Review of final-state structure of pp interactions at the LHC Paolo Gunnellini
|
|
- Ferdinand Frederick Bradley
- 6 years ago
- Views:
Transcription
1 Review of final-state structure of pp interactions at the LHC Paolo Gunnellini DESY (Deutsches Elektronen Synchrotron), Hamburg QCD at cosmic energies Kalchida (Greece) May 6 Paolo Gunnellini QCD at cosmic energies May 6
2 Outline Final states at the LHC Generalities on Monte Carlo event generators Generator tuning and machinery Available tunes Our understanding of QCD exp. data Current issues and incompatibilities Comparison between predictions and measurements Diffractive selections Hard QCD events and multijet scenarios Vector-boson final states op-antitop final states 5 Universality of tunes? 6 Summary and conclusions DISCLAIMER: Mainly results from ALAS and CMS! Paolo Gunnellini QCD at cosmic energies May 6
3 Hard scattering at the LHC o simulate proton-proton collisions, physicists generally use Monte Carlo event generators Ingredients of the hard scattering Factorization theorem Parton distribution functions Matrix element calculation..starting from lowest order in α S but might include additional real and virtual corrections σ ab F (Q ) = dx dx f a (x, Q ) f b (x, Q ) ˆσ ab (x, x, Q ) otal Cross Section Partonic Cross Section Parton Distribution Functions with x = longitudinal proton momentum fraction carried by the parton Q = scale of the scattering Paolo Gunnellini QCD at cosmic energies May 6
4 he underlying event at the LHC Paolo Gunnellini QCD at cosmic energies May 6
5 Final states at the LHC What can be produced in proton-proton collisions? From soft to hard.. Soft particles Jets Heavy flav. jets Vector boson op quark Vector boson pair Higgs... Standard Model otal Production Cross Section Measurements Status: Nov 5 σ [pb] 8 µb ALAS Preliminary heory Run, s = 7, 8, ev LHC pp s = 7 ev 6 Data.5.9 fb LHC pp s = 8 ev 5 5 pb Data. fb 5 pb LHC pp s = ev Data 85 pb. fb total. fb VBF VH t th pp W Z t t tt chan WW H Wt WZ ZZ ts chan t tw t tz Huge collection of measurements about these final states..in this talk only some of them with focus on our understanding of the experimental results! Paolo Gunnellini QCD at cosmic energies May 6 5
6 MC generator types Pure matrix element (ME) simulation MC integration of cross section + PDF No hadronization nor UE Useful for theoretical studies, no exclusive events generated Event generators Combination of ME and parton showers Generator for fixed-order ME combined with leading log (LL) parton shower MC Exclusive events, useful for experimentalists Paolo Gunnellini QCD at cosmic energies May 6 6
7 MC generator types Paolo Gunnellini QCD at cosmic energies May 6 7
8 MC generator types Paolo Gunnellini QCD at cosmic energies May 6 8
9 MC generator types Paolo Gunnellini QCD at cosmic energies May 6 9
10 Details of the Monte Carlo generators Example: multijet final state PYHIA8 and HERWIG++: LO MC generators with extra jets from PS & MPI SHERPA, MADGRAPH: matrix element with N-jets (extra real emission) POWHEG: matrix element with a hard NLO (real & virtual) PYHIA, HERWIG SHERPA MADGRAPH@LO POWHEG Paolo Gunnellini QCD at cosmic energies May 6
11 he Underlying Event at the LHC [mb] σ eff CMS (W + jets) ALAS (W + jets) 5 CDF ( jets) CDF (γ + jets) Corrected CDF (γ + jets) D (γ + jets) UA ( jets - lower limit) 5 AFS ( jets - no errors given) 5 5 Hard scattering Initial and Final State Radiation Multiple Parton Interactions (MPI) Beam-beam remnants Hadronization... 5 s [ev] In general, the UE is a softer contribution but.. some MPI can be hard! Double Parton Scattering σ DPS AB σ DPS AB = m σ eff P A = σ A σ pp tot P B = σ B σ pp tot m P AP B σ pp tot σ pp tot σ A σ B σ eff Need for correlations! Paolo Gunnellini QCD at cosmic energies May 6
12 How do we deal with that? Montecarlo event generators (PYHIA, HERWIG, SHERPA..) Parameters need to be adjusted (tuned) to describe data MPI Primordial k Parton shower Hadronization e.g. p = pref (E/E ref ) ɛ Proton matter distribution profile Colour reconnection e.g. Width of the gaussian used for modelling the parton primordial k inside the proton e.g. Strong coupling value Regularization cut-off Upper scale e.g. Length of fragmentation strings Strange baryon suppression How does one tune all these? Choice of parameter ranges and sensitive observables Predictions for different parameter choices and interpolation of the MC response Data-MC difference and minimisation over parameter space Paolo Gunnellini QCD at cosmic energies May 6
13 Some official tunes from the authors.. PYHIA 8 HERWIG++ Monash une - PDF: NNPDF.LO (EPJ C7 () 8) UE-EE-5C - PDF: CEQ6L (JHEP () ) PYHIA 8 Monash HERWIG++ UE-EE-5C (soft) MPI UE pp( p) data at various s UE pp( p) data at various s Value of measured σ eff Primordial k p spectrum of lepton pair p spectrum of Z boson from Z decays in hadronic collisions in hadronic collisions Parton shower Event shapes in p p interactions Jet multiplicity, jet rates and (taken from previous tune) shapes at various colliders Hadronization Particle multiplicities in hadronic Particle production at Z decays in e + e collisions various colliders General approach is a factorized tuning procedure with only some of the components investigated N.B. For the DPS simulation, generators normally use parameters of soft MPI and extrapolate to harder scales Paolo Gunnellini QCD at cosmic energies May 6
14 Can they be refined? How well do they describe observables at different energy? N ch and p sum as a function of the leading charged particle RANS MIN: sensitive to MPI RANS MAX: sensitive to MPI and PS RANS DIF: sensitive to PS RANS AVE: sensitive to MPI and PS PURPOSE: uning MPI and colour reconnection parameters Leading Object Direction Δφ ransverse- oward Away ransverse- Jet # Pmax Direction ransmax oward Away oward-side Jet Δφ ransmin Away-Side Jet Paolo Gunnellini QCD at cosmic energies May 6
15 Results of the energy-dependence tuning Charged particle mult. in the MAX (left) and 7 (right) ev (/Nevents)dN ch/dηdφ MC/data (/Nevents)dN ch/dηdφ MC/data ransmaxcharged-particledensity s =9GeV CDF data PYHIA8 une C CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M p max [GeV] ransmaxcharged-particledensity s =9GeV CDF data HERWIG++ une UE-EE-5C CUEHppS p max [GeV] MC/data (/Nevents)dN ch/dηdφ MC/data (/Nevents)dN ch/dηdφ ransmaxcharged-particledensity s =7eV CMS data PYHIA8 une C CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO. CUEP8M p max [GeV] ransmaxcharged-particledensity s =7eV CMS data HERWIG++ une UE-EE-5C CUEHppS p max [GeV] New tunes! PYHIA 8 (CUEP8) HERWIG++ (CUEHpp) with various PDFs Better constrain of the energy extrapolation CR changes with the choice of the PDF Rising part and plateaux region are well predicted by the new tunes (arxiv 5.85) Paolo Gunnellini QCD at cosmic energies May 6 5
