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pQCD%20?%20JETS

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Kinematics of Neutral Current (NC) Deep Inelastic Scattering (DIS) Luca Stanco - Padova ... H1 data in the kinematic region: Luca Stanco - Padova. QCD at HERA, ... – PowerPoint PPT presentation

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Title: pQCD%20?%20JETS


1
LISHEP 2006 Workshop Rio de Janeiro, April 3-7,
2006
pQCD ? JETS
(AND)
at HERA
Luca Stanco INFN Padova
on behalf of H1 and ZEUS collaborations
2
more or less
Single particles production Charged
multiplicities Bose-Einstein correlation Neutral,
strange, Baryons Charm fragmentation Remnant/Multi
ple interactions Prompt Photon Resolved-Direct
g-production Parton Evolutions Color dynamics,
Energy flow Multiscale Strong coupling Dijets,
Trijets Inclusive Jets production Forward Jets
production Heavy Quarks Jets Diffractive Jets
QCD items
JETS items
3
QCD
  • WHAT ?

4
WHY ?
at least 3 answers
  1. NOT TRUE it is so well understood ..
  2. Strong coupling, aS, measurement
  3. Parton Density Functions measurements (see
    previous talk)

5
Z.Czyczula et al., pT of Higgs (120 GeV) from
different Parton-Showers (PS) models and QCD
scale choices
  • Uncertainties
  • up to 170 due to PS (which evolution type ?
    which ordering ?)
  • up to 100 due to the choice of QCD scale (Q2,
    m2, s etc.)

? low-x and forward jets
6
HOW ?
7
before going into physics, let us look at
environment...
Results on pQCD?JETS only from HERA-I (up till
now)
8
...if nobody else has already shown ...
9
Kinematics of Neutral Current (NC) Deep
Inelastic Scattering (DIS)
10
Processes at HERA
(defined by Initial States of HARD Scattering)
Electron beam
Proton beam
quark/gluon PARTONS
11
Jets Production in NC Deep Inelastic Scattering
12
Inclusive JETS in DIS
The BREIT frame !
  • Frame where virtual boson
  • is enterely spacelike
  • At lowest order, quark is
  • back scattered

In pratice, high Et jet events must be at least
of order aS
13
JETS observables in the BREIT Frame
more technically
14
NLO pQCD calculations
and
  • interfaced to various PDFs (like CTEQ, MRST)
  • Parton Level cross sections need to rely on LO
    MC for hadronisation
  • corrections

15
Excellent agreement between DATA and NLO over
many orders of magnitude !
16
...and the experimental error is smaller than the
theoretical one !
17
ZEUS Inclusive Jet Production in DIS
18
measurements at different Q2 also for ZEUS
19
Running and Extraction of aS from Inclusive jets
aS vs Et
aS vs Q2
Best result for Q2 bins with Q2gt500 GeV2 ?
uncertainties minimised
20
and H1
before showing the whole sets of aS measurements,
look at the MULTI-JET data sets ?
21
Di-Jet and Tri-Jet PRODUCTION in DIS
larger errors, but ...
The aS dependency of their ratio is a sensitive
test of pQCD
22
3-jet / 2-jet cross section ratio
23
aS measurements from 3-jet / 2-jet cross section
ratio
H1
room for improvements (HERA-II)
24
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25
aS running
26
JETS in g-production
again, another testing ground for QCD
27
Well observed from the first days
ZEUS
xg0.8 cut
28
H1
Proton structure
More QCD fits from H1 will come !
29
Similar situation for ET distributions
ZEUS high Et di-jets in g-p
  • Consider the enriched sample of
  • direct-g
  • Good agreement with NLO at high ET
  • small experimental uncertainties
  • ? jet energy scale (?1)
  • ? 5 on the cross section
  • small theoretical uncertainties

30
Gluon Parton Distribution
  • Disadvantages of ortodox method (inclusive ep
    scattering)
  • gluon distribution contributes indirectly
  • Fixed-target DIS higher twists, heavy target
    corrections,
  • isospin symmetry assumption
  • With HERA, sufficient sensitivity to determine
    the proton PDF within a single (ep) experiment.
  • Use of measurements of jet cross section
  • Directly sensitive to the gluon density with
    small
  • experimental theoretical uncertainties

Recent results from ZEUS on old data are very
good, improving the determination of the proton
PDF
31
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32
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33
Color and sub-jet dynamics
Photo-production of three-jet events
Direct-g processes provide a clean way to study
the effects of the different color configuration
34
Angular observables for angular correlations
Comparisons to fixed order calculations based on
different symmetry group
The prediction of SU(3) describes reasonably well
the data
35
ZEUS Sub-jet distributions
DIS
36
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37
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38
H1 g-p data
The jets in the region xglt0.75 are broader than
in the region xggt0.75
Consistent with a larger fraction of gluon
(broad) jets in resolved-photon events than in
direct-photon events
39
QCD dynamics
HERA DIS at low-xBj down to 10-5 ? large
gp center of mass energy (W)
Inclusive F2 measurement not able to
discriminate between different QCD approaches ?
Study of Hadronic Final States (JETS)
40
HERA extends xBj until 10-5
  • FORWARD JETS
  • (proton direction)

possibility to study parton dynamics, by looking
for effects beyond DGLAP
Caveat different Monte Carlo models not clear
where applicable
41
H1 data in the kinematic region
  • LO-DGLAP fails completely !
  • NLO-DGLAP well below data at low-x
  • Monte Carlo models with extra parton
  • radiation provide an improved description
  • of the data
  • inclusion of a resolved-photon component
  • (RG-DIRES)
  • parton emissions not ordered in kT (CDM)

42
ZEUS data less striking (NLO(aS2)-DISENT MC
below the data but within theoretical errors) ?
needs of next NLO ?
( but ZEUS uses mR2Q2, while H1 takes
mR2ltpT2gt )
Is it a HERA business ? or HERA phase space too
limited to distinguish between different
evolution models ?
43
...if nobody else is going to show ...
Definitively, physics has to be clarified.
Also consider Structure Functions results at low-x
44
Conclusions
  • QCD is a lively field at HERA !
  • Up till now studies on 1996-2000 DATA
  • Statistical Theoretical errors
  • HERA-II will lower systematics errors
  • Need THEORY works !
  • Most precise aS measurement !
  • Use of Jets for PDF
  • Forward Jet discrepancy
  • pQCD evolution(s) not clear yet
  • low-xBj regime not clear yet

45
Backup Slides
46
PENTAQUARKS at HERA
q(1530) still compatibility ZEUS/H1, need
HERA-II DATA
47
Not seen by ZEUS
qC(3100) still compatibility H1/ZEUS, need
HERA-II DATA
48
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