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[Rivet] DISLepton Class fails to find outgoing leptonDavid Grellscheid david.grellscheid at durham.ac.ukWed Nov 15 11:44:00 GMT 2017
Andrii, can you please provide a test plot some time, showing the old and new behaviour of the projection before/after your fix in some exemplary analysis? I'm trying to assemble a set of interface stability tests (also for the XYZFinders), and this would be a good addition. Thanks, David On 15/11/2017 11:38, David Grellscheid wrote: > Do I understand right that the answer to the "correct" lepton to pick > becomes analysis-specific, and a global projection is not suited for > everyone. > > If the experimental analysis folds in some correction for the fact that > you may not have identified the "real" DIS lepton experimentally, then > going through the event tree in Rivet is (grudgingly ;-) ) acceptable. > > If the analysis relies on a final-state definition of which lepton to > choose, then Rivet should use the same final-state definition, and would > not need to look at event trees. > > See you, > > David > > > On 14/11/2017 18:32, Andrii Verbytskyi wrote: >> Hi Andy, >> >> >> 1) the code for electron finding works for me fine. >> Maybe because I use HEPMC_TREE_LIKE=1 for Sherpa. Maybe for other >> reasons. That is just an observation. I suggest Marian will use it and >> skip events with no lepton/broken lepton. Another option is to ignore >> state=3 particles in the finder. >> >> 2) I'm sure there are cases where your arguments are valid, but >> as of 2017, (simple NC) DIS is well defined in PDG. >> http://pdg.lbl.gov/2017/reviews/rpp2016-rev-qcd.pdf >> Not the case you describe. Of course that might be different next year, >> but I see no reasons for that and do not know anything about theoretical >> advances that can change it. >> >> 2a) Yes, final state definition is a good thing. That is why I find the >> fact that Sherpa puts final state particles into hadronisation blob >> problematic. But that is an implementation, not definition. >> >> Best regards, >> Andrii >> >> >> On Tue, 2017-11-14 at 18:01 +0000, Andy Buckley wrote: >>> Hi Andrii, >>> >>> I'm not sure what you mean by your point 1)...? >>> >>> On (2), I'm sure you're aware that the evoution of experimental >>> well-definedness has been gently evolving. There are also areas like >>> precision EW physics where definitions long held to be solid are being >>> challenged by theoretical advances. Also, HepMC and associated >>> standards are the operative definition of well-definedness: if those >>> standards are currently incompatible with a theoretically well-defined >>> process, then we should revisit the standards. "The lepton momentum >>> that interacts with a W/Z" is the sort of definition that has caused >>> problems, however, hence the ongoing shift towards more final-state >>> oriented fiducial definitions. >>> >>> I had no idea that the distinction between this definition and the >>> former one was so strong... I thought we were talking about more like >>> a few percent. Obviously we need to find a balance. >>> >>> Andy >>> >>> >>> On 14 November 2017 at 17:53, Andrii Verbytskyi >>> <andrii.verbytskyi at desy.de> wrote: >>>> Hi Andy, >>>> >>>> I had a long day, so in short: >>>> 1) works for me. With Sherpa as well. >>>> 2) DIS is well defined since many years, in many experiments and MC >>>> programs. Regardless of Rivet, HepMC, you and me. Sad but true. >>>> 3) Last time "some accuracy" was 50% or so (I honestly do not remember). >>>> Not a good idea. For sure there will be a bunch of students that will >>>> not be aware (or will forget) that "some accuracy" is missing. >>>> >>>> Andrii >>>> >>>> >>>> >>>> On Tue, 2017-11-14 at 17:32 +0000, Andy Buckley wrote: >>>>> Unfortunately that DIS definition doesn't correspond to something >>>>> well-defined in HepMC. There is no standard for hard-process >>>>> interaction representation. >>>>> >>>>> It would be good to know if this works with the Sherpa tree-like mode, >>>>> but generally we want to avoid such sensitivities. I am more inclined >>>>> to sacrifice some accuracy >>>> >>>> >>>>> for robustness... and an observable >>>>> definition that cannot be reproduced is a fundamentally problematic >>>>> thing. >>>> >>>> >>>> >>>> >>>> >>>>> Andy >>>>> >>>>> >>>>> On 14 November 2017 at 17:05, Andrii Verbytskyi >>>>> <andrii.verbytskyi at