A. Drutskoy, ITEP, Moscow Recent results from Belle QFTHEP’ 2010, Golitsyno, Moscow, Russia, September 8-15, 2010 Mt.Tsukuba: Nyotai-san 877m, Nantai-san 871m QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy
Recent results from Belle. A. Drutskoy, ITEP, Moscow. Mt.Tsukuba: Nyotai-san 877m, Nantai-san 871m. QFTHEP’ 2010, Golitsyno, Moscow, Russia, September 8-15, 2010. - PowerPoint PPT Presentation
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A. Drutskoy, ITEP, Moscow
Recent results from Belle
QFTHEP’ 2010, Golitsyno, Moscow, Russia, September 8-15, 2010
Mt.Tsukuba:Nyotai-san 877m,Nantai-san 871m
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy
Belle detector
e+ source
cavity
Belle
3.5 GeV e + 8 GeV e
-
Belle detector and KEKB collider
Belle is general purpose detector with high efficiencyand accuracy charged track and photon reconstruction,good particle identification and precise vertex resolution.
KEKB is asymmetricenergy e+e- collider
2QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 3
Theories confirmed in B factories with high precision
1. Standard Model elements: quarks, leptons, photon, gluons, Z boson, W± bosons. No effects beyond Standard Model have been observed with >5 in particle physics.
2. Hadrons have fixed combinations of valence quarks: quark-antiquark pairs, or three quarks.
GOAL now: find effects contradicting to 1 or 2
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 4
How to search for BSM and exotics in B factories
1. Test unitarity of CKM matrix
It’s very smart and subtle method. Many BSM contributions will destroy unitarity. However it’s not easy to make predictions and conclusions.
2. Compare branching fractions and asymmetries of B, D, and decays obtained experimentally and predicted theoretically within SM. If Bf is unobservably small in SM => just search for such forbidden decays.
Look for hadrons with exotic masses, quantum numbers, decay rates anddecay final states.
Search for BSM:
Search for exotic hadrons:
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 5
CPV in B0 mixing and decays
t (decay time)[ps]
B0
B0 fcpfcpB0
B0
A
A
=mixing Decay: A
_A
1
2
3
Vtd Vtb
Vcd Vcb
Vud Vub*
*
*
f [S sin(md t ) + A cos(md
t )]
B0
B0_
sin 21
Pro
b.
ACP
S = sin
21
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 6
sin 2φ1 ≠ sin 2φ1eff
_
d
b_ c
csd
_wB0
J/ψ
K0 d
b_ _
sssd
_gtB0
K0
φ, f0
wb ccs tree
_b sqq penguin
_
S = sin2φ1, A ≈ 0 S = sin2φ1eff, A ≈ 0
In case of extra CP phasefrom NP in penguin loop
_
CP violation measurement in B0 K+ K–
KS0
Physics motivation for CP violation measurement in
b sqq transition
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 7
BSM contributions in b s penguin loop
SM Charged Higgs Chargino+squark 4-generation
Simplest BSM processes which could contribute in b->s loop
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 8
CP violation measurement in B0 K+ K–
KS0
Unfortunately 4 solutions were obtained for phases and amplitudes of signals.These 4 solutions are consistent with each other within statistical errors.First solution (preferable) was used to measure CP violating parameters.
B 0 KS
0K +K
– signal => 1176±5Background Continuum ~ 47%
Other B decays ~3%Significant part of signal K+K-KS
0 goes via intermediate -> K+ K- and f0->
K+K-
657 x 106 BB pairs at (4S)
KS0
f0(980)KS0
Dalitz-plot
s+ = M 2(K+KS
0)
s – =
M 2(K
–K
S0)
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 9
Belle preliminary, arXiv:1007.3848
fS1
eff = (31.3 ± 9.0 ± 3.4 ± 4.0)0 fS1
eff = (31.3 ± 9.0 ± 3.4 ± 4.0)0
S1
eff = (32.2 ± 9.0 ± 2.6 ± 1.4)0 S1
eff = (32.2 ± 9.0 ± 2.6 ± 1.4)0
BG
Third error accounts for uncertainty from Dalitz model.
SM prediction
0.30 0.29 0.11 0.09CPA = - ± ± ±
[solution #1]Belle preliminary, arXiv:1007.3848 657 x 106 BB pairs_
Only in the φmass region
Only in the φmass region
0.04 0.20 0.10 0.02CPA = + ± ± ±
1 (all charm, J/ K0 …) = (21.1 ±
0.9) 0
CP violation measurement in B0 K+ K–
KS0
S(all charm) = 0.673 ± 0.023 S( K0)
~ 0.9
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 10
Summary of New CPV search
All charm, B0-> J/K0 ...Reference point of SM
No clear deviation seenin all modes (1~2). Resultsare in agreement with SM.
