PDF Studies at LHCb! Simone Bifani. On behalf of the LHCb collaboration. University of Birmingham (UK)

Similar documents
Electroweak Measurements at LHCb!

PoS(ICHEP2012)300. Electroweak boson production at LHCb

PANIC August 28, Katharina Müller on behalf of the LHCb collaboration

Electroweak results. Luca Lista. INFN - Napoli. LHC Physics

PoS(EPS-HEP2015)309. Electroweak Physics at LHCb

Inclusive. W & Z measurements in CMS. Georgios Daskalakis. on behalf of CMS Collaboration. .C.S.R. Demokritos

W, Z and top production measurements at LHCb

W/Z inclusive measurements in ATLAS

Recent LHCb measurements of Electroweak Boson Production in Run-1

Inclusive W and Z: Precision LHC Measurements

First V+jets results with CMS. Vitaliano Ciulli (Univ. & INFN Firenze) V+jets workshop, 8-10 Sep 2010, Durham

Measurements of the Vector boson production with the ATLAS Detector

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

Z boson studies at the ATLAS experiment at CERN. Giacomo Artoni Ph.D Thesis Project June 6, 2011

Proton anti proton collisions at 1.96 TeV currently highest centre of mass energy

Physics with Tau Lepton Final States in ATLAS. Felix Friedrich on behalf of the ATLAS Collaboration

LHCb results in proton-nucleus collisions at the LHC

Higgs-related SM Measurements at ATLAS

Electroweak Physics at the Tevatron

Higgs and Z τ + τ in CMS

Precision Forward Measurements at LHCb with Vector Bosons. Philip Ilten on behalf of the LHCb Collaboration. Massachusetts Institute of Technology

Overview of PDF-sensitive measurements from Run I in ATLAS

Top Quark Production at the LHC. Masato Aoki (Nagoya University, Japan) For the ATLAS, CMS Collaborations

Measurement of W-boson Mass in ATLAS

Measurements of the vector boson production with the ATLAS detector

Measurement of W and Z boson cross sections in pp collisions at 7 TeV with the ATLAS detector

Physics at Tevatron. Koji Sato KEK Theory Meeting 2005 Particle Physics Phenomenology March 3, Contents

From Precision Electro-weak Physics to Beyond-the-SM Physics Searches

Measurement of the Z ττ cross-section in the semileptonic channel in pp collisions at s = 7 TeV with the ATLAS detector

Latest results on the SM Higgs boson in the WW decay channel using the ATLAS detector

W/Z + jets and W/Z + heavy flavor production at the LHC

tt production in the forward region at LHCb

Moriond QCD. Latest Jets Results from the LHC. Klaus Rabbertz, KIT. Proton Structure (PDF) Proton Structure (PDF) Klaus Rabbertz

PoS(CKM2016)117. Recent inclusive tt cross section measurements. Aruna Kumar Nayak

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

Searches for exotica at LHCb

Measurement of t-channel single top quark production in pp collisions

Top production measurements using the ATLAS detector at the LHC

Proton PDFs constraints from measurements using the ATLAS experiment

Dimitris Iliadis AUTh, LAPP. On behalf of the ATLAS collaboration. XIIth Quark Confinement and the Hadron Spectrum 29 August 2016, Thessaloniki

Measurement of jet production in association with a Z boson at the LHC & Jet energy correction & calibration at HLT in CMS

QCD at CDF. Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration

Tests of QCD Using Jets at CMS. Salim CERCI Adiyaman University On behalf of the CMS Collaboration IPM /10/2017

Measurement of the jet production properties at the LHC with the ATLAS Detector

ATLAS-CONF October 15, 2010

PoS(EPS-HEP 2013)215. WW, WZ, and ZZ production at CMS. Jordi DUARTE CAMPDERROS (on behalf of CMS collaboration)

High-pT lepton final states at 13 TeV (W and Z searches)

Precision QCD at the Tevatron. Markus Wobisch, Fermilab for the CDF and DØ Collaborations

Recent Results on Top Physics at CMS

A search for heavy and long-lived staus in the LHCb detector at s = 7 and 8 TeV

V0 cross-section measurement at LHCb. RIVET analysis module for Z boson decay to di-electron

tt + X production at ATLAS and CMS

Introduction. The LHC environment. What do we expect to do first? W/Z production (L 1-10 pb -1 ). W/Z + jets, multi-boson production. Top production.