16 une performance at the new energy N ch /dη dφ> <d / dη ch dn /N ev.5.5. MC / Data n ch, ALAS p > 5 MeV, Preliminary s <.5 η = ev Data PYHIA 8 A PYHIA 8 Monash HERWIG++ UE-EE5 EPOS LHC QGSJE II η.5 ransverse region ALAS Preliminary...9 p >.5 GeV, η <.5 lead p > GeV DAA (uncorrected) PYHIA 8 A HERWIG++ EE5 s = ev EPOS PYHIA 8 A PYHIA 8 Monash dn ch /dη CMS pp s = ev inelastic data PYHIA8 CUEP8S EPOS LHC (GeV) η ( φ) / p Σ data/mc data.8 Pythia8 + CUEP8M CMS.6 Pythia8 + Monash Preliminary EPOS. Herwig + CUEHS Leading rack p (GeV) plead [GeV] Paolo Gunnellini QCD at cosmic energies May 6 6 η HIS_data_syserror - 8 nb transmin Stat. Uncertainty Stat. + Syst. Uncertainty ( ev) s = ev OP: dn/dη ALAS-CONF-5-8, PLB75 (5) BOOM: N ch vs p lead ALAS-PHYS-5-9, CMS-FSQ-5-7 Current tunes reproduce the data at ev! May the energy dependence of the MPI be improved in the generators? p = pref (E/E ref ) ɛ
17 What about other observables? (arxiv 5.85) dn ch/dη Min. Bias observables Charged-particlemultiplicity, s =7eV Forward region UE vs p jet MC/data.. ALICE data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M η Incl. jet cross sections Z-boson observables DPS observables Paolo Gunnellini QCD at cosmic energies May 6 7
18 What about other observables? (arxiv 5.85) dn ch/dη MC/data. Min. Bias observables Charged-particlemultiplicity, s =7eV ALICE data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M η Incl. jet cross sections dn ch/d η MC/data.5 Forward region Charged-particlemultiplicity, s =7eV OEM data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M η Z-boson observables UE vs p jet DPS observables Paolo Gunnellini QCD at cosmic energies May 6 8
19 What about other observables? (arxiv 5.85) dn ch/dη MC/data. Min. Bias observables Charged-particlemultiplicity, s =7eV ALICE data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M η Incl. jet cross sections dn ch/d η MC/data Forward region. Charged-particlemultiplicity, s =7eV OEM data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M η Z-boson observables d N ch/dηdφ UE vs p jet.... ransaven chdensity, s =.76eV CMS data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M CUEHppS p(leading charged-particle jet)[gev] DPS observables Paolo Gunnellini QCD at cosmic energies May 6 9
20 What about other observables? (arxiv 5.85) dn ch/dη MC/data d σ/dpdy[pb/gev] MC/data. Min. Bias observables Charged-particlemultiplicity, s =7eV ALICE data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M η Incl. jet cross sections CMS,Inclusivejets, s =7eV,.5 < y < CMS data PH+CUEP8M PH+CUEP8S-HERAPDF.5LO p[gev] dn ch/d η MC/data Forward region. Charged-particlemultiplicity, s =7eV OEM data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M η Z-boson observables d N ch/dηdφ UE vs p jet.... ransaven chdensity, s =.76eV CMS data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M CUEHppS p(leading charged-particle jet)[gev] DPS observables Paolo Gunnellini QCD at cosmic energies May 6
21 What about other observables? (arxiv 5.85) dn ch/dη MC/data d σ/dpdy[pb/gev] MC/data. Min. Bias observables Charged-particlemultiplicity, s =7eV ALICE data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M η Incl. jet cross sections CMS,Inclusivejets, s =7eV,.5 < y < CMS data PH+CUEP8M PH+CUEP8S-HERAPDF.5LO p[gev] dn ch/d η MC/data /σ dσ/dp(z)[/gev] Forward region. 5 6 Charged-particlemultiplicity, s =7eV OEM data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M η Z-boson observables Zbosonpinleptonicdecay.. CMS data CUEP8M PH+CUEP8M PH+CUEP8S-HERAPDF.5LO p(z)[gev] d N ch/dηdφ UE vs p jet.... ransaven chdensity, s =.76eV CMS data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M CUEHppS p(leading charged-particle jet)[gev] DPS observables Paolo Gunnellini QCD at cosmic energies May 6
22 What about other observables? (arxiv 5.85) dn ch/dη MC/data d σ/dpdy[pb/gev] MC/data. Min. Bias observables Charged-particlemultiplicity, s =7eV ALICE data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M η Incl. jet cross sections CMS,Inclusivejets, s =7eV,.5 < y < CMS data PH+CUEP8M PH+CUEP8S-HERAPDF.5LO p[gev] dn ch/d η MC/data /σ dσ/dp(z)[/gev] Forward region. 5 6 Charged-particlemultiplicity, s =7eV OEM data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M η Z-boson observables Zbosonpinleptonicdecay.. CMS data CUEP8M PH+CUEP8M PH+CUEP8S-HERAPDF.5LO p(z)[gev] d N ch/dηdφ (/σ)dσ/d S MC/data UE vs p jet.... ransaven chdensity, s =.76eV CMS data CUEP6S CUEP8S-CEQ6L CUEP8S-HERAPDF.5LO CUEP8M CUEHppS p(leading charged-particle jet)[gev] DPS observables X.. Normalized Sinpp j, s=7ev CMS data CUEP8M CUEHppS S Paolo Gunnellini QCD at cosmic energies May 6
23 Further look at UE/DPS comparisons (arxiv 5.85) une name σ eff value (mb) CUEP8M CUEHppS ransaven ch density, s = 7eV Dedicated tune to DPS-sensitive observables in four-jet final state CDPSP8S σ eff = mb Normalized Sinpp j, s=7ev d N ch /dηdφ..... ALAS data CDPSP8S-j p (leadingtrack)[gev] (/σ)dσ/d S MC/data.. CMS data CUEP8M CUEHppS S Not able to describe both UE and DPS observables at with the same set of tunes Indication for need of a refinement of the current MPI model? Paolo Gunnellini QCD at cosmic energies May 6
24 High multiplicity scenarios /N dn /dp - ) ch.jet ch.jet (GeV/c MC/data >(GeV/c) <p MC/data Low multiplicities mainly softer MPI components High multiplicities contribution of harder MPI ch.jet CMS, pp s = 7 ev η < < N ch data PYHIA8 MPI-off PYHIA8 C PYHIA6 Z* Herwig++.5 UE_EE_M p (GeV/c) CMS, pp s = 7 ev all ch. particles ch.particle ch.particle η <., p >.5 GeV/c data PYHIA8 MPI-off PYHIA8 C PYHIA6 Z* Herwig++.5 UE_EE_M 6 8 N ch 6 8 N ch /N dn /dp - ) ch.jet ch.jet (GeV/c MC/data /N ch.jetdnch.jet/dp[gev/c] ch.jet CMS, pp s = 7 ev η < < N ch data PYHIA8 C PYHIA6 Z* Herwig++.5 UE_EE_M p (GeV/c) p (GeV/c) CMS, s =7eV, η ch.jet <.9, <N ch CMS data CUEP8S-CEQ6L CDPSP8S-j CUEP6S Monash p[gev/c] - Charged-particle measurement - Jet measurement Good agreement for UE tunes at low multiplicities but worse for increasing multiplicities Better description at high multiplicities for the DPS tunes! Normalized jet p spectrum at different multiplicities (top and bottom right) Charged particle spectra p as a function of multiplicity (bottom left) Eur.Phys.J. C7 () 67 Paolo Gunnellini QCD at cosmic energies May 6
