Simulation studies of the PANDA detector at GSI

Size: px
Start display at page:

Download "Simulation studies of the PANDA detector at GSI"

Transcription

1 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 Simulation of Detector components Micro Vertex Tracker Straw Tube Tracker DIRC RICH Calorimeter Summary & Outlook

2 GSI HESR High Energy Storage Ring Momenta GeV/c Spread (<8 GeV/c) Beam Ø 100 um p stored in ring 5 x L (pellet target) 2 x cm -2 s -1 Int. L 10 pb -1 /day

3 Physics Program Charmonium spectroscopy Glueballs Hybrids Medium modifications of D mesons and J/Ψ in nuclei CP violation Hypernuclei

4 Simulation framework: C++ Geant4 Root Event Generation DPM pbar+p background UrQMD pbar+a PndEvtGen (Pluto) PndSimApp GEANT4 modelling of the detector PndRecoApp Tracking, EMC-cluster finding, RICH rings... PandaApp 'user analysis', PID, spectra Full simulation Fast simulation

5 Angular Acceptance Formation of ψ and decay in muons ψ µ + µ - µ + µ - ψ J/ψ + X similarly electrons: -->for large angles calorimeter needed.

6 PANDA Detector Target spectrometer Forward spectrometer

7 Micro Vertex Detector (MVD) 7.2 mio. barrel pixels 50 x 300 µm pellet pipe beam pipe 2 mio. forward pixels 100 x 150 µm Layers 5 barrel, 5 endcap thickness 200 µm thick. 5 layers % X 0 resolution σ φz µm Readout: ASICs (ATLAS/CMS) 0.37% X 0 or pixel one side - readout other side (TESLA)

8 MVD geometry y D 0 z Z 0 x

9 Geant4 and multiple scattering MeV pc z x X ln x X 0

10 Straw tubes DIRC STT MVD Number of double layers Skew angle of double layers 1 and 15 Skew angle of double layers 2-14 Straw tube wall thickness Wire thickness Gas Length Diameter of tubes in double layers 1-5, 6-10, and Number of straw tubes 15 0 o 2 o -3 o Transverse resolution σ x,y 150 µm Longitudinal resolution σ 1 mm z 26 µm 20 µm 90%He+10%C 4 H cm 4, 6, 8 mm 8734 Event example: pp --> φφ --> 4K

11 DIRC Detecting Internally Reflected -light PID: tracking --> p, RICH --> β --> m less space than aerogels costs of calorimeter no problems with field

12 DIRC degree degree degree degree K eff. χ 2 /n=2.4 pion beta= photons π miss-id. reaction pp φφ at s = 3.6 GeV/c 2

13 T1 T2 DIRC Time Of Propagation (discussed at Belle) T, reduced # of PMT for Kaon PID very good time resolution required (~ 100 ps)

14 DIRC radiator quality Edge losses Edge thickn. Sharpness of edges should be 50 µm

15 Forward RICH Search for good combination radiator photon detector magnetic field Aerogel (n=1.02) visible light PD HPD C 6 F 14 (n=1.24) CsI coated photo cath. (λ < 210 nm = UV) 4 10 cm Proximity "focussing" compact detector

16 Aerogel and Rayleigh scattering Aerogel C 6 F 14 Photon # generated Det. Eff. Rayleigh scattered Detected Wavelength [nm] Wavelength [nm] Combination of aerogel radiator and CsI-photo cathode is not working. Visible light???

