hot topics at d0 david buchholz (northwestern univ) on behalf of the dØ collaboration
DESCRIPTION
4/9/2006 D. Buchholz 3 Excellent Tevatron Performance Data sample corresponding to over 1 fb -1 of the integrated luminosity used for the Bs mixing analysis Results are being reported on this 1 fb -1 sampleTRANSCRIPT
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Hot Topics at D0
David Buchholz (Northwestern Univ)On behalf of the DØ
Collaboration
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4/9/2006 D. Buchholz 2
D0 Results
D0 Talks at this conference- b physics
B mixing and lifetimes- PiedraBs decays and B leptonic decays- Van Kooten
t physicsTop Physics – Clement
Many new b and t physics resultsWatch for these in other talks
Hot Topics at D0Bs and Bd mixingCP violation result in B decaysFlavor Changing Neutral Current results (D±→ π±μ+μ- )
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4/9/2006 D. Buchholz 3
Excellent Tevatron Performance
Data sample corresponding to over 1 fb-1 of the integrated luminosity used for the Bs mixing analysis
Results are being reported on this 1 fb-1 sample
Run II Integrated Luminosity
0.00.10.20.30.40.50.60.70.80.91.01.11.21.31.41.51.61.71.81.92.0
Apr-02 Jul-02 Oct-02 Jan-03 Apr-03 Jul-03 Oct-03 Jan-04 Apr-04 Jul-04 Oct-04 Jan-05 Apr-05 Jul-05 Oct-05 Jan-06 Apr-06 Jul-06
Lum
inos
ity (f
b-1)
DeliveredRecorded
19 April 2002 - 22 February 2006
1.19
1.41
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4/9/2006 D. Buchholz 4
D0 Detector
B Physics Program based on excellent performance of1) muon system, |η|<2.0, pT > 3,4,5 GeV2) silicon microstrip tracker3)Good single and dimuon triggers
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4/9/2006 D. Buchholz 5
Unitarity Triangle- B Mixing Contribution
(0,0) (0,1)
(,)
*
ubud
*tbtd
VVVVarg
*cbcd
*tbtd
VVVV
*
tbtd
*cbcd
VVVVarg
*
cbcd
*ubud
VVVVarg
*cbcd
*ubud
VVVV
(0,0) (0,1)
(,)
*
ubud
*tbtd
VVVVarg
*cbcd
*tbtd
VVVV
*
tbtd
*cbcd
VVVVarg
*
cbcd
*ubud
VVVVarg
*cbcd
*ubud
VVVV
tdV
0dB0
sB
0dB0sB
b
sd , b
sd ,tcu ,,tcu ,, W
W
*tdV*
tsV
tsV
Measurement of Δms contributes to better determination of Vtdms ~ (lots of QCD)x|Vts|
md ~ (lots of QCD)x|Vtd|
ms/md ~ (much less QCD)x|Vts|/|Vtd|
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4/9/2006 D. Buchholz 6
Mixing and OscillationsBB
tms cosA
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4/9/2006 D. Buchholz 7
Analysis Outline
Select Bs candidate Concentrate on the most clean decay mode BsνμDs(φπ)
For each Bs candidate BS flavor at decay time from muon sign at the reconstructed side Transverse length LT and its error Transverse momentum PT(Bs) (use PT(Dsμ)) B-hadron flavor at the opposite side (indicates BS flavor at production time)
μ+
π -
K+K-
φD-
S
μ(e) B
ν
00ss BB
XReconstructed Side
Opposite Side
LT
KKBB ss 00
sD
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4/9/2006 D. Buchholz 8
Proper Decay Length
Proper Decay Length is determined from the Visible Proper Decay Length
K-factor takes into account the escaping neutrino and other missing particles
From MC for each decay mode- different excited states
Kxct MBs
s
s
BT
DT
ppK
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4/9/2006 D. Buchholz 9
Resolution Calibration Using Data Use J/ψ→μμ sample
Fit pull distribution for J/ψ Proper Decay Length with 2 Gaussians Resolution Scale Factor is 1.0 for 72% of the events and 1.8 for the rest Confirmed by Impact Parameter tuning procedure in MC