Inclusive top pair production at Tevatron and LHC in electron/muon final states

P-P PHYSICS AT LHC. W and Z produc1on. Data and MC comparison. Lecture 4

Inclusive and differential vector boson (W, Z) measurements from CMS Kadir Ocalan (Necmettin Erbakan University) On behalf of the CMS Collaboration

Measurement of EW production! of Z+2j at the LHC

Reconstruction and identification of hadronic τ decays with ATLAS

QCD and jets physics at the LHC with CMS during the first year of data taking. Pavel Demin UCL/FYNU Louvain-la-Neuve

Results on QCD jet production at the LHC (incl. Heavy flavours)

QCD at the Tevatron: The Production of Jets & Photons plus Jets

WZ di-boson production at CMS

Measurements of the production of a vector boson in association with jets in the ATLAS and CMS detectors

Top Quark Studies with CMS

Application of the Tau Identification Capability of CMS in the Detection of Associated Production of MSSM Heavy Neutral Higgs Bosons Souvik Das

La ricerca dell Higgs Standard Model a CDF

EW Physics at LHC. phi= mu_4: pt=7.9 GeV, eta=-1.13, phi=0.94. Toni Baroncelli:

Single-Top at the Tevatron

Review of LHCb results on MPI, soft QCD and diffraction

+ High p T with ATLAS and CMS in Heavy-Ion 2.76TeV

Search for the Standard Model Higgs Boson in H WW lν lν with the ATLAS experiment

LHCb Semileptonic Asymmetry

Double Parton Scattering in CMS. Deniz SUNAR CERCI Adiyaman University On behalf of the CMS Collaboration Low-x th June 2017 Bari, Italy

Physics at Hadron Colliders

Miguel Villaplana Università degli Studi e INFN Milano. on behalf of the ATLAS Collaboration. September 11, 2017

Results and Prospects for Ion Physics at LHCb

Title Text. ATLAS Higgs Boson Discovery Potential

Dilepton Forward-Backward Asymmetry and electroweak mixing angle at ATLAS and CMS

Direct Measurement of the W Total Decay Width at DØ. Outline

Higgs search in WW * and ZZ *

b and c production in CMS

Physics at Hadron Colliders Part II

Differential Top Cross-section Measurements

ATLAS Run 2 Higgs Prospects

LHCb status. Marta Calvi. for the LHCb Collaboration. 103 rd LHCC meeting University Milano-Bicocca and INFN

Feasibility of a cross-section measurement for J/ψ->ee with the ATLAS detector

Preparations for SUSY searches at the LHC

in Section The H ZZ 4l channel

Top, electroweak and recent results from CDF and combinations from the Tevatron

Tevatron Results on W and Z Boson Production

Search for New Physics with b sll LHCb

From the TeVatron to the LHC UK HEP Forum, 7-8 May 2009 Emily Nurse

Recent QCD results from ATLAS

Recent ATLAS measurements in Higgs to diboson channels

Z-dark search with the ATLAS detector

Measurements of BB Angular Correlations based on Secondary Vertex Reconstruction at sqrt(s) = 7 TeV in CMS

Inclusive BB cross section at 8 TeV

Electroweak scale physics & exotic searches at LHCb

TESTING THE STANDARD MODEL IN THE FORWARD REGION AT THE LHC

Highlights of top-quark measurements in hadronic nal states at ATLAS

Transcription:

PDF Studies at LHCb! Simone Bifani University of Birmingham (UK) On behalf of the LHCb collaboration MENU 213 Rome 3th September - 4th October 213

Outline Introduction Analyses» Z/γ* ll, l =, e, τ#» W ν#» Z/γ* +jet Summary and Outlook Simone Bifani MENU 213 2

LHCb A Forward Spectrometer Designed to look at CP violation in B decays @ LHC Fully instrumented within 2. < η < 5.» 2.-2.5: overlap with ATLAS & CMS» 2.5-5.: complementary range 25 mrad 1 mrad Beam Beam Simone Bifani MENU 213 3

Analyses based on 21/211 data samples at 7 TeV» L 21 ~37 pb -1» L 211 ~1 fb -1 Datasets Due to luminosity levelling, same running conditions throughout fills and throughout year EW trigger thresholds unchanged between 21, 211 and 212 Simone Bifani MENU 213 4

