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001     618824
005     20250715170846.0
024 7 _ |a 10.1140/epjc/s10052-024-12816-4
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024 7 _ |a arXiv:2309.14154
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088 _ _ |a arXiv:2309.14154
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088 _ _ |a IFT-UAM/CSIC-23-114
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100 1 _ |a Bussone, Andrea
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245 _ _ |a Hadronic physics from a Wilson fermion mixed-action approach: charm quark mass and $D_{(s)}$ meson decay constants
260 _ _ |a Heidelberg
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500 _ _ |a 44 pages, 21 figures
520 _ _ |a We present our first set of results for charm physics, using the mixed-action setup introduced in a companion paper [1]. Maximally twisted Wilson valence fermions are used on a sea of non-perturbatively O(a)-improved Wilson fermions, made up by CLS $N_\mathrm {\scriptstyle f}=2+1$ ensembles. Our charm-sector observables are free from $O(am_c)$ discretisation effects, without need of tuning any improvement coefficient, and show continuum-limit scaling properties consistent with leading cutoff effects of $O(a^2)$. We consider a subset of CLS ensembles – including four values of the lattice spacing and pion masses down to 200 MeV – allowing to take the continuum limit and extrapolate to the physical pion mass. A number of techniques are incorporated in the analysis in order to estimate the systematic uncertainties of our results for the charm quark mass and the $D_{(s)}$-meson decay constants. This first study of observables in the charm sector, where the emphasis has been on the control of the methodology, demonstrates the potential of our setup to achieve high-precision results.
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650 _ 7 |a fermion: Wilson
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650 _ 7 |a pi: mass
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650 _ 7 |a quark: mass
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650 _ 7 |a meson: decay
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650 _ 7 |a down: mass
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650 _ 7 |a fermion: valence
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650 _ 7 |a effect: discrete
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650 _ 7 |a charm
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700 1 _ |a Conigli, Alessandro
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700 1 _ |a Frison, Julien Francois
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700 1 _ |a Herdoíza, Gregorio
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700 1 _ |a Pena, Carlos
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700 1 _ |a Preti, David
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700 1 _ |a Sáez, Alejandro
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700 1 _ |a Ugarrio, Javier
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700 1 _ |a Alpha Collaboration
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|t Hadronic physics from a Wilson fermion mixed-action approach: charm quark mass and $D_{(s)}$ meson decay constants
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999 C 5 |2 Crossref
|u A. Bussone, A. Conigli, J. Frison, G. Herdoíza, C. Pena, D. Preti, J.Á. Romero, A. Sáez, J. Ugarrio, Hadronic physics from a Wilson fermion mixed-action approach: setup and scale setting (to appear)
999 C 5 |a 10.1007/JHEP04(2011)104
|9 -- missing cx lookup --
|1 M Lüscher
|p 104 -
|2 Crossref
|u M. Lüscher, S. Schaefer, Non-renormalizability of the HMC algorithm. JHEP 04, 104 (2011). https://doi.org/10.1007/JHEP04(2011)104. arXiv:1103.1810
|t JHEP
|v 04
|y 2011
999 C 5 |a 10.1016/j.nuclphysb.2010.11.020
|9 -- missing cx lookup --
|2 Crossref
|u ALPHA collaboration, Critical slowing down and error analysis in lattice QCD simulations. Nucl. Phys. B 845, 93 (2011). https://doi.org/10.1016/j.nuclphysb.2010.11.020. arXiv:1009.5228
999 C 5 |a 10.1016/0550-3213(83)90468-6
|9 -- missing cx lookup --
|1 K Symanzik
|p 187 -
|2 Crossref
|u K. Symanzik, Continuum limit and improved action in lattice theories. 1. Principles and $$\varphi ^4$$ theory. Nucl. Phys. B 226, 187 (1983). https://doi.org/10.1016/0550-3213(83)90468-6
|t Nucl. Phys. B
|v 226
|y 1983
999 C 5 |a 10.1016/0550-3213(83)90469-8
|9 -- missing cx lookup --
|1 K Symanzik
|p 205 -
|2 Crossref
|u K. Symanzik, Continuum limit and improved action in lattice theories. 2. O(N) Nonlinear sigma model in perturbation theory. Nucl. Phys. B 226, 205 (1983). https://doi.org/10.1016/0550-3213(83)90469-8
|t Nucl. Phys. B
|v 226
|y 1983
999 C 5 |a 10.1007/BF01206178
|9 -- missing cx lookup --
|1 M Lüscher
|p 59 -
|2 Crossref
|u M. Lüscher, P. Weisz, On-shell improved lattice gauge theories. Commun. Math. Phys. 97, 59 (1985). https://doi.org/10.1007/BF01206178
|t Commun. Math. Phys.
