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Changes between Version 1 and Version 2 of Private/RefereeComments/Section_6


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Timestamp:
Aug 26, 2013, 9:01:13 AM (11 years ago)
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cp3-support
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  • Private/RefereeComments/Section_6

    v1 v2  
    11= Section 6 =
    22
     3PAGE 12:
     4
     5Section 6.1
     6Last line: What does ”alternatively” mean ? If one choice is for electrons
     7and the other for muons, the authors should state it clearly.
     8
     9Footnote: this statement deserves a complete section, with the list of
     10parameters used in the default CMS and ATLAS configurations, as well
     11as possible explanations as to why this parameter choice was made, and a
     12comparison with the actual CMS and ATLAS resolutions and granularities.
     13
     14PAGE 13
     15
     16Figure 3
     17
     18 * It is not clear what the grey bands are in this plot. Shouldn’t they be
     19removed? In CMS, they are supposed to cover differences between the
     20simulation and the data in CMS, not the difference between Delphes
     21and CMS. This comment is valid for all plots
     22Strangely enough, the ATLAS fred band width is way smaller than that
     23for CMS. Does it represent the same thing ?
     24 * For all plots, it is important to have the statistical uncertainty bars
     25indicated, or to state that they are covered by the size of the markers.
     26In the latter case, an explanation is needed for the apparent scatter
     27of the DELPHES points, and to compare this scatter with the input
     28resolution function.
     29 * For all plots, label, legends, etc... are way too small to be readable.
     30
     31Figure 4
     32
     33Looking at Ref. [20], and in particular its slide 33, my impression is that
     34the DELPHES resolution is a factor 2 optimistic with respect to the CMS
     35resolution. It seems that DELPHES parametrized the Gaussian width of the
     36core of the CMS resolution, rather than the effective 68% width.
     37
     38PAGE 14
     39
     40Figure 5
     41
     42On the CMS side, it would be nice to have an explanation for the following
     43effects (already alluded to above):
     44 * why does the calo jet resolution curve saturates at low jet pT ?
     45 * why does the PF jet resolution curve of Delphes departs from CMS at high pT? (it’s probably because the tracker pT resolution is used to
     46determine the PF track pT) And at low pT ? Actually, the DELPHES jet pT resolution is almost independent with pT: it goes from 10 to 7%
     47when varying the pt from 30 to 500 GeV/c, while the actual CMS PF varies from 14% to 5%.
     48 * why does the PF curve show a discontinuity between the 1st and 2nd points ?
     49
     50Once the effects are understood, it would be important to fix the imple-
     51mentation in DELPHES. These differences are important for data analysis,
     52and may to DELPHES user draw wrong conclusions from his DELPHES
     53studies (of particular importance if DELPHES is used to define the upgrade
     54strategy of the expensive LHC detectors).
     55
     56Section 6.3
     57
     58Par 2:
     59
     60It is not clear if the CMS study is made with of without pile-up. As pile-up
     61and its particle-flow mitigation are an important adds-on to DELPHES 3.0,
     62it would be nice to have an illustration of their performance here.
     63
     64PAGE 16
     65
     66Par 1:
     67
     68L3: The anti-kT algorithm has no ”cone” - and ”a cone R = 0.5” has
     69no meaning even for a cone algorithm. (Note: the same mistake occurs in
     70Section 7.2)
     71
     72L9/11: The slight difference of efficiency is a large difference (20%), which
     73might the DELPHES user draw incorrect conclusions from the abilities of
     74his/her analysis. The explanation given here should be checked, and the cul-
     75prit (jet energy correction or b tagging efficiency should be fixed in DELPHES.
     76
     77Par 2:
     78
     79Bullet 1: ”any parton from the top quark decay” ! ”any parton from the
     80decay of either of top quarks”. I find the definition of unmatched rather un-
     81natural. If the three jets from the ”hadronically-decaying top” were matched,
     82I fail to understand why the event is classified as unmatched, even if the other
     83b for the other top is unmatched.
     84
     85Par 3:
     86
     87L5: Why are the distributions not normalized to the number of events ? Is
     88it because the number of permutations/event is vastly different in DELPHES
     89and in CMS ? If it is the case, shouldn’t DELPHES be fixed ?
     90
     91L9/10: ”Pile-up, not considered in the present study, can degrade the jet
     92energy resolution.” : A strong emphasis is put on the ability of Delphes 3.0
     93to simulate pile up, and to simulate its mitigation procedures based on the
     94PF reconstruction. Since Delphes is fast, I would assume that it would take
     95no time to redo this study with pile-up. It is disappointing for the reader not
     96to see this validation in the paper. It actually casts doubts on the DELPHES
     97ability to accurately simulate pile-up and its mitigation, which is surely not
     98what the authors aim at.
     99
     100PAGE 17
     101
     102Figure 7
     103
     104The bottom inserts of all plots are difficult to understand. The label ”rel.
     105diff.” makes the reader guess that they show the relative difference (i.e.,
     106the ratio - 1) of the two distributions, but a quick look at the distributions
     107leads the reader to doubt about it. For exampe, the right plot shows a 20%
     108difference between the two distributions around the maximum, which is not
     109visible in the ”rel. diff.” plot. Maybe the wrong scale was chosen for the
     110bottom inserts ?
     111
     112PAGE 18
     113
     114Par 4: The reader is again disappointed to see that, in the search for VBF-
     115produced Higgs boson with pile-up, for which it is said that pile-up has a
     116pretty large and negative impact, the authors decided to use calorimeter jets
     117instead of particle-flow reconstruction, aimed exactly at mitigating pile-up
     118effects. Again, it casts doubts on the ability of DELPHES to simulate pile-up
     119in particle reconstruction, and to simulate its mitigation with particle-flow
     120reconstruction. The paper has therefore the effect opposite to what the
     121authors are aiming at.
     122
     123Criterion 2.
     124
     125The pT cut used to count light jets between j1 and j2 ought to be given.
     126Are these four cuts used in the CMS analysis which the authors are using for
     127comparison ?
     128
     129PAGE 20
     130
     131Par 2:
     132
     133L4: ”accurate productions in high pile-up scenarios should solely rely on
     134full simulation tools” is very strong, and probably incorrect statement, and
     135should probably be removed (or seriously rephrased).
     136
     137First, it casts again large doubts on the pertaining DELPHES ability to
     138simulate pile up interactions.
     139
     140Second, the fact that, maybe, DELPHES cannot deal with high PU en-
     141vironment does not mean that other fast simulation tools cannot do. For
     142example, it seems the CMS fast simulation deals pretty well with the high
     143pile-up produced by LHC in 2012.
     144