search for fcnc decays b s(d) → μ + μ -
DESCRIPTION
Search for FCNC Decays B s(d) → μ + μ -. Matthew Herndon, May 2006 University of Wisconsin Carnegie Mellon University High Energy Physics Seminar. Motivation Tevatron and CDF Analysis Method Results Conclusion. BEACH 04. J. Piedra. 1. The Standard Model. - PowerPoint PPT PresentationTRANSCRIPT
![Page 1: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/1.jpg)
BEACH 04 J. Piedra 1
Search for FCNC Decays Bs(d) → μμ-
Motivation
Tevatron and CDF
Analysis Method
Results
Conclusion
Matthew Herndon, May 2006University of Wisconsin
Carnegie Mellon University High Energy Physics Seminar
![Page 2: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/2.jpg)
2
The Standard ModelSuccesses of the Standard Model
Simple comprehensive theory
Explains the hundreds of common particles:
atoms, protons, neutrons, electrons
Explains the interactions between them
Basic building blocs
6 quarks: up, down...
6 leptons: electrons...
Force carrier particles: photon...
Predictions of the Standard Model have been verified to high precision
M. HerndonCMU Seminar
All common matter particles are
composites of the quarks & leptons
which interact by the exchange of
force carrier particles
![Page 3: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/3.jpg)
3
Beyond the Standard ModelWhy look for physics beyond the Standard Model
Look for new physics that would explain these mysteries:
SUSY, Extra Dimensions ...M. Herndon
Gravity not a part of the SM
What is the very high energy
behaviour?
At the beginning of the universe?
Grand unification of forces?
Where is the Antimatter?
Why is the observed universe mostly matter?
Dark Matter?
Astronomical observations of gravitational
effects indicate that there is more matter than
we see
Standard Model fails to answer many fundamental questions
CMU Seminar
![Page 4: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/4.jpg)
4
Searches For New PhysicsHow do you search for new physics at a collider?
Direct searches for production of new particles
Particle-antipartical annihilation
Example: the top quark
Indirect searches for evidence of new particles
Within a complex decay new particles can occur
virtually
A unique window of opportunity to find new physics before the LHC
M. Herndon
Tevatron is at the energy frontier and
a data volume frontier: 1 billion B and Charm events on tape
So much data that we can look for some very unusual decays
Where to look
Many weak decays of B and charm hadrons are very low probability
Look for contributions from other low probability processes – Non Standard Model
CMU Seminar
![Page 5: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/5.jpg)
5
Bs → μμ: Beyond the SMLook at decays that are suppressed in the
Standard Model: Bs(d) →μμ-
Flavor changing neutral currents(FCNC) to leptons
No tree level decay in SM
Loop level transitions: suppressed
CKM , GIM and helicity(ml/mb): suppressed
SM: BF(Bs(d) →μμ-) = 3.5x10-9(1.0x10-10)G. Buchalla, A. Buras, Nucl. Phys. B398,285
New physics possibilities
Loop: MSSM: mSugra, Higgs Doublet
3 orders of magnitude enhancement
Rate tan6β/(MA)4
Babu and Kolda, Phys. Rev. Lett. 84, 228
Tree: R-Parity violating SUSY
M. Herndon
One of the best indirect search channels at the TevatronCMU Seminar
![Page 6: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/6.jpg)
1.96TeV pp collider
Performance substantially improving
each year
Record peak luminosity in 2006:
1.8x1032sec-1cm-2
6
CDF and the Tevatron
CDF Integrated Luminosity
~1fb-1 with good run requirements
All critical systems operating
including silicon
Analysis presented here uses 780pb-1
Doubled data in 2005, predicted to
double again in 2006
-
Bs(d) →μμ- benefits from new dataCMU Seminar
![Page 7: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/7.jpg)
Silicon Tracker
|η|<2, 90cm long, rL00 =1.3 - 1.6cm
Drift Chamber(COT)
96 layers between 44 and 132cm
7
CDF DetectorMuon coverage
|η|<1.5
Triggered to |η|<1.0
Outer chambers: high purity muons
EXCELLENT TRACKING
