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Future Prospects for B Physics at a Super B Factory

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Future Prospects for B Physics at a Super B Factory. Hitoshi Yamamoto. Tohoku University ... Underlining mechanism by new physics implied. Why 3 generations? ... – PowerPoint PPT presentation

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Title: Future Prospects for B Physics at a Super B Factory


1
Future Prospects for B Physics at a Super B
Factory
M. Hazumi M. Yamauchi T. Browder and many others
Thanks to
  • Hitoshi Yamamoto
  • Tohoku University
  • DIF06, Frascati, March 2, 2006

2
We have done quite well so far ...
PEPII,KEK-B both exceeded design lum. 0.8
ab-1total
3
Main Aim of B-factories To test the CKM
mechanism of CPV
CPV by the irreducible complex phases in quark-W
coupling
V CKM matrix
Unitarity of V (Unitarity triangle)
Measure the sides and angles in different modes
4
Status of Unitarity Triangle
(Normalized to the length of the bottom)
Summer 2005
Lines by sin2b, eK, Vub/Vcb. a, g, and Dms,d
all cross at a single point!
Striking confirmation of the CKM paradigm. A
part of SM.
5
Problems of Standard Model
  • Quadratic divergence of Higgs mass correction.
  • Indicates new physics in TeV scale.
  • SUSY? Little Higgs?
  • Pattern of CKM matrix is not explained.
  • Underlining mechanism by new physics implied.
  • Why 3 generations?
  • Cannot explain the matter excess of universe.
  • CKM not enough. Other source of CPV implied.
  • Does not have dark matter candidates
  • WMAP 1/4 of universe is dark matter
  • Implies new particles (e.g. SUSY has).

6
New Physics New Flavor Structure
  • Standard Model quark-W coupling
  • Left-handed coupling only
  • Pattern of Cabibbo suppressions in CKM matrix
  • No additional CPV phases
  • New flavor structures
  • Could be right-handed
  • Pattern of mixing matrix element different from
    CKM
  • New CPV phases

High-luminosity Flavor physics
Mass matrix (general)
Energy frontiers (LHC, ILC)
7
For example MSSM
Down type squark mass matrix
Super B factory
8
Need for a Super B Factory
  • New flavor physics would be likely to appear in
    loops of b?s,d transitions.
  • B?s,d transitions currently limited by
    statistics.
  • Increasing the statistics by 100 (thereby
    reducing the error by 1/10) is imperative.
  • ? Super B-factory.
  • Preparations/studies underway in Japan, US, and
    Europe.

9
Super KEK-B
  • Luminosity 41035/cm2s
  • 40KEKB design luminosity (25achieved peak)
  • 5109 BB pairs/yr
  • 4109 tt pairs/yr, 5109 cc pairs/yr
  • A super B factory is a super tau-charm factory
  • LOI in 2004
  • http//belle.kek.jp/superb/loi
  • Physics at Super B Factory hep-ex/0406071
  • Official Budget request submitted to Japanese
    government in Aug 2005.
  • (Not approved yet)

10
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11
In order to increase the luminosity. . .
12
Super KEK-B Upgrades
Interaction Region Crab crossing q30mrad. by
3mm New QCS
New Beam pipe
More RF power
Damping ring
Linac upgrade
13
Probes for New Flavor Structure
  • New CPV phase in b?sqq
  • Time-dependent CPV analsysis (tCPV)
  • Right-handed current in b?sg
  • tCPV
  • Lepton AFB in b?sll
  • LFV in t decays
  • Charged Higgs in B ? Dtn, tn
  • ...and many more
  • (b?snn, mm, nn, gg ....)

14
Time-dependent decay distribution on Y4S
H. Miyake
A
S
A -C
S Dtasymmetry, A tag area difference
15
Current status of b?sqq
S - xfsin2f1 for J/YKS,L (xf CP
eigenvalue) Define sin2f1eff - xfS D sin2f1eff
sin2f1eff -sin2f1
16
b?sqq at Super B Factory
summer 2005
50ab-1
assuming present WA
?S(fKs) at 50ab-1 XX ?0.03(stat) ? 0.01(syst)
?0.04(th)
17
fKs
How can it constrain theories?
Summer 2005
Mass matrix elements between and are
constrained.
based on S.Khalil and E.Kou PRD67, 055009
(2003) and SuperKEKB LoI
18
fKs
Theory may need some mechanism to explain
suppressed d or f
19
Right-handed current in b?sg
  • In SM, s is left-handed ? g is left-handed.
  • In the
    CP conjugate mode,

  • g is right-handed.

  • Flavor-specific ?no tCPV.

