Kay Schönwald
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
Kay Schönwald has a total of 54 co-authors. Here are the top co-authors by number of shared publications:
- Matthias Steinhauser
Karlsruhe Institute of Technology (KIT)
32 shared publications - Matteo Fael
Università di Padova
21 shared publications - Carsten Schneider
Johannes Kepler University Linz
20 shared publications - Johannes Bluemlein
Deutsches Elektronen-Synchrotron DESY
14 shared publications J. Blümlein
Deutsches Elektronen-Synchrotron DESY, Platanenallee 6, 15738 Zeuthen, Germany
13 shared publicationsA. De Freitas
12 shared publications
Latest Publications
- Open Access
- 9 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10) , 114
The photon-energy spectrum in B → Xsγ to N3LO: light-fermion and large-Nc corrections
A bstract: We consider the photon-energy spectrum of the inclusive radiative decay B → X s γ , induced by the electromagnetic dipole operator O 7 , to next-to-next-to-next-to-leading order and calculate the complete corrections for light fermions, for the contributions with two closed massive fermion loops, and for the limit of large QCD colour factors N c in the remaining part. We discuss the integrated decay rate both without and with a cut on the photon energy. In addition to the on-shell renormalization of the bottom-quark mass, we also consider the kinetic mass and the MSR mass schemes. The latter two lead to an improved perturbative behaviour of the decay rate.
- 9 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10) , 114
Open AccessThe photon-energy spectrum in B → Xsγ to N3LO: light-fermion and large-Nc corrections
A bstract: We consider the photon-energy spectrum of the inclusive radiative decay B → X s γ , induced by the electromagnetic dipole operator O 7 , to next-to-next-to-next-to-leading order and calculate the complete corrections for light fermions, for the contributions with two closed massive fermion loops, and for the limit of large QCD colour factors N c in the remaining part. We discuss the integrated decay rate both without and with a cut on the photon energy. In addition to the on-shell renormalization of the bottom-quark mass, we also consider the kinetic mass and the MSR mass schemes. The latter two lead to an improved perturbative behaviour of the decay rate.
- Open Access
- 7 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10) , 76
Analytic next-to-leading order electroweak corrections to Higgs boson pair production at high energies
A bstract: We compute the complete top-quark-induced next-to-leading order electroweak corrections to the form factors entering gluon-induced Higgs boson pair production. We consider the top quark contribution in the limit where the Mandelstam variables are much larger than all other scales involved in the process and compute about a hundred expansion terms in analytic form. They are used to obtain precise numerical results even for fairly low values of the transverse momentum of the Higgs boson. We show that these electroweak corrections at high energies are of the order of −10%. We also discuss the leading logarithmic corrections of the analytic expressions.
- 7 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10) , 76
Open AccessAnalytic next-to-leading order electroweak corrections to Higgs boson pair production at high energies
A bstract: We compute the complete top-quark-induced next-to-leading order electroweak corrections to the form factors entering gluon-induced Higgs boson pair production. We consider the top quark contribution in the limit where the Mandelstam variables are much larger than all other scales involved in the process and compute about a hundred expansion terms in analytic form. They are used to obtain precise numerical results even for fairly low values of the transverse momentum of the Higgs boson. We show that these electroweak corrections at high energies are of the order of −10%. We also discuss the leading logarithmic corrections of the analytic expressions.
- Open Access
- 16 July 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (7) , 146
gg → ZH at NLO matched to parton showers with ggxy and POWHEG
A bstract: We implement the recently-calculated analytic expressions for the next-to-leading order QCD corrections to gg → ZH in ggxy. This provides a flexible framework for investigating partonic and hadronic cross sections for various top quark mass renormalization schemes. We augment the Z boson with leptonic decays, including spin correlations and off-shell effects, and furthermore provide an interface to POWHEG. This enables simulations with parton showers, performed using Pythia.
- 16 July 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (7) , 146
Open Accessgg → ZH at NLO matched to parton showers with ggxy and POWHEG
A bstract: We implement the recently-calculated analytic expressions for the next-to-leading order QCD corrections to gg → ZH in ggxy. This provides a flexible framework for investigating partonic and hadronic cross sections for various top quark mass renormalization schemes. We augment the Z boson with leptonic decays, including spin correlations and off-shell effects, and furthermore provide an interface to POWHEG. This enables simulations with parton showers, performed using Pythia.
