Review of relevant Cherenkov imaging i devices in particle/nuclear experiments currently running, under construction and planned
|
|
|
- Beverly Gilmore
- 5 years ago
- Views:
Transcription
1 Review of relevant Cherenkov imaging i devices in particle/nuclear experiments currently running, under construction and planned David Websdale Imperial College London 6th International Workshop on Ring Imaging Cherenkov Counters (RICH2007) Stazione Marittima, Trieste, Italy October 2007 D.Websdale, RICH2007, Trieste, Italy 1
2 Outline of this talk Review of relevant Cherenkov imaging devices in particle/nuclear experiments currently running, under construction and planned What is included? Detectors of focused Cherenkov radiation in accelerator/collider experiments Why is the RICH needed? Physics motivation How is the RICH detector used? highlighting specific features of current/planned experimental devices Review Preview a pointer to contributed papers presented here Apologies for omissions does not mean irrelevant! Acknowledgements to experiment websites for presentation material D.Websdale, RICH2007, Trieste, Italy 2
3 Outline of this talk What? Types of RICH detector in use/proposed Image focused by lens/mirror Classic RICH detector (Seguinot, Ypsilantis) Proximity focusing thin solid/liquid radiator Pin-hole focusing DIRC (Detector of Internally Reflected Cherenkov light) Imaging using timing Water Cherenkov TOP time of propagation D.Websdale, RICH2007, Trieste, Italy 3
4 Why are RICH detectors used? Physics motivation Reported at RICH2007 Flavour physics and CP violation LHCb, BELLE, BABAR, NA62 Hadron ID: to identify quark flavours in decays Hadron (low p T ) physics PANDA, MIPP, COMPASS Hadron ID: to identify final states, particle production, spectroscopy Nucleon structure COMPASS, HERMES Hadron ID: charmed hadrons as probe of gluons in nucleons Heavy Ion physics and QGP ALICE, JLAB, CBM, PHENIX Electron ID: nuclear matter transparent to leptons so probe interior Neutrino physics Event reconstruction for oscillation studies T2K (MIPP) D.Websdale, RICH2007, Trieste, Italy 4
5 Flavour physics BABAR DIRC _ Babar detector at PEPII electron-positron collider bb factory CP violation in decay of B u,d mesons DIRC Cherenkov D.Websdale, RICH2007, Trieste, Italy 5
6 Flavour physics BABAR DIRC 11,000 PMTs: 29mm diameter π / K separation: GeV/c N_photons detected > 30 / track σ θ <10 mrad x 6 reduction in D 0 Kπ background D.Websdale, RICH2007, Trieste, Italy 6
7 Flavour physics BABAR DIRC DIRC (SuperB) Upgrade to handle x 100 luminosity Focusing DIRC Reduced photon detector pixel size ~ 5mm Improved timing i resolution (e.g. MCP) ~100ps Determine colour of photon and correct chromatic error on θ C See talk by: JS J.Schwiening i D.Websdale, RICH2007, Trieste, Italy 7
8 Flavour physics BELLE upgrade _ BELLE detector at KEK electron-positron collider bb factory CP violation in decay of B u,d mesons Currently uses aerogel threshold Upgrade proposed for super B factory x 100 luminosity π / K separation: GeV/c Focusing / Time of Propagation (TOP) DIRC D.Websdale, RICH2007, Trieste, Italy 8 Proximity focusing aerogel RICH
9 Flavour physics BELLE upgrade TOP barrel DIRC: MultichannelPlate PMTs with time resolution ~ 40ps End Cap proximity focused aerogel 20mm-thick Aerogel tiles to limit emission-point error FlatPanel (H8500) PMTs σ θ ~ 14 mrad N_detected photons ~ 6 Increase N_ph by using graded-n aerogel tiles (FARICH) Degraded Angle precision Angular Precision of single tile See talks by: K.Inami T.Iijima E.Kravchenko PKrizan P.Krizan S.Nishida D.Websdale, RICH2007, Trieste, Italy 9
10 Flavour physics CLEOc Beauty and Charm physics at CESR electron-positron collider Proximity focused LiF RICH 12mm π/k separation up to 3 GeV/c CH 4 -TEA gas photo detector t 20m 2 (biggest out there) 230k pixels: 8mm x 8mm N_detected photons ~ 12 σ θ ~ 14 mrad D.Websdale, RICH2007, Trieste, Italy 20cm 10
11 Flavour physics HERA-B Beauty and Charm physics with fixed target at HERA proton ring Classic C4F10 gas RICH 5 yrs stable good performance Pioneered use of MultiAnode PMTs Hamamatsu M4, M16 equipped with lenses D.Websdale, RICH2007, Trieste, Italy 11 N_detected photons ~ 30 σ θ ~ 1 mrad
12 Flavour physics LHCb See talks by: N.Harnew C.D Ambrosio S.Eisenhardt S.Brisbane C.Buszello T.Bellunato A.Papanestis F.Metlica M.Sannino D.Wiedner FM F.Muheim D.Websdale, RICH2007, Trieste, Italy 12
13 Flavour physics LHCb Hadron ID from 1-100GeV/c 3 radiators: Aerogel, C 4 F 10, CF HPDs: 2.8m 2 with 2.5 x 2.5mm 2 pixels Allows rare B-decay to be cleanly identified D.Websdale, RICH2007, Trieste, Italy 13
14 Hybrid Photon Detectors in LHCb RICH LHCb has pioneered use of HPD (DEP-Photonis) 1000 pixels per tube: readout chip bump-bonded to sensor and encapsulated in vacuum tube D.Websdale, RICH2007, Trieste, Italy 14
15 Flavour physics NA62 at CERN Measure K + π + ν ν K + μ + ν background: branching fraction to extract V td SMprediction:08x See talk by: F.Bucci x rejection required (RICH x μ-veto x kinematics) 18m Ne radiator classic RICH with 16mm PMTs will deliver σ θ < 0.1 mrad e- μ- π separation over GeV/c 800 MHz 11 MHz 50 MHz π + K + ~ 75 GeV ν ν CKM (ktev2) Similar expt Was planned for FNAL Main injector D.Websdale, RICH2007, Trieste, Italy 15
16 Nucleon structure physics - HERMES HERA electron beam on polarized gas-jet target Probe spin structure of nucleon See talk by: R.De Leo C 4 F 10 gas + Aerogel radiators ( Pioneered Aerogel RICH) Hadron ID in range 2 15 GeV/c Completed in 2007 after 7 years stable running Carbon fibre mirrors < 1% X PMTs 23mm diameter N_photon hits ~12 σ θ ~ 7mrad θ C4F10 gas radiator D.Websdale, RICH2007, Trieste, Italy 16
17 Nucleon structure physics - COMPASS 160 GeV polarized muons on polarized target at CERN SPS Probe of gluon structure function and spin of nucleon Charm is signature of gluon (no vertex detector so hadron ID is crucial) RICH: C 4 F 10 gas radiator, mirror (20m 2 ) focused RICH 5m 2 CsI photocathode + MWPC (1cm 2 pixel) See talk by: FT F.Tessarotto F.Sozzi M.Sulc A.Teufel D.Websdale, RICH2007, Trieste, Italy 17
18 Nucleon structure physics - COMPASS Compass operation stable after 2 years running in 2006 upgrade: Replaced central CsI photon detectors by M16 MaPMTs Big improvement Nγ ~ 60 (cf 14) σ ring ~ 0.3mrad(0.6) PID up to 55 GeV (43) Δt ~ 1ns (3μs) D.Websdale, RICH2007, Trieste, Italy 18
19 Hadron physics (low p T ) - PANDA AntiProton ANihilations at Darmstadt (~2013) PANDA: 100% acceptance fixed target spectrometer at FAIR (Facility for Antiproton and Ion Research at GSI) Exotic hadron spectroscopy glueballs, quark molecules, hybrids Barrel-DIRC RICH Endcap Disc DIRC D.Websdale, RICH2007, Trieste, Italy 19
20 Cherenkov Detectors in PANDA HERMES-style RICH BaBar-style DIRC Disc focussing DIRC 2-dimensional imaging type See talk by: KFöhl K.Föhl C.Schwarz PSchönmeier P.Schönmeier ϑ* measurement one-dimen nsional imaging DI RC type ϕ* measurement fused silica radiator D.Websdale, RICH2007, Trieste, Italy 20 side view front view Ω* ϕ* ϑ*
21 Hadron physics (low p T ) MIPP See talk by: NGraf N.Graf 100% acceptance spectrometer π,k,p beam from FNAL Main Injector CO 2 classic RICH, 3000 PMTs 3σ π / K separation up to 90 GeV Planned upgrade for neutrino beam and dilc studies (verification of Hadron interaction simulation codes) COMPASS also moves on to its hadron spectroscopy programme D.Websdale, RICH2007, Trieste, Italy 21
22 Heavy Ion physics - ALICE ALICE studies the physics of strongly interacting matter and the quark-gluon plasma (QGP) in nucleus-nucleus l collisions i at the LHC. See talk by: A.Di Mauro G.Volpe D.Di Bari The HMPID RICH identifies hadrons π/k/p in the range 1/3/5 GeV/c D.Websdale, RICH2007, Trieste, Italy 22
23 Heavy Ion physics - ALICE Measurement of particle ratios over a wide momentum range de/dx, TOF, RICH, TRD are used The HMPID RICH covers the range 1-5GeV/c 7 modules of 1.5m x 1.5m (5% of barrel) C 6 F 14 liquid radiator, proximity focused CsI + MWPC (8mm x 8mm pixels) VHMPID: upgrade planned to extend PID to 30 GeV/c. C 5 F 12 gas radiator (1m) mirror-focused RICH CsI photocathode th + GEM photon detector t See talk by: G.Volpi D.Websdale, RICH2007, Trieste, Italy 23
