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Lowx AND Low Q2

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Parton Density Functions measurements. Parton evolutions ... Also consider Structure Functions results at low-x. Luca Stanco - Padova ... – PowerPoint PPT presentation

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Title: Lowx AND Low Q2


1
Small-x and Diffraction 2007 Workshop FermiLab,
March 28-30, 2007
Low-x AND Low Q2
at HERA with JETS
Luca Stanco INFN Padova
on behalf of H1 and ZEUS collaborations
2
Kinematics of Neutral Current (NC) Deep
Inelastic Scattering (DIS)
W gP c.o.m. energy
3
Processes at HERA
(defined by Initial States of HARD Scattering)
Electron beam
low-x regime
Proton beam
gluons quarks PARTONS
4
HERA exploits many (correlated) processes over
large kinematic regimes !
Q2
XBj
LHC
Tevatron
  • Allow to take care of
  • low-x effects
  • saturation
  • multiple interactions

HERA
perturbative
QCD DYNAMICS (DGLAP vs BFKL evolutions)
Non-pert
Low-x regime
5
...if nobody else have already shown ...
Gluons and QCD dynamics
6
WHY studying pQCD ?
at least 4 answers
  • NOT TRUE it is so well understood ..
  • Strong coupling, aS, measurement (see next talk)
  • Parton Density Functions measurements
  • Parton evolutions

7
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
8
Hard FORWARD Jets (near proton direction where
effects of gluon radiation should be largest -
A. Mueller 1990)
9
before going into physics, let us look at the
environment...
  • HeraI H1 and ZEUS took
  • about 130 pb-1
  • 2001 luminosity upgrade
  • 2002/03 background problems
  • 2004 positrons (50 pb-1)
  • 2005 electrons
  • 2006 positrons
  • 2007 from March HERA for
  • Low Energy Run (FL measure)
  • END oh HERA PETRAIII

H1 and ZEUS will end up with 0.5 fp-1, each
Results on JETS mainly from HERA-I (up till now)
10
QCD dynamics Evolution Resummation
HERA DIS at low-xBj down to 10-5 ? large
gp center of mass energy (W 1/x)
11
two different parton ladders.
?Expect more energetic jets in forward region
(LEPTO, DISENT)
(ColorDipM)
(CASCADE)
12
saturation
Inclusive F2 measurement not able to
discriminate between different QCD approaches ?
Study of Hadronic Final States (JETS)
13
HERA extends xBj until 10-5 (with jets until 10-4)
  • FORWARD JETS
  • (proton direction)

possibility to study parton dynamics, by looking
for effects beyond DGLAP
  • Where ? in the BREIT frame
  • where virtual boson is enterely spacelike
  • at lowest order, quark is back scattered

Caveat different Monte Carlo models not fully
clear where applicable
14
JETS observables in the BREIT Frame
more technically
15
NLO pQCD calculations
and
  • interfaced to various PDFs (like CTEQ, MRST)
  • Parton Level cross sections need to rely on LO
    MC for hadronisation
  • corrections

16
FORWARD JETS
H1 data in the kinematic region
L13.7 pb-1
10-4ltxlt4.10-3 and 5ltQ2lt85 GeV2
  • 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
  • (RAPGAP DIRES)
  • parton emissions not ordered in kT (CDM)

0.5 lt (pT,jet)2/Q2 lt 2 to suppress DGLAP and
enhance BFKL
17
FORWARD JETS
ZEUS data less striking
L81.8 pb-1
4.10-4ltxlt5.10-3 and 20ltQ2lt100 GeV2
E?jetgt5 GeV, 2lthjetlt3.5
0.5 lt (E?jet)2/Q2 lt 2
18
FORWARD JETS
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 ?
19
Very detailed investigation from H1 to enhance
BFKL phase space
Select dijets plus forward-jet
  • different Dh1 and Dh2
  • regions affect
  • Kt-ordering
  • Gluon radiation
  • Evolution chain

Compute differential cross-sections of Dh1 Dh2
20
FORWARD JETS
Data towards NLO
too little Phase Space for NLO
21
FORWARD JETS
Data towards CCFM
NO description !
Data towards CDM and gres
gres not sufficient
CDM may mimic BFKL evolution
22
MULTIJETS (dijets, trijets) ANALYSIS
Kinematic selection to enhance (unordered) gluon
radiation and to study parton dynamics (at low-x)
H1 ?Ldt 44.2 pb-1
10-4ltxBjlt10-2, 5ltQ2lt80 GeV2
ZEUS ?Ldt 82.2 pb-1
10-4ltxBjlt10-2, 10ltQ2lt100 GeV2
Hadronic Center-of-Mass (like Breit-frame boosted)
Comparisons with NLO at order O(aS2) and O(aS3)
NLOJET, DISENT
Conparisons with Monte Carlos LO-PS with/out
gres (CDM-DJANGOH, RAPGAP)
H1 compares to parton level, ZEUS compares to
hadron level
23
MULTIJETS JETS
H1
All the data
Low-x
E?gt 4 GeV, E?1E?2gt 9 GeV
24
MULTIJETS JETS
H1
Select TWO subsamples with Forward JETS
(qjetlt200, xjetEjet/Ep gt 0.035)
NLO comparison
NLO at O(aS3) GREAT !
One central jets plus two forward
Two central jets plus one forward
25
MULTIJETS JETS
H1
LO Monte Carlos comparison
RAPGAP directresolved contributions
Resolved contribution NOT working !
26
MULTIJETS JETS
ZEUS
NLO not bad
27
MULTIJETS JETS
ZEUS
Dijets comparison
NLO consistent.
28
MULTIJETS JETS
ZEUS
Trijets comparison
but theor. errors (mF, mR) too large
Need next order
29
...if nobody else is going to show ...
Definitively, physics has to be clarified.
Also consider Structure Functions results at low-x
30
Conclusions
  • low-xBj regime very messy at HERA
  • Statistical Theoretical errors
  • need more data and theory computations
  • unordered gluon emission significant at low-x ?

A VERY EXCITING FIELD WHERE TO LOOK DEEPLY
INSIDE QCD PARTON EVOLUTION DYNAMICS
31
Backup Slides
32
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
33
Jets Production in NC Deep Inelastic Scattering
34
5 jets event at low-x (H1)
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