Particle Identification of the LHCb detector
|
|
- Winifred Robbins
- 6 years ago
- Views:
Transcription
1 HCP 2005 Particle Identification of the LHCb detector on behalf of the LHCb collaboration CERN 5th July 2005
2 The LHCb experiment : introduction precision measurements of CP violation and rare phenomena in B meson decays Standard Model consistency?, new physics? Experimental requirements: Efficient trigger (see talk by Mitesh Patel) Vertex identification High track reconstruction efficiency pp interaction (primary vertex) b-hadron B 0 L l π + π Κ π + π + Control of systematics Particle identification 1. π/k separation RICH 2. lepton id muon + calo
3 RICH detectors for hadron identification RICH1 Z ~ m aerogel:2 ~10 GeV/c C 4 F 10 :10 ~60 GeV/c RICH2 Z ~ m CF 4 :16 ~100GeV/c pp interaction point Magnet efficient pion/kaon separation up to ~100 Gev/c
4 Lepton identification : muons and electrons B J/ψ K s access to angle β Rare decays B μμ e h HCAL μfe + scintillator tiles 1468 cells, MWPC s 5.6 λ Ι σ/e ~ 75% / E + GEMs Info used in 1 st level trigger ECAL Shashlik type 66layers 2mm Pb/4mm scintillator 25 X o σ/e ~ 10%/ E
5 RICH detector requirements Goal: π/k separation in ~ 1-100GeV/c range 400 Polar angle versus momentum Number of tracks 300 (a) (b) B ππ decay tagging kaons θ [mrad] RICH1 RICH mrad RICH2 B d0 ππ RICH mrad Momentum (GeV/c) Momentum [GeV/c ]
6 RICH detector specifications RICH system divided into 2 detectors with 3 radiators θ C (mrad) e μ π K π p Aerogel Aerogel C 4 F 10 gas CF 4 gas Momentum (GeV/c) K C4F10 CF4 θ C max 242 mrad R I C H 1 RICH2 53 mrad 32 mrad
7 RICH1: low momentum tracks Magnetic shielding Photon Detectors Aerogel Thickness 5 cm n = ± Aerogel C 4 F mrad Spherical Mirror Beam pipe Aerogel Support Structure VELO exit window Track Be Mirrors y Plane Mirror z (cm)
8 RICH2: high momentum tracks (CF4) x z Photon Detectors plane
9 56 spherical mirrors on two planes -> installed and aligned with precision σθ 50 μrad
10 Photon Detectors Requirements: 2.5x2.5 mm 2 granularity => σ(θ CH ) = 0.6 mrad (RICH1) Coverage of 2.6 m 2 Single photon sensitive λ nm Read-out speed 40 MHz B B Hybrid Photon Detector (HPD) S20 multi-alkali photocathode Cross-focusing electron optics (~20kV, demagnification factor of 5) Photo-electrons focused on anode assembly (16x16 mm2), fully encapsulated in the vacuum enclosure 83mm Mu-metal shielding 120mm 140mm
11 Mumetal shield 20G Simulated B field distribution in RICH1 B B 0G B 30 G Calibration pattern 0 G B 50 G B field in shielding boxes measured! Most important effects from axial fields RICH1 Effect = PARAMETRISABLE in situ calibration pattern runs, Study effect in physics data
12 RICH simulation and pattern recognition Simulation in Geant4 RICH1 RICH1 B->Kpi events RICH2 get rings out multitude of hits!
