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cms:exo-16-025 [04/11/2016 06:30] arcidiac |
cms:exo-16-025 [04/11/2016 07:08] arcidiac |
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- | Dear authors, ARC, congratulations on this well-written, clear paper. Below we have some questions/comments to your attention. | ||
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- | Best wishes for a speedy publication. | ||
- | The Torino group | ||
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- | === da roberta === | ||
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- | I concur with the above mentioned congratulations to the authors and ARC. Very well written and well exposed paper. | ||
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- | Type B comments | ||
- | ---------------- | ||
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- | 1. 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. | ||
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- | Type A comments | ||
- | ----------------- | ||
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- | L 58 nonisolated particles --> non-isolated particles | ||
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- | The silicon tracker measures charged particles within the pseudorapidity range |η| < 2.5. For nonisolated particles of 1 < pT < 10 GeV and |η| < 1.4, the track resolutions are typically 1.5% in pT and 25–90 (45–150) μm in the transverse (longitudinal) impact parameter [20]. | ||
- | --> why it is given in this way? | ||
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- | L62 At larger values of |η|, the size of the towers increases and the matching ECAL | ||
- | arrays contain fewer crystals. ? | ||
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- | L 87 corrected for zero-suppression effects what does that mean exactly? | ||
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- | L104 candidates in a cone ∆R --> in a cone of radius | ||
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- | L112 The 8 TeV analysis employs the Cambridge–Aachen (CA) clustering algorithm [25], | ||
- | while the 13 TeV analysis uses the anti-kt algorithm [26], | ||
- | --> what are the main reasons/pros or cons for one or another choice? | ||
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- | L118 The requirement on jet η allows to further suppress the background from γ+jets | ||
- | and QCD multijet events --> not 100% clear, further suppress wrt what? | ||
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- | L132 pruned jets are split into two subjets by reversing the final iteration in the jet clustering algorithm | ||
- | -- subjects? sub-jets? | ||
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- | L158 a resonance somewhat broader --> can one avoid "somewhat"? | ||
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- | L164-169 one would like to know maybe what you would expect to gain in 2015 with the different (more uptodate ?) choice of MC generators. | ||
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- | L183 the background rejection due to b tagging exceeds a factor of 100 --> the background rejection in this category exceeds .. | ||
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- | L186 into the two SRs. --> in this sentence it is probably better to say it without acronyms? into the two search regions. | ||
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- | L138 narrow and wide resonance --> narrow and broad resonance | ||
- | please keep using "broad" | ||
- | L241 remove wide, not really needed, it is clear that you are discussing this case | ||
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- | L249 Most of the uncertainties affect the overall signal efficiency, and only the b tagging efficiency uncertainty can result in signal category migration. --> is one worst than the other? is one going to affect more the result on the search? | ||
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- | L270 The background-only fit is consistent with both 8 and 13 TeV data. --> what does that mean exactly? | ||
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- | Table 2: caption needs to be re-adjusted! description of columns looks wrong. | ||
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- | L280 The expected and observed limits for spin-0 resonances --> please specify (again) on what are those limits intended to be (on the production cross) - same comment is valid for the Table 3 caption. expected means? | ||
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- | L290 This ratio increases --> which ratio? | ||
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- | L306 in in -> remove one in | ||
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- | Figure 5 showing relative contribution of --> showing the relative contribution | ||