17 Forward RICH LHCb Multi pad gas Detector Mismatch photons<-> CsI photon conversion Aerogel n=1.02 proximity focusing mirrors

18 Calorimeter PbWO 4 Length = 17 X 0 APD readout (in field) σ(e) = 1.54% / E ½ + 0.3% (PM) pp J/ψ + η γγ

19 Summary & Outlook Status Design of PANDA for GSI Future Project Simulations in a framework of C++, Geant4, and ROOT Target spectrometer nearly implemented Future tasks Completion of detector implementation (forward spectrometer) Intensive background simulations Annihilations ~ 100 mb Reactions nb need 10 8 events for each valid event to prove background supression --> fast simulation

20 Antiproton Physics Study Group T. Barnes 1, D. Bettoni 2, R. Calabrese 2, W. Cassing 3, M. Düren 3, P.Thörngren Engblom 4, S. Ganzhur 5, A. Gillitzer 6, O. Hartmann 7, V. Hejny 6, P. Kienle 8, H. Koch 5, W. Kühn 3, Agnes Lundborg 9, Elin Lundström 9, U. Lynen 7, R. Meier 10, V. Metag 3, P. Moskal 6, Örjan Nordhage 9, H. Orth 7, S. Paul 8, K. Peters 5, J. Pochodzalla 11, J. Ritman 3, Y. Rogov 12, H. Rohdjess 13, M. Sapozhnikov 12, L. Schmitt 8, 7, K. Seth 14, A. Sokolov 7, V. Uzhinsky 12, N. Vlassov 12, W. Weise 8, U. Wiedner 9 1) University of Tennessee, Knoxville 2) INFN, Ferrara 3) Universität Gießen 4) Uppsala University 5) Experimentalphysik 1, Bochum 6) Institut für Kernphysik, FZ Jülich 7) GSI Darmstadt 8) Technische Universität München 9) ISV, Uppsala 10) Physikalisches Institut, Tübingen 11) Institut für Kernphysik, Mainz 12) JINR, Dubna 13)Universität Bonn 14) Northwestern University, Evanston

Monte Carlo Simulations for PANDA

Monte Carlo Simulations for PANDA Monte Carlo Simulations for PANDA Diego Bettoni Istituto Nazionale di Fisica Nucleare, Ferrara International Workshop on Heavy Quarkonia 2008 Nara, Japan, 3 December 2008 Outline Introduction The PANDA

More information

Charmonium Physics with PANDA at FAIR. FZ-Juelich & Uni Bochum

Charmonium Physics with PANDA at FAIR. FZ-Juelich & Uni Bochum Charmonium Physics with PANDA at FAIR Contents Overview of PANDA Physics program Charmonium Physics Issues with PANDA FAIR Accelerator Facility PANDA Detector Summary Hadron Structure with Precision Measurements

More information

The PANDA experiment at FAIR

The PANDA experiment at FAIR The PANDA experiment at FAIR Ulrich Wiedner Uppsala University Elba, June 7, 2004 The key issues creation of mass QCD exotics (glueballs, hybrids) charmed hadrons in nuclei confinement exotics states of

More information

Prospects for X(3872) Detection at Panda

Prospects for X(3872) Detection at Panda Prospects for X(3872) Detection at Panda Jens Sören Lange, Martin Galuska, Thomas Geßler, Wolfgang Kühn, Stephanie Künze, Yutie Liang, David Münchow, Björn Spruck, Matthias Ullrich, and Marcel Werner II.

More information

The PANDA Detector at FAIR

The PANDA Detector at FAIR at FAIR Lars Schmitt, GSI on behalf of the PANDA Collaboration PANIC 2008, Eilat, Israel, November 11th 2008 The Facility Overview of PANDA Physics Summary and Outlook Facility for Antiproton and Ion Research

More information

Physics with PANDA at FAIR

Physics with PANDA at FAIR Physics with PANDA at FAIR Inti Lehmann University of Glasgow Tbilisi, Sept. 5th, 2006 Some Open Questions in generation of hadron masses spin puzzle Non-Perturbative QCD strong interaction at large distances

More information

Nuclear and Hadron Physics with Antiprotons

Nuclear and Hadron Physics with Antiprotons Nuclear and Hadron Physics with Antiprotons PANDA @ FAIR Olaf N. Hartmann INFN Laboratori Nazionali di Frascati Overview The Facility: FAIR, HESR The Physics Program The Detector The Collaboration Outlook

More information

Hadron Physics with Antiprotons

Hadron Physics with Antiprotons Hadron Physics with Antiprotons Introduction HESR/PANDA - Project at GSI ( W. Henