Response to comments for AN-20-100
General comments:
Many plots, descriptions of systematic uncertainties, etc. appear to only be shown for 2016 and 2017, please add the 2018 equivalents as well, since that is what this iteration of the analysis adds.
This also leads to the question : are the 2016/2017 plots corresponding to the re-analysis (with UL dataset) or are they the old plots from the previous iteration of the analysis?
- For distribution, limits plots, 2018 dataset is added and UL dataset is used in all years.
Some section/table/figure references appeared to be broken. Some examples are L61, L108, L110, L213-214, L225-226, L261, and L283.
Certain parts of the text also appear to be broken (eg. L210-211, L281), please correct.
Some symbols appeared to be missing, maybe due to failed macros. Examples include L107 ("of is"), Tables 7-10, L210-211 (presumably should all be Z'?), L260 "()", Table 15 (for QCD, PDF, and MC stat. Maybe these should be qq->Z?), Table 16 ("80 << 100
GeV"), and L307.
Please be sure to label figures as "CMS Work in Progress" as described in
https://twiki.cern.ch/twiki/bin/viewauth/CMS/PhysicsApprovals#Thesis_endorsement
- Label added for distribution and limits plots.
Detailed comments:
Abstract: "These are the first dedicated limits on the Lμ − Lτ model at the LHC." - what about EXO-18-008? Actually, are the upper limits listed here for the full Run 2, or are they from EXO-18-008?
Section 2: Please add more information about the samples used, e.g. which global tags, which lumi JSON file is used, etc.
Table 1: It looks like the period H datasets are listed along with period F (or should the "H" have said "F" there?). Please double check the datasets being used for 2016 based on
https://twiki.cern.ch/twiki/bin/view/CMS/PdmVDatasetsUL2016, e.g.
Run2016B ver1 and
Run2016B ver2 should both be used.
Section 2.1.2: For your tag-and-probe method, what selection is used? You mention that events with four muons are used, but are any other requirements applied, e.g. Z mass constraints, muon pT, etc.? It sounds as though the same probe muon can added to the denominator of your efficiency multiple times (i.e. once for each tag muon). If so, this may be a source of double-counting that you don't actually want. Please clarify the text.
- I didn't reproduced this part.
Please add description for 2018 as well, and and figures as in Figure 2. Are the plots in Fig 2 corresponding to the updated
UltraLegacy datasets?
- I didn't reproduced this part.
L81-82: "for 2016, the last 6% of the dataset was not used for the trigger efficiency measurement" - please motivate why in the text
- I didn't reproduced this part.
L86: "ggH" - Is this ggH->ZZ*->4l, or some other process?
L89: "applies the efficiency" - applies the efficiency itself, or efficiency correction factors?
- Apply correction factors.
L97: Please motivate these uncertainty values and how they are determined. Are they fixed across years?
- I didn't reproduced the uncertainty part.
Figure 2 and elsewhere: please double check the integrated luminosities you quote against those from the Lumi POG (
https://twiki.cern.ch/twiki/bin/view/CMS/TWikiLUM#TabLum)
- Figure 2 is directly from AN-17-321
Section 2.2: Please add the to the Table 10-12 the remaining path of the MC sets as part of captions as done in tables 7-9. Are all the samples used produced using UL reconstruction corresponding to the datasets used?
- Path added. Background samples are using UL.
Section 3.1.2 Muon Isolation: Is there a reason that you use a PF isolation cut value of 0.35 rather than one of the values corresponding to the WPs from
https://twiki.cern.ch/twiki/bin/view/CMS/SWGuideMuonSelection#Particle_Flow_isolation? Do you derive data-to-MC scale factors for the muon isolation cut that you use?
- Just used the same isolation cut as AN-17-321. I didn't derive the scale factors.
L163: Which Loose ID do you refer to here? The "loose muons" from L123, or the muon POG loose WP? Please clarify.
L210-211 : some of the text seems to be missing, please add the missing text in the brackets to complete the description.
Table 13: What does "total events" correspond to? i.e. which luminosity does it correspond to, does it only correspond to a particular background process, etc.? Table 13: Please describe the mass window size of 2% in the analysis strategy section; currently it doesn't appear until Section 6.2, so it isn't quite obvious from this table currently.
- This table is from AN-17-321. Deleted from the update version.
