Recent b physics results from OPAL David Waller, Carleton University for the OPAL Collaboration EPS...

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Recent b physics results from OPAL David Waller, Carleton University for the OPAL Collaboration EPS Conference HEP2003 Heavy Flavour Physics Session Aachen, Germany 17 July 2003

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July 17, 2003EPS Conference D. Waller/Carleton U.3 Semileptonic decay of b hadrons to orbitally excited D mesons Measure D **0 are L=1 orbitally excited charm mesons. –Measure narrow J q = 3/2 states (D 1 0, D 2 *0 ). –Wide J q = 1/2 states not visible with statistics. Reconcile difference between measured inclusive and exclusive semileptonic branching ratios. Reduce uncertainty in |V cb |. Test HQET predictions. Object Motivation

Transcript of Recent b physics results from OPAL David Waller, Carleton University for the OPAL Collaboration EPS...

Page 1: Recent b physics results from OPAL David Waller, Carleton University for the OPAL Collaboration EPS Conference HEP2003 Heavy Flavour Physics Session Aachen,

Recent b physics results from OPAL

David Waller, Carleton University for the OPAL Collaboration

EPS Conference HEP2003 Heavy Flavour Physics Session

Aachen, Germany 17 July 2003

Page 2: Recent b physics results from OPAL David Waller, Carleton University for the OPAL Collaboration EPS Conference HEP2003 Heavy Flavour Physics Session Aachen,

July 17, 2003 EPS Conference D. Waller/Carleton U. 2

Outline•

– Object, motivation– Method– Results

• Charm counting in beauty decays– Object, motivation– Method– Results

• Conclusions

X)D b( *0*Br

Analyses of Z0 data!

Page 3: Recent b physics results from OPAL David Waller, Carleton University for the OPAL Collaboration EPS Conference HEP2003 Heavy Flavour Physics Session Aachen,

July 17, 2003 EPS Conference D. Waller/Carleton U. 3

Semileptonic decay of b hadrons to orbitally excited D mesons

• Measure • D**0 are L=1 orbitally excited

charm mesons.– Measure narrow Jq= 3/2

states (D10, D2

*0).

– Wide Jq= 1/2 states not visible with statistics.

• Reconcile difference between measured inclusive and exclusive semileptonic branching ratios.

• Reduce uncertainty in |Vcb|.• Test HQET predictions.

X)D b( *0*Br

Object Motivation

Page 4: Recent b physics results from OPAL David Waller, Carleton University for the OPAL Collaboration EPS Conference HEP2003 Heavy Flavour Physics Session Aachen,

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Semi-leptonic decay of b hadrons to orbitally excited D mesons: Method

• Identify high p lepton (,e)– high efficiency and purity for

p> 3 GeV/c, pe> 2 GeV/c• Exclusively reconstruct D**0

D**0 D*+ **- D0 +

slow

K-+(+ -)• Background cuts to remove

fake **- ( from fragmentation)– main background from

decays plus fake **-

– ANN (p, pT, d0/σd0) to select **-

XD b *0

3 mm

Page 5: Recent b physics results from OPAL David Waller, Carleton University for the OPAL Collaboration EPS Conference HEP2003 Heavy Flavour Physics Session Aachen,

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D**0 – D*+ mass difference

Combine D0→ K and K3 channels to reduce uncertainty due to background.

Unbinned ML fit to determine number ofD1 and D2

* events (B.-W. Gaussian).

Number of wrong sign and right sign background events fit simultaneously.

Page 6: Recent b physics results from OPAL David Waller, Carleton University for the OPAL Collaboration EPS Conference HEP2003 Heavy Flavour Physics Session Aachen,

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Results for X)D b( *0*

Br

3-

-*01

-01

10syst))(39.00.79(stat)(2.64

)πDD(X) DB()B(b

BrBrBr

C.L.) %95(101.4

)πDD(X) DB()B(b3-

-**02

-*02

BrBrBr

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Charm counting in b decays: Object and Motivation

• Object:(1) measure with inclusive method. (2) use to calculate average

number of c plus anti-c quarks per b quark decay, nc.

• Motivation: compare experimental value of nc to theoretical prediction:

nc = 1.20 ± 0.06 (Neubert & Sachrajda)

X)DD b( BrX)DD b( Br

charm) no b( - X))( b( X)DDb(1 BrccBrBrnc

Use PDG values

Page 8: Recent b physics results from OPAL David Waller, Carleton University for the OPAL Collaboration EPS Conference HEP2003 Heavy Flavour Physics Session Aachen,

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Charm counting in b decays: Inclusive method

• Differentiate b→1 charm from b→2 charm using topology.

• Impact parameter significance, S (=d0/σd0), of tracks from D decay greater than S of tracks from b decay.

• In b→2 charm most tracks from D decay.

• Combine S of tracks in jet into single joint probability variable: PJ

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Charm counting in b decays:Probability Density Functions and Fits

1 and 2 charm PDFs for –ln(PJ)for different track multiplicities (TM)

Hatched = 2 charmGreen = 1 charmRed = 0 charm, charmonium, bckgd

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Charm Counting in b decays: Results

• measured for each year separately.• Results for each year combined → consistent.

• Two dominant systematics from physics modelling: – charged particle multiplicity in fragmentation (±6.2%)– neutral K and multiplicities in D decays ( %)

• combined with and to yield nc. 11.0

10.012.1 cn

X)DD b( Br

X)DD b( Br)X)cc( b( Br

charm) no b( Br

)phys((det)3.2(stat) 10.0 X)DD b( 4.100.9

2.42.9-

Br

+7.2- 4.6

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Conclusion• Results of these recent OPAL charm counting and

analyses consistent with previous measurements and theoretical predictions.

this result:pink band

X)D b( *0*Br

01D

Semileptonic B decays to narrow L=1 D mesons

This result: 3-

-*01

-01

10syst))(39.00.79(stat)(2.64

)πDD(X) DB()B(b

BrBrBr

ALEPH (1997):

3-

-*01

-01

-

10syst))(52.00.85(stat)(3.73

)πDD() DB(

BrBr

3-

-*01

-01

10syst))(29.00.38(stat)(1.68

)πDD(X) DB(

BrBr

CLEO (1998):

*02D

This result:CL) (95% 104.1

)πDD(X) DB()B(b3-

-**02

-*02

BrBrBr

ALEPH (1997):

CL) (90% 106.1

)πDD() DB(3-

-**02

-*02

-

BrBr

CL) %95( 1029.1

)πDD(X) DB(3-

-**02

-*02

BrBr

CLEO (1998):

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Key variables

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Cross check of results

angle between **- and slow

in rest frame of D*+.

Signal peaks at higher |cos()|while background is flat.

peak sidebands

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Extra slide: charm counting