factorisation in diffraction
DESCRIPTION
Factorisation in diffraction. Representing H1 and ZEUS experiments. Hadron structure ´09 Tatranská Štrba. Alice Valk árová Charles University, Pra gue. HERA collider experiments. 27.5 GeV electrons/positrons on 920 GeV protons →√s=318 GeV two experiments: H1 and ZEUS - PowerPoint PPT PresentationTRANSCRIPT
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31.08.2009 1Hadron Structure 2009
Factorisation in diffraction
Alice Valkárová Charles University, Prague
Representing H1 and ZEUS experiments
Hadron structure ´09 Tatranská Štrba
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HERA collider experiments• 27.5 GeV electrons/positrons on 920 GeV protons →√s=318 GeV• two experiments: H1 and ZEUS• HERA I: 16 pb-1 e-p, 120 pb–1 e+p• HERA II: ∼ 550 pb-1, ∼ 40% polarisation of e+,e-• closed July 2007, still lot of excellent data to analyse……
e
DIS: Probe structure of proton → F2
Diffractive DIS: Probe structure of
color singlet exchange → F2D
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22
22
IP WQ
MQ
pq
ppqx X
22
2
XIP MQ
Q
x
x
W
´
HERA: ~10% of low-x DIS events are diffractive
Diffraction and diffraction kinematics
momentum fraction of color singlet exchange
fraction of exchange momentum, coupling to γ*
2, )( ppt t
4-momentum transfersquared
My
Two classes of diffractive events:
Q2~0 → photoproductionQ2>>0 → deep inelastic scattering (DIS)
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1) Proton Spectrometers: ZEUS: LPS (1993-2000) H1: FPS (1995-2007),VFPS (2004-07)t measurementaccess to high xIP rangefree of p-dissociation background at low xIP
small acceptance low statistics ☠
2) Large Rapidity Gap, H1, ZEUS:Require no activity beyond η max
t not measured, very good acceptance at low xIP
p-diss background ~ 20% ☠2ln
2lnxMB
x
CeDMd
dN
diff. non-diff
)ln(tan- η 2θ
e
p
Diffractive Event Selection
e
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What is QCD factorisation?
),(),,,()( 2*2
_
* QxtxQxfXpp iIP
D
ipartoni
D
),/(),(),,,( 2/
2 QxxftxftxQxf IPIPiIPpIPIP
Di
Factorisation holds for inclusive and non-inclusive processes when:• photon is point-like (Q2 is high enough)• higher twist corrections are negligible
It allows to extract DPDFs from the (DIS) data
Dif→ DPDFs – obey DGLAP, universal for diff. ep DIS (inclusive,dijet,charm)
i* → universal hard scattering cross section (same as in inclusive DIS)
H1 and ZEUS –QCD fits assuming Regge factorisation for DPDF
pomeron PDF1)(2/ ),( tIP
Bt
IPpIP xe
txf pomeron flux factor
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How to profit from factorisation?
• to extract DPDFs from inclusive DIS and to estimate cross sections for dijet and D* production – then compare with data tests of factorisation
• to extract DPDFs from inclusive and semi-inclusive DIS (dijets,D*) – only semi-inclusive data are sensitive to gluon contribution, mainly at large zIP
Used by H1 and ZEUSsemi-inclusive data dijets in DIS
4 < Q2 < 80 GeV2
0.1 < y < 0.7xIIP < 0.03
P*tjet1 > 5.5 GeVP*tjet2 > 4 GeV-3. < η*jets < 0.
EPJ C52 (2007) 813
JHEP 0710 042 (2007)
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H1 QCD inclusive+dijet fit
Largestdifference
Largestdifference
JHEP 0710:042,2007
AB
A
Inclusive fits A and B
Fit jets uses dijets in DIS
No difference for quarks,large difference for gluonsat large zIP.
jets
Fit A Fit B
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ZEUS QCD inclusive+dijet fit
ZEUS fit C is the fit with same conditions as H1 fit B
The results of fits of both experiments are similar.
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pp
γ*p
Exporting DPDFs fromHERA to Tevatron…..
xIP integrated effective DPDFsfrom CDF single diff. dijets (run I)
Factorisation broken by β-dependent factor ~ 10, S ~ 0.1
Factorisation in hadron-hadron collisions
Must be understood for LHC…e.g. CEP Higgs,(S=1-3%), related to underlying event…..
Succesfully explained by terms of rescatteringand absorption (see Kaidalov,Khoze,Martin,Ryskin:Phys.Lett.B567 (2003),61)
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Tests of factorisation - HERA
• dijets in DIS – factorisation holds – H1 → ZEUS →• D* in DIS and photoproduction -
EPJ C52 (2007) 813
H1 Coll. EPJ C50 (2007) 1
RγpDIS= (data/theory)γp/(data/theory)DIS
Rγp DIS=1.15 ± 0.40 (stat.) ± 0.09 (syst.)
