b – физика на lhcb
DESCRIPTION
А.И. Голутвин (ИТЭФ). b – физика на LHCb. Нарушение Редкие распады CP чётности. LHCb – forward spectrometer (running in pp – collider mode) Data taking starts next year Expect ~10 fb -1 by 2013 - PowerPoint PPT PresentationTRANSCRIPT
b – физика на LHCb
А.И. Голутвин (ИТЭФ)
Нарушение Редкие распадыCP чётности
LHCb – forward spectrometer (running in pp – collider mode) Data taking starts next year
Expect ~10 fb-1 by 2013 B physics is also a part of the ATLAS and CMS early program
LHCb is designed to run at an average luminosity of 2 1032 and be able to handle 51032 cm-2s-1 for short periods
For a “nominal” year of 107 seconds this corresponds to 2 fb-1 . Most physics
goals are expressed in terms of the reach for 10 fb-1 (i.e. 5 nominal years)
Super LHCb (SLHCb) will run at 10 times the initial design luminosity with twice more efficient trigger
and record data sample of > 100 fb-1 Start data taking after 2014
Working Group set up to identify the R&D required to make an upgrade of LHCb feasible, and to make the physics case
Issues of triggering, fast vertex detection, electronics, radiation dose, handling the pile-up and higher occupancy, etc…→ Expression of Interest for R&D towards an upgrade is in preparation
LHCb Collaboration
LHCb is a collaboration of ~ 670 members from 48 institutes
– in Brazil, China, France, Germany, Ireland, Italy, Poland, Romania, Russia, Spain, Switzerland, Ukraine, UK, and the US
Российские Институты:
ИТЭФ(Москва), ИФВЭ(Протвино), ИЯИ(Троицк), ПИЯФ(Гатчина), ИЯФ(Новосибирск) внесли определяющийвклад в создание калориметрической системы имюонного детектора
Планируется вступление в коллаборацию НИИЯФ МГУ
4
The LHCb Experiment
p
p
Interaction point
Dipole magnet
10 – 300 mrad forward acceptance
Forward geometry
Running with less focused
beam is sufficient
At 21032 1012 bb pairs
are produced per year
Experimental infrastructure
Shielding wall(against radiation)
Electronics + CPU farm in barracks(Control Room on surface)
Offset interaction point To maximize space
Most detectors opentransversely for access
Shielding wall
• Upper part completed
• Assembly of lower part is progressing wellPaused while a problem with leaking
cooling-water pipes is investigated
Labour intensive “Egyptian work” as inaccessible by crane…
It’s full!Installation of major structures is essentially complete
Commissioning is ongoing !
Muon detector
Calorimeters
RICH-2
Magnet
OT
VELO
RICH-1
UT as a standard approach to test the consistency of SM
Mean values of angles and sides of UT are consistent with SM predictions
Accuracy of sides is limited by theory:
- Extraction of |Vub|
- Lattice calculation of
Accuracy of angles is limited by experiment:
= ± 13° = ± 1° = ± 25°
Search for NP comparing observables measured in tree and loop topologies
(tree+box) in B J/Ks (tree) in many channels(tree+box) in Bs J/
(peng+tree) in B,, (peng+box) in BKs (peng+box) in Bs
New heavy particles, which may contribute to d- and s- penguins,could lead to some phase shifts in all three angles:
(NP) = (peng+tree) - (tree)
(NP) = (BKs) - (BJ/Ks) ≠ 0 (NP) = (Bs) - (BsJ/)
Contribution of NP to processes mediated by loops (present status)
to boxes:
vs |Vub / Vcb | is limited by theory (~10% precision in |Vub|) (d-box)
not measured with any accuracy (s-box)
to penguins:
((NP)) ~ 30° (d-penguin) ((NP)) ~8° (s-penguin) ((NP)) not measured (s-penguin)
PS (NP) = (NP) (NP) measured in B and B decays may differ depending on penguin contribution to and final states
Search for NP comparing observables measured in tree and loop topologies
: LHC prospects
In SM S = - 2arg(Vts) = - 22 ~ - 0.04
Sensitive to New Physics effects in the Bs-Bs system if NP in
mixing S = S(SM) + S(NP)
2 CP-even, 1 CP-odd amplitudes, angular analysis needed to separate, then fit to S, S, CP-odd fraction
LHCb yield in 2 fb-1 131k, B/S = 0.12
Bs J/ is the Bs counterpart of B0J/ KS
will reach s(s) ~ 0.08 (10/fb, ms=20/ps, 90k J/ evts)
LHCb
ATLAS
0.021
0.021
Vcs* Vub: suppressedFavored: Vcb Vus
*
b
u
s
u u
b
u
cD(*)0
K(*)-
B-
u
s
u
c
D(*)0
f
Common
final state
K(*)-
B-
Interference between tree-level decays
iiBKDBA
KDBA eer B
0
0 Parameters: γ, (rB, δB) per mode
Three methods for exploiting interference (choice of D0 decay modes):
(GLW): Use CP eigenstates of D(*)0 decay, e.g. D0 K + K- / π+π– , Ksπ0
(ADS): Use doubly Cabibbo-suppressed decays, e.g. D0 K+π -
(Dalitz): Use Dalitz plot analysis of 3-body D0 decays, e.g. Ks π+ π-
Mixing induced CPV measurement in Bs Ds K decays Specific for LHCb
UT angle : LHCb (BaBAr & BELLE & Tevatron ~12° precision for at best)
LHCb status report
B± → D(KSπ+π−) K±
• Mode used by B factories to give best existing constraint on CKM angle :
[BaBar] 12114192[Belle] 9 3 53 15
18
B+(stat, syst, model) B
~ 400 events each
• LHCb yield ~ 5000 events/2 fb-1
• Spot the difference between the Dalitz plots for B+ and B → effect of CP violation
• Binning can reduce model dependence
Precision on ~ 12º (in one year)
Simulated data for LHCb (1 year)hep/ph 0703267
Model-independent approach
A.Bondar, A.Poluektov Eur.Phys.J C47,347(2006) hep-ph/0510246
50 ab-1 at SFF factory should be enough for model-independent γ/φ3 measurement with accuracy below 2°
1fb-1 at ψ(3770) corresponds 2100 CP-tagged KS+ - events (first estimation based on CLEO-c data by David Asner)
~10 fb-1 at ψ(3770) needed to accompany SuperB measurement
angle ( 3 ) at SFF
Combined precision after 2 fb-1 () 5 (from tree only)
UT angle : LHCb summary table
LHCb (10fb-1 ) and SFF (50-75 ab-1) & SLHCb (>100 fb -1) sensitivities
LHCb
SFF & SLHCb
Channel Yield Precision
From tree channels () < 3
Bd +-0
B +0, +-,00 70k45k,10k,5k
() < 4
Bd J/()KS
Bd KS
1200k 4k
(sin2) < 0.01(sin2) ~ 0.1
s Bs J/()Bs
750k 20k
(s) ~ 0.01(s) ~ 0.05
> 2014
SLHCb (stat. only) ~ 0.003 < 1 (BsDsK) - - -
S(K0S) 0.02-0.03
S() 0.01
Search for New Physicsin Rare Decays
Exclusive b s BK* Bs
B hs, sll inclusive
Experimental challenge: keep backgrounds under control
We are just approaching sensitivity promising for discovery…
LHCb
SFF
b s exclusive
LHCb control channel: Bd K* ~75k signal events per 2fb-1
Bs BELLE observed 16±8 events
2 weeks run at (5S); no TDCPV
LHCb annual yield ~11k with B/S < 0.6
b s exclusive
b (L) + (ms/mb) (R)
Measurement of the photon helicity is very sensitive test of SM
Methods: Mixing induced CP asymmetries in Bs , BKs 0 Photon helicity can be measured directly in radiative B decays to final state with 3 hadrons.
