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LISHEP 2009, M. Ruspa, 21.01.09 1 Inclusive Diffraction at HERA Marta Ruspa (Univ. Piemonte Orientale, Italy) LISHEP 2009 Rio de Janeiro, 19-23 February,

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Presentation on theme: "LISHEP 2009, M. Ruspa, 21.01.09 1 Inclusive Diffraction at HERA Marta Ruspa (Univ. Piemonte Orientale, Italy) LISHEP 2009 Rio de Janeiro, 19-23 February,"— Presentation transcript:

1 LISHEP 2009, M. Ruspa, 21.01.09 1 Inclusive Diffraction at HERA Marta Ruspa (Univ. Piemonte Orientale, Italy) LISHEP 2009 Rio de Janeiro, 19-23 February, 2009  Diffractive structure function data  Regge fits and QCD fits  Data comparisons  H1/ZEUS weighted average

2 LISHEP 2009, M. Ruspa, 21.01.09 2  27.5 GeV electrons/positrons on 920 GeV protons → √s=318 GeV  2 collider experiments: H1 and ZEUS  HERA I: 16 pb -1 e-p, 120 pb –1 e+p HERA II (after lumi upgrade): 500 pb -1, polarisation of e+,e- Closed July 2007, still lot of excellent data to analyse…… HERA collider experiments Detectors not originally designed for forward physics, but diffraction at HERA great success story! ZEUS forward instrumentation no longer available in HERA II

3 LISHEP 2009, M. Ruspa, 21.01.09 3 ´ Standard DIS ´ GAP Diffractive DIS Diffractive DIS at HERA GAP x IP Probes proton structure Probes structure of color singlet exchange According to Regge phenomenology: - exchanged Pomeron (IP) trajectory - exchanged Reggeon (IR) and π when proton loses a higher energy fraction, x IP

4 LISHEP 2009, M. Ruspa, 21.01.09 4  Single diffractive dissociation: N=proton  Double diffractive dissociation: proton-dissociative system N  represents a relevant background x IP Probe structure of proton → F 2 ´ Standard DIS ´ Kinematics of diffractive DIS GAP Q2Q2 W t Q 2 = virtuality of photon = = (4-momentum exchanged at e vertex) 2 W = invariant mass of γ * -p system M X = invariant mass of γ * -IP system x IP = fraction of proton’s momentum carried by IP ß = fraction of IP momentum carried by struck quark x = β ∙ x IP, Bjorken’s scaling variable t = (4-momentum exchanged at p vertex) 2 typically: |t|<1 GeV 2

5 LISHEP 2009, M. Ruspa, 21.01.09 5 x IP Why study diffractive DIS? ´ ´ GAP Q2Q2 W t  Significant fraction of the inclusive DIS cross section  New window on QCD  transition from soft to hard regimes  parton dynamics at low x  applicability of QCD factorisation approach  DPDFs essential to predict diffractive processes and potential search channels at the LHC

6 LISHEP 2009, M. Ruspa, 21.01.09 6 f i/p (z,Q 2,x IP, t) expresses the probability to find, with a probe of resolution Q 2, in a proton, parton i with momentum fraction z, under the condition that the proton remains intact, and emerges with small energy loss, x IP, and momentum transfer, t – the DPDFs are a feature of the proton and evolve according to DGLAP  Assumption  proton vertex factorisation: At large x IP, a separately factorisable sub-leading exchange (IR), with different x IP dependence and partonic composition  Diffractive DIS, like inclusive DIS, is factorisable: [Collins (1998); Trentadue, Veneziano (1994); Berera, Soper (1996)…] QCD factorization in hard diffraction universal partonic cross section Diffractive Parton Distribution Function (DPDF) Regge-motivated IP flux σ (γ*p  Xp) ≈ f i/p (z,Q 2,x IP,t) x σ γ*q (z,Q 2 ) σ (γ*p  Xp) ≈ f IP/p (x IP,t) x f i/IP (z,Q 2 ) x σ γ*q (z,Q 2 )

7 LISHEP 2009, M. Ruspa, 21.01.09 7 LPS method PROS: no p-diss. background direct measurement of t, x IP high x IP accessible CONS: low statistics PROS: near-perfect acceptance at low x IP CONS: p.-diss background Diffractive event selection Large Rapidity Gap (LRG) method η max cut M x method Fit: D + c∙ e b∙lnM X 2 ZEUS Leading Proton Spectrometer (LPS) H1 Forward Proton Spectrometer (FPS) x L = p z ’ /p z

