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NLO EW ZH production at FCCee #25

Merged
merged 41 commits into from
Dec 9, 2024
Merged

NLO EW ZH production at FCCee #25

merged 41 commits into from
Dec 9, 2024

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arossia94
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@arossia94 arossia94 commented Oct 23, 2024

Implementation of the NLO EW results for ZH production at FCCee from this paper.
This has to be done for all the ZH FCCee datasets, including the ones for each Higgs decay channel.

  • Implementation of Op sensitivity
  • Implementation of all other NLO corrections in Higgs inclusive datasets.
  • Extend the former to the CEPC files.
  • Implementation of all other NLO corrections for each Higgs decay channel.
  • Extend the former to the CEPC files.

Optional task:

  • Implement files with only LO predictions so one can remove NLO EW easily without removing all the NLO QCD datasets.

@arossia94 arossia94 marked this pull request as ready for review October 25, 2024 15:03
Check and correct file addresses before running the Mathematica and Jupyter notebooks. It uses files from the smefit-ewpo repository.
…ns under both LO and NLO options.

The names of these files include "_loew_" to distinguish them from the ones that include NLO EW
corrections under the NLO option. This allows us to study the impact of these NLO EW corrections
without removing NLO QCD corrections from other datasets.
@jacoterh
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Adding @TommasoArmadillo to this PR as he already started working on implementing ZH at NLO independently (with Fabio and Eleni)

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Hi Alejo, thanks for this!
I just skimmed it and I have a bunch of comments. There are also come conflicts for one of the OOS file, not exactly clear why they are modified at all in this PR, maybe it's a remnant of some previous state of main when you branched out.

theory/FCCee_zh_gg_loew_240GeV.json Outdated Show resolved Hide resolved
Corrected sign of `cpd` inside the Mathematica notebook used to generate the files.
@TommasoArmadillo
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Hello! I went through the PR, in particular the file ZH_NLO_EW_2409.11466.nb and I have some comments. I already discussed a bit with Alejo, but I report here for keeping record.

  • In the paper from Dawson et al. they report the Wilson coefficient for the operator $$O_{\varphi\Box}=(\varphi^\dagger \varphi)\Box (\varphi^\dagger \varphi)$$ in the Warsaw basis. However, in smefit, we use the operator $$O_{\varphi d}=\partial^\mu(\varphi^\dagger \varphi)\partial_\mu(\varphi^\dagger \varphi)$$. The two operators are related by integration by parts identities $$\partial_\mu((\varphi^\dagger \varphi)\partial^\mu(\varphi^\dagger \varphi))=O_{\varphi\Box}+O_{\varphi d}$$. So there should be a minus sign between $$C_{\varphi \Box}$$ and $$C_{\varphi d}$$;
  • In the paper they introduce the coefficient $$C_2^{4f}=C_{ll}[1,2,2,1]+C_{ll}[2,1,1,2]$$ in eq. A.3. In smefit we use the operator $$O_{ll}=(\bar{\ell_1} \gamma_\mu \ell_2)(\bar{\ell_2} \gamma_\mu \ell_1)$$. So I think there should be a factor 2 between the two. Alejo had a doubt that the factor 2 might already be taken into account in smefit. He proposed to check it by computing the interference of some process that includes $$C_{ll}$$ at LO and is included in SMEFiT (ee>mumu) with SMEFTsim in MG5 turning on only one of them and relating it with the results already in SMEFiT. I am currently working on it.

jacoterh and others added 5 commits November 5, 2024 13:03
Printed files for NLO EW ZH with corrected sign for cpd. The new files are kept in the working temporary folder nlo_ew_implementation until the check on cll is finished.
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I have news concerning the $$C_{ll}$$ coefficient.

I generated $$e^+ e^- \to \mu^+ \mu^-$$ at LO with SMEFTsim in MG5. I considered only the contribution due to $$C_{ll}[1,2,2,1]$$. The number I obtain agrees with the one for $$C_{ll}$$ that is already present in SMEFit in FCCee_mumu_240GeV.json.

This means that we need to take into account an extra factor 2 for the WC $$C_{2}^{4f}$$ in ZH_NLO_EW_2409.11466.nb.

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jacoterh commented Nov 6, 2024

That's great news! Have you also checked whether the other flavour combination actually gives the same contribution as we expect?

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jacoterh commented Nov 6, 2024

@arossia94 are we sure
image
implements correctly the definition of ctZ from here?
image
I would expect cu3W to also enter the linear combination to get our ctZ.

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@arossia94 are we sure image implements correctly the definition of ctZ from here? image I would expect cu3W to also enter the linear combination to get our ctZ.

I'm quite sure it does, I did the computation by hand at the level of operators and WCs in the Lagrangian. I don't have my handwritten notes at hand now, I can share them next week. The transformation is quite non intuitive.

Cards for ee>ZH with Higgs decayed printed after correcting the sign of Opd and the factor of 2 in Oll. Cards with Higgs decayed should be moved onto the theory folder and results for inclusive in Higgs copied onto the corresponding files.
Files inside the `nlo_ew_implementation` and `theory` folders have been updated with the following fixes:
-Deleted the `NLO` category from the predictions and replaced it with the `NLO_EW` one.
-In `NLO_EW` one, corrected the sign of the `cpd` contribution from the inclusive ZH production
-In `NLO_EW`, corrected the missing factor of 2 in the ZH contribution to the dependence on `cpd`.
-The `best_sm` is set to be equal to the SM in `NLO_EW`.
-All this done for FCCee/CEPC, ZH production with and without Higgs decay
@jacoterh
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@arossia94 are we sure image implements correctly the definition of ctZ from here? image I would expect cu3W to also enter the linear combination to get our ctZ.

I'm quite sure it does, I did the computation by hand at the level of operators and WCs in the Lagrangian. I don't have my handwritten notes at hand now, I can share them next week. The transformation is quite non intuitive.

I already managed to convince myself you did everything correctly! It's the same transformation that confuses me sometimes with O3pq and OpqMi. One needs to check at the Lagrangian level what it means to turn on ctW = 1 in SMEFiT. This turns on OtW and ObW weighted by cW/sW.

arossia94 and others added 4 commits November 21, 2024 07:18
Zh datasets for FCCee in commondata are updated to the NLO EW standard. The data_central value corresponds to the NLO EW SM prediction and the statistical uncertainty was updated accordingly.
All CEPC Zh files in commondata updated to NLO EW standard. Central value is the NLO EW SM prediction and statistical uncertainty was rescaled accordingly.
And copying the HL-LHC dataset onto `commondata` for consistency.
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Given PR#99 on smefit_release we can remove all files in nlo_ew_implementation and put them all in theory instead, can't we?

@arossia94 arossia94 linked an issue Nov 28, 2024 that may be closed by this pull request
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There are three files in the interface_oos that I do not understand why they are there, but for the rest it looks good to me.

external_chi2/optimal_observables/interface_oos_161.py Outdated Show resolved Hide resolved
@arossia94 arossia94 merged commit a463b4a into main Dec 9, 2024
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@arossia94 arossia94 deleted the NLO-EW-ZH branch December 9, 2024 10:08
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diHiggs projection
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