25 Diffractive-enhanced final states (I) Diffractive dissociation cross sections as a function of the fraction of the dissociated mass in different ranges dominated by different components est of models for diffractive scenarios (mb) ξ dσ/dlog X CMS <.5 log M Y - 6. µb (7 ev) log (a) ξ X (mb) ξ dσ/dlog X CMS Data PYHIA version: P8-MBR (ε=.8) P8-MBR (ε=.) P8-C P6-Z* <..5 < log M Y - 6. µb (7 ev) log (c) ξ X Best description is provided by MBR generator (arxiv.) which fully simulates the diffractive components and is tuned to evatron data It uses different hadronization parameters to describe charged particle p spectra LEF: SD-enhanced, RIGH: DD-enhanced Phys. Rev. D 9 (5) Paolo Gunnellini QCD at cosmic energies May 6 5
26 Diffractive-enhanced final states (II) /dη ch ) dn events (/N.6.. CMS Preliminary N ch in η <. p >.5 GeV ( ev) SD selection data PYHIA8 CUEM PYHIA8 CUES PYHIA8 CUEM MBR PYHIA8 C MBR /dη ch ) dn events (/N.8.6. CMS Preliminary N ch in η <. p >.5 GeV ( ev) SD selection data PYHIA8 CUEM PYHIA8 CUES PYHIA8 CUEM MBR PYHIA8 C MBR SD-enhanced selection: activity in one region, veto in the other... d N ch/dηdp [(GeV/c) ] Charged hadron p for η =. at s = 7eV Data CUEP8M CUEP8M-MBR CUEP8M-PomFlux p [GeV/c] η (/πp ) d Nch/dηdp [(GeV/c) ] Charged hadron p for η <. at.. s = 7eV Data CUEP8M CUEP8M-MBR CUEP8M-PomFlux 5 6 p [GeV/c] η MBR diffraction model and parameters help to improve the SD observables, due to a better description of low trans.mom. region CMS-FSQ-5-8 Need for different hadronization parameters for diffractive observables than for nondiffractive? Ongoing work! Paolo Gunnellini QCD at cosmic energies May 6 6
27 Jet observables at ev dy (pb/gev) σ / dp d CMS Preliminary C NP anti-k R =.7-7 pb ( ev) 6 y <.5 (x ) 5.5< y <. (x ).< y <.5 (x ).5< y <. (x ).< y <.5 (x ).5< y <. (x ).< y <.7 (x ) Jet p (GeV) Inclusive jet cross section in different rapidity bins Various cone sizes probe different aspects of parton evolution Jets clustered with R =.7 are described by NLO fixed-order calculations and predictions from NLO MC generators LO MC event generators are not able to reproduce the measurement Ratio to C Ratio to PH+P8 CUEM CMS Preliminary R =.7 anti-k y <.5-7 pb ( ev) Data HERAPDF.5 NNPDF. MMH Exp. uncert. heory uncert. Jet p (GeV) - 7 pb ( ev) CMS Preliminary R =.7 anti-k y <.5 Data PH+P8 CUES-CEQ6L PH+P8 CUES-HERAPDF P8 CUEM Hpp CUES Exp. uncert. Jet p (GeV) Fixed-order NLO ME corr. for NP effects with diff. PDF sets MC generators with LO or NLO dijet ME + PS and UE sim. CMS-PAS-SMP-5-7 ALAS-CONF-5- Paolo Gunnellini QCD at cosmic energies May 6 7
28 Jet observables at ev dy (pb/gev) σ / dp d CMS Preliminary C NP anti-k R =. - 7 pb ( ev) 6 y <.5 (x ) 5.5< y <. (x ).< y <.5 (x ).5< y <. (x ).< y <.5 (x ).5< y <. (x ).< y <.7 (x ) Jet p (GeV) Inclusive jet cross section in different rapidity bins Various cone sizes probe different aspects of parton evolution Jets clustered with R =. are not described by NLO fixed-order calculations but only by predictions from NLO MC generators Effect of missing PS contributions relevant for smaller cones Ratio to C Ratio to PH+P8 CUEM CMS Preliminary anti-k R =. y <.5-7 pb ( ev) Data HERAPDF.5 NNPDF. MMH Exp. uncert. heory uncert. Jet p (GeV) - 7 pb ( ev) CMS Preliminary anti-k R =. y <.5 Data PH+P8 CUES-CEQ6L PH+P8 CUES-HERAPDF P8 CUEM Hpp CUES Exp. uncert p [GeV] Paolo Gunnellini QCD at cosmic energies May 6 8 Ratio w.r.t. NLO pqcd (C)... Relative uncertainty of 9% in the integrated luminosity not included Jet p ALAS - 78 pb ev anti-k t jets, y <.5 (GeV) Preliminary R=. DAA (syst., total) NLOJE++ Non-pert. corr. max µ = µ = p F R C MMH NNPDF
29 Multijet observables (I) σ/dm dy* [pb/ev] d ALAS - L dt =.5 fb s = 7 ev anti-k t jets, R =. Systematic uncertainties NLOJE++ C, µ=p exp(. y*) Non-pert. & EW corr y * <.5 ( ) - y * <. ( ) -6 y * <.5 ( ) -9 y * <. ( ) - y * <.5 ( ) -5 y * <. ( ) Inclusive dijet cross section in different rapidity bins as a function of dijet mass Jets clustered with R =. are reproduced by NLO fixed-order calculations JHEP5()59 [ev] m heory/data y* <.5 P obs =.5 =.6.5 C.5 y* <. C HERA P obs HERA P obs =.98 P obs = 6.5 P obs =.68 P obs =.5.5. y* <.5 C HERA - [ev] m heory/data.5 y* <. C HERA P obs =. P obs =.8. y* <.5 C HERA P obs =. P obs = 6.5 y* <. C HERA P obs =.96 P obs = [ev] m ALAS - L dt =.5 fb s = 7 ev anti-k t jets, R =. Statistical uncertainty Systematic uncertainties NLOJE++ µ=p exp(. y*) Non-pert. & EW corr. C HERAPDF.5 epaljet exp. only HERAPDF.5 exp. only Paolo Gunnellini QCD at cosmic energies May 6 9
30 Multijet observables (II) σ/dm dy* [pb/ev] d ALAS - L dt =.5 fb s = 7 ev anti-k t jets, R =. Systematic uncertainties NLOJE++ C, µ=p exp(. y*) Non-pert. & EW corr y * <.5 ( ) - y * <. ( ) -6 y * <.5 ( ) -9 y * <. ( ) - y * <.5 ( ) -5 y * <. ( ) Inclusive dijet cross section in different rapidity bins as a function of dijet mass Jets clustered with R =. are reproduced by MC event generators using NLO dijet ME but sensitivity to UE tunes JHEP5()59 [ev] m heory/data y* < y* <... y* <.5 - [ev] m heory/data y* <.. y* <.5.5 y* < [ev] m ALAS - L dt =.5 fb s = 7 ev anti-k t jets, R =. Statistical uncertainty Systematic uncertainties POWHEG Born C, µ=p EW corr. + PYHIA shower AUEB Perugia Paolo Gunnellini QCD at cosmic energies May 6
31 Multijet observables (III) ) [fb/gev] () dσ / d(p heory/data ) [fb/gev] () dσ / d(p heory/data ALAS ALAS s=8 ev, 95 pb. fb p [GeV] () s=8 ev, 95 pb. fb () p [GeV] Data HEJ (.9) BlackHat/Sherpa (.) NJet/Sherpa (.) () p > GeV otal experimental systematic uncertainty NLO (scale PDF) uncertainty Data Pythia 8 ( ) Herwig++ (.) MadGraph+Pythia (.) () p > GeV otal experimental systematic uncertainty Four-jet scenarios also well described in a wide region of the phase space JHEP (5) 5 Phys.Rev.D89()9 η <.7 SHERPA st nd, jet: POWHEG+P6 Z' MADGRAPH+P6 Z* p > 5 GeV PYHIA8 C rd th, jet: HERWIG++ UE-EE- p > GeV otal Uncertainty - CMS, s = 7 ev, L = 6 pb, pp j+x Subleading jet Jet #pt Paolo Gunnellini QCD at cosmic energies May Leading jet Jet #pt hird jet Fourth jet Jet #pt Jet 5 p (GeV) 5
32 Z boson observables Jets associated to a Z boson Measurement of differential cross sections for different jet multiplicities Crucial test of our QCD predictions! dσ/dh (jets) [pb/gev] CMS Preliminary -.5 fb ( ev) Data (5ns) amc@nlo + PY8 ( j NLO + PS) dσ/dh (jets) [pb/gev] CMS Preliminary -.5 fb ( ev) Data (5ns) amc@nlo + PY8 ( j NLO + PS) ) [pb] jets σ(z( µµ)+n - Z µ + µ + jets Data ALAS Preliminary - ev, 85 pb Sherpa Madgraph anti-k t, R=. jet p > GeV jet y <.5 amc@nlo/data.5.5 anti-k (R =.) Jets jet jet p > GeV, y <. Z/γ* µµ channel Stat. unc. (gen) 6 8 H, N [GeV] jets amc@nlo/data anti-k (R =.) Jets jet jet p > GeV, y <. Z/γ* µµ channel Stat. unc. (gen) 6 8 H, N [GeV] jets Data / Pred... CMS-SMP-5- ALAS-CONF-5- Predictions describe measurements as long as the multiplicity matches the number of partons in the matrix element N jets N jets Paolo Gunnellini QCD at cosmic energies May 6