13 RICH simulation and pattern recognition RICH1 RICH2 Aerogel C 4 F 10 CF 4 L (cm) n N pe σ totθ (mrad) RICH Pattern recognition approaches: Track based (local/global) Other algorithms (ring fitting) Difference in log-likelihood under different hypotheses significance of π/k separation for true pions Chromatic Emission Point Pixel Size σ totθ (mrad) RICH +Tracks
14 RICH hadron ID performance Heavy PID Light PID Kaon identification eff ~88% K K,p Kaon misidentification ~12% K e,μ,π pion identification ~ 97% π e,μ,π pion misidentification ~ 3% π K,p
15 RICH hadron ID performance: B s -> D s K Time dependant asymmetries in B s -> D s K with CP asymmetry in B 0 S -> J/ψ φ γ with σ(γ) = 15 0 per year Very little theoretical uncertainties Insensitive to new physics ~ 5400 evts per year expected BUT! Entries m Bs = 5.37 GeV/c 2 σ Bs = 13.8 MeV/c 2 D s K D s π m Bs = 5.42 GeV/c 2 σ Bs = 24.0 MeV/c Bs Ds π Bs Ds K ΔlnL Kπ mass [GeV/c 0 B s contamination ~ 90% 2 ]
16 RICH hadron ID performance: B (s) -> h + h - B-> ππ α measurement precision per year Combination of B-> ππ and B -> KK -> γ measurement precision 5 0 per year -> sensitive to new physics Yields: 26k B 0 π+π and 37k B s -> KK B 0 π + π - Tree diagram B 0 (B 0 ) s b B s K + K - d(s) W Penguin diagram (example) b d(s) W t c u g d(s) u u d(s) d(s) u u d(s) π + (K + ) π (K ) π + (K + ) π (K ) With RICH Purity=84%, ε=79% No RICH Purity=13%
17 Muon identification Search of hits in muon stations compatible with reconstructed track extrapolations B J/ψ K s ; p > 3 GeV/c μ eff 96.5% π eff 2.1% σ Μ 10 MeV Further reduction of bkg with other algorithms and multivariable analysis =>μ eff ~ 90%, π eff 0.8% Provide global PID with DLL
18 Electron identification Difference in log likelihood for (DLL): signal (e) and bkg hypothesis based on 4 variables Corrected cluster energy position matching e+/e h/μ Energy deposition in preshower χ 2 e e+/eh/μ Bremsstrahlung correction e+/eh/μ e+/eh/μ E PS (MeV) Energy deposition along extrapolated track in HCAL χ 2 brem E HCAL (GeV)
19 Electron identification performance B 0 -> J/ψ K 0 S J/ψ -> e+ e - within calorimeter acceptance: Eff 95% Eff 81% π misid 0.7% Combined with RICH B S -> J/ψ φ J/ψ -> e + e - Tail from Bremsstrahlung Bkg rejected with p T cut, mainly coming from secondary electrons and ghosts Performance e eff 78%, π misid 1%
20 Conclusions Particle identification is essential for the LHCb physics program! Hadron identifcation 3σ π-k separation from GeV/c provided by 2 RICH detectors RICH2 construction almost complete, RICH1 construction underway photon detector understood and being produced Installation expected to be completed by October 2006 Electron identification ECAL installed, HCAL underway Muon identification Muon project well advanced (480 chambers produced = 1/3 of the total) Combined PID improves performance
21 Dipole Magnet Installation progress in point 8 ECAL ½ HCAL Muon filters RICH1 magnetic shielding Eager for first collisions in 2007!
Status of the LHCb RICH and hadron particle identification
Status of the LHCb RICH and hadron particle identification M. Adinolfi University of Oxford On behalf of the LHCb collaboration (with many thanks to all the people whose presentations have been n hacked)
More informationEarly physics with the LHCb detector
XXVIII PHYSICS IN COLLISION - Perugia, Italy, June, 25-28, 2008 Early physics with the LHCb detector Dirk Wiedner CERN for the LHCb collaboration 27 June 2008 Dirk Wiedner at PIC2008 Perugia 1 Outline
More informationLHCb: Reoptimized Detector & Tracking Performance
LHCb: Reoptimized Detector & Tracking Performance Gerhard Raven NIKHEF and VU, Amsterdam Representing the LHCb collaboration Beauty 2003, Carnegie Mellon University, Oct 14-18, Pittsburgh, PA, USA 1 The
More informationObservation of the rare B 0 s µ + µ decay
Observation of the rare B 0 s µ + µ decay The combined analysis of CMS and LHCb data Luke Pritchett April 22, 2016 Table of Contents Theory and Overview Detectors Event selection Analysis Flavor physics
More informationRICH detectors for LHCb
RICH detectors for LHCb Tito Bellunato INFN Milano-Bicocca On behalf of the LHCb RICH collaboration 10th International Conference on Instrumentation for Colliding Beam Physics 10th International Conference
More informationStatus of the LHCb RICH detector and the HPD
Beauty 2005 Status of the LHCb RICH detector and the HPD Tito Bellunato Università degli Studi di Milano Bicocca & INFN On behalf of the LHCb RICH group Assisi 23 June Assisi 2005 23 June Tito Bellunato
More informationThe LHCb detector. Eddy Jans (Nikhef) on behalf of the LHCb collaboration
The LHCb detector Eddy Jans (Nikhef) on behalf of the LHCb collaboration design of sub-detectors, trigger and DAQ performance: resolutions and PID-properties commissioning with cosmics and beam induced
