Publikationen
2024
| J Blümlein, A. De Freitas, P. Marquard, C. Schneider | Challenges for analytic calculations of the massive three-loop form factors | arXiv:2408.07046 |
| J. Ablinger, A. Behring, J. Blümlein, A. De Freitas, A. von Manteuffel, C. Schneider, K. Schoenwald | The three-loop single-mass heavy flavor corrections to deep-inelastic scattering | arXiv:2407.02006 |
| J. Blümlein, M. Saragnese | Next-to-Next-to-Leading Order Evolution of Polarized Parton Densities in the Larin Scheme | arXiv:2405.17252 |
| J. Ablinger, A. Behring, J. Blümlein, A. De Freitas, A. von Manteuffel, C. Schneider, K. Schönwald | The non-first-order-factorizable contributions to the three-loop single-mass operator matrix elements A^(3)_Qg and ΔA^(3)_Qg | arXiv:2403.00513 |
2023
| J. Ablinger, A. Behring, J. Blümlein, A. De Freitas, A. von Manteuffel, C. Schneider, K. Schönwald | The first-order factorizable contributions to the three-loop massive operator matrix elements A(3)Qg and ΔA(3)Qg | arXiv:2311.00644 |
| Johannes Bluemlein, Nikolai Fawwdeev, Carsten Schneider | Computing Mellin representations and asymptotics of nested binomial sums in a symbolic way: the RICA package | arXiv:2308.06042 |
| Johannes Blümlein, Abilio De Freitas, Peter Marquard, Narayan Rana, Carsten Schneider | Analytic results on the massive three-loop form factors: quarkonic contributions | arXiv:2307.02983 |
| J. Ablinger, A. Behring, J.Blümlein, A. De Freitas et al. | Recent 3-Loop Heavy Flavor Corrections to Deep-Inelastic Scattering | arXiv:2306.16550 |
| Andrei Afanasev, Jan C. Bernauer, Peter Blunden, Johannes Blümlein, Ethan W. Cline et al. | Radiative Corrections: From Medium to High Energy Experiments | arXiv:2306.14578 |
| Johannes Blümlein | Deep-Inelastic Scattering: What do we know? | arXiv:2306.01362 |
| A. Behring, J. Blümlein, K. Schönwald | The inverse Mellin transform via analytic continuation | arXiv:2303.05943 |
2022
| I. Bierenbaum, J. Blümlein, A. De Freitas, A. Goedicke, S. Klein, K. Schönwald | O(α2s) Polarized Heavy Flavor Corrections to Deep-Inelastic Scattering at Q2≫m2 | arXiv:2211.15337 |
| J. Blümlein, P. Marquard, C. Schneider, K. Schönwald | The massless three-loop Wilson coefficients for the deep-inelastic structure functions F2,FL,xF3 and g1 | arXiv:2208.14325 |
| J. Blümlein, A. Maier, P. Marquard, G. Schäfer | Gravity in binary systems at the fifth and sixth post-Newtonian order | arXiv:2208.04552 |
| J. Blümlein, P. Marquard, C. Schneider, K. Schönwald | The 3-loop anomalous dimensions from off-shell operator matrix elements | arXiv:2207.07943 |
| J. Blümlein, C. Schneider | The SAGEX Review on Scattering Amplitudes, Chapter 4: Multi-loop Feynman Integrals | arXiv:2203.13015 |
| J. Blümlein, K. Schönwald | High Precision QED Initial State Corrections for e+e−→γ∗/Z∗ Annihilation | arXiv:2202.08476 |
| J. Blümlein, P. Marquard, C. Schneider, K. Schönwald | The Two-Loop Massless Off-Shell QCD Operator Matrix Elements to Finite Terms | arXiv:2202.03216 |
2021
| J. Blümlein, M. Saragnese, C. Schneider | Hypergeometric Structures in Feynman Integrals | arXiv:2111.15501 |
| J. Blümlein, P. Marquard, C. Schneider, K. Schönwald | The three-loop polarized singlet anomalous dimensions from off-shell operator matrix elements | arXiv:2111.12401 |
| J. Blümlein, A. Maier, P. Marquard, G. Schäfer | The fifth-order post-Newtonian Hamiltonian dynamics of two-body systems from an effective field theory approach | arXiv:2110.13822 |
| J. Ablinger, J. Blümlein, A. De Freitas, M. Saragnese, C. Schneider, K. Schönwald | New 2- and 3-loop heavy flavor corrections to unpolarized and polarized deep-inelastic scattering | arXiv:2107.09350 |
| J. Blümlein, P. Marquard, C. Schneider, K. Schönwald | The three-loop unpolarized and polarized non-singlet anomalous dimensions from off shell operator matrix elements | arXiv:2107.06267 |
| J. Blümlein, M. Saragnese | The N3LO Scheme-invariant QCD Evolution of the Non-singlet Structure Functions FNS2(x,Q2) and gNS1(x,Q2) | arXiv:2107.01293 |
| J. Blümlein, A. De Freitas, M. Saragnese, C. Schneider, K. Schönwald | The Logarithmic Contributions to the Polarized and Operator Matrix Elements in Deeply Inelastic Scattering | arXiv:2105.09572 |
| J. Blümlein | Analytic integration methods in quantum field theory: an Introduction | arXiv:2103.10652 |
| J. Ablinger, J. Blümlein, C. Schneider | Iterated integrals over letters induced by quadratic forms | arXiv:2103.08330 |
| J. Blümlein, A. De Freitas, K. Schönwald | The QED Initial State Corrections to the Forward-Backward Asymmetry of e+e−→γ∗/Z0∗ to Higher Orders | arXiv:2102.12237 |