|v 97
|y 1985
999 C 5 |a 10.1016/0550-3213(96)00378-1
|9 -- missing cx lookup --
|1 M Lüscher
|p 365 -
|2 Crossref
|u M. Lüscher, S. Sint, R. Sommer, P. Weisz, Chiral symmetry and O(a) improvement in lattice QCD. Nucl. Phys. B 478, 365 (1996). https://doi.org/10.1016/0550-3213(96)00378-1. arXiv:hep-lat/9605038
|t Nucl. Phys. B
|v 478
|y 1996
999 C 5 |a 10.1140/epjc/s10052-019-7354-7
|9 -- missing cx lookup --
|2 Crossref
|u Flavour Lattice Averaging Group collaboration, FLAG Review 2019: Flavour Lattice Averaging Group (FLAG), Eur. Phys. J. C series 80, 113 (2020). https://doi.org/10.1140/epjc/s10052-019-7354-7. arXiv:1902.08191
999 C 5 |a 10.1140/epjc/s10052-022-10536-1
|9 -- missing cx lookup --
|2 Crossref
|u Flavour Lattice Averaging Group (FLAG) collaboration, FLAG Review 2021. Eur. Phys. J. C 82, 869 (2022). https://doi.org/10.1140/epjc/s10052-022-10536-1. arXiv:2111.09849
999 C 5 |a 10.1007/JHEP02(2015)043
|9 -- missing cx lookup --
|1 M Bruno
|p 043 -
|2 Crossref
|u M. Bruno et al., Simulation of QCD with N$$_{f} =$$ 2 $$+$$ 1 flavors of non-perturbatively improved Wilson fermions. JHEP 02, 043 (2015). https://doi.org/10.1007/JHEP02(2015)043. arXiv:1411.3982
|t JHEP
|v 02
|y 2015
999 C 5 |a 10.1007/JHEP07(2011)036
|9 -- missing cx lookup --
|1 M Lüscher
|p 036 -
|2 Crossref
|u M. Lüscher, S. Schaefer, Lattice QCD without topology barriers. JHEP 07, 036 (2011). https://doi.org/10.1007/JHEP07(2011)036. arXiv:1105.4749
|t JHEP
|v 07
|y 2011
999 C 5 |a 10.1016/j.cpc.2012.10.003
|9 -- missing cx lookup --
|1 M Lüscher
|p 519 -
|2 Crossref
|u M. Lüscher, S. Schaefer, Lattice QCD with open boundary conditions and twisted-mass reweighting. Comput. Phys. Commun. 184, 519 (2013). https://doi.org/10.1016/j.cpc.2012.10.003. arXiv:1206.2809
|t Comput. Phys. Commun.
|v 184
|y 2013
999 C 5 |a 10.1088/1126-6708/2001/08/058
|9 -- missing cx lookup --
|2 Crossref
|u ALPHA collaboration, Lattice QCD with a chirally twisted mass term. JHEP 08, 058 (2001). https://doi.org/10.1088/1126-6708/2001/08/058. arXiv:hep-lat/0101001
999 C 5 |a 10.1088/1126-6708/2004/09/069
|9 -- missing cx lookup --
|1 C Pena
|p 069 -
|2 Crossref
|u C. Pena, S. Sint, A. Vladikas, Twisted mass QCD and lattice approaches to the Delta I = 1/2 rule. JHEP 09, 069 (2004). https://doi.org/10.1088/1126-6708/2004/09/069. arXiv:hep-lat/0405028
|t JHEP
|v 09
|y 2004
999 C 5 |a 10.1088/1126-6708/2004/08/007
|9 -- missing cx lookup --
|1 R Frezzotti
|p 007 -
|2 Crossref
|u R. Frezzotti, G.C. Rossi, Chirally improving Wilson fermions. 1. O(a) improvement. JHEP 08, 007 (2004). https://doi.org/10.1088/1126-6708/2004/08/007. arXiv:hep-lat/0306014
|t JHEP
|v 08
|y 2004
999 C 5 |a 10.1051/epjconf/201817513018
|9 -- missing cx lookup --
|1 G Herdoíza
|p 13018 -
|2 Crossref
|u G. Herdoíza, C. Pena, D. Preti, J.A. Romero, J. Ugarrio, A tmQCD mixed-action approach to flavour physics. EPJ Web Conf. 175, 13018 (2018). https://doi.org/10.1051/epjconf/201817513018. arXiv:1711.06017
|t EPJ Web Conf.
|v 175
|y 2018
999 C 5 |a 10.22323/1.334.0271
|9 -- missing cx lookup --
|2 Crossref
|u ALPHA collaboration, First results for charm physics with a tmQCD valence action. PoS LATTICE2018, 271 (2018). https://doi.org/10.22323/1.334.0271. arXiv:1812.05458
999 C 5 |a 10.22323/1.334.0270
|9 -- missing cx lookup --
|2 Crossref
|u ALPHA collaboration, Heavy-quark physics with a tmQCD valence action. PoS LATTICE2018, 270 (2019). https://doi.org/10.22323/1.334.0270. arXiv:1812.01474
999 C 5 |a 10.22323/1.334.0318
|9 -- missing cx lookup --
|2 Crossref
|u ALPHA collaboration, Matching of $${N_{\rm f}}=2+1$$ CLS ensembles to a tmQCD valence sector. PoS LATTICE2018, 318 (2019). https://doi.org/10.22323/1.334.0318. arXiv:1903.00286
999 C 5 |a 10.22323/1.396.0091
|9 -- missing cx lookup --
|2 Crossref
|u A. Conigli, A. Bussone, J. Frison, G. Herdoíza, C. Pena, D. Preti, J.Á. Romero, J. Ugarrio, Charm physics with a tmQCD mixed action. PoS LATTICE2021, 091 (2022). https://doi.org/10.22323/1.396.0091. arXiv:2112.00666
999 C 5 |a 10.22323/1.396.0258
|9 -- missing cx lookup --
|2 Crossref
|u A. Bussone, A. Conigli, G. Herdoíza, J. Frison, C. Pena, D. Preti, J.Á. Romero, A. Sáez, J. Ugarrio, Light meson physics and scale setting from a mixed action with Wilson twisted mass valence quarks. PoS LATTICE2021, 258 (2022). https://doi.org/10.22323/1.396.0258
999 C 5 |a 10.22323/1.430.0357
|9 -- missing cx lookup --
|2 Crossref
|u A. Sáez, A. Conigli, J. Frison, G. Herdoíza, C. Pena, J. Ugarrio, Scale setting from a mixed action with twisted mass valence quarks. PoS LATTICE2022, 357 (2023). https://doi.org/10.22323/1.430.0357
999 C 5 |a 10.22323/1.430.0351
|9 -- missing cx lookup --
|2 Crossref
|u A. Conigli, J. Frison, G. Herdoíza, C. Pena, A. Sáez, J. Ugarrio, Towards precision charm physics with a mixed action. PoS LATTICE2022, 351 (2023). https://doi.org/10.22323/1.430.0351. arXiv:2212.11045
999 C 5 |a 10.1103/PhysRevD.103.114502
|1 WI Jay
|9 -- missing cx lookup --
|2 Crossref
|u W.I. Jay, E.T. Neil, Bayesian model averaging for analysis of lattice field theory results. Phys. Rev. D 103, 114502 (2021). https://doi.org/10.1103/PhysRevD.103.114502. arXiv:2008.01069
|t Phys. Rev. D
|v 103
|y 2021
999 C 5 |2 Crossref
|u J. Frison, Towards fully bayesian analyses in Lattice QCD. arXiv:2302.06550
999 C 5 |a 10.1016/j.cpc.2022.108643
|1 M Bruno
|9 -- missing cx lookup --
|2 Crossref
|u M. Bruno, R. Sommer, On fits to correlated and auto-correlated data. Comput. Phys. Commun. 285, 108643 (2023). https://doi.org/10.1016/j.cpc.2022.108643. arXiv:2209.14188
|t Comput. Phys. Commun.
|v 285
|y 2023
999 C 5 |a 10.1103/PhysRevD.82.034512
|1 C McNeile
|9 -- missing cx lookup --
|2 Crossref
|u C. McNeile, C.T.H. Davies, E. Follana, K. Hornbostel, G.P. Lepage, High-precision c and b masses, and QCD coupling from current-current correlators in lattice and continuum QCD. Phys. Rev. D 82, 034512 (2010). https://doi.org/10.1103/PhysRevD.82.034512. arXiv:1004.4285
|t Phys. Rev. D
|v 82
|y 2010
999 C 5 |a 10.1103/PhysRevD.82.114504
|1 CTH Davies
|9 -- missing cx lookup --
|2 Crossref
|u C.T.H. Davies, C. McNeile, E. Follana, G.P. Lepage, H. Na, J. Shigemitsu, Update: precision $$D_s$$ decay constant from full lattice QCD using very fine lattices. Phys. Rev. D 82, 114504 (2010). https://doi.org/10.1103/PhysRevD.82.114504. arXiv:1008.4018
|t Phys. Rev. D
|v 82
|y 2010
999 C 5 |a 10.1103/PhysRevD.85.114506
|9 -- missing cx lookup --
|2 Crossref
|u Fermilab Lattice, MILC collaboration, B- and D-meson decay constants from three-flavor lattice QCD. Phys. Rev. D 85, 114506 (2012). https://doi.org/10.1103/PhysRevD.85.114506. arXiv:1112.3051
999 C 5 |a 10.1103/PhysRevD.86.054510
|1 H Na
|9 -- missing cx lookup --
|2 Crossref
|u H. Na, C.T.H. Davies, E. Follana, G.P. Lepage, J. Shigemitsu, $$|V_{cd}|$$ from D meson leptonic decays. Phys. Rev. D 86, 054510 (2012). https://doi.org/10.1103/PhysRevD.86.054510. arXiv:1206.4936
|t Phys. Rev. D
|v 86
|y 2012
999 C 5 |a 10.1007/JHEP03(2014)016
|9 -- missing cx lookup --
|2 Crossref
