Download - Belle results on Lepton Flavor Violation in tau decays

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Page 1: Belle results on Lepton Flavor Violation in tau decays

Belle results onLepton Flavor Violation

in tau decays

K. Inami (Nagoya Univ.)for Belle collaboration

Page 2: Belle results on Lepton Flavor Violation in tau decays

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B-factory at KEK

KEKB: e+(3.5 GeV) e-(8GeV)  

()~0.9nb, (bb)~1.1nb A B-factory is also a -factory!

Good track reconstruction and particle identifications

Belle Detector:

Lepton efficiency:90%Fake rate : O(0.1) % for e O(1)% for μ

Peak luminosity: 2.1x1034 cm-2s-1 World highest luminosity!

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Luminosity history

Belle is finished in 2010/6/30. Belle-II upgrade started. Analysis with full data sample is on going.

Integrated luminosity: >1000 fb-1 ⇒~109 BB and -pairs

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Lepton Flavor Violation in tau decaySUSY is the most popular candidate among new physics models

naturally induce LFV at one-loopdue to slepton mixing

l mode has the largest branching fractionin SUSY-Seesaw (or SUSY-GUT) models

ℓ~ e or~

~

LFV associated with a neutral Higgs boson (h/H/A)

Higgs coupling is proportional to mass ⇒ or ss (, ’ and so on) are favored and B.R. is enhanced more than that of .

When sleptons are much heavier than weak scale

2m

e or

Higgs (h/H/A)

ss

To distinguish which model is favored, all of decay modes are important.

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Analysis procedure

e+e+

(signal side)

1 prong + missing (tag side)

)( 22 pEm

CMbeam

CM EEE

Blind analysis Blind signal region⇒ Estimate number of BG in the signal regionusing sideband data and MC

Signal extraction: mE plane

e e

generic decay

3 ellipse: blinded region mm ~

0~E

Sideband region

Br~85%

Fully reconstructed

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LFV decays; Signal and Background

2photon process f=leptons,quarks

Neutrinos in both sideMissing energy in signal side

radiative Bhabha process

e+ e

eee

e

qq _

many tracks

signal

Neutrino(s) in tag sideParticle IDMass of mesons

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Analysis strategy

• Rare decay searches– Need to understand background and reduce as much as possible

• ℓℓℓ• ℓKs

• ℓV0(hh’)• ℓP0()• ℓhh’• ℓ

– Analyze the modes from simple selection to hard for background reduction

• Provide feedback to next analysis of similar final state

Difficulty ofreducing the background

Hard

Simple

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Search for 3leptons

• Data: 782fb-1

• No event is found in the signal region.

• Almost BG free– Because of good

lepton ID

• Br<(1.5-2.7)x10-8

at 90% CL.

Phys.Lett.B 687,139 (2010)

Mode (%) NBGEXP syst (%) UL (x10-8)

eee 6.0 0.21+-0.15 9.8 2.7 7.6 0.13+-0.06 7.4 2.1e 6.1 0.10+-0.04 9.5 2.7ee 9.3 0.04+-0.04 7.8 1.8e 10.1 0.02+-0.02 7.6 1.7ee 11.5 0.01+-0.01 7.7 1.5

ee+e + e+

e+e e+ e+e

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Search for ℓV

• Search with 854fb-1 data sample • Select one lepton and two hadrons• Require invariant mass to be a vector meson mass

The requirement reduces background rather easily.• Possible background

• For ℓ=, hadronic tau decay and qq with miss -ID• For ℓ=e, 2photon process could be large BG.• It turns out that not only 2photon process but also ee+X process

become large background. Reduced using missing-momentum direction

e+

e-

M

data

signalMC (e)

and qq MC

qq

(missing)

2photon BG

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Result for ℓV

Eff. NBGexp Nobs.

ULx10-

8

Eff. NBGexp Nobs.

ULx10-8

e 7.6% 0.29±0.15 0 1.8 eK*0 4.4% 0.39±0.14 0 3.2

7.1% 1.48±0.35 0 1.2 K*0 3.4% 0.53±0.20 1 7.2

e 4.2% 0.47±0.19 0 3.1 eK*0 4.4% 0.08±0.08 0 3.4

3.2% 0.06±0.06 1 8.4 K*0 3.6% 0.45±0.17 1 7.0

e 2.9% 0.30±0.14 0 4.8 2.4% 0.72±0.18 0 4.7

After event selection• 1 event , K*0, K*0

• 0 events others

No signal compared to expected BG

Br(ℓV0) < (1.2-8.4)x10-8

Expected number of background(0.1-1.5) events

Phys.Lett.B 699,251 (2011)

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Search for ℓhh’

• Update with 854fb-1 data– BaBar; Br<(7-48)x10-8 at 221fb-1

• 14 modes are investigated (h,h’= and )– →ℓ-h+h’-: 8 modes (lepton flavor violation)– →ℓ+h-h’-: 6 modes (lepton number violation)

e or

e e

e e

signal generic BGmiss-ID as

e e

ee

miss-ID as

Missing momentum can help to reject this kind of BGs since signal has only on tag side.

