BTeV Physics Reach LHC 2003 Symposium K. Honscheid Ohio State University LHC2003 K. Honscheid Ohio State B Physics Today CKM Picture okay VCKM = Vud Vus Vub Vcd Vcs Vcb Vtd Vts Vtb CP Violation observed sin(2b) = 0.734 +/- 0.054 No conflict with SM LHC2003 K. Honscheid Ohio State Surprising B Physics Year Item 1983 tb 1987 2001 Theory Prediction ~Value # B’s Too small to be observed ~ < 0.1ps 1 ps 2x104 Bo-Bo mixing Too small to see (~ < 1%) as mtop is believed to be ~30 GeV 20% 2x105 sin(2b) No direct prediction, but consistent with other measurements 3/4 107 a,b,g >1011 b hadrons (including Bs) LHC2003 K. Honscheid Ohio State B Physics at Hadron Colliders The Tevatron as b (and c) source b cross section b fraction Inst. Luminosity Bunch spacing Int./crossing Luminous region ~100 mb, c cross section ~1000 mb 2x10-3 2x1032 2x1011 b pairs/year 132 ns (396 ns) <2> (<6>) sz = 30 cm Forward Geometry bg LHC2003 K. Honscheid Ohio State The BTeV Detector RICH Detector Pixel Detector Gas (C4F10) + Liquid Radiator (C5F12) Vacuum Vessel PbWO4 EM Calorimeter HPD + PMT read-out 10500 crystals 220 mm long, 28x28 mm2 Beam Line p/K/p separation up to 70 GeV/c s(h->gg) ~ 5 MeV e/m separation at low momenta Proper time resolution: 46 fs s(p->gg) ~ 3 MeV CLEO/BaBar/BELLE-like performance in a hadron Collider environment! LHC2003 K. Honscheid Ohio State • 60 pixel planes • inside magnet • s = 5-10 mm Efficiencies and Tagging For a requirement of at least 2 tracks detached by more than 6s, we trigger on only 1% of the beam crossings and achieve the following trigger efficiencies for these states (<2> int. per crossing): Decay efficiency(%) B p+p63 Bs DsK 74 B- DoK70 B- Ksp27 LHC2003 K. Honscheid Ohio State Decay efficiency(%) Bo K+p63 Bo J/y Ks 50 Bs J/yK* 68 Bo K*g 40 e efficiency; D Dilution or (Nright-Nwrong)/(Nright+Nwrong) Effective tagging efficiency eD2 Extensive study for BTeV uses Opposite sign K± Jet Charge Same side p± (for Bo) or K± for (Bs) Leptons Conclusion: eD2 (Bo) = 0.10, eD2 (Bs) = 0.13, difference due to same side tagging The Physics Goals There is New Physics out there: Baryon Asymmetry of Universe & by Dark Matter Hierarchy problem Plethora of fundamental parameters … BTeV is in a unique position to: Perform precision measurements of CKM Elements with small model dependence. Search for New Physics via CP phases Search for New Physics via Rare Decays Help interpret new results found elsewhere (LHC, neutrinos) Complete a broad program in heavy flavor physics Weak decay processes, B’s, polarization, Dalitz plots, QCD… Semileptonic decays including Lb b & c quark Production Structure: B baryon states Bc decays LHC2003 K. Honscheid Ohio State Part 1: Is the CKM Picture correct? Use different sets of measurements to define apex of triangle (adopted from Peskin) Also have eK (CP in KL system) Bd mixing phase Magnitudes Bs mixing phase Can also measure g via B-DoK- LHC2003 K. Honscheid Ohio State Measuring a Using Borp p+p-po A Dalitz Plot analysis gives both sin(2a) and cos(2a) (Snyder & Quinn) Measured branching ratios are: B(B-rop-) Nearly empty (r polarization) ~10-5 = B(Bor-p+ + r+p-) = ~3x10-5 B(Boropo) <0.5x10-5 Snyder & Quinn showed that 1000-2000 tagged events are sufficient Not easy to measure p0 reconstruction Not easy to analyze 9 parameter likelihood fit LHC2003 K. Honscheid Ohio State Slow p0’s Dalitz Plot for Borp Yields for Borp Based 9.9x106 background events Bor+p5400 events, S/B = 4.1 Boropo 780 events, S/B = 0.3 Background p o LHC2003 K. Honscheid Ohio State g Boropo Signal g mB (GeV) mB (GeV) Our Estimate of Accuracy on a Geant simulation of Borp, (for 1.4x107 s) a (gen) Rres Rnon a (recon) Da 77.3o 0.2 0.2 77.2o 1.6o 77.3o 0.4 0 77.1o 1.8o 93.0o 0.2 0.2 93.3o 1.9o 93.0o 0.4 0 93.3o 2.1o 111.0o 0.2 0.2 111.7o 3.9o 111.0o 0.4 0.2 110.4o 4.3o minimum c2 Example: 1000 Borp signal + backgrounds With input a=77.3o LHC2003 K. Honscheid Ohio State non-resonant non-rp bkgrd resonant non-rp bkgrd Bs Mixing (Vtd/Vts) BTeV reaches sensitivity to xs of 80 in 3.2 years 6 5 4 3 2 1 LHC2003 K. Honscheid Ohio State Measuring c In the SM the phases and magnitudes are correlated: sinb sing sin c = l