New CPV effect can beseen with much larger data
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 11
Bellenew B0-> KS
Difference between Sin 21 in b -> ccs tree decays and b -> sqq penguin decays disappeared.
__
Physics motivation
.
• In SM interference between the tree and penguin diagrams can cause small direct CP violation in B+ -> J/ψK+ . SM: ACP (B+ -> J/ψK+) ≈ 0.3 %
• BSM contributions in b->s penguin loop can increase asymmetry
TreeBelle –2.6±2.2±1.7
Phys. Rev. D67, 032003 (2003)
BABAR +3.0±1.4±1.0Phys. Rev. Lett. 94, 141801 (2005)
D0 +0.75±0.61±0.30Phys. Rev. Lett. 100, 211802 (2008)
W/A +0.9±0.8 (PDG2009)
Previous measurementsof ACP (B+ -> J/ψK+) [%]
CP violation measurement in B+ J/ψ K+
Penguin
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 12
Signal = single GaussianBackground = ARGUS functionPeaking BG is negligibly small.
Complicated methodis used to obtain K+ reconstruction(detector) asymmetry.
Corrections for detectorasymmetry obtainedusing Ds
+-> + andD0-> K- + decays.
ACP (B+ -> J/ψ K+) = (-0.76 ± 0.50 ± 0.22) %
Result is in agreement with Standard Model prediction (~0.3%).
CP violation measurement in B0 J/ψ K+
772 x 106 BB pairs_
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 13
Belle preliminary, arXiv:1008.2567
Measurement of B+ K+and B0
KS0
Radiative penguin diagram
In SM: S(b->s) ~ 0.03S ~ 2(ms/mb) sin(21)
772 x 106 BB pairs_
1176±5
136±175.4
9.6 K+
KS
B (B+-> K+ = (2.34 ± 0.29 ± 0.29 ) x 10-
6 B (B0-> Ks
= (2.66 ± 0.60 ± 0.32 ) x 10-
6
First measurement K+ :
A.Drutskoy et al (Belle) PRL 92, 051801 (2004)
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 14
Belle preliminary, arXiv:0911.1779
CP violation measurement in B0
KS0
ACP (B+ -> K+ ) = (-0.03 ± 0.11 ± 0.08) %
S (B0 -> Ks ) = (+ 0.74 +0.72 +0.10) %
-1.05 - 0.24
A (B0 -> Ks ) = (+ 0.35 ± 0.58 +0.23 ) %
- 0.10
Ks
More results in H.J.Hyun talk: “Rare electroweak penguin decays in Belle”
Results are in agreement with Standard Model predictions.
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 15
Belle preliminary, ICHEP10
Measurement of B XS
Penguin loop diagram can potentially contribute to charmless B decays with .Difficult to predict: s,u,d quark content of meson and - ’ mixing.
_657 x 106 BB pairs
B (B-> XsMx< 2.6GeV/c2 = (26.1 ± 3.0 +1.9 + 4.0 (model) ) x 10-
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 19
hadronic events at (5S)
u,d,s,c continuum
Bs* Bs Bs BsBs* Bs* channel
Bs events
b continuum5S) events
Hadronic event classification at (5S)
B0, B+ events
fs = N(Bs(*) Bs
(*)) / N(bb)
bb cross-section
f(Bs*Bs*)
1,2S) X
bb events
Bs*Bs*
Bs*Bs
BsBs
~ 90% Bs events
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 20
Bs-> Ds* Ds*Bs-> Ds* DsBs-> Ds+ Ds
-
sCP / s measurement from B (Bs -> Ds
+(*) Ds-(*))
s = sCP cos s
Due to CP violation directly measured s/s can be smaller than one
from Bs rate
B [Bs(CP+) – Bs(CP-)]. CPV in Bs decays in SM is small (small phase of Vts element).
In SM : cos s ≈ 1Assuming Bs -> Ds+(*) Ds
-(*) decays dominating CP=+
Belle preliminary, arXiv:1005.5177 L = 23.6 fb-1
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 21
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 22
Belle results on Bs0 decays at (5S)
B (Bs-> ) = (5.7 +1.8 +1.2) x 10-5-1.5 -1.1
B (Bs-> ) < 8.7x10-6 (90% CL)
Belle coll., PRL 100, 121801 (2008)
B (Bs-> Ds+-) = (3.67 +0.35 ± 0.65 ) x 10-3
- 0.33Belle coll., PRL 102, 021801 (2008)
Belle coll., PRL 104, 231801 (2010)
B (Bs->J/) = ( 3.1 1.2 + 0.5 0.38 (fs)) x 10-4
Belle coll.,
arXiv:0912.1434
B ( Bs-> K+K-)=( 3.8 +1.0 0.5 0.5 (fs)) x 10-5 - 0.9
Belle coll., arXiv:1006.5115
Obtained results on Bs decays are in good agreement with expectations
B (Bs->J/) = ( 3.32 0.87 +0.32 0.42 (fs)) x 10-4 - 0.28
- 0.6
Branching fractions for lepton flavor changing decays are negligibly smallin the Standard Model even taking into account neutrino oscillations.
(EPJ C8 513 (1999))
Observation of LFV is clear signature of New Physics.
Several extensions of the SM predict LFV decays. Some BSM models (SUSY-seesaw, SUSY-GUT, specific coupling neutral Higgs) predict rather large branching fractions which are comparable with current experimental sensitivity.
Tau lepton decays => good place to search for BSM
(or e)
W-
(or e)
54
2
2
2
10)(
WSM m
mBr
Lepton flavor violation (LFV) in tau decays
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 23
e+e+
(signal side)
1 prong + missing ( tag side)
e e
generic decay
3 ellipse signal regionThe size was obtained
from MC (resolution).
)( 22 pEM
CMbeam
CM EEE
Number of BG events is estimatedusing sideband data and MC
Signal extraction: M- E plane mM ~
0~E
Experimental method to search for decay + +
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 24
Eff. NBGexp UL Eff. NBG
exp x10-8
8.2% 0.63±0.37 3.6 ’ 8.1% 0.00+0.16-0.00 10.0
6.9% 0.23±0.23 8.6 ’ 6.2% 0.59±0.41 6.6
comb 2.3 ’ comb
3.8
e 7.0% 0.66±0.38 8.2 e’ 7.3% 0.63±0.45 9.4
e 6.3% 0.69±0.40 8.1 e’ 7.5% 0.29±0.29 6.8
ecomb 4.4 e’ comb 3.6
4.2% 0.64±0.32 2.7 e 4.7% 0.89±0.40 2.2
UL(x10-8) UL(x10-8)
Belle preliminary, ICHEP10
Search for decays + ℓ+ P0 (0,,’) with 901 fb-1
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 25
Eff. NBGexp Eff. NBG
exp
e- 7.6% 0.29±0.15 1.8 e-K*0 4.4% 0.39±0.14 3.2
7.1% 1.48±0.35 1.2 K*0 3.4% 0.53±0.20 7.2
e- 4.2% 0.47±0.19 3.1 e-K*0 4.4% 0.08±0.08 3.4
3.2% 0.06±0.06 8.4 K*0 3.6% 0.45±0.17 7.0
e- 2.9% 0.30±0.14 4.8 2.4% 0.72±0.18 4.7
UL(x10-8) UL(x10-8)
Search for decays + ℓ+ V0 (0,K*0) with 854 fb-1
Belle preliminary, ICHEP10
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 26
Our sensitivity reaches O(10-8)!
New upper limits for LFV tau decays
The world best upper limits are obtained. No evidence of LFV tau decays.
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 27
Potential models,energy splitting
s2
cc
L
L (S1 S2)
L=0 0-
1-
L=1
J/c
hc1+
2S1-
’’c
1S
c0
c1
c2
1+
0+
2+
Mas
s
S12
0-
1P
s1
Energy splitting: singlet and triplet.
Potential models predictmasses of conventional states with fixed quantum numbers.
Generally, accuracy of mass predictions should notexceed few tens of MeV/c2.
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy
Charmonium spectroscopy
28
’
Even
ts/1
0
Mev
Belle
X(3872)
X(3872)
230 pb-1
PRL 91 (2003) 262001
304M B’s
PRL 93 (2004) 162002
X(3872) > J/ +- decay
First observed by Belle in B± -> K±(J/+-).Then confirmed by CDF, D0 and BaBar.
455M B’s
PRL 93 (2004) 072001
X(3872)
220 pb-1
X(3872)’
M(J/ +-)
PRD 77 (2008) 111101
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 29
Interpretations of X(3872) and X(4260) are unclear. Most popular for X(3872) ismolecular interpretation (X(3872)-> J/ branching fraction is small for 1++ ’c1 ).
Y(4260)
Is X(3872)D*D molecular?
QFTHEP 2010, Recent results from Belle Golitsyno, Moscow, Russia, September 8 - 15 A. Drutskoy 30