CMU Seminar
TRIGGERED TO 1.5 GeV/c
![Page 8: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/8.jpg)
8
Rare B Decay Physics & TriggersLarge production rates
σ(pp → bX, |y| < 1.0, pT(B) > 6.0GeV/c) = ~30μb, ~10μb
All heavy b states produced
B0, B+, Bs, Bc, Λb, Ξb
Backgrounds: > 3 orders of magnitude higher
Inelastic cross section ~100 mb
Challenge is to pick one B decay from >103 other QCD events
Di-muon trigger
pT(μ) > ~1.5 GeV/c, |η| < ~1.0
B yields 2x Run I (lowered pT threshold, increased acceptance)
Di-muon triggers for rare decay physics
Bs(d) →μμ-, B+ →μμ-K+, B0 →μμ-K*0, Bs →μμ-φ, Λb→μμ-Λ
Trigger on di-muon masses from near 0GeV/c2 to the above Bs mass
Reduce rate by requiring outer muon chamber hits: pT(μ) > ~3.0 GeV/c or pTμ >
5.0GeV/c
TRIGGERS ARE CRITICAL
M. Herndon
-
1 Billion B and Charm Events on Tape
![Page 9: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/9.jpg)
9
Bs → μμExperimental Challenge
M. Herndon
Primary problem is large background at hadron colliders
Analysis and trigger cuts must effectively reduce the large background around mBs
= 5.37GeV/c2 to find a possible handful of events
Key elements of the analysis are determining the efficiency and rejection
of the discriminating variables and estimating the background levelCMU Seminar
![Page 10: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/10.jpg)
10
Analysis Method
M. Herndon
Performing this measurement requires that we
Demonstrate an understanding of the background
Optimize the cuts to reduce background
Accurately estimate α and ε: for triggers, reconstruction and selection cuts
SM predicts 0 events, this is essentially a search
Emphasis on accurately predicting the Nbg and performing an unbiased optimization
Blind ourselves to the signal region
Estimate background from sidebands and test background predictions in orthogonal
samples
€
BF(Bs → μ +μ−) =(Ncand −Nbg )
α BsεBs•αB +εB +
NB +
•fuf s
•
BR(B+ → J /ψK +) • BR(J /ψ → μ +μ−)
CMU Seminar
![Page 11: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/11.jpg)
11
Data Sample
M. Herndon
Start the with di-muon trigger
2 CMU muons or 1 CMU and 1CMX muon with pTμ > 5.0GeV/c
CMU: pT(μ) > ~1.5 GeV/c, |η| < ~0.6, CMX: pT(μ) > ~2.0 GeV/c, 0.6 < |η| < 1.0
1 CMUP muon: pT(μ) > ~3.0 GeV/c and 1 CMU(X) muon
Apply basic quality cuts
Track, vertex and muon quality cuts
Loose preselection on analysis cuts
PT(μμ-) > 4.0 GeV/c, 3D Decay length significance > 2 …
In the mass region around the Bs: 4.669 < Mμμ < 5.969 GeV/c2
Blind region: 4σ(Mμμ), 5.169 < Mμμ < 5.469 GeV/c2
Sideband region 0.5 GeV/c2 on either side of the blinded region
Sample still background dominated
Expect < 10 Bs(d) →μμ- events to pass these cuts: based on previous limits
100M Events
23K Events
CMU Seminar
![Page 12: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/12.jpg)
12
Normalization Data Sample
M. Herndon
Normalize to the number of
B J/K+ events
Relative normalization analysis
Some systematic uncertainties
will cancel out in the ratios of the
normalization
Example: muon trigger efficiency
the same for J/ or Bs muons for
a given pT
Apply same sample selection
criteria as for Bs(d) →μμ-
€
BF(Bs → μ +μ−) =(Ncand −Nbg )
α BsεBs•αB +εB +
NB +
•fufu
•
BR(B+ → J /ψK +) • BR(J /ψ → μ +μ−) 9.8 X 107 B+ events
![Page 13: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/13.jpg)
Need to discriminate signal from background
Reduce background by a factor of > 1000
Signal characteristics
Final state fully reconstructed
Bs is long lived (cτ = 438 μm)
B fragmentation is hard: few additional tracks
Background contributions and characteristics
Sequential semi-leptonic decay: b → cμ-X → μ+μ-X
Double semileptonic decay: bb → μ+μ-X
Continuum μ+μ-
μ + fake, fake+fake
Partially reconstructed, short lived,
has additional tracks
13
Signal vs. Background
M. Herndon
+
-
L3D
primary vertex
di-muon vertex
PT()L3D
LT
primary vertex
di-muon vertex
+
-
PT()LT
-
Cut on mass, lifetime, how well pT points to the vertex and isolationCMU Seminar
23K Events
