muon tag efficiency puzzle
DESCRIPTION
?. ?. ?. ?. Muon Tag Efficiency Puzzle. Remember the problem pointed out by Niels:. Before trigger, tag ( ) is much smaller for offsel B than for offsel B J/ ( )K* (and also the wrong-tag fraction ). - PowerPoint PPT PresentationTRANSCRIPT
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 1
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Muon Tag Efficiency PuzzleMuon Tag Efficiency Puzzle
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Before trigger, tag() is much smaller for offsel B than for offsel BJ/()K* (and also the wrong-tag fraction ).Possible explanation: misID prob increases with increasing number of true muons in the Muon System (MS).
Remember the problem pointed out by Niels:
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 2
PiMu and MuMu efficienciesPiMu and MuMu efficiencies
Try to reproduce and efficiency numbers of reop-TDR
In ntuples: 26k offline-selected Bs->KK and 20k Bs->J/()Store in ntuple all Particles (Long and VTT)
Store a subset of MCParticles:All , , e (not from ) and K , if they have Ekin>1 GeV, <0.5 rad
+ all those associated to a stored Particle or MuonID (+signal B and other-side B)
Note: somewhat different definition of reference event samplesTDR: require extrapolation of the track to be in M1-5 and p>3GeV/c
Here: require Long track and p>3GeV/c, use offline-selected events
In addition, modify the DaVinci DLL: if no MS Info, then set DLL to –inf. (DV: if (!proto->muonBit()) … i.e. do not attempt muon identification without MS info)
Was this also the case for the TDR ?
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 3
DLLmupi without Muon System Info
DLLmupi without Muon System Info
RICH provides some PID for pi-museparation, however:
Not very powerful as it is nowNote the zooming factor 300 for muons!
Note in passing:Was it optimized for low-momentum particles ?BTeV claims using this for pi-mu separation (tagging)
This study: will set all these DLLs to-infinity.(If “RICH-only” PID is allowed, then one should at least put a more stringent cut onDLL for those events, than in the case the MS info isavailable.)
(looks the same for Bs->KK)
Bs->J/()
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 4
Various definitions of efficiency
Various definitions of efficiency
Say efficiency = N/D.
The 3 pairs of plots show the result
for and with 3 different
definitions of the numerator N and
denominator D:
Do not require MS info for either N and D (“RICH-only” identification allowed)
Require MS info for positive identification (i.e. for N only) NOTE THE DIFFERENT SCALES!
Require MS info in the reference sample (i.e. for both N & D)
Bs->KKBs->J/()
Use this one!
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 5
Muon p and pT spectraMuon p and pT spectra
Bs->KK
Bs->J/()
Difference in muon p and pT spectra due to the fact that most muon come from the B in one case and not in the other. This explains difference in muon PID efficiency.
Do not get confused ! This should not be the reason for the difference in muon tag efficiency (tag ) for B-> and for Bs-> J/()K*, because the tag muon is supposed to be from a B in both cases!
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 6
PiMu and MuMu efficienciesPiMu and MuMu efficiencies
Part
icle
s (p
>3G
eV/c
and
Lon
g tr
ack)
mat
ched
to M
C
MC= MC=
effi
cien
cy
(
%) efficiency
(%
)
DLL DLL (note: if MS Info, DLL set to –inf.)
Bs->KK
efficiency
(%)ef
fici
ency
(
%)
Bs->J/()
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 7
PiMu and MuMu efficienciesPiMu and MuMu efficienciesef
fici
ency
(
%)
DLL(note: if MS Info, DLL set to –inf.)
Bs->KK
efficiency
(%)
efficiency (%)
Bs->J/()
Summary: DLLcut OTDR (Bs->JPsiKs) 93 % 1 % -8Here (Bs->JPsiPhi) 95.7% 1.0% -8Here (Bs->KK) 70.3 % 0.5% -8
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 8
What ’s are id’ed as ’s ?What ’s are id’ed as ’s ?
Mostly decays.