24 Heavy Ion physics - JLAB JLAB: fixed target High Resolution Spectrometer RICH for K physics Same technology as ALICE HMPID Electron scatter from nuclei (ee K) reaction creates hypernuclei important to physics of neutron stars Pion rejection factor ~ 1000 ( GeV/c) Upgrade foreseen for 2008 running See talk by: E.Cisbani D.Websdale, RICH2007, Trieste, Italy 24
25 Heavy Ion physics - CBM CBM: Compressed p Baryonic y Matter at FAIR, GSI (2013) Fixed target: AGeV, 10MHz rate Detect low-mass vector mesons leptons PID up to 10GeV/c with excellent electron ID RICH: Classic mirror-focussed RICH 2.2m gas radiator Be-glass mirrors MaPMT photon detectors See talk by: C.Höhne D.Websdale, RICH2007, Trieste, Italy 25
26 Heavy Ion physics - RHIC Relativistic Heavy Ion Collider: E CM = 200 AGeV Physics requirements Compare hadron ratios: e.g. meson/baryon in p-p vs A-A Identify electron pairs: nuclear matter is transparent so probe interior Three of the experiments use RICH for PID BRAHMS C 4 F 10 /C 5 F 14 gas: M4 MaPMTs: hadron ID up to 30GeV PHENIX CF 4 gas: CsI photocathode: hadron blind electron ID STAR (ALICE-like RICH) C 6 F 14 liquid: proximity focused: π/k/p ID from 1/3/5GeV/c D.Websdale, RICH2007, Trieste, Italy 26
27 Neutrino physics T2K (2009) Super Kamiokande The largest Cherenkov in use at an accelerator-based experiment will soon be fully repaired, operational with upgraded DAQ 50ktonnes water viewed by 13, PMTs Upgrade : deadtime-less acquisition and enhanced DAQ allow refined trigger and lower (~2MeV) threshold Aim is to measure mixing angle θ 13 D.Websdale, RICH2007, Trieste, Italy 27
28 Summary - 1 Many accelerator/collider experiments use or plan to use RICH detectors Flavour physics and CP violation Nucleon structure Hadron (low p T ) physics Heavy Ion physics, QGP Neutrino oscillations BELLE, BABAR, HERA-B, LHCb, NA62 HERMES, COMPASS PANDA, MIPP, COMPASS ALICE, JLAB, CBM, STAR, BRAHMS, PHENIX T2K (MIPP) Bold type = reporting at RICH 2007 NB: Not in high p T collider detectors Tevatron, LHC GPDs D.Websdale, RICH2007, Trieste, Italy 28
29 Summary - 2 Personal observations and interpretations Ubiquity of the RICH detector Diversity of RICH detector types choice informed by: physics requirements space constraints cost Current trends Classic mirror-focused gas RICH for high energies Use of vacuum tube photon detectors where feasible Proximity focused + CsI+MWPC/GEM photon detectors for large areas Emergence of DIRC as favoured technique for barrel configuration Future trends Exploring benefits of precise timing (TOP) Development of solid state photon detectors D.Websdale, RICH2007, Trieste, Italy 29
Tests 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
Cherenkov light imaging in particle and nuclear physics experiments
Cherenkov light imaging in particle and nuclear physics experiments K. Inami (Nagoya univ.) 2016/9/5, RICH2016 Topics in the session 2 Performance of the LHCb RICH detectors during the LHC Run II ALICE-HMPID
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)
The 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
RICH 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
The Quark-Gluon Plasma and the ALICE Experiment
The Quark-Gluon Plasma and the ALICE Experiment David Evans The University of Birmingham IoP Nuclear Physics Conference 7 th April 2009 David Evans IoP Nuclear Physics Conference 2009 1 Outline of Talk
Particle Identification of the LHCb detector
HCP 2005 Particle Identification of the LHCb detector Ann.Van.Lysebetten@cern.ch on behalf of the LHCb collaboration CERN 5th July 2005 The LHCb experiment : introduction precision measurements of CP violation
An 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
PANDA. antiproton Annihilation at DArmstadt
