SciPost Submission Page
QED at NNLO with McMule
by P. Banerjee, T. Engel, A. Signer, Y. Ulrich
This Submission thread is now published as
Submission summary
| Authors (as registered SciPost users): | Tim Engel · Adrian Signer · Yannick Ulrich |
| Submission information | |
|---|---|
| Preprint Link: | https://arxiv.org/abs/2007.01654v1 (pdf) |
| Date accepted: | 2020-08-20 |
| Date submitted: | 2020-07-06 02:00 |
| Submitted by: | Signer, Adrian |
| Submitted to: | SciPost Physics |
| Ontological classification | |
|---|---|
| Academic field: | Physics |
| Specialties: |
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| Approaches: | Theoretical, Phenomenological |
Abstract
McMule is a framework for fully differential higher-order QED calculations of scattering and decay processes involving leptons. It keeps finite lepton masses, which regularises collinear singularities. Soft singularities are treated with dimensional regularisation and using FKS$^\ell$ subtraction. We describe the implementation of the framework in Fortran 95, list the processes that are currently implemented, and give instructions on how to run the code. In addition, we present new phenomenological results for muon-electron scattering and lepton-proton scattering, including the dominant NNLO corrections. While the applications presented focus on MUonE, MUSE, and P2, the code can be used for a large number of planned and running experiments.
Published as SciPost Phys. 9, 027 (2020)
Reports on this Submission
Anonymous Report 2 on 2020-7-31 (Invited Report)
- Cite as: Anonymous, Report on arXiv:2007.01654v1, delivered 2020-07-31, doi: 10.21468/SciPost.Report.1871
Report
This paper describes the new program McMule. It is a framework written in Fortran that performs high-order calculations in QED for scattering and decay processes involving leptons.
At the moment, the program implements muon decay, muon-electron scattering and proton-electron scattering. Depending on the process, it considers NLO, NNLO or dominant NNLO corrections, i.e., NNLO corrections only to the single photon exchange. The authors plan further developments of the existing code either by by including new processes or by improving the prediction for the existing ones.
Even if several of this processes were already computed in the past to various levels of precision, McMule represents the first comprehensive framework that includes all of them and that is fully differential, thus allowing studies with arbitrary cuts. The code is in a stable stage and it has been cross-checked with other independent calculations for all processes that are implemented.
The computational techniques used in McMule are briefly described in section 2. Sections 3 and 4 discuss the code's structure and how to run it. Sections 5 and 6 presents phenomenological results for muon-electron scattering, connected to the MUonE experiment, and proton-electron scattering, for P2 and MUSE experiments.
I think the work presented in this paper will have a large impact in particle physics in the following years and it will be strategic for future analysis in low-energy experiments like MUonE, P2, MUSE but also MEG and Mu3e. Therefore I am happy to recommend the manuscript for publication.
I want to make two minor suggestions to the authors.
1) In section 6.1 it is mentioned that their code substantially disagrees with the NNLO corrections in ref. [84]. I think they should better quantify it. Is it 1% or 100%? The reader might also wonder which experimental analyses employed the findings in [84] and therefore could be affected by them.
2) In section 2 it is briefly mentioned that if two-loop amplitudes are available only for massless external particles, "massification" can be used. However it is not explained what is is meant by that.
Anonymous Report 1 on 2020-7-24 (Invited Report)
- Cite as: Anonymous, Report on arXiv:2007.01654v1, delivered 2020-07-24, doi: 10.21468/SciPost.Report.1856
Strengths
1- The paper contains very important results needed for the interpretation of forthcoming high-precision experiments with lepton scattering
2- The paper is well written
Weaknesses
None
Report
The paper should be published.
Requested changes
1- In section 2, equations 2, 5, 6 the authors use the symbol \cal{M} and call this 'the matrix element', but for the calculation of cross sections one would need squares of matrix elements.
2- Some plots (e.g. in Fig.4, 6) or tables (e.g. Tab.2) do not exhibit units, and in Figs.8, 10, 12, the units are wrong. This should be corrected.
Author: Adrian Signer on 2020-09-08 [id 944]
(in reply to Report 1 on 2020-07-24)
1) We have made our statement more precise just after Eq.(2.c) 2) We have added the units where there was an ambiguity, e.g. in Figure 6. We refrain from repeating the units of (e.g. the energy) on the y-axis if they have been given in the x-axis, e.g. in Figure 10 we do not write the full d\sigma/d|t| / (\mu b/MeV^2) . We think this is a reasonable and unambiguous short cut to state our units.
Author: Adrian Signer on 2020-09-08 [id 945]
(in reply to Report 2 on 2020-07-31)1) We have added a remark in Section 6.1 to make it clear that the disagreement is not small (i.e. more 100% than 1% ). Since the total cross section is affected, so are all distributions. 2) We have added a sentence in the first paragraph of Section 2 to say what "massification" is. The details of this procedure are described in the references given there.