For the LHCb Collaboration

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Presentation transcript:

For the LHCb Collaboration S. Stone LHCb Physics As You Like It For the LHCb Collaboration

The LHCb Detector LHCC, CERN Nov. 17, 2010

Limits on New Physics It is oft said that we have not seen New Physics, yet what we observe is the sum of Standard Model + New Physics. How to set limits on NP? Assume that tree level diagrams are dominated by SM and loop diagrams could contain NP Tree diagram example Loop diagram example Vcb or Vub LHCC, CERN Nov. 17, 2010

What are limits on NP from quark decays? Tree diagrams are unlikely to be affected by physics beyond the Standard Model LHCC, CERN Nov. 17, 2010

CP Violation in Bo & Ko Only Absorptive (Imaginary) of mixing diagram should be sensitive to New Physics. Lets compare LHCC, CERN Nov. 17, 2010

They are Consistent But consistency is only at the 5% level Same for Bs – CP violation in J/y f (not including D0 Asl) limits on NP are not so strong LHCC, CERN Nov. 17, 2010

Running Conditions Because the # of bunches in the LHC was limited we decided that the trigger had enough time to process data with multiple interactions per crossing This gets to 6x larger m than design m # interactions/crossing Design LHCC, CERN Nov. 17, 2010

Life at large m For m+m- triggers, take almost everything, SPD<900. Other triggers require rejecting events with large numbers of tracks. Cut on SPD multiplicity as it correlates well & is provided in L0; the cut value changed with L This still is a large gain for all modes than the original plan of m=0.4 2 1 3 LHCC, CERN Nov. 17, 2010

Integrated Luminosity LHCC, CERN Nov. 17, 2010

Sub-detector efficiencies Some “small” problems: VCSELs in several systems, HV & high current problems in a few systems LHCC, CERN Nov. 17, 2010

Detector Performance Time resolution on typical B decay modes is ~60 fs, very good but, worse than the expected ~40 fs LHCC, CERN Nov. 17, 2010

Particle ID PID performing well Close to MC level performance Data MC Momentum GeV/c Momentum GeV/c LHCC, CERN Nov. 17, 2010

Some Interesting Near Future Measurements & Sensitivities LHCb expectations: 37 pb-1 in 2010 ✓ ~ 2 fb-1 for nominal yr ~ 6 fb-1 for “1st run” ~60 fb-1 for upgrade LHCC, CERN Nov. 17, 2010

Infancy: 15 nb-1 Measure s(ppbbX) using bD0X -, DoK-p+, ~280 events  - Single Muon Trigger + Average Error on theory x -Untriggered In 2<h<6, (75.35.413.0) mb LEP frag In 2<h<6, 89.6 mb Tevatron frag Also measured charm cross-section, ~20x b LHCC, CERN Nov. 17, 2010

Childhood 3 pb-1 LHCC, CERN Nov. 17, 2010 RS Dfb = 28531±193 Prompt = 715±44 sideband = 1776±33 Dfb Prompt D0 Fake D0 WS Dfb = 422±43 Prompt = 204±19 sideband = 1410±21 LHCC, CERN Nov. 17, 2010

Also D+, Ds, Lb D+ Ds D+→K-p+ Ds→K-K+-p+ LHCC, CERN Nov. 17, 2010 LHCb Fake D0 D+ Dfb Prompt D0 LHCb Preliminary D+→K-p+ LHCb Preliminary Dfb: 9406±110 Ds→K-K+-p+ Ds LHCb Preliminary LHCb Preliminary Dfb: 2446±60 LHCC, CERN Nov. 17, 2010

Extract Bs fraction Must correct for Bs→DoK+Xmn, also Lb→DopXmn Will use to determine fs/(fd+fu) Ds2(2573)  D0 K+ Ds1(2536)  D*(2007)0 K+ missed p0 or g GPDG < 2.3 MeV GPDG= 20±5 MeV  D0K+  WS Kaon: D0K- √s = 7 TeV LHCb Preliminary LHCC, CERN Nov. 17, 2010

Bs→Ds2Xmn, Ds2→DoK+ New decay mode observed using 20 pb-1, Seen by D0 in 1.3 fb-1 using D*+Ks, 46±9 events Wrong sign

Exclusive semileptonic decays Accurate measurement of B-flight direction allows missing neutrino reconstruction For Bs→Ds X mn Ds: 0.26±0.06 Ds*: 0.49±0.069 Ds**: 0.25±0.12 LHCb preliminary n No systematic errors yet LHCb Preliminary LHCC, CERN Nov. 17, 2010

Adolescence: m+m- Inclusive J/y→m+m- 0.7 pb-1 LHCC, CERN Nov. 17, 2010

cc→g J/y M(cc)-(J/y) Events/10 MeV LHCC, CERN Nov. 17, 2010 LHCb Preliminary LHCC, CERN Nov. 17, 2010

J/yp+p- #y(2s)=2991±101 #X(3872)=433±95 LHCC, CERN Nov. 17, 2010 Y(2S)