antiproton Annihilation at DArmstadt Physics programme Quark confinement: Charmonium spectroscopy Excited gluons: Exotic hybrid mesons & glueballs Nucleon spin puzzle: transverse quark spin distribution
7 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
from outside Europe: 27 CERN
WORKSHOP HIGHLIGHTS RICH2007 summary in short: great VITALITY of Cherenkov Imaging Detectors! 1 OUTLINE OUTLINE RICH2007 figures the key role played by Cherenkov Imaging detectors in a variety of fields
Particle Identification at a super B Factory. FRASCATI WORKSHOP DISCUSSION ON PID
Particle Identification at a super B Factory. FRASCATI WORKSHOP DISCUSSION ON PID Do no harm! ( The Hippocratic oath of detector designers, especially for those outside you ). Keep a minimum thickness
Kaon 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
The PANDA experiment at FAIR
The PANDA experiment at FAIR Helmholtz-Institut Mainz, Germany On behalf of the PANDA collaboration Facility for Antiproton and Ion Research (FAIR) PANDA physics program PANDA spectrometer PANDA phases
CLAS12 at Jefferson Lab
CLAS12 at Jefferson Lab Daria Sokhan University of Glasgow, UK IPPP/NuSTEC Topical Meeting on Neutrino-Nucleus Scattering IPPP, Durham, UK 19 April 2017 Jefferson Lab 6 GeV era Jefferson Lab CEBAF: Continuous
MEIC Central Detector Zhiwen Zhao for JLab MEIC Study Group
MEIC Central Detector Zhiwen Zhao for JLab MEIC Study Group MEIC Collaboration Meeting 2015/10/07 MEIC Design Goals Energy Full coverage of s from 15 to 65 GeV Electrons 3-10 GeV, protons 20-100 GeV, ions
International Workshop on Heavy Quarkonium Oct. 2007, DESY Hamburg. Prospects for Panda. Charmonium Spectroscopy
International Workshop on Heavy Quarkonium 17 20 Oct. 2007, DESY Hamburg Prospects for Panda Charmonium Spectroscopy M. Pelizäus (Ruhr Universität Bochum) for the Panda Collaboration 1 FAIR accelerator
The Barrel DIRC Detector for the PANDA Experiment at FAIR
The Barrel DIRC Detector for the PANDA Experiment at FAIR TIPP 2017 conference (GSI) for the PANDA Cherenkov Group PANDA experiment Barrel DIRC design Expected performance Validation in beam tests Summary
Status 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
Accelerator Based Particle Physics Experiments
Accelerator Based Particle Physics Experiments Su Dong Stanford Student Orientation SLAC session Sep/16/2010 1 The Fundamental Questions Are there undiscovered principles of nature: new symmetries, new
A Very High Momentum Particle Identification Detector for ALICE
A Very High Momentum Particle Identification Detector for ALICE Daniel Mayani for the VHMPID proto-collaboration 5th Workshop on High-pt Physics at LHC September 27th October 1st Collaboration members
Flavour Physics at hadron machines
Flavour Physics at hadron machines KIAS Phenomenology Workshop Seoul, Korea, 17-19 November 2011 T. Nakada EPFL-LPHE Lausanne, Switzerland B physics, started with hadron machine First discovery of b-quark
The Fast Interaction Trigger Upgrade for ALICE
Chicago State University, Chicago, USA E-mail: edmundo.garcia@csu.edu On Behalf of the ALICE Collaboration The ALICE Collaboration is preparing a major detector upgrade for the second LHC long shutdown
Tests 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 Jožef Stefan Institute, Ljubljana, Slovenia; currently CERN, Geneva, Switzerland November 30 December 5, 2004 for BELLE Aerogel
High Energy Frontier Recent Results from the LHC: Heavy Ions I
High Energy Frontier Recent Results from the LHC: Heavy Ions I Ralf Averbeck ExtreMe Matter Institute EMMI and Research Division GSI Helmholtzzentrum für Schwerionenforschung Darmstadt, Germany Winter
PoS(CPOD07)056. The CBM Experiment at FAIR. Volker Friese 1. for the CBM Collaboration
The CBM Experiment at FAIR 1 Gesellschaft für Schwerionenforschung mbh Planckstraße 1, 64291 Darmstadt, Germany E-mail: v.friese@gsi.de for the CBM Collaboration The CBM experiment will investigate heavy-ion
ALICE Detector Status and Commissioning
ALICE Detector Status and Commissioning Hans-Åke Gustafsson, For the ALICE Collaboration CERN, Geneva, Switzerland and Lund University, Sweden Abstract. The Large Hadron Collider (LHC) will start operation