JHEP 0710 042 (2007)
within large errors no evidence for suppression,factorisation holds
ZEUS Coll. EPJ C51 (2007) 301
H1 double ratio
• what about dijets in photoproduction????
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Photoproduction, γ⋆p, Q2→0
direct photoproduction (Q2≃0): photon directly involved in hard scattering
xγ=1 (at parton level)
resolved photoproduction (Q2≃0): photon fluctuates into hadronic
system, which takes part in hadronic scattering,dominant at Q2≃0
xγ<1(at parton level)
hadronsz
jetszOBS
pE
pExx
)(
)(
xγ - fraction of photon’s momentum in hard subprocess
In LO!
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Photoproduction as hadronic process
resolved contribution expected to be suppressed by factor 0.34 see Kaidalov et al.
Typical models that describe suppression at Tevatron assume secondary interactions of spectators as the cause:
HERA resolved photoproduction
Secondary interactionsbetween spectators
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H1: Etjet1 > 5 GeV suppression of factor ~0.5ZEUS: Etjet1 > 7.5 GeV weak (if any) suppression (0.6-0.9)
Neither collaboration sees difference between the resolved and direct regions, in contrast to theory!
Possible explanation of differences between H1 and ZEUS (DIS 2007)Different phase space of both analyses ……..?
2007 - DIS 07….
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H1 – double ratio, Et dependence?
Double ratio of Data/NLO for photoproduction and DIS→
Figure extracted from published results
Double ratio is within errors Et dependent!
Very useful – full or partial cancellation of many uncertainties (energy scales for data, DPDFs used…etc ).
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New H1 analysis -two cut scenarios
To crosscheck previous H1 results To approach closest to ZEUS cuts
Tagged dijet photoproduction, data 99/00, three times larger statistics, LRG
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Integrated survival probabilities (ISP)
No difference in survival probabilitiesfor resolved and direct regions of xγ,
like in previous H1 and ZEUS analyses
Within errors no difference in ISPusing different DPDFs
Lower Et cut scenario
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Higher Et cut scenario
Now much more „direct-like“ events thanin low Et analysis, peak at higher xγ
Integrated survival probabilities (ISP)
Larger ISP than for lower Et cut scenario → more close to ZEUS results!!!
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Published data: EPJ C55 (2008) 177
Very good description → no evidence for suppressionfor ZEUS combined fit and H1 fit jets.
New ZEUS fit-comparison with old data
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Ratio diffractive to inclusiveProposed by Kaidalov et al. Phys.Lett B567 (2003) 61
Distribution of xγ sensitive to gap survival.
H1 - measured in same kinematic rangewith same method as diffractivecross sectionsAcceptance corrections – PYTHIA
Problem → describes low Et inclusive data with inclusion of multiple interactions only,large hadronisation corrections!
With such a low Et jets problems also with NLO description of data –see for example H1 inclusive jet paper (EPJ C 129 (2003) 497)
Full or partial cancellation of PDF uncertainties,scales…..
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Ratio diffractive to inclusive
• comparison to MC models - RAPGAP/PYTHIA• very different phase space for incl.& diffr.• large sensitivity to multiple interactions (MI) for inclusive dijets• better agreement of data ratio with PYTHIA MI
zIP < 0.8
Ep=820 GeV
Ep=930 GeV
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Summary • for dijets in photoproduction gap survival probability: significantily less than 1. for events with low Et leading jets, for higher Et (DPDF H1 fit jets 2007) ~ 0.8, consistent with ZEUS results (ZEUS combined fit 2009) ~ 1.
• hint that suppression is dependent on Et of the leading jet,
→ evidence that gap destruction becomes less likely as Et
increases
• the evidence that suppression is not different for direct and resolved events remains (from theory not expected )
• ratio diffractive dijets/inclusive dijets measured for the first time – the multiple interactions play important role for inclusive dijets → interpretation difficult
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Backup
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Tests of factorisation - HERA
• dijets in DIS – factorisation holds – H1 → ZEUS →• D* in DIS and photoproduction -
EPJ C52 (2007) 813
H1 Coll. Eur.Phys. J C50,1,(2007)
RγpDIS= (data/theory)γp/(data/theory)DIS
Rγp DIS=1.15 ± 0.40 (stat.) ± 0.09 (syst.)
JHEP 0710 042 (2007)
within large errors no evidence for suppression,factorisation holds
DIS
ZEUS coll. EPJ C51 (2007) 301
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Lower Et cut scenario
Another hint of Et harder slope for datathan NLO
Hadronization corrections
δhadr=MC(hadr)/MC(parton)