Also,qq eventscan be BG

signa

lsid

e

tag

side

Updated this summer

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Result for ℓhh’

予想される背景事象(0.1-1.5)events

Set upper limits at 90%CL: Br(ℓhh’)< (2.0-8.6)x10-8

(preliminary)

1event : in and no events: in other modes

⇒ no significant excess

In the signal region

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Upper limits on LFV decays

Updated this summerUnder studying with full data sample

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Effect to physics models

• Experimental results have already ruled out some parts of the parameter space.– Exclude large tan, small SUSY/Higgs mass

– Accessing other models and other parameter space

reference

SM+ mixing PRD45(1980)1908, EPJ C8(1999)513 10-40 10-14

SM + heavy Maj RPRD 66(2002)034008 10-9 10-10

Non-universal Z’ PLB 547(2002)252 10-9 10-8

SUSY SO(10) PRD 68(2003)033012 10-8 10-10

mSUGRA+seesaw PRD 66(2002)115013 10-7 10-9

SUSY Higgs PLB 566(2003)217 10-10 10-7

Undetectable

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Future prospects

Old estimation

New estimation

• Belle-II will produce >1010 tau leptons.

• Sensitivity depends on BG level.– Recent improvement of

the analysis(BG understanding, intelligent selection)

Improve achievable sensitivity

• B()~O(10-10) at 50ab-1

– Improvement of BG reduction is important.

• Beam BG• Signal resolution

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Summary

• Search for LFV decays using ~109 decays– 48 modes have been investigated.

• No evidence is observed yet.• Upper limits on branching ratio around O(10-8)

– B()<2.1x10-8, Br(V0) < (1.2-8.4)x10-8

– B(hh’) < (2.1-8.6)x10-8, Br(h) < (2.8-4.2)x10-8 etc.– Exploring some new-physics parameters space.

• Update /e with full data sample (~1000fb-1)• Optimization for BG reduction is important for future

experiment– Belle-II try to obtain the sensitivity of O(10-9~10).

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Result for ℓP0(=’)

Eff. %

NBGexp Nobs. UL

x10-8

8.2 0.63±0.37 0 3.6

6.9 0.23±0.23 0 8.6

comb 2.3

e 7.0 0.66±0.38 1 8.2

e 6.3 0.69±0.40 0 8.1

ecomb 4.4

’ 8.1% 0.00+0.16-0.00 0 10.0

’ 6.2% 0.59±0.41 0 6.6

’ comb

3.8

e’ 7.3% 0.63±0.45 0 9.4

e’ 7.5% 0.29±0.29 0 6.8

e’ comb

3.6

4.2% 0.64±0.32 0 2.7

e 4.7% 0.89±0.40 0 2.2

(2.1-4.4) times more stringent results than previous Belle result (401fb-1)

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eK*, eK*, e modes

Other BG for eK*, eK* and e ⇒ Event with conversion

   For example, eK*mode 0 with conversion from 0

τ-

-

0

e-

Fake K*e+ as miss KID

overlap dE/dx regionbetween e and K

data

P(K+) (GeV)

Mee w

ith e-K+

-conversion generic MC

eK* MC

Require large invariant mass of e+e- candidate, to reduce the BG

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Search for h

4 modes are searched for. (h=and K)• -→h-: (L-B) conserving decay• -→h-: (L-B) violating decay Current upper limits

• Belle Br<(7.2-14)x10-8 @ 154fb-1

• BaBar Br<(5.8-15)x10-8 @ 237fb-1update with 906fb-1

@Belle

(no search for K on Belle)

e e

signa

lsid

e

tag

side

p

signal

e eKs0

misid as e e

p

p

Generic BG qqBG

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BG rejection for h

To reduce BG including KS0

⇒ reconstruct KS0 and reject

eventsthat are likely to be KS

0

qq MC

A half of Ks0 BG events are rejected.

To reduce qqBG including ⇒ reject events with a proton in tag side(due to BN conservation, the eventsincluding a tend to have baryon on tag side.)

qq MC

p

A third of qq BG events are rejected.

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Results of h

no camdodate event are found ⇒ no significant excess

In the signal region

0000

2.32.22.22.1

Set upper limits@90%CL:Br()<2.8x10-8

Br()<3.1x10-8

Br()<3.0x10-8

Br()<4.2x10-8

(L-V) cons.

(L-V) viol.

Around x(2-3) improvementfrom the previous BaBar results

(preliminary)

(preliminary)