| J. Blümlein, A. Maier, P. Marquard, G. Schäfer | The 6th Post-Newtonian Potential Terms at O(G4N) | arXiv:2101.08630 |
| A. Behring, J. Blümlein, A. De Freitas, A. von Manteuffel, K. Schönwald, C. Schneider | The Polarized Transition Matrix Element Agq(N) of the Variable Flavor Number Scheme at O(α3s) | arXiv:2101.05733 |
2020
| J. Blümlein, A. Maier, P. Marquard, G. Schäfer | The fifth-order post-Newtonian Hamiltonian dynamics of two-body systems from an effective field theory approach: potential contributions | arXiv:2010.13672 |
| S. Alekhin, J. Blümlein, S. Moch | Heavy-flavor PDF evolution and variable-flavor number scheme uncertainties in deep-inelastic scattering | arXiv:2006.07032 |
| J. Ablinger, J. Blümlein, A. De Freitas, A. Goedicke, M. Saragnese, C. Schneider, K. Schönwald | The Two-mass Contribution to the Three-Loop Polarized Operator Matrix Element A_{gg,Q}^{(3)} | arXiv:2004.08916 |
| J. Ablinger, J. Blümlein, A. De Freitas, K. Schönwald | Subleading Logarithmic QED Initial State Corrections to e^+e^- \rightarrow γ^*/{Z^{0}}^* to O(α^6 L^5) | arXiv:2004.04287 |
| J. Blümlein, A. De Freitas, C. Raab, K. Schönwald | The O(α^2) Initial State QED Corrections to e^+e^- \rightarrow γ^*/Z_0^* | arXiv:2003.14289 |
| J. Blümlein, A. Maier, P. Marquard, G. Schäfer | Testing binary dynamics in gravity at the sixth post-Newtonian level | arXiv:2003.07145 |
| J. Blümlein, A. Maier, P. Marquard, G. Schäfer | Fourth post-Newtonian Hamiltonian dynamics of two-body systems from an effective field theory approach | arXiv:2003.01692 |
2019
| J. Blümlein, P. Marquard, C. Schneider | A refined machinery to calculate large moments from coupled systems of linear differential equations | arXiv:1912.04390 |
| J. Blümlein, A. Maier, P. Marquard | The Gravitational Potential of Two Point Masses at Five Loops | arXiv:1912.03089 |
| J. Ablinger, A. Behring, J. Blümlein, A. De Freitas, A. von Manteuffel, C. Schneider, K. Schönwald | The three-loop single mass polarized pure singlet operator matrix element | arXiv:1912.02536 |
| J. Ablinger, J. Blümlein, A. De Freitas, M. Saragnese, C. Schneider, K. Schönwald | The three-loop polarized pure singlet operator matrix element with two different masses | arXiv:1911.11630 |
| A. Behring, J. Blümlein, A. de Freitas, A. Goedicke, S. Klein, A. van Manteuffel, C. Schneider, K. Schönwald | The Polarized Three-loop Anomalous Dimensions from a Massive Calculation | arXiv:1911.06189 |
| J. Blümlein, A. de Freitas, C. Raab, K. Schönwald | Revisiting the O(alpha^2) Initial State QED Corrections to e^+ e^- Annihilation into a Neutral Boson | arXiv:1911.05029 |
| J. Blümlein, A. Maier, P. Marquard, G. Schäfer, C. Schneider | From Momentum Expansions to Post-Minkowskian Hamiltonians by Computer Algebra Algorithms | arXiv:1911.04411 |
| S. Alekhin, J. Blümlein, S.-O. Moch | Resummation of large logarithms in the VFN scheme for DIS heavy-quark production | arXiv:1910.11165 |
| J. Blümlein, A. De Freitas, C.G. Raab, K. Schönwald | The effects of O(alpha^2) initial state QED corrections to e^+ e^- --> gamma*/Z* at very high luminosity colliders | arXiv:1910.05759 |
| S. Alekhin, J. Blümlein, S.-O. Moch | An Update of the ABM16 PDF Fit | arXiv:1909.03533 |
| A. Behring, J. Blümlein, A. De Freitas, A. Goedicke, S. Klein, A. von Manteuffel, C. Schneider, K. Schönwald | The Polarized Three-Loop Anomalous Dimensions from On-shell Massive Operator Matrix Elements | arXiv:1908.03779 |
| J. Blümlein, P. Marquard, N. Rana, C. Schneider | The Heavy Fermion Contributions to the Massive Three Loop Form Factors | arXiv:1908.00357 |
| J. Ablinger, J. Blümlein, P. Marquard, N. Rana, C. Schneider | Three loop heavy quark form factors and their asymptotic behavior | arXiv:1906.05829 |
| J. Ablinger, J. Blümlein, P. Marquard, N. Rana, C. Schneider | Three loop QCD corrections to heavy quark form factors | arXiv:1905.03728 |
| J. Blümlein | Large scale analytic calculations in quantum field theories | arXiv:1905.02148 |
| J. Blümlein, C. Raab, K. Schönwald | The Polarized Two-Loop Massive Pure Singlet Wilson Coefficient for Deep-Inelastic Scattering | arXiv:1904.08911 |
| J. Blümlein, A. De Freitas, C.G. Raab, K. Schönwald | The unpolarized two-loop massive pure singlet Wilson coefficients for deep-inelastic scattering | arXiv:1903.06155 |
| J. Blümlein, A. Maier, P. Marquard | Five-Loop Static Contribution to the Gravitational Interaction Potential of Two Point Masses | arXiv:1902.11180 |
| J. Blümlein, A. De Freitas, C.G. Raab, K. Schönwald | The O(alpha^2) Initial State QED Corrections to e^+ e^- Annihilation to a Neutral Vector Boson Revisited | arXiv:1901.08018 |