Title: B ATLAS
1?????? B-??????? ?? ????????? ATLAS
- ?.?.???????
- (? ??????? ??
- B-??????)
- http//nuclphys.npi.msu.su/b/index.html
- 18.04.2005
1
2??????????? LHC
- LHC Large Hadron Collider ??????? ????????
????????? ???????? ? ????????? ????? ? CERN?
pp-???????????? (14 ???). - ??????????? ?????? ?????? ????? 2007 ?.
- ?????? ?????????
- ATLAS, CMS ??? ?????? ?????? ??????,
?????????????? ? ?????? ?????, ? ??? ?????
???????????? ??????? b-??????? - LHCb ????????????? ??? B-??????
- ALICE ??? ???????????? ??????? ???.
3(No Transcript)
4(No Transcript)
5- ?? ???????????????? ?? ?????? ??????
- ?-???????? ?? ????????? ATLAS ??????
- ??????, ??? ?????? ??? ??????? ?????????
- ??????? ? ?????? ??????.
- ??????? ????? ?????, ??? ????????????
- CMS ?, ????????, LHCb ????? ?? ?????
- ???????? ????????? ?? ?????? ??????
- ????????
6Introduction - I
- Physics b ? d, s transitions (FCNC) are
forbidden at the tree level in SM and occur at
the lowest order through one-loop-diagrams
penguin and box. - Main points for study
- a) The good test of SM and its possible
extensions - - SUSY, Two Higgs-doublet, LR, Extra
Dimensions - b) Information of the long-distance QCD effects
- c) Determination of the Vtdand Vts
- d) Some of rare decays as BG to other rare
decays - (for example B0d ? p0 µ µ- as BG to B0s
?µ µ- ? ).
2
7Introduction - II
Branching Ratios Hierarchi in SM Br(B0d ?µ
µ- ) a few 10-10 Br(B0d ?µ µ- ? )
a few 10-10 Br(B0s ?µ µ- ) a few
10-9 Br(B0s ?µ µ- ? ) a few 10-8
Br(B0d ? p0 µ µ- ) a few 10-8 Br(B0d ? ?0
µ µ- ) a few 10-7 Br(B0d ? K µ µ-)
(4.8 1.2) 10-7 (BaBar, Belle, 02) Br(B0s ?
f µ µ- ) a few 10-6 Br(B0d ? K µ µ-)
(1.17 0.33) 10-6 (BaBar, Belle, 03) Br(B0d
? K?) (4.3 0.4) 10-5 (CLEO, 93)
3
8Which new measurements can LHC make comparing
with B-factories?
- a) The rare decays of B0s meson (B0s?f? ,
B0s?f µ µ- , B0s ?µ µ- ? and B0s ?µ µ-) and ?b
- baryon - b) Differencial distributions for rare
semileptonic B-meson decays (dimuon-mass spectra,
forward-backward asymmetries) very sensitive to
the SM extensions - c) Branching fractions of rare muonic and rare
radiative muonic B-meson decays good
sensitivity to the SM extensions. -
4
9The basic theoretical description -I
- Effective Hamiltonian for b ? d,s transition
- Heff (b ? q) GFVtqVtb? Ci(µ) Oi (µ),
- includes the lowest EW-contributions and
perturbative - QCD corrections for Wilson coefficients Ci(µ) .
- µ - scale parameter 5 GeV separates SD
(perturba- - tive) and LD (nonperturbative) contributions of
the - strong interactions.
- SM NLO A.Buras, M.Munz, PRD52, p.182, 1995
- SM NNLO C.Bobeth et al., JHEP 0404, 071, 2004
- MSSM NNLO C.Bobeth et al., hep-ph/0409293.
5
10The basic theoretical description -II
Oi (µ) set of the basic operators (specific for
each model SM, MSSM, LR and
others) LD (nonperturbative) contribution of
the strong inte- ractions are contained in the
hadronic matrix elements and are described in
the terms of relativistic invariant function -
transition formfactors.
Need the nonperturbative methods (SR, QM,
Lat).
6
11The accuracy of calculations
- Stability of the Wilson coefficients to the
choice of - mt and µ mb /2, 2mb
- SM NLO approximately 15
- SM NNLO approximately 6 - 7
- MSSM NNLO 30 depends from the
-
parameters set. - Accuracy of the nonperturbative calculations
- depends on a method, but its not less, than 15
. - For SM calculations NLO, for MSSM NNLO.
7
12Simulations of rare B-decays for ATLAS detector
8
13B0d,s ?µµ- decays in ATLAS
- Points for study in ATLAS
- Branching ratio - sensitive to the SUSY .
