Differenze

Queste sono le differenze tra la revisione selezionata e la versione attuale della pagina.

Link a questa pagina di confronto

Prossima revisione
Revisione precedente
Ultima revisione Entrambe le parti successive la revisione
cms:exo-16-025 [25/10/2016 19:07]
solano creata
cms:exo-16-025 [04/11/2016 07:08]
arcidiac
Linea 1: Linea 1:
 http://​cms.cern.ch/​cds/​EXO-16-025 http://​cms.cern.ch/​cds/​EXO-16-025
 +
 +
 +===== da Stefano ====
 +
 +Dear authors, ARC, congratulations on this well-written,​ clear paper. Below we have some questions/​comments to your attention.
 +
 +Best wishes for a speedy publication.
 +The Torino group
 +
 +Type B comments
 +----------------
 +
 +1. The hardest part of the analysis, to the non-expert reader, seems to be the accurate identification of Z decays coming from merged jets.
 +To convince that the jet substructure identification works, a check on data would be appropriate,​ if possible. For example, one could measure the ratio  Z->jj / Z->​mu+mu- with merged jets, taking into account the appropriate efficiencies,​ and check that the ratio of branching ratios is consistent with expectations.
 +If something like this was done, it is worth mentioning, if not, please consider a similar test.
 +
 +2. In the discussion of systematic uncertainties,​ it is not clear how b-tagging, the uncertainty on efficiency of which is up to 60%, can increase the sensitivity by 50%. Can you explain ? Table 2 is very important, but not very clear in understanding the origin and effect of the uncertainties.
 +
 +
 +Type A comments
 +-----------------
 +
 +L4 Invert : "​Searches ... are of particular interest"​
 +
 +L 77 " 170 or 180 GeV" -> (180) GeV
 +
 +L 82 "​corrected for zero suppression effects"​ -> the ecal corrections are so many and complicated that I would not mention zero suppression,​ which to my knowledge is irrelevant at pt>150 GeV
 +
 +L 83-88 I understand this is boilerplate PF descriptive text, but why bother describing electron and muon reconstruction,​ which are not used in this analysis ?
 +
 +L111-112 if possible add a sentence to explain briefly why two different algorithms are chosen at 8 and 13 TeV
 +
 +L132-141 hard to understand
 +
 +L187 acceptance mentioned here for the first time, it is not defined and you don't say how it is calculated
 +
 +Throughout the paper  subjet -> sub-jet
 +
 +L207 - 208 I would omit saying that this fit function was chosen among others by using a Fisher test. It is a function that describes the background well, period.
 +
 +L248 source of the systematic uncertainty -> remove "​the"​
 +
 +L265 " only the effect .. on signal acceptance"​ -> what does it mean ? that the impact on yield and efficiency was not taken into account ?
 +
 +Table 2 : In this form, the table is quite confusing. It is not clear if the "​magnitude"​ column is the relative uncertainty on sigma x BR or on the quantity indicated by the last column. In the first case, I would remove the last column. For the label of the second column "​Magnitude"​ is best described as "​relative uncertainty"​ . In the caption: " the second column, the third column indicates " -> there is an offset in the column count, "​Source"​ is the first column, therefore "​Affected quantity"​ is the fourth, not the third, and "​Effect on yield" is the third, not the second.
 +
 +
 +
 +
 +