W & Z Production and PDFs LHCb s forward acceptance provides very interesting possibilities to study the proton Parton Density Functions Take large-x from one proton and a small-x from the other probe two distinct regions in the (x, Q 2 ) space 1 9 1 8 1 7 1 6 ATLAS/CMS LHCb CDF/D W&Z HERA Fixed Target LHC 7 TeV Kinematics Can probe the low-x, high-q 2 region inaccessible to other experiments» W and Z (x of 1-4 and 1-1 )» Low-mass Drell-Yan (x down to 1-6 ) Q 2 [GeV 2 ] 1 5 1 4 1 3 1 2 1 1 W&Z γ* γ* y =6 y =4 y =2 y = y =2 y =4 y =6 1 1 7 1 6 1 5 1 4 1 3 1 2 1 1 1 x x 1,2 = M p s e ±y Q 2 = M 2 Simone Bifani MENU 213 5

W & Z Production and PDFs Theoretical predictions» Partonic cross-sections known at NNLO to few %» PDF uncertainty dominates at large rapidities (1% for y<2, 6-8% at y~5) Experimental measurements» Muon modes provide clean signature and easily reconstructible final states» Electron and tau modes provide complementary measurements and test lepton universality Cross-section measurements @ LHCb can constrain PDFs Simone Bifani MENU 213 6

Cross Section The cross-section for boson production can be expressed as BR= 1 R L N Candidates A " T rigger " Tracking " P articleid " Selection f FSR Measurements performed in the forward region (2.<η<4.5) for leptons with p T >2 GeV/c: Acceptance = 1 for Z and W ν, but obtained from MC for Z ee and Z ττ Efficiencies determined mostly from data and cross checked with simulation FSR correction evaluated using HERWIG++ and PHOTOS+PYTHIA Simone Bifani MENU 213 7

Z/γ*! LHCb-CONF-213-7 Preliminary L ~1 fb -1 (211) Single muon trigger: p T > 1 GeV/c 2 reconstructed muons» p T > 2 GeV/c» 2. < η < 4.5» 6 < M < 12 GeV/c 2 Backgrounds» Heavy flavour (Data)» K/π mis-id (Data)» Z ττ (MC) -» tt (MC)» WW (MC) N Candidates = 52626 Purity > 99% ) 2 Events / (1 GeV/c 7 6 5 4 3 2 1 LHCb preliminary Data Z/γ* + 6 8 1 12 Dimuon invariant mass [GeV/c ] 2 Simone Bifani MENU 213 8

Z/γ* ee! LHCb-PAPER-212-36 arxiv:1212.462 L ~945 pb -1 (211) Single electron trigger: p T > 15 GeV/c 2 reconstructed electrons» p T > 2 GeV/c» 2. < η < 4.5» E ECal / pc >.1» E HCal / pc <.5» M ee > 4 GeV/c 2 Backgrounds» K/π mis-id (Data)» Heavy flavour (Data)» Z ττ (MC)» tt - (MC) N Candidates = 2142 Purity ~ 95% Events / (2 GeV/c 2 ) 12 1 8 6 4 2 LHCb 4 6 8 1 12 e - ) [GeV/c 2 ] Simone Bifani MENU 213 9 M (e Data Signal Background Mass peak distorted by bremsstrahlung +

Z/γ* ττ! LHCb-PAPER-212-29 arxiv:121.6289 L ~1 fb -1 (211) Single lepton trigger:» p T,(e) > 1(15) GeV/c 5 final states:, e, e, h, eh» p T,1 > 2 GeV/c, p T,2 > 1 GeV/c» 2. < η l < 4.5, 2.25 < η h < 3.75» M 12 > 2 GeV/c 2 Backgrounds» QCD (Data)» EW (Data) -» tt (MC)» WW (MC)» Z ll (MC) Simone Bifani MENU 213 1

