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This study presents the observation of single-diffractive W boson production using the CMS detector, highlighting its feasibility. Emphasizing the rediscovery of hard diffraction at the LHC, the investigation assesses the sensitivity to quark components of diffractive Parton Distribution Functions (dPDFs) and the Rapid Gap Survival Probability (S2). W bosons are selected via a muon channel, ensuring an efficient analysis of background and systematics without pile-up. This work contributes to understanding diffractive processes and their implications in high-energy collisions.
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Observation of single-diffractive W production with CMS: a feasibility study Antonio Vilela Pereira (Università degli Studi di Torino & INFN Torino) On behalf of the CMS Collaboration DIS 2008 - London
Outline • W selection • Observation of single-diffractive (SD) W signal • Background & Systematics (Large Rapidity Gap) NB: No pile-up Effective luminosity for single-interactions – 100 pb-1 DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
Motivation • Rediscover hard-diffraction at LHC • Sensitive to quark component of diffractive PDF’s (dPDF’s) • Probe Rapidity Gap Survival Probability (S2) – connection to multiple partonic interactions and soft rescattering effects … dPDF (Large Rapidity Gap) Ratio of diffractive to inclusive W’s measured at Tevatron (~1%) (cf. K. Goulianos’s talk) DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
W selection W selection: (same as inclusive analysis) 1 isolated pT > 25 GeV 50 < MT < 200 GeV || < 2.0 = - (,ETmiss) < 1 rad n jets(ET > 40 GeV) 3 n muons(pT > 20 GeV) < 2 Overall efficiency: Pomwig SD W: 34% (2.4k evts/100pb-1) Pythia W: 28% (600k evts/100pb-1) NB: Diffractive W: Pomwig v2.0beta (dPDF: NLO H1 2006 Fit B) DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
Forward detectors CMS Hadronic Forward (HF) Hadronic Forward (HF) (3.0 < || < 5.0) (3.0 < || < 5.0) CASTOR CASTOR ZDC ZDC TOTEM T2 TOTEM T2 (|| > 8.1) (|| > 8.1) (5.2 < || < 6.6) (5.2 < || < 6.6) Not present in start-up TOTEM T1 TOTEM T1 TOTEM: Total Cross Section, Elastic Scattering and Diffraction Dissociation at the LHC DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
Selecting diffractive events • Diffractive events historically selected through Large Rapidity Gaps (LRG’s) in (forward) hadronic final state • Select diffractive events based on multiplicities in CMS Forward Hadron Calorimeter (HF) and/or CASTOR • In addition, look at activity in central tracker Generated particles – energy weighted Diffractive sample generated with gap in –plus side For selection: exploit different multiplicity distributions in forward and central regions (cf. Tevatron, HERA) DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
Observation of diffractive signal • Selection of Rapidity Gap side: • Observed gap side: side with lowest energy sum in HF (HF-plus vs HF-minus) • Pre-selection on central Track Multiplicity • Maximum number of reconstructed tracks in central tracker (|| < 2.0, pT > 0.9 GeV) • HF tower multiplicity in “low ” vs. HF tower multiplicity in “ high ” region • HF tower multiplicity vs. CASTOR sector multiplicity in gap side CMS (3.0 < || < 5.0) HF HF ZDC CASTOR ZDC CASTOR (|| > 8.1) (5.2 < || < 6.6) DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
HF multiplicity at “low ” vs HF multiplicity at “high” “low ”: 3.0 < || < 4.0 “high ”: 4.0 < || < 5.0 Excess in low multiplicity visible Non-diffractive background clusters in the low multiplicity (signal) region DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
HF tower multiplicity vs CASTOR -sector multiplicity in gap side • CASTOR: (5.2 < || < 6.6) • no segmentation, 16 -sectors • Generator level information: number of -sectors with energy above threshold (E > 10 GeV) • For start-up (2008), installed only in one side (z-minus) • Reject events in which observed gap side is not the z-minus (CASTOR) side Potential signal increase by factor ~2 with CASTOR in both sides Clear peak at low multiplicity DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
Effect of central track pre-selection Increased non-diffractive background when loosening the track pre-selection Diffractive signal less visible when no track pre-selection is present – but still visible ~ 100 – 200 events in zero multiplicity bin (S/B ~ 6 - 20) DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
