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A new subtraction scheme at NLO exploiting the privilege of kT-factorization
High Energy Physics - Phenomenology · Submitted 5 Dec 2023
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The main difference with existing methods for collinear factorization is that we subtract the momentum recoil, occurring due to the mapping from an (n+1)-particle phase space to an n-particle phase space, from the initial-state momenta, instead of distributing it over the final-state momenta.
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The abstract, sentence by sentence
We present a subtraction method for the calculation of real-radiation integrals at NLO in hybrid kT-factorization. The main difference with existing methods for collinear factorization is that we subtract the momentum recoil, occurring due to the mapping from an (n+1)-particle phase space to an n-particle phase space, from the initial-state momenta, instead of distributing it over the final-state momenta.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a subtraction method for the calculation of real-radiation integrals at NLO in hybrid kT-factorization. | contribution 0.99 | 0.94 | 0.28 | asserted 1.00 |
| s1 | The main difference with existing methods for collinear factorization is that we subtract the momentum recoil, occurring due to the mapping from an (n+1)-particle phase space to an n-particle phase space, from the initial-state momenta, instead of distributing it over the final-state momenta. | method 0.73 | 0.86 | 0.35 | asserted 1.00 |
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The paper
Original abstract
We present a subtraction method for the calculation of real-radiation integrals at NLO in hybrid kT-factorization. The main difference with existing methods for collinear factorization is that we subtract the momentum recoil, occurring due to the mapping from an (n+1)-particle phase space to an n-particle phase space, from the initial-state momenta, instead of distributing it over the final-state momenta.
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References
How the literature uses it
2 arXiv papers cite this in 2 sentences
Papers citing it
Cites it as background 2 papers
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Furthermore, newer methods at NLO have also been developed [ref] .
Idealised Antenna Functions for Higher Order QCD Calculations · Slicing and Subtraction · 0.93
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Other methods have been established, notably the Nagy-Soper scheme [ref] , and others continue to be developed [ref] .
Initial-Final and Initial-Initial antenna functions for real radiation at next-to-leading order · Introduction · 0.97
What it cites
Uses the method or tool of 2 papers
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In particular, we augmented the phase space generator Kaleu ( [ref] ) with the channels matching the subtraction terms within the adaptive multi-channel method [ref] , in order to achieve convergent Monte Carlo estimates of the phase space integrals.
Kaleu: a general-purpose parton-level phase space generator · Numerical checks · 1.00
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In particular, we augmented the phase space generator Kaleu ( [ref] ) with the channels matching the subtraction terms within the adaptive multi-channel method [ref] , in order to achieve convergent Monte Carlo estimates of the phase space integrals.
Weight optimization in multichannel Monte Carlo · Numerical checks · 1.00
Uses data or values from 3 papers
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The parton branching PDFs PB-NLO-HERAI+II-2018set2 [ref] , taken from TMDlib [ref] , were employd for the space-like side, and CT18nlo [ref] , taken from LHAPDF [ref] , for the on-shell side.
LHAPDF6: parton density access in the LHC precision era · Numerical checks · 0.92
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The parton branching PDFs PB-NLO-HERAI+II-2018set2 [ref] , taken from TMDlib [ref] , were employd for the space-like side, and CT18nlo [ref] , taken from LHAPDF [ref] , for the on-shell side.
Progress in the CTEQ-TEA NNLO global QCD analysis · Numerical checks · 0.92
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We present results for both $k_T$-dependent PDFs PB-NLO-HERAI+II-2018set2 and KS-2013-linear [ref] .
Gluon saturation in dijet production in p-Pb collisions at Large Hadron Collider · On-shell limit · 0.84
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