b s signal selection

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B s signal selection Donatella Lucchesi University and INFN Padova for B s Mixing group CDF Collaboration Meeting June 7, 2006

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B s signal selection. Donatella Lucchesi University and INFN Padova for B s Mixing group. CDF Collaboration Meeting June 7, 2006. The Blessed Selections: hadronic decays. Signal B s D s  D s . B s D s  D s  KK D s K *0 K K *0 K D s 3 B s D s 3 - PowerPoint PPT Presentation

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Page 1: B s  signal selection

Bs signal selection

Donatella Lucchesi University and INFN Padova

forBs Mixing group

CDF Collaboration MeetingJune 7, 2006

Page 2: B s  signal selection

June 7,2006 Donatella Lucchesi 2

The Blessed Selections: hadronic decays

BsDs Ds KK Ds K*0K K*0 K Ds 3BsDs3 Ds Ds K*0K

Signal BsDs Ds

Partially reconstructed B mesons

Combinatorial backgroundB0 D-

Page 3: B s  signal selection

June 7,2006 Donatella Lucchesi 3

Hadronic Bs decays summary

Decay channel Yield

BsDs Ds 1587

BsDs Ds K*0K 762

BsDs Ds 3 627

BsDs3 Ds 428

BsDs3 Ds K*0K 200

Total 3604

B+ D0 ~ 26,000

B0 D- ~ 22,000

Page 4: B s  signal selection

June 7,2006 Donatella Lucchesi 4

Blessed selection Bs semileptonic Decays

BsDsX Ds KK Ds K*0K K*0 K Ds 3

Total yield: Dsl ~37,000 events

Page 5: B s  signal selection

June 7,2006 Donatella Lucchesi 5

What can we do to improve it?

Include PID in the selection

Use NN to discriminate signal from background

Add new decay modes

Page 6: B s  signal selection

June 7,2006 Donatella Lucchesi 6

Including PID in the selections

BsDs Ds K*0K K*0 K has reflection from B0D D K when you give K mass to

A. Heijboer Standard analysis useD+ veto: |MK– MD+|>24 MeV

Page 7: B s  signal selection

June 7,2006 Donatella Lucchesi 7

Including PID in the selections

Aart proposal:|MK– MD+|>18 MeV OR CCL0 19.223.0Give this to NN

A. Heijboer

LR cut event by eventincreases Ds 1640In progress the Bs

significance evaluation

J. Mulmestadt

BSS/

Johannes idea:

BSS/

Page 8: B s  signal selection

June 7,2006 Donatella Lucchesi 8

Neural Network selectionsB. Casal, K. Anikeev

Use ROOTSNNS v3.0 Train NN to separate signal from bckg (side bands) Optimize to maximize Fit mass distribution using the actual mixing fitter

Rectangular cuts NN cuts

Increase 33% like adding 78% of more data

BSS/

BSS/

Page 9: B s  signal selection

June 7,2006 Donatella Lucchesi 9

Neural Network selections summary

B. Casal, K. Anikeev

Use wrong charge events as background in the future?

57.78/43.30=1.3 improvement A

Page 10: B s  signal selection

June 7,2006 Donatella Lucchesi 10

Partially Reconstructed B

BD, D*D*D/ treated as hadronic? Large yields (same order of fully reconstructed)

High k-factor, lose soft /

Lower S/B

Different K def. investigatedfinally use the standard one

Jeff Miles

Kp

MLct reco

T

PDGxy

Depend on mass

Page 11: B s  signal selection

June 7,2006 Donatella Lucchesi 11

Partially Reconstructed B

B0D* -[D0 -] +

Kp

mLct

T

Bxy

*

***

**

*

xy

xy

B

B

T

T

L

L

m

m

p

pK

Above 5.17 GeV D* and D*K

Low combinatorial background

5.00 <mass<5.35 GeV/c2

c 2= 464.6 +14.2 –13.5

m

Amanda Deisher

Page 12: B s  signal selection

June 7,2006 Donatella Lucchesi 12

New Decay Modes

BsDs Ds KsK Ks has reflection from

B0D D 3 as for Ds K*0K K*0 K Different topology easy to separate

Simone Pagan Griso

16% increase

~270 events 1fb-1

BSS/

Using PID

Page 13: B s  signal selection

June 7,2006 Donatella Lucchesi 13

Semileptonic decay modesV. Tiwari, G. Gomez-Ceballos

Improve event selection including PID BsDslx:

Dscombinatorial bck reduce by factor

2 Ds K*K yield increased by factor ~2.5

and combinatorial bck reduced by factor 2 Include l+SVT dataset Remove the ct* cut Noticeable

gain

Page 14: B s  signal selection

June 7,2006 Donatella Lucchesi 14

Summary

The number of events can be increased by includingnew decay modes, partially reconstructed eventsand by optimizing cuts.

Plan for the summer:Include partially reconstructed modes and optimize cuts.The actual gain on ms significance will be the combination of all the effect. Expected improvements on A:o 1.3 for the hadronic decay modes cuts optimizationo “Something” for semileptonic decayso Under evaluation for adding partially reconstructed hadronic decay