Novel sensors for Cherenkov counters
Novel sensors for Cherenkov counters Peter Križan University of Ljubljana and J. Stefan Institute Advanced Instrumentation Seminar, SLAC, June 10, 2009 Contents Why particle identification? Ring Imaging
Flavour Physics at LHC
Flavour Physics at LHC ICFP2009, Hanoi, September 2009 Tatsuya Nakada LPHE/EPFL Introduction (I) There exist solid observations for physics beyond the Standard Model T. Nakada ICFP2009 Hanoi September
ALICE A Large Ion Collider Experiment
ALICE A Large Ion Collider Experiment Purpose: study the physics of strongly interacting matter at extreme energy densities CERN LHC: Colliding Pb ions at E CM =5.5 A TeV, p-p, light ions collisions 84
Recent 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,
LHCb 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,
CMS 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
Particle Detectors A brief introduction with emphasis on high energy physics applications
Particle Detectors A brief introduction with emphasis on high energy physics applications TRIUMF Summer Institute 2006 July 10-21 2006 Lecture I measurement of ionization and position Lecture II scintillation
Study of Baryon Form factor and Collins effect at BESIII
Study of Baryon Form factor and Collins effect at BESIII Wenbiao Yan On behalf of BESIII Collaboration INT Program INT-17-3 Hadron imaging at Jefferson Lab and at a future EIC 1 Bird s View of BEPCII &
LHC Detectors and their Physics Potential. Nick Ellis PH Department, CERN, Geneva
LHC Detectors and their Physics Potential Nick Ellis PH Department, CERN, Geneva 1 Part 1 Introduction to the LHC Detector Requirements & Design Concepts 2 What is the Large Hadron Collider? Circular proton-proton
Barrel time-of-flight (TOF) detector for the PANDA experiment at FAIR
Barrel time-of-flight (TOF) detector for the PANDA experiment at FAIR K. Suzuki 1, D. Steinschaden 1, S. Zimmermann 1 2, N. Kratochwil 1, L. Gruber 3, C. Schwarz 4, H. Orth 4, L. Schmitt 5, K. Gtzen 4,
Status 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
b 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
Experimental overview of the PANDA experiment
Experimental overview of the PANDA experiment Elisa Fioravanti for the PANDA Collaboration INFN Ferrara, Via Saragat 1, 44100 Ferrara, Italy E-mail: fioravanti@fe.infn.it Abstract. The physics program
Heavy Ion Physics Program of CERN: Alice Setup at LHC.
Heavy Ion Physics Program of CERN: Alice Setup at LHC. Dr.Sc. Mais Suleymanov Department of Physics CIIT Islamabad First School on LHC Physics: ALICE week NCP Islamabad, 12-30 October,2009 1 1 ρc 7 10
Vol. 5 (2012) Acta Physica Polonica B Proceedings Supplement No 4 PANDA AT FAIR. Tord Johansson. representing the PANDA Collaboration
Vol. 5 (2012) Acta Physica Polonica B Proceedings Supplement No 4 PANDA AT FAIR Tord Johansson representing the PANDA Collaboration Departmet of Physics and Astronomy, Uppsala University Box 516, 75120
Stars Nuclei Baryons Quarks. STRANGENESS IN NUCLEI UNIQUE OPPORTUNITIES at FAIR Josef Pochodzalla
Stars Nuclei Baryons Quarks STRANGENESS IN NUCLEI UNIQUE OPPORTUNITIES at FAIR Josef Pochodzalla Facility for Antiproton and Ion Research GSI, Darmstadt heavy ion physics nuclear structure atomic and plasma
The 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,
Drell-Yan experiments at Fermilab/RHIC/J-PARC. QCD Frontier 2013 Jefferson Lab October 21, 2013 Yuji Goto (RIKEN)
Drell-Yan experiments at Fermilab/RHIC/J-PARC QCD Frontier 2013 Jefferson Lab October 21, 2013 Yuji Goto (RIKEN) Outline Fermilab Drell-Yan experiments Unpolarized program Flavor asymmetry of sea-quark
ALICE Commissioning: Getting ready for Physics
ALICE Commissioning: Getting ready for Physics Christian Lippmann, CERN for the ALICE Collaboration Moriond QCD and High Energy Interactions March 14th - March 21st 2009 1 Outline Introduction to ALICE
Search 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.