|u ETM collaboration, B-physics from $${N_{\rm f}}$$ = 2 tmQCD: the Standard Model and beyond. JHEP 03, 016 (2014). https://doi.org/10.1007/JHEP03(2014)016. arXiv:1308.1851
999 C 5 |a 10.1103/PhysRevD.91.054508
|1 B Chakraborty
|9 -- missing cx lookup --
|2 Crossref
|u B. Chakraborty, C.T.H. Davies, B. Galloway, P. Knecht, J. Koponen, G.C. Donald, R.J. Dowdall, G.P. Lepage, C. McNeile, High-precision quark masses and QCD coupling from $$n_f=4$$ lattice QCD. Phys. Rev. D 91, 054508 (2015). https://doi.org/10.1103/PhysRevD.91.054508. arXiv:1408.4169
|t Phys. Rev. D
|v 91
|y 2015
999 C 5 |a 10.1016/j.nuclphysb.2014.07.025
|9 -- missing cx lookup --
|2 Crossref
|u European Twisted Mass collaboration, Up, down, strange and charm quark masses with N$$_f$$ = 2+1+1 twisted mass lattice QCD. Nucl. Phys. B series 887, 19 (2014). https://doi.org/10.1016/j.nuclphysb.2014.07.025. arXiv:1403.4504
999 C 5 |a 10.1103/PhysRevD.90.074501
|1 C Alexandrou
|9 -- missing cx lookup --
|2 Crossref
|u C. Alexandrou, V. Drach, K. Jansen, C. Kallidonis, G. Koutsou, Baryon spectrum with $${N_{\rm f} }=2+1+1$$ twisted mass fermions. Phys. Rev. D 90, 074501 (2014). https://doi.org/10.1103/PhysRevD.90.074501. arXiv:1406.4310
|t Phys. Rev. D
|v 90
|y 2014
999 C 5 |a 10.1103/PhysRevD.92.034517
|1 Y-B Yang
|9 -- missing cx lookup --
|2 Crossref
|u Y.-B. Yang et al., Charm and strange quark masses and $$f_{D_s}$$ from overlap fermions. Phys. Rev. D 92, 034517 (2015). https://doi.org/10.1103/PhysRevD.92.034517. arXiv:1410.3343
|t Phys. Rev. D
|v 92
|y 2015
999 C 5 |a 10.1103/PhysRevD.91.054507
|1 N Carrasco
|9 -- missing cx lookup --
|2 Crossref
|u N. Carrasco et al., Leptonic decay constants $$f_{K}, f_{D},$$ and $$f_{{D}_{s}}$$ with $$N_{f} = 2+1+1$$ twisted-mass lattice QCD. Phys. Rev. D 91, 054507 (2015). https://doi.org/10.1103/PhysRevD.91.054507. arXiv:1411.7908
|t Phys. Rev. D
|v 91
|y 2015
999 C 5 |a 10.1103/PhysRevD.94.054507
|1 K Nakayama
|9 -- missing cx lookup --
|2 Crossref
|u K. Nakayama, B. Fahy, S. Hashimoto, Short-distance charmonium correlator on the lattice with Möbius domain-wall fermion and a determination of charm quark mass. Phys. Rev. D 94, 054507 (2016). https://doi.org/10.1103/PhysRevD.94.054507. arXiv:1606.01002
|t Phys. Rev. D
|v 94
|y 2016
999 C 5 |a 10.1103/PhysRevD.98.074512
|1 A Bazavov
|9 -- missing cx lookup --
|2 Crossref
|u A. Bazavov et al., $$B$$- and $$D$$-meson leptonic decay constants from four-flavor lattice QCD. Phys. Rev. D 98, 074512 (2018). https://doi.org/10.1103/PhysRevD.98.074512. arXiv:1712.09262
|t Phys. Rev. D
|v 98
|y 2018
999 C 5 |a 10.1007/JHEP12(2017)008
|9 -- missing cx lookup --
|1 PA Boyle
|p 008 -
|2 Crossref
|u P.A. Boyle, L. Del Debbio, A. Jüttner, A. Khamseh, F. Sanfilippo, J.T. Tsang, The decay constants $${\mathbf{f_D} }$$ and $${\mathbf{f_{D_{s}}} }$$ in the continuum limit of $${\mathbf{{N_{\rm f}}=2+1} }$$ domain wall lattice QCD. JHEP 12, 008 (2017). https://doi.org/10.1007/JHEP12(2017)008. arXiv:1701.02644
|t JHEP
|v 12
|y 2017
999 C 5 |a 10.1103/PhysRevD.98.054517
|9 -- missing cx lookup --
|2 Crossref
|u Fermilab Lattice, MILC, TUMQCD collaboration, Up-, down-, strange-, charm-, and bottom-quark masses from four-flavor lattice QCD. Phys. Rev. D 98, 054517 (2018). https://doi.org/10.1103/PhysRevD.98.054517. arXiv:1802.04248
999 C 5 |a 10.1140/epjc/s10052-020-7965-z
|9 -- missing cx lookup --
|1 R Balasubramamian
|p 412 -
|2 Crossref
|u R. Balasubramamian, B. Blossier, Decay constant of $$B_s$$ and $$B^*_s$$ mesons from $${{N_{\rm f }}}=2$$ lattice QCD. Eur. Phys. J. C 80, 412 (2020). https://doi.org/10.1140/epjc/s10052-020-7965-z. arXiv:1912.09937
|t Eur. Phys. J. C
|v 80
|y 2020
999 C 5 |a 10.1103/PhysRevD.100.034519
|1 P Petreczky
|9 -- missing cx lookup --
|2 Crossref
|u P. Petreczky, J.H. Weber, Strong coupling constant and heavy quark masses in (2+1)-flavor QCD. Phys. Rev. D 100, 034519 (2019). https://doi.org/10.1103/PhysRevD.100.034519. arXiv:1901.06424
|t Phys. Rev. D
|v 100
|y 2019
999 C 5 |a 10.1103/PhysRevD.102.054511
|9 -- missing cx lookup --
|2 Crossref