desy.de> wrote: >>>>>> Hi Marian, Andy, >>>>>> >>>>>> 0) The event contains loops. It is better to generate events with Sherpa >>>>>> with HEPMC_TREE_LIKE=1 or so. See docs. Have you used it? >>>>>> >>>>>> >>>>>> 1) >>>>>> On Tue, 2017-11-14 at 16:43 +0000, Andy Buckley wrote: >>>>>>> Hi Andrii, >>>>>>> >>>>>>> If the particle status codes are not 1 or 2, there is no guarantee >>>>>>> that HepMC vertices correspond to physical processes. They may just be >>>>>>> bookkeeping devices, e.g. to absorb parton shower recoils (or in this >>>>>>> case perhaps the QED radiation treatment) -- this wouldn't be a Sherpa >>>>>>> bug, but a valid use of the freedoms in the HepMC standard. So we >>>>>>> can't have projection code that assumes particular vertex structures, >>>>>>> because there will always be such edge-cases. >>>>>> >>>>>> In general you are right, but not for electron in DIS that is coming >>>>>> from hard process. The only thing one expects from it is e->e+gamma or >>>>>> e-> W nu ( not in Rivet anyway). But no hadronisation vertices. >>>>>> >>>>>> >>>>>> Sherpa mixes everything together, in one vertex. >>>>>> I haven't said that is a bug, but a *problem*. A problem for kinematics >>>>>> reconstruction. >>>>>> >>>>>> >>>>>> >>>>>> >>>>>>> Can you explain what the logic of your DIS lepton finder is? (The code >>>>>>> is not super-easy to follow.) Hopefully an understanding of the >>>>>>> intention will help us to find a safer definition. >>>>>> >>>>>> The logic comes from DIS definition: scattered lepton is the beam >>>>>> electron that went through e->e gamma/Z0 or e-> W nu vertices. >>>>>> >>>>>> >>>>>> Best regards, >>>>>> Andrii >>>>>> >>>>>>> Thanks, >>>>>>> Andy >>>>>>> >>>>>>> >>>>>>> On 14 November 2017 at 16:32, Andrii Verbytskyi >>>>>>> <andrii.verbytskyi at desy.de> wrote: >>>>>>>> Hi Marian, Andy, >>>>>>>> >>>>>>>> 0) I see no attachment. It is hard to guess which kind of process will >>>>>>>> produce electron+ some leptons from a single electron. >>>>>>>> If that is not SM process, the code was not designed to handle BSM. >>>>>>>> 1) Yes, it is complicated with Sherpa. It merges too many things >>>>>>>> together in one vertex. Just skip events with no electron/bad electron. >>>>>>>> 2) Everything "works" in "some way" with some conditions. >>>>>>>> 3) I cannot say without looking at the event that this is Sherpa >>>>>>>> problem, but I suspect it is, so it is not clear if any fix is needed. >>>>>>>> >>>>>>>> >>>>>>>> Best regards, >>>>>>>> Andrii >>>>>>>> >>>>>>>> >>>>>>>> On Tue, 2017-11-14 at 15:06 +0000, Andy Buckley wrote: >>>>>>>>> Hi Marian, >>>>>>>>> >>>>>>>>> Thanks for the report. I've CC'd Andrii, who provided that updated >>>>>>>>> DISLepton logic. Andrii, can you comment on how we can fix this >>>>>>>>> behaviour in a generator-independent way? >>>>>>>>> >>>>>>>>> Andy >>>>>>>>> >>>>>>>>> >>>>>>>>> On 10 November 2017 at 16:32, Marian Heil <marian.heil at durham.ac.uk> wrote: >>>>>>>>>> Dear rivet authors, >>>>>>>>>> >>>>>>>>>> I think I found a bug in the DISLepton class in rivet version 2.5.4: It does >>>>>>>>>> not find the outgoing lepton for a DIS scattering generated with Sherpa (the >>>>>>>>>> corresponding HepMC file is attached). >>>>>>>>>> >>>>>>>>>> As far as I understand it in DISLepton::project the iteration over all >>>>>>>>>> vertices and fails on the vertex "-6", because there are two outgoing >>>>>>>>>> leptons ("10009" and "10015"). The first electron loops over vertex "-5" >>>>>>>>>> back into vertex "-6" (for what ever reason), so it is not an actual final >>>>>>>>>> state particle. The old code from version 2.5.3 does actually work for the >>>>>>>>>> event. >>>>>>>>>> >>>>>>>>>> Cheers, >>>>>>>>>> Marian >>>>>>>>>> >>>>>>>>>> >>>>>>>>>> _______________________________________________ >>>>>>>>>> Rivet mailing list >>>>>>>>>> Rivet at projects.hepforge.org >>>>>>>>>> https://www.hepforge.org/lists/listinfo/rivet >>>>>>>>> >>>>>>>>> >>>>>>>>> >>>>>>>> >>>>>>>> >>>>>>> >>>>>>> >>>>>>> >>>>>> >>>>>> >>>>> >>>>> >>>>> >>>> >>>> >>> >>> >>> >> >> >> _______________________________________________ >> Rivet mailing list >> Rivet at projects.hepforge.org >> https://www.hepforge.org/lists/listinfo/rivet >> > _______________________________________________ > Rivet mailing list > Rivet at projects.hepforge.org > https://www.hepforge.org/lists/listinfo/rivet >
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