L213-214: "KNNLO" - to be sure, is this a ratio from NLO to NNLO, or LO to NNLO? It should be the former, since you already apply KNLO. Please specify in the text.
- It is NLO to NNLO. Added explaination text.
Figure 3: Text in captions (of subplots as well as for the plot) is missing, please update after adding missing text.
Figure4 : 2018 plot is missing. Is the bottom plot cross section, or cross section x branching ratio? The axis titles and captions are in contradiction, please clarify in the text captions / figure axes, Figure 4: 2018 seems to be missing? The bottom plot is labeled as 35.9 fb^-1, but presumably applies equally well to all 13
TeV datasets. For the top two plots: How do you do this interpolation between 40 and 50
GeV, where the Z1 vs. Z2 choice changes? It might be safer to generate masses near the threshold rather than to extrapolate here. Figure 4 "Left: central line is shown in black while the red and blue color shows interpolation ..." - is this referring to the red and green lines in the top plots, or something else? Is the interpolation in the top two plots linear, or based on some fit function? The systematic variations described in this caption are not apparent.
- Plots of three years are added.
Section 5 Systematics: Please describe the uncertainties relevant for 2018 as well.
- I didn't reproduced the uncertainty part.
L232-233: "7% if the lowest pT muons if less than 7
GeV" - how is this used? It sounds like a flat 4.9% uncertainty is used, which is smaller than this value?
- I didn't reproduced the uncertainty part.
L236: Please provide more information, as well as the impact of these uncertainties. Or are L240-246 also intended to describe how you assess this uncertainty?
- I didn't reproduced the uncertainty part.
L238 "We neglect the
PileUp uncertainty of 2%" - are you sure it is negligible? It's of a similar size as your luminosity uncertainty, and many of the uncertainties are fairly small.
- I didn't reproduced the uncertainty part.
L252: "root mean square" - The difference is likely small, but I believe the current
PDF4LHC recommendation (Section 6.3.1 of
https://arxiv.org/pdf/2203.05506.pdf
) is to take the central 68% interval over the variations.
- I didn't reproduced the uncertainty part.
Figure 6: It is hard to tell if there are differences between the nominal and the variations; it might be easier if the three fits are overlaid (e.g. in different colors) on the same canvas.
- I didn't reproduced the uncertainty part.
Table 15: "Interference effect" - please describe this in the text as well.
- Added a interference section.
L264-267: Although the impact is small, it would be good to treat the correlations properly.
- I didn't reproduced the uncertainty part.
L281-283: It doesn't sound like a single "bin", given the windows used. Please clarify.
Certain parts of the text seem to be missing, please fix.
Table 16: Which dataset is this? It would be good to see for each of 2016, 2017, 2018, and combined. Table 16: "uncertainty" - no uncertainties appear to be shown?
- Full RunII dataset. And uncertainty is shown.
Figure 9: Seeing 2018 would also be interesting here, since that is what this analysis is adding on top of the previous result (at least plots of the background estimate and predicted signal).
- A new set of plots are added, including all three years.
L322-325: As mentioned in the meeting on March 16th, it would be useful to overlay the limits from the 2016+2017 analysis with those from full Run 2, to better see the gains that 2018 brings.
- A comparison on Figure 30 and Table 17.
Figure 14: Please explain the large drops in the observed limits and 95% bands in the right-hand plot for many mass hypotheses.
- That was using full CL method and is removed from update version.
Figure 21: Does this include the 2018 dataset? It would be interesting to see the expected limits in the right-hand plot for full Run 2 as well.
- This one is only 2016-2017 and removed.
Editorial comments:
L52: "during 2016 and 2017" - 2016--2018
L53: "(2017) 59.7 fb−1 and (2018)" - typo, should be "(2017), and 59.7 fb−1 (2018)"
Table 3: Missing dashes between run numbers
L100: "Production of via" - missing a word between "of" and "via"
L107: "leptophilic coupling to muons (gμ = 0.1)" - since you discuss alternative coupling values in the results section, it might be useful to already mention here that alternative couplings will be discussed later, so that the reader is aware that they will be considered.
- Added a sentence to mention it.
L123: Please add units for the pT, dxy, dz
L146: "subtraced" - typo
L209: subscripts 1 and 2 are in the line but the text before the subscript (Z ?) does not appear.
L230: "taste" -> "years"?
L235: This line may be a mistake?
L309: "FEWZ and " - missing something after the "and"?
