Abstract

The past several years have witnessed important developments in the QCD theory of jet production and jet substructure in hadronic collisions. In the framework of soft-collinear effective theory, semi-inclusive jet functions and semi-inclusive fragmenting jet functions have allowed us to combine higher order calculations with resummation of potentially large logarithms of the jet radius, ln R. Very recently, the semi-inclusive jet functions for partons fragmenting into heavy flavor jets were computed by Dai, Kim and Leibovich. In this paper we show how the formalism can be extended to c-jet and b-jet production in heavy ion collisions. The semi-inclusive jet functions for heavy flavor jets in a QCD medium are evaluated up to the next-to-leading order in αs and first order in opacity. For phenomenological applications, we also consider the inclusion of the cold nuclear matter effects and the jet energy dissipation due to collisional interactions in matter. We present the numerical predictions for the cross sections and the corresponding nuclear modification factors in proton-nucleus and nucleus-nucleus collisions and compare our results to data from the Large Hadron Collider.

Highlights

  • We presented a formalism to study heavy flavor jet production in hadronic and heavy-ion collisions using the heavy flavor semi-inclusive jet functions

  • This approach relies on hard-collinear factorization, where the cross section is expressed as the convolution of the PDFs, the hard kernel, and jet functions

  • For light-flavor jets, similar formalism has been applied to the inclusive jet production and jet substructure yielding gains in the accuracy of theoretical predictions

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Summary

Semi-inclusive jet functions for heavy flavor

We discuss in detail the definition of the heavy quark-tagged SiJFs. For completeness, we briefly recall some analytical results from ref. [17] for the vacuum SiJFs. For completeness, we briefly recall some analytical results from ref. [17] for the vacuum SiJFs We extend these SiJFs to the case of heavy-ion collisions in the perturbative theory

Jet functions in vacuum
Medium corrections
Numerical results
Findings
Conclusions
Full Text
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