• No se han encontrado resultados

PPT Searches for Rare & Forbidden B and Charm decays with BaBar

N/A
N/A
Protected

Academic year: 2024

Share "PPT Searches for Rare & Forbidden B and Charm decays with BaBar"

Copied!
24
0
0

Texto completo

(1)

Study of B  Kππ γ decays at BaBar

Eugeni Graugés

Universitat de Barcelona

International Conference On High Energy

Physics: ICHEP2014 València

(2)

Outline:

– The BaBar Detector & Dataset – Introduction

– Event Selection and reconstruction – Analysis strategy

– Analysis of B + K + π - π + γ – Analysis of B 0  K 0 s π - π + γ – Results

– Conclusions All r esul

ts sh own her e ar e PR ELIM INA RY,

not yet pub lishe d (p ape r in prep arati on)

(3)
(4)

Dataset:

530/fb recorded in 9 years of operation :

Not only BB pairs:

690M cc pairs 500M τ τ pairs

~470M BB pairs but also:

7 x (Belle + Cleo) ϒ(3s)

0.5 x (Belle + Cleo) ϒ(2s)

(5)

– The BKππ γ is an effective FCNC b sγ

– Forbidden in the SM at tree level, they are very suppressed since they can only proceed via loop diagrams 

SM Branching Fractions (BF) of ~ 10

-5

-10

-6

– The presence of physics beyond the SM, could significantly change the BF’s, CP asymetries and the polarization of the decay photon

+ ?

Introduction:

(6)

– The photon polarization probes the V-A structure in the loop:

In the SM b (b-bar) decays in left-handed (right-handed) photon up to

~m

s

/m

b

≈2%

– The photon polarization can be accessed from the angular

distribution of the kaonic resonance decay into 3 bodies K

res

Kππ in B K

res

γ

Ref: Gronau, Grossman, Pirjol & Ryd

PRL88:0511802, 2002 & PRD66:054008, 2002

Introduction:

(7)

– NP particle may be present in the loop and enhance right-handed photons

– In the SM b sγ

L

or b sγ

R

 CP asymmetry parameters ~ 0

– NP presence  b sγ

L

or b sγ

R

 CP asymmetry parameters ≠ 0

– Time dependent CP asymmetry measurement

Introduction:

Objective: Measurement of S in B

0

 K

0s

ρ(π

-

π

+

) γ decays

(8)

Event selection & reconstruction

Signal B mesons:

Characterized kinematically by m

ES

and ∆E observables

 Good k/π separation

Background rejection:

Mainly qq continuum: e

+

e

-

qq (q=u,d,s,c);

supressed using a Fischer discriminant based on six variables that exploit the different event

topologies

 Background from other B decays: classified by kinematical and topological properties.

Different variables are then combined to be used into a maximum likelihood fit to both signal/bkg separation and to measure the physics

parameters of interest

(9)

Analysis strategy

Added challenge:

 Presence of irreducible contribution from from non CP-eigenstates

 Amplitude analysis required to extract the dilution factor

 The limited statistics prevent the amplitude analysis from the B

0

K

0s

π

-

π

+

γ channel.

 Therefore D is extracted from B

+

K

+

π

-

π

+

γ decays, assuming isospin symmetry

 The 4-body final state makes the boundaries of the (kπ-ππ) phase space to

vary event by event.

(10)

Analysis of B +  K + π - π + γ

a) Maximum likelihood fit to mES,

∆E and the Fischer a) Extraction

of the m

kππ

and m

spectra (using sPlot technique) a) Fit to m

kππ

and m

(projection) to extract

amplitudes  From the amplitudes, the dilution factor D and the BF’s are obtained

Preliminary Preliminary

Preliminary

Preliminary

(11)

Dilution factor from B +  K + π - π + γ

(12)

Results from B +  K + π - π + γ : BFs

(13)

Results from B +  K + π - π + γ : BFs

Several of this

measurements are to be the world best…,

or

measured for the first

time

(14)

Results from B 0 K 0 s π - π + γ : S

Ks ρ γ
(15)

Conclusions:

– BaBar stopped taking data in 2008, but the available dataset is still a very rich and

fruitful playground for physics analysis.

– All (preliminary) results shown agree with Standard Model predictions

– With the addition of larger samples (LHCb,

Belle-II) it should be possible to disentangle

whether or not there could be indications of

NP processes.

(16)

BACKUP

(17)
(18)
(19)
(20)
(21)
(22)
(23)
(24)

Referencias

Documento similar

Javakhishvili Tbilisi State University, Tbilisi; b High Energy Physics Institute, Tbilisi State University, Tbilisi, Georgia 52 II Physikalisches Institut,

Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan Institut de Física d’Altes Energies and Departament de Física de la Universitat Autònoma de Barcelona,

32 (a) Institute of High Energy Physics, Chinese Academy of Sciences, Beijing; (b) Department of Modern Physics, University of Science and Technology of China, Anhui; (c) Department

6 High Energy Physics Division, Argonne National Laboratory, Argonne, IL, United States of America 7 Department of Physics, University of Arizona, Tucson, AZ, United States of

Institute of High Energy Physics, Chinese Academy of Sciences, Beijing; (b) Department of Modern Physics, University of Science and Technology of China, Anhui; (c) Department

Institute of High Energy Physics, Chinese Academy of Sciences, Beijing; (b) Department of Modern Physics, University of Science and Technology of China, Anhui; (c) Department

33 (a) Institute of High Energy Physics, Chinese Academy of Sciences, Beijing, China; (b) Department of Modern Physics, University of Science and Technology of China, Hefei,

Department of Physics, Gazi University, Ankara, Turkey Division of Physics, TOBB University of Economics and Technology, Ankara, Turkey 3e Turkish Atomic Energy Authority,