Tomas Jezo
University of Milan
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Featured researches published by Tomas Jezo.
Physical Review D | 2016
Karol Kovarik; A. Kusina; Tomas Jezo; D. B. Clark; C. Keppel; Florian Lyonnet; J. Morfin; F. Olness; J.F. Owens; Ingo Schienbein; J. Yu
We present the new nCTEQ15 set of nuclear parton distribution functions with uncertainties. This fit extends the CTEQ proton PDFs to include the nuclear dependence using data on nuclei all the way up to 208^Pb. The uncertainties are determined using the Hessian method with an optimal rescaling of the eigenvectors to accurately represent the uncertainties for the chosen tolerance criteria. In addition to the Deep Inelastic Scattering (DIS) and Drell-Yan (DY) processes, we also include inclusive pion production data from RHIC to help constrain the nuclear gluon PDF. Furthermore, we investigate the correlation of the data sets with specific nPDF flavor components, and asses the impact of individual experiments. We also provide comparisons of the nCTEQ15 set with recent fits from other groups.
Journal of High Energy Physics | 2015
Florian Lyonnet; A. Kusina; Tomas Jezo; Karol Kovarik; Fred Olness; Ingo Schienbein; ans Ji-Young Yu
A bstractHeavy quark parton distribution functions (PDFs) play an important role in several Standard Model and New Physics processes. Most analyses rely on the assumption that the charm and bottom PDFs are generated perturbatively by gluon splitting and do not involve any non-perturbative degrees of freedom. It is clearly necessary to test this hypothesis with suitable QCD processes. Conversely, a non-perturbative, intrinsic heavy quark parton distribution has been predicted in the literature. We demonstrate that to a very good approximation the scale-evolution of the intrinsic heavy quark content of the nucleon is governed by non-singlet evolution equations. This allows us to analyze the intrinsic heavy quark distributions without having to resort to a full-fledged global analysis of parton distribution functions. We exploit this freedom to model intrinsic bottom distributions which are so far missing in the literature in order to estimate the impact of this non-perturbative contribution to the bottom-quark PDF, and on parton-parton luminosities at the LHC. This technique can be applied to the case of intrinsic charm, albeit within the limitations outlined in the following.
Physical Review D | 2012
Tomas Jezo; Ingo Schienbein; Michael Klasen
General SU(2)xSU(2)xU(1) models represent a well-motivated intermediate step towards the unification of the Standard Model gauge groups. Based on a recent global analysis of low-energy and LEP constraints of these models, we perform numerical scans of their various signals at the LHC. We show that total cross sections for lepton and third-generation quark pairs, while experimentally easily accessible, provide individually only partial information about the model realized in Nature. In contrast, correlations of these cross sections in the neutral and charged current channels may well lead to a unique identification.
arXiv: High Energy Physics - Phenomenology | 2012
T. Stavreva; Tomas Jezo; K. Kovarik; A. Kusina; F. Olness; J. Yu; I. Schienbein
We analyze the properties of the ACOT scheme for heavy quark production and make use of the MS-Bar massless results at NNLO and N3LO for the structure functions F2 and FL in neutral current deep-inelastic scattering to estimate the higher order corrections. The dominant heavy quark mass effects at higher orders can be taken into account using the massless Wilson coefficients together with an appropriate slow-rescaling prescription implementing the phase space constraints. Combining the exact ACOT scheme at NLO with these expressions should provide a good approximation to the full calculation in the ACOT scheme at NNLO and N3LO.
Proceedings of XXIV International Workshop on Deep-Inelastic Scattering and Related Subjects — PoS(DIS2016) | 2016
D. B. Clark; Eric Godat; Tomas Jezo; Karol Kovarik; A. Kusina; Florian Lyonnet; Fred Olness; I. Schienbein; J. Yu
The discovery potential of the LHC depends sensitively on the input PDFs. Despite extensive efforts, the precision of the heavy quark distributions have significant uncertainties. We illustrate some of these issues for the case of the strange quark whose extraction is intertwined with the corresponding nuclear corrections. The use of LHC W/Z production data from both proton and heavy-ion beams could substantively improve the precision of both the PDFs and the nuclear corrections.
Proceedings of XXIII International Workshop on Deep-Inelastic Scattering — PoS(DIS2015) | 2016
A. Kusina; K. Kovarik; Tomas Jezo; Benjamin D Clark; Cynthia Keppel; Florian Lyonnet; J. Morfin; Fred Olness; J.F. Owens; Ingo Schienbein; Ji Young Yu
We present the first official release of the nCTEQ nuclear parton distribution functions with errors. The main addition to the previous nCTEQ PDFs is the introduction of PDF uncertainties based on the Hessian method. Another important addition is the inclusion of pion production data from RHIC that give us a handle on constraining the gluon PDF. This contribution summarizes our results from arXiv:1509.00792 and concentrates on the comparison with other groups providing nuclear parton distributions.
Proceedings of XXIII International Workshop on Deep-Inelastic Scattering — PoS(DIS2015) | 2016
Florian Lyonnet; A. Kusina; Karol Kovarik; Tomas Jezo; Fred Olness; I. Schienbein; Ji Young Yu
We demonstrate that to a very good approximation the scale-evolution of the intrinsic heavy quark content of the nucleon is governed by non-singlet evolution equations. This allows us to analyze the intrinsic heavy quark distributions without having to resort to a full-fledged global analysis of parton distribution functions. This freedom is then exploited to model intrinsic bottom distributions which are so far missing in the literature in order to estimate the impact of this non-perturbative contribution to the bottom-quark PDF, and on parton--parton luminosities at the LHC. This technique can be applied to the case of intrinsic charm, albeit within the limitations outlined in the following.
arXiv: High Energy Physics - Phenomenology | 2013
A. Kusina; Tomas Jezo; K. Kovarik; T. Stavreva; Fredrick I. Olness; S. Berge; J. Yu; I. Schienbein; K. Park
We investigate the impact of parton distribution functions (PDFs) uncertainties on W/Z production at the LHC, concentrating on the strange quark PDF. Additionally we examine the extent to which precise measurements at the LHC can provide additional information on the proton flavor structure.
arXiv: High Energy Physics - Phenomenology | 2013
A. Kusina; Fred Olness; Ingo Schienbein; Tomas Jezo; K. Kovarik; T. Stavreva; Ji Young Yu
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 explicit dependence on number of active flavors
arXiv: High Energy Physics - Phenomenology | 2013
K. Kovarik; Tomas Jezo; A. Kusina; T. Stavreva; F. Olness; J. Yu; I. Schienbein
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