Z/γ* ττ! LHCb-PAPER-212-29 arxiv:121.6289 Events / (5 GeV/c 2 ) 4 Data 35 3 25 2 15 1 LHCb Ô s =7TeV Z æ QCD EWK t t æ WW æ Z æ Events / (5 GeV/c 2 ) 8 Data 7 Z æ QCD 6 EWK t t æ e 5 WW æ e 4 3 2 LHCb Ô s =7TeV Events / (5 GeV/c 2 ) 4 Data 35 Z æ QCD 3 EWK t t æ e 25 WW æ e 2 15 1 LHCb Ô s =7TeV 5 1 5 2 4 6 8 1 12 M [GeV/c 2 ] 2 4 6 8 1 12 M e [GeV/c 2 ] 2 4 6 8 1 12 M e [GeV/c 2 ] N Candidates = 99 Events / (5 GeV/c 2 ) 35 3 25 2 15 1 5 Data Z æ QCD EWK t t æ h WW æ h Z æ LHCb Ô s =7TeV Events / (5 GeV/c 2 ) 3 25 2 15 1 5 Data Z æ QCD EWK t t æ eh WW æ eh Z æ ee LHCb Ô s =7TeV Purity ~6-7% 2 4 6 8 1 12 M h [GeV/c 2 ] 2 4 6 8 1 12 M eh [GeV/c 2 ] Simone Bifani MENU 213 11

Results Z/γ* ll LHCb-CONF-213-7 Preliminary Fiducial volume: p T,l > 2 GeV/c, 2. < η l < 4.5, 6 < M ll < 12 GeV/c 2 LHCb Preliminary Z LHCb preliminary (75.4 ±.3 stat ± 1.9 syst ± 2.6 lumi ) pb Z ee (76. ±.8 stat ± 2. syst ± 2.6 lumi ) pb Z ττ NNLO(MSTW8) (71.4 ± 3.5 stat ± 2.8 syst ± 2.5 lumi ) pb (74.7 +1.6 1.4 PDF ±.4 T heory) pb 5 6 7 8 9 1 σ(z ll) [pb] Results agree with NNLO Measurements limited by statistics (ττ) or luminosity (ee, ) Main systematics: reconstruction (), tracking efficiency (ee), backgrounds and efficiency (ττ) Simone Bifani MENU 213 12

Results Z/γ* ll LHCb-CONF-213-7 Preliminary dσ/dy [pb] 7 LHCb preliminary Data (stat) 6 Data Data (tot) (tot) MSTW8 NNLO - MSTW8 (NNLO) 5 ResBos CT1 Powheg (NNLO) + PS 4 NNPDF23 (NNLO) ABM11 (NNLO) 3 2 1 2 3 4 Z boson rapidity dσ/dy [pb] 7 LHCb preliminary 6 5 4 3 2 1 Graph Data (stat) Data (tot) Z ee 2 2.5 3 3.5 4 Z boson rapidity Good agreement with NNLO Good agreement between and ee final states Good agreement with ATLAS (after adapting to ATLAS cuts) dσ/dy [pb] 14 12 1 8 6 4 2 LHCb 211 preliminary, Z extrapolated LHCb 211, Z ee extrapolated ATLAS 21, Z, Z ee.5 1 1.5 2 2.5 3 3.5 4 4.5 y(z) Simone Bifani MENU 213 13

Results Z/γ* ll LHCb-CONF-213-7 Preliminary dσ/dφ* [pb] 3 1 LHCb preliminary Data (stat) Data (tot) NNLO - MSTW8 ResBos Powheg + PS 2 1-2 1-1 1 1 φ* prediction/data 1.7 1.6 1.5 1.4 1.3 1.2 1.1 1.9.8.7 LHCb preliminary Data (stat) Data (tot) NNLO - MSTW8 ResBos Powheg + PS -2 1-1 1 1 φ* = tan (( )/2) cosh ( /2) p T m Z NNLO fails to describe φ* Bett er agreement when compared to ResBos and POWHEG dσ/dφ* [pb] 3 1 LHCb preliminary 1 2 1 1-2 1 Graph -1 1 1 Data (stat) Data (tot) Z ee φ* Simone Bifani MENU 213 14

W L ~37 pb-1 (21) LHCb-PAPER-212-8 arxiv:124.162 ν! Single muon trigger: pt > 1 GeV/c ν# 1 reconstructed & isolated muon» pt > 2 GeV/c» 2. < η < 4.5» Cone pt (R=.5) < 2 GeV/c W+ + (charged & neutral information) Backgrounds» Z/γ*» W τν and Z ττ» Heavy flavour» K/π punchthrough» K/π decay in flight Simone Bifani R (MC) (MC) (Data) (Data) (Data) R= MENU 213 p 2 + 2 15

