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Related papers: PQCD Formulations with Heavy Quark Masses and Glob…

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We examine the relevance of the heavy quarks masses in the perturbative QCD description of hard interactions where charged kaons are produced in the final state. We extract a set of parton-to-kaon hadronization probabilities from a next to…

High Energy Physics - Phenomenology · Physics 2019-01-02 Manuel Epele , Carlos García Canal , Rodolfo Sassot

In a consistently formulated pQCD framework incorporating non-zero mass heavy quark partons, there is still the freedom to define parton distributions obeying either mass-independent or mass-dependent evolution equations, contrary to…

High Energy Physics - Phenomenology · Physics 2009-10-30 Fredrick I. Olness , Randall J. Scalise

We define a new variable flavour number scheme for use in deep inelastic scattering, motivated by the need to consistently implement high energy resummations alongside a fixed order QCD expansion. We define the DIS(chi) scheme at fixed…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. D. White , R. S. Thorne

I explore the rich phase diagram of two-flavor QCD as a function of the quark masses. The theory involves three parameters, including one that is CP violating. As the masses vary, regions of both first and second order transitions are…

High Energy Physics - Phenomenology · Physics 2011-02-03 Michael Creutz

We study the effect of the charm quark mass in the CTEQ global analysis of parton distribution functions (PDFs) of the proton. Constraints on the $\bar{\rm MS}$ mass of the charm quark are examined at the next-to-next-to-leading order…

High Energy Physics - Phenomenology · Physics 2015-06-15 Jun Gao , Marco Guzzi , Pavel M. Nadolsky

I discuss advances in the determination of strange, charm, and bottom quark parton distribution functions obtained in the CTEQ6.5 and CTEQ6.6 global analyses. These results affect electroweak precision observables and certain new physics…

High Energy Physics - Phenomenology · Physics 2008-09-08 Pavel M. Nadolsky

Where appropriate, the abbreviation 'VFNS' is replaced by 'CSN' to indicate the scheme using massive heavy quark coefficient functions proposed in this paper. The text below Eq. (2.13) and between Eqs. (2.33) and (2.36) has been…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Chuvakin , J. Smith , W. L. van Neerven

The FONLL general-mass variable-flavour number scheme provides a framework for the matching of a calculation in which a heavy quark is treated as a massless parton to one in which the mass dependence is retained throughout. We describe how…

High Energy Physics - Phenomenology · Physics 2016-02-17 Richard D. Ball , Valerio Bertone , Marco Bonvini , Stefano Forte , Patrick Groth Merrild , Juan Rojo , Luca Rottoli

We present the matching relations of the variable flavor number scheme at next-to-leading order, which are of importance to define heavy quark partonic distributions for the use at high energy colliders such as Tevatron and the LHC. The…

High Energy Physics - Phenomenology · Physics 2018-07-04 J. Blümlein , A. De Freitas , C. Schneider , K. Schönwald

Recent accurate data on F_2(x,Q) and on F_2^c(x,Q) from HERA at small-x require a more precise treatment of charm production in the global QCD analysis of parton distributions. We improve on existing global analyses by implementing the…

High Energy Physics - Phenomenology · Physics 2007-05-23 H. L. Lai , W. K. Tung

We present a new prescription to account for heavy quark mass effects in the determination of parton distribution functions (PDFs) based on the FONLL scheme. Our prescription makes explicit use of the freedom to choose the number of active…

High Energy Physics - Phenomenology · Physics 2024-10-04 Andrea Barontini , Alessandro Candido , Felix Hekhorn , Giacomo Magni , Roy Stegeman

I consider variations in the definition of a General-Mass Variable Flavour Number Scheme (GM-VFNS) for heavy flavour structure functions, both at next-to-leading order (NLO) and at next-to-next-to leading order (NNLO). I also define a new…

High Energy Physics - Phenomenology · Physics 2010-11-19 R. S. Thorne

We discuss the implementation of the FONLL general-mass scheme for heavy quarks in deep-inelastic scattering in the FastKernel framework, used in the NNPDF series of global PDF analysis. We present the general features of FONLL and…

High Energy Physics - Phenomenology · Physics 2010-11-19 J. Rojo , R. D. Ball , V. Bertone , F. Cerutti , L. Del Debbio , S. Forte , A. Guffanti , J. I. Latorre , M. Ubiali

We introduce a Hybrid Variable Flavor Number Scheme for heavy flavors, denoted H-VFNS, which incorporates the advantages of both the traditional Variable Flavor Number Scheme (VFNS) as well as the Fixed Flavor Number Scheme (FFNS). By…

High Energy Physics - Phenomenology · Physics 2013-11-22 A. Kusina , F. I. Olness , I. Schienbein , T. Jezo , K. Kovarik , T. Stavreva , J. Y. Yu

We present a detailed discussion of the collinear subtraction terms needed to establish a massive variable-flavour-number scheme for the one-particle inclusive production of heavy quarks in hadronic collisions. The subtraction terms are…

High Energy Physics - Phenomenology · Physics 2011-09-13 B. A. Kniehl , G. Kramer , I. Schienbein , H. Spiesberger

I give an introduction to the QCD-based theory of the heavy flavor hadrons and their weak decays. Trying to remain at the next-to-elementary level and skip technicalities, I concentrate on the qualitative description of the most important…

High Energy Physics - Phenomenology · Physics 2007-05-23 Nikolai Uraltsev

Considered as a function of the quark mases, two-flavor QCD depends on three parameters, including one that is CP violating. As the masses vary to unphysical values, regions of both first- and second-order phase transitions are expected.…

High Energy Physics - Phenomenology · Physics 2011-10-20 Michael Creutz

We introduce a Hybrid Variable Flavor Number Scheme (H-VFNS) for heavy flavors, which incorporates the advantages of both the traditional Variable Flavor Number Scheme (VFNS) as well as the Fixed Flavor Number Scheme (FFNS). We include an…

High Energy Physics - Phenomenology · Physics 2013-12-13 A. Kusina , F. I. Olness , I. Schienbein , T. Jezo , K. Kovarik , T. Stavreva , J. Y. Yu

We give an overview of recent progress in the study of fermion mass and flavor mixing phenomena. The hints exhibited by the quark and lepton mass spectra towards possible underlying flavor symmetries, from which realistic models of mass…

High Energy Physics - Phenomenology · Physics 2014-11-17 Harald Fritzsch , Zhi-zhong Xing

We study the sensitivity of our recent MSTW 2008 NLO and NNLO PDF analyses to the values of the charm- and bottom-quark masses, and we provide additional public PDF sets for a wide range of these heavy-quark masses. We quantify the impact…

High Energy Physics - Phenomenology · Physics 2010-11-23 A. D. Martin , W. J. Stirling , R. S. Thorne , G. Watt