Backgrounds • Non-diffractive W • Inclusive QCD events • Applied full selection to sample of “-enriched” QCD sample (Pythia) • Inclusive W selection: ~ 50k events/100pb-1 (< 10% of inclusive W rate) • Negligible contribution at low HF/CASTOR multiplicity (< 1% level wrt diffractive W yields) • Proton-dissociative events: ppXN (with X containing a W boson and N a low mass state into which the proton diffractively dissociates) • Cross section expected to be of the same order as signal • If N escapes detection (limited forward coverage), it’s an irreducible background (but it’s also diffraction) • Around 50% can be rejected by vetoing on ZDC • Expect enhancement in signal region by ~ 30% (cf. S. Ovyn’s talk) http://cms-physics.web.cern.ch/cms-physics/public/DIF-07-001-pas-v4.pdf DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
Systematics • Rapidity Gap Survival Probability (S2): • Assumed 5% (as indicated by theory) • Ndiff S2 • Extraction of diffractive yields provides S2 measurement • W selection and reconstruction: from inclusive analysis (cf. S. Bolognesi’s talk) • Same for diffractive and non-diffractive • Negligible effect on acceptance • UE description: • Generator level study: Pythia Tune DWT (default) vs Tune A • Selection applied on full simulated Alpgen W events • Potential background enhancement by factor 3 – 5 in signal region http://cms-physics.web.cern.ch/cms-physics/public/EWK-07-002-pas-v8.pdf DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
Summary • Procedure discussed to observe single-diffractive W production with an effective 100pb-1 for single interactions • Diffractive selection based on forward hadron multiplicities in HF and CASTOR calorimeters, as well as multiplicity in central tracker • For S2 = 0.05, expected O(100) reconstructed signal events per 100pb-1 • S/B of up to 20 with CASTOR • This study emphasizes the need of CASTOR (ideally on both sides) • TOTEM T1/T2 information (similar acceptance as HF/CASTOR) should add to the background rejection DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
BACKUP DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
MC samples • Diffractive W samples: • Pomwig v2.0beta • Proton PDF: CTEQ6M • dPDF: NLO H1 2006 Fit B (IP(0) = 1.111, ' = 0.06 GeV-2, BIP = 5.5 GeV-2) • Non-diffractive samples: • Pythia W • Pythia Inclusive QCD (-enriched) • Alpgen W • Cross sections: • - Diffractive W: ~ 69 pb (NLO PDFs) (Assumes S2 = 5%) • - Non-difractive W: ~ 21 nb (NLO cross section) This gives a ratio of diffractive to inclusive cross sections of ~0.3% DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
distribution MX=(s)1/2 = p/p DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
Choosing the gap side • Gap side: side with lowest energy sum in HF (HF-plus vs. HF-minus) • Energy thresholds for counting HF towers minimizing the probability of choosing the gap side incorrectly • HF alone has limited • coverage for gap side • selection Fraction of times the gap side is chosen incorrectly DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
HF tower multiplicity in gap side • HF multiplicities in gap side for diffractive (Pomwig) vs non-diffractive (Pythia) W events • Gap side: side with lowest energy sum in HF (HF-plus vs HF-minus) • Pre-selection on number of reconstructed tracks in central tracker (|| < 2.0, pT > 0.9 GeV) Diffractive signal cannot be clearly distinguished in “data” sample DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
Effect on track pre-selection – HF “low ” vs HF “high ” S/B for zero multiplicity bin: O(1) or less Diffractive signal most visible when track pre-selection is tighter > 200 events in zero multiplicity bin even for strict track pre-selection DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
CMS Forward detectors (D. d’Enterria hep-ex/0708.0551) (3.0 < || < 5.0) CMS (3.0 < || < 5.0) Not present in start-up CASTOR CASTOR ZDC ZDC HF HF T2 (|| > 8.1) (|| > 8.1) T2 (5.2 < || < 6.6) (5.2 < || < 6.6) DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira
CASTOR & ZDC • CASTOR: Centauro And Strange Object Research • Quartz tungsten sampling calorimeter • 5.2 < || < 6.6 – charged & neutrals • EM + HAD sections • CMS Zero Degree Calorimeter • Quartz tungsten sampling calorimeter • || > 8.1 - neutrals • EM + HAD sections DIS08 Observation of single-diffractive W production with CMS A. Vilela Pereira