More informationb Physics Prospects For The LHCb Experiment Thomas Ruf for the LHCb Collaboration Introduction Detector Status Physics Program
b Physics Prospects For The LHCb Experiment Thomas Ruf for the LHCb Collaboration Introduction Detector Status Physics Program b Primary goal of the LHCb Experiment Search for New Physics contributions
More informationStatus of the LHCb Experiment. Ueli Strauman, University of Zurich, Switzerland. Sept. 13, 2001
Status of the LHCb Experiment Ueli Strauman, University of Zurich, Switzerland. Sept. 13, 2001 1 P b b P Number of pp inelastic interactions in one bunch crossing (σ inelastic = 80 mb): b b correlation
More informationThe LHCb Experiment II Detector XXXIV SLAC Summer Institute, July, 2006
The LHCb Experiment II Detector XXXIV SLAC Summer Institute, 17-28 July, 2006 Tatsuya NAKADA CERN and Ecole Polytechnique Fédérale de Lausanne (EPFL) 1) Introduction Physics requirements for the detector
More information(Towards) First Physics with LHCb
(Towards) First Physics with LHCb Beam induced splash in LHCb Physics at LHC 2008 Split, Croatia, 29 Sep - 4 Oct 2008 Introduction Detector overview and performance Extracting physics from (very) first
More informationB-Physics Potential of ATLAS, CMS, LHCb and BTeV
B-Physics Potential of ATLAS, CMS, LHCb and BTeV Neville Harnew University of Oxford 8th International Symposium on Heavy Flavour Physics N.Harnew 29th July 1999 1 Outline Introduction The 2nd Generation
More informationLHCb Calorimetry Impact
LHCb Calorimetry Impact Preema Pais! On behalf of the LHCb Collaboration! Workshop on the physics of HL-LHC, and perspectives at HE-LHC! November 1, 2017! THE LHCb DETECTOR Calorimetry! Located ~12.5 m
More informationLHCb status. Marta Calvi. for the LHCb Collaboration. 103 rd LHCC meeting University Milano-Bicocca and INFN
LHCb status 103 rd LHCC meeting 22.09.2010 Marta Calvi University Milano-Bicocca and INFN for the LHCb Collaboration Data taking 3.2 pb -1 on tape eff ~91% Stable data taking, high efficiency in all systems,
More informationLHCb: From the detector to the first physics results
LHCb: From the detector to the first physics results Olivier Callot Laboratoire de l Accélérateur Linéaire, IN2P3/CNRS and Université Paris XI, Orsay, France On behalf of the LHCb collaboration In this
More informationReconstruction of. events in LHCb. Benjamin Carron
Reconstruction of B s J/ψ η, η c φ, J/ψ φ events in LHCb Benjamin Carron sanne Neuchâtel, March 3rd, 4 Swiss Physical Society 4 Physics Motivations Selection Procedure B s Channels analysis Selection Cuts
More informationFlavor Physics beyond the SM. FCNC Processes in the SM
Flavor Physics beyond the SM 48 FCNC Processes in the SM A SM ( B ΔF = ΔF = 1 W q W b b u, c, t q b u, c, t q 0 q B ) ~ ( V V 0 q ) tb tq g m 16π m t W A SM ( b q) = V V tb tq g 16π m m t W FCNC in SM
More informationThe LHCb Flavour Physics Experiment
The LHCb Flavour Physics Experiment University of Glasgow AGH, University of Science and Technology, Krakow, Poland, 4 March 2010 Outline Motivation LHC @ CERN @ Geneva The LHCb experiment The 2010 LHC(b)
More informationStatus of the LHCb experiment and minimum bias physics
Status of the LHCb experiment and minimum bias physics Sebastian Bachman Heidelberg University on behalf of the LHCb collaboration 6/19/2010 Sebastian Bachmann 1 Beauty and Charm at the LHC LHC is a factory
More informationBenjamin Carron Mai 3rd, 2004
Physics Motivations Reconstruction of B s J/ψ η Benjamin Carron Mai 3rd, 4 B s J/ψ (µ + µ ) η (γγ) and B s J/ψ (e + e ) η (γγ) Selection Cuts Resolutions BR of the η B/S Ratios Annual Signal Yields and
More informationD 0 -D 0 mixing and CP violation at LHC
D -D mixing and CP violation at LHC Patrick Spradlin on behalf of the LHCb collaboration University of O Particle P 5 th International Workshop on the CKM Unitarity Triangle Rome, Italy 9-13 September
More informationSearch for New Physics with b sll LHCb
Search for New Physics with b sll decays @ LHCb Simone Bifani University of Birmingham (UK) On behalf of the LHCb Collaboration CERN Seminar, 18th April 17 A Forward Spectrometer Optimized for beauty and
More informationMeasurement of the baryon number transport with LHCb
Measurement of the baryon number transport with LHCb Marco Adinolfi University of Bristol On behalf of the LHCb Collaboration 13 April 2011 / DIS 2011 Marco Adinolfi DIS 2011-13 April 2011 - Newport News
More informationFirst 5 observation of CP violation in the decays of B0. B s at LHCb. Maria Zangoli Per la collaborazione LHCb
First 5 observation of CP violation in the decays of 0 B s at LHCb Maria Zangoli Per la collaborazione LHCb XCIX Congresso Nazionale SIF Trieste 25 settembre 2013 Maria Zangoli First 5 observation of CP