W ν! LHCb-PAPER-212-8 arxiv:124.162 Specific cuts implemented to reduce each background component Z/γ*» Veto on 2 nd muon with p T > 2 GeV/c W τν, Z ττ and Heavy flavour» Impact parameter < 4 m K/π punchthrough» E / pc <.4 Largest residual backgrounds» Decays in flight of K/π» Z events with one muon outside the acceptance.1.2.3.4.5 IP [mm] Simone Bifani MENU 213 16 Event probability Event probability -1 1 1 1-2 -3 1-4 1 1 1-1 1-2 -3 1-4 1 LHCb LHCb Pseudo-W (Data) W ν (Simulation) bb X (Simulation) cc X (Simulation) Pseudo-W (Data) W ν (Simulation) Hadrons (Data).5 1 1.5 E / pc

W ν LHCb-PAPER-212-8 arxiv:124.162 Fit positive and negative muon p T spectra in data to expected shapes for signal and backgrounds in 5 η bins Events / (1 GeV/c) 8 7 6 5 4 3 2 1 LHCb + (a) 2 3 4 5 6 7 2 3 4 5 6 7 2. < η < 4.5 p [GeV/c] Data K/π ν Fit Z W ν T - W τν & Z ττ Heavy Flavour Signal and decay in flight templates free to vary; remaining backgrounds fixed N + Candidates = 1466 N - Candidates = 11618 Purity + ~ 79% Purity - ~ 78% W and Z muon p T spectrum at NNLO Simone Bifani MENU 213 17

Results W ν LHCb-PAPER-212-8 arxiv:124.162 Fiducial volume: p T,l > 2 GeV/c, 2. < η l < 4.5 (831 ± 9 stat ± 27 syst ± 29 lumi ) pb (656 ± 8 stat ± 19 syst ± 23 lumi ) pb 1.27 ±.2 stat ±.1 syst Results in general agreement with NNLO predictions Main systematics: background templates, efficiencies (statistical in nature) Simone Bifani MENU 213 18

l Results W ν LHCb-PAPER-212-8 LHCb-CONF-213-5 [pb] dσ W ν/dη 8 LHCb, s = 7 TeV 7 6 5 4 3 2 1 p T > 2 GeV/c + W + ν stat + W + ν tot - - W ν stat - - W ν tot 2 2.5 3 3.5 4 4.5 Data Data Data Data MSTW8 ABKM9 JR9 NNPDF21 HERA15 CTEQ6M (NLO) η [pb] dσ/dη 7 6 5 4 3 2 1 + LHCb 21, W ν - LHCb 21, W ν + ATLAS 21, W ν - ATLAS 21, W ν extrapolated extrapolated.5 1 1.5 2 2.5 3 3.5 4 4.5 η l Good agreement with NNLO Good agreement with ATLAS (after adapting to ATLAS cuts) Simone Bifani MENU 213 19

Results W ν LHCb-PAPER-212-8 LHCb-CONF-213-5 A.6.4.2 -.2 -.4 LHCb, Datastat Datatot s = 7 TeV MSTW8 ABKM9 JR9 NNPDF21 HERA15 CTEQ6M (NLO) -.6 1 2 3 4 p T > 2 GeV/c η Lepton charge asymmetry.4.2 -.2 -.4 -.6 l p T LHCb 21, W ν CMS 21, W ν CMS 21, W eν > 25 GeV/c.5 1 1.5 2 2.5 3 3.5 4 4.5 l eta Good agreement with NNLO Good agreement with CMS (after adapting to CMS cuts) Simone Bifani MENU 213 2

Z/γ* +jet! LHCb-CONF-212-16 Preliminary L ~1 fb -1 (211) Same trigger & selection as Z Jet reconstruction» Particle Flow: tracks, calorimeter clusters, Vs» Anti-k t algorithm (R=.5)» Jet ID: veto on isolated particles, require tracks from primary vertex» Jet Energy Correction from MC Jet requirements» p T > 1 GeV/c» 2. < η < 4.5» ΔR(jet, ) >.4 Event Rate [GeV/c] T p 8 7 6 5 4 3 2 1.12.1.8.6.4.2 LHCb Preliminary s = 7 TeV Data 3 LHCb preliminary s = 7 TeV 2 Inclusive Z Inclusive Z + Jet 6 8 1 12 Reconstructed Z Decay Muons Jet 1 φ -1-2 -3 M() [GeV] 2 3 η 4 5 Simone Bifani MENU 213 21

