NARISON 2013A determines ${\mathit m}_{{{\mathit b}}}$ using HQET sum rules to order ${{\mathit \alpha}_{{{s}}}^{2}}$ (NNLO) and the ${{\mathit B}}$ meson mass and decay constant.

²⁸ HOANG 2012 determine ${\mathit m}_{{{\mathit b}}}$ using non-relativistic sum rules for the ${{\mathit \Upsilon}}$ system at order ${{\mathit \alpha}_{{{s}}}^{2}}$ (NNLO) with renormalization group improvement.

²⁹ NARISON 2012 determines ${\mathit m}_{{{\mathit b}}}$ using exponential sum rules for the vector current correlator to order ${{\mathit \alpha}_{{{s}}}^{3}}$, including the effect of gluon condensates up to dimension eight.

³⁰ Determines ${\mathit m}_{{{\mathit b}}}$ to order ${{\mathit \alpha}_{{{s}}}^{3}}$ (N3LO), including the effect of gluon condensates up to dimension eight combining the methods of NARISON 2012 and NARISON 2012A.

³¹ NARISON 2012A determines ${\mathit m}_{{{\mathit b}}}$ using sum rules for the vector current correlator to order ${{\mathit \alpha}_{{{s}}}^{3}}$, including the effect of gluon condensates up to dimension eight.

³² MCNEILE 2010 determines ${\mathit m}_{{{\mathit b}}}$ by comparing order ${{\mathit \alpha}_{{{s}}}^{3}}$ (N3LO) perturbative results for the pseudo-scalar current to lattice simulations with ${{\mathit n}_{{{f}}}}$ = 2+1 sea-quarks by the HPQCD collaboration.

³³ NARISON 2010 determines ${\mathit m}_{{{\mathit b}}}$ from ratios of moments of vector current correlators computed to order ${{\mathit \alpha}_{{{s}}}^{3}}$ and including the dimension-six gluon condensate. These values are taken from the erratum to that reference.

³⁴ ABDALLAH 2008D determine ${{\overline{\mathit m}}_{{{b}}}}({{\mathit M}_{{{Z}}}}$) = $3.76$ $\pm1.0$ GeV from a leading order study of four-jet rates at LEP.

³⁵ GUAZZINI 2008 determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) from a quenched lattice simulation of heavy meson masses. The $\pm0.08$ is an estimate of the quenching error.

³⁶ DELLA-MORTE 2007 determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) from a computation of the spin-averaged ${{\mathit B}}$ meson mass using quenched lattice HQET at order 1/${{\mathit m}}$. The $\pm0.08$ is an estimate of the quenching error.

³⁷ KUHN 2007 determine ${{\overline{\mathit m}}_{{{b}}}}({{\mathit \mu}}$ = 10 GeV) = $3.609$ $\pm0.025$ GeV and ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) from a four-loop sum-rule computation of the cross-section for ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons in the bottom threshold region.

³⁸ ABDALLAH 2006D determine ${\mathit m}_{{{\mathit b}}}({{\mathit M}_{{{Z}}}}$) = $2.85$ $\pm0.32$ GeV from ${{\mathit Z}}$-decay three-jet events containing a ${{\mathit b}}$-quark.

³⁹ BOUGHEZAL 2006 $\overline{\rm{}MS}$ scheme result comes from the first moment of the hadronic production cross-section to order ${{\mathit \alpha}_{{{s}}}^{3}}$.

⁴⁰ BUCHMUELLER 2006 determine ${{\mathit m}_{{{b}}}}$ and ${{\mathit m}_{{{c}}}}$ by a global fit to inclusive ${{\mathit B}}$ decay spectra.

⁴¹ PINEDA 2006 $\overline{\rm{}MS}$ scheme result comes from a partial NNLL evaluation (complete at order ${{\mathit \alpha}_{{{s}}}^{2}}$ (NNLO)) of sum rules of the bottom production cross-section in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ annihilation.

⁴² GRAY 2005 determines ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) from a lattice computation of the ${{\mathit \Upsilon}}$ spectrum. The simulations have 2+1 dynamical light flavors. The ${{\mathit b}}$ quark is implemented using NRQCD.

⁴³ AUBERT 2004X obtain ${\mathit m}_{{{\mathit b}}}$ from a fit to the hadron mass and lepton energy distributions in semileptonic ${{\mathit B}}$ decay. The paper quotes values in the kinetic scheme. The $\overline{\rm{}MS}$ value has been provided by the BABAR collaboration.