8 LISHEP 2009, M. Ruspa, 21.01.09 8 Data sets “ZEUS LPS” [arXiv:0812.2003, submitted to NPB] “ZEUS LRG” [arXiv:0812.2003, submitted to NPB] x IP up to 0.1 x IP up to 0.02M N =m P “ZEUS FPC II” (M X method) [NPB 800 (2008)] “ZEUS FPC I” (M X method) [NPB 713 (2005)] IR suppressed M N < 2.3 GeV 35% of LPS events selected by LRG Overlap LRG-M X ~75% “H1 FPS” [EPJ C48 (2006)] “H1 LRG” [EPJ C48 (2006)] x IP up to 0.1 x IP up to 0.03M N < 1.6 GeV FPS and LRG measurements statistically independent and only very weakly correlated through systematics ZEUS H1 x IP coverageM N coverage

9 LISHEP 2009, M. Ruspa, 21.01.09 9  Diffractive cross section  Diffractive structure function F 2 D(4) and reduced cross section σ r D(4)  When t is not measured  R D = σ L γ*p  Xp /σ T γ*p  Xp ; σ r D = F 2 D when R D = 0 Diffractive structure function

10 LISHEP 2009, M. Ruspa, 21.01.09 10 How does diffraction behave vs t, x IP, Q 2 ?

11 LISHEP 2009, M. Ruspa, 21.01.09 11 t dependence LPS data LISHEP 2009, M. Ruspa, 21.01.2009 Fit to e -b|t|  b = 7.0 ± 0.4 GeV -2 0.0002<x IP <0.010.01<x IP <0.1 2<M X <5 GeV5<M X <10 GeV10<M X <40 GeV

12 LISHEP 2009, M. Ruspa, 21.01.09 12 t dependence LPS/FPS data 2<M X <5 GeV5<M X <10 GeV10<M X <40 GeV  Support Regge factorisation hypothesis

13 LISHEP 2009, M. Ruspa, 21.01.09 13 LISHEP 2009, M. Ruspa, 21.01.2009 x IP dependence of σ r D(4) LPS data First measurement in two t bins  Low x IP : σ r D(4) falls with x IP faster than 1/x IP  High x IP : x IP σ r D(4) flattens or increases with x IP (Reggeon and π)  Same x IP dependence in two t bins |t|= 0.13 GeV 2 |t| = 0.3 GeV 2

14 LISHEP 2009, M. Ruspa, 21.01.09 14 LISHEP 2009, M. Ruspa, 21.01.2009 Regge fit LPS/FPS data α IP (0) = + 1.11 ± 0.02(stat) + 0.01 - 0.02(syst) +++++++++++++ 0.02(model) α’ IP = - 0.01 ± 0.06(stat) + 0.04 - 0.08(syst) GeV -2 H1: α IP ’ = + 0.06 + 0.19 - 0.06 GeV -2 α IP (0) = + 1.114 ± 0.018(stat) ciao ± 0.013(syst) ciao + 0.040 - 0.020(model)  Assumption of Regge factorisation works  IP intercept consistent with soft IP (1.096)  α’ IP significantly smaller than 0.25 GeV -2 of hadron-hadron collisions α IP (t) = α IP (0) + α’ IP ∙ t |t|= 0.13 GeV 2 |t| = 0.3 GeV 2

15 LISHEP 2009, M. Ruspa, 21.01.09 15  Rise with x IP not visible as x IP < 0.02 LISHEP 2009, M. Ruspa, 21.01.2009 x IP dependence of σ r D(3) ZEUS LRG data

16 LISHEP 2009, M. Ruspa, 21.01.09 16 LISHEP 2009, M. Ruspa, 21.01.2009  Rise with x IP not visible as x IP < 0.02  Wide kinematic coverage and very good statistical precision x IP dependence of σ r D(3) ZEUS LRG data

17 LISHEP 2009, M. Ruspa, 21.01.09 17 Regge fit ZEUS LRG data α IP (0) = 1.108 ± 0.008(stat+syst) +0.022 - 0.007(model)  Assumption of Regge factorisation works LISHEP 2009, M. Ruspa, 21.01.2009

18 LISHEP 2009, M. Ruspa, 21.01.09 18 Q 2 dependence of σ r D(3) ZEUS FPC data  At fixed β shape depends on x IP : this data seem to contradict Regge factorisation assumption

