Johannes Bluemlein
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Johannes Bluemlein has a total of 202 co-authors. Here are the top co-authors by number of shared publications:
- Carsten Schneider
Johannes Kepler University Linz
37 shared publications - Sergey Alekhin
Universität Hamburg
20 shared publications - Abilio De Freitas
Johannes Kepler University Linz
19 shared publications - Sven-Olaf Moch
Hamburg University
19 shared publications - Kay Schönwald
Theoretical Physics Department, CERN
14 shared publications - Peter Marquard
Deutsches Elektronen-Synchrotron DESY
13 shared publications
Latest Publications
- Open Access
- 21 August 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (4) , 045017
μ -extension of iterated integrals and nested sums in quantum field theory
The analytic integration of single-scale Feynman integrals emerging in perturbative calculations in quantum field theories can be performed within special classes of functions, which appear as consecutive generalizations of the polylogarithm in form of Kummer-Poincaré iterative integrals over special alphabets and extensions thereof. These are the polylogarithms, Nielsen integrals, iterated integrals over linear denominator terms, cyclotomic letters, letters induced by quadratic forms, and square-root valued letters. These integrals are solutions of first-order factorizing differential equations. They are related to specific nested sums via the Mellin transform and their expansions around x = 0 . We construct the μ -extensions of these iterated integrals and the associated nested sums. We present closed form solutions or provide algorithms in the case of more involved cases to derive the respective μ -extensions and study the algebras of the μ -extended function spaces. Except for the case of square-root valued alphabets, the μ -extension maps into the same function space polynomially in μ . This is also the case for the associated nested sums. For square-root valued alphabets or sums containing central binomials, the μ -extension leads to higher transcendental functions. In all other cases the μ - extension preserves the Hopf algebra structure implied by the (quasi)shuffle product, by supplementing μ to the ground field.
- 21 August 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (4) , 045017
Open Accessμ -extension of iterated integrals and nested sums in quantum field theory
The analytic integration of single-scale Feynman integrals emerging in perturbative calculations in quantum field theories can be performed within special classes of functions, which appear as consecutive generalizations of the polylogarithm in form of Kummer-Poincaré iterative integrals over special alphabets and extensions thereof. These are the polylogarithms, Nielsen integrals, iterated integrals over linear denominator terms, cyclotomic letters, letters induced by quadratic forms, and square-root valued letters. These integrals are solutions of first-order factorizing differential equations. They are related to specific nested sums via the Mellin transform and their expansions around x = 0 . We construct the μ -extensions of these iterated integrals and the associated nested sums. We present closed form solutions or provide algorithms in the case of more involved cases to derive the respective μ -extensions and study the algebras of the μ -extended function spaces. Except for the case of square-root valued alphabets, the μ -extension maps into the same function space polynomially in μ . This is also the case for the associated nested sums. For square-root valued alphabets or sums containing central binomials, the μ -extension leads to higher transcendental functions. In all other cases the μ - extension preserves the Hopf algebra structure implied by the (quasi)shuffle product, by supplementing μ to the ground field.
- Open Access
- 11 May 2026
- Published by Elsevier in Physics Letters B
- Vol. 878
The three-loop single-mass heavy-flavor corrections to the structure functions F2(x, Q2) and g1(x, Q2)
- 11 May 2026
- Published by Elsevier in Physics Letters B
- Vol. 878
Open AccessThe three-loop single-mass heavy-flavor corrections to the structure functions F2(x, Q2) and g1(x, Q2)
- Open Access
- 1 April 2026
- Published by Elsevier in Physics Letters B
- Vol. 876
The heavy quark-antiquark asymmetry in the variable flavor number scheme
- 1 April 2026
- Published by Elsevier in Physics Letters B
- Vol. 876
Open AccessThe heavy quark-antiquark asymmetry in the variable flavor number scheme
- Open Access
- 26 March 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (3) , 248
The single-mass variable flavor number scheme at three-loop order
A bstract: The matching relations in the unpolarized and polarized variable flavor number scheme at three-loop order are presented in the single-mass case. They describe the process of massive quarks becoming light at large virtualities Q 2 . In this framework, heavy-quark parton distributions can be defined. Numerical results are presented on the matching relations in the case of the single-mass variable flavor number scheme for the light parton, charm and bottom quark distributions. These relations are process independent. In the polarized case we generally work in the Larin scheme. To two-loop order we present the polarized massive OMEs also in the $$ \overline{\textrm{MS}} $$ scheme. Fast numerical codes for the single-mass massive operator matrix elements are provided.- 26 March 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (3) , 248
Open AccessThe single-mass variable flavor number scheme at three-loop order
A bstract: The matching relations in the unpolarized and polarized variable flavor number scheme at three-loop order are presented in the single-mass case. They describe the process of massive quarks becoming light at large virtualities Q 2 . In this framework, heavy-quark parton distributions can be defined. Numerical results are presented on the matching relations in the case of the single-mass variable flavor number scheme for the light parton, charm and bottom quark distributions. These relations are process independent. In the polarized case we generally work in the Larin scheme. To two-loop order we present the polarized massive OMEs also in the $$ \overline{\textrm{MS}} $$ scheme. Fast numerical codes for the single-mass massive operator matrix elements are provided. - Open Access