|u HPQCD collaboration, Charmonium properties from lattice $$QCD$$+QED: hyperfine splitting, $$J/\psi $$ leptonic width, charm quark mass, and $$a^c_\mu $$. Phys. Rev. D 102, 054511 (2020). https://doi.org/10.1103/PhysRevD.102.054511. arXiv: 2005.01845
999 C 5 |a 10.1103/PhysRevD.104.074515
|9 -- missing cx lookup --
|2 Crossref
|u Extended Twisted Mass collaboration, Quark masses using twisted-mass fermion gauge ensembles. Phys. Rev. D 104, 074515 (2021). https://doi.org/10.1103/PhysRevD.104.074515. arXiv:2104.13408
999 C 5 |a 10.1007/JHEP05(2021)288
|9 -- missing cx lookup --
|2 Crossref
|u ALPHA collaboration, Determination of the charm quark mass in lattice QCD with $$2+1$$ flavours on fine lattices. JHEP 05, 288 (2021). https://doi.org/10.1007/JHEP05(2021)288. arXiv:2101.02694
999 C 5 |a 10.1016/0370-2693(85)90966-9
|9 -- missing cx lookup --
|1 M Lüscher
|p 250 -
|2 Crossref
|u M. Lüscher, P. Weisz, Computation of the action for on-shell improved lattice gauge theories at weak coupling. Phys. Lett. B 158, 250 (1985). https://doi.org/10.1016/0370-2693(85)90966-9
|t Phys. Lett. B
|v 158
|y 1985
999 C 5 |a 10.1016/0550-3213(85)90002-1
|9 -- missing cx lookup --
|1 B Sheikholeslami
|p 572 -
|2 Crossref
|u B. Sheikholeslami, R. Wohlert, Improved continuum limit lattice action for QCD with Wilson fermions. Nucl. Phys. B 259, 572 (1985). https://doi.org/10.1016/0550-3213(85)90002-1
|t Nucl. Phys. B
|v 259
|y 1985
999 C 5 |a 10.1103/PhysRevD.95.074504
|1 M Bruno
|9 -- missing cx lookup --
|2 Crossref
|u M. Bruno, T. Korzec, S. Schaefer, Setting the scale for the CLS $$2 + 1$$ flavor ensembles. Phys. Rev. D 95, 074504 (2017). https://doi.org/10.1103/PhysRevD.95.074504. arXiv:1608.08900
|t Phys. Rev. D
|v 95
|y 2017
999 C 5 |a 10.1051/epjconf/201817502010
|9 -- missing cx lookup --
|1 D Mohler
|p 02010 -
|2 Crossref
|u D. Mohler, S. Schaefer, J. Simeth, CLS 2+1 flavor simulations at physical light- and strange-quark masses. EPJ Web Conf. 175, 02010 (2018). https://doi.org/10.1051/epjconf/201817502010. arXiv:1712.04884
|t EPJ Web Conf.
|v 175
|y 2018
999 C 5 |a 10.1103/PhysRevD.102.074506
|1 D Mohler
|9 -- missing cx lookup --
|2 Crossref
|u D. Mohler, S. Schaefer, Remarks on strange-quark simulations with Wilson fermions. Phys. Rev. D 102, 074506 (2020). https://doi.org/10.1103/PhysRevD.102.074506. arXiv:2003.13359
|t Phys. Rev. D
|v 102
|y 2020
999 C 5 |a 10.1103/PhysRevD.10.2445
|9 -- missing cx lookup --
|1 KG Wilson
|p 2445 -
|2 Crossref
|u K.G. Wilson, Confinement of quarks. Phys. Rev. D 10, 2445 (1974). https://doi.org/10.1103/PhysRevD.10.2445
|t Phys. Rev. D
|v 10
|y 1974
999 C 5 |a 10.1088/1126-6708/2004/10/070
|9 -- missing cx lookup --
|1 R Frezzotti
|p 070 -
|2 Crossref
|u R. Frezzotti, G.C. Rossi, Chirally improving Wilson fermions. II. Four-quark operators. JHEP 10, 070 (2004). https://doi.org/10.1088/1126-6708/2004/10/070. arXiv:hep-lat/0407002
|t JHEP
|v 10
|y 2004
999 C 5 |a 10.1140/epjc/s10052-018-5870-5
|9 -- missing cx lookup --
|2 Crossref
|u ALPHA collaboration, Non-perturbative quark mass renormalisation and running in $${N_{\rm f}}=3$$ QCD. Eur. Phys. J. C 78, 387 (2018). https://doi.org/10.1140/epjc/s10052-018-5870-5. arXiv:1802.05243
999 C 5 |a 10.1088/1126-6708/2006/04/038
|9 -- missing cx lookup --
|1 R Frezzotti
|p 038 -
|2 Crossref
|u R. Frezzotti, G. Martinelli, M. Papinutto, G.C. Rossi, Reducing cutoff effects in maximally twisted lattice QCD close to the chiral limit. JHEP 04, 038 (2006). https://doi.org/10.1088/1126-6708/2006/04/038. arXiv:hep-lat/0503034
|t JHEP
|v 04
|y 2006
999 C 5 |a 10.1088/1126-6708/2009/07/007
|9 -- missing cx lookup --
|1 P Dimopoulos
|p 007 -
|2 Crossref
|u P. Dimopoulos, H. Simma, A. Vladikas, Quenched B(K)-parameter from Osterwalder–Seiler tmQCD quarks and mass-splitting discretization effects. JHEP 07, 007 (2009). https://doi.org/10.1088/1126-6708/2009/07/007. arXiv:0902.1074
|t JHEP
|v 07
|y 2009
999 C 5 |a 10.1016/j.physrep.2008.03.001
|9 -- missing cx lookup --
|1 A Shindler
|p 37 -
|2 Crossref
|u A. Shindler, Twisted mass lattice QCD. Phys. Rep. 461, 37 (2008). https://doi.org/10.1016/j.physrep.2008.03.001. arXiv:0707.4093
|t Phys. Rep.