- Open Access
- 1 July 2026
- Published by Elsevier in Nuclear Physics B
- Vol. 1029
Heavy-quark production in deep-inelastic scattering Mellin moments of structure functions
- 1 July 2026
- Published by Elsevier in Nuclear Physics B
- Vol. 1029
Open AccessHeavy-quark production in deep-inelastic scattering Mellin moments of structure functions
- 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
- 20 March 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (3) , 200
Two-loop QCD corrections to ZH and off-shell Z boson pair production in gluon fusion
A bstract: We compute two-loop corrections to the associated production of a Higgs boson with a Z boson and to off-shell Z boson pair production in the gluon fusion channel, mediated by a heavy quark. We perform deep expansions in the high-energy region and around the forward limit and show that their combination covers the whole phase space. Our results constitute the next-to-leading order virtual corrections to these processes. Their numerical evaluation is fast and the dependence on all parameters is maintained, thus a change of parameter values or renormalization scheme is straightforward. As a by-product of our calculation, we also obtain the two-loop heavy quark mediated virtual corrections to the processes of off-shell di-photon and photon- Z production.
- 20 March 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (3) , 200
Open AccessTwo-loop QCD corrections to ZH and off-shell Z boson pair production in gluon fusion
A bstract: We compute two-loop corrections to the associated production of a Higgs boson with a Z boson and to off-shell Z boson pair production in the gluon fusion channel, mediated by a heavy quark. We perform deep expansions in the high-energy region and around the forward limit and show that their combination covers the whole phase space. Our results constitute the next-to-leading order virtual corrections to these processes. Their numerical evaluation is fast and the dependence on all parameters is maintained, thus a change of parameter values or renormalization scheme is straightforward. As a by-product of our calculation, we also obtain the two-loop heavy quark mediated virtual corrections to the processes of off-shell di-photon and photon- Z production.
- Top Cited PapersOpen Access
- 11 March 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (3) , 109
Polarized neutral and charged current semi-inclusive deep-inelastic scattering at NNLO in QCD
A bstract: The semi-inclusive production of identified hadrons in deeply inelastic lepton scattering on polarized nucleons allows to probe the spin structure of the nucleon target in a more detailed level than through fully inclusive processes. We compute the NNLO QCD corrections to longitudinally polarized semi-inclusive deep inelastic processes mediated by electroweak neutral and charged currents. We present the first calculation of polarized electroweak structure functions in the Larin scheme up to NNLO. Additionally, we reformulate the finite scheme transformation to the $$ \overline{\textrm{MS}} $$ scheme in a quark flavour basis and identify issues in its assignment to partonic channels in previous calculations. Using our results we perform a detailed phenomenological study of polarized cross sections and of single and double spin asymmetries. We observe large electroweak effects, which need to be included in precision studies of polarized observables.- 11 March 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (3) , 109
Top Cited PapersOpen AccessPolarized neutral and charged current semi-inclusive deep-inelastic scattering at NNLO in QCD
A bstract: The semi-inclusive production of identified hadrons in deeply inelastic lepton scattering on polarized nucleons allows to probe the spin structure of the nucleon target in a more detailed level than through fully inclusive processes. We compute the NNLO QCD corrections to longitudinally polarized semi-inclusive deep inelastic processes mediated by electroweak neutral and charged currents. We present the first calculation of polarized electroweak structure functions in the Larin scheme up to NNLO. Additionally, we reformulate the finite scheme transformation to the $$ \overline{\textrm{MS}} $$ scheme in a quark flavour basis and identify issues in its assignment to partonic channels in previous calculations. Using our results we perform a detailed phenomenological study of polarized cross sections and of single and double spin asymmetries. We observe large electroweak effects, which need to be included in precision studies of polarized observables. - Open Access
- 18 February 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (2) , 191
Three-loop corrections to gg → ZH in the large top quark mass limit
A bstract: We compute three-loop virtual corrections to the associated production of a Higgs boson with a Z boson in the large- m t limit. We describe in detail the application of the asymptotic expansion and provide, for all form factors, analytic results for the first three terms in the 1/ m t expansion. We also provide numerical routines implemented in the C++ library ggxy.
- 18 February 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (2) , 191
Open AccessThree-loop corrections to gg → ZH in the large top quark mass limit
A bstract: We compute three-loop virtual corrections to the associated production of a Higgs boson with a Z boson in the large- m t limit. We describe in detail the application of the asymptotic expansion and provide, for all form factors, analytic results for the first three terms in the 1/ m t expansion. We also provide numerical routines implemented in the C++ library ggxy.