The complete three-loop unpolarized and polarized massive operator matrix elements and asymptotic Wilson coefficients
We report on the three-loop unpolarized and polarized massive operator matrix elements, with single- and two-mass corrections, and the associated deep-inelastic massive Wilson coefficients in the region $Q^2 \gg m_Q^2$, the calculation of which has been completed recently. We also provide fast and precise numerical representations of the massless Wilson coefficients, splitting functions to tree-loop order, and target-mass corrections in $x$-space well suited for QCD-fitting codes.Open AccessThe complete three-loop unpolarized and polarized massive operator matrix elements and asymptotic Wilson coefficients
We report on the three-loop unpolarized and polarized massive operator matrix elements, with single- and two-mass corrections, and the associated deep-inelastic massive Wilson coefficients in the region $Q^2 \gg m_Q^2$, the calculation of which has been completed recently. We also provide fast and precise numerical representations of the massless Wilson coefficients, splitting functions to tree-loop order, and target-mass corrections in $x$-space well suited for QCD-fitting codes. - Open Access
- 4 February 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (2) , 49
Erratum: The three-loop polarized singlet anomalous dimensions from off-shell operator matrix elements
- 4 February 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (2) , 49
Open AccessErratum: The three-loop polarized singlet anomalous dimensions from off-shell operator matrix elements
- Open Access
- 16 January 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (1) , 111
The two-mass contributions to the three-loop massive operator matrix elements ${\widetilde{A}}_{Qg}^{(3)}$ and ${\Delta \widetilde{A}}_{Qg}^{(3)}$A bstract: We calculate the two-mass three-loop contributions to the unpolarized and polarized massive operator matrix elements $${\widetilde{A}}_{Qg}^{(3)}$$ and $${\Delta \widetilde{A}}_{Qg}^{(3)}$$ in x -space for a general mass ratio by using a semi-analytic approach. We also compute Mellin moments up to N = 2000(3000) by an independent method, to which we compare the results in x -space. In the polarized case, we work in the Larin scheme. We present numerical results. The two-mass contributions amount to about 50% of the full $$O({T}_{F}^{2})$$ and $$O({T}_{F}^{3})$$ terms contributing to the operator matrix elements. The present result completes the calculation of all unpolarized and polarized massive three-loop operator matrix elements.- 16 January 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (1) , 111
Open AccessThe two-mass contributions to the three-loop massive operator matrix elements ${\widetilde{A}}_{Qg}^{(3)}$ and ${\Delta \widetilde{A}}_{Qg}^{(3)}$A bstract: We calculate the two-mass three-loop contributions to the unpolarized and polarized massive operator matrix elements $${\widetilde{A}}_{Qg}^{(3)}$$ and $${\Delta \widetilde{A}}_{Qg}^{(3)}$$ in x -space for a general mass ratio by using a semi-analytic approach. We also compute Mellin moments up to N = 2000(3000) by an independent method, to which we compare the results in x -space. In the polarized case, we work in the Larin scheme. We present numerical results. The two-mass contributions amount to about 50% of the full $$O({T}_{F}^{2})$$ and $$O({T}_{F}^{3})$$ terms contributing to the operator matrix elements. The present result completes the calculation of all unpolarized and polarized massive three-loop operator matrix elements. - Open Access
- 17 September 2024
- Published by Sissa Medialab Srl
- Vol. 467, 047
The three-loop single-mass heavy flavor corrections to deep-inelastic scattering
We report on the status of the calculation of the massive Wilson coefficients and operator matrix elements for deep-inelastic scatterung to three-loop order. We discuss both the unpolarized and the polarized case, for which all the single-mass and nearly all two-mass contributions have been calculated. Numerical results on the structure function $F_2(x,Q^2)$ are presented. In the polarized case, we work in the Larin scheme and refer to parton distirbution functions in this scheme. Furthermore, results on the three-loop variable flavor number scheme are presented.- 17 September 2024
- Published by Sissa Medialab Srl
- Vol. 467, 047
Open AccessThe three-loop single-mass heavy flavor corrections to deep-inelastic scattering
We report on the status of the calculation of the massive Wilson coefficients and operator matrix elements for deep-inelastic scatterung to three-loop order. We discuss both the unpolarized and the polarized case, for which all the single-mass and nearly all two-mass contributions have been calculated. Numerical results on the structure function $F_2(x,Q^2)$ are presented. In the polarized case, we work in the Larin scheme and refer to parton distirbution functions in this scheme. Furthermore, results on the three-loop variable flavor number scheme are presented. - Open Access
- 17 September 2024
- Published by Sissa Medialab Srl
- Vol. 467, 031
Challenges for analytic calculations of the massive three-loop form factors
The calculation of massive three-loop QCD form factors using in particular the large moments method has been successfully applied to quarkonic contributions in [1]. We give a brief review of the different steps of the calculation and report on improvements of our methods that enabled us to push forward the calculations of the gluonic contributions to the form factors.
- 17 September 2024
- Published by Sissa Medialab Srl
- Vol. 467, 031
Open AccessChallenges for analytic calculations of the massive three-loop form factors
The calculation of massive three-loop QCD form factors using in particular the large moments method has been successfully applied to quarkonic contributions in [1]. We give a brief review of the different steps of the calculation and report on improvements of our methods that enabled us to push forward the calculations of the gluonic contributions to the form factors.
- 9 September 2024
- Published by World Scientific Pub Co Pte Ltd
- p. 37-56
Deep-inelastic Scattering: What do we Know?
- 9 September 2024
- Published by World Scientific Pub Co Pte Ltd
- p. 37-56
Deep-inelastic Scattering: What do we Know?