001     586744
005     20241211214813.0
024 7 _ |a Ablinger:2023cbp
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024 7 _ |a arXiv:2306.16550
|2 arXiv
024 7 _ |a 10.3204/PUBDB-2023-03982
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037 _ _ |a PUBDB-2023-03982
041 _ _ |a English
088 _ _ |a arXiv:2306.16550
|2 arXiv
088 _ _ |a DESY-23-089
|2 DESY
088 _ _ |a DO-TH 23/09
|2 Fermilab
088 _ _ |a CERN-TH-2023-122
|2 CERN
088 _ _ |a ZU-TH 29/23
|2 Other
088 _ _ |a RISC Report Series 23-09
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088 _ _ |a MSUHEP-23-018
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100 1 _ |a Ablinger, J.
|b 0
245 _ _ |a Recent 3-Loop Heavy Flavor Corrections to Deep-Inelastic Scattering
260 _ _ |c 2023
336 7 _ |a Preprint
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336 7 _ |a ARTICLE
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500 _ _ |a Proc RADCOR 2023, 7 pages, 1 figure
520 _ _ |a We report on recent progress in calculating the three loop QCD corrections of the heavy flavor contributions in deep--inelastic scattering and the massive operator matrix elements of the variable flavor number scheme. Notably we deal with the operator matrix elements $A_{gg,Q}^{(3)}$ and $A_{Qg}^{(3)}$ and technical steps to their calculation. In particular, a new method to obtain the inverse Mellin transform without computing the corresponding $N$--space expressions is discussed.
536 _ _ |a 611 - Fundamental Particles and Forces (POF4-611)
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536 _ _ |a TOPUP - Theory of particle collider processes at ultimate precision (101019620)
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536 _ _ |a SAGEX - Scattering Amplitudes: from Geometry to Experiment (764850)
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588 _ _ |a Dataset connected to INSPIRE
650 _ 7 |a quantum chromodynamics, correction
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650 _ 7 |a heavy quark
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650 _ 7 |a scattering
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650 _ 7 |a flavor
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650 _ 7 |a deep inelastic scattering
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693 _ _ |0 EXP:(DE-MLZ)NOSPEC-20140101
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700 1 _ |a Behring, A.
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700 1 _ |a Blümlein, J.
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700 1 _ |a Freitas, Abilio de
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700 1 _ |a Goedicke, A.
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700 1 _ |a von Manteuffel, A.
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700 1 _ |a Schneider, C.
|b 6
700 1 _ |a Schönwald, K.
|0 P:(DE-H253)PIP1026518
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856 4 _ |u https://bib-pubdb1.desy.de/record/586744/files/2306.16550v1.pdf
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913 1 _ |a DE-HGF
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914 1 _ |y 2023
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980 _ _ |a I:(DE-H253)Z_ZPPT-20210408
980 _ _ |a UNRESTRICTED
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