H1 FPS + ZEUS LPS1 FPS/LPS Combination Preliminary request M.Ruspa, V. Sola, M.Kapishin, R.Polifka.

Slides:



Advertisements
Similar presentations
Measurement of F 2 and F L at low Q 2 in ep Interactions at HERA  H1 and ZEUS analyses at low Q 2  Extraction of F L  Summary and Outlook Tomáš Laštovička.
Advertisements

ZEUS high Q 2 e + p NC measurements and high-x cross sections A.Caldwell Max Planck Institute for Physics On behalf of the ZEUS Collaboration Allen Caldwell.
Low x workshop Helsinki 2007 Joël Feltesse 1 Inclusive F 2 at low x and F L measurement at HERA Joël Feltesse Desy/Hamburg/Saclay On behalf of the H1 and.
Effect of b-tagging Scale Factors on M bb invariant mass distribution Ricardo Gonçalo.
Interjet Energy Flow. Patrick Ryan, Univ. of Wisconsin Collaboration Meeting, June 6, Patrick Ryan University of Wisconsin Claire Gwenlan Oxford.
14 Sept 2004 D.Dedovich Tau041 Measurement of Tau hadronic branching ratios in DELPHI experiment at LEP Dima Dedovich (Dubna) DELPHI Collaboration E.Phys.J.
H1 FPS + ZEUS LPS1 H1 / ZEUS data consistency α β=0.56,x IP = β=0.018,x IP = Q2Q2 (β, x IP ) bins, where there is a tension between H1 HERA2.
Precision Measurement of F 2 with H1 Workshop on DIS and QCD, Florence, Max Klein for the H1 Collaboration Towards today The Measurement Results.
July 2001 Snowmass A New Measurement of  from KTeV Introduction The KTeV Detector  Analysis of 1997 Data Update of Previous Result Conclusions.
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
Kevin Black Meenakshi Narain Boston University
Heavy Flavor Production at the Tevatron Jennifer Pursley The Johns Hopkins University on behalf of the CDF and D0 Collaborations Beauty University.
2015/6/23 1 How to Extrapolate a Neutrino Spectrum to a Far Detector Alfons Weber (Oxford/RAL) NF International Scoping Study, RAL 27 th April 2006.
Diffractive W/Z & Exclusive CDF II DIS 2008, 7-11 April 2008, University College London XVI International Workshop on Deep-Inelastic Scattering and.
Recent Results on Diffraction and Exclusive Production from CDF Christina Mesropian The Rockefeller University.
25 th of October 2007Meeting on Diffraction and Forward Physics at HERA and the LHC, Antwerpen 1 Factorization breaking in diffraction at HERA? Alice Valkárová.
M.KapishinDiffraction using Proton Spectrometers at HERA 1 Results on Diffraction using Proton Spectrometers at HERA Low-x Meeting: Paphos, Cyprus, June.
Paul Laycock University of Liverpool BLOIS 2007 Diffractive PDFs.
LISHEP 2009, M. Ruspa, Inclusive Diffraction at HERA Marta Ruspa (Univ. Piemonte Orientale, Italy) LISHEP 2009 Rio de Janeiro, February,
M.KapishinDiffraction and precise QCD measurements at HERA 1 Rencontres de Moriond QCD 2012 M.Kapishin, JINR on behalf of the H1 and ZEUS Collaborations.
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
25/07/2002G.Unal, ICHEP02 Amsterdam1 Final measurement of  ’/  by NA48 Direct CP violation in neutral kaon decays History of the  ’/  measurement by.
Unfolding jet multiplicity and leading jet p T spectra in jet production in association with W and Z Bosons Christos Lazaridis University of Wisconsin-Madison.