  • (suppression factor ms/mb)
  • In BSM, s may be right handed.
  • ? tCPV
  • LRSM, SUSY, Randall-Sundrum, etc.
  • LRSM SU(2)L?SU(2)R?U(1)
  • S0.5 is allowed

s
g
b
X
X
20
tCPV in B? Ksp0g
Belle (386M BB pairs) use Ks vertex for Dt
S 0.080.410.10 (MXlt1.8 GeV)
consistent with zero
SM S -2 ms/mb sin2f1 0
21
CPV in b g s and SUSY models (Super B)
S(Ksp0)Kg error 0.5(now) ? 0.14(5ab-1)
T.Goto, Y.Okada, Y.Shimizu,T.Shindou, M.Tanaka
(2002, 2004) SuperKEKB LoI
Expected precision at 5ab-1
  • Correlations are useful to differentiate new
    physics models

22
AFB(ll) in b?sll
Polarization of ll system (or whatever is
creating it) L/R couplings to l ? AFB(ll)
l
l -
b quark
s quark
?
sensitive to new physics SUSY, heavy Higgs and
extra dim.
SM and SUSY models
AFB
SM also has large Asymmetry Z-g interference
S(ll) q2
23
AFB(ll) in b?sll Sensitivities
Sensitivity at Super KEKB
Experimental results with 0.35 ab-1
Belle, 2005
Standard model
MC, 50 ab-1
Zero-crossing q2 for AFB will be determined
with 5 error.
Belle, 2005
Control sample B?Kll Helicity(ll system) 0 ?
No FB asymmetry.
24
AFB(ll) in b?sll now
G(q2,cosq) function of A7, A9, A10
These (radical) models are already excluded by
recent data from Belle.
25
Search for LFV in t decays
  • SUSY Seesaw, or GUT
  • Large LFV possible

Br(t?mg)O(10-79)
mSUGRA
26
Search for LFV in t decays
Well within range!
SUSY t?mg
Present limit
Super-B limit
t?lg
t?lp/h/h
t?3l
t?l Ks
t?Bg/p
Gaugino mass 200GeV
27
More tests of SUSY breaking scenarios
T.Goto, Y.Okada, Y.Shimizu,T.Shindou, M.Tanaka
(2002, 2004) SuperKEKB LoI
28
Sensitivity for Charged Higgs
Constraint from B?Xs g
B?Dtn
D(Form-factor) 5
D(Form-factor) 15
B?tn (present)
LHC 100fb-1
29
Unitarity triangle at 50ab-1
It may not close. Something new in loops!
Triangle closes, or...
30
DNA Identification of BSMby Flavor Physics
Unitarity triangle
Rare decays
Bd- unitarity e D m(Bs) B-gtfKs B-gtMsg indirect CP b-gtsg direct CP
mSUGRA - - - - -
SU(5)SUSY GUT nR (degenerate) - - -
SU(5)SUSY GUT nR (non-degenerate) - -
U(2) Flavor symmetry
Large, sizable, - small
Okada et al (2004).
31
Comparison with LHCb
SuperKEKB
5ab-1
50ab-1
LHCb 2fb-1
CPV (b g s)
FCNC
w/ n
CKM
32
Advantages of Super B Factory
  • B decays with neutrinos B g Dtn, tn, uln
    etc.
  • B decays with g, p0 B g Xsg, p0p0 etc.
  • B vertex reconstruction with Ks only !
  • B g Ksp0, Ksp0g etc.

Dtn etc.
B meson beam !
B
e- (8GeV)
e(3.5GeV)
?(4S)
p
B
full (0.10.3) reconstruction BgDp etc.
33
Summary
  • B-factories have been successful, and now
    beginning to probe new physics.
  • Many new physics are well within reach of Super B
    factory.
  • Super B factory can distinguish various BSM
    models.
  • New particles that would be discovered at LHC/ILC
    will be tested/measured in their flavor sector.
  • Super B factory is sensitive to mass scale beyond
    the reach of LHC/ILC.

34
Back Ups
35
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36
Hint of Problems?
Limited by statistics at the moment.
37
Direct CP Violation
38
Projection of integrated luminosity
  • Crab cavity installation in 2006
  • 2?109 BB pairs by 2008 (4?now)
  • Long shutdown (14months) in 2009-2010
  • Constant improvement from 2010
  • realistic and reliable plan based on experiences
    at KEKB
  • Crab cavities well tested before 2010 a big
    advantage !

39
Bkg TRG rate in future
x20 Bkg
KEKB SuperB
Luminosity (1034cm-2sec-1) 1 40
HER curr. (A) LER curr. (A) vacuum (10-7Pa) 1.2 1.6 1.5 4.1 9.4 5
Bkg increase - x 20
TRG rate (kHz) phys. origin Bkg origin 0.4 0.2 0.2 14 10 4
x10 Bkg
KEKB Bkg
SVD
CDC
PID / ECL
KLM
Synchrotron radiation Beam-gas scattering (inc.
intra-beam scattering) Radiative Bhabha
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