--
KunShi - 2022-04-19
Comments from slides:
Discussed during the talk: Limit plots say cross section, it should be
cross section X branching ratio. Please fix in the AN.
From your talk: Slide 14: is there a point at 45
GeV? If so, please
note it in the figure caption, since it is hard to see in the AN. In the
long term, can go for more granular mass samples near the transition
area.
- Yes, there is a point at 45 GeV, it is completely covered by the fitted green line.
Discussed during the talk: limits comparison: please provide an
overlay plot and table for expected limits. Both for full Run-2 vs
previous limits and as a cross check for re-analysis of 2016/17 vs
previous limits.
- Added cross check plots. Provided the comparison side by side. Since I don't have the datacard from previous analysis, cannot plot the overlay plots.
AN Section 5: There are still descriptions missing for 2018, for e.g.
(but not limited to) L305,L315, Table14, 15. Please add more description
of 2018, even if it is just that the same values are used as e.g. 2017.
- Added some description of 2018.
AN Figures 12-14: What drives the phi distribution for the ZZ
background events here? (i.e. why isn't it uniform?)
- Plots changed. Now are the real phi distribution.
Long term comments. (will be addressed in longer term)
General: For the full result, please study the uncertainties assigned
and the trigger efficiency for 2018 as well as UL. Discussed during the talk: Slide 15: Please check if the interference
has any dependence on the mass.
L95 : Was any check/study performed for 2018 also?
Figure 5: This plot and the corresponding text are a bit confusing.
The SM Higgs width is 4
MeV, so what is the difference between the
top-left and top-right plots? Is it that the width varies with off-shell
mass? The cross sections between the two plots differ by four orders of
magnitude, is that correct?
L189: In general the MET filters can be used even for analyses that do
not use MET explicitly since the function of the MET filters is to
remove mis-reconstructed events.
Figure 6: Ratios might be useful here to better understand the
difference between the two distributions. Showing this on a linear scale
may also be useful.
L279-280: "4.9% for 2016 dataset and 4.6% for 2017 dataset" - what
about 2018?
Figure 7: Is the impact of the interference at all mass-dependent as
well?
Figure 10: Which dataset is this? We suggested this previously, but
overlays would be useful.
Figure 11: Hard to be sure looking by eye, but it seems like there are
~10 data events for pT > 140
GeV with a prediction of only 1 or 2
background events? Is this understood?
Fig 19: At the peak, the difference looks larger for 2018 compared to
2017/2016 -> is this understood?
Figures 21 and 22: Did these change at all with respect to the
published result for 2016+2017?
Table 17: Difference at 40
GeV is ~30%, but much smaller (~10-15%) for
the other masses. Is there a reason for this?
Fig 30: Including both sets of lines in one figure (overlaying past and
current limits) would be helpful to estimate the overall improvement
Editorial comments
Abstract: "These are the update limits" -> These improve upon the
limits / These are the updated limits
L154: "substracted" - typo
L187: Npv -> ndof
L211: May be useful here to mention that the Ref. [28] is for H->4L
search (as one would naively have guessed that it was the AN for the
2016+2017 Z->4mu search)
Figure 3: Labeling the axes (or at least mentioning in the caption)
here would be useful, so we know which is m(Z1) and which is m(Z2).
- Added description in caption
L264-265: "Because the windows have to be narrow at low masses" - this
seems to be the first mention of the window sizes in the AN? It would be
good to mention this sooner.
- Mention the window at beginning of the AN
Table 14: Please label these uncertainties as percentages (assuming
that is the case). Do you have the same table for 2018?
-Table 15 caption: Please add description of what the Table contents
placed in brackets refer to (presumably 2017)
- Label added for 14. I don't have the same table for 2018. Description added for 15.
L290-291: Please add extra information into the text to clarify this.
Since this is the first mention of a dimuon selection, the reader may
initially be confused since you've selected events with four muons
everywhere else!
L304-305: What about for 2018 samples?
Figure 20: Very fine bins shown on the right-hand plot at low mass;
hard to see them very well. Could imagine an additional version of this
plot with a log-x scale? Unsure if it would help...
Fig 19 caption: 20162017 -> 2016, 2017
L473: "CMS-AN-16-2442" - should be "AN-16-442" (including the
hyperlink here and for other references might be nice)
--
KunShi - 2022-05-08