Abstract
We calculate the two-mass three-loop contributions to the unpolarized and polarized massive operator matrix elements $tilde{A}_{Qg}^{(3)}$ and $Delta tilde{A}_{Qg}^{(3)}$ 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 textcolor{blue}{$O(T_F^2)$} and textcolor{blue}{$O(T_F^3)$} terms contributing to the operator matrix elements. The present result completes the calculation of all unpolarized and polarized massive three-loop operator matrix elements.
arXiv:2510.09403 [hep-ph]
arXiv:2510.09403 [hep-ph]
| Original language | English |
|---|---|
| Article number | 111 |
| Pages (from-to) | 1-52 |
| Number of pages | 52 |
| Journal | The Journal of High Energy Physics |
| Volume | 2026 |
| Issue number | 1 |
| DOIs | |
| Publication status | Published - Jan 2026 |
Fields of science
- 101013 Mathematical logic
- 101 Mathematics
- 101012 Combinatorics
- 101005 Computer algebra
- 101009 Geometry
- 101001 Algebra
- 101020 Technical mathematics
JKU Focus areas
- Digital Transformation