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Charged hadron fragmentation functions from collider data

, S. Kumano, A. Accardi, Phys. Rev. D 94(11), 114004 (2016)ADSCrossRefGoogle Scholar 18. V. Bertone, S. Carrazza, N.P. Hartland, E.R. Nocera, J. Rojo, Eur. Phys. J. C 77(8), 516 (2017 ... , L. Del Debbio, S. Forte, A. Guffanti, J.I. Latorre, J. Rojo, M. Ubiali, Nucl. Phys. B 838, 136 (2010)ADSCrossRefGoogle Scholar 38. R.D. Ball, V. Bertone, F. Cerutti, L. Del Debbio, S. Forte, A

Impact of the heavy-quark matching scales in PDF fits

17. O. Zenaiev, PoS DIS2016 , 033 ( 2016 ) 18. V. Bertone , S. Carrazza , J. Rojo , Comput. Phys. Commun . 185 , 1647 ( 2014 ). https://doi.org/10.1016/j.cpc. 2014 . 03 .007 19. V. Bertone , A. Glazov ... , JHEP 09 , 132 ( 2016 ). https://doi.org/10.1007/JHEP09( 2016 ) 132 25. R.D. Ball , V. Bertone , L. Del Debbio , S. Forte , A. Guffanti , J. Rojo , M. Ubiali , Phys. Lett. B 723 , 330 ( 2013 ). https

Kaon mixing beyond the SM from Nf = 2 tmQCD and model independent constraints from the UTA

We present the first unquenched, continuum limit, lattice QCD results for the matrix elements of the operators describing neutral kaon oscillations in extensions of the Standard Model. Owing to the accuracy of our calculation on ∆S = 2 weak Hamiltonian matrix elements, we are able to provide a refined Unitarity Triangle analysis improving the bounds coming from model independent...

Determination of the strong coupling constant \({\varvec{{\alpha _\mathrm{s} (m_\mathrm{Z})}}}\) in next-to-next-to-leading order QCD using H1 jet cross section measurements

. Begzsuren A. Belousov 14 V. Bertone A. Bolz 7 V. Boudry 0 G. Brandt V. Brisson 25 D. Britzger 7 A. Buniatyan 16 A. Bylinkin L. Bystritskaya 13 A. J. Campbell 5 K. B. Cantun Avila 12 K. Cerny 3 V. Chekelian 24 ... ). arXiv: 1506 . 06042 57. R.D. Ball , V. Bertone , L. Del Debbio , S. Forte , A. Guffanti , J.I. Latorre , S. Lionetti , J. Rojo , M. Ubiali , Phys. Lett. B 707 , 66 ( 2012 ). arXiv: 1110 . 2483 58. L.A