search for lepton flavor violating decays t - l - p 0 , l - h , l - h ’ at belle
DESCRIPTION
筑波山. Search for Lepton Flavor violating decays t - l - p 0 , l - h , l - h ’ at Belle. Yuji Enari Nagoya University. Mt. Tsukuba. KEKB. Belle collaboration. Contents KEKB-Belle experiment Lepton Flavor violation Analysis Discussion and conclusion. 1. KEKB-Belle experiment. - PowerPoint PPT PresentationTRANSCRIPT
Search for Lepton Flavor violating decays l , l , l ’ at Belle
Yuji Enari Nagoya University
Mt. Tsukuba
KEKBBelle collaboration
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 2
Contents1. KEKB-Belle experiment2. Lepton Flavor violation3. Analysis4. Discussion and conclusion
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 3
1. KEKB-Belle experiment
e : 8GeV e : 3.5GeV
s = 10.58 GeV
Lpeak = 1.58 1034cm-2s-1
Cross section : 0.9 nb BB : 1.0 nb
KEKB : Asymmetric energy e+e Collider
KEKB is -Factory
約1 5H zで対が生成される。
Ldt = 450 fb-1World Record
Continuous injection mode
LER: 1.7A
HER: 1.2A
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 4
History of integrated luminosity
Continuous injection
2003 Summer: SVD/CDC inner partreplacement
Ldt = 154fb-1
Ldt = 450fb-1
Ldt = 244fb-1
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 5
1.2 Belle detectorKLM RPC+Fe, sandwich structure
CDCsmall cell +He/C2H6
ECLCsI(Tl) 16X0
ACC n=1.015~1.030 S/K ~ 3 @ p < 3.5GeV/c
SVD3 lyr. DSSD
TOF Scinti + FM-PMT TOF = 100ps, S/K ~ 2 @ p<1.4GeV/c
SC solenoid 1.5T8 GeV e
3.5 GeV e
Size : 7m×7m×7m 、 Weight : 2000t
Cylindrical Coordinate :e Beam axis as z axis.
E resol.E /E = 1.8% @E=1GeV
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 6
1.2 Performance of Lepton IDEf
ficie
ncy
(%)
Fake
rate
(%)
Electron IDECL : (a) E/p (b) XECL-Xtrk
(c) E9/E25
Muon IDKLM: (a) # of Hit layer (b) Shower Shape
CDC: (d) dE/dx
ACC: (e) Nphoton
~90%
~1.5%
~92.5%
~0.25%
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 7
Small cell drift chamber installation (2003. Aug.)
• SVD upgrade (3Layer 4 layer)• To fit CDC configuration for SVD upgrade.• To reduce hit rate of Cathode part.
Layer
Hit
rat e
/wire
(kH
z) HER 1.1ALER 1.5AL=9.6x1033cm-1s-1
MainInner
Cathode
Partial cross section of CDC (50 layer.)
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 8
Small cell drift chamber• Replace Cathode chamber (1cm-cell 3 layers w/ cathode r~8cm) to Small cell chamber (5mm-cell / 2 layers r~10cm).
Small cell Installation
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 9
Alignment after installation
• Measure following variable using cosmic track. – rotation angle – shift length x,y
for both forward and backward in each layer.
of endplate
Result: Large y~200m were observed in Inner layers at forward.
Main partInnerSmall cell
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 10
Tracking performance after installation (CDC)
Make alignment and calibration constants.pt resolutionspatial resolution
Small cell
Normal cell
= 120 m
= 100 m
di-muon data sample.
pt/pt = 1.5%
CDC tracking system work well with having good resolution.
( before)
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 11
Search for Lepton Flavor Violating decays.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 12
In Standard Model, there is no Lepton Flavor Violation.Each lepton number is strongly conserved.
Recently neutrino oscillation has been observed.Although take into account neutrino oscillation, expected branching ratio of LFV in charged sector is B < 10-40.