More informationStatus and expectations for first physics with LHCb. M. Needham On behalf of the LHCb collaboration Symmetries and Spin July 20 th - 26 th Prague
Status and expectations for first physics with LHCb M. Needham On behalf of the LHCb collaboration Symmetries and Spin July 20 th - 26 th Prague Outline Introduction to LHCb Tour of the detector First
More informationR. Mureşan. University of Oxford On behalf of LHCb Collaboration. Prepared for the CERN Theory Institute "Flavour as a Window to New Physics at LHC"
May 8 CERN Theory Institute Charm Physics at LHCb R. Mureşan University of Oxford On behalf of LHCb Collaboration Prepared for the CERN Theory Institute "Flavour as a Window to New Physics at LHC" R. Mureşan
More informationStatus and prospects of the LHCb experiment
Status and prospects of the LHCb experiment Overview Spectrometer Vertex Detector RICH Physics Program Trigger Strategy Status and Outlook U. Straumann, Uni Zuerich Geneva, 13. April 2005 pt vs for detected
More informationParticle identification at LHC: Alice and LHCb
F. Machefert To cite this version: F. Machefert. Particle identification at LHC: Alice and LHCb. R. Fleischer, N. Harnew, V. Vagnoni. 14th International Conference on B-Physics at Hadron Machines (Beauty
More informationKaon Identification at NA62. Institute of Physics Particle, Astroparticle, and Nuclear Physics groups Conference 2015
Kaon Identification at NA62 Institute of Physics Particle, Astroparticle, and Nuclear Physics groups Conference 2015 Francis Newson April 2015 Kaon Identification at NA62 K πνν NA48 and NA62 K + π + νν
More informationResults from HARP. Malcolm Ellis On behalf of the HARP collaboration DPF Meeting Riverside, August 2004
Results from HARP Malcolm Ellis On behalf of the HARP collaboration DPF Meeting Riverside, August 2004 The HAdRon Production Experiment 124 physicists 24 institutes2 Physics Goals Input for precise calculation
More informationHadronic vs e + e - colliders
Hadronic vs e + e - colliders Hadronic machines: enormous production of b-hadrons (σ bb ~ 50 µb) all b-hadrons can be produced trigger is challenging complicated many-particles events incoherent production
More informationSearch for K + π + νν decay at NA62 experiment. Viacheslav Duk, University of Birmingham for the NA62 collaboration
Search for K + π + νν decay at NA62 experiment Viacheslav Duk, University of Birmingham for the NA62 collaboration Durham, 04-06.09.2017 1 Outlook 1. Motivation 2. NA62 experiment 3. Event selection 4.
More informationNA62: Ultra-Rare Kaon Decays
NA62: Ultra-Rare Kaon Decays Phil Rubin George Mason University For the NA62 Collaboration November 10, 2011 The primary goal of the experiment is to reconstruct more than 100 K + π + ν ν events, over
More informationV0 cross-section measurement at LHCb. RIVET analysis module for Z boson decay to di-electron
V0 cross-section measurement at LHCb. RIVET analysis module for Z boson decay to di-electron Outline of the presentation: 1. Introduction to LHCb physics and LHCb detector 2. RIVET plug-in for Z e+e- channel
More informationStatus of LHCb and Physics Prospects
Status of LHCb and Physics Prospects Beam induced splash in LHCb HEP-MAD 09 Antananarivo, 22 August 2009 Physics motivation Detector overview and performance Physics prospects presented by Andreas Schopper
More informationPoS(QFTHEP2011)002. Recent results from LHCb. Yu. Guz IHEP, Protvino, Russia
IHEP, Protvino, Russia E-mail: Iouri.Gouz@cern.ch The LHCb detector at LHC is designed for searches of New Physics in CP violation and rare decays. Since the LHC startup, LHCb accumulated a large sample
More informationLavinia-Elena Giubega
Lavinia-Elena Giubega *on behalf of LHCb collaboration Horia Hulubei National Institute for Physics and Nuclear Engineering (IFIN-HH), Bucharest, Romania Beach 2018 - XIII International Conference on Beauty,
More informationMuon reconstruction performance in ATLAS at Run-2
2 Muon reconstruction performance in ATLAS at Run-2 Hannah Herde on behalf of the ATLAS Collaboration Brandeis University (US) E-mail: hannah.herde@cern.ch ATL-PHYS-PROC-205-2 5 October 205 The ATLAS muon
More informationResults and Prospects for Ion Physics at LHCb
Discovery Physics at the LHC Kruger 2016 Results and Prospects for Ion Physics at LHCb Patrick Robbe, LAL Orsay, 7 December 2016, For the LHCb Collaboration Outline The LHCb experiment Results in ppb and
More informationOverview of LHCb Experiment
Overview of Physics @ LHCb Experiment Yuanning Gao, Tsinghua University Representing the LHCb Collaboration Detector performance CKM triangles Other topics (selected) Conclusions A very selective review!