|v 461
|y 2008
999 C 5 |a 10.1007/JHEP08(2010)071
|9 -- missing cx lookup --
|1 M Lüscher
|p 071 -
|2 Crossref
|u M. Lüscher, Properties and uses of the Wilson flow in lattice QCD. JHEP 08, 071 (2010). https://doi.org/10.1007/JHEP08(2010)071. arXiv:1006.4518
|t JHEP
|v 08
|y 2010
999 C 5 |a 10.1007/JHEP05(2023)035
|9 -- missing cx lookup --
|2 Crossref
|u RQCD collaboration, Scale setting and the light baryon spectrum in N$$_{f}$$ = 2 + 1 QCD with Wilson fermions. JHEP 05, 035 (2023). https://doi.org/10.1007/JHEP05(2023)035. arXiv:2211.03744
999 C 5 |a 10.22323/1.396.0135
|9 -- missing cx lookup --
|2 Crossref
|u B. Strassberger et al., Scale setting for CLS 2+1 simulations. PoS LATTICE2021, 135 (2022). https://doi.org/10.22323/1.396.0135. arXiv:2112.06696
999 C 5 |a 10.1016/j.physletb.2010.07.031
|9 -- missing cx lookup --
|1 GM de Divitiis
|p 157 -
|2 Crossref
|u G.M. de Divitiis, R. Petronzio, N. Tantalo, Distance preconditioning for lattice Dirac operators. Phys. Lett. B 692, 157 (2010). https://doi.org/10.1016/j.physletb.2010.07.031. arXiv:1006.4028
|t Phys. Lett. B
|v 692
|y 2010
999 C 5 |a 10.22323/1.256.0368
|9 -- missing cx lookup --
|2 Crossref
|u S. Collins, K. Eckert, J. Heitger, S. Hofmann, W. Soeldner, Charmed pseudoscalar decay constants on three-flavour CLS ensembles with open boundaries. PoS LATTICE2016, 368 (2017). https://doi.org/10.22323/1.256.0368. arXiv: 1701.05502
999 C 5 |a 10.1016/S0010-4655(03)00467-3
|9 -- missing cx lookup --
|2 Crossref
|u ALPHA collaboration, Monte Carlo errors with less errors. Comput. Phys. Commun. 156, 143 (2004). https://doi.org/10.1016/S0010-4655(03)00467-3. arXiv:hep-lat/0306017
999 C 5 |a 10.1016/j.cpc.2018.12.020
|9 -- missing cx lookup --
|1 A Ramos
|p 19 -
|2 Crossref
|u A. Ramos, Automatic differentiation for error analysis of Monte Carlo data. Comput. Phys. Commun. 238, 19 (2019). https://doi.org/10.1016/j.cpc.2018.12.020. arXiv:1809.01289
|t Comput. Phys. Commun.
|v 238
|y 2019
999 C 5 |a 10.1088/1126-6708/2009/04/094
|9 -- missing cx lookup --
|1 B Blossier
|p 094 -
|2 Crossref
|u B. Blossier, M. Della Morte, G. von Hippel, T. Mendes, R. Sommer, On the generalized eigenvalue method for energies and matrix elements in lattice field theory. JHEP 04, 094 (2009). https://doi.org/10.1088/1126-6708/2009/04/094. arXiv:0902.1265
|t JHEP
|v 04
|y 2009
999 C 5 |a 10.1093/ptep/ptac097
|9 -- missing cx lookup --
|2 Crossref
|u Particle Data Group collaboration, Review of particle physics. PTEP 2022, 083C01 (2022). https://doi.org/10.1093/ptep/ptac097
999 C 5 |a 10.1088/1126-6708/2004/08/004
|9 -- missing cx lookup --
|2 Crossref
|u QCD-TARO collaboration, Contribution of disconnected diagrams to the hyperfine splitting of charmonium. JHEP 08, 004 (2004). https://doi.org/10.1088/1126-6708/2004/08/004. arXiv:hep-lat/0404016
999 C 5 |a 10.1103/PhysRevD.86.094501
|1 GC Donald
|9 -- missing cx lookup --
|2 Crossref
|u G.C. Donald, C.T.H. Davies, R.J. Dowdall, E. Follana, K. Hornbostel, J. Koponen, G.P. Lepage, C. McNeile, Precision tests of the $$J/{\psi }$$ from full lattice QCD: mass, leptonic width and radiative decay rate to $${\eta }_c$$. Phys. Rev. D 86, 094501 (2012). https://doi.org/10.1103/PhysRevD.86.094501. arXiv:1208.2855
|t Phys. Rev. D
|v 86
|y 2012
999 C 5 |a 10.1103/PhysRevD.91.114509
|9 -- missing cx lookup --
|2 Crossref
|u HPQCD collaboration, B-meson decay constants: a more complete picture from full lattice QCD. Phys. Rev. D 91, 114509 (2015). https://doi.org/10.1103/PhysRevD.91.114509. arXiv:1503.05762
999 C 5 |a 10.1103/PhysRevD.108.014513
|9 -- missing cx lookup --