33 op observables (I) Underlying event in top pair events Measurement of event content in terms of charged particle multiplicity and p est of final-state universality of UE contribution ν μ μ + W + b t t t t W - b ) [/GeV] ch dn ev /d(p /N ev q q CMS Preliminary overall away transverse toward tt -. fb ( ev) Powheg + Pythia 8 (CUEP8M) [GeV] ch p.5 CMS fb ( ev) Preliminary detector-level data tt Powheg + Pythia 8 (CUEP8M) tt Powheg + Pythia 8 (CUEP8M) (Q) tt Powheg + Pythia 8 (CUEP8M) (Q/) tt Powheg + Herwig++ (EE5C) transverse CMS- OP ch p [GeV].5. tt p [GeV] Predictions of POWHEG NLO matrix-element interfaced to P8 tunes from hadronic events are able to reproduce all measured observables in each considered region Paolo Gunnellini QCD at cosmic energies May 6
34 op observables (II) ] op pair in lepton + jets final states Measurement of differential cross sections as a function of top pair p and jet multiplicity est of reliability of predictions in top sector - [pb GeV (tt) dσ dp CMS l+jets particle Preliminary -. fb ( ev) data sys stat stat. MG5_aMC@NLO P8 [FxFx] MG5_aMC@NLO P8 [MLM] Powheg P8 Powheg H++ MG5_aMC@NLO P8 MG5_aMC@NLO H++ dσ d n-jet 5 CMS l+jets particle Preliminary -. fb ( ev) data sys stat stat. MG5_aMC@NLO P8 [FxFx] MG5_aMC@NLO P8 [MLM] Powheg P8 Powheg H++ MG5_aMC@NLO P8 MG5_aMC@NLO H++ theory data.. 5 p (tt) [GeV] theory data.5 >= additional jets NLO predictions describe well the measurements but sensitivity to matching scheme and PS generator CMS-OP-6-8 Paolo Gunnellini QCD at cosmic energies May 6
35 Parton shower and MPI tuning UNING OF PYHIA 8 O OBSERVABLES MEASURED IN DIFFEREN PROCESSES Observables rack jet properties Jet shapes Dijet decorrelations Multijets Z boson p t t gap and jet shapes rack-jet and jet UE Study of the interplay between MPI and parton shower Various PDF sets investigated Extremely important for: testing the universality of the parton shower in leptonic and hadronic collisions testing the performance of UE simulation for different hard scattering processes AL-PHYS-PUB-- Paolo Gunnellini QCD at cosmic energies May 6 5
36 Parton shower and MPI tuning Significant improvement of description of observables in: Drell-Yan (left), top-antitop (center) and jet substructure (right) sectors dσ fid. σ fid. dp Z p dressed muons ALAS Data AU CEQ6L Monash A-CEQ A-MSW A-NNPDF A-HERA ALAS Simulation Z p f gap Gap fraction vs. Q for veto region: y < ALAS Simulation ALAS Data AU CEQ6L Monash A-CEQ A-MSW A-NNPDF A-HERA Q [GeV] /σdσ/dτ Cambridge-Aachen jets, R =., GeV < p < GeV α S values are similar for all PDF used quite high for the hard processes lower for initial- and final-state radiation significantly lower than previous tunes for ISR and FSR Damped shower needed to describe gap fraction in t t events and p Z simultaneously. ALAS Data AU CEQ6L Monash A-CEQ A-MSW A-NNPDF A-HERA ALAS Simulation... N-subjettiness τ Paolo Gunnellini QCD at cosmic energies May 6 6
37 uning higher-order ME matched to parton showers OBSERVABLES: gap fraction, jet shapes and jet multiplicity in t t events GENERAORS: PYHIA 8 standalone, MADGRAPH amc@nlo and POWHEG + PYHIA 8 Different steps of tuning: tuning of ISR and FSR separately, then simultaneous tune to account for their interplay application of tune to matched generators tune of the matched MADGRAPH amc@nlo + PYHIA 8 (Some of the) Outcomes Significant improvement in the description of t t observables Parameters of simultaneous ISR-FSR tune do not differ much from the separate tunes une of matched MADGRAPH+PYHIA 8 has similar parameters to standalone PYHIA 8 AL-PHYS-PUB-5-7, AL-PHYS-PUB-5-8 Paolo Gunnellini QCD at cosmic energies May 6 7
38 Summary and conclusions High energy physics strongly relies on predictions from Monte Carlo event simulation Very sophisticated tunes are available and are able to describe a wide range of observables at different collision energies Actual measurements are sensitive to ME, UE and PS contributions and are able to disentangle them unes obtained at 7 ev (or below) are able to reproduce data at ev in a good level of agreement It is difficult to reproduce data relative to some corners of the phase space within a unique set of parameters (e.g. DPS-sensitive observables, diffraction) Need for more sophisticated models/parametrizations? New measurements, more advanced simulation.. Stay tuned! Paolo Gunnellini QCD at cosmic energies May 6 8
39 Summary and conclusions High energy physics strongly relies on predictions from Monte Carlo event simulation Very sophisticated tunes are available and are able to describe a wide range of observables at different collision energies Actual measurements are sensitive to ME, UE and PS contributions and are able to disentangle them unes obtained at 7 ev (or below) are able to reproduce data at ev in a good level of agreement It is difficult to reproduce data relative to some corners of the phase space within a unique set of parameters (e.g. DPS-sensitive observables, diffraction) Need for more sophisticated models/parametrizations? New measurements, more advanced simulation.. Stay tuned! HANK YOU FOR YOUR AENION Paolo Gunnellini QCD at cosmic energies May 6 9
40 BACKUP SLIDES Paolo Gunnellini QCD at cosmic energies May 6
41 A double parton scattering (DPS) wo different x values for the two partons in each proton Impact parameter b σ DPS A,B = m dx dx ˆσ A(x, x ) dx dx ˆσ B(x, x ) d b f (x, x, b) f (x, x, b) DPS Cross Section Partonic cross sections Double parton distribution functions If the partons are assumed to be uncorrelated: f (x, x, b) = f (x )f (x )F (b) he two scatterings factorize in the cross section formula: σab DPS = m dx dx ˆσ A f (x )f (x ) dx dx ˆσ B f (x )f (x ) d b [F (b)] It is thus defined: σ eff = d b [F (b)] Paolo Gunnellini QCD at cosmic energies May 6
42 Combined fits to whole MPI spectrum Combined fits of observables sensitive to soft, semi-hard and hard MPI (/σ)dσ/d S [/rad] Normalized S in pp j in η <.7 at s = 7 ev CMS data DPS-UE-MB une dn/dη Pseudorapidity (s) = 7 ev, INEL > ALICE data DPS-UE-MB une (/Nevents) dn ch/dηdφ ransmin charged particle density s = 7eV CMS data DPS-UE-MB une (/σ)dσ/d S [/rad] S (rad) Normalized S in pp j in η <.7 at s = 7 ev....9 CMS data DPS-UE-MB-Weighted une S (rad) dn/dη η Pseudorapidity (s) = 7 ev, INEL > ALICE data DPS-UE-MB-Weighted une η No hope to get the measurements well described altogether (/Nevents) dn ch/dηdφ pmax[gev/c] ransmin charged particle density s = 7eV.. CMS data DPS-UE-MB-Weighted une pmax[gev/c] Paolo Gunnellini QCD at cosmic energies May 6
