semileptonic & rare charm decays

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Semileptonic & Rare Charm Decays Will E. Johns Vanderbilt University FPCP 2003, June 4

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Semileptonic & Rare Charm Decays. Will E. Johns Vanderbilt University FPCP 2003, June 4. Rare Charm Decays. Box and Penguin Diagrams are Smallish for Charm. Potential FCNC Decays are Suppressed. No Top Quuark in the loop. Short Distance. 10 -19. 10 -16. 10 -8. Rare Charm Decays. - PowerPoint PPT Presentation

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Page 1: Semileptonic & Rare   Charm Decays

Semileptonic & Rare Charm Decays

Will E. Johns

Vanderbilt University

FPCP 2003, June 4

Page 2: Semileptonic & Rare   Charm Decays

Rare Charm Decays Potential FCNC Decays are Suppressed

10-19

10-16 γγ)( oDBR

)( oDBR

10-8 )( DBR

Short Distance

Page 3: Semileptonic & Rare   Charm Decays

Rare Charm Decays

10-13

10-8 γγ)( oDBR

)( oDBR

10-6 )( DBR

Long Distance

Enhancement from Long Distance Effects

Even More room for decays:

X eX

Page 4: Semileptonic & Rare   Charm Decays

New Result from CDF oD

Use D* tagged Do’s

Use Similar Normalization Mode Very Similar Kinematics Keep cuts “same”

Need Anyway: - Background from Normalization ~(MISID)2 = (0.013)2 or (1/5 ev.)

The “MISID ZONE”

Back of the Envelope:

1.5E-3 (2.2/1371) = 2.4E-6

)()( 00 DBReff

eff

N

NDBR

RARE

NORM

NORM

RARE

)5.1/( BS Optimal:

)5.2cut( M

KSideband + (MISID)2

Page 5: Semileptonic & Rare   Charm Decays

•Expected background– events•Fake: •Combinatorial:

• 0 events in window

•New best limitBr < 2.4 x 10-6 at 90% CLBr < 3.1 x 10-6 at 95% CL

New Result from CDF oD

Background Sideband(Combinatorial Estimate)

Previous Bests: 4.1 x 10-6 at 90% CL (BEATRICE)4.2 x 10-6 at 90% CL (E771)

7.07.1 2.022.0

7.05.1

Page 6: Semileptonic & Rare   Charm Decays

New Result from CLEO oD

13.8 fb-1

Form D0 mass from 2 photons

(Cuts optimized on )oooD

MoM 3)(

Mass must be within of M(D0)M5.2

Veto candidate when extra photons form mass:

(reduces bkgnd from 4 to 1)oo

Find soft pion consistent with D momentum cuts and Particle ID

Form )()*( oDMDMQ

Fit data to Gaussian and threshold function

Gaussian width and center fixed from Monte Carlo

)(8.310.628 eventsoooD

)(3.92.19 eventsoD

Page 7: Semileptonic & Rare   Charm Decays

0094.00194.0)(

)(0

0

RARE

NORM

NORM

RARE

eff

eff

N

NooDBR

DBR

New Result from CLEO oD

Systematic error 13.1% from finding efficiencies, fits, MC stats, D selection, Event selection (added in quadrature with stat error for upper limit estimate)

90% ofProbability is above 0.0194

0.033

0.0194

(stat)

Sigma is total error

My toyexplanation

..%[email protected])(

)(0

0

LCooDBR

DBR

40 10)2.24.8()( Using ooDBR

..%[email protected])( 50 LCDBR

Phys. Rev. Lett. 90:101801, 2003hep-ex/0212045

Page 8: Semileptonic & Rare   Charm Decays

Final Results from FOCUS ),()( KD S

Look for 3 bodies with 2 muonsCut Grid, based on vertexing, Particle ID

L/ – vary from >5-21 Lp

s

ISO1 – CL DK’s in prim (vary <0.1 –0.001)

DCL – CL of DK vertex (>1 -- 4%)MuCL – CL for Muon ID (>1 – 10%)

Cuts on P( for ’s, Cerenkov for ’s and K’s

Loosest Cuts

Tightest cuts

Page 9: Semileptonic & Rare   Charm Decays

Final Results from FOCUS ),()( KD S

Systematic Check uses a single cut

(makes better plots!)

- First Bootstrap sets cuts for optimal Sensitivity (Blind)

- Second Bootstrap calculates quoted Sensitivity and Branching Ratio

Signal Excluded

D SD

Page 10: Semileptonic & Rare   Charm Decays

Final Results from FOCUS

Decay

Mode

Dual

Bootstrap

Sensitivity Sys.

Error

Result

W/sys

Single

Cut(w/sys)

Previous

(E791)

D+ ++- 9.1x10-6 7.5x10-6 7.5% 9.2x10-6 12x10-6 44x10-6

D+ -++ 13x10-6 4.8x10-6 7.5% 13x10-6 12x10-6 120x10-6

D+ ++- 8.8x10-6 7.6x10-6 7.5% 8.8x10-6 7.4x10-6 15x10-6

D+ -++ 4.9x10-6 5.6x10-6 7.5% 4.8x10-6 5.2x10-6 17x10-6

Ds+ ++- 3.3x10-5 3.3x10-5 27.5% 3.6x10-5 3.8x10-5 1.4x10-4

Ds+ -++ 1.3x10-5 2.1x10-5 27.5% 1.3x10-5 2.0x10-5 1.8x10-4

Ds+ ++- 2.4x10-5 3.1x10-5 27.5% 2.6x10-5 1.8x10-5 1.4x10-4

Ds+ -++ 2.6x10-5 2.3x10-5 27.5% 2.9x10-5 2.2x10-5 0.8x10-4

(E687)Dominated by PDG rate to normalizing mode

Final Results from FOCUS ),()( KD S

Page 11: Semileptonic & Rare   Charm Decays

Rare Decay Round-Up

OD

Closing in on Long rangeSM predictions

Sets MSSM constraint

Close to Long Distance Predictions

A 1st !

Lots of RoomAt the bottom!

Page 12: Semileptonic & Rare   Charm Decays

Semileptonic Charm Decays

022222

2

cossin4sin})cos1()cos1{(coscos

VVVdd

d

(D decay, No form factors, V decays to spin 0 particles)

Neutrino is left handed

Prefers W spin along muon,e

V products spinless

Prefer LZ=0

Form FactorsBaryons (spin ½)Scalar Resonance?

CP?

More than just CKM measurement tools…

)Asymmetry CP(

)M Factors, Form(

Factors) Form(

)(

)(,

)(

)(

ce)Interferen()(

0

Pole0

0*

0*

e

e

KD

D

D

KD

KD

KD

C

C

S

S

Page 13: Semileptonic & Rare   Charm Decays

FOCUS saw discrepancies in the data

2

20

2

2

2

5

0*

)(sincos2

)()cos1(sin

)()cos1(sin

coscos

obey) NOT Did(

0*

0*

0*

qHB

qHBe

qHBe

ddddqdm

d

KD

KV

K

iV

K

iV

Vk

Phys.Lett.B535:43-51, 2002hep-ex/0203031

Page 14: Semileptonic & Rare   Charm Decays

FOCUS added a term, things got better

2

20

2

2

2

5

)()(cossin2

)(sin)cos1(

)(sin)cos1(

coscos

0*

0*

0*

qHAeB

qHBe

qHBe

ddddqdm

d

i

KV

K

iV

K

iV

Vk

L=0 ansatz

Clean

The data(error bars)preferred theL=0 ansatz(solid) overno extra term(dashed)

Bkgnd

Page 15: Semileptonic & Rare   Charm Decays

FOCUS BR MeasurementsCuts similar to rare search:

even

ts /

5 M

eV/c

2

ISO1 ISO2 – No unused tracks consistent with charm vertex (CL < 0.1%)OoM – Charm vertex outside of target and silicon by Vertex3

)(

)(,

)(

)(0*

S

S

D

D

KD

KD

) cuts(/18.0}){(}){( 0*2 DDcGeVKMKM

KD 0*KD

SDSD

0*KD Includes S-wave interference

)(048.0)(033.054.0

)(

)(

sysstat

D

D

S

S

(1.5) 2.2,e)(quadratur Total

(0.94) 1.57, ff) (Bk,fit Vary

(1.12) 1.57, Samples Splitting

(1.06) 0.71, CutsVary

:)( for

offraction a as expressed

:errors Systematic

stat

SDD

(add in if > 1)

Phys.Lett.B540:25-32, 2002hep-ex/0206013

)(021.0)(010.0602.0

)(

)(0*

sysstat

KD

KD

Page 16: Semileptonic & Rare   Charm Decays

FOCUS Form Factors

and ,parameters waveS and)0(

)0(

)0(

)0( Fit to

)/1.2(,/1

)0()()/5.2(,

/1

)0()(

)(4)())((2

1)(

0set factor, has )()(2)()()(

1

22

1

222

2222

2

22

222

1222

2

20

22221

2

AA

Ar

A

Vr

cGeVMMq

VqVcGeVM

Mq

AqA

qAmM

KMqAmMqmM

qmqH

mqHqVmM

KMqAmMqH

v

VV

AA

ii

KD

DKDKD

K

tKD

DKD

Tried in fit,no sensitivity (E791?)