More informationLHCb Status and Physics
LHCb Status and Physics Tatsuya Nakada CERN and EPFL SUSY in 2010 s 20-22.06.07, Sapporo 1 1) Introduction Contents 2) LHC(b) Experiments 3) Physics with 2008 data 4) Flavour Physics >2008 also ATLAS/CMS
More informationPoS(KAON)049. Testing the µ e universality with K ± l ± ν decays
University of Sofia "St. Kl. Ohridski" E-mail: Venelin.Kozhuharov@cern.ch The ratio R K = Γ(K ± e ± ν)/γ(k ± µ ± ν) provides a very powerful probe for the weak interactions structure. This ratio of decay
More informationMeasurements of R K and R K* at LHCb
Measurements of R K and R K* at LHCb Marie-Hélène Schune Laboratoire de l Accélérateur Linéaire, Orsay On behalf of the LHCb Collaboration B K* (K π) e + e - candidate Instant Workshop on B meson anomalies,may
More informationTests of the BURLE 64-anode MCP PMT as the detector of Cherenkov photons
Tests of the BURLE 64-anode MCP PMT as the detector of Cherenkov photons Peter Križan University of Ljubljana and J. Stefan Institute Contents Motivation and requirements BURLE MCP-PMT Beam test results
More informationNew Limits on Heavy Neutrino from NA62
CERN E-mail: michal.koval@cern.ch The NA6 experiment at CERN collected large samples of charged kaon decays in flight with a minimum bias trigger configuration in 7 and in 15 using a completely new detector
More informationAtlas Status and Perspectives
Atlas Status and Perspectives Bruno Mansoulié (IRFU-Saclay) On behalf of the Topics The hot news: Heavy Ion analysis Data taking in 2010 Luminosity, Data taking & quality, trigger Detector performance
More informationB 0 s physics at LHCb
PRAMANA c Indian Academy of Sciences Vol. 63, No. 6 journal of December 2004 physics pp. 1135 1150 B 0 s physics at LHCb R W FORTY, for the LHCb Collaboration CERN, CH-1211, Geneva 23, Switzerland E-mail:
More informationFrederic Teubert CERN, EP Department
* Frederic Teubert CERN, EP Department With my gratitude to the speakers at the LHCb Future Upgrades Meeting in Manchester (6-7) April: Theatre of Dreams: Beyond the LHCb Phase-I upgrade 1 On behalf of
More informationAn Overview of RICH Detectors From PID to Velocity Spectrometers
An RICH Detectors From PID to Velocity Spectrometers, January 29, 2008 Goal - a broad overview for this afternoon s session I. Introduction II. Recent RICH history. A review of some experiments and their
More informationCMS Conference Report
Available on CMS information server CMS CR 2001/004 CMS Conference Report April 13, 2001 Prospects of B-Physics with CMS a) Sunanda Banerjee 1) Abstract Prospects of studies of properties of b flavoured
More informationRelative branching ratio measurements of charmless B ± decays to three hadrons
LHCb-CONF-011-059 November 10, 011 Relative branching ratio measurements of charmless B ± decays to three hadrons The LHCb Collaboration 1 LHCb-CONF-011-059 10/11/011 Abstract With an integrated luminosity
More informationPhysics Motivation The Vertex Locator The Outer Tracker Tracking in HERA-B and LHCb LHCb Optimization
b-physics: HERA-B and LHCb Marcel Merk (for Jo van den Brand) April 8, 22 Physics Motivation The Vertex Locator The Outer Tracker Tracking in HERA-B and LHCb LHCb Optimization b b Physics What does LHCb
More informationLepton Number and Lepton Flavour Violation
Lepton Number and Lepton Flavour Violation Search for Majorana neutrinos in B-decays, lepton flavour violation in τ - µ - µ - µ + and baryon number violation with LHCb seen Paul Seifert's talk today LHCb
More informationRare decays of beauty mesons
Rare decays of beauty mesons on behalf of the LHCb collaboration - The LHCb experiment ECAL, HCAL Particle Id RICH system Muon chambers Interaction point Velo Tracking Tracking stations 2 / 25 B 0 (s)
More informationThe TORCH project. a proposed detector for precision time-of-flight over large areas. Roger Forty (CERN)
The TORCH project a proposed detector for precision time-of-flight over large areas Roger Forty (CERN) DIRC 2013, Giessen, 4 6 September 2013 Introduction TORCH (Time Of internally Reflected CHerenkov
More informationV 0 production studies at LHCb. Mathias Knecht, EPFL , joint SPS-ÖPG-ÖGA 2 meeting, Innsbrück, Österreich, September 2-4, 2009
V 0 production studies at LHCb Mathias Knecht, EPFL 2 9 2009, joint SPS-ÖPG-ÖGA 2 meeting, Innsbrück, Österreich, September 2-4, 2009 Outline One of the first measurements to be done with the LHCb detector...
