arXiv:1005.3288 submitted to Phys. Rev. D

15
arXiv:1005.3288 submitted to Phys. Rev. D

description

arXiv:1005.3288 submitted to Phys. Rev. D. Motivation. ℓ -. V ub. W -. q. u. b. B.  , . ¯. q. q. ¯. β known within 1º. ¯. Data sample: 377 million BB pairs. Motivation. ℓ -. V ub. W -. q. u. b. B.  , . ¯. q. q. ¯. | V ub | uncertainty. ¯. - PowerPoint PPT Presentation

Transcript of arXiv:1005.3288 submitted to Phys. Rev. D

Page 1: arXiv:1005.3288 submitted to  Phys. Rev. D

arXiv:1005.3288 submitted to Phys. Rev. D

Page 2: arXiv:1005.3288 submitted to  Phys. Rev. D

ICHEP 24 July 2010 W. Wulsin, B→(π/ρ)ℓν at BaBar 2

Motivation

b u

ℓ-

B ,

Vub

q

W-

β known within 1º

Data sample: 377 million BB pairs

¯

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ICHEP 24 July 2010 W. Wulsin, B→(π/ρ)ℓν at BaBar 3

|Vub

| uncertainty

Motivation

b u

ℓ-

B ,

Vub

q

W-

Data sample: 377 million BB pairs

¯

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ICHEP 24 July 2010 W. Wulsin, B→(π/ρ)ℓν at BaBar 4

Sample components

• Signal: very small relative to bkgd.

• B→Xu

lν (Xu

≠ π,ρ): similar to signal

• other BB: B→Xclν control samples used as cross-check

• e+e-→qq (q=u,d,s,c) continuum: off-resonance data used to correct fit variable shapes

Signal candidate selectionUntagged

non-signal B is not

reconstructed

Y(4S)

e+ e-

Bsignal

Xu

= , →

X1

X2

Xn

Bgeneric

B0→π-ℓ+ after preselection

¯

¯

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ICHEP 24 July 2010 W. Wulsin, B→(π/ρ)ℓν at BaBar 5

Neural net background suppression• Neural nets trained against each of 3 backgrounds, in each q2 bin• Sample plots shown for B0→-ℓ+ in 3 selected q2 bins

0<q2<4 GeV2

Continuum background

Jet-like events differ from isotropic B

decays

B→Xclν background

largest background,

Γ(b→clν) ~ 50×Γ(b→ulν)

B→Xu

lν background

Mostly at high q2,

hard to separate

4<q2<8 GeV2 20 GeV2 <q2 signal

B→Xu

other BB

qq

¯

¯cut cut

cut

B0→-ℓ+ S/B before NN = 3%

B0→-ℓ+ S/B after NN = 12%

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ICHEP 24 July 2010 W. Wulsin, B→(π/ρ)ℓν at BaBar 6

B→ℓ yields

Low q2 Mid q2 High q2

2

s

s

ppE Bbeams

Signal peaks at ΔE = 0

Signal peaks at

mES

≈ mB

= 5.28 GeV/c2

2

22/

Bbeams

BbeamsES p

E

ppsm

Backgrounds vary with q2.

Single mode yields

4-mode yield used to find BF

σstat

= 3.5%; σsyst

= 5.0%; σtot

= 6.1%

signal

B→Xu

other BB

qq

¯

¯

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ICHEP 24 July 2010 W. Wulsin, B→(π/ρ)ℓν at BaBar 7

B→ρℓ yields

Large B→Xu

lν background is highly

correlated with signal and must be fixed in

the fit.

Smaller yield than

B→πlν

σstat

= 8.6%; σsyst

= 15%; σtot

= 18%

signal

B→Xu

other BB

qq

¯

¯

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ICHEP 24 July 2010 W. Wulsin, B→(π/ρ)ℓν at BaBar 8

Shaded band indicates uncertainty on BGL fit.

Form factor parameterizations

All 4 parameterizations agree with each other and are consistent with the

data.

q2 spectrum corrected for detector efficiency &

resolution, bremsstrahlung, and radiative effects

• BCL and BGL expansions avoid ad hoc assumptions and are

based on fundamental QCD concepts.

• We use BGL 3-parameter fit as default (consistent with BGL

2-parameters).

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ICHEP 24 July 2010 W. Wulsin, B→(π/ρ)ℓν at BaBar 9

• Probabilities exclude theory errors and use

full q2 range.

• Calculations valid only for partial q2 range.

Theory curves scaled to area of

the data.

Comparison with theory

Errors too large to distinguish between B→ρℓ

predictions.

LCSR

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ICHEP 24 July 2010 W. Wulsin, B→(π/ρ)ℓν at BaBar 10

Theory needed to calculate

form factor.

• Probabilities exclude theory errors and use

full q2 range.

• Calculations valid only for partial q2 range.

|Vub| from partial q2 range

σexp

= 3-5%; σthy

= ~15%

Theory error dominates

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ICHEP 24 July 2010 W. Wulsin, B→(π/ρ)ℓν at BaBar 11

|Vub| from full q2 range

Simultaneous fit to data and theory

• 3 parameters: BGL quadratic polynomial

• 4th parameter: relative normalization between theory and

data, α |Vub

|2

• Theory points are correlated, so not all are used in fit.

σ(data BF) = 3%

σ(data q2 shape) = 5%

σ(theory FF norm.) = 8.5%

σtotal

= 10.5%

Errors reduced compared to

|Vub

| from partial q2 range

PRD 79, 054507 (2009)

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UT Fit Values

✚ average exclusive

average inclusive

Global “all other” fit =

(3.48 ± 0.16) × 10-3

Conclusion• Most precise branching fraction measurements:

– BF(B0→-ℓ+) = (1.41 ± 0.05 ± 0.07) × 10-4

– BF(B0→ρ-ℓ+) = (1.75 ± 0.15 ± 0.27) × 10-4

• Tests of q2 spectrum agreement with theoretical predictions.

• Determination of |Vub

|:

• LCSR, low q2 = (3.63 ± 0.12 +0.59-0.40

) × 10-3

• HPQCD, high q2 = (3.21 ± 0.17 +0.55-0.36

) × 10-3

• FNAL/MILC, full q2 = (2.95 ± 0.31) × 10-3

BF(B0→-ℓ+) [× 10-4]

BF(B0→ρ-ℓ+) [× 10-4]

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Backup

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Form factor parameterizations

Red-highlighted variables vary in the fit.

¯

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Systematic uncertaintiesFrom combined 4-mode fit