- Simulations
- Full Inner detector simulation and reconstruction
at low and nominal LHC luminosity - 1) for TDR layout signal background (ATLAS
TDR 15, Vol.II, 1999) - 2) for Initial layout only signal
(ATL-COM-PHYS-2003-003 ). - 3) signal background in DC2.
- Results
- Using SM teoretical predictions Br(B0d,?µµ- )
1.510-10 and Br(B0d,?µµ- ) 3.510-9 - we obtaned the following sensitivities for ATLAS
- After 3 year LHC work at L1033 cm-2s-1 (30
fb-1) will be expected - B0d 4 signal ev., B0s 27
signal ev., 93 BG ev. common to both - After 1 year LHC work at L1034 cm-2s-1 (100
fb-1) will be expected - B0d 14 signal ev., B0s 92
signal ev., 660 BG ev. common to both - We expect the 31010 sensitivities at CL 95 for
rare leptonic decays.
9
14B0d?K(892)µµ- decay at ATLAS
- Points for study in ATLAS
- Branching ratio - sensitive to the SUSY
- Differencial distributions (dimuon-mass spectra,
AFB) very good - sensitivity to the
SUSY. - Simulations
- Full ATLAS Inner detector simulation and
reconstruction at low - luminosity (ATLAS TDR 15, Vol.II, 1999) using
theoretical matrix - element from paper D.Melikhov, N.Nikitin,
S.Simula, PRD57, 6814, 1998. - Results of simulation
- After 3 year LHC work at L1033 cm-2s-1 (30
fb-1) will be expected - 2000 signal events at
290 BG events
10
15Radiative penguins in ATLAS
Points for study in ATLAS Branching for Bsf g,
polarization measurements and CP-violation
effects.
Preliminary results Non-optimized offline cuts,
resolution (gt100 MeV/c2) could be improved.
Using DC1 simulation tools estimations including
trigger and off-line selection cuts for 1year
LHC work at L21033cm2s-1 (20fb-1)
Bsf g 3200 signal ev., S/vBG gt 7
BdK0 g 8500 signal ev., S/vBG gt 5. B?K0p0 BG
rejection under investigation combining p0/ ?
rejection cuts, kinematics and angle between B0
and K at Krest frame cuts.
11
16Baryonic rare decay of ?b? ? µ µ-
Points for study in ATLAS Branching ratio -
sensitive to the SUSY FB asymmetry - very
sensitive to the SUSY . Generation
procedure EvtGen used to generate events using
amplitudes from works (C-H.Chen, C.Q.Geng, PRD64,
074001, 2001 ) and (T.M.Aliev et.al. , NPB649, p.
168-188 , 2003). Results of DC1-simulation At
Br(?b? ? (p p-) µ µ- ) 210-6 after 1 year LHC
work at L21033 cm-2s-1 (20 fb-1) will be
expected 1800 events of the decay ?b? ? (p p-)
µ µ- .
12
17B0d ? p0 µ µ- as BG to B0d,s ?µµ-? and B0d,s
?µµ- decays
- ?(µ) lt 2.5, pT(µ) gt 6 GeV, p0 ? ? ? , pT(p0) lt
4GeV - The decay B0d ?p0 µ µ- are essential background
for the decay - B0d,s ?µ µ- (?) at the particle level
simulation.
16
18SUSY in rare B-decays at ATLAS detector
19SUSY main motivations for study in rare B-decays
- I) Many kinds of heavy (m gt 1 TeV) SUSY
particles. - II) Only lightest of these particles can be
detected on LHC. - III) Other SUSY-particles give the tiny
contributions as - virtual particles in SM processes.To find
the information - on such particles it is necessary to
choose the decays - a) where SM contributions are suppressed
as much as - possible
- b) QCD nonperturbative corrections well
known - c) branchings can be measured in ATLAS.
- Rare B0d,s and ?b decays are IDEAL CHOICE for
that!
18
20MSSM for B0d,s?µµ- decays and ATLAS sensitivity
- C.Bobeth et al., PRD66, 074021, (2002)
- The B0d,s?µµ- barnchings as functions of charge
- Higgs boson mass MH for two choice the tan ß.
19
21MSSM in B ?K(892) µµ- decay and ATLAS precision
Sensitivity of AFB to the choice of the Wilson
coefficients in one MSSM scenario P.Cho,
M.Misiak, D.Wyller, PRD54, p.3329, 1996.
Three intervals for variable q2 /M2B. If in the
first interval the negative average asymmetry
will be measured, it will be convincing
demonstration of a SM exten- sions reality.
20