Showing 1 - 19 results of 19 for search 'K. Schönwald', query time: 0.05s Refine Results
  1. 1
    The inverse Mellin transform via analytic continuation

    The inverse Mellin transform via analytic continuation by A. Behring, J. Blümlein, K. Schönwald

    Published 2023-06-01
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  2. 2
    The polarized two-loop massive pure singlet Wilson coefficient for deep-inelastic scattering

    The polarized two-loop massive pure singlet Wilson coefficient for deep-inelastic scattering by J. Blümlein, C. Raab, K. Schönwald

    Published 2019-11-01
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  3. 3
    The two-loop massless off-shell QCD operator matrix elements to finite terms

    The two-loop massless off-shell QCD operator matrix elements to finite terms by J. Blümlein, P. Marquard, C. Schneider, K. Schönwald

    Published 2022-07-01
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  4. 4
    The massless three-loop Wilson coefficients for the deep-inelastic structure functions F 2 , F L , xF 3 and g 1

    The massless three-loop Wilson coefficients for the deep-inelastic structure functions F 2 , F L , xF 3 and g 1 by J. Blümlein, P. Marquard, C. Schneider, K. Schönwald

    Published 2022-11-01
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  5. 5
    The variable flavor number scheme at next-to-leading order

    The variable flavor number scheme at next-to-leading order by J. Blümlein, A. De Freitas, C. Schneider, K. Schönwald

    Published 2018-07-01
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  6. 6
    Subleading logarithmic QED initial state corrections to e+e−→γ⁎/Z0⁎ to O(α6L5)

    Subleading logarithmic QED initial state corrections to e+e−→γ⁎/Z0⁎ to O(α6L5) by J. Ablinger, J. Blümlein, A. De Freitas, K. Schönwald

    Published 2020-06-01
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  7. 7
    The O(α2) initial state QED corrections to e+e− annihilation to a neutral vector boson revisited

    The O(α2) initial state QED corrections to e+e− annihilation to a neutral vector boson revisited by J. Blümlein, A. De Freitas, C.G. Raab, K. Schönwald

    Published 2019-04-01
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  8. 8
    The O(α2) initial state QED corrections to e+e−→γ⁎/Z0⁎

    The O(α2) initial state QED corrections to e+e−→γ⁎/Z0⁎ by J. Blümlein, A. De Freitas, C.G. Raab, K. Schönwald

    Published 2020-07-01
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  9. 9
    The unpolarized two-loop massive pure singlet Wilson coefficients for deep-inelastic scattering

    The unpolarized two-loop massive pure singlet Wilson coefficients for deep-inelastic scattering by J. Blümlein, A. De Freitas, C.G. Raab, K. Schönwald

    Published 2019-08-01
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  10. 10
    The two-mass contribution to the three-loop pure singlet operator matrix element

    The two-mass contribution to the three-loop pure singlet operator matrix element by J. Ablinger, J. Blümlein, A. De Freitas, C. Schneider, K. Schönwald

    Published 2018-02-01
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  11. 11
    O(αs2) polarized heavy flavor corrections to deep-inelastic scattering at Q2 ≫ m2

    O(αs2) polarized heavy flavor corrections to deep-inelastic scattering at Q2 ≫ m2 by I. Bierenbaum, J. Blümlein, A. De Freitas, A. Goedicke, S. Klein, K. Schönwald

    Published 2023-03-01
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  12. 12
    The three-loop polarized pure singlet operator matrix element with two different masses

    The three-loop polarized pure singlet operator matrix element with two different masses by J. Ablinger, J. Blümlein, A. De Freitas, M. Saragnese, C. Schneider, K. Schönwald

    Published 2020-03-01
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  13. 13
    The two-mass contribution to the three-loop gluonic operator matrix element Agg,Q(3)

    The two-mass contribution to the three-loop gluonic operator matrix element Agg,Q(3) by J. Ablinger, J. Blümlein, A. De Freitas, A. Goedicke, C. Schneider, K. Schönwald

    Published 2018-07-01
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  14. 14
    The polarized transition matrix element Agq(N) of the variable flavor number scheme at O(αs3)

    The polarized transition matrix element Agq(N) of the variable flavor number scheme at O(αs3) by A. Behring, J. Blümlein, A. De Freitas, A. von Manteuffel, K. Schönwald, C. Schneider

    Published 2021-03-01
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  15. 15
    The $$Q_{1,2}$$ Q 1 , 2 – $$Q_7$$ Q 7 interference contributions to $$b \rightarrow s \gamma $$ b → s γ at $${\mathcal O}(\alpha _{\mathrm s}^2)$$ O ( α s 2 ) for the physical value of $$m_c$$ m c

    The $$Q_{1,2}$$ Q 1 , 2 – $$Q_7$$ Q 7 interference contributions to $$b \rightarrow s \gamma $$ b → s γ at $${\mathcal O}(\alpha _{\mathrm s}^2)$$ O ( α s 2 ) for the physical valu... by M. Czaja, M. Czakon, T. Huber, M. Misiak, M. Niggetiedt, A. Rehman, K. Schönwald, M. Steinhauser

    Published 2023-12-01
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  16. 16
    The two-mass contribution to the three-loop polarized gluonic operator matrix element Agg,Q(3)

    The two-mass contribution to the three-loop polarized gluonic operator matrix element Agg,Q(3) by J. Ablinger, J. Blümlein, A. De Freitas, A. Goedicke, M. Saragnese, C. Schneider, K. Schönwald

    Published 2020-06-01
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  17. 17
    The first–order factorizable contributions to the three–loop massive operator matrix elements AQg(3) and ΔAQg(3)

    The first–order factorizable contributions to the three–loop massive operator matrix elements AQg(3) and ΔAQg(3) by J. Ablinger, A. Behring, J. Blümlein, A. De Freitas, A. von Manteuffel, C. Schneider, K. Schönwald

    Published 2024-02-01
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  18. 18
    The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements

    The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements by A. Behring, J. Blümlein, A. De Freitas, A. Goedicke, S. Klein, A. von Manteuffel, C. Schneider, K. Schönwald

    Published 2019-11-01
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  19. 19
    The unpolarized and polarized single-mass three-loop heavy flavor operator matrix elements A gg,Q and ∆A gg,Q

    The unpolarized and polarized single-mass three-loop heavy flavor operator matrix elements A gg,Q and ∆A gg,Q by J. Ablinger, A. Behring, J. Blümlein, A. De Freitas, A. Goedicke, A. von Manteuffel, C. Schneider, K. Schönwald

    Published 2022-12-01
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