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Looking for New Physics: Prospects of B-Physics at LHCb

Discover the prospects of searching for New Physics through B-decays at LHCb, including precision tests of the Standard Model and key measurements like CKM angles. Learn about tree and loop decays, CP asymmetries, and Bs sector exploration.

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Looking for New Physics: Prospects of B-Physics at LHCb

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  1. s b Looking for New Physics: Prospects of B-Physics at LHCb Ulrich Uwer Physikalisches Institut Heidelberg On behalf of the LHCb Collaboration

  2. Search for New Physics in B decays New Physics W New Physics W …precision test of the SM at loop level box diagramms penguin amplitudes Deviations from Standard Model: absolute rates and phase dependent CP asymmetries • measurement of  in tree and loop decays • exploring the Bs sector - mixing phase s • bs  penguin transitions • very rare FCNC decays key measurement: Outline

  3. LHCb – Key Properties e (KK) = 88% e (pK) = 3% • High statistics • L ~ 2 x 1032 cm-2 s-1 • ~ 1012 bb events / year (2 fb-1) • 50 kHz bb-events • B±, B0, Bs, Bc, Lb … • Tracking & Vertexing • B Mass resolution: ~ 15…20 MeV • Proper time resolution:~ 40 fs • Particle identification • p/K separation over 2 GeV < p < 100 GeV • Trigger (2 kHz to tape) • “High pT”lepton, photon & hadron 1st level trigger w/ 1 MHz: Example: sin2(B0J/Ks) 0.5 fb-1 52k evts (sin2)=0.020 (2 fb-1) m/e/h/g: 1.1/2.8/3.6/2.6 GeV (sin2)=0.023 (today)

  4. CKM Angle  Indirect Directmeasurement • A lot of pioneering work from B factories • No significant constrain from direct measurements yet Precise determination of  in tree and loop decays.

  5.  from B  DK Tree Decays Tree decays:  fD  fD ADS (Atwood,Dunietz,Soni) method: Common flavour state fD=(K+ p–)Note: D0→K+p–doubly Cabibbo suppr. GLW (Gronau,London,Wyler) method: fD is a CP eigenstate, fD= K+K-, +- sg= 11° – 13° 2 fb-1

  6.  from B  DK Tree Decays GGSZ Method: Use Dalitz decays: 2 fb-1: ~ 5k evts 2 fb-1 Statistical uncertainty sg= 10° Amplitude model sg = 13° Binned fit/Cleo-C data Combined sensitivity sg 2fb-1 LHCb-2008-031 + ??????

  7. Time dependent Asymmetry Tree b->c & b->u decays interfere through Bs mixing Time dependent CP asymmetry: Use BsDs to determine tagging dilution simultaneously 2 fb-1 2 fb-1 Bs→ Ds-K+

  8.  Sensitivity /K /K Bd/s Bd/s /K /K LHCb-2008-031 Tree Level Processes • Combination: • BD0K • B0D0K*0 • Time dependent: B0  Dp Bs  DsK 2o …3o reachable after 5 yr Loop Processes R.Fleischer Measure time dependent CP asymmetries (direct, mixing) in Bd   and Bs KK. Crucial: P/T described by (d, ) 7…10o (2fb-1) ~5o (10 fb-1) Uspin constraint: dpp= dKK 20% • from interference between mixing tree (T) and penguin (P) amplitudes,

  9. Bs Mixing Phase s New Physics W s from ACP(BsJ/) mixing First results from CDF/D0 A.Lenz, U.Nierste

  10. BsJ/ Experimental challenge: Performing an angular analysis to distinguish between CP-odd and CP-even components. Pure CP eigenstates small yield, large bckg. BsJ/ is VV state: L=0, 2  CP-even L=1  CP-odd J/  117k 0.030 Transversity basis: CDF ~4%

  11. s Sensitivity LHCb-Roadmap-2009 • One of first key measurements SM value: s=-0.0368±0.017 Penguin Decays Standard Model: Bs   = s-Decay = 0  zero CP asymmetry 2 fb-1 (10 fb-1) Yield (2 fb-1): 3100 evts, B/S <0.8

  12. Search for New Physics in penguin A.Lenz and very rare decays

  13. Radiative bs penguins Time dependent CP asymmetry to determine photon polarization (SM: mainly LH) _ XsgL(R) B0 B0 XsgR(L) SM: Adir = 0 (direct CPV) Amix= sin2sin0 A = sin2cos 2 fb-1: (A)=0.22 (Adir,mix)=0.11 Fraction of “wrong” polarized photons tan= |A(bsR)|/ |A(bsl)| LHCb-Roadmap-2009

  14. B0  K* Standard Model Model independent approach using Operator Product Expansion Corresponding Wilson coefficients Ci describe short-range physics.

  15. Angular observables in B0  K* Forward-backward asymmetry Observables:l, K, , m2 • Angular observables sensitive to New Physics models • AFB zero-crossing point: dominant theoretical error (FF) cancels Offers a powerful test bench for any New Physics model

  16. B0  K* - LHCb prospects 2 fb-1 2) Fits to decay angle projections: Other angular observables: e.g. K* polarization 1) Simple Counting 10 fb-1 AFB(s) LHCb-20008-041 2 fb-1 3) Full angular fit s [GeV2] Maximum discrimination of NP models

  17. “Very” rare decays: Bs ATLAS < 10-8 (2 fb-1) < 5.8·10-895% CL PRL 100,101802 (2008) 2 fb-1 CMS < 1.4  10-8 (10 fb-1) < 9.3·10-895% CL D0 Note 5344-Conf (2007) 90%CL upper limit BR (x10–9) Expected final CDF+D0 limit Uncertainty from MC stats on bkg SM prediction SM: BR(Bsμ+μ-)= (3.42±0.54)x10-9 BR (x10–9) Large SUSY contributions possible 5 observation SM prediction 3 evidence Discovery  L dt (fb–1)

  18. Conclusion s b • CKM mechanism is dominating effect for CP violation and flavor mixing in the quark sector… but there is room for sizable new effects in B meson decays. • LHCb will try to map-out effects of New Physics • Interesting results can come early (0.5 fb-1) •  from trees w/ precision 8 … 10o • s(BsJ/) w/ precision of 0.06 • Limit for BR(Bs) < 10-8 • LHCb has a lot of opportunities to discover New Physics in a few years of data taking (10 fb-1).

  19. Backup

  20. Outlook – LHCb beyond 10 fb-1 100 fb-1 LHCb upgrade • Run at 10 design luminosity: 21033 • Needs detector and trigger upgrade • Increase trigger efficiency for hadrons by at least a factor 2 • Accumulate data sample of 100 fb-1 100 fb-1 Physics case • CPV in Bs mixing (tree and penguins) • CKM angle  with ~1o precision • Chiral structure of bs decays • Lepton flavor violation in 

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