7/9/2005U. Heintz - PiC 20051 heavy flavor production Ulrich Heintz Boston University.
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Transcript of 7/9/2005U. Heintz - PiC 20051 heavy flavor production Ulrich Heintz Boston University.
7/9/2005 U. Heintz - PiC 2005 1
heavy flavor production
Ulrich Heintz
Boston University
7/9/2005 U. Heintz - PiC 2005 2
disclaimers/acknowledgements• not a comprehensive review but selected
results with concentration on b-production at the Tevatron
• not covered at all– c-production– results from e+e- collisions
• material from talks at Moriond, La Thuile, Beauty 2005
• thanks to D.Bauer, I.Belyaev, I.Bloch, M.D’Onofrio, M.Hildreth, V.Papadimitriou
7/9/2005 U. Heintz - PiC 2005 3
why?• check our understanding of QCD
– heavy flavor production at high energies checks perturbative QCD
– extracting fundamental parameters of the standard model at hadron colliders requires deep understanding of QCD
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b production at high energies• HERA (H1/ZEUS) 30/920 GeV
– photoproduction Q2<1 GeV2
• hard scales: mb, pT
– deep inelastic scattering Q2>1 GeV2
• hard scales: mb, pT, Q2
• Tevatron (D0/CDF) √s=1.96 TeV– hard scales: mb, pT
• at least one hard scale pQCD should work
concentrate on Tevatron
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b production at high energies
DO Run I (PRL 84 (2000) 5478) CDF Run I (PRL 85 (2002) 5068)
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DØ
• excellent muon acceptance |η|<2• excellent tracking coverage |η|<3• (impact parameter trigger @L2)
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CDF
• excellent mass resolution• particle id: tof and dE/dx• impact parameter trigger @L2
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Tevatron performance• since June 2003 3-fold
increase in – peak luminosity– integrated luminosity per
week– total integrated luminosity
• instantaneous luminosities above 1032cm-2s-1
• total integrated luminosity just reached 1 fb-1
• analyses shown use 40-300 pb-1
7/9/2005 U. Heintz - PiC 2005 9
b production at Tevatron• b production cross section at √s=1.96 TeV 50b
– rate few kHz at current luminosities
• many developments in theory in recent years– full calculations to NLO – resummation of log(pT/mb) terms (fixed order NLO +NLL FONLL)– substantial changes in fragmentation functions– new pdf’s
leading order next to leading order
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b cross section measurements• J/ and b-hadron production cross
sections (CDF)
• Inclusive b-jet cross section (CDF)
• High pT cross section for -tagged jets (DØ)
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b cross section using J/ (CDF)• use exclusive decays of b-hadrons to
measure the b-production cross section– inclusive J/ cross section– fraction of J/ from decay of b-hadrons
– b-hadron cross section for all pT
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b cross section using J/ (CDF)• J/’s can originate from
– direct production– decay of excited cc-states– decay of b-hadrons
• dimuon trigger– ¼ 300k J/ events– mass resolution 15-
20 MeV
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b cross section using J/ (CDF)• inclusive J/ cross section
nb 12406.0, 21
19 syststatJByXJpp
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b cross section using J/ (CDF)• long life time of b-hadrons
– c¼ 450 m
• J/ decay vertex displaced
• plot pseudo proper decay time x=Lxy m/pT in bins of pT of J/
• max likelihood fit for b-fraction
p pB
K
fb = 9.4%
fb = 33.7%
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b cross section using J/ (CDF)• systematic error on b-fraction ¼ 3-13%
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b cross section using J/ (CDF)• total inclusive b-hadron cross section
b 4.06.176.0, 5.2
3.2 syststatyXhpp b
%10.016.1/ XJhB b
%10.088.5/ JB
comparison with Run I B+ cross sectionRun II scaled for B+ fragmentation, |y|<1
Ldt¼ 40 pb-1 PRD 71, 032001 (2005)
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high-pT b-jet cross section (CDF)• reconstruct b-decay vertex using displaced
tracks in jet
• Rjet=0.7, |yjet|<0.7
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high-pT b-jet cross section (CDF)• determine b-fraction of tagged jets
in bins of jet pT using mass of particles that point to secondary vertex
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high-pT b-jet cross section (CDF)• b-jet cross section for 38<pT<400 GeV
L dt = 300 pb-1
source of syst error low pT high pT
luminosity 6% 6%
jet energy scale 15% 40%
jet energy scale 6% 6%
b-tagging efficiency 10% 15%
b-fraction 10% 40%
unfolding 8% 8%
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high pT -tagged jet cross section (DØ)• first step to b-production cross section• jet with in cone Ldt = 300 pb-1
• Rjet=0.5, |yjet|<0.5
• 4660 -tagged jets
• PYTHIA: 55% of all -tagged jets from heavy flavor (b,c)
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high pT -tagged jet cross section (DØ)• unsmear detector resolution
NLO: Z. Nagy, Phys. Rev. D 68, 094002
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what changed?• long-standing “discrepancies” between predicted
and measured cross sections seem resolved• better theory:
– sum terms with log(pT/mb) (FONLL) • e.g. Cacciari, Frixione,Mangano, Nason, Ridolfi, JHEP 0407 (2004) 033
– better understanding of fragmentation functions– better estimate of theory errors (upward!)