μ
PVJ/ψ vertex
μ
L±σL
DØ Run II Preliminary
resolution resolution plus decays
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4/9/2006 D. Buchholz 10
Efficiency Dependence on VPDL
From MC Cross-checked and tuned using data
Note that efficiency at VPDL=0 is not 0
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4/9/2006 D. Buchholz 11
Opposite Side Tagging
6.0||
6.0||
pqp
QSV
t
t
pqp
Q)(
Pa
t
tev p
qpQ
)(
e
Tagging side
Bs
Ds
Primary VertexSecondary Vertex
K K
e
B
Reconstructed B-meson
Muon (electron) jet charge defined as: Sum is taken over all tracks in the cone ΔR<0.5 around muon;
SV Charge:
Event charge: all tracks with ΔR < 1.5 w.r.t. reconstructed B direction are used
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4/9/2006 D. Buchholz 12
Calibration of Dilution Using BdD*±μνXIn
crea
sing
dilu
tion
Incr
easi
ng d
ilutio
n
ΔmHFAG = 0.507 ± 0.004 ps-1
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4/9/2006 D. Buchholz 13
Final Signal Selection
Use likelihood ratio method Set of discriminating variables xi
constructed for each eventHelicity Angle (Ds,K1) Ds Isolation pT(K1K2)m(Ds) 2 of Ds Vertex Fitm(K1K2 or K1)
Construct likelihood ratio for each variablebgrd from m(Ds) sidebandssignal from bgrd-sub peak
)()(
iB
i
iS
ii xf
xfy
Combine into single variableUse for final selection
n
iiyY
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4/9/2006 D. Buchholz 14
μ sample @ D0 (~1 fb-1)
μDs: 26,710±560
Opposite-side flavortagging
Tagging efficiency ~20%
μD±: 7,422±281
μD±: 1,519±96
μDs: 5,601±102
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4/9/2006 D. Buchholz 15
Cross-check Using BdXμD±()
The Amplitude Scan reveals the Bd oscillations at correct place no lifetime bias with correct amplitude correct dilution calibration
Amplitude ScanDØ Run II Preliminary
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4/9/2006 D. Buchholz 16
Event-by-Event Fit
Minimize the Likelihood function Probability Density Functions (PDF) for each
source Proper Decay Length Dilution Proper Decay Length Error Mass Signal Selection Variable
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4/9/2006 D. Buchholz 17
Vertex Resolution
Determined by vertex fitting procedure
e.g. Period of oscillations @ 19ps-1
DØ Run II Preliminary
Limit of sensitivity to mixing at 22ps-1
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4/9/2006 D. Buchholz 18
Results of the Lifetime Fit
Different background models are used for cross-check and systematic errors Trigger biases have been studied
Different efficiency models Central values for cτBs= 404 − 416 μm
Statistical error ~10 μm HFAG value cτBs = 438 ± 12 μm
Most important region
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4/9/2006 D. Buchholz 19
Amplitude Scan For Bs
Deviation of the amplitude at 19 ps-1 2.5σ from 0 1.6σ from 1
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4/9/2006 D. Buchholz 20
Log Likelihood Scan
ms < 21 ps-1 @ 90% CL assuming Gaussian errorsMost probable value of ms = 19 ps-1
Systematic
Resolution K-factor variation BR (BsDsX) VPDL model BR (BsDsDs)
In agreement with the amplitude scan
Have no sensitivity above 22 ps-1
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4/9/2006 D. Buchholz 21
World Average
@19ps-1: 1.5σ 2.3σ
HFAG PreliminaryCorrelated systematics not yet included
With current D0 result
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4/9/2006 D. Buchholz 22