More informationThe HERMES Dual-Radiator Ring Imaging Cerenkov Detector N.Akopov et al., Nucl. Instrum. Meth. A479 (2002) 511
The HERMES Dual-Radiator Ring Imaging Cerenkov Detector N.Akopov et al., Nucl. Instrum. Meth. A479 (2002) 511 Shibata Lab 11R50047 Jennifer Newsham YSEP student from Georgia Institute of Technology, Atlanta,
More informationLuminosity measurement and K-short production with first LHCb data. Sophie Redford University of Oxford for the LHCb collaboration
Luminosity measurement and K-short production with first LHCb data Sophie Redford University of Oxford for the LHCb collaboration 1 Introduction Measurement of the prompt Ks production Using data collected
More informationB. Hoeneisen. Universidad San Francisco de Quito Representing the DØ Collaboration Flavor Physics and CP violation (2013)
Status report on the like-sign dimuon charge asymmetry in p p collisions and Measurement of the direct CP asymmetry in B J/ψK and B J/ψπ decays B. Hoeneisen Universidad San Francisco de Quito Representing
More informationParticle ID in ILD. Masakazu Kurata, KEK Calorimeter Workshop IAS program 01/19/2018
Particle ID in ILD Masakazu Kurata, KEK Calorimeter Workshop IAS program 01/19/2018 1 Outline Introduction Requirement of the TPC for the ILD de/dx of ILD TPC Requirement of the Calorimeters for the ILD
More information3.1 The Large Hadron Collider
3 T H E L H C b E X P E R I M E N T 3.1 The Large Hadron Collider The Large Hadron Collider (LHC) is a particle collider based at CERN, accelerating two beams of hadrons, either protons or lead ions. It
More informationA search for heavy and long-lived staus in the LHCb detector at s = 7 and 8 TeV
A search for heavy and long-lived staus in the LHCb detector at s = 7 and 8 TeV Trần Minh Tâm minh-tam.tran@epfl.ch on behalf of the LHCb Collaboration LHCb-CONF-2014-001 EPFL, Laboratoire de Physique
More informationA. Oyanguren (IFIC U. Valencia/CSIC)
A. Oyanguren (IFIC U. Valencia/CSIC) Outline Radiative b decays B s φγ B 0 K *0 e + e - [PRL 118(2017)021801] [JHEP04(2015)064] b-baryons: Λ b Λγ, Ξ b Ξ γ, Ω b Ωγ Conclusions A. Oyanguren 2 The LHCb experiment
More informationThe HARP Experiment. G. Vidal-Sitjes (INFN-Ferrara) on behalf of the HARP Collaboration
The HARP Experiment (INFN-Ferrara) on behalf of the HARP Collaboration New Views in Particle Physics Outline Goals for a HAdRon Production experiment Example: KEK PS Neutrino beam-line Detector layout
More informationThe LHCb Upgrade. On behalf of the LHCb Collaboration. Tomasz Szumlak AGH-UST
The LHCb Upgrade Outline LHCb Detector Selected Physics Results Upgrade Plans Test beam campaign (just a flash) Summary On behalf of the LHCb Collaboration Tomasz Szumlak AGH-UST 1 XII International Conference
More informationAerogel RICH counter for the Belle II forward PID
Aerogel RICH counter for the Belle II forward PID a, I. Adachi b, N. Hamada c, M. Higuchi d, T. Iijima e, S. Iwata f, H. Kakuno f, H. Kawai g, S. Korpar ah, P. Križan ai, S. Nishida b, S. Ogawa c, R. Pestotnik
More informationJet reconstruction in LHCb searching for Higgs-like particles
Jet reconstruction in LHCb searching for Higgs-like particles Alessandro Camboni (on behalf of LHCb Collaboration) DISCRETE'08 Valencia Dec 12th, 2008 Motivation Jet reconstruction is important for searches
More informationSearch for B 0 s φφγ at LHCb
Master Project Search for B 0 s φφγ at LHCb Author: Violaine Bellee Supervised by: Prof. Karim Trabelsi Dr. Albert Puig Navarro February 12, 2015 Contents 1 Introduction 3 1.1 Theoretical context............................