⁴⁴ BAUER 2004 determine ${\mathit m}_{{{\mathit b}}}$, ${\mathit m}_{{{\mathit c}}}$ and ${\mathit m}_{{{\mathit b}}}−{\mathit m}_{{{\mathit c}}}$ by a global fit to inclusive ${{\mathit B}}$ decay spectra.

⁴⁵ HOANG 2004 determines ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) from moments at order ${{\mathit \alpha}_{{{s}}}^{2}}$ of the bottom production cross-section in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ annihilation.

⁴⁶ MCNEILE 2004 use lattice QCD with dynamical light quarks and a static heavy quark to compute the masses of heavy-light mesons.

⁴⁷ BAUER 2003 determine the b quark mass by a global fit to ${{\mathit B}}$ decay observables. The experimental data includes lepton energy and hadron invariant mass moments in semileptonic ${{\mathit B}}$ $\rightarrow$ ${{\mathit X}_{{{c}}}}{{\mathit \ell}}{{\mathit \nu}_{{{{{\mathit \ell}}}}}}$ decay, and the inclusive photon spectrum in ${{\mathit B}}$ $\rightarrow$ ${{\mathit X}_{{{s}}}}{{\mathit \gamma}}$ decay. The theoretical expressions used are of order 1/m${}^{3}$, and $\alpha {}^{2}_{s}\beta _{0}$.

⁴⁸ BORDES 2003 determines m$_{b}$ using QCD finite energy sum rules to order $\alpha {}^{2}_{s}$.

⁴⁹ CORCELLA 2003 determines ${{\overline{\mathit m}}_{{{b}}}}$ using sum rules computed to order $\alpha {}^{2}_{s}$. Includes charm quark mass effects.

⁵⁰ DEDIVITIIS 2003 use a quenched lattice computation of heavy-heavy and heavy-light meson masses.

⁵¹ EIDEMULLER 2003 determines ${{\overline{\mathit m}}_{{{b}}}}$ and ${{\overline{\mathit m}}_{{{c}}}}$ using QCD sum rules.

⁵² ERLER 2003 determines ${{\overline{\mathit m}}_{{{b}}}}$ and ${{\overline{\mathit m}}_{{{c}}}}$ using QCD sum rules. Includes recent BES data.

⁵³ MAHMOOD 2003 determines ${{\mathit m}}{}^{1S}_{b}$ by a fit to the lepton energy moments in ${{\mathit B}}$ $\rightarrow$ ${{\mathit X}_{{{c}}}}{{\mathit \ell}}{{\mathit \nu}_{{{{{\mathit \ell}}}}}}$ decay. The theoretical expressions used are of order 1/m${}^{3}$ and $\alpha {}^{2}_{s}\beta _{0}$. We have converted their result to the $\overline{\rm{}MS}$ scheme.

⁵⁴ BRAMBILLA 2002 determine ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) from a computation of the ${{\mathit \Upsilon}{(1S)}}$ mass to order ${{\mathit \alpha}_{{{s}}}^{4}}$, including finite ${{\mathit m}_{{{c}}}}$ corrections.

⁵⁵ PENIN 2002 determines ${{\overline{\mathit m}}_{{{b}}}}$ from the spectrum of the ${{\mathit \Upsilon}}$ system.

${\mathit {\mathit b}}$-QUARK $\overline{\rm{}MS}$ MASS (GeV)

References:

APARISI

2022

PRL 128 122001

$m_b$ at $m_H$: the running bottom quark mass and the Higgs boson

HATTON

2021

PR D103 114508

Determination of $\overline{m}_b/\overline{m}_c$ and $\overline{m}_b$ from $n_f=4$ lattice QCD$+$QED

2020

PL B802 135221

$\overline m_c$ and $\overline m_b$ from $M_{Bc}$ and improved estimates of $f_{Bc}$ and $f_{Bc(2S)}$

EPJ C78 473

Combination and QCD analysis of charm and beauty production cross-section measurements in deep inelastic $ep$ scattering at HERA

BAZAVOV

PR D98 054517

Up-, down-, strange-, charm-, and bottom-quark masses from four-flavor lattice QCD

2018A

IJMP A33 1850045

QCD parameter correlations from heavy quarkonia

2018B

PL B784 261

Updating $\bar m_{c,b}(\bar m_{c,b})$ from SVZ-moments and their ratios

PESET

JHEP 1809 167

The charm/bottom quark mass from heavy quarkonium at N$^{3}$LO

KIYO

2016

PL B752 122

Determination of ${\mathit m}_{{{\mathit c}}}$ and ${\mathit m}_{{{\mathit b}}}$ from Quarkonium $1S{}^{}{}^{}$ Energy Levels in Perturbative QCD

ALBERTI

PRL 114 061802

Precision Determination of the Cabibbo-Kobayashi-Maskawa Element ${\it V}_{\it cb}$

BENEKE

NP B891 42

The Bottom-Quark Mass from Non-Relativistic Sum Rules at NNNLO

COLQUHOUN

PR D91 074514

$\Upsilon$ and $\Upsilon^{\prime}$ Leptonic Widths, $a_{\mu}^b$ and $m_b$ from full lattice QCD

DEHNADI

JHEP 1508 155

Bottom and Charm Mass Determinations with a Convergence Test

2014A

JHEP 1409 127

Measurement of Beauty and Charm Production in Deep Inelastic Scattering at HERA and Measurement of the Beauty-Quark Mass

AYALA

2014A

JHEP 1409 045

The Bottom Quark Mass from the ${{\mathit \Upsilon}{(1S)}}$ System at NNNLO

BERNARDONI

PL B730 171

The ${\mathit {\mathit b}}$-Quark Mass from non-Perturbative $\mathit N_{f}$ = 2 Heavy Quark Effective Theory at (1/${\mathit m}_{{{\mathit h}}}$)

JHEP 1404 120

Bottom Quark Mass from ${{\mathit \Upsilon}}$ Sum Rules to (${{\mathit \alpha}_{{{s}}}^{3}}$)

LEE

2013O

PR D87 074018

Mass of the ${\mathit {\mathit b}}$ Quark from Lattice NRQCD and Lattice Perturbation Theory

LUCHA

PR D88 056011

Accurate Bottom-Quark Mass from Borel QCD Sum Rules for $\mathit f_{{{\mathit B}}}$ and $\mathit f_{{{\mathit B}_{{{s}}}}}$

2013A

PL B721 269

Revisiting ${{\mathit f}_{{{B}}}}$ and ${{\overline{\mathit m}}_{{{b}}}}({{\overline{\mathit m}}_{{{b}}}}$) from HQET Spectral Sum Rules

PL B718 1321

A Fresh Look into ${{\overline{\mathit m}}_{{{c,b}}}}({{\overline{\mathit m}}_{{{c,b}}}}$) and Precise ${{\mathit f}}_{{{\mathit D}}_{(s)},{{\mathit B}}_{(s)}}$ from Heavy$−$Light QCD Spectral Sum Rules

BODENSTEIN

PR D85 034003

Bottom-Quark Mass from Finite Energy QCD Sum Rules

DIMOPOULOS

JHEP 1201 046

Lattice QCD Determination of ${{\mathit m}_{{{b}}}}$, ${{\mathit f}_{{{B}}}}$ and ${{\mathit f}_{{{Bs}}}}$ with Twisted Mass Wilson Fermions

JHEP 1210 188

Renormalization Group Improved Bottom Mass from $\Upsilon $ Sum Rules at NNLL Order

2012A

PL B706 412

Gluon Condensates and Precise ${{\overline{\mathit m}}_{{{c,b}}}}$ from QCD-Moments and their Ratios to Order $\mathit \alpha {}^{3}_{s}$ and $<\mathit G{}^{4}>$

PL B707 259

Gluon Condensates and m$_{b}$ (m$_{b}$ ) from QCD-Exponential Sum Rules at Higher Orders

LASCHKA

2011

PR D83 094002

Quark-Antiquark Potential to Order 1/${{\mathit m}}$ and Heavy Quark Masses

2010A

PR D81 032003

Measurement and Interpretation of Moments in Inclusive Semileptonic Decays ${{\overline{\mathit B}}}$ $\rightarrow$ ${{\mathit X}_{{{c}}}}{{\mathit \ell}^{-}}{{\overline{\mathit \nu}}}$

PR D82 034512

High-Precision ${\mathit {\mathit c}}$ and ${\mathit {\mathit b}}$ Masses, and QCD Coupling from Current-Current Correlators in Lattice and Continuum QCD

PL B693 559

Gluon Condensates and ${\mathit {\mathit c}}$, ${\mathit {\mathit b}}$ Quark Masses from Quarkonia Ratios of Moments

Also

PL B705 544 (errat.)

