Heavy-flavor parton distributions without heavy-flavor matching prescriptions
A bstract We show that the well-known obstacle for working with the zero-mass variable flavor number scheme, namely, the omission of O 1 mass power corrections close to the conventional heavy flavor matching point (HFMP) μ b = m , can be easily overcome. For this it is sufficient to take advantage o...
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Published in | The journal of high energy physics Vol. 2018; no. 4; pp. 1 - 32 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
01.04.2018
Springer Nature B.V SpringerOpen |
Subjects | |
Online Access | Get full text |
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Summary: | A
bstract
We show that the well-known obstacle for working with the zero-mass variable flavor number scheme, namely, the omission of
O
1
mass power corrections close to the conventional heavy flavor matching point (HFMP)
μ
b
=
m
, can be easily overcome. For this it is sufficient to take advantage of the freedom in choosing the position of the HFMP. We demonstrate that by choosing a sufficiently large HFMP, which could be as large as 10 times the mass of the heavy quark, one can achieve the following improvements: 1) above the HFMP the size of missing power corrections
O
m
is restricted by the value of
μ
b
and, therefore, the error associated with their omission can be made negligible; 2) additional prescriptions for the definition of cross-sections are not required; 3) the resummation accuracy is maintained and 4) contrary to the common lore we find that the discontinuity of
α
s
and pdfs across thresholds leads to improved continuity in predictions for observables. We have considered a large set of proton-proton and electron-proton collider processes, many through NNLO QCD, that demonstrate the broad applicability of our proposal. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP04(2018)046 |