![Page 14: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/14.jpg)
14
Discriminating Variables
M. Herndon
Mass M
choose 2.5σwindow: σ = 25MeV/c2
exp(λ=cτ/cτBs)
α : |φB – φvtx| in 3D
Isolation: pTB/( trk + pTB
)
exp(λ), α and Iso:
used in likelihood ratio
Optimization
Unbiased optimization
Based on simulated signal and data
sidebands
Optimize based on likely physics result
a priori expected BF limit
4 primary discriminating variables
CMU Seminar
![Page 15: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/15.jpg)
15
CDF 3D Silicon Vertex Detector
M. Herndon
8 layer silicon detector
4 double sided layers with stereo
strips at a small angle
3 double sided layers layers with
strips at 90
3D vertexing is a powerful
discriminant
2D from previous
analysis
CMU Seminar
![Page 16: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/16.jpg)
16
Likelihood Ratio
M. Herndon
Probability distributions used to construction the likelihood ratio
Use binned histograms to estimate the probabilities
Resulting likelihood with signal
MC and data sidebandsCMU Seminar
![Page 17: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/17.jpg)
17
Background Estimate
M. Herndon
Estimate the background for
any given set of requirements
Typical method: apply all cuts, see
how many sideband events pass
Optimal cuts may be chosen to
reject 1-2 unusual events
Flat background distribution allows
use of wide mass window
Need to show that mass is distribution is linear
Need to investigate backgrounds that may peak in signal region: B hh
Design crosschecks to double check background estimates
Analysis dependent on an accurate background estimate
CMU Seminar
![Page 18: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/18.jpg)
18
Background Estimate
M. Herndon
Expected number of combinatorial background in a 60 MeV/c2 signal
window
Extrapolation from sideband
0.99 expected to be near optimal cut, 1 background event typical of optimal search
Optimal point looks achievable
LH cut
Predicted Background
CMU-CMU
Predicted Background CMU-CMX
LH > 0.90 13.3±1.3 10.4±1.1
LH > 0.98 1.0±0.5 1.0±0.3
LH > 0.99 0.7±0.3 0.4±0.2 Cross-checks needed!
CMU Seminar
![Page 19: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/19.jpg)
19
Background Cross-Checks
M. Herndon
Use independent data samples to test
background estimates
OS-: opposite sign muons, negative lifetime
(signal sample is OS+)
SS+ and SS-: same sign muons,
positive and negative lifetime
FM: OS- and OS+ fake μ enhanced,
one μ fails the muon reconstruction quality cuts
Compare predicted vs. observed # of bg. events:
3 sets of cutsLoose: LR > 0.5
Medium: LR > 0.9
Tight: LR > 0.99
+
primary vertex
Fake di-muon vertex
CMU Seminar
![Page 20: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/20.jpg)
20
Bg. Cross-Checks Cont.
OS- Excellent control sample:
SS and fake muon could represent some bb backgroundsM. Herndon
[cm]
For >0: hist: OS pts: SS
OS+ vs. OS- OS+ vs. SS+
-CMU Seminar
![Page 21: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/21.jpg)
21
Bg. Cross-Checks Cont.
M. Herndon
OS- and Fake μ samples
SS+,SS-: expect and find 0 events for tighter cuts
OS-Predicted Observed Probability
LR > 0.50 840±16 821 28%
LR > 0.90 118±6 136 7%
LR > 0.99 8.7±1.9 17 2%
SS- LR > 0.50 8.7±1.7 6 27%
SS+ LR > 0.50 11.0±1.8 12 40%
FMPredicted Observed Probability
LR > 0.50 221±8 196 7%
LR > 0.90 40±3 29 6%
LR > 0.99 5.1±1.1 9 12%
Using 150 MeV/c2 mass
window for cross-check
Combined CMU-CMU(X)
Think about results with tight
cuts and FM
Investigated B hh carefully
Generated inclusive MC to look for anomalous background sources - no surprises found
CMU Seminar
![Page 22: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/22.jpg)
22
B hh Background
M. Herndon
Clearly peaks in signal region
Sideband estimates not useful
Observed/measured at CDF
ModeN Bs Mass Window
N Bd Mass Window
Bd 0.008 0.095
Bd K 0.005 0.55
Bd KK 0 0
Bs 0.035 0.006
Bs K 0.048 0.061
Bs KK 0.089 0.66
Total 0.19±0.06 1.37±0.16
Convolute known branching ratios and
acceptance with K and fake rates.