Results Z/γ* +jet! LHCb-CONF-212-16 Preliminary Number of Candidates 3 1 2 1 LHCb preliminary s = 7 TeV Data Simulation Number of Candidates 16 14 12 1 8 6 4 LHCb preliminary s = 7 TeV Data Simulation 1 2 4 6 8 1 p (Jet) [GeV] T 2 2 2.5 3 3.5 4 4.5 η(jet) Simulation well describes the data JEC is validate on data 1 st step for jet measurements at LHCb Event Rate.8.7.6.5.4.3.2.1 LHCb Preliminary s = 7 TeV Data.5 1 1.5 2 p 211 Data Simulation T (Jet) / p (Z) T Simone Bifani MENU 213 22

Results Z/γ* +jet! LHCb-CONF-212-16 Preliminary + n Jets) σ(z ) σ (Z 1-1 1 LHCb preliminary s = 7 TeV ] -1 ) [GeV / σ(z.7.6.5.4 LHCb preliminary s = 7 TeV -2 1 dσ (Z +Jet) d pt (Z ).3.2.1 1 2 >2 Jet Multiplicity 2 4 6 8 1 p (Z T o ) [GeV] Z!+jet Z! Data :.229 ±.6 stat ±.9 syst Theory :.219 +.6.9 PDF ±.12 scale Simone Bifani MENU 213 23

Summary and Outlook LHCb probes a unique region in η and low p T reach at LHC Z and W production cross-sections measured at 7 TeV in the forward region by using different final states Results consistent with theoretical predictions calculated at NNLO using recent parameterisation of the PDFs Upcoming updates with full 211 and 212 data sets for all analyses Z/γ* +jet paper coming out soon Low mass Drell-Yan: LHCb-CONF-212-12 Simone Bifani MENU 213 24

Backup

LHCb A Forward Spectrometer Complementary η range to ATLAS & CMS» Overlap for cross check 2. < η < 2.5» Unique to LHCb 2.5 < η < 5. η# in LHCb 17%(16%) of W + (W - ) within LHCb 8% of Z within LHCb Simone Bifani MENU 213 26

W & Z Production and PDFs Cancel or highlight PDF uncertainties with ratios» A = (dσ W+ - dσ W- ) / (dσ W+ + dσ W- ) tests u V and d V difference A # R W#» R W = dσ W+ / dσ W- tests d V /u V ratio» R WZ = dσ W / dσ Z almost insensitive to PDFs precise test of SM Many systematic errors cancel Simone Bifani MENU 213 27

Reconstruction Efficiencies Trigger» Tag: triggered muon#» Probe: offline identified muon Tracking Tracking» Tag: identified muon track» Probe: trajectory from muon stub and minimal tracking information Particle ID Particle ID» Tag: identified muon#» Probe: reconstructed track Simone Bifani MENU 213 28

Z/γ* ll Simone Bifani MENU 213 29

Z/γ*! Simone Bifani MENU 213 3

Z/γ* ee! Simone Bifani MENU 213 31

Z/γ* ττ! Simone Bifani MENU 213 32

Z/γ* ττ! Simone Bifani MENU 213 33

W ν Event probability -1 1 1 1-2 LHCb Pseudo-W (Data) W ν (Simulation) IP > 8 m (Data) Event probability 1 1-1 1-2 LHCb Pseudo-W (Data) W ν (Simulation) IP > 8 m (Data) -3 1-3 1-4 1 1 2 3 [GeV/c] pcone T -4 1 1 2 3 [GeV] cone E T Simone Bifani MENU 213 34

W ν Fit positive and negative muon p T spectra in data to expected shapes for signal and backgrounds in 5 η bins Events / (1 GeV/c) 25 2 15 1 5 2 3 4 5 6 7 2 3 4 5 6 7 LHCb + - (b) 2 3 4 5 6 7 2 3 4 5 6 7 2. < η < 2.5 p [GeV/c] T Events / (1 GeV/c) 2 3 4 5 6 7 2 3 4 5 6 7 3 LHCb + - 25 (c) 2 15 1 5 2 3 4 5 6 7 2 3 4 5 6 7 2.5 < η < 3. p [GeV/c] T 22 2 LHCb + - 18 (d) 16 14 12 1 8 6 4 2 2 3 4 5 6 7 2 3 4 5 6 7 3. < η < 3.5 p [GeV/c] Events / (1 GeV/c) T Events / (1 GeV/c) 1 8 6 LHCb + (e) - Events / (1 GeV/c) 25 2 15 LHCb + (f) - 4 1 2 5 2 3 4 5 6 7 2 3 4 5 6 7 3.5 < η < 4. p [GeV/c] T 2 3 4 5 6 7 2 3 4 5 6 7 4. < η < 4.5 p [GeV/c] W and Z muon p T spectrum at NNLO Simone Bifani MENU 213 35 T