43 Why do we actually tune? Not only for fun! Correct description of the data Pile-up simulation Evaluation of detector effects and unfolding Estimation of background (in MC-driven approach) Models are not allowed to fail Good physics predictions Correct evaluation of physics effects Models are allowed to fail he danger is overtuning! Paolo Gunnellini QCD at cosmic energies May 6
Hard And Soft QCD Physics In ATLAS
Hard And Soft QCD Physics In ALAS Stefanie Adomeit on behalf of the ALAS collaboration International Conference on New Frontiers in Physics - Crete, June -6, QCD Measurements in ALAS at LHC every kind
More informationMulti-differential jet cross sections in CMS
Multi-differential jet cross sections in CMS A. Bermudez Martinez on behalf of the CMS collaboration. Deutsches Elektronen-Synchrotron (DESY) April 07 A. Bermudez (DESY) April 07 / 5 QCD Main background
More informationarxiv: v1 [hep-ex] 2 Nov 2017
Proceedings of the Fifth Annual LHCP CR-7/358 November 3, 7 Measurement of jet properties in arxiv:7.654v [hep-ex] Nov 7 Patrick L.S. Connor DESY, Notkestrasse 87, 67 Hamburg, Germany ABSRAC We present
More informationMeasurements of the production of a vector boson in association with jets in the ATLAS and CMS detectors
Measurements of the production of a vector boson in association with s in the ALAS and CMS detectors Vieri Candelise University of rieste and INFN rieste, Via Valerio 2, 3428, rieste, Italy Abstract. he
More informationPhysics at Hadron Colliders Part II
Physics at Hadron Colliders Part II Marina Cobal Università di Udine 1 The structure of an event One incoming parton from each of the protons enters the hard process, where then a number of outgoing particles
More informationMeasurement of the jet production properties at the LHC with the ATLAS Detector
Measurement of the jet production properties at the LHC with the ALAS Detector Stanislav okar Comenius University, Bratislava On behalf of the ALAS collaboration Different features of the jet production
More informationOverview of QCD measurements at high pt
Overview of QCD measurements at high p () Material from ALAS, CMS, LHCb and evatron QCD in all its beauty in MCs Hadronization Parton Shower Hard Process Beam Beam Underlying Event Challenges at the LHC
More informationMeasurements of event properties and multi-differential jet cross sections and impact of CMS measurements on Proton Structure and QCD parameters
Measurements of event properties and multi-differential cross sections and impact of measurements on Proton Structure and QCD parameters Anterpreet Kaur Panjab University, Chandigarh (India On behalf of
More informationInclusive jet cross section in ATLAS
Inclusive jet cross section in ALAS (on behalf of the ALAS collaboration) Pavel Starovoitov CERN -04-0 he researcher is supported by Marie Curie Incoming International Fellowship of the European Commission
More informationTests of QCD Using Jets at CMS. Salim CERCI Adiyaman University On behalf of the CMS Collaboration IPM /10/2017
Tests of QCD Using Jets at CMS Salim CERCI Adiyaman University On behalf of the CMS Collaboration IPM-2017 24/10/2017 2/25 Outline Introduction QCD at LHC QCD measurements on the LHC data Jets The strong
More informationSmall-x QCD and forward physics results from CMS
Small-x QCD and forward physics results from CERN E-mail: gabor.veres@cern.ch he Collaboration has a comprehensive program of small-x QCD and forward physics measurements, which is supported by an excellent
More informationLHC MPI and underlying event results
LHC MPI and underlying event results Marianna Testa (ATLAS) for the ALICE, ATLAS, CMS & LHCb collaborations SM@LHC 2012, Copenhagen, 10-13 April 2012 The Underlying Event Everything in hadron collisions
More informationATLAS Measurements Sensitive to the Proton Structure
EPJ Web of Conferences will be set by the publisher DOI: will be set by the publisher c Owned by the authors, published by EDP Sciences, 05 ALAS Measurements Sensitive to the Proton Structure P. J. Bussey,a
More informationDouble parton scattering studies in CMS
CBPF-Centro Brasileiro de Pesquisas Fisicas, Rio de Janeiro, Brazil E-mail: gilvan@cern.ch he double parton scattering (DPS) process in proton-proton collisions at a center-of-mass energy of 7 and 3 ev
More informationInclusive W and Z: Precision LHC Measurements
Inclusive W and : Precision LHC Measurements Philip Ilten on behalf of the ALAS, CMS, and LHCb Collaborations Massachusetts Institute of echnology May 3, 6 Ilten LHC W and Measurements May 3, 6 / 6 Introduction
More informationDifferential Top Cross-section Measurements
Differential op Cross-section Measurements ALPS207 Obergurgl Michael Fenton on behalf of the ALAS Collaboration University of Glasgow m.fenton.@research.gla.ac.uk April 8, 207 Michael Fenton Differential
More informationNew results from CMS for PDF studies
New results from CMS for PDF studies Oleksandr Zenaiev (DESY) on behalf of the CMS Collaboration PDF4LHC 7.3.7 / O. Zenaiev New results from CMS for PDF studies Outline Measurement of double-differential
More informationProton anti proton collisions at 1.96 TeV currently highest centre of mass energy
Tevatron & Experiments 2 Proton anti proton collisions at 1.96 TeV currently highest centre of mass energy Tevatron performing very well 6.5 fb 1 delivered (per experiment) 2 fb 1 recorded in 2008 alone
More informationAtlas results on diffraction
Atlas results on diffraction Alessia Bruni INFN Bologna, Italy for the ATLAS collaboration Rencontres du Viet Nam 14th Workshop on Elastic and Diffractive Scattering Qui Nhon, 16/12/2011 EDS 2011 Alessia
More informationLatest CMS results on low x physics and di raction
Latet CMS reult on low x hyic and di raction Benoit Roland (DESY) On behalf of the CMS Collaboration eracale Workho 04-3 December 04 DESY, Hamburg Benoit Roland (DESY) Latet CMS reult low x and di raction
More informationDouble Parton Scattering in CMS. Deniz SUNAR CERCI Adiyaman University On behalf of the CMS Collaboration Low-x th June 2017 Bari, Italy
Double Parton Scattering in CMS Deniz SUNAR CERCI Adiyaman University On behalf of the CMS Collaboration Low-x 2017 17th June 2017 Bari, Italy Outline Introduction to DPS DPS measurements with CMS 2b +
More informationATLAS jet and missing energy reconstruction, calibration and performance in LHC Run-2
Prepared for submission to JINS International Conference on Instrumentation for Colliding Beam Physics 7 February - March, 7 Budker Institute of Nuclear Physics, Novosibirsk, Russia ALAS jet and missing
More informationQCD and jets physics at the LHC with CMS during the first year of data taking. Pavel Demin UCL/FYNU Louvain-la-Neuve
QCD and jets physics at the LHC with CMS during the first year of data taking Pavel Demin UCL/FYNU Louvain-la-Neuve February 8, 2006 Bon appétit! February 8, 2006 Pavel Demin UCL/FYNU 1 Why this seminar?
