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B ATLAS

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LHC Large Hadron Collider ??????? ???????? ????????? ???????? ? ????????? ... of B0s meson (B0sf? , B0sf - , B0s - ? and B0s -) and ?b - baryon; ... – PowerPoint PPT presentation

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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 ??? ???????????? ??????? ???.

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  • ?? ???????????????? ?? ?????? ??????
  • ?-???????? ?? ????????? ATLAS ??????
  • ??????, ??? ?????? ??? ??????? ?????????
  • ??????? ? ?????? ??????.
  • ??????? ????? ?????, ??? ????????????
  • CMS ?, ????????, LHCb ????? ?? ?????
  • ???????? ????????? ?? ?????? ??????
  • ????????

6
Introduction - 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
7
Introduction - 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
8
Which 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
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The 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.

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The 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
11
The 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.

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12
Simulations of rare B-decays for ATLAS detector
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B0d,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
14
B0d?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

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Radiative 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.
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16
Baryonic 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
17
B0d ? 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.

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SUSY in rare B-decays at ATLAS detector
19
SUSY 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
20
MSSM 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
21
MSSM 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
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