Inclusive Jet Cross-Sections in Inclusive Jet Cross-Sections in Neutral Current DIS Events Using the Neutral Current DIS Events Using the

Breit FrameBreit FrameAnalysis Status

Jeff StandageYork University

Thomas SchoernerHamburg University

Marcos Jiminez

Claudia Glasman

Juan TerronUniversidad Autonoma de Madrid

Contents

• Cross-section & NLO:Data ratio comparisons

• Differences between two analyses – so far

QCD Meeting, 10th March 2005 Jeff Standage, York University

Q2

JT/OG

(DESY 02-112)

96-97

JS/TSS

98-00

MJ/CG/JT

99p-00

QCD Meeting, 10th March 2005 Jeff Standage, York University

JS/TSS

98-00

MJ/CG/JT

99p-00

ET(jet)

QCD Meeting, 10th March 2005 Jeff Standage, York University

JT/OG

(DESY 02-112)

96-97

JS/TSS

98-00

MJ/CG/JT

99p-00

η (jet)

QCD Meeting, 10th March 2005 Jeff Standage, York University

JT/OG

(DESY 02-112)

96-97

Differences Between JS/TS and MJ/CG/JT Analyses

• Analysis codeOrange/phantom 2004a(.1,.2) Private EAZE job

Orange variables for cuts Release 2004a.1 (pro)

Zufos/cells for offline jet finding

• Noise Suppression (noise02s.fpp)

ecut(1) = 0.08 ecut(1) = 0.10

ecut(2) = 0.14 ecut(2) = 0.15

imbacut = 0.7 imbacut = 0.9

• CAL corrections (escale03.fpp)

Individual RCAL cell corrections No RCAL cell by cell corrections

Global corrections - Global corrections -

FCAL HAC: 0.941 FCAL HAC: 0.95

FCAL EMC: 1.024 FCAL EMC: 1.04BCAL HAC: 1.0962 BCAL HAC: 1.08BCAL EMC: 1.05315 BCAL EMC: 1.04RCAL HAC: 1.022 RCAL HAC: 1.025RCAL EMC: 1.022 RCAL EMC: 1.025

JS/TS MJ/CG/JT

QCD Meeting, 10th March 2005 Jeff Standage, York University

Differences Between JS/TS and MJ/CG/JT Analyses

• VertexCell position corrected for Cell position corrected for z-vertex only.

X,Y,Z vertices

• Lepton beam energyOrange: Ee = 27.56 GeV Ee = 27.5 GeV

Offline: Ee = 27.52 GeV

• Isolation (cone) cutA cut is put on the electron candidate such that the total energy not associated with the candidate in a radius of R is eta-phi space is less than 10%. This removes

photoproduction events and events where a jet remnant is falsely identified as the positron.

R = 0.8 R = 0.7

• Sinistra electronElectron corrected for dead material. Uncorrected Sinistra candidate

is used.Orange variable: Siecorr(3,1) Corresponds to SiCalEne(1)

• Event variablesOrange variables being used, All values calculated directly from cells

e.g. SiQ2da(1), SiCeHMom(4,1) information.

Evidence of further orange corrections/differences.

JS/TS MJ/CG/JT

QCD Meeting, 10th March 2005 Jeff Standage, York University

Summary

• Analysis differences lead to ~10% difference in events selected

Claudia had 992 events that I have rejected or have no jets.

I have 825 such events that Claudia doesn’t.• Analysis differences lead to complete discrepancy in number of jets in each event.• Have over-ridden orange routines to implement her analysis criteria.

Of those 992 events are still losing 20:

(i) 1 event: Q2 difference (2 cells have different energy).

(ii) 2 events: cosGammaHad.

(iii) 11 events: isolated cone cut (after moving to 0.7).

(iv) 6 events have no jets (still to look into jet finding).

not using orange jets!

QCD Meeting, 10th March 2005 Jeff Standage, York University

Future steps

• Nail down last few events cut differences. • Compare jet finding/boost procedure.• Repeat process for the hadron level in MC

(using JT/CG get_hadsys.fpp).• Compare acceptance corrections.• Jet energy corrections.• Cross-sections.• Decide which methods/corrections are the right ones (why)?

QCD Meeting, 10th March 2005 Jeff Standage, York University