(estimated for LH > 0.99)
B hh background substantial!
CMU Seminar
![Page 23: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/23.jpg)
23
Acceptance & Efficiencies
: efficiency - from data where possible
Using J/ψ → μ+μ- and B+ → J/ψK+ data and special unbiased J/ψ triggers
Most efficiencies relative: Exception - and LH and K
M. Herndon
From Data
From MC:
Checked with Data
From MC
Second critical part of the analysis is estimating the efficiencies
€
α • total =α • ε trig • εreco • εLH
€
reco = εSVX • εCOT • εmuon • εVtx
€
trig = εL1 • εL2 • εL 3
From Data
CMU Seminar
![Page 24: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/24.jpg)
24
Example: SVX EfficiencyMeasurement of the efficiency of adding silicon hits to COT tracks
Use J/ψ → μ+μ- data
M. Herndon
εSVX = 74.5 ± 0.3(stat) ± 2.2(sys)%(2001-2003 data)
Average efficiency for adding silicon to two tracks: In silicon fid.
(2001-2002 data) (2001-2002 data)
Very low and went down
with pT and time!
![Page 25: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/25.jpg)
25
New SVX EfficiencyImproved silicon pattern recognition code and detector performance
M. Herndon
old avg (88%)w/ same data(2003)
+2% and flat - improved code
+5% εSVX improved code and
new quality cuts
εSVX = 74.5% → 88.5%
2001-2003 → 2001-2005 data
CMU Seminar
![Page 26: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/26.jpg)
26
LR Efficiency Cross-CheckEfficiencies determined using realistic MC
MC efficiencies validated by comparing with data using B+ → J/ψK+ events
Pt and isolation distributions
reweighed to match data Same
treatment for Bs
M. Herndon
LR Cut LR(data) LR(MC) Ratio
LR>0.90 0.70±0.01 0.71±0.01 0.98
LR>0.92 0.68±0.01 0.68±0.01 1.00
LR>0.96 0.60±0.01 0.61±0.01 0.98
LR>0.98 0.52±0.01 0.53±0.01 0.98
LR>0.99 0.41±0.01 0.43±0.01 0.96
Agreement good
4% systematic uncertainty assigned
5% from isolation reweighingCMU Seminar
![Page 27: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/27.jpg)
27
Final Efficiencies & AcceptancesLR efficiencies determined using realistic MC
Pt and isolation distributions reweighed to match data using Bs J/ events
M. Herndon
LR Cut LR(CMUCMU) LR(CMUCMX)
LR>0.90 0.65±0.01 0.68±0.01
LR>0.95 0.57±0.01 0.61±0.01
LR>0.98 0.47±0.01 0.49±0.01
LR>0.99 0.37±0.01 0.41±0.01
Very good efficiency for large
background rejection
For LR > 0.99
39% efficiency, 7% sys
~Factor 2000 of rejection
Acceptance ratio:
α(B+/Bs) = 0.297 ± 0.006 (CMUCMU), 0.191 ± 0.008 (CMUCMX): 7% sys - generation model
Most efficiency ratios near 1
Two absolute efficiencies:
K+COT = 95% and K+SXV = 96%
CMU Seminar
![Page 28: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/28.jpg)
28
Optimization ResultsTried Likelihood ratios from 0.9-0.99: LR Cut 0.99
M. Herndon
NB+: 5763 ± 101
εLR: 39%
Backgrounds:
a priori Bs limit: 1.1x10-7 95% CL
Optimized for 1fb-1
Systematic uncertainties
Bg. estimation: 28%
Bg statistical error
Sensitivity: 16%
12% fs/fu
7% acceptance
7% LR
Previous CDF result 2.0x10-7
Decay
Bhh Background
Combinatoric Background
Total Background
Bs
0.19±0.06 1.08±0.36 1.27±0.36
Bd
1.37±0.16 1.08±0.36 2.45±0.39
CMU Seminar
![Page 29: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/29.jpg)
CDF 1 Bs result: 3.010-6
CDF Bs result: 365pb-1 2.010-7
D0 Bs result: 240pb-1 4.110-7
BaBar Bd result: 8.310-8(90%)
29
Bs(d) → μ+μ- Search Result
M. Herndon
PRL 95, 221805 2005
Results: 1(2) Bs(d) candidates observed
consistent with background expectation
Worlds Best Limits!