More informationMonte Carlo activities in ALICE
Monte Carlo activities in ALICE status and prospects Jochen Klein for the ALICE Collaboration CERN 8th International Workshop on Multiple Partonic Interactions at the LHC San Cristóbal de las Casas, Chiapas,
More informationRecent results on soft QCD topics from ATLAS
Recent results on soft QCD topics from ATLAS Roman Lysák Institute of Physics, Prague on behalf of the ATLAS collaboration Bormio 2016 Overview Understanding of soft-qcd interactions has direct impact
More informationMC ATLAS Stephen Jiggins on behalf of the ATLAS Collaboration University College London (UCL)
MC Tuning @ ATLAS Stephen Jiggins on behalf of the ATLAS Collaboration University College London (UCL) Contents Contents: 1) Monte Carlo models/event generation 2) Basic Tuning Methodology 3) A2 tune series
More informationarxiv: v1 [hep-ex] 17 Aug 2016
arxiv:8.95v [hep-ex] 7 Aug Measurement of the underlying-event properties with the detector Yuri Kulchitsky, on behalf of the collaboration Institute of Physics, National Academy of ciences, Minsk, Belarus
More informationPoS( EPS-HEP 2013)435
AL-PHYS-PROC-0-5/09/0 Inclusive and dijet jet production measured with the ALAS detector University of Oxford E-mail: lucy.anne.kogan@cern.ch Inclusive jet and dijet double differential cross sections
More informationarxiv: v1 [hep-ex] 15 Jan 2019
CMS-CR-8/37 January 7, 9 Top Quark Modelling and Tuning at CMS arxiv:9.559v [hep-ex] 5 Jan 9 Emyr Clement on behalf of the CMS Collaboration University of Bristol Recent measurements dedicated to improving
More informationarxiv: v1 [hep-ex] 28 Aug 2017
Proceedings of the Fifth Annual LHCP AL-PHYS-PROC-7-99 November 9, 8 Boosted top production in ALAS and arxiv:78.864v [hep-ex] 8 Aug 7 Marino Romano On behalf of the ALAS and Collaborations, INFN, Sezione
More informationMeasurement of multijets and the internal structure of jets at ATLAS
Measurement of multijets and the internal structure of jets at ALAS Bilge M. Demirköz, on behalf of the ALAS Collaboration Institut de Fisica d Altes Energies, Barcelona, SPAIN also at Middle East echnical
More informationLatest results on top production from the CMS and ATLAS collaborations: inclusive and differential measurements
Latest results on top production from the CMS and ALAS collaborations: inclusive and differential measurements E. assi On behalf of the CMS and ALAS Collaborations XLV International Symposium on Multiparticle
More informationW/Z + jets and W/Z + heavy flavor production at the LHC
W/Z + jets and W/Z + heavy flavor production at the LHC A. Paramonov (ANL) on behalf of the ATLAS and CMS collaborations Moriond QCD 2012 Motivation for studies of jets produced with a W or Z boson Standard
More informationRecent QCD results from ATLAS
Recent QCD results from ATLAS PASCOS 2013 Vojtech Pleskot Charles University in Prague 21.11.2013 Introduction / Outline Soft QCD: Underlying event in jet events @7TeV (2010 data) Hard double parton interactions
More informationW/Z inclusive measurements in ATLAS
/Z inclusive measurements in J-B. Blanchard On behalf of the Atlas collaboration Standard Model @ LHC 1-1/4/1 Introduction /Z physics at the LHC LHC: a /Z factory... heoretically well understood bosons,
More informationOther ATLAS Jet Measurements
Other ALAS Jet Measurements Michael Begel Aril, Jets as Hard Probes Michael Begel Standard Model @ LHC ALAS Jet Measurements Aril, High dijet roduction rovides a owerful robe of the hard scatter recision
More informationTevatron Energy Scan. Energy Dependence of the Underlying Event. Rick Field Craig Group & David Wilson University of Florida
Rick Field Craig Group & David Wilson University of Florida Tevatron Energy Scan Energy Dependence of the Underlying Event Outline of Talk Wine & Cheese talk, October 4, 2002. Studying the underlying event
More informationMulti-jet production and jet correlations at CMS
Multi-jet production and jet correlations at Gábor I. Veres on behalf of the Collaboration CERN E-mail: gabor.veres@cern.ch Hadronic jet production at the LHC is an excellent testing ground for QCD. Essential
More informationOverview of PDF-sensitive measurements from Run I in ATLAS
Overview of PDF-sensitive measurements from Run I in ATLAS on behalf of ATLAS Parton Distributions for the LHC 05 February 5- ATLAS SM Measurements Traditional processes for PDF fits include jets, Drell-Yan
More informationSOFT QCD AT ATLAS AND CMS
SAHAL YACOOB UNIVERSITY OF CAPE TOWN ON BEHALF OF THE ATLAS AND CMS COLLABORATIONS SOFT QCD AT ATLAS AND CMS 28th Rencontres de Blois INTRODUCTION IN 15 MINUTES 2 Inelastic cross section ATLAS and CMS
More informationThe Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS CR -2013/016 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 18 January 2013 (v2, 21 January 2013)
More informationQCD Studies at LHC with the Atlas detector
QCD Studies at LHC with the Atlas detector Introduction Sebastian Eckweiler - University of Mainz (on behalf of the ATLAS Collaboration) Examples of QCD studies Minimum bias & underlying event Jet-physics
More informationMeasurement of diffractive and exclusive processes with the ATLAS detector
EPJ Web of Conferences will be set by the publisher DOI: will be set by the publisher c Owned by the authors, published by EDP Sciences, 15 Measurement of diffractive and exclusive processes with the ALAS
More informationMeasurement of jet production in association with a Z boson at the LHC & Jet energy correction & calibration at HLT in CMS
Measurement of jet production in association with a Z boson at the LHC & Jet energy correction & calibration at HLT in CMS Fengwangdong Zhang Peking University (PKU) & Université Libre de Bruxelles (ULB)
More informationUsing Drell-Yan to Probe the
Using Drell-Yan to Probe the Underlying Event in Run 2 at CDF Deepak Kar University of Florida (On behalf of the CDF Collaboration) Experimental Particle Physics Seminar 30 th October 2008 Prologue: We
More informationPrecision QCD at the Tevatron. Markus Wobisch, Fermilab for the CDF and DØ Collaborations
Precision QCD at the Tevatron Markus Wobisch, Fermilab for the CDF and DØ Collaborations Fermilab Tevatron - Run II Chicago Ecm: 1.8 1.96 TeV more Bunches 6 36 Bunch Crossing 3500 396ns CDF Booster Tevatron
More informationPDF Studies at LHCb! Simone Bifani. On behalf of the LHCb collaboration. University of Birmingham (UK)
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
More informationReview of LHCb results on MPI, soft QCD and diffraction
Review of LHCb results on MPI, soft QCD and diffraction Marcin Kucharczyk on behalf of LHCb collaboration HNI Krakow EDS Blois 2015, Borgo (Corse), 30.06.2015 Outline LHCb - general purpose forward experiment
More informationQCD at Cosmic Energies - VII May 16-20, 2016 Chalkida, Greece Multiparton interactions in Herwig
QCD at Cosmic Energies - VII May 6-20, 206 Chalkida, Greece Multiparton interactions in Herwig Frashër Loshaj Table of Contents Introduction 2 MPI and the Underlying event 3 Soft interactions 4 Diffraction
More informationElectroweak Measurements at LHCb!