sin(b+g ) 2 Silva & Wolfenstein (hep-ph/9610208) Aleksan, Kayser & London l = |Vus| = 0.2205±0.0018 c is the phase of Vts -> Bs Mixing Good: Bs->J/yf plus non-trivial angular analysis Better: Bs -> CP eigenstate such as BsJ/yh() , hgg, hrg LHC2003 K. Honscheid Ohio State Measuring c II BTeV can reconstruct h and h’ Yield in one year BsJ/y h: 2,800 events with S/B = 15 BsJ/y h: 9,800 events with S/B = 30 Error on sin(2c) = 0.024 With c ~ 2o a precision measurement will require a few years. LHC2003 K. Honscheid Ohio State Physics Reach (CKM) in 107 s Reaction B(B) (x10-6) S/B Parameter Error or (Value) Bs Ds K- 300 7500 7 g - 2c 8o Bs Ds p- 3000 59,000 3 xs (75) 445 168,000 10 7 250 2.3 B-Do (K+p-) K- 0.17 170 1 B-Do (K+K-) K- 1.1 1,000 >10 BoJ/y KS J/y l+ l - BoJ/y Ko, Ko p l n BsJ/y h, 330 2,800 15 BsJ/y h 670 9,800 30 Bor+p- 28 5,400 4.1 Boropo 5 780 0.3 Reaction B(B) (x10-6) LHC2003 K. Honscheid Ohio State # of Events # of Events S/B sin(2b) 0.017 cos(2b) ~0.5 13o g sin(2c) 0.024 a ~4o Parameter Error B-KS p- 12.1 4,600 1 BoK+p- 18.8 62,100 20 Bop+p- 4.5 14,600 3 Asymmetry 0.030 BoK+ K- 17 18,900 6.6 Asymmetry 0.020 <4o + g Theory err. Part II: Search for New Physics LHC2003 K. Honscheid Ohio State For a nice overview see: S. Stone “BTeV Physics” at http://doe-hep.hep.net/P5StoneMarch2003.pdf First Example: Supersymmetry Supersymmetry: In general 80 constants & 43 phases MSSM: 2 phases (Nir, hep-ph/9911321) New Physics in Bo mixing: qD , Bo decay: qA, Do mixing: fKp Process Quantity SM New Physics BoJ/yKs CP asym sin(2b) sin2(b+qD) BofKs CP asym sin(2b) sin2(b+qD+qA) DoK-p+ CP asym 0 ~sin(fKp) New Physics LHC2003 K. Honscheid Ohio State Difference NP Rare b Decays Search for New Physics in Loop diagrams New fermion like objects in addition to t, c or u New Gauge-like objects in addition to W, Z or g Inclusive Rare Decays including g, l+l- bsg bdg bsl+l- Exclusive Rare Decays such as Brg, K*g BK*l+lDalitz plot & polarization LHC2003 K. Honscheid Ohio State BoK*g Yield, S/B for Rare b Decays Reaction LHC2003 K. Honscheid Ohio State B (10-6) Signal S/B 11 BoK*om+m- 1.5 2530 B-K-m+m- 0.4 1470 3.2 bsm+m- 5.7 4140 0.13 Physics Polarization; Rate Rate Rate; Wilson coefficents Polarization in BoK*om+mBTeV data compared to Burdman et al calculation Dilepton invariant mass distributions, forward-backward asymmetry discriminate among the SM and various supersymmetric theories. Ali et. al, hep-ph/9910221 (Ali, Lunghi, Greub & Hiller, hep-ph/0112300) LHC2003 K. Honscheid Ohio State One year for K*l+l-, enough to determine if New Physics is present Second Example: Extra Dimensions Aranda & Lorenzo Diaz-Cruz, “Flavor Symmetries in Extra Dimensions” (hep-ph/0207059) (Buras et al. hep-ph/0212143) Extra spatial dimension is compactified at scale 1/R = 250 GeV on up No effect on |Vub/Vcb|, DMd/DMs , sin(2b) Bs -> mm –8% |Vtd| LHC2003 K. Honscheid Ohio State –100 g +72% Summary Heavy quark physics at hadron colliders provides a unique opportunity to measure fundamental parameters of the Standard Model with no or only small model dependence discover new physics in CP violating amplitudes or rare decays. interpret new phenomena found elsewhere (e.g. LHC) Some scenarios are clear others will be a surprise This program requires a general purpose detector like BTeV with an efficient, unbiased trigger and a high performance DAQ a superb charged particle tracking system good particle identification excellent photon detection LHC2003 K. Honscheid Ohio State Changes wrt Proposal in Event Yields & Sensitivities We lost one arm, factor = 0.5 We gained on dileptons From RICH ID in proposal we used only m+m-, now we include e+efactor = 2.4 (or 3.9), depending on whether analysis used single (dilepton) id We gained on DAQ bandwidth, factor = 1.15 Gained on eD2 for Bs only, factor = 1.3 LHC2003 K. Honscheid Ohio State Mode Yield proposal BoJ/y Ks 80,500 BsJ/yh() 9,940 Bs Ds K- 13,100 Yield factor Yield one-arm Quantity Err(prop) (eD2) Quantity Err(1arm) (eD2) 0.5*3.9* 1.15=2.24 168,000 sin(2b) 0.025 (0.10) sin(2b) 0.017 (0.10) 0.5*2.4* 1.15=1.38 12,600 sin(2c) 0.033 (0.10) sin(2c) 0.024 (0.13) 0.5*1.15 =0.58 7,500 g 6o (0.10) g 8o (0.13)