|2 Crossref
|u HPQCD$$\dagger $$ collaboration, Precise determination of decay rates for $$\eta _c\rightarrow \gamma \gamma $$, $$J/\psi \rightarrow \gamma \eta _c$$, and $$J/\psi \rightarrow \eta _c e^+e^-$$ from lattice QCD. Phys. Rev. D 108, 014513 (2023). https://doi.org/10.1103/PhysRevD.108.014513. arXiv:2305.06231
999 C 5 |a 10.1016/0370-2693(90)91128-X
|9 -- missing cx lookup --
|1 H Georgi
|p 447 -
|2 Crossref
|u H. Georgi, An effective field theory for heavy quarks at low-energies. Phys. Lett. B 240, 447 (1990). https://doi.org/10.1016/0370-2693(90)91128-X
|t Phys. Lett. B
|v 240
|y 1990
999 C 5 |a 10.1007/JHEP10(2014)076
|9 -- missing cx lookup --
|1 PA Baikov
|p 076 -
|2 Crossref
|u P.A. Baikov, K.G. Chetyrkin, J.H. Kühn, Quark mass and field anomalous dimensions to $${\cal{O}}(\alpha _s^5)$$. JHEP 10, 076 (2014). https://doi.org/10.1007/JHEP10(2014)076. arXiv:1402.6611
|t JHEP
|v 10
|y 2014
999 C 5 |a 10.1007/JHEP01(2017)081
|9 -- missing cx lookup --
|1 T Luthe
|p 081 -
|2 Crossref
|u T. Luthe, A. Maier, P. Marquard, Y. Schröder, Five-loop quark mass and field anomalous dimensions for a general gauge group. JHEP 01, 081 (2017). https://doi.org/10.1007/JHEP01(2017)081. arXiv:1612.05512
|t JHEP
|v 01
|y 2017
999 C 5 |a 10.1007/JHEP04(2017)119
|9 -- missing cx lookup --
|1 PA Baikov
|p 119 -
|2 Crossref
|u P.A. Baikov, K.G. Chetyrkin, J.H. Kühn, Five-loop fermion anomalous dimension for a general gauge group from four-loop massless propagators. JHEP 04, 119 (2017). https://doi.org/10.1007/JHEP04(2017)119. arXiv:1702.01458
|t JHEP
|v 04
|y 2017
999 C 5 |a 10.1103/PhysRevLett.118.082002
|1 PA Baikov
|9 -- missing cx lookup --
|2 Crossref
|u P.A. Baikov, K.G. Chetyrkin, J.H. Kühn, Five-loop running of the QCD coupling constant. Phys. Rev. Lett. 118, 082002 (2017). https://doi.org/10.1103/PhysRevLett.118.082002. arXiv:1606.08659
|t Phys. Rev. Lett.
|v 118
|y 2017
999 C 5 |a 10.1007/JHEP02(2017)090
|9 -- missing cx lookup --
|1 F Herzog
|p 090 -
|2 Crossref
|u F. Herzog, B. Ruijl, T. Ueda, J.A.M. Vermaseren, A. Vogt, The five-loop beta function of Yang–Mills theory with fermions. JHEP 02, 090 (2017). https://doi.org/10.1007/JHEP02(2017)090. arXiv:1701.01404
|t JHEP
|v 02
|y 2017
999 C 5 |a 10.1007/JHEP03(2017)020
|9 -- missing cx lookup --
|1 T Luthe
|p 020 -
|2 Crossref
|u T. Luthe, A. Maier, P. Marquard, Y. Schroder, Complete renormalization of QCD at five loops. JHEP 03, 020 (2017). https://doi.org/10.1007/JHEP03(2017)020. arXiv:1701.07068
|t JHEP
|v 03
|y 2017
999 C 5 |a 10.1016/j.physletb.2015.05.023
|9 -- missing cx lookup --
|1 T Liu
|p 330 -
|2 Crossref
|u T. Liu, M. Steinhauser, Decoupling of heavy quarks at four loops and effective Higgs-fermion coupling. Phys. Lett. B 746, 330 (2015). https://doi.org/10.1016/j.physletb.2015.05.023. arXiv:1502.04719
|t Phys. Lett. B
|v 746
|y 2015
999 C 5 |a 10.1016/S0010-4655(00)00155-7
|9 -- missing cx lookup --
|1 KG Chetyrkin
|p 43 -
|2 Crossref
|u K.G. Chetyrkin, J.H. Kuhn, M. Steinhauser, RunDec: a Mathematica package for running and decoupling of the strong coupling and quark masses. Comput. Phys. Commun. 133, 43 (2000). https://doi.org/10.1016/S0010-4655(00)00155-7. arXiv:hep-ph/0004189
|t Comput. Phys. Commun.
|v 133
|y 2000
999 C 5 |a 10.1016/j.cpc.2012.03.023
|9 -- missing cx lookup --
|1 B Schmidt
|p 1845 -
|2 Crossref
|u B. Schmidt, M. Steinhauser, CRunDec: a C++ package for running and decoupling of the strong coupling and quark masses. Comput. Phys. Commun. 183, 1845 (2012). https://doi.org/10.1016/j.cpc.2012.03.023. arXiv:1201.6149
|t Comput. Phys. Commun.