Decay
Total Background Observed
Bs
1.27±0.36 1
Bd
2.45±0.39 2 BF(Bs +- ) < 1.0x10-7 at 95% CL
BF(Bd +- ) < 3.0x10-8 at 95% CL
DO Note 4733-Conf
PRL 94, 221803 2005
CMU Seminar
![Page 30: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/30.jpg)
30
Bs →μμPhysics Reach
Strongly limits specific SUSY models: SUSY SO(10) models
Allows for massive neutrino
Incorporates dark matter results
M. Herndon
BF(Bs +- ) < 1.0x10-7 at 95% CL
Excluded at 95% CL
BF(Bs +- ) = 1.0x10-7
Dark matter constraints
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
R. Dermisek et al.hep-ph/0507233R. Dermisek JHEP 0304 (2003) 037
Looks like the theorists
have a little work to do!
CMU Seminar
![Page 31: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/31.jpg)
31
Bs →μμPhysics ReachIn addition to limiting S0(10) models – starting to impact standard MSSM scenarios: CMSSM
Blue BF(Bs → μ+μ-)
Light green: b → s
Cyan: dark matter constraints
Dashed red: Higgs mass bound
Red brown areas: excluded
Incorporates errors from fBs and mtop
M. Herndon
BF(Bs +- ) < 1.0x10-7 at 95% CL
J. Ellis Phys. Lett. B624, 47 2005
CMU Seminar
BF(Bs +- ) = 2.0(1.0)x10-7
![Page 32: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/32.jpg)
M. Herndon 32
Conclusions
Best Bs and Bd results: well ahead of D0 and the B factories
Limit excludes part of parameter space allowed by SO(10) models
Expanding sensitivity to interesting areas of MSSM parameter space
Improving analysis to include selection NN and advanced lepton ID(from CMU: Vivek)
Improved fs results could also improve result by 10-20%(from CMU: Karen)
CDF B(s,d) →μ+μ- results
BF(Bs +- ) < 1.0x10-7 at 95% CL
BF(Bd +- ) < 3.0x10-8 at 95% CL
Worlds Best Limits!
CMU Seminar
Goal for 1fb-1 analysis: BF(Bs +- ) < 7.0x10-8 at 95% CL
![Page 33: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/33.jpg)
33
Muon & Trigger EfficienciesL1 eff: Use J/ψ → μ+μ- trigger that only requires one muon
L3 eff: Use autoexcept trigger
M. Herndon
trig
ger
effic
ienc
y (%
)75
1
0075
10075
10
0
75
100
75
100
2 6 10PT (GeV)
L1 Muon L1(pT,η), L3 1 number
Convolute εL1 for each muon and εL3
Systematic errors L1 and L3:
Kinematic difference between
J/ψ → μ+μ- and Bs(d) →μμ-
2-Track correlations
Sample statistics
εtrig = 85 ± 3%
Offline muon reconstruction
From J/ψ → μ+μ- L1 trigger with one
muon found
Systematic from comparison to Z
εmuon = 95.9 ±1.3(stat) ± 0.6(sys)%
![Page 34: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/34.jpg)
34
COT EfficiencyEstimated by embedding COT hits from MC muons in real data
Occupancy effects correctly accounted for
Efficiency driven by loss of hits when hit density is high
Demonstrate agreement between hit usage in data and MC
Tunable parameters can lower or raise the hit usage and the efficiency to bracket the data
M. Herndon
εCOT = 99.62 ± 0.02%
Systematic errors
Isolation dependence dominant
systematic
Pt dependence
2-track correlations
Varying the simulation tuning
Error: +0.34 -0.91
Consistent with true tracking eff.
using high pt elections identified in
the calorimeter
![Page 35: Search for FCNC Decays B s(d) → μ + μ -](https://reader035.vdocuments.net/reader035/viewer/2022062519/56815414550346895dc210dd/html5/thumbnails/35.jpg)
35
Bs →μμPhysics ReachIn addition to limiting S0(10) models – starting to impact standard MSSM scenarios: mSugra
Blue BF(Bs → μ+μ-)
Light green: b → s
Cyan: dark matter constraints
Dashed red: Higgs mass bound
Red brown areas: excluded
Incorporates errors from fBs and mt
M. Herndon
BF(Bs +- ) < 1.0x10-7 at 95% CL
J. Ellis Phys. Lett. B624, 47 2005