Promising channels for LHCb are B K and B K decays
Expected yield per 2 fb-1
BR(B+ K+-+) ~ 2.5 10-5 rich pattern of resonances ~60k BR(B+ K+) ~ 3 10-6 highly distinctive final state ~ 7k
b s exclusive
Mixing induced CP asymmetries
BKs0 (B-factories)
S = - (2+O(s))sin(2)ms/mb + (possible contribution from bsg) = - 0.022 ± 0.015 P.Ball and R.Zwicky hep-ph/0609037Present accuracy: S = - 0.21 ± 0.40 (BaBar : 232M BB) S = - 0.10 ± 0.31 (BELLE: 535M BB)
Bs (LHCb)
LHCb sensitivity with 10fb-1 :
(A) = 0.09
B K*
In SM this bs penguin decay contains right-handed calculable contribution but this could be added to by NP resultingin modified angular distributions
SM
B K*: LHCb prospects
Forward-backward asymmetry AFB (s) in - rest frame is a sensitive NP probe Predicted zero of AFB (s) depends on Wilson
coefficients C7eff / C9
eff
AFB(s), fast MC, 2 fb–1
s = (m)2 [GeV2]
7.2 k events / 2fb-1 with B/S ~ 0.4 After 10 fb-1zero of AFB located to ±0.28 GeV2 providing 7% stat. error on C7
eff / C9eff
Full angular analysis gives better discrimination between models. Looks promising
23
Bs
This decay could be strongly enhanced in some SUSY models.
Current limit from CDF BR(Bs) < 4710-9 (2010-9 expected final D0+CDF limit)With loose selection LHCb expects ~40 signal events (2fb-1/SM BR) on top of ~1500 background events (mostly form b , b )
Particle ID, vertexing and invariant mass resolution (M )~ 18 MeV provide excellent separation of signal from background
Very smal BR in SM(3.4 ± 0.5) x 10-9
24
OUTLOOK Clean experimental signature of NP is unlikely at currently operating experiments
From now to 2014A lot of opportunities (LHCb will start data taking next year)Important measurements to search for NP and test SM in CP violation : if non-zero NP in boxes < 2010 vs Rb and vs Rt (Input from theory !) (NP) and (NP): if non-zero NP in penguins in Rare decays BR(Bs ) down to SM prediction < 2010 Photon helicity in exclusive bs decays FBA & transversity amplitudes in exclusive bsll decays < 2010
After 2014ATLAS and CMS might or might not discovered New Particles. At the same timeLHCb might or might not see NP phenomena beyond SM.In either case it is important to go on with B physics at SFF & Upgraded LHCb
Need much improved precision because any measurement in b-system constrains NP models
high pTB’s
25
LHCb calorimeter system
• Scintillating Pad Detector / PreShower • Electromagnetic Calorimeter• Hadron Calorimeter
Fast response within 25 ns is a 1st priority requirement for L0 trigger All 3 calorimeter are using the “same” technology: absorber/scintillator readout with WLS fibres
Back of SPD
Lead
Front of PS
Andrey Golutvin VCI 2007 26
PS+SPD built from 16 super modules Side view of upper part
Overview of LHCb Overview of LHCb SPD and PSSPD and PS
Inner + Middle + Outer Modules
MAPMT+ VFER/O
cables
Moving cable trays
Scintillator + coiled fiber
Super module frame
Super modulewith 2 x 13 modules
TDR estimations (2000): • outer ~ 20 ph.el. • inner ~ 30 ph.el.
Preshower cosmic test before Super-Module installation # phe/MIP for each tile:
Inner: 25 pheMiddle 29 pheOuter: 19 phe
27
Overview Overview of LHCb ECALof LHCb ECAL
3312 shashlik modules with 25 X0 Pb
Scintillators, lead-plates, covers
Fibres with loops
PMT and CW base
Two halves on chariots and electronics platform on top
Chariot
Electron.platform
End-cover
Lead plateScintillator
TYVEK
Front-cover
CW base
PMT
Middle module
Inner module
Outermodule
modules
Beam plug
28
Overview of Overview of LHCb HCALLHCb HCAL
particles
PMT
scintillators
fibers
light-guide
Internal cabling
CW base
PMT housingModule with optics assembled
Electron.platform
Chariot
52 modules with longitudinal tiles
modules
Beam plug