2. Lepton Flavor Violation
レプトンフレーバー保存則 レプトンの世代を超える遷移を禁止
How strong is Lepton number? (Simple motivation)
If we find LFV, Direct evidence of New physics.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 13
LFV in BSM
If our sensitivity is O(10-7), reach MSSM level.
If m ~ 1 eV : B(→LFV)<10
B(→LFV)
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 14
Minimal Super-symmetric Standard Model
• Higgs mediated process
(1) Phase space → 2 body decay is bigger.(2) Color effect. → 3 times bigger.(3) Mass difference. → B / B ( ms/m ) 2
B → is 8 times bigger
than B →
A0:CP-odd neutral Higgs boson.
M. Sher, Phys.Rev.D66 05731(2002)K.S.Babu PRL,89,241802 (2002)A. Dedes, et.al. PLB 549,2442 (2002)
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 15
Purpose of this analysis.
We search for LFV tau decay using pair events of e+e annihilation process, as evidence beyond the Standard Model.
Signal modes : l M0
lepton pseudo-scalar meson
e
e
e ’
’
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 16
Previous experimental results• Using ee → process
Data : 4.26106 eventsEfficiency : → : 2.9% →0: 6.8% Background : → : 0ev. → 0: 0ev./0.5ev. (obs./exp.)
Number of events
MSSM
MARKII
ARGUS
CLEO
90%
C.L
. U. L
. on
Br
? This analysis N = 137
M
B() = 99%B() = 39%
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 17
3. Analysis
Procedure1 . Selection criteria
- High signal efficiency- BG suppression
2 . Signal extraction- e/ and ’- set signal box- BG estimation
3 . Determine branching ratio
(→ add subdecay mode for M0 .)
Blind Analysis method To avoid making vias into results,we shaded around signal region at very first level until end of BG estimation.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 18
Additional mode.
3.1 Signal event reconstruction
signal side ( e ’) + tag side (1 trk + n + missing.)
(e+)
・ recon. modes for ’
22.7%
39.4%
B MmodeType
→1 - 3
→1 - 1
1 - 1 → 98.8%
1 - 3 ’→ 17.5%
tag side: 1 prong decay
signal side : 1or 3 prong
Br(1 prong) = 84 %
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 19
3.2 BG suppression Level-1Bhabha, process
2 photon process
ee ~ 120 nb = 1 nb
eexx ~ 20 nbFeature: Large Cross section Low Pt. particles escape to Beam pipe. Rejection: pt, missing momentum towards acceptance.
Feature : Huge Cross section No missing momentum ↓ Rejection: e/ veto in tag side
Total Energy
signal : 5% loss : →1/45ee : →1/4900
These events account for 95%. → Reject at first level.
→ Rej. Factor : 1/10000
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 20
3.2 BG suppression Level-2
pair process
qq process
= 0.9 nb
qq = 4.2 nbFeature : Multi prong include ’ 。
Feature: Similar topology with signal Include e ・ Having large missing p.
sig : 2 % loss : 67% rej.uds: 65% rej.
Opening angle of l and M0.
veto for ’s Mtag < 1.777 GeV/c2
Rej. factor : 1/2900 .
→ Rej. Factor : 1/83000
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 21
3.2 BG suppression
• Hard to reject events : Main BG.
Level-1 Level-2Data -----
Bhabha 120nb nb
2photon nb qq 4.2nb nb
Need additional criterion to reject process
← :Can be reject.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 22
3.2 BG suppression - newly applying cut - Signal event : are only in tag side. process : are in both tag and signal side.
Having effective missing mass: mmissing become large.
black: signal MC Blue: generic
Signal event : 17% loss process : 95% reject.
2
Signal ev. process
Apply this cut :
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 23
3. Analysis
Procedure1 . Selection criteria
- High signal efficiency- BG suppression
2 . Signal extraction- e/ and ’- set signal box- BG estimation
3 . Determine branching ratio
Blind region also explained.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 24
3.3 Signal extraction – e/ and ’ –
109ev. 100±5.9
背景事象の構成 レプトンの誤識別: 全体の 80 % ( , を と間違える)
Lepton ID requirement for track.Invariant mass distribution.
