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cms:sus-11-016 [03/10/2012 09:15]
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cms:sus-11-016 [03/10/2012 12:29] (versione attuale)
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 http://​cms.cern.ch/​cds/​SUS-11-016 http://​cms.cern.ch/​cds/​SUS-11-016
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 +Stefano A.
 +----------
 +
 +Type A:
 +
 +Abstract: ​
 +1. "up to 4.98 fb-1": we would suggest to write the actual range instead of "up to" (throughout the paper)
 +
 +2. "range of mass parameters"​ : which mass ?
 +
 +
 +L1-L6: the word "​particle"​ is repeated 3 times in two lines
 +
 +L5: "one theoretical model ..." This is coming out of the blue, we should at least say (in one sentence) why this particular one is used in most CMS analyses.
 +
 +L5 : "in most CMS analyses " -> In most of the analyses performed by the CMS collaboration (or similar rephrasing)
 +
 +L7 : principal -> principle (or at least, this seems to be the intended meaning) or remove the word and commas.
 +
 +L7/9 : repetition of the word "​particle"​
 +
 +L13-14 : "For each SimplM, values of  Axepsilon can be calculated to translate a number of signal events into a cross section " . This needs rephrasing, e.g. "can be calculated to measure a cross section given the number of observed signal candidates"​. But it is not clear at this point if it _can_  be calculated or if actually did it.
 +
 +L15/16: We would suggest: "an upper limit on the xs times the br ($[\sigma \times BF]_{UL}$)",​ then remove ($[\sigma \times BF]$) at the end of the sentence. The definition in symbols without the UL is not used in the rest of the paper if we are not mistaken. ​
 +
 +
 +L113 : "​denoted the " -> denoted as the
 +
  
 Nicolo` Nicolo`
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 L.198 (and Fig.1): L.198 (and Fig.1):
-While it is clear how efficiency*acceptance is extracted it is less clear why the figures on the right do not show the same pattern (e.g. isolines) of those on the left just with a different scale.  +While it is clear how efficiency*acceptance is extracted it is less clear why the figures on the right do not show the same pattern (e.g. isolines) of those on the left just with a different scale (e.g. % on the left, pb on the right)
-More specifically:​ the text mentions "the predicted background"​. Is the number of predicted background events the same for all the points in the (m(~g),​m(LSP)) plane and the difference in the isoline patterns between left and right plots arises only when including it in the CLs calculation?​ Or is the selection of the events different in different regions of the (m(~g),​m(LSP)) plane, so the number of selected events changes as well? +More specifically:​ the text mentions "the predicted background"​. Is the number of predicted background events the same for all the points in the (m(~g),​m(LSP)) plane and the difference in the isoline patterns between left and right plots arises only when including it in the CLs calculation? ​ 
 +Or is the change in the isolines pattern due to the fact the points with the same value efficiency*acceptance have different uncertainties on the efficiency*acceptance itself?  
 +Or, finally, ​is the selection of the events different in different regions of the (m(~g),​m(LSP)) plane, so the number of selected events changes as well? 
 +Whatever is the reason it is probably worthwhile to explain it in the text.
  
 L.214: remove "The limits are thus subject to statistical fluctuations" ​ (as everything...) L.214: remove "The limits are thus subject to statistical fluctuations" ​ (as everything...)
  
-Fig.1  ​In the top header of each plot: Why m(~q)>>​m(~g) and not the opposite? +Fig.1  caption "​chargino"​ -> "​neutralino"​
-caption "​chargino"​ -> "​neutralino"​+
  
 I have also two conceptual questions about these plots: I have also two conceptual questions about these plots:
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 2) The fine dashed lines diagonal seem to indicate a kinematic limit, e.g. m(LSP)<​m(~g),​ which is probably wrong for the topology analyzed as for the cascade ~g->​N_0^2->​N_0^1 is m(LSP)<​m(~g)-m(N_0^2) 2) The fine dashed lines diagonal seem to indicate a kinematic limit, e.g. m(LSP)<​m(~g),​ which is probably wrong for the topology analyzed as for the cascade ~g->​N_0^2->​N_0^1 is m(LSP)<​m(~g)-m(N_0^2)
-Also the fact that there is a constant offset between the dashed line and the edge of the "​color"​ region is not intuitive ​as I would expect a constant offset ​for a constant ​value of m(N_0^2), specifically 200 GeV.  +Also the fact that there is a constant offset between the dashed line and the edge of the "​color"​ region is not intuitive ​Why do you expect a constant offset? Does this correspond to a constant m(N_0^2), specifically 200 GeV?