| 1 | = Section 3 = |
| 2 | |
| 3 | PAGE 6 |
| 4 | |
| 5 | Section 3.1.1 |
| 6 | |
| 7 | Par 1 |
| 8 | |
| 9 | L3/4 : ”while leptonic decays can be indirectly studied from the decay |
| 10 | products when processing the DELPHES output” is very vague a sentence, |
| 11 | with no real meaning. Suggestion is to drop it. |
| 12 | The rest of the section is extremely verbose, and could be replaced by |
| 13 | one sentence stating that electron and muon energy/momentum is smeared |
| 14 | with resolutions parameterized as a function of pT and eta (and mention |
| 15 | that these parameterizations can be changed by the user?). The convoluted |
| 16 | explanations about what a typical collider experiment is actually doing is of |
| 17 | no interest for the reader, as DELPHES does not do the same anyway. This |
| 18 | text could be replaced by a figure showing the resolutions used to reproduce |
| 19 | the CMS and ATLAS performance for electrons and muons, as well as a |
| 20 | comparison with the actual detector resolutions. |
| 21 | |
| 22 | Section 3.1.2 |
| 23 | |
| 24 | Last line : ”Neutral pions are automatically classified as photons”. As al- |
| 25 | ready mentioned, neutral pions are not long-lived particles in any generator. |
| 26 | Instead they decay promptly to two photons, which obviously are classified |
| 27 | as photons. The authors might want to drop the comments about neutral |
| 28 | pions. |
| 29 | |
| 30 | PAGE 7 |
| 31 | |
| 32 | Section 3.2.2 |
| 33 | |
| 34 | L2/3: ”as these might indicate the production of heavy unstable particles” |
| 35 | carries little meaning is the context of this article (and probably in a wider |
| 36 | context too) without additional explanation. Suggestion is to drop it. |
| 37 | |
| 38 | PAGE 8 |
| 39 | |
| 40 | Section 3.2.2 |
| 41 | |
| 42 | Par 1: |
| 43 | |
| 44 | L1/2 : It is not useful to indicate what is done in real experiments. Instead, |
| 45 | it is important to describe what is done in DELPHES. |
| 46 | 1.8.2 Section 3.1.3 |
| 47 | |
| 48 | As a general comment, the isolation definition chosen here is very much |
| 49 | hadron collider biassed. One would not do the same in e+e- collisions. This |
| 50 | comment supports the initial request that the abstract includes a sentence |
| 51 | stating that DELPHES is aimed at simulating hadron collider experiments |
| 52 | (so far). |
| 53 | |
| 54 | PAGE 9 |
| 55 | |
| 56 | ”Charged pile-up subtraction” |
| 57 | |
| 58 | There are several problems in this paragraph. |
| 59 | |
| 60 | * It is not stated if this paragraph is specific to PF or not. If it’s not, the |
| 61 | procedure to remove charged particles from the event in which purely |
| 62 | calorimetric jets are reconstructed needs to be spelt out clearly. |
| 63 | |
| 64 | * Even if the paragraph is PF specific, it is not clear what ”subtracted |
| 65 | from the event: means. For example, are the pile-up charged hadrons |
| 66 | removed from the event before computing the missing transverse en- |
| 67 | ergy ? To the best of my knowledge, it is not what is done in LHC |
| 68 | experiments. |
| 69 | |
| 70 | * The criterion ”a distance |z| > Zvtx” is obscure. What if the hard |
| 71 | interaction is produced with |z| > Zvtx ? and what is the definition |
| 72 | of this ”distance” ? If is is the distance between the vertex of a PU |
| 73 | interaction with respect to the vertex of the hard interaction, the use of |
| 74 | ”z” instead of ”z” (with the proper definition in the text) is in order. |
| 75 | |
| 76 | ”Residual pile-up subtraction” |
| 77 | |
| 78 | * It is not clear how ”rho” is obtained in DELPHES |
| 79 | |
| 80 | * ”mainly the jet energies and the isolation” : is ”rho” used for anything |
| 81 | else ? if yes, it should be stated. If not, ”mainly” should be removed. |
| 82 | |
| 83 | PAGE 10 |
| 84 | |
| 85 | Par 2: |
| 86 | |
| 87 | L4: It would be useful to mention one of the advantages of the PF recon- |
| 88 | struction in the context of PU mitigation, namely the fact that the calorime- |
| 89 | ter energy deposits associated to PU charged hadrons are ”automatically” |
| 90 | removed. In DELPHES, however, this does not happen when a charged |
| 91 | hadron and a neutral deposit fall in the same calorimeter tower, because the |
| 92 | charged hadron is then ignored by DELPHES. |
| 93 | |