19 LISHEP 2009, M. Ruspa, 21.01.09 19 Apparent contradiction: - Regge fit works within errors for LPS/FPS and LRG data - FPC and LRG (see later) show violation of Regge factorisation  Data consistent with Regge factorisation; violation too mild to have impact on the fit quality What if we fitted LPS/FPS/LRG without assuming Regge factorisation? Not done yet but done for the FPC data  BEKW fit works well! [Bartels, Ellis, Kowalski, Wustoff, see NPB 800 (008)] Mild violations should not affect QCD fits, which assume factorisation Regge factorisation: yes or no? (my interpretation)

20 LISHEP 2009, M. Ruspa, 21.01.09 20 F 2 σ r D(3) shows positive scaling violations up to high-β values  Diffractive exchange is gluon-dominated Q 2 dependence of σ r D(3) ZEUS FPC data

21 LISHEP 2009, M. Ruspa, 21.01.09 21 Diffractive Parton Distribution Functions

22 LISHEP 2009, M. Ruspa, 21.01.09 22 Reduced cross section constrains quark density lnQ 2 dependence constrains gluon density DPDFs extraction H1 LRG data

23 LISHEP 2009, M. Ruspa, 21.01.09 23 Regge factorisation assumed Fit A: zg(z,Q 0 2 ) = A(1-z) C Fit B: C=0, gluon constant at Q 0 2  Well constrained singlet  Weakly constrained gluons, exp. at high values of z needed further input DPDFs extraction z = fractional momentum of the diffractive exchange participating to the hard scattering

24 LISHEP 2009, M. Ruspa, 21.01.09 24 Fit A: zg(z, Q 0 2 ) = A(1-z) C Fit B: C=0, gluon constant at Q 0 2 Fit JET: zg(z,Q 0 2 )=Az B (1-z) C  The singlet and gluons are constrained with similar precision across the whole kinematic range Combined fit H1 LRG+dijet data jet X Y See A. Valkarova ’ s talk

25 LISHEP 2009, M. Ruspa, 21.01.09 25 Comparison between data sets

26 LISHEP 2009, M. Ruspa, 21.01.09 26 ZEUS LPS vs H1 FPS The cleanest possible comparison in principle … … but large normalisation uncertainties (LPS:+11-7%, FPS: +-10%)  ZEUS and H1 proton-tagged data agree within normalisation uncertainties

27 LISHEP 2009, M. Ruspa, 21.01.09 27  Proton dissociation left in H1 LRG data: [19+-11]% Consistent number obtained with DIFFVM: [13 +11 -6]% Data first corrected to M N < 1.6 GeV (corr. factor: -8.6% ± 5.8%) H1 LRG vs H1 FPS Proton dissociation-background in the H1 LRG data  LRG/FPS independent of x IP, Q 2, β

28 LISHEP 2009, M. Ruspa, 21.01.09 28  LPS/LRG independent of Q 2, x IP, β, as in the H1 case: proton vertex factorises  Fraction of proton-dissociative background in the ZEUS LRG data: [24 +-1(stat) +2-3(sys) +5-8(norm)]% Consistent number obtained with PYTHIA: [25 +-1(stat) +-3(sys) ]% ZEUS LRG vs ZEUS LPS Proton dissociation-background in the ZEUS LRG data  Similarity between ZEUS and H1 p.-diss fraction expected given similar forward detector acceptance  Precise knowleadge (and correction) of p.-diss background key point in the data comparison!

29 LISHEP 2009, M. Ruspa, 21.01.09 29 ZEUS LRG vs ZEUS FPC DIS08, London, M. Ruspa 07/04/08 FPC data (M N < 2.3 GeV) normalised here to LRG (M N =m p ): factor 0.83 ± 0.04 (determined via a global fit) estimates residual p-diss. background in FPC sample  Overall agreement satisfactory  Different x IP dependence ascribed to IR suppressed in FPC data

30 LISHEP 2009, M. Ruspa, 21.01.09 30 ZEUS LRG vs H1 LRG ZEUS corrected to M N < 1.6 GeV with PYTHIA  Remaining normalisation difference of 13% (global fit) covered by uncertainty on p-diss. correction (8%) and relative normalisation uncertainty (7%)  Shape agreement ok except low Q 2 DIS08, London, M. Ruspa 07/04/08

31 LISHEP 2009, M. Ruspa, 21.01.09 31 DIS08, London, M. Ruspa 07/04/08 (M N < 1.6 GeV)x0.87 (M N < 1.6 GeV) Towards HERA inclusive diffraction!  Time for data combination, global fits!

32 LISHEP 2009, M. Ruspa, 21.01.09 32 DIS08, London, M. Ruspa 07/04/08 (M N < 1.6 GeV)x0.87 (M N < 1.6 GeV) Towards HERA inclusive diffraction!  Time for data combination, global fits!

