CMS_Z0J_13TEV#2360
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I think there's something wrong with the kinematics.
This might be a good opportunity to start using m_ll instead of the square...
RE data Vs theory something is wrong with the first bin (this is theory / data), it is systematically 30% off (probably some normalization or I did wrong a cut in my theory predictions).
The second bin and third bins seem ok.
Third and fourth a bit worse, I guess the statistics are all around the place but so is the data:
ratio = array([0.63142557, 0.69191467, 0.72222455, 0.72407745, 0.76986966,
0.82255564, 1.04158693, 1.03487063, 1.01877841, 1.01176393,
1.01778132, 1.00585585, 1.00522577, 0.99522485, 0.99550279,
1.00101172, 1.00696618, 1.01148373, 1.02241088, 1.0466769 ,
1.06189633, 1.07604775, 1.06241513, 1.1156114 , 1.03361906,
0.98315902, 0.97514231, 0.97673345, 0.93802319, 1.00462591,
0.98311333, 0.97416855, 0.88055417, 1.07630434, 1.00228661,
0.8514168 ])
And the plots for the 2nd, 3rd and 5th bins (disregard the value of the mass which is wrong and filled just to get different plots)
…cts. Value of the cut to be confirmed
…cts. Value of the cut to be confirmed
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scarlehoff
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I'm a bit worried about this dataset still because the agreement of the second bin is quite good (which is also special since it is the one that contains the Z mass).
But, here's the problem, I'm not normalising by the bin width, and according to the hepdata info, it is normalized. So I'd like to have a second look.
fwiw, the differences I see (the sames as I put above) are clearly not a factor of the bin width either.
| - uncertainties.yaml | ||
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| theory: | ||
| conversion_factor: 1000.0 |
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| conversion_factor: 1000.0 | |
| conversion_factor: 0.001 |
Data is in pb and theory in fb
| description: "Z boson mass squared" | ||
| label: '$m^2_{\ell \ell}$' | ||
| units: "GeV^2" |
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| description: "Z boson mass squared" | |
| label: '$m^2_{\ell \ell}$' | |
| units: "GeV^2" | |
| description: "invariant mass of the dilepton system" | |
| label: '$m_{\ell \ell}$' | |
| units: "GeV" |
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…ted metadata information. ATLAS: implemented the correct electron-muon data set
…tils for specialised theory covmat prescriptions
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This PR has become very messy, as it incorporates changes well beyond those in the title. This PR is going to be split in three sub-PRs:
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@scarlehoff Concerning the second point above, as you may remember, we discovered that the commondata implementation was bugged because only a fraction of the pT bins were implemented and the uncertainty was one order of magnitude too large. So we really need a brand new data set implementation (this is not a variant, this is not a new observable of the existing data set, this is really a dataset implementation version 2, the bugged version 1 having been used in the pheno paper). In this case, I have to confess that I don't remember what the workflow is. Is it sufficient to erase the previous implementation and have a new one (with version: 2 in the metadata) or should I create a new folder called, say |
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Version 2 in the metadata, comment: fix to bug in version 1. If you want to keep the bug as a variant you can do that. |
Sorry @scarlehoff : are you sure that I can keep the variant? The variant will also differ for the kinematics (the number of pT bins has changed). |
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Ah, no, in that case no. And then also fktables will differ. I would just replsce it. The pheno paper version lives in the tags of the repo. |
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Very good. That's what I wanted to hear. |



This PR incorporates the commondata implementation for the data set in the title.