Ensemble Tests Using data Simulate Δms=∞ by randomizing the sign of flavor tagging Probability to observe Δlog(L)>1.9 (as deep as ours) in the range 16 < Δms < 22 ps-1 is 3.8%
5% using lower edge of syst. uncertainties band Region below 16 ps-1 is experimentally excluded No sensitivity above 22 ps-1
Using MC Probability to observe Δlog(L)>1.9 for the true
Δms=19 ps-1 in the range 17 < Δms < 21 ps-1 is 15%
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4/9/2006 D. Buchholz 23
Impact on the Unitarity Triangle
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4/9/2006 D. Buchholz 24
Impact on the Unitarity Triangle
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4/9/2006 D. Buchholz 25
if eAA
pq
f
||||
||||
CP Violation in MixingCP Violation in Mixing
Three phenomenological signatures
00 MqMpMCP
CPV in MixingK: L B: ll ll
CPV in Decay//: KL ACP:
Mixing vs Decay: L ?: J/s
First in K
Last in B
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4/9/2006 D. Buchholz 26
)()()()(
XbbNXbbNXbbNXbbNASL
Analysis StrategyAnalysis Strategy
Goal is to measure with part per mil precision by looking for asymmetry in like-sign dimuons
How?Using independent spectrometers and
reversing the polarities
Toroid
Solenoid
Solenoid Toroid
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4/9/2006 D. Buchholz 27
Tor*Sol polarity -1 +1
N++ 177,950 156,183N-- 176,939 156,148N+- 1,175,547 1,029,604
Raw ResultsRaw Results
)(0008.0)(0012.00013.0 syststatA
Now need the fraction of from B
AfA BSL
After removing detector based asymmetries:
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4/9/2006 D. Buchholz 28
Sample CompositionSample Composition
signal
Backgrounds that dilute the
asymmetry
Backgrounds with false asymmetries:
Reaction KNYπ (Y=Λ,Σ...) has no K+N analog
bb b
bb c
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4/9/2006 D. Buchholz 29
Sample CompositionSample Composition
signal
Backgrounds that dilute the
asymmetry
Backgrounds with false asymmetries:
Reaction KNYπ (Y=Λ,Σ...) has no K+N analog
bb b
bb c
Cross-check:
0076.01281.0)(024.0001.0136.0)0(
PDGD
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4/9/2006 D. Buchholz 30
)syst(0008.0)stat(0012.00013.0A
)syst(0028.0)stat(0040.00044.0ASL
)syst(0007.0)stat(0010.00011.0ε1
)εRe(2
B
B
0
0
ResultsResults
Raw Asymmetry:
Asymmetry from Mixing:
41
)Re(2
0
0 SL
B
B A
CP Violation Parameter:
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4/9/2006 D. Buchholz 31
ResultsResults
)syst(0007.0)stat(0010.00011.0ε1
)εRe(2
B
B
0
0
(0.4±1.4±0.9)
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4/9/2006 D. Buchholz 32
Flavor Changing Neutral Currents
D+
m(GeV) 0.5 1.0 1.5
(1/
)(d
/dm
2 )G
eV-
2 )
10-4
10-6
10-8
10-10
RPV in the up sector and not the down sector
Burdman et al. hep-ph/0112235cu
Little Higgs models with new up sector vector quark
Fajfer et al. hep-ph/0511048
factors of >1000 over SM not ruled out. Similar in magnitude to Bs
but orthogonal parameter space
Strict limits from b s and s d Possible to have effects in up sector and not down sector
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4/9/2006 D. Buchholz 33
cc u u Analysis StrategyAnalysis Strategy
First find Ds BF(Ds BF(2.85 +/- 0.19) x 10-4
Product ~ 1 x 10-5
Then search for excess in the continuum region Dwith m(
Start with low mass dimuon candidate, add track to form D candidate
Reduce background with lifetime and topological cuts