More informationB-physics with ATLAS and CMS
Physics at LHC-2008 Split-CROATIA, 29.9. 4.10.2008 B-physics with ATLAS and CMS Brigitte Epp, Astro- and Particle Physics, University of Innsbruck, Austria representing ATLAS / CMS collaborations B-physics
More informationMixing and CP violation
Mixing and CP violation in the B s system with ATLAS Study from B s 0 J/ψ φ decay with and without flavour tagging Toyonobu OKUYAMA University of Tokyo On behalf of the ATLAS Collaboration PASCOS 2013
More informationElectron reconstruction and identification in CMS at LHC
Electron reconstruction and identification in CMS at LHC on behalf of CMS collaboration 1 Outline The CMS detector @ LHC Electron reconstruction components Performance Electron identification Measurements
More informationIntroduction. Tau leptons. SLHC. Summary. Muons. Scott S. Snyder Brookhaven National Laboratory ILC Physics and Detector workshop Snowmass, Aug 2005
Leptons and Photons at the (S)LHC Scott S. Snyder Brookhaven National Laboratory ILC Physics and Detector workshop Snowmass, Aug 2005 Outline: Introduction. e/γ. Muons. Tau leptons. SLHC. Summary. Leptons
More informationStatus and physics at LHCb
Vienna Seminar, Particle physics and the LHC, 26.11.11 Status and physics at LHCb, Jeroen van Tilburg 1/42 Status and physics at LHCb Vienna Central European Seminar Particle Physics and the LHC Jeroen
More informationTracking at the LHC. Pippa Wells, CERN
Tracking at the LHC Aims of central tracking at LHC Some basics influencing detector design Consequences for LHC tracker layout Measuring material before, during and after construction Pippa Wells, CERN
More informationRare Exclusive Decays. Results from BaBar on the. DPF-2002, College of William and Mary. University of California, Jeffrey Berryhill.
Results from BaBar on the Rare Exclusive Decays B K l + l and B K* l + l Jeffrey Berryhill University of California, Santa Barbara DPF2002, College of William and Mary May 24, 2002 B K (*) l + l in the
More informationPoS(HQL 2012)021. The LHCb upgrade. Tomasz Szumlak 1
The LHCb upgrade Tomasz Szumlak 1 AGH - University of Science and Technology al. Mickiewicza 30, 30-059 Kraków, Poland E-mail: szumlak@agh.edu.pl The LHCb experiment is designed to perform high-precision
More informationLHCb physics with the first pb 1
LHCb physics with the first 10-20 pb 1 Raluca Mureşan EPFL on behalf of the LHCb collaboration R. Mureşan, LHCb physics with the first 10-20 pb 1 p.1/30 Outline LHCb detector First data analysis and rapidity
More informationHARP (Hadron Production) Experiment at CERN
HARP (Hadron Production) Experiment at CERN 2nd Summer School On Particle Accelerators And Detectors 18-24 Sep 2006, Bodrum, Turkey Aysel Kayιş Topaksu Çukurova Üniversitesi, ADANA Outline The Physics
More informationMaster Project. June 19, Author : Aurélie Flandi. Supervised by: Dr. Karim Trabelsi Dr. Albert Puig Navarro
Master Project Search for Λ b Λ γ at LHCb June 19, 215 Author : Aurélie Flandi Supervised by: Dr. Karim Trabelsi Dr. Albert Puig Navarro Abstract The Λ b Λ γ decay plays an important role in the determination
More informationBrief Report from the Tevatron. 1 Introduction. Manfred Paulini Lawrence Berkeley National Laboratory Berkeley, California 94720
Brief Report from the Lawrence Berkeley National Laboratory Berkeley, California 9472 1 Introduction It might appear surprising to include a report from the Fermilab, a proton-antiproton collider, in a
More informationThe LHCb Upgrade and beyond
The LHCb Upgrade and beyond Tomasz Szumlak on behalf of the LHCb Collaboration AGH-University of Science and Technology XIII International Conference on Heavy Quarks and Leptons (HQL) 22/05 27/05/2016,Virginia
More informationHeavy Hadron Production and Spectroscopy at ATLAS
Heavy Hadron Production and Spectroscopy at ALAS Carlo Schiavi on behalf of the ALAS Collaboration INFN Sezione di Genova ALAS has studied heavy flavor production and measured the production cross sections
More informationRadiative penguins at hadron machines. Kevin Stenson! University of Colorado!
