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CP Violation and B-factory Experiments KEK and JSPS M. Kobayashi 2010/05/28

CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

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Page 1: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

CP Violation

and

B-factory Experiments

KEK and JSPSM. Kobayashi

2010/05/28

Page 2: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

Discovery of Antiparticle

Special Relativity (1905)Quantum Mechanics (1925)

1928 Dirac Dirac equation

Antiparticle

1932 Anderson Discovery of Positron

Relativistic Quantum Field Theory

Every particle has its corresponding antiparticle

• same mass• opposite charge

Page 3: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

Discovery of Parity Violation

1956 Lee, Yang

1957 Wu

e

-6060eNiCo

V-A Theory

• P and C are violated

• Still CP is conserved

Page 4: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

Discovery of CP violation

1964 Cronin, Fitch et al

~0.2% of KL decay into LK

LL KKCP CP

'2

'

00

00

00

S

L

S

L

KA

KA

KA

KA

3

3

1065.1/'Re

1023.2

Page 5: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

1973 Kobayashi, Maskawa

Standard Model

6-Quark Model for CP Violation

b

t

s

c

d

u

b

s

d

VVV

VVV

VVV

b

s

d

tbtstd

cbcscd

ubusud

11

21

21

23

22

32

AiA

A

iA

VVV

VVV

VVV

tbtstd

cbcscd

ubusud

Wu

b

Complex Coupling Constant

Page 6: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

Why do complex coupling constants violate CP?

• Coupling Constants

particle antiparticle

*g *g

xHxt

i

• Schrodinger Equation

/iEte

Page 7: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

• 1974 discovery of J/

• 1975 discovery of t -lepton

• 1977 discovery of U

c-quark

b-quark

• 1995 discovery of t-quark

Large CP asymmetry in the B-meson system

Sd KJB /Sd KJB /

Asymmetry in decay time distribution

Page 8: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

dd BBee

e

e

BorB

tagFlavor

/J

SK

z

B B

c/zt 0

Page 9: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

E(e)=8GeV,

E(e)=3.5GeVFinite angle beam crossing

E(e)=9GeV, E(e)=3.1GeV

Zero angle beam crossing

Governmental Approval

Experiment

Feature

1994 1993

May 1999 –still running

May 1999 –Apr. 2008

Page 10: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe
Page 11: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe
Page 12: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe
Page 13: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe
Page 14: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe
Page 15: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe
Page 16: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

1234 sec101.2 KEKB cmL

1234 sec102.1 II-PEP cmL

Page 17: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

KLM (m / KL detection)14/15 lyr. RPC+Fe

CDC (drift chamber)Tracking + dE/dxsmall cell + He/C2H5

ECL CsI(Tl) 16X0

ACC (Aerogel Cherenkov counter)

TOF (plastic scintillator bars)

SVD (Si vtx. det. 3 lyr. DSSD)

SC solenoid

1.5T

8GeV e

3.5GeV e

Page 18: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe
Page 19: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

BABAR layoutInstrumented Flux Return19 layers of RPCs 1.5 T Solenoid

Cherenkov Detector(DIRC)144 synthetic fused silica bars~11000 PMTs

Drift Chamber40 layers (24 stereo)

ElectromagneticCalorimeter6580 CsI crystals

Silicon Vertex Detector5 layers of double sided silicon strips

The BaBar detector

e–(9.0 GeV)

e+(3.1 GeV)

Page 20: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe
Page 21: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe
Page 22: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe
Page 23: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

Belle, July 05

B0J/KS B0

J/KS

Page 25: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

Present status of CP violation

• The Standard Model explains the dominant part of CP violation in both K-mesons and B-mesons.

• The Standard Model, however, cannot explain the matter dominance of the Universe.There will be yet unknown particles and unknownCP violating interactions.

• Hints of slight deviation from the Standard Model are observed in the B-factory experiments.

Page 26: CP Violation and B-factory Experiments · 2010. 6. 14. · CP violation in both K-mesons and B-mesons. •The Standard Model, however, cannot explain the matter dominance of the Universe

Congratulations for

• the great accomplishment of SLAC and KEK in construction and operation of the B-factorieswith the luminosity of the record high,

• the success of BaBar and Belle in verifyingthe CP violation mechanism of the Standard Model.