~51k ~55k
Dimuon invariant mass
DØ Preliminary1 fb-1
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4/9/2006 D. Buchholz 34
Results for Results for DD
n(Ds) = 65 ± 11
Optimized cuts
n(D+) = 26 ± 9
DØ: BF( D (1.75 +/- 0.70 +/- 0.50) x 10-6
CLEO-c: (2.7 +3.6 -1.8 +/- 0.2) x 10-6 Expected: 1.77 x 10-6
m( GeV/c2 for candidates with 0.96 < m() < 1.06 GeV/c2
DØ Preliminary
1 fb-1
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4/9/2006 D. Buchholz 35
Results for Results for DD
DØ Preliminary DØ Preliminary1 fb-1 1 fb-1
0.96 < m() < 1.06 GeV/c20.2 < m() < 0.96 GeV/c2
1.06 < m() < 1.76 GeV/c2
n(D) = 6
n(S+B) = 5.3 +/- 1.5
n(Ds) = 3
n(S+B) = 4.6 +/- 0.7
Good agreement with expectations
n(bkg) = 20.9 +/- 3.4
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4/9/2006 D. Buchholz 36
Results for Results for DD
DØ Preliminary1 fb-1
0.2 < m() < 0.96 GeV/c2
1.06 < m() < 1.76 GeV/c2
n = 17 n(bkg) = 20.9 +/- 3.4
Branching fraction limit D+
DØ: < 4.7 x 10-6 (at 90%)
CLEO-c(e+e-): 7.4x 10-6 at 90%
FOCUS: 8.8 x 10-6 at 90%
New limit on second generation RPV couplings
002.02122 kk
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4/9/2006 D. Buchholz 37
Check of SM with Lifetimes and BRIn SM ( with CP conserved)
eigenstates are CP specific- check decay portion of matrix
Measure of decay rates and widths in Bs
0-Bs0 system
Γs measures lifetime average1/ΔΓs measures off diagonal decay matrix element
(*)(*)0sss DDB
MeasureFlavor specific, e.g.
Branching ratios
Lifetimes Differences /0 JBs
ssss DBDB 00
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4/9/2006 D. Buchholz 38
1 Sigma Contours on ΔΓs and 1/Γs
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4/9/2006 D. Buchholz 39
Conclusions Tevatron’s first fb-1 opening up several new opportunities in flavor physics
Today, 3 world’s best results Rare FCNC charm decays CP Violation in B mixing First double sided bound on ms
More improvements this summer- extend analysis and new hardware = layer 019 years after the observation of Bd mixing and 12 years after
the first lower limit on ms, we now have first direct double sided bound on the Bs oscillation frequency.
ms < 21 ps-1 @ 90% CL
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4/9/2006 D. Buchholz 40
Backup Slides
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4/9/2006 D. Buchholz 41
Initial State Tagging
Get best estimate for reconstructed B meson to contain b(b) at origin
Definitions:Efficiency:
Dilution:
Tagging power:use to compare the performance of taggers
WSRS
WSRS
NNNND
total
tagged
NN
2D
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4/9/2006 D. Buchholz 42
dpr
D
Dilution
Determine dilution on event-by-event basis from BdD*±μνX events
Use opposite side events
Plot dpr ( predicted) versus D measured
%d0%a3%d1%87%d0%b5%d0%b1%d0%bd%d1%8b%d0%b9%d0%9f%d0%bb%d0%b0%d0%bd %d0%a4%d1%83%d0%bd%d0%b4%d0%9c%d0
%d0%93%d0%90%d0%a3%d0%97%20%20%d0%a0%d0%9f%d0%a6%20%d0%b3 %d0%a3%d0%bb%d0%b0%d0%bd %d0%a3%d0%b4%d1%8
%d0%a1%d0%b1%d0%be%d1%80%d0%bd%d0%b8%d0%ba%20%d0%9c%d0%b5%d0%b4 %20%d0%b7%d0%b0%d0%b2 %20%d0%b4%d0%b
%d0%9f%d1%80%d0%be%d0%b3%d1%80%d0%b0%d0%bc%d0%bc%d0%b0 %d0%a1%d1%8a%d0%b5%d0%b7%d0%b4%d0%a2%d0%b5%d1
%d0%9c%d0%b0%d0%b3 %d0%95%d0%ba%d0%b1 %d0%91%d1%96%d0%be%d1%82%d0%b5%d1%85%d0%bd%d0%be%d0%bb%d0%be%d
1060204 %d0%bb%d0%b8%d1%81%d1%82%d0%be%d0%b2%d0%ba%d0%b0 %d0%bf%d0%be %d1%82%d0%b5%d0%bf%d0%bb%d0%be
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