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For a precise determination of the m_u and m_d quark masses, it is useful to combine isospin symmetric results of lattice or sum rules QCD techniques with some isospin breaking study performed in chiral perturbation theory (ChPT).
R. F. Dashen, Chiral SU(3) x SU(3) as a symmetry of the strong interactions, Phys. Rev. 183 (1969) 1245–1260
1969
Earlier work this paper cites.
J. Gasser, H. Leutwyler, Chiral Perturbation Theory: Expansions in the Mass of the Strange Quark, Nucl. Phys. B250 (1985) 465
1985
Earlier work this paper cites.
arXiv:hep-ph/9507319
M. Knecht, B. Moussallam, J. Stern, N. H. Fuchs, The Low-energy π π \pi\pi amplitude to one and two loops, Nucl. Phys. B457 (1995) 513–576 · 1995
Earlier work this paper cites.
arXiv:hep-ph/9509374
J. Kambor, C. Wiesendanger, D. Wyler, Final State Interactions and Khuri-Treiman Equations in η → 3 π \eta\to 3\pi decays, Nucl. Phys. B465 (1996) 215–266 · 1996
Earlier work this paper cites.
arXiv:hep-ph/9601237
A. V. Anisovich, H. Leutwyler, Dispersive analysis of the decay η → 3 π \eta\to 3\pi , Phys. Lett. B375 (1996) 335–342 · 1996
Earlier work this paper cites.
arXiv:hep-ph/9610360
J. Bijnens, J. Prades, Electromagnetic corrections for pions and kaons: Masses and polarizabilities, Nucl. Phys. B490 (1997) 239–271 · 1997
Earlier work this paper cites.
arXiv:hep-ph/0101127
G. Amoros, J. Bijnens, P. Talavera, QCD isospin breaking in meson masses, decay constants and quark mass ratios, Nucl. Phys. B602 (2001) 87–108 · 2001
Earlier work this paper cites.
D. B. Kaplan, A. V. Manohar, Current Mass Ratios of the Light Quarks, Phys. Rev. Lett. 56 (1986) 2004
2004
Cited alongside, same era.
arXiv:hep-ph/0405206
B. Ananthanarayan, B. Moussallam, Four-point correlator constraints on electromagnetic chiral parameters and resonance effective Lagrangians, JHEP 0406 (2004) 047 · 2004
Cited alongside, same era.
J. Bijnens, K. Ghorbani, η → 3 π \eta\to 3\pi at Two Loops In Chiral Perturbation Theory, JHEP 11 (2007) 030 · 2007
Cited alongside, same era.
F. Ambrosino, et al., Determination of η → π + π − π 0 \eta\to\pi^{+}\pi^{-}\pi^{0} Dalitz plot slopes and asymmetries with the KLOE detector, JHEP 05 (2008) 006 · 2008
Cited alongside, same era.
A. Kastner, H. Neufeld, The K ℓ 3 K_{\ell 3} scalar form factors in the standard model, Eur. Phys. J. C57 (2008) 541–556 · 2008
K. Nakamura, et al., Review of particle physics , J. Phys. G37 (2010) 075021
2010
Later among the works it cites.
T. Blum, et al., Electromagnetic mass splittings of the low lying hadrons and quark masses from 2+1 flavor lattice QCD+QED, Phys. Rev. D82 (2010) 094508 · 2010
Later among the works it cites.
J. Laiho, E. Lunghi, R. S. Van de Water, Lattice QCD inputs to the CKM unitarity triangle analysis, Phys.Rev. D81 (2010) 034503 · 2010
Later among the works it cites.
F.-K. Guo, C. Hanhart, U.-G. Meißner, Extracting the light quark mass ratio m u / m d m_{u}/m_{d} from bottomonia transitions, Phys. Rev. Lett. 105 (2010) 162001 · 2010
Later among the works it cites.
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Cited alongside, same era.
H. Leutwyler, Light quark masses, PoS CD09 (2009) 005 · 2009
Cited alongside, same era.
G. Colangelo, S. Lanz, E. Passemar, A New Dispersive Analysis of η → 3 π \eta\to 3\pi , PoS CD09 (2009) 047 · 2009
Cited alongside, same era.
Cited in the paper.
Cited in the paper.
R. Kaiser, H. Leutwyler, Pseudoscalar decay constants at large N(c), arXiv:hep-ph/9806336
Cited in the paper.
S. Durr, et al., Lattice QCD at the physical point: Simulation and analysis details, arXiv:1011.2711
Cited in the paper.
C. Dominguez, Quark masses in QCD: a progress report, Mod. Phys. Lett. A26 (2011) 691–710 · 2011
Closest in time.
G. Colangelo, et al., Review of lattice results concerning low energy particle physics, Eur. Phys. J. C71 (2011) 1695 · 2011
Closest in time.
S. P. Schneider, B. Kubis, C. Ditsche, Rescattering effects in η → 3 π \eta\to 3\pi decays, JHEP 1102 (2011) 028 · 2011
Closest in time.