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cms:exo-10-026 [27/02/2011 00:38]
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cms:exo-10-026 [15/03/2011 16:11] (versione attuale)
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 The paper is well organized, short and well focused. ​ We have two general comments: ​ The paper is well organized, short and well focused. ​ We have two general comments: ​
  
-1) However we do not agree with the separation of this paper from  the similar public PAS EXO-10-19. ​ The two analyses combined would show a much more organic effort. We suggest the inclusion in this paper of the results of EXO-10-19. ​+1)  ​We ​do not agree with the separation of this paper from  the similar public PAS EXO-10-19 ​( for example Tab 1 is the same in both papers).  The two analyses combined would show a much more organic effort. We suggest the inclusion in this paper of the results of EXO-10-19. ​
  
 2) Quite often the explanations are so dense that they are difficult to follow. 2) Quite often the explanations are so dense that they are difficult to follow.
- 
  
  
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 l.15: (EM) is the "​diphoton"​ the only "​diboson"​ final state allowed? if other final states like ZZ are possible, you should specify why they are suppressed, similarly to what is written for fermionic final states. ​ l.15: (EM) is the "​diphoton"​ the only "​diboson"​ final state allowed? if other final states like ZZ are possible, you should specify why they are suppressed, similarly to what is written for fermionic final states. ​
  
-l.15-25 (NC): The reader might wonder why D0 has done the 2-jet and dielectron analyses and we did not. We should explain the status/​reason for not having done it.+l.15-25 (NC+NP): The reader might wonder why D0 has done the 2-jet and dielectron analyses and we did not. We should explain the status/​reason for not having done it.
  
 l.25: (EM) all the "​scales"​ in the paper are in GeV/c^2 apart this where they are in TeV l.25: (EM) all the "​scales"​ in the paper are in GeV/c^2 apart this where they are in TeV
- 
- 
  
 eqs.1, 2, 3: (EM) are these equations really needed? Naively one can interpret them as a toolbox to convert limits on M_S between the different models, but this seems to be not the case if one looks at the values in Table 3, e.g. M_S(GRW) != (pi/​2)^(1/​4) M_S(Hewett) ​   ​ eqs.1, 2, 3: (EM) are these equations really needed? Naively one can interpret them as a toolbox to convert limits on M_S between the different models, but this seems to be not the case if one looks at the values in Table 3, e.g. M_S(GRW) != (pi/​2)^(1/​4) M_S(Hewett) ​   ​
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 l.48-49: (EM) why the threshold of the double-photon trigger is larger than that of the single-photon trigger? ​ If the single-photon is prescaled, you should mention it. l.48-49: (EM) why the threshold of the double-photon trigger is larger than that of the single-photon trigger? ​ If the single-photon is prescaled, you should mention it.
  
-l.53 (NC): The eta-cut value of 1.4442 is peculiar. What is our resolution in eta? DO we really know eta to the 4th decimal point?+l.53 (NC): The eta-cut value of 1.4442 is peculiar. What is our resolution in eta? DO we really know eta to the 4th decimal point?  
 + 
 +(NP):Since this value is due to the exclusion of the 2 outermost ECAL barrel rings, has to be mentioned?  
 + 
 +l.60-73 (NC):  this list is hard to follow. Why not separate the points (i),​(ii),​(iii) using also new lines
  
-l.60-73 ​(NC):  this list is hard to followWhy not separate ​the points (i),​(ii),​(iii) using also new lines?+(NP): ideally one would like to read that isolation criteria are applied both to charghed tracks and to e.m. and hadronic energy depositions within defined DeltaR acceptances around ​the photon directions
  
 l.65-66: (EM) specify if the "​rectangular strip" is centered around the direction of the photon candidate l.65-66: (EM) specify if the "​rectangular strip" is centered around the direction of the photon candidate
  
-l.74-82: (EM) difficult to follow what it was done. Also about the optimal choice for |eta|, we found the tone of the explanation too confidential. Perhaps just say that you choose the barrel/​endcap boundary and this was driving the M(gamma-gamma)>​500 GeV choice. Furthermore in the rest of the paper it is not clear how the intermediate region is used.+l.74-82: (EM+ NP) difficult to follow what it was done. Also about the optimal choice for |eta|, we found the tone of the explanation too confidential. Perhaps just say that you choose the barrel/​endcap boundary and this was driving the M(gamma-gamma)>​500 GeV choice. Furthermore in the rest of the paper it is not clear how the intermediate region is used.
  
 l.77-79 (NC): "We alternate between..."​ it does not sound very good. Just quote the result. l.77-79 (NC): "We alternate between..."​ it does not sound very good. Just quote the result.
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 l.83-84: (NC+EM) This explanation is really too short, and you end with a  scale factor compatible with one. why is it needed? Just quote that you have checked with Z->ee the MC prediction l.83-84: (NC+EM) This explanation is really too short, and you end with a  scale factor compatible with one. why is it needed? Just quote that you have checked with Z->ee the MC prediction
  
 +l.83-84: (NP) Comparing to EGM-10-006 the efficiency was computed on the data Zee sample and than corrected by the same factor
 +for the difference e/gamma.
  
-l.85-87 (NC):  The K-factor choice needs a longer explanation. It's difficult is a reader has to go to a reference to figure-out this choice. Flat in pt? +l.89-97 (NC):  The K-factor choice needs a longer explanation. It's difficult is a reader has to go to a reference to figure-out this choice. Flat in pt? 
  
 l.103: (EM) remove ","​ after sample l.103: (EM) remove ","​ after sample
  
 l.105: (EM) "​orthogonal to each other" -> "​independent"​ l.105: (EM) "​orthogonal to each other" -> "​independent"​
 +
 +l.118: (NP) why the error on K factor is 0.3 here and 0.1 in l.96?
  
 l.125, 137, 173: (EM) GeV->​GeV/​c^2 l.125, 137, 173: (EM) GeV->​GeV/​c^2
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 Fig. 3 caption: n =>n_ED (to be consistent). Fig. 3 caption: n =>n_ED (to be consistent).
 +
 +l.152: panel
  
 l.154: (EM) 1/M_S^4 (n=2,​95%)=0.078 TeV^-4 -> 1/​M_S^4=0.078 TeV^-4 95% CL with n_ED=2 l.154: (EM) 1/M_S^4 (n=2,​95%)=0.078 TeV^-4 -> 1/​M_S^4=0.078 TeV^-4 95% CL with n_ED=2
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 EM: Ernesto EM: Ernesto
 NC: Nicolo NC: Nicolo
 +NP: Nadia
 +
 +=== Answers to the comments to draft1 ===
 +
 +https://​hypernews.cern.ch/​HyperNews/​CMS/​get/​EXO-10-026/​37.html ​
 +
 +=== Draft 2 ===
 +[[http://​cdsweb.cern.ch/​record/​1335448|Entry on CERN Document Server for Draft 2]]