Particle 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
Early 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
Accelerators. Acceleration mechanism always electromagnetic Start with what s available: e - or p Significant differences between accelerators of
Accelerators Acceleration mechanism always electromagnetic Start with what s available: e - or p Significant differences between accelerators of e - : Always ultra-relativistic, therefore constant speed
The achievements of the CERN proton antiproton collider
The achievements of the CERN proton antiproton collider Luigi DiLella Scuola Normale Superiore, Pisa, Italy Motivation of the project The proton antiproton collider UA1 and UA2 detectors Discovery of the
Last Friday: pp(bar) Physics Intro, the TeVatron
Last Friday: pp(bar) Physics Intro, the TeVatron Today: The Large Hadron Collider (LHC) The Large Hadron Collider (LHC) 7 TeV + 7 TeV Protons Protons 10 11 Protons per bunch Bunch Crossings 4x10 7 Hz Proton
PoS(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
Helicity: Experimental Status. Matthias Grosse Perdekamp, University of Illinois
Helicity: Experimental Status Matthias Grosse Perdekamp, University of Illinois Content o The Experimental Effort o Quark and Sea Quark Helicity è DIS, SIDIS, pp è new FFs for global analysis è results
The 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)
Guest Lecture PHY 7361: Harnessing Cherenkov Radiation SteveSekula, 13 April 2010 (created 9 April 2010)
Physics Notebook - 2010 Steve Sekula's Analysis Notebook Physics Notebook - 2010 Steve Sekula's Analysis Notebook Guest Lecture PHY 7361: Harnessing Cherenkov Radiation SteveSekula, 13 April 2010 (created
Perspectives with PANDA. The new accelerator complex of GSI The antiproton s s activity The PANDA scientific program Paola Gianotti LNF
Perspectives with PANDA The new accelerator complex of GSI The antiproton s s activity The PANDA scientific program Paola Gianotti LNF FAIR The GSI future facility FAIR Facility for Antiproton and Ion
Simulation studies of the PANDA detector at GSI
Simulation studies of the PANDA detector at GSI Carsten Schwarz for the Antiproton Physics Study Group PANDA = Proton ANtiproton at DArmstadt Introduction HESR (High Energy Storage Ring) Physics program
Highlights from. Part I HEPP-EPS EPS Lisbon, Portugal, July 21 st 27 th, International Europhysics Conference on High Energy Physics
Highlights from HEPP-EPS EPS 2005 International Europhysics Conference on High Energy Physics Lisbon, Portugal, July 21 st 27 th, 2005 Part I Uta Stösslein (DESY) Zeuthen, September 7 th, 2005 Programme
The Aerogel Forward RICH detector for PANDA
The Aerogel Forward RICH detector for PANDA Presented by Sergey Kononov A.Yu.Barnyakov abe, M.Yu.Barnyakov abc, K.I.Beloborodov abe, V.S.Bobrovnikov ab, A.F.Danilyuk bd, A.A.Katcin ac, S.A.Kononov abe,
Year- 1 (Heavy- Ion) Physics with CMS at the LHC
Year- 1 (Heavy- Ion) Physics with CMS at the LHC Edwin Norbeck and Yasar Onel (for the CMS collaboration) University of Iowa For the 26 th Winter Workshop on Nuclear Dynamics Ocho Rios, Jamaica 8 January
Francesco Barile for the ALICE Collaboration. Università degli Studi di Bari & INFN
Produzione di deutoni e anti-deutoni nelle collisioni centrali Pb-Pb a snn= 2.76 TeV con il rivelatore Cherenkov HMPID nell'ambito dell'esperimento ALICE ad LHC Francesco Barile for the ALICE Collaboration
The CBM experiment - a status report
The CBM experiment - a status report V. Friese 1, * 1 GSI Helmholtzzentrum fur Schwerionenforschung mbh, Darmstadt, Germany The CBM experiment is being designed to study strongly interacting matter at
e + e - (1) Silicon Vertex Detector
3.1 GeV (4) Electromagnetic Calorimeter (3) Cerenkov- Detector (2) Drift Chamber (5) 1.5 T Solenoid (6) Instrumented Iron Yoke e + e - (1) Silicon Vertex Detector 9.0 GeV e + e - Colliders as B Factories
Flavor 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
PoS(CPOD2017)028. Prospect of Heavy-ion Collision Experiments at J- PARC. Hiroyuki Sako 1
Prospect of Heavy-ion Collision Experiments at J- PARC 1 Japan Atomic Energy Agency Tokai, Naka, Ibaraki, Japan E-mail: hiroyuki.sako@j-parc.jp University of Tsukuba Tsukuba, Ibaraki, Japan In order to
(a) (b) Fig. 1 - The LEP/LHC tunnel map and (b) the CERN accelerator system.