Erratum to NARISON 2010: Gluon Condensates and ${\mathit {\mathit c}}$, ${\mathit {\mathit b}}$ Quark Masses from Quarkonia Ratios of Moments

CHETYRKIN

2009

PR D80 074010

Charm and Bottom Quark Masses: An Update

2008D

EPJ C55 525

Study of ${\mathit {\mathit b}}$-Quark Mass Effects in Multijet Topologies with the DELPHI Detector at LEP

GUAZZINI

JHEP 0801 076

Precision for $\mathit B$-Meson Matrix Elements

SCHWANDA

PR D78 032016

Measurement of the Moments of the Photon Energy Spectrum in ${{\mathit B}}$ $\rightarrow$ ${{\mathit X}_{{{s}}}}{{\mathit \gamma}}$ Decays and Determination of $\vert {\it V}_{\it cb}\vert $ and ${\mathit m}_{{{\mathit b}}}$ at Belle

DELLA-MORTE

JHEP 0701 007

Heavy Quark Effective Theory Computation of the Mass of the Bottom Quark

KUHN

NP B778 192

Heavy Quark Masses from Sum Rules in Four-Loop Approximation

2006D

EPJ C46 569

Determination of the ${\mathit {\mathit b}}$ Quark Mass at the $\mathit M_{Z}$ Scale with the DELPHI Detector at LEP

BOUGHEZAL

PR D74 074006

Charm- and Bottom-Quark Masses from Perturbative QCD

BUCHMUELLER

PR D73 073008

Fit to Moments of Inclusive ${{\mathit B}}$ $\rightarrow$ ${{\mathit X}_{{{c}}}}{{\mathit \ell}}{{\overline{\mathit \nu}}}$ and ${{\mathit B}}$ $\rightarrow$ ${{\mathit X}_{{{s}}}}{{\mathit \gamma}}$ Decay Distributions using Heavy Quark Expansions in the Kinetic Scheme

PINEDA

PR D73 111501

Renormalization-Group Improved Sum Rule Analysis for the Bottom-Quark Mass

GRAY

2005

PR D72 094507

Upsilon Spectrum and $\mathit m_{b}$ from Full Lattice QCD

2004X

PRL 93 011803

Determination of the Branching Fraction for ${{\mathit B}}$ $\rightarrow$ ${{\mathit X}_{{{c}}}}{{\mathit \ell}}{{\mathit \nu}}$ Decays and of $\vert {{\mathit V}_{{{cb}}}}\vert $ from Hadronic-Mass and Lepton-Energy Moments

PR D70 094017

Global Analysis of Inclusive ${{\mathit B}}$ Decays

PL B594 127

$\overline{\rm{}MS}$ Charm Mass from Charmonium Sum Rules with Contour Improvement

PL B600 77

An Unquenched Lattice QCD Calculation of the Mass of the bottom Quark

PR D67 054012

${{\mathit B}}$ Decay Shape Variables and the Precision Determination of |$\mathit V_{cb}$| and $\mathit m_{b}$

BORDES

PL B562 81

Bottom Quark Mass QCD Duality

CORCELLA

PL B554 133

Uncertainties in the $\overline{\rm{}MS}$ Bottom Quark Mass from Relativistic Sum Rules

DEDIVITIIS

NP B675 309

Heavy Quark Masses in the Continuum Limit of Quenched Lattice QCD

EIDEMULLER

PR D67 113002

QCD Moment Sum Rules for Coulomb Systems: the Charm and Bottom Quark Masses

ERLER

PL B558 125

Precision Determination of Heavy Quark Masses and the Strong Coupling Constant

MAHMOOD

PR D67 072001

Measurement of Lepton Momentum Momentsin the Decay ${{\overline{\mathit B}}}$ $\rightarrow$ ${{\mathit X}}{{\mathit \ell}}{{\overline{\mathit \nu}}}$ and Determination of Heavy Quark Expansion Parameters and |$\mathit V_{cb}$|

BRAMBILLA

PR D65 034001

Quarkonium Spectroscopy and Perturbative QCD: Massive Quark-Loop Effects