|
[Rivet] CMS dressed top questionLars Sonnenschein sonne at mail.cern.chWed Nov 12 12:37:36 GMT 2014
Hello Andy, so if I understood you right we should only look at the vector sum of all neutrinos in a generated event and then reconstruct the tops up to an eight-fold ambiguity in the ttbar dilepton channel, assuming that we are not able to distinguish a b-jet from a bbar-jet? Lars ______________________________________ Dr. rer. nat. habil. Lars Sonnenschein ______________________________________ Home Institution: RWTH Aachen III. Phys. Inst. A, 26A204 Physikzentrum 52056 Aachen Germany -------------------------------------- ______________________________________ CERN: PH/UCM, 32/2C-07 CH-1211 Geneve 23 Switzerland Tel.:+41(22)767-9875 -------------------------------------- ______________________________________ FNAL: D0, PK151 Mailstop #352 Fermilab, P.O.Box 500 Batavia, IL 60510-500 USA Tel.: +1(630)840-8740 ______________________________________ On Wed, 12 Nov 2014, Andy Buckley wrote: > On 12/11/14 09:45, Lars Sonnenschein wrote: >> Hello Andy, > > Hi Lars, > > Please contact the Rivet list rather than me personally. I've CC'd it > (again ;-) ) > >> we are still struggling with the first top analysis getting into Rivet. >> In the ttbar dilepton channel we get two oppositely charged leptons and >> two neutrinos we are touching in Rivet to reconstruct the two W bosons. >> >> Are we allowed to make use of the information if it is a neutrino or an >> anti-neutrino we are dealing with? > > It's up to you, but I'd advise against it unless CMS has some > extraordinary subdetector that I'm not aware of which can do detailed > neutrino particle ID ;-) The experimental analysis needs to resolve the > ambiguity, therefore it's best that the equivalent MC analysis does so, too. > > And of course it's actually a worse problem than you say -- you can only > see one missing energy vector, not two separate (anti)neutrino > components within it, so you can't treat the two tops independently. > >> This would remove one ambiguity. >> The temporary version of the Rivet code is right now making a choice: >> >> |(lepton1+neutrino1).M()-W.M()| >> + |(lepton2+neutrion2).M()-W.M()| >> < |(lepton1+neutrino2).M()-W.M()| >> + |(lepton2+neutrion1).M()-W.M()| >> >> for the pair which matches better the W boson mass without exploiting >> neutrino/anti-neutrino information. > > Again, how can you experimentally determine the momentum vectors of > multiple neutrinos in a single event? If you think you can do that > safely, then being able to tell whether they are nu's or anti-nu's is > not a big leap. The important thing to think about is whether you can > safely use this sort of experimentally unavailable truth information at > all -- naively the answer is no. > > The (only?) situation in which it *is* appropriate is where the data has > been unfolded, using MC models and adding significant modelling > systematics, to an MC analysis which used this full information. Then > you would be writing a Rivet analysis using identical logic to the MC > truth analysis that went into the data analysis. That is fine, but doing > the data analysis that way (i.e. relying on unfolding to perfectly deal > with an intrinsic experimental analysis ambiguity) is rather > unsatisfactory and I suspect is not the case. > > Andy > > -- > Dr Andy Buckley, Royal Society University Research Fellow > Particle Physics Expt Group, University of Glasgow / PH Dept, CERN >
More information about the Rivet mailing list |