W ν Simone Bifani MENU 213 36

Z/γ* +jet! Simone Bifani MENU 213 37

Z/γ* +jet! Jet Efficiency 1.8.6 LHCb simulation s = 7 TeV Jet Efficiency 1.8.6 LHCb simulation s = 7 TeV.4.2 p p jet T jet T > 5 GeV > 15 GeV.4.2 1.5<η <5. jet 2.<η <4.5 jet 2 3 4 5 jet η 1 2 3 4 jet p T (GeV) Simone Bifani MENU 213 38

References Simone Bifani MENU 213 39

Low Mass DY! LHCb-CONF-212-12 Preliminary L ~37 pb -1 (21) Dimuon trigger: p T > 2.5 GeV/c 2 reconstructed muons» p > 1 GeV/c» p T > 3(15) GeV/c (M > 4 GeV/c 2 )» 2. < η < 4.5» 5 < M < 12 GeV/c 2 Backgrounds» Heavy flavour (Data)» K/π mis-id (Data)» Υ (MC) Fit muon isolation spectrum in data to expected shapes for signal and backgrounds in 9 M bins isolation = p T /p-jet T Purity varies from ~7% (at low mass) to ~1% Simone Bifani MENU 213 4

Results Low Mass DY LHCb-CONF-212-12 Preliminary )] 2 [pb/(gev/c dσ γ* /dm Theory/Data 2 1 LHCb Preliminary, s = 7 TeV 1 1 1.5 1.5 1 p > 1 GeV/c p > 3 (15) GeV/c T 2. < η < 4.5 Data stat Data tot LO PYTHIA (CTEQ5L) NLO FEWZ (MSTW8) NLO DYNNLO (MSTW8) 2 2 ] 1 Dimuon invariant mass [GeV/c [pb] γ* dσ γ* /dy 4 35 3 25 2 15 1 5 p p T > 1 GeV/c > 3 GeV/c 1.5 < M < 2 GeV/c 2 LHCb Preliminary, Data stat Data tot s = 7 TeV LO PYTHIA (CTEQ5L) NLO FEWZ (MSTW8) NLO FEWZ (NNPDF2) NLO FEWZ (CTEQ66) 2 2.5 3 3.5 4 4.5 Dimuon rapidity Main systematic at low mass comes from the fit PYTHIA predictions agree in shape but too low in normalisation Reasonable agreement with NLO predictions where calculations are available Simone Bifani MENU 213 41

Low Mass DY! Events Events Events 22 LHCb preliminary 2 21 data 18 16 14 12 1 8 6 4 2 5 4 3 2 1 12 1 2 5. < M < 7. GeV/c Drell-Yan Upsilon Heavy Flavour Hadron mis-id 2. < y < 4.5.5 1 Minimum muon isolation.5 1 Minimum muon isolation 8 6 4 2 2 12.5 < M < 15. GeV/c 2 3. < M < 4. GeV/c 2. < y < 4.5 2. < y < 4.5.5 1 Minimum muon isolation Events Events Events 2 7. < M < 9. GeV/c 2. < y < 4.5 24 22 2 18 16 14 12 1 8 6 4 2.5 1 Minimum muon isolation 2 15. < M < 2. GeV/c 2. < y < 4.5 45 4 35 3 25 2 15 1 5.5 1 Minimum muon isolation 8 7 6 5 4 3 2 1 2 4. < M < 6. GeV/c 2. < y < 4.5.5 1 Minimum muon isolation Events Events Events 8 7 6 5 4 3 2 1 3 25 2 15 1 2 1.5 < M < 12.5 GeV/c.5 1 Minimum muon isolation 5 2 2. < M < 3. GeV/c 2 6. < M < 12 GeV/c 2. < y < 4.5 2. < y < 4.5.5 1 Minimum muon isolation 2. < y < 4.5 9 8 7 6 5 4 3 2 1.5 1 Minimum muon isolation Simone Bifani MENU 213 42

Low Mass DY! Simone Bifani MENU 213 43