33 LISHEP 2009, M. Ruspa, 21.01.09 33 First step towards the data combination Error weigthed average:  before averaging, H1 points swum to ZEUS Q 2 values with H1 fit B  ZEUS normalised to H1 applying 13% factor (see slide 36)  normalisation uncertainty of combined data beyond 10%  correlations between systematic errors ignored so far Hints at precision achievable through combination: for many points errors at 3-4% level (excluding normalisation uncertainty)

34 LISHEP 2009, M. Ruspa, 21.01.09 34 First step towards the data combination Error weigthed average:  before averaging, H1 points swum to ZEUS Q 2 values with H1 fit B  ZEUS normalised to H1 applying 13% factor (see slide 36)  normalisation uncertainty of combined data beyond 10%  correlations between systematic errors ignored so far Hints at precision achievable through combination: for many points errors at 3-4% level (excluding normalisation uncertainty)

35 LISHEP 2009, M. Ruspa, 21.01.09 35 Highlights  A wealth of inclusive diffractive data from ZEUS and H1: consistency reached between different experiments, methods and data sets  Data ready to be combined and/or fitted globally!  Diffractive parton density functions available which can be used to predict other processes  Inclusion of dijet data in the QCD fits provides a much better constraint of the gluon density at high fractional momentum

36 LISHEP 2009, M. Ruspa, 21.01.09 36 Backup

37 LISHEP 2009, M. Ruspa, 21.01.09 37 x IP dependence of σ r D(4) FPS data

38 LISHEP 2009, M. Ruspa, 21.01.09 38 W dependence of dσ diff /dM X ZEUS M X data  Low M X : moderate increase with W and steep reduction with Q 2  Higher M X : substantial rise with W and slower decrease with Q 2

39 LISHEP 2009, M. Ruspa, 21.01.09 39  Substantial rise with W W dependence of dσ diff /dM X ZEUS M X data HERALHC Workshop, M. Ruspa, 27/05/08

40 LISHEP 2009, M. Ruspa, 21.01.09 40 Why is the high β gluon so poorly known?  Low β: evolution driven by g  qqbar, Q 2 dependence of σ r D(3) sensitive to the gluon density  With increasing β relative error on derivative and hence on the gluon density larger  High β: evolution driven by q  qg Q 2 dependence of σ r D(3) not sensitive to the gluon density

41 LISHEP 2009, M. Ruspa, 21.01.09 41 Combined fit H1 LRG+dijet data See A. Valkarova ’ s talk

42 LISHEP 2009, M. Ruspa, 21.01.09 42 Proton dissociation @ZEUS: correction to M N = m p ii) Monte Carlo (PYTHIA)  2 samples of proton- dissociative data, one with LPS ( “ LPS P-DISS ” ) and one with Forward Plug Calorimeter ( “ LRG P-DISS ” )  coverage of full M N spectrum  PYTHIA reweigthed to best describe E FPC and x L  p-diss. background in LRG data R diss = [25 +-1(stat) +-3(sys) ]%  consistent with the ratio LPS/LRG  25% correction applied to LRG data

43 LISHEP 2009, M. Ruspa, 21.01.09 43 DIS08, London, M. Ruspa 07/04/08 (M N < 1.6 GeV)x0.87 (M N < 1.6 GeV) Towards HERA inclusive diffraction!  Time for data combination, global fits!

44 LISHEP 2009, M. Ruspa, 21.01.09 44 DIS08, London, M. Ruspa 07/04/08 (M N < 1.6 GeV)x0.87 (M N < 1.6 GeV) Towards HERA inclusive diffraction!  Time for data combination, global fits!

45 LISHEP 2009, M. Ruspa, 21.01.09 45 Fit with BEKW parameterisation (Bartels, Ellis, Kowalski, Wustoff 1988) L limited to β ~1  Fit gives a good description of the 427 data points FPC I + II

46 LISHEP 2009, M. Ruspa, 21.01.09 46 Q 2 dependance of α IP (0)  α IP (0) does not exhibit a significant dependance on Q 2

47 LISHEP 2009, M. Ruspa, 21.01.09 47 Diffr. Non-diffr.  D, c, b from a fit to data  contamination from reaction ep  eXN Properties of M x distribution: - exponentially falling for decreasing M x for non- diffractive events - flat vs ln M x 2 for diffractive events Forward Plug Calorimeter (FPC): CAL acceptance extended by 1 unit in pseudorapidity from η=4 to η=5  higher M x and lower W  if M N > 2.3 GeV deposits E FPC > 1 GeV recognized and rejected! Diffr. Non-diffr. M X method

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