• better parton distributions: – add more gluons
• better experimental observables:– not b-quarks but b-hadrons
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quarkonia production• slightly different theoretical context
– non-relativistic QCD (NRQCD) • Lepage et al., PRD 46 4052 (1992)
– production described by short distance cross sections and nonperturbative matrix elements for evolution to quarkonium state.
– color octet modes required on top of color singlet to describe production (demonstrated by CDF in Run I)
• results: – DØ: Υ(1s) production, Υµµ final state– CDF: prompt J/ polarization
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Y(1S) production (DØ)• test boundary between perturbative and non-perturbative QCD
– perturbative color singlet production suppressed by s
– color evaporation (soft gluons carry away color/spin non-perturbative)
– perturbative color octet production can reproduce high pT region
• V.A. Khoze , A.D. Martin, M.G. Ryskin, W.J. Stirling, hep-ph/0410020
– resum logs to address low pT region
• E.L. Berger, J.Qiu, Y.Wang, Phys Rev D 71 034007 (2005)
color singlet process color octet process
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Y(1S) production (DØ)• unlike charmonium,
all bb-states are produced directly
• 50% of Y(1S) from decay of other bb-states
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Y(1S) production (DØ)• fix mass splittings and relative widths in fit
• 5 free parameters: – m(1S), (1S), n(1S), n(2S), n(3S)
|y(Y)|<0.6 0.6<|y(Y)|<1.2 1.2<|y(Y)|<1.8
all three: 4 GeV < pT(Y) < 6 GeV
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Y(1S) production (DØ)• little variation in the shape of
the cross section as a function of rapidity
• reasonable agreement with calculations by Berger et al, hep-ph/0411026
Ldt = 159 pb-1 hep-ex/0502030, PRL 94 232001 (2005)
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prompt J/ polarization (CDF)• large prompt J/ cross section (Run I)
– color octet mechanism Braaten/Fleming PRL 74 3327 (1995)
– transversely polarized J/ at large pT
transverse alignment (symmetric decays)
longitudinal alignment (asymmetric decays)
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HERA• contributing processes:
• g fusion• resolved
– contributes to photoproduction
– suppressed at high Q2
• 1999-2000 • H1
– e§ p (72 pb-1)
• ZEUS– e+ p (50 pb-1)
920 GeV
28 GeV
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HERA• + dijet• photoproduction
– Q2<1 GeV2
• H1:– b-identification
• large mass– pT of relative to jet
• long life time– impact parameter of
– vis(epebbXejjX)=38.4§3.4(stat)§5.4(syst) pb– prediction: 23.8-5.1
+7.4 GeV
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HERA• + jet
• deep inelastic scattering– 2 GeV2 < Q2 < 100 GeV
• vis(epebbXejX)=16.3§2.0(stat)§2.3(syst) pb• prediction: 9.0-1.6
+2.6 GeV
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HERA• see discrepancy at low p and high
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HERA• discrepancy at high also seen in ZEUS data
• ZEUS vis(epebbXejX)=40.9§5.7(stat)-4.4
+6.0(syst) pb– prediction: 20.6-2.2
+3.1 GeV
hep-ex/0405069 hep-ex/0502010
7/9/2005 U. Heintz - PiC 2005 34
conclusions• b production at the Tevatron
– finally NLO QCD and data agree• better theory calculation:
– FONLL + fragmentation functions + pdf’s
• well-defined observables
• quarkonium production– Y(1S) production agrees with pQCD + resummation
predictions – J/ is not transversely polarized as expected by color
octet production
• b production at HERA– pQCD predictions are ¼ 2 low– discrepancies at low pT and high
7/9/2005 U. Heintz - PiC 2005 35