Radiative penguins at hadron machines Kevin Stenson! University of Colorado! Introduction γ + b q u,c,t W s q b q u,c,t W + s q b q ν W W + u,c,t s q!! Radiative penguins involve b to s,d transitions with
More informationRecent results from the LHCb experiment
Recent results from the LHCb experiment University of Cincinnati On behalf of the LHCb collaboration Brief intro to LHCb The Large Hadron Collider (LHC) proton-proton collisions NCTS Wksp. DM 2017, Shoufeng,
More informationObservation of the decay
Master Project Supervised by: Prof. Olivier Schneider Dr. Albert Puig Observation of the decay B + K + + γ at LHCb Master Project report, winter semester Isaure Leboucq isaure.leboucq@epfl.ch CONTENTS
More informationFuture prospects for the measurement of direct photons at the LHC
Future prospects for the measurement of direct photons at the LHC David Joffe on behalf of the and CMS Collaborations Southern Methodist University Department of Physics, 75275 Dallas, Texas, USA DOI:
More informationLikelihood Methods for Beam Particle Identification at the COMPASS Experiment
Likelihood Methods for Beam Particle Identification at the Experiment Tobias Weisrock for the Collaboration Graduate School Symmetry Breaking Johannes Gutenberg-Universität Mainz SPIN-Praha-22 July 7,22
More informationB the Tevatron
B Physics @ the Tevatron Stephanie Hansmann-Menzemer Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg DESY, 9 th of November 7 xxx p.1/1 Tevatron p p collisions at s = 1.96 TeV observed by
More informationValidation of Geant4 Physics Models Using Collision Data from the LHC
Journal of Physics: Conference Series Validation of Geant4 Physics Models Using Collision from the LHC To cite this article: S Banerjee and CMS Experiment 20 J. Phys.: Conf. Ser. 33 032003 Related content
More informationPerformance of muon and tau identification at ATLAS
ATL-PHYS-PROC-22-3 22/2/22 Performance of muon and tau identification at ATLAS On behalf of the ATLAS Collaboration University of Oregon E-mail: mansoora.shamim@cern.ch Charged leptons play an important
More informationCP Violation in the B(s) meson system at LHCb Julian Wishahi on behalf of the LHCb collaboration
CP Violation in the B(s) meson system at Julian Wishahi on behalf of the collaboration 5th Rencontres de Moriond, Electroweak Session, 2th of March 215 CPV in Interference of Mixing/Decay interference
More information7 Particle Identification. Detectors for Particle Physics Manfred Krammer Institute of High Energy Physics, Vienna, Austria
7 Particle Identification Detectors for Particle Physics Manfred Krammer Institute of High Energy Physics, Vienna, Austria 7.0 Content 7.1 Methods for Particle Identification 7.2 Mass of Charged Particles
More informationLepton Universality in ϒ(nS) Decays at CLEO
Hajime Muramatsu, University of Rochester BNM2008@ATAMI JAPAN JAN/2008 1 Lepton Universality in ϒ(nS) Decays at CLEO Hajime Muramatsu University of Rochester For the CLEO Collaboration Hajime Muramatsu,
More informationLFV in Tau Decays: Results and Prospects at the LHC. Tau th International Workshop on Tau Lepton Physics Beijing September 22th, 2016
LFV in Tau Decays: Results and Prospects at the LHC Kristof De Bruyn On behalf of the ATLAS, CMS & LHCb Collaborations Tau 216 14th International Workshop on Tau Lepton Physics Beijing September 22th,
More informationclfv & BNV LHCb Gerco Onderwater on behalf of the LHCb collaboration
clfv & BNV Searches @ LHCb Gerco Onderwater on behalf of the LHCb collaboration Flavour2017, Qui Nhơn, Việt Nam, 13-19 August 2017 2 34 Outline LHCb Experiment LFV with muons : τ LFV with electrons : D0
More informationLatest time-dependent CP-violation results from BaBar
Latest time-dependent CP-violation results from BaBar Owen Long, UC Santa Barbara TM All results are preliminary XXXVIIth Rencontres de Moriond QCD and Hadronic Interactions March 17, 2002 The CKM matrix
More informationEarly flavor physics at the LHC
Early flavor physics at the LHC Walter M. Bonivento sezione di Cagliari on behalf of the ATLAS, CMS and LHCb collaborations Thanks to: M.Smizanska (ATLAS), Urs Langenegger (CMS) and LHCb colleagues The
More informationTrack measurement in the high multiplicity environment at the CBM Experiment
Track measurement in the high multiplicity environment at the CBM Experiment Pradeep Ghosh 1,, for the CBM Collaboration 1 Goethe University, Max-von-Laue-Straße 1, D-60438 Frankfurt am Main GSI Helmholtz
More informationRadiative decays: The photon polarization in b s γ penguin transitions
Radiative decays: The photon polarization in b s γ penguin transitions from Bs φγ at LHCb Mostafa HOBALLAH 1 Introduction Quarks form 3 isospin doublets: The CKM matrix: It gives us the strength of the
More informationThe LHC Heavy Flavour Programme
The LHC Heavy Flavour Programme Tatsuya Nakada CERN and EPFL LHC Flavour Workshop 26-28.03.07, CERN 1 Contents 1) Introduction 2) LHC Experiments 3) Physics with 2008 data 4) Flavour Physics >2008 5) Conclusions
More information