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001     293672
005     20211110133230.0
024 7 _ |a 10.3204/DESY-PROC-2012-02/272
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024 7 _ |a arXiv:1206.2325
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024 7 _ |a inspire:1117879
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088 1 _ |a arXiv:1206.2325
088 _ _ |a arXiv:1206.2325
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100 1 _ |a Stavreva, T.
|b 0
111 2 _ |a 20th International Workshop on Deep-Inelastic Scattering and Related Subjects
|g DIS 2012
|c Bonn
|d 2012-03-26 - 2012-03-30
|w Germany
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245 _ _ |a Heavy Quark Production in the ACOT Scheme Beyond NLO
260 _ _ |a Hamburg
|c 2012
|b Deutsches Elektronen-Synchrotron, DESY
300 _ _ |a 243-246
336 7 _ |a Conference Paper
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336 7 _ |a INPROCEEDINGS
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520 _ _ |a 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.
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650 _ 7 |a heavy quark: production
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650 _ 7 |a heavy quark: mass
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650 _ 7 |a deep inelastic scattering: neutral current
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650 _ 7 |a correction: higher-order
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650 _ 7 |a mass: effect
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650 _ 7 |a structure function
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650 _ 7 |a phase space
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700 1 _ |a Olness, F. I.
|b 1
700 1 _ |a Schienbein, I.
|b 2
700 1 _ |a Jezo, T.
|b 3
700 1 _ |a Kusina, A.
|b 4
700 1 _ |a Kovarik, K.
|b 5
700 1 _ |a Yu, J. Y.
|b 6
773 _ _ |a 10.3204/DESY-PROC-2012-02/272
787 0 _ |a Brock, Ian
|d Hamburg : Deutsches Elektronen-Synchrotron, DESY, Hamburg, 2013
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|r DESY-PROC-2012-02
|t Proceedings, 20th International Workshop on Deep-Inelastic Scattering and Related Subjects (DIS 2012)
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