Data: 57ev. MC : 48.1±4.0
0
-5 < M < 3
77ev. 81.6 ± 8.4
’
-3 < M ’ < 3
Good agreement are seen for sideband events.
Data: MC :
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 25
3.3 Signal event extraction
(a) Inv. mass Ml should be tau mass. Ml= E2
l p2l
(b) energy El should have beam energy. E = El – Ebeam
*
→ 信頼度の高い測定を行うため ブラインド・アナリシスを適用.
±10
±10
low=25±2 MeV/c2
hi=14±2 MeV/c2
low=57±4 MeV
hi=35±1 MeV
signal region : Elliptical shape which having efficiency of 90%. Shape is determined by minimize the area. S/N is improved 1.5 times than sqare shape
Blind region: 0.5< E < 0.5(GeV), 5 < Ml< 5
Blind region
signal event : Ml M=m, E=0
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 26
3.4 Background property(153.8, 428, 232fb-1)
- BG of muon modes are larger than electron modes. The fake rate of lepton ID.- There is no peaking BG around signal region.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 27
3.4 Background Estimation
Using sideband events. - Projection in each axis. - Fit BG events by
Gaussian and 3rd polynomial - Normarized by sideband events.
b0 =Func
Difference : 0.30 take account as systematic error
b0 =Flat
Try two pattern for BG function.
Flat distribution.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 28
3.5 Signal efficiency and BG events S/N
High signal efficiencyHigh BG suppression If B = , S/N=3~12 . → 3 observation can be achieved.
Open Blind.
are obtained
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 29
3.6 Results - Observed events ー5 ev.
1 ev.
1 ev.
0 ev. 0 ev. 0 ev.
0 ev. 0 ev.
BG expect 0.2±0.2 0.2±0.2 0.0±0.4 0.3±0.2
BG expect 3.9±1.2 0.6±0.4 3.0±0.8 0.9±0.4
# of observed events are consistent with estimation .→ Set upper limit on Branching ratio .
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 30
3.7 Systematic uncertainty
• Concerning to s0
→ BG estimation Difference of two pattern - If b0< 1, set b0=0 in order to obtain conservative limit.
B =
s0
2 N B0 effB =
Total: 30 ~ 66 %
• Concerning to sensitivityM0 recon. 2.0~4.0%Tracking 2.0%0 veto 0 or 5.5%e ID 1.0% ID 2.0%Trigger 0.5~0.7%Beam BG 2.1~2.3%MC model 0.5%MC stat. 0.8~1.7% Total: 4.2 ~ 8.6%
N 1.4%B0 0.7~3.4%
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 31
Upper limit on branching ratio ( 90 % C.L.)
•Upper limit evaluation (POisson Limit Estimator program)– Frequentist approach.
Systematic uncertainty: using the Gaussian error.J. Conrad et al., PRD 012002 (2003)
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 32
4. Discussion
First search result!
Efficiency : Add M0 recon. mode → Gain 1.5~1.7MSSM Higgs mediatedR-parity-V
Improve in efficiency and BG suppression from previous result. → Reach 10-7 level which is expected from MSSM.
Ldt # of BGCLEO 4.7 0.5→16Belle 154 3.0 ratio 32 1/5
CLEO
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 33
Constraint on tan vs mA
This limit is comparable with Energy frontier experiment, Tevatron
In tan> 50,mA > 110GeV/c2
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 34
Summary• Search for LFV decays e, , e, , e’, ’ using 137
106 pair events which are accumulated at KEKB-Belle experiment.
• Achievement : Improve sensitivity by 64 (max.)(1) # of : Using 32 times larger statistics.(2) Efficiency : Add recon. M0 mode . → Gain 1.5~1.7
→ First search for ’ mode.(3) BG : Newly missing cut apply →~ 5 times improve.(4) Reliability : Blind analysis
Apply two pattern in BG estimation.