1 Jets in diffraction and factorization at HERA Alice Valkárová Charles University, Prague On behalf of H1 and ZEUS collaborations.
Rare B  baryon decays Jana Thayer University of Rochester CLEO Collaboration EPS 2003 July 19, 2003 Motivation Baryon production in B decays Semileptonic.
News on ZEUS Leading Baryon analyses Roberto Sacchi Università di Torino and INFN DIS2004 Workshop Slovakia, April 14-18, 2004 Introduction Study of the.
Mean Charged Multiplicity in DIS, Michele Rosin U. WisconsinZEUS Monday Meeting, Apr. 18th Preliminary Request: Mean Charged Multiplicity in DIS.
16/04/2004 DIS2004 WGD1 Jet cross sections in D * photoproduction at ZEUS Takanori Kohno (University of Oxford) on behalf of the ZEUS Collaboration XII.
Kalanand Mishra April 27, Branching Ratio Measurements of Decays D 0  π - π + π 0, D 0  K - K + π 0 Relative to D 0  K - π + π 0 Giampiero Mancinelli,
H1 FPS + ZEUS LPS1 Regge fit, H1 FPS HERA II data 1 Parameterization of x IP and t dependences for IP and IR Fixed parameters for IR (from H1 DPDF Fits):
Neutral Current Deep Inelastic Scattering in ZEUS The HERA collider NC Deep Inelastic Scattering at HERA The ZEUS detector Neutral current cross section.
H1 FPS + ZEUS LPS1 t-slope: H1 FPS HERA II DESY H1 FPS HERA II t-slope as a function of β,Q 2,x IP (108 data points) ─ Regge fit IP+IR to σ r D(4)
Does KNO scaling hold for DIS and Diffractive DIS? Dependence of multiplicities upon various variables in DIS and diffractive DIS (DDIS). Comparison of.
LISHEP Rio de Janeiro1 Factorization in diffraction Alice Valkárová Charles University, Prague On behalf of H1 and ZEUS collaborations.
Inclusive Diffraction at HERA Marcella Capua – INFN and Calabria University Small X and Diffraction FNAL Chicago (USA) 17 – 20 September 2003 on behalf.
DIS Conference, Madison WI, 28 th April 2005Jeff Standage, York University Theoretical Motivations DIS Cross Sections and pQCD The Breit Frame Physics.
Inclusive Measurements of inelastic electron/positron scattering on unpolarized H and D targets at Lara De Nardo for the HERMES COLLABORATION.
Hadron Structure 2009 Factorisation in diffraction Alice Valkárová Charles University, Prague Representing H1 and ZEUS experiments Hadron structure.
Isabell-A. Melzer-Pellmann Photon 2005, Diffractive interactions in ep collisions Diffractive interactions in ep collisions Isabell-Alissandra.
1 Diffractive dijets at HERA Alice Valkárová Charles University, Prague Representing H1 and ZEUS experiments.
Jets and α S in DIS Maxime GOUZEVITCH Laboratoire Leprince-Ringuet Ecole Polytechnique – CNRS/IN2P3, France On behalf of the collaboration On behalf of.
DIJET (and inclusive-jet) CROSS SECTIONS IN DIS AT HERA T. Schörner-Sadenius (for the ZEUS collaboration) Hamburg University DIS 06, April 2006 Tsukuba,
Search for High-Mass Resonances in e + e - Jia Liu Madelyne Greene, Lana Muniz, Jane Nachtman Goal for the summer Searching for new particle Z’ --- a massive.