Electroweak Measurements at LHCb! Simone Bifani University of Birmingham (UK) on behalf of the LHCb collaboration LHCb workshop on quantum interference effects, QCD measurements and generator tuning CERN,
More informationPrecise measurements of the W mass at the Tevatron and indirect constraints on the Higgs mass. Rencontres de Moriond QCD and High Energy Interactions
Precise measurements of the W mass at the evatron and indirect constraints on the Higgs mass Rafael Lopes de Sá for the CDF and DØ Collaborations March 11, 212 Rencontres de Moriond QCD and High Energy
More informationThe Monash 2013 Tune of PYTHIA 8
he Monash 3 une of PYHIA Peter Skands (CERN) Current Default = C (from ) LEP tuning undocumented (from 9) LHC tuning only used very early data + S. Rojo & S. Carrazza recently added a new PDF set: NNPDF.3
More informationLHCP QCD at the Tevatron. Rick Field University of Florida (for the CDF & D0 Collaborations) Outline of Talk. with help from Christina Mesropian
with help from Christina Mesropian QCD at the Tevatron Rick Field University of Florida (for the CDF & D0 Collaborations) Outline of Talk D0 Photon + Jet Measurements. CDF W/Z + Upsilon Search. CDF Measurements
More informationATLAS Measurements of Boosted Objects
BOOS24 University College London, 8-22 August 24 ALAS Measurements of Boosted Objects Christoph Anders on behalf of the ALAS collaboration Physikalisches Institut Universita t Heidelberg August 9th 24
More informationMini-Bias and Underlying Event Studies at CMS
Yuan Chao Department of Physics National Taiwan University 1617 Taipei, TAIWAN 1 Introduction The Tevatron experiments provide us very good information for the quantum chromodynamics (QCD) modelings of
More informationElectroweak results. Luca Lista. INFN - Napoli. LHC Physics
Electroweak results Luca Lista INFN - Napoli EWK processes at LHC p p W and Z production in pp collisions proceeds mainly form the scattering of a valence quark with a sea anti-quark The involved parton
More informationPANIC August 28, Katharina Müller on behalf of the LHCb collaboration
Measurements with electroweak bosons at LHCb PANIC August 28, 2014 on behalf of the LHCb collaboration Outline LHCb detector Measurements with electroweak bosons Motivation Z production Z plus jets, Z
More informationTop production measurements using the ATLAS detector at the LHC
Top production measurements using the ATLAS detector at the LHC INFN, Sezione di Bologna and University of Bologna E-mail: romano@bo.infn.it This paper is an overview of recent results on top-quark production
More informationTesting QCD at the LHC and the Implications of HERA DIS 2004
Testing QCD at the LHC and the Implications of HERA DIS 2004 Jon Butterworth Impact of the LHC on QCD Impact of QCD (and HERA data) at the LHC Impact of the LHC on QCD The LHC will have something to say
More informationInclusive. W & Z measurements in CMS. Georgios Daskalakis. on behalf of CMS Collaboration. .C.S.R. Demokritos
Inclusive W & Z measurements in CMS Georgios Daskalakis.C.S.R. Demokritos on behalf of CMS Collaboration 1 Overview LHC hopefully will be proven to be a discovery machine but before that the measurement
More informationFirst 13 TeV results from CMS
First 3 TeV results from Ferenc Siklér Wigner RCP, Budapest for the Collaboration ISMD 5, Wildbad Kreuth 9 Oct 5 Introduction pp at s = 3 TeV First physics basics, QCD d/dη of charged hadrons 55 k and
More informationAzimuthal Correlations for Inclusive 2-jet, 3-jet and 4-jet events in pp collisions at s = 13 TeV with CMS
Azimuthal Correlations for Inclusive 2-jet, 3-jet and 4-jet events in pp collisions at s = 13 TeV with CMS Paris Gianneios University of Ioannina 29 th March 2018, HEP Athens Outline 1 2 3 4 5 CMS Detector
More informationResults on QCD jet production at the LHC (incl. Heavy flavours)
Results on QCD jet production at the LHC (incl. Heavy flavours) R. Seuster (TRIUMF) On behalf of the ATLAS and CMS collaborations Recontres du Vietnam August 11th 17th, 2013 Windows on the Universe Outline
More informationMeasurements of the Vector boson production with the ATLAS Detector
EPJ Web of Conferences will be set by the publisher DOI: will be set by the publisher c Owned by the authors, published by EDP Sciences, 07 Measurements of the Vector boson production with the ALAS Detector
More informationP-P PHYSICS AT LHC. W and Z produc1on. Data and MC comparison. Lecture 4
P-P PHYSICS A LHC W and Z producon. Data and MC comparison Lecture 4 RIGGER URN ON rigger Efficiency 0.8 0.6 CMS preliminary, nb 8 67 y < 0.5 s = 7 ev 0 0.4 0. 0 MinBias Jet6u Jet5u Jet0u Anti-k R=0.5
More informationParticle spectra in Minimum Bias events at 13TeV
Particle spectra in Minimum Bias events at TeV Juan Manuel Grados Luyando on behalf of the CMS collaboration Deutsches Elektronen-Synchrotron, Hamburg MPI@LHC 05 Trieste, Italy Motivation Probe the different
More informationQCD at CDF. Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration
QCD at CDF Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration Jet Inclusive Cross-Section Underlying event studies Jet Shapes Specific processes _ W+Jets, γ + γ, γ + b/c, b-jet / bb jet Diffraction
More informationTop Quark Production at the LHC. Masato Aoki (Nagoya University, Japan) For the ATLAS, CMS Collaborations
Top Quark Production at the LHC Masato Aoki (Nagoya University, Japan) For the ATLAS, CMS Collaborations Phys. Rev. D 83 (2011) 091503, Phys. Rev. D 82 (2010) 054018, Phys. Rev. D 81 (2010) 054028, Comput.
More informationPoS(LeptonPhoton2015)020
Soft QCD Measurements at LHC Status and Outlook CERN E-mail: jgrosseo@cern.ch he first run of the LHC (009 0) has resulted in a tremendous legacy of soft physics results measured by ALICE, ALAS, CMS, LHCb,
More informationQuarkonia and heavy-quark production in proton and nuclear collisions at the LHC
Quarkonia and heavy-quark production in proton and nuclear collisions at the LHC Michael Schmelling / MPI for Nuclear Physics Introduction Double Parton Scattering Cold Nuclear Matter Effects Quark Gluon
More informationMeasurement of the charged particle density with the ATLAS detector: First data at vs = 0.9, 2.36 and 7 TeV Kayl, M.S.