• Result : No excess in signal region. Set 90% C.L. upper limit on branching ratio . The limits reach 10 level , put constraint on MSSM .
In tan> 50, mA > 110GeV/c2
→ Comparable sensitivity with Tevatron .
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 35
Backup
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 36
(1) # of pair (N)
(2) Signal detection efficiency (eff)
(3) Background
Suppression factor:1/108
BG estimation.
Remarkable points
s0
2 N ・ eff ・ BM0B = BM0 : Branching ratio of M0
s0 : # of signal eventsSensitivity:
→ Add reconstruction mode for M0
→ Reliability
Event selectioncriteria is
most important.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 37
For future, Super B-factory project.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 38
Status of LFV search in BelleNew result of this summer.
CLEOBabar
Belle Published Preliminary
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 39
Systematic uncertainty
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 40
Signal MC model dependence.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 41
Status for mu to e transition e
eX < 1011~12
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 42
Belle collaboration.• ~ 400 physicists from 59 institutions, 13 regions. • ~ 100 scientific papers were published.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 43
Belle detector.• General purpose detector.• Super conducting Magnet. (1.5T)
Belle control room
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 44
XT Curve & Max. Drift Time
Small cell
Normal cell
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 45
運動量測定 : 軌跡測定から pt/pt ~ 0.19pt 0.30/ %
光子 : 軌跡を伴わない ECL のヒット E /E = 1.8%@E=1GeV
CDC
ACC
ECL
TOF
r 平面
e+e → → ・ ・
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 46
We are here.
Official Goal
Installation of Crab Cavity
• 550 /fb will be reached before the Crab Cavity.• The Official Goal (=1 /ab) will be achieved before Summer 2007.
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 47
Installation of Crab Cavity
• Shutdown for 18-26 months in 2009-2010 for upgrade.• 0.6 /ab/month in 2020.
We are here.Shutdown
SuperKEKB
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 48
Motivation - l l l ’ - • In MSSM at large tan region may have large branching ra
tio by Higgs mediated process.
• Correlation between other mode– Br( 3l ) Br( ) ~ 0.2 – Br() Br( ) ~ 0.006– Br(’) Br( ) ~ 0.004
M. Sher, Phys.Rev.D66 05731(2002)K.S.Babu PRL,89,241802 (2002)A. Dedes, et.al. PLB 549,2442 (2002)
A.Brignole and A Rossi, hep-ph/0404211
The ratio could be a few times larger or smaller. It depend on radiative correction.
Our sensitivity reach this level.We can put constraint on tan and mA
backup
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 49
2.1 Selection criteria ( 1-3 prong + ’)– 1-3 prong + n2
E > 0.1 GeV , barrel and endcapptrk>0.06GeV/c barrel.ptrk >0.1GeV/c endcap.
net charge=0. dzrms < 1cm, drrms < 1cm to reject junk track.signal side: eID > 0.9 + 2trk(+,–).
– Missing momentum towards tag side.– pmiss vs. mmiss
2 2-D cut.– 0.5 < cos’ < 0.92– -3 < M < 3
using thrust axis, divide 2 hemisphere
for tag side, mtag < 1.777 GeV/c2
’
e/
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 50
2.2 Selection criteria (1-1 prong + )– 1-1 prong + n 2
signal side: eID > 0.9 + 2 . Pe>0.7GeV/c, E > 0.22GeV– 0 veto for ’s tag side:– NOT (e)– Mtag < 1.777 GeV/c2
Kinematical cut.– Missing momentum towards tag side.– pmiss vs. mmiss
2 2-D cut.– 0.5 < cos’ < 0.92– -5 < M < 3
e/
Seminar@Fermi Lab, 2005.6.19 Search for LFV decays at Belle, Y. Enari 51
3.0 過去の実験
• ee → で生成されたレプトンを使用
信号領域に検出事象はなかった. →検出効率3~5%.背景事象の抑制率は 1/106 .
対事象の数
MSSM からの予想
MARKII
ARGUS
CLEO
崩壊分岐比の上限値
DELPHI
?