Results on Inclusive Diffraction From The ZEUS Experiment Data from the running period The last period with the ZEUS Forward Plug Calorimeter.
Isabell-A. Melzer-Pellmann DIS 2007 Charm production in diffractive DIS and PHP at ZEUS Charm production in diffractive DIS and PHP at ZEUS Isabell-Alissandra.
Calibration of the ZEUS calorimeter for hadrons and jets Alex Tapper Imperial College, London for the ZEUS Collaboration Workshop on Energy Calibration.
Charged Particle Multiplicity, Michele Rosin U. WisconsinQCD Meeting May 13, M. Rosin, D. Kçira, and A. Savin University of Wisconsin L. Shcheglova.
1 Measurement of the Mass of the Top Quark in Dilepton Channels at DØ Jeff Temple University of Arizona for the DØ collaboration DPF 2006.
A. Bertolin on behalf of the H1 and ZEUS collaborations Charm (and beauty) production in DIS at HERA (Sezione di Padova) Outline: HERA, H1 and ZEUS heavy.
4/12/05 -Xiaojian Zhang, 1 UIUC paper review Introduction to Bc Event selection The blind analysis The final result The systematic error.
Kalanand Mishra June 29, Branching Ratio Measurements of Decays D 0  π - π + π 0, D 0  K - K + π 0 Relative to D 0  K - π + π 0 Giampiero Mancinelli,
Kalanand Mishra February 23, Branching Ratio Measurements of Decays D 0  π - π + π 0, D 0  K - K + π 0 Relative to D 0  K - π + π 0 decay Giampiero.
H1 and ZEUS Combined PDF Fit DIS08 A M Cooper Sarkar on behalf of ZEUS and H1 HERA Structure Function Working Group NLO DGLAP PDF fit to the combined HERA.
QM2004 Version1 Measurements of the  ->     with PHENIX in Au+Au Collisions at 200 GeV at RHIC PPG016 Figures with Final Approval Charles F. Maguire.
Outline Motivation DDIS kinematics Introduction of different diffractive data sets Global fit procedure Results and conclusion Sara Taheri Monfared (Semnan.
Heavy Quark Production in 920GeV Proton Nucleus Interactions Michael Danilov ITEP, Moscow Representing HERA-B Collaboration Outline 1.Detector and data.
Stano Tokar, slide 1 Top into Dileptons Stano Tokar Comenius University, Bratislava With a kind permissison of the CDF top group Dec 2004 RTN Workshop.
Low Mass Vector Mesons Nuclear Modification Factors in d+Au 200GeV Lei Guo Los Alamos National Laboratory PHENIX Collaboration.
1 D *+ production Alexandr Kozlinskiy Thomas Bauer Vanya Belyaev
LNF 12/12/06 1 F.Ambrosino-T. Capussela-F.Perfetto Update on        Dalitz plot slope Where we started from A big surprise Systematic checks.
Quarkonia production with the HERA-B experiment J. Spengler, MPI Heidelberg.
MINERνA Overview  MINERνA is studying neutrino interactions in unprecedented detail on a variety of different nuclei  Low Energy (LE) Beam Goals: t Study.
Charged Current Cross Sections with polarised lepton beam at ZEUS
Status of the HERA-B Analysis 58th PRC Open session, May 26, 2005
NA61 and NA49 Collaboration Meeting May 14-19, 2012, Budapest
Charged Particle Multiplicity in DIS
Charged Particle Multiplicity in DIS
Charged Particle Multiplicity in DIS
Charged Current Cross Sections with polarised lepton beam at ZEUS
Preliminary Request: Mean Charged Multiplicity in DIS
Presentation transcript:

H1 FPS + ZEUS LPS1 FPS/LPS Combination Preliminary request M.Ruspa, V. Sola, M.Kapishin, R.Polifka

H1 FPS + ZEUS LPS2 Combine H1-ZEUS diffractive cross sections with Sasha Glasov’s combination code Available samples  H1 HERA II FPS (published, [2])  ZEUS 2000 LPS (published, [3]) Goal In this talk report on combination of proton spectrometer results (LPS-FPS) [2] DESY [3] DESY

H1 FPS + ZEUS LPS3 What/how/when to combine? M. RuspaZEUS General Meeting - 30/06/20113 Combining σ r D(4) point to point not possible >> different xIP, t, Q2, beta binning >> swimming in xIP depends on t through alpha’ Averaging the t-slope possible but needs time >> significant discrepancy Swimming σ r D(4) in beta, Q2 and making a combined Regge fit looks the cleanest way The fit will give b, IP and IR paramenters Work in progress timescale beyond summer Combining σ r D(3) point to point possible Done, to be realeased for EPS Will focus on this in the following

H1 FPS + ZEUS LPS4 Average t-slope as a function of x IP --- Regge fit uncertainty band H1 FPS HERA II DESY H1 FPS HERA I DESY ZEUS LPS 2 DESY ─ H1 FPS HERA II Regge fit

H1 FPS + ZEUS LPS5 Average t-slope as a function of x IP, free ΔB ─/─ upper lines for ZEUS data ─/─ lower lines for H1 data ─ H1 FPS HERA II Regge fit  H1/ZEUS uncertainty band ΔB~ GeV 2  uncertainty of H1+ZEUS cross section extrapolation from |t|-range [ ] GeV 2 to |t|<1 GeV 2 Δσ/σ~ 6-8% B IP +ΔB, B IR +ΔB

H1 FPS + ZEUS LPS6 Measured in the t range [0.1 – 0.7] GeV 2 Extrapolation to t min < |t| < 1 GeV 2 with algebrical integration Available σ r D(3) measurements Measured in the t range [ ] GeV 2 Extrapolation to t min < |t| < 1 GeV 2 hidden in acceptance corr

H1 FPS + ZEUS LPS7 7  ZEUS 2000 LPS (33 pb -1 ) and H1 FPS HERA II (156 pb -1 )  Binning originally very different (fixed Mx for ZEUS, fixed beta for H1) ZEUS points swam to H1 bins  Correlated systematics from [2] (H1) and [3] (ZEUS) All systematics in [2] taken as correlated though no explicit mention in that paper  Normalization Each sample left with its normalization and related uncertainty N.B.: Bringing samples to a fixed (average) normalization makes no difference Fit ingredients t rangeNorm. unc. ZEUSNorm. unc. H1Ratio H1/ZEUS [t min -1] GeV 2 +11% -7% 6%H1 / ZEUS = 0.85 ± 0.01 (stat) ± 0.03 (syst) / (norm) [ ] GeV 2 7%4.5%H1/ZEUS = 0.91 ± 0.01 (stat) ± 0.03 (syst) (norm)

H1 FPS + ZEUS LPS8 Systematics H1 FPS hadronic energy scale electromagnetic energy scale scattered electron angle measurement energy and momentum of leading proton background subtraction reconstruction of event vertex bin centre correction x IP reweighting β reweighting Q 2 reweighting t reweighting (correlated systematics) ZEUS LPS electron position electron energy scale hadronic energy scale proton dissociation background vertex recontruction momentum of the leading proton proton position x IP reweighting t reweighting

H1 FPS + ZEUS LPS9 SGfit in the ZEUS t range fit -> χ 2 = 52 / 58 = 0.89 Fitted systematics: 1 HadEn_h ElecEn_h ElecTh_h DifBeta_h DifXpom_h DifT_h EpFPS_h PxFPS_h PyFPS_h DifQ2_h VtxEff_h Backgr_h Bcccor_h Norm_h Ehscale_zeus Eescale_zeus Pdiss_zeus xIPweight_zeus Tweight_zeus Norm_zeus

H1 FPS + ZEUS LPS10 Pull distributions 10

H1 FPS + ZEUS LPS11 Gain in Precision M. RuspaZEUS General Meeting - 30/06/ Q2 beta xIP xsec_fit err_fit (%) xsec_h1 err_h1 (%) err_fit/err_h

H1 FPS + ZEUS LPS12 Second analysis – full t range 12 R.Polifka

H1 FPS + ZEUS LPS13 H1 FPS HERA II data Averaged method: DA / Elec y av = y e 2 +y da ∙(1-y da ) → Q av 2,x av x IP = 1 – E p /920 β= x / x IP for x IP >0.01 → β-dependence at fixed Q 2,x IP → β does not depend on M x scale β = Q 2 /(Q 2 +M x 2 ) for x IP <0.01 M X = 1.10∙ M x had ∙√ y av /y had E had → E had (1±Δ), M x →M x √(1±Δ) H1 LAr scale dependence