UvA-DARE (Digital Academic Repository) Measurement of the charged particle density with the ALAS detector: First data at vs = 0.9,.36 and 7 ev Kayl, M.S. Link to publication Citation for published version
More informationExploring Jet Properties in p+p Collisions at 200 GeV with STAR
Exploring Jet Properties in p+p Collisions at 200 GeV with SAR Helen Caines - Yale University - for the SAR Collaboration Outline Quark Matter 2009 Knoxville,N, USA March 30 th -April 4 th What we know
More informationPoS(ICHEP2012)194. Measurements of the t t forward-backward asymmetry at CDF. Christopher Hays
Measurements of the t t forward-backward asymmetry at CDF On behalf of the CDF Collaboration Oxford University E-mail: hays@physics.ox.ac.uk At next-to-leading order in QCD, the t t forward-backward asymmetry
More informationW/Z+jet results from the Tevatron
W/Z+jet results from the Tevatron Dmitry Bandurin Florida State University On behalf of D0 and CDF Collaborations Moriond QCD 2012, March 15, La Thuile, Italy Precision QCD tests Photon, W, Z etc. p parton
More informationRecent forward physics and diffraction results from CMS
EPJ Web of Conferences will be set by the publisher DOI: will be set by the publisher c Owned by the authors, published by EDP Sciences, 6 Recent forward physics and diffraction results from Gábor Veres
More informationMeasurement of t-channel single top quark production in pp collisions
Measurement of t-channel single top quark production in pp collisions (on behalf of the CMS collaboration) INFN-Napoli & Università della Basilicata E-mail: Francesco.Fabozzi@cern.ch Measurements of t-channel
More informationMinimum Bias and Underlying Event Studies at CDF
FERMILAB-CONF--531-E Minimum Bias and Underlying Event Studies at CDF INFN, Bologna E-mail: moggi@bo.infn.it Soft, non-perturbative, interactions are poorly understood from the theoretical point of view
More informationEarly physics with Atlas at LHC
Early physics with Atlas at LHC Bellisario Esposito (INFN-Frascati) On behalf of the Atlas Collaboration Outline Atlas Experiment Physics goals Next LHC run conditions Physics processes observable with
More informationMeasurement of EW production! of Z+2j at the LHC
Measurement of EW production! of Z+j at the LHC Frontiers of Fundamental Physics, Marseille Kiran Joshi On behalf the ATLAS and CMS collaborations /7/ Overview Introduction and motivation ATLAS measurement
More informationarxiv: v1 [hep-ex] 12 Sep 2014
op Quark Measurements in CMS Efe Yazgan a, a Department of Physics and Astronomy, Ghent University, Proeftuinstraat 86 B-9 Gent, Belgium. arxiv:9.3737v [hep-ex] Sep Abstract Measurements involving top
More informationRecent CMS results in the forward region with the CASTOR detector. Sebastian Baur for the CMS Collaboration
Recent CMS results in the forward region with the CASTOR detector Sebastian Baur for the CMS Collaboration The Forward Instrumentation of CMS 2 Overview CMS has an excellent calorimetric instrumentation
More informationPhysics at Hadron Colliders
Physics at Hadron Colliders Part 2 Standard Model Physics Test of Quantum Chromodynamics - Jet production - W/Z production - Production of Top quarks Precision measurements -W mass - Top-quark mass QCD
More informationStandard Model Tests at the LHC. A. Salzburger, CERN on behalf of the ATLAS and CMS collaborations
Standard Model ests at the LHC A. Salzburger, CERN on behalf of the ALAS and CMS collaborations main Run- dataset 900 GeV.76 ev 7 ev LHC Run- and Run- Run- has started 8 ev 009 3 ev 0 0 0 05 LHC - he main
More informationDistinguishing quark and gluon jets at the LHC
Distinguishing quark and jets at the LHC Giorgia Rauco (on behalf of the ALAS and CMS Collaborations) Universität Zürich, Zürich, Switzerland Abstract: Studies focused on discriminating between jets originating
More informationLatest results on the SM Higgs boson in the WW decay channel using the ATLAS detector
Latest results on the SM iggs boson in the decay channel using the detector arxiv:188.954, accepted by PRB Claudia Bertella, on behalf of Collaboration The 4th China LC Physics Workshop (CLCP 218) 21-December-218
More informationMoriond QCD. Latest Jets Results from the LHC. Klaus Rabbertz, KIT. Proton Structure (PDF) Proton Structure (PDF) Klaus Rabbertz
Latest Jets Results from the LHC Proton Structure (PDF) Proton Structure (PDF), KIT 1 Flash Menu Motivation Accelerators and Detectors Jet Algorithms and Calibration Inclusive Jets Dijets and 3-Jets The
More informationInclusive top pair production at Tevatron and LHC in electron/muon final states
Inclusive top pair production at Tevatron and LHC in electron/muon final states Andreas Jung for the ATLAS, CDF, CMS and D Collaboration Fermilab, DAB5 - MS 357, P.O. Box 5, Batavia, IL, 651, USA DOI:
More informationQCD Jets at the LHC. Leonard Apanasevich University of Illinois at Chicago. on behalf of the ATLAS and CMS collaborations
QCD Jets at the LHC Leonard Apanasevich University of Illinois at Chicago on behalf of the ATLAS and CMS collaborations Outline Physics at the LHC Jet Reconstruction and Performance Clustering Algorithms
More information51 st Cracow School of Theoretical Physics The Soft Side of the LHC Min-Bias and the Underlying Event at the LHC Rick Field University of Florida
5 st Cracow School of Theoretical Physics The Soft Side of the LHC Min-Bias and the Underlying Event at the LHC Rick Field University of Florida Lecture : Outline Review: The CDF Tevatron underlying event
More informationMeasurement of W and Z boson cross sections in pp collisions at 7 TeV with the ATLAS detector
Measurement of W and Z boson cross sections in pp collisions at 7 ev with the ALAS detector Ryan Reece University of Pennsylvania On behalf of the ALAS Collaboration [1] photo: naotakem he International
More informationMultiple Parton-Parton Interactions: from pp to A-A
Multiple Parton-Parton Interactions: from pp to A-A Andreas Morsch CERN QCD Challenges at LHC Taxco, Mexico, Jan 18-22 (2016) Multiple Parton-Parton Interactions Phys. Lett. B 167 (1986) 476 Q i 2 Λ QCD
More informationToward an Understanding of Hadron-Hadron. Collisions From Feynman-Field to the LHC
Toward an Understanding of Hadron-Hadron Collisions From Feynman-Field to the LHC Rick Field University of Florida Outline of Talk The old days of Feynman-Field Phenomenology. XXIèmes Rencontres de Blois
More informationRecent Results on Jet Physics and α s
Recent Results on Jet Physics and α s XXI Physics in Collision Conference Seoul, Korea June 8, Presented by Michael Strauss The University of Oklahoma Outline Introduction and Experimental Considerations
More informationMeasurement of distributions sensitive to the underlying event in inclusive Z-boson production in pp collisions at s = 7TeV with the ATLAS detector
Eur. Phys. J. C (204) 74:395 DOI.40/epjc/s052-0495-6 Regular Article - Experimental Physics Measurement of distributions sensitive to the underlying event in inclusive -boson production in pp collisions
More informationDIBOSON PRODUCTION AT LHC AND TEVATRON
November 6, 3 3: WSPC/INSRUCION FILE PIC Jian International Journal of Modern Physics: Conference Series c World Scientific Publishing Company DIBOSON PRODUCION A LHC AND EVARON JIAN WANG on behalf of
More informationUnderlying Event Studies Using Calorimeter Jets with the ATLAS Detector at LHC
Underlying Event Studies Using Calorimeter Jets with the ALAS Detector at LHC Sebastian Wahrmund supervised by Deepak Kar, Arno Straessner DPG Frühjahrstagung Karlsruhe Introduction Motivation 2 / 2 Introduction
More informationP-P PHYSICS AT LHC. Minimum Bias events. W/Z Produc1on. Lecture 3
P-P PHYSICS A LHC Minimum Bias events. W/Z Producon Lecture MINIMUM BIAS EVENS rigger requirements bias the type of events towards interesting hard scattering processes single high pt lepton high pt leptons
More informationSoft interactions in Herwig
Soft interactions in Herwig Stefan Gieseke Institut für Theoretische Physik KIT work with Patrick Kirchgaeßer and Frashër Loshaj MPI@LHC6 San Cristóbal de las Casas 28 Nov 2 Dec 206 Stefan Gieseke MPI@LHC
More informationJet and photon production and
Jet and photon production and extraction of at HERA Radek Žlebčík1 On behalf of H1 and ZEUS collaborations 1 Deutsches Elektronen-Synchrotron (DESY) New Frontiers in Physics Kolymbari, August 24 HERA Collider
More informationMeasurements of the vector boson production with the ATLAS detector
Measurements of the vector boson production with the ATLAS detector A. Lapertosa 1,2,, on behalf of the ATLAS Collaboration 1 Università degli Studi di Genova 2 INFN Sezione di Genova Abstract. Measurements
More information