|v 183
|y 2012
999 C 5 |a 10.1016/j.cpc.2017.11.014
|9 -- missing cx lookup --
|1 F Herren
|p 333 -
|2 Crossref
|u F. Herren, M. Steinhauser, Version 3 of RunDec and CRunDec. Comput. Phys. Commun. 224, 333 (2018). https://doi.org/10.1016/j.cpc.2017.11.014. arXiv:1703.03751
|t Comput. Phys. Commun.
|v 224
|y 2018
999 C 5 |a 10.1103/PhysRevLett.119.102001
|9 -- missing cx lookup --
|2 Crossref
|u ALPHA collaboration, QCD coupling from a nonperturbative determination of the three-flavor $$\Lambda $$ parameter. Phys. Rev. Lett. 119, 102001 (2017). https://doi.org/10.1103/PhysRevLett.119.102001. arXiv:1706.03821
999 C 5 |a 10.1103/PhysRevD.78.054513
|9 -- missing cx lookup --
|2 Crossref
|u HPQCD collaboration, High-precision charm-quark mass from current-current correlators in lattice and continuum QCD. Phys. Rev. D 78, 054513 (2008). https://doi.org/10.1103/PhysRevD.78.054513. arXiv:0805.2999
999 C 5 |a 10.1103/PhysRevD.94.034507
|1 Y Maezawa
|9 -- missing cx lookup --
|2 Crossref
|u Y. Maezawa, P. Petreczky, Quark masses and strong coupling constant in 2+1 flavor QCD. Phys. Rev. D 94, 034507 (2016). https://doi.org/10.1103/PhysRevD.94.034507. arXiv:1606.08798
|t Phys. Rev. D
|v 94
|y 2016
999 C 5 |a 10.1016/0550-3213(92)90248-A
|9 -- missing cx lookup --
|1 B Grinstein
|p 369 -
|2 Crossref
|u B. Grinstein, E.E. Jenkins, A.V. Manohar, M.J. Savage, M.B. Wise, Chiral perturbation theory for f D(s) / f D and B B(s) / B B. Nucl. Phys. B 380, 369 (1992). https://doi.org/10.1016/0550-3213(92)90248-A. arXiv:hep-ph/9204207
|t Nucl. Phys. B
|v 380
|y 1992
999 C 5 |a 10.1103/PhysRevD.46.3929
|9 -- missing cx lookup --
|1 JL Goity
|p 3929 -
|2 Crossref
|u J.L. Goity, Chiral perturbation theory for SU(3) breaking in heavy meson systems. Phys. Rev. D 46, 3929 (1992). https://doi.org/10.1103/PhysRevD.46.3929. arXiv:hep-ph/9206230
|t Phys. Rev. D
|v 46
|y 1992
999 C 5 |1 AV Manohar
|y 2000
|2 Crossref
|u A.V. Manohar, M.B. Wise, Heavy quark physics. Camb. Monogr. Part. Phys. Nucl. Phys. Cosmol. 10, 1 (2000)
999 C 5 |a 10.1016/0370-2693(91)91916-J
|9 -- missing cx lookup --
|2 Crossref
|u X.-D. Ji, M.J. Musolf, Subleading logarithmic mass dependence in heavy meson form-factors. Phys. Lett. B 257, 409 (1991). https://doi.org/10.1016/0370-2693(91)91916-J
999 C 5 |a 10.1103/PhysRevD.84.074505
|9 -- missing cx lookup --
|2 Crossref
|u PACS-CS collaboration, Charm quark system at the physical point of 2+1 flavor lattice QCD. Phys. Rev. D 84, 074505 (2011). https://doi.org/10.1103/PhysRevD.84.074505. arXiv:1104.4600
999 C 5 |a 10.1088/1674-1137/abcd8f
|9 -- missing cx lookup --
|2 Crossref
|u $${\chi }$$QCD collaboration, Charmed and $$\phi $$ meson decay constants from 2+1-flavor lattice QCD. Chin. Phys. C 45, 023109 (2021). https://doi.org/10.1088/1674-1137/abcd8f. arXiv:2008.05208
999 C 5 |2 Crossref
|u RBC/UKQCD collaboration, SU(3)-breaking ratios for $$D_{(s)}$$ and $$B_{(s)}$$ mesons. arXiv:1812.08791
999 C 5 |a 10.22323/1.363.0234
|9 -- missing cx lookup --
|2 Crossref
|u J. Frison, A. Bussone, G. Herdoíza, C. Pena, J.Á. Romero, J. Ugarrio, Heavy semileptonics with a fully relativistic mixed action. PoS LATTICE2019, 234 (2019). https://doi.org/10.22323/1.363.0234. arXiv:1911.02412
999 C 5 |a 10.22323/1.430.0408
|9 -- missing cx lookup --
|2 Crossref
|u J. Frison, A. Conigli, G. Herdoíza, C. Pena, A comparison of Wilson and twisted mass valence quarks for charmed semileptonic form factors. PoS LATTICE2022, 408 (2023). https://doi.org/10.22323/1.430.0408

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