Upsilons too LHCC, CERN Nov. 17, 2010

Z0 & W± Require two m+m-, each with pt>20 GeV Require single isolated m, with pt>20 GeV & small pt opposite L~16 pb-1 LHCb Preliminary L~16 pb-1 Pt(m) LHCb Preliminary LHCb Preliminary M(m+m-) LHCC, CERN Nov. 17, 2010

pp→ppJ/y(cc) We can also do g’s po’s 12 pb-1 “Standard Candle” QCD processes, arXiv: 1005.0695 [hep=ph] LHCC, CERN Nov. 17, 2010

Bo→K*og 37 pb-1 199 events LHCC, CERN Nov. 17, 2010

Fully Reconstructed Hadronic Decays Needed for CP Violation Studies LHCC, CERN Nov. 17, 2010

Exclusive B J/y h ~15 pb-1 J/y K+ 7226 events 3193 events J/y K*o B(B→J/y K+)●B(J/y→m+m-)=6x10-5 J/y Ks 692 events 405 events J/y f

B-→Doh- ~12 pb-1 LHCC, CERN Nov. 17, 2010 B-→Dop-, Do→K-p+ B-→DoK-, Do→K-p+ B(B→Dop-) ●B(Do→p+K-) =1.9x10-4 162 events 2431 events ~12 pb-1 B-→Dop-, Do→p-p+ B-→Dop-, Do→K-K+ 55 events 126 events LHCC, CERN Nov. 17, 2010

B→pK, pp, KK 35 pb-1, “loose cuts” We will get as many Kp in 0.5-0.7 fb-1 as Belle in 1000 fb-1 Bo→K±p+ 838 events Bs→K±p+ B(B→p+p-)=5x10-6 254 events 229 events

B→pK: CPV Bs/Bo yield = (10.7±2.0)%, obvious CPV in both Using loose cuts ACP(Bo)=-0.134±0.041 stat error only, no corrections (HFAG: -0.098±0.012) Using tight cuts ACP(Bs)=-0.43±0.17 stat error only, no corrections (CDF: 0.39±0.15±0.08 in 1 fb-1) Tight cuts loose 1/3 of events LHCC, CERN Nov. 17, 2010

Lb’s appearing b→c+Xmn, c+→pKp Dfb = 3250±71 Lb  pp Lb  Lb  pK 35 events 32 events 60 events Lb  J/yL Lb  pK Lb  pp b→c+Xmn, c+→pKp Dfb = 3250±71 LHCC, CERN Nov. 17, 2010 M(pKp)

Expectations: Soldiering on Next year make world class measurements. With a few hundred pb-1 we believe we can begin to make more sensitive measurements than CDF & D0 in many cases. Ex: Bs→J/y f We expect to reach sensitivities which are good enough to see NP in e.g. CPV in J/y f + J/y f0,K*m+m- angular distributions, Bs→m+m- charm CPV…. LHCC, CERN Nov. 17, 2010

Great Prospects in Charm M2(KK) M2(Kp) LHCC, CERN Nov. 17, 2010

Future acts: The LHCb Upgrade Run at 1033 cm-2/s Requires that detector be readout at 40 MHz crossing rate  new front end electronics for most of the detector Improve hadron trigger eff. Improve tracking, necessary due to large numbers of tracks in multiple interaction xings More radiation damage and trigger speed necessitates a new VELO based on pixels LHCC, CERN Nov. 17, 2010

Conclusions Perhaps we have reached adolescence “All the world's a stage, and all the men & women merely players; they have their exits and their entrances; & one man in his time plays many parts, his acts being seven ages. At first the infant…” Perhaps we have reached adolescence Well known decays have been seen, & we have started to observe new decay modes We are ready to make the worlds best measurements next year & hopefully find evidence of something really interesting! We would love to get 1-2 fb-1 next year! LHCC, CERN Nov. 17, 2010

The End LHCC, CERN Nov. 17, 2010

All the world’s a stage LHCC, CERN Nov. 17, 2010 "All the world's a stage, And all the men and women merely players; They have their exits and their entrances; And one man in his time plays many parts, His acts being seven ages. At first the infant, Mewling and puking in the nurse's arms; And then the whining school-boy, with his satchel And shining morning face, creeping like snail Unwillingly to school. And then the lover, Sighing like furnace, with a woeful ballad Made to his mistress' eyebrow. Then a soldier, Full of strange oaths, and bearded like the pard, Jealous in honour, sudden and quick in quarrel, Seeking the bubble reputation Even in the cannon's mouth. And then the justice, In fair round belly with good capon lin'd, With eyes severe and beard of formal cut, Full of wise saws and modern instances; And so he plays his part. The sixth age shifts Into the lean and slipper'd pantaloon, With spectacles on nose and pouch on side; His youthful hose, well sav'd, a world too wide For his shrunk shank; and his big manly voice, Turning again toward childish treble, pipes And whistles in his sound. Last scene of all, That ends this strange eventful history, Is second childishness and mere oblivion; Sans teeth, sans eyes, sans taste, sans everything." — Jaques (Act II, Scene VII, lines 139-166) LHCC, CERN Nov. 17, 2010