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Janusz Szuba (DESY) On behalf of ZEUS and H1 Collaborations Inclusive diffraction in DIS Lake Louise Winter Institute 2009 Introduction Results in inclusive diffraction Diffractive parton density functions Summary

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Page 1: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Janusz Szuba (DESY)

On behalf of ZEUS and H1 Collaborations

Inclusive diffraction in DIS

Lake Louise Winter Institute 2009

•Introduction

•Results in inclusive diffraction

•Diffractive parton density functions

•Summary

Page 2: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Diffractive DIS at HERA

2

pe pe

Inclusive DIS Diffractive DIS

•Photon probes internal structure of proton

•Parton densities in proton

•Photon probes internal structure

of colorless exchange - Pomeron

•Parton densities in Pomeron

LRG

Large Rapidity Gap

Page 3: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Diffractive DIS kinematics and cross section

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Q2 = virtuality of photon =

= (4-momentum exchanged at e vertex)2

MX = invariant mass of γ* -IP system

xIP = fraction of proton’s momentum

carried by IP

ß = Bjorken’s variable for the IP

= fraction of IP momentum

carried by struck quark

= x/xIP

t = (4-momentum exchanged at p vertex)2

typically: |t|<1 GeV2

t is integrated over when not measured:

Reduced cross section

Page 4: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Factorisation in diffractive DIS

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Universal diffractive

parton density functions

Hard scattering

cross section

QCD factorisation at fixed xIP and t (Collins)

Proton vertex factorisation of (β, Q2) from (xIP, t)

This is the basis of performing Regge and NLO QCD (DGLAP) fits

to extract diffractive parton distribution functions

Pomeron flux Partonic structure

Page 5: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Experimental signatures of diffraction

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LPS method

Pros: no proton-diss. background

direct measurement of t and xIP

Cons: limited statistics

xL=p’z/pz

Large rapidity gap (LRG) method MX method

Pros: large acceptance

Cons: proton diss. background

ZEUS Leading Proton Spectrometer (LPS)

H1 Forward Proton Spectrometer (FPS)

Fit: D + c∙ eb∙lnMX

2

Page 6: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Data sets

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“ZEUS LPS” [arXiv:0812.2003, submitted to NPB]

“ZEUS LRG” [arXiv:0812.2003, submitted to NPB]

xIP up to 0.1

xIP up to 0.02 MN=mP

“ZEUS FPC II” (MX method)[NPB 800 (2008)]

“ZEUS FPC I” (MX method)[NPB 713 (2005)]

IR suppressed

IR suppressed

MN < 2.3 GeV

MN < 2.3 GeV

35% of LPS events selected by LRG Overlap LRG-MX ~75%

“H1 FPS” [EPJ C48 (2006)]

“H1 LRG”[EPJ C48 (2006)]

xIP up to 0.1

xIP up to 0.03 MN < 1.6 GeV

FPS and LRG measurements statistically independent and only very weakly correlated through systematics

ZEUS

H1

Page 7: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

New LRG ZEUS

results

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Wide kinematic coverage and

very good precision

Page 8: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Inclusive diffractive

cross section

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H1/

H1 and ZEUS measurements

in good agreement

ZEUS cross section scaled

by 13% to account for

normalization and proton

dissociation background

uncertainties

Page 9: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Inclusive diffractive

cross section (2)

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ZEUS and H1 proton-tagged

data agree within normalisation

uncertainties

H1/

Page 10: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Diffractive PDFs

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NLO QCD (DGLAP) fits to inclusive cross sections – as in proton PDFs extraction from inclusive DIS

Different gluon density parameterisations: Fit A and Fit B

Quark distributions are well constrained

Gluons weakly constrained especially at high z – need further input

Pomeron is dominated by gluons

z = fractional momentum of the diffractive

exchange participating to the hard scattering

Page 11: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Comparison with diffractive dijet in DIS

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At low zIP (< 0.3) Fit A and Fit B are similar

At high zIP the diffractive dijet data clearly prefer Fit B

Include the diffractive dijet in DIS in simultaneous fit with inclusive diffraction data

Sensitive to gluon

Page 12: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Combined fit of diffractive dijets and

inclusive DIS data

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The diffractive dijet data can be used as an additional constraint in a NLO QCD fit procedure

Details of a fit similar to the inclusive case but can now constrain 3 parameters for the gluon

Very good simultaneous fit of both inclusive and dijet data achieved

Page 13: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Combined fit

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New PDFs are similar to Fit B but different from Fit A

Quarks and gluons are constrained with similar precision over the whole kinematic range

Page 14: Slajd 1bib-pubdb1.desy.de/record/87740/files/llwi09-j.szuba.pdf · Title: Slajd 1 Author: jszuba Created Date: 2/21/2009 6:43:02 AM

Summary

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A wealth of diffractive data from ZEUS and H1

using Leading Proton, LRG and MX methods

Consistency reached for different experiments and

methods

Inclusion of dijets data into in the QCD fits

provides a much better constraint of the gluon

density at high fractional momentum

Higher precision expected through combining H1

and ZEUS data