(common – vary generated parameters in Montecarloby using agreement with reconstructed distributions and data)

Pioneered by D.M. Schmidt for E691 K*ev analysis: NIM A 328 (1993)

0*KD

2max

2V /in 3 and in 3 ,cosin 5 ,cosin bins 5 qq

Kmin 4 and in 3 ,cosin 3 ,cosin bins 3 V

S-wave termBreaks symmetry

S-wave term andr’s essentially decouple

Page 17: Semileptonic & Rare   Charm Decays

FOCUS Form Factors 0*KD

Cuts similar to previous, some change to get uniform acceptance, one extra

OoM – Charm vertex outside of target and silicon by Vertex1Cut on q2 < 0.2 GeV2/c2 r’s are flat, feeling mμ? Goodness of fit issue

Right sign – Wrong sign

Charm Background

Systematic ChecksS-wave – varied cuts35 fits – Sample VarianceForm Factor (3 sources)1) Varied Cuts2) Split sample

3) Vary MC input Charm Backgrounds

)/9.0(2,, cGeVKD mDDP

2)0(

)0(2

1

3 A

A 064.0049.0875.02

039.0057.0504.1

)()(

05.007.068.0

015.0022.0330.0

r

r

sysstat

A

V

Phys.Lett.B544:89-96, 2002hep-ex/0207049

Page 18: Semileptonic & Rare   Charm Decays

CLEO Form Factors and CP eC0

Spin ½ Λ baryon adds a new wrinkle…

Körner and Krämer use supplementary definitions for X and the lepton angle

0,1,1,0,1,12

1

2

1

2

1

2

1

2

1

2

1

)}cos1(sinsincos)Re(

)cos1(sinsincos)Re(

)cos1(sin||

)cos1(sin||

)cos1()cos1((||

)cos1()cos1((|{|

coscos

22

3*

22

3*

24

32

24

32

28

32

28

32

2

4

12

102

1

12

102

1

02

1

02

1

12

1

12

1

WW

WW

W

W

W

W

W

HH

HH

H

H

H

H

ddddq

d

eC0

One pole mass describes the decay222

22

22 )/1(

/1

)()( PoleMax

Pole

Max MqMq

qfqf

Helicty H’s made from 2 form factors:

)0,( isspin

|)(||)(|expect

2

22

21

fsticky

qfqf

CBIntegrate over variables and look at asymmetries:

)cos1(cos2

2

Cddq

d(other choices possible)

(no sign change for particle and anti-particle)

Page 19: Semileptonic & Rare   Charm Decays

CLEO Form Factors and CP eC0

2

12

/)(10.0)(07.013.2

)(04.0)(05.031.0/

cGeVsysstatM

sysstatffR

pole

(To be sent to PRL)

Systematics: -Background Normalizations-Kinematic Closing-Fitting simulation-Efficiencies

KK

13.4 fb-1 from CLEO II and II.5

Look for Λe+ pairs where Λ→p π –

directionPFindP C )(?)( - Event thrust axis for direction- Try to close kinematics:

22

)( PPPP eC

(use fragmentation to break ambg)

(again the Schmidt meth)

Page 20: Semileptonic & Rare   Charm Decays

CLEO Form Factors and CP eC0

Page 21: Semileptonic & Rare   Charm Decays

Semileptonic Round-up

(From K. Stenson’s APS review)

0*KD

Interference effectsNeed other experiments to look Probably more in there…

Lowers by 5.5%

Page 22: Semileptonic & Rare   Charm Decays

Semileptonic Round-up

We all seem to agree!)(

)(

S

S

D

D eC0

No CP violation

expected toclose/ 12 ff

C Expect ~-1 from HQET

Good agreementin the Distributions

Page 23: Semileptonic & Rare   Charm Decays

I didn’t miss ‘em!

y)prelininar (Too CLEO

y)preliminar (Too CLEO

y)prelininar (Too CLEO *

py)Spectroscoin cover willChistov(Ruslan BELLE

0

0

0

S

eC

C

D

e

eKD

Would be nice to measure:

BARBARandBELLECDFfromDecaysRare

VDPD

KD

eKDeD ee

,

/

confirmed effects ceInterferen

,0*

00