The rest is probably punch-through or random combinations (“overflows”)
Zend / mm of MC asso’ed to a p>3GeV/c Long track id’ed as
Bs->J/()
Bs->KK
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 9
Sources of MuonsSources of Muons
Bs->J/() Bs->KK
# MC in event with MuonCoords>1 # MC in event with MuonCoords>1
Each color should add up to ~20k Each color should add up to ~26k
MC Origin:z<400mmx,y<5mm
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 10
Number of Muons per EventNumber of Muons per Event
# MC with MuonCoords>1 excluding from -decay
# MC with MuonCoords>1 excluding from -decay
Try to unravel effect of random combinations on misId: Bin the number of MC muons per event which hit M2-5 but
which are not from a decaying pion (see plots below) For each such bin sum up isidentified pions over all events
Bs->J/() Bs->KK
Mean 0.438Mean 2.467
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 11
… the result… the result# Particles associated to a MC and id’ed as
# Particles associated to a MC =
(Particle = Long track and p>3GeV/c.Sum numerator and denominator over all events)
ef
fici
ency
# MC with MuonCoords>1 excluding from -decay
# MC with MuonCoords>1 originating from near IP
Bs->KK Bs->J/()
Clear dependence of misId efficiency on number of muons!
Note: All these isidentified MC pions have 0 or 1 MuonCoords. Misidentification most probably due to random combinations.
Clear dependence of misId efficiency on number of muons!
Note: All these isidentified MC pions have 0 or 1 MuonCoords. Misidentification most probably due to random combinations.
ef
fici
ency
DLL>-8.0 and MS info available
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 12
MCParticle <-> MuonIDMCParticle <-> MuonIDTo support the rnd combination hypothesis: tried to associate MS info of isidentified pions to MCParticles…
Done in a shaky way: retrieve MuonId object, from which I retrieve a (number of)
MuonCoord, each being then associated to a MCParticle.
Problem: several MCParticles in the basket …
Take the one that comes most often (the 1st one in case of a draw)
How good is this ? I have no clue.
If correct, it confirms that misId is not due to punch-thru, but rather to rnd associations.
e
K
Probable HEP ID of MCParticle associated to the MuonID object of a isidentified non-decaying MC pion (when it is a different MCParticle)
Bs->KK(looks the same for Bs->JPsiPhi)
There are 12 more events where it is the same MC pion !
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 13
Can this explain the Muon Tag Efficiency Puzzle ?
Can this explain the Muon Tag Efficiency Puzzle ?
Fully explains the jump in the average presented a few slides up:
Bs->KK = 0.5%
Bs->J/() = 1.0%
But can it explain the tag puzzle ?
B-> tag = 6.5%
Bs-> J/()K* tag = 10%
Did a rapid small exercise: pseudo tagging muons: use DLL>-9 and add pT>1.2 GeV/c and p>5 GeV/c and
remove muons which are associated to an MC muon from signal B.
Get for 26k offline-selected events:0.43 % x 49911 = 215 215+1323
88.7 % x 1491 = 1323 26157
1.14 % x 40146 x R = 586 586+1467
88.8 % x 1290 x R = 1467 26157
R = 26157/20427 (ratio of offline selected events)
= 5.9%
= 7.9%
Bs->KK
Bs->J/()
To be continued…
Signal daughter clone problem ?
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 14
ID of MCParticle associated to the selected TagMuon
ID of MCParticle associated to the selected TagMuon
Bs->KK Bs->J/() (26k off-sel) (20k off-sel)
K- 46 68
- 91 145
+ 422 319
E+ 0 4
none 63 52
e- 1 10
- 862 664
+ 83 177
K+ 69 97
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LHCb Trigger Meeting – December 15, 2003, CERN Massimiliano Ferro-Luzzi 15
Mu-pi opening angle in Lab
Mu-pi opening angle in Lab
Pion => muon + neutrino
Muon momentum = 30 MeV/c in pion rest frame
Maximum muon opening angle versus boost (pion energy in lab frame)
Max
muo
n an
gle
(de
g)
Lab Epion / GeV