H1 FPS + ZEUS LPS14 SGfit/WA Nominal H1 Had escale taken out from error grid  H1 Had escale partially responsible of raise towards low x IP ( and ) N.B.: when taking out Had escale, SGfit highest beta and lowest x IP

H1 FPS + ZEUS LPS15 How to deal with the Lar shift  Use as default the observed shifts HadEn_H ElecEn_H Olaf Behnke: use values from the inclusive combination to estimate a procedural uncertainty related to the energy scales h8H_caleLar h3EeLar Overall effect ~ 1%, up to 5% for the lowest x IP bins  Take the LAr escale uncertainty as uncorrelated between H1 data points - the correlation between the first two x IP bins and the rest is minimal - in the first two x IP bins the uncertainty swaps from negative to positive in different β and Q 2 bins, i.e. the reaction of the cross section to the energy shift is different Decided to consider the latter as procedural uncertainty

H1 FPS + ZEUS LPS16 Olaf Proposal

H1 FPS + ZEUS LPS17 Ratio nominal case to case with H1 hadronic escale taken as uncorrelated H1 LAr hadronic escale taken as uncorrelated

H1 FPS + ZEUS LPS18 Procedural Uncertainties M. RuspaZEUS General Meeting - 30/06/ ZEUS Swimming factors  Average effect ~ 1% Additive VS Multiplicative Only normalization uncertainties taken as multiplicative while all other uncertainties treated as additive (see slide 19)  Average effect ~ 4.3% Correlations between H1 and ZEUS Similar systematic uncertainties identified >> electromagnetic energy scale >> background subtraction >> x IP reweighting >> t reweighting  Average effect ~ 2 % H1 hadronic energy scale not correlated between H1 data points

H1 FPS + ZEUS LPS19 Procedural Uncertainties M. Ruspa19ZEUS General Meeting - 30/06/2011 Ratio nominal case to case with all uncertainties except normalization taken as additive

H1 FPS + ZEUS LPS20 Procedural Uncertainties Ratio nominal case to case with all correlations ZEUS-H1 taken together

H1 FPS + ZEUS LPS21 Q 2 = 2.5 GeV x IP = β = Including single points (not matching with other experiments) does not change the fit results (nor the χ 2 nor the systematic shifts) but allow to obtain a wider kinematical coverage → do not changed χ2 in the combination fit 121 H1 points 58→106 ZEUS points 169 H1+ZEUS combined points Additional ZEUS LPS points

H1 FPS + ZEUS LPS22 Plots for EPS 2011

H1 FPS + ZEUS LPS23 Plots for EPS 2011

H1 FPS + ZEUS LPS24 Plots for EPS 2011

H1 FPS + ZEUS LPS25 Summary & Outlook Fit to σ r D(3 LPS-FPS in the ZEUS t-range [ GeV 2 ] ready - combined cross section plots vs x IP, Q 2 - pull distributions - procedural uncertainties - second analysis Following plots to be realeased for EPS, zoomed plots will be prepared for H1ZEUS plenary Combined Regge fit to LPS-FPS data on the way

H1 FPS + ZEUS LPS26 Backup: H1 E had scale shift for x IP <0.01 x IP = x IP = log 10 β Linear Y scale H1 FPS log 10 β-bin limits: -3.0, -2.5, -2.0, -1.5, -1.0, -0.5, 0.0 E had -7% → MC hadron energy scale shifted at -1.75δ relative to default MC for 2 lower x IP bins β = Q 2 / (Q 2 + M x 2 )

H1 FPS + ZEUS LPS27 Backup: H1 E had scale shift for x IP <0.01 x IP = x IP = log 10 β LogY scale H1 FPS log 10 β - bin limits: -3.0, -2.5, -2.0, -1.5, -1.0, -0.5, 0.0 E had -7% → MC hadron energy scale shifted at -1.75δ relative to default MC for 2 lower x IP bins