Introduction One of the main events in the field of particle physics at the beginning of the next century will be the construction of the Large Hadron Collider (LHC). This machine will be installed into
arxiv: v1 [physics.ins-det] 3 Dec 2018 Fast Interaction Trigger for the upgrade of the ALICE experiment at CERN: design and performance
![arxiv: v1 [physics.ins-det] 3 Dec 2018 Fast Interaction Trigger for the upgrade of the ALICE experiment at CERN: design and performance](/thumbs/96/128514105.jpg "arxiv: v1 [physics.ins-det] 3 Dec 2018 Fast Interaction Trigger for the upgrade of the ALICE experiment at CERN: design and performance")
arxiv:1812.00594v1 [physics.ins-det] 3 Dec 2018 Fast Interaction Trigger for the upgrade of the ALICE experiment at CERN: design and performance Alla Maevskaya for the ALICE collaboration 1, 1 Institute
: status and prospects
Charm at : status and prospects Gagan Mohanty Tata Institute, Mumbai DHEP Seminar February 2, 2012 Outline of the talk 1) Introduction and motivation 2) KEKB SuperKEKB 3) Enter Belle II detector 4) Status
Flavour physics in the LHC era
Maria Laach school, september 2012 An introduction to Flavour physics in the LHC era and quest for New Physics (an experimentalist s point of view) Clara Matteuzzi INFN and Universita Milano-Bicocca 1
Beauty physics with B s and Λ b
Beauty physics with B s and Λ b Rolf Oldeman INFN Roma 1 "La Sapienza" Selected topics Masses Lifetimes B s lifetime difference Charmless B s and Λ b decays B s oscillations Rare decays covered today by
Exploring dense matter at FAIR: The CBM Experiment
Exploring dense matter at FAIR: The CBM Experiment What s it all about Landmarks of the QCD phase diagram: deconfinement phase transition chiral phase transition critical point 2 Signatures of phase transition
New Physics with a High Intensity PS (in Italy)
1 New Physics with a High Intensity PS (in Italy) F. Cervelli I.N.F.N. Pisa 2 At present, in the worldwide requests of constructing a High Intensity Proton Machine are rising. Why? 3 The central issues
Experimental results on nucleon structure Lecture I. National Nuclear Physics Summer School 2013
Experimental results on nucleon structure Lecture I Barbara Badelek University of Warsaw National Nuclear Physics Summer School 2013 Stony Brook University, July 15 26, 2013 Barbara Badelek (Univ. of Warsaw
17/01/17 F. Ould-Saada
Chapter 3 3.1 Why Do We Need Accelerators? 3.1.1 The Center-of-Mass (c.m.) System 3.1.2 The Laboratory System 3.1.3 Fixed Target Accelerator and Collider 3.2 Linear and Circular Accelerators 3.2.1 Linear
QGP event at STAR. Patrick Scott
QGP event at STAR Patrick Scott Overview What is quark-gluon plasma? Why do we want to study quark-gluon plasma? How do we create quark-gluon plasma? The past and present SPS and RHIC The future LHC and
The 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
The Gamma Factory proposal for CERN
The Gamma Factory proposal for CERN Photon-2017 Conference, May 2017 Mieczyslaw Witold Krasny LPNHE, CNRS and University Paris Sorbonne 1 The Gamma Factory in a nutshell Accelerate and store high energy
B-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
Results from B-Physics (LHCb, BELLE)
Prospects for Charged Higgs Uppsala, Sweden, 16-18 September 2014. Results from B-Physics (LHCb, BELLE) Valery Pugatch Kiev Institute for Nuclear Research, NASU On behalf of the LHCb Collaboration 1 OUTLINE
Collider physics. Introduction Some e + e - collider physics. Hadronic machines. R(e + e - hadrons/ e + e - µ - µ + ) Z 0 and W at LEP
Collider physics Introduction Some e + e - collider physics R(e + e - hadrons/ e + e - µ - µ + ) Z 0 and W at LEP Hadronic machines Total cross sections Hard and soft collisions Triggers An example: LHCb
Cherenkov Detectors in Particle Physics. Brad Wogsland University of Tennessee
Cherenkov Detectors in Particle Physics Brad Wogsland University of Tennessee Outline Cherenkov light RICH detectors CRID detectors The DIRC Design & performance Potential for use in Future experiments
First results with heavy-ion collisions at the LHC with ALICE
First results with heavy-ion collisions at the LHC with ALICE Domenico Elia INFN, Bari (Italy) on behalf of the ALICE Collaboration D. Elia (INFN Bari, Italy) PANIC 011 / Boston, MA (USA) July 4-9, 011
Status 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
High Momentum Particle IDentification (HMPID) in ALICE. Pusan National University In-Kwon Yoo For ALICE / HMPID Collaboration
High Momentum Particle IDentification (HMPID) in ALICE Pusan National University In-Kwon Yoo For ALICE / HMPID Collaboration Why HMPID? Pre-ALICE RHIC Physics Physics of the HMPID PID in ALICE HMPID RICH
The Mystery of Vus from Tau decays. Swagato Banerjee
The Mystery of Vus from Tau decays Swagato Banerjee Flavor generations in the Standard Model Vij: Mixing between Weak and Mass Eigenstates 2 Unitarity of the CKM matrix 1!! 3! 1! 2! 3! 2 1 V ud = 0.97408
ALICE and LHCb in the HL-LHC era
ALICE and LHCb in the HL-LHC era LHC CHAMONIX 2011 January 27, 2011 Sergio Bertolucci CERN General considerations In the last couple of years, the LHC original experimental programme is undergoing the
Identifying Particle Trajectories in CMS using the Long Barrel Geometry
Identifying Particle Trajectories in CMS using the Long Barrel Geometry Angela Galvez 2010 NSF/REU Program Physics Department, University of Notre Dame Advisor: Kevin Lannon Abstract The Compact Muon Solenoid
BaBar DIRC in SoLID. P. Nadel-Turonski, Z. Zhao, C. Hyde... SoLID bi-weekly meeting, January 15, 2013
BaBar DIRC in SoLID P. Nadel-Turonski, Z. Zhao, C. Hyde... SoLID bi-weekly meeting, January 15, 2013 1 Emerging opportunity 1. BaBar DIRC suddenly becomes available in December 2012 SuperB (next generation
Will LHCb be running during the HL-LHC era? Burkhard Schmidt for the LHCb Collaboration
Will LHCb be running during the HL-LHC era? Burkhard Schmidt for the LHCb Collaboration Helpful discussions with L. Rossi and several other colleagues from the machine acknowledged Outline: Introduction
The ALICE Forward Multiplicity Detector from Design to Installation. Christian Holm Christensen
The ALICE Forward Multiplicity Detector from Design to Installation Overview Matter and the Quark Gluon Plasma Heavy Ion Collisions and ALICE The Forward Multiplicity Detector: Motivation, sensors, electronics,
Nuclear and Particle Physics 3: Particle Physics. Lecture 1: Introduction to Particle Physics February 5th 2007
Nuclear and Particle Physics 3: Particle Physics Lecture 1: Introduction to Particle Physics February 5th 2007 Particle Physics (PP) a.k.a. High-Energy Physics (HEP) 1 Dr Victoria Martin JCMB room 4405
Lecture 4 Calorimetry. Lecture 5a - Particle Identification. Lecture 5b - Detector Systems/ Design
Outline Lecture - Introduction Lecture - Tracking Detectors Lecture 3 - Scintillation and Photodetection Lecture 4 Calorimetry Lecture 5a - Particle Identification C. Joram, L. Ropelewski L. Ropelewski,
Future Belle II experiment at the KEK laboratory
Future Belle II experiment at the KEK laboratory Jarosław Wiechczyński 27.03.2017 Rencontres de Moriond QCD and High Energy Interactions 2 Outline B factories and their features SuperKEKB collider and
Particle Identification and Forward Detectors
ACT Lectures on Detectors (4/5) CERN, May 12, 2011 Particle Identification and Forward Detectors Peter Križan University of Ljubljana and J. Stefan Institute University of Ljubljana Jožef Stefan Institute
Meson spectroscopy at CLAS and CLAS12: the present and the future. Raffaella De Vita INFN Genova for the CLAS Collaboration
Meson spectroscopy at CLAS and CLAS12: the present and the future Raffaella De Vita INFN Genova for the CLAS Collaboration Why hadron spectroscopy? QCD is responsible for most of the visible mass in the
The Jefferson Lab 12 GeV Program
The Jefferson Lab 12 GeV Program The Jefferson Lab facilities have undergone a substantial upgrade, both of accelerator, CEBAF, and of the experimental installations. We will discuss the progress to completion
Physics opportunities with an upgraded LHCb detector in the HL-LHC era
Physics opportunities with an upgraded LHCb detector in the HL-LHC era Sascha Stahl, CERN on behalf of the LHCb collaboration Some slides inspired by the very nice experimental and theoretical flavour
Beyond Standard Model Effects in Flavour Physics: p.1
Beyond Standard Model Effects in Flavour Physics: Alakabha Datta University of Mississippi Feb 13, 2006 Beyond Standard Model Effects in Flavour Physics: p.1 OUTLINE Standard Model (SM) and its Problems.
The Alice Experiment Felix Freiherr von Lüdinghausen
The Alice Experiment Felix Freiherr von Lüdinghausen Alice, who is Alice? Alice is A Large Ion Collider Experiment. Worldwide hit in 1977 for the band Smokie Alice is the dedicated heavy ion experiment