1.

Asymptotic behavior of the heavy quark form factors at higher order
/ Blümlein, J. ; Marquard, P. ; Rana, N.
In the asymptotic limit ${Q}^{2}\gg {m}^{2}$, the heavy quark form factors exhibit Sudakov behavior. [...]
Published in Physical Review D 99 (2019)
10.1103/PhysRevD.99.016013
arXiv:1810.08943
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2.

Automated solution of first order factorizable systems of differential equations in one variable
/ Ablinger, J. ; Blümlein, J. ; Marquard, P. ; Rana, N. ; et al
We present an algorithm which allows to solve analytically linear systems of differential equations which factorize to first order. [...]
Published in Nuclear Physics B 939 (2019) 253291
10.1016/j.nuclphysb.2018.12.010
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3.

NLO PDFs from the ABMP16 fit
/ Alekhin, S. ; Blümlein, J. ; Moch, S.
We perform a global fit of parton distribution functions (PDFs) together with the strong coupling constant αs and the quark masses mc , mb and mt at nexttoleading order (NLO) in QCD. [...]
Published in EPJC 78 (2018) 477
10.1140/epjc/s1005201859471
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4.

Heavy quark form factors at three loops in the planar limit
/ Ablinger, J. ; Blümlein, J. ; Marquard, P. ; Rana, N. ; et al
We compute the colorplanar and complete light quark nonsinglet contributions to the heavy quark form factors in the case of the axialvector, scalar and pseudoscalar currents at three loops in perturbative QCD. [...]
Published in Physics letters B (2018)
10.1016/j.physletb.2018.05.077
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5.

Heavy quark form factors at two loops
/ Ablinger, J. ; Behring, A. ; Blümlein, J. ; Falcioni, G. ; et al
We compute the twoloop QCD corrections to the heavy quark form factors in the case of the vector, axialvector, scalar and pseudoscalar currents up to second order in the dimensional parameter $\u03f5=(4D)/2$. [...]
Published in Physical Review D 97 (2018)
10.1103/PhysRevD.97.094022
arXiv:1712.09889
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6.

The variable flavor number scheme at nexttoleading order
/ Blümlein, J. ; De Freitas, A. ; Schneider, C. ; Schönwald, K.
We present the matching relations of the variable flavor number scheme at nexttoleading order, which are of importance to define heavy quark partonic distributions for the use at high energy colliders such as Tevatron and the LHC. [...]
Published in Physics letters B (2018)
10.1016/j.physletb.2018.05.054
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7.

The twomass contribution to the threeloop gluonic operator matrix element Agg,Q(3)
/ Ablinger, J. ; Blümlein, J. ; De Freitas, A. ; Goedicke, A. ; et al
We calculate the twomass QCD contributions to the massive operator matrix element Agg,Q at O(αs3) in analytic form in Mellin N  and z space, maintaining the complete dependence on the heavy quark mass ratio. [...]
Published in Nuclear Physics B (2018)
10.1016/j.nuclphysb.2018.04.023
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8.

The twomass contribution to the threeloop pure singlet operator matrix element
/ Ablinger, J. ; Blümlein, J. ; De Freitas, A. ; Schneider, C. ; et al
We present the twomass QCD contributions to the pure singlet operator matrix element at three loop order in x space. [...]
Published in Nuclear Physics B (2017)
10.1016/j.nuclphysb.2017.12.018
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9.

Strange sea determination from collider data
/ Alekhin, S. ; Blümlein, J. ; Moch, S.
We consider determinations of the strange sea in the nucleon based on QCD analyses of data collected at the LHC with focus on the recent highstatistics ATLAS measurement of the W±  and Z boson production. [...]
Published in Physics letters B (2017)
10.1016/j.physletb.2017.12.024
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10.

Running of the charmquark mass from HERA deepinelastic scattering data
/ Gizhko, A. ; Geiser, A. ; Moch, S. ; Abt, I. ; et al
Combined HERA data on charm production in deepinelastic scattering have previously been used to determine the charmquark running mass mc(mc) in the MS‾ renormalisation scheme. [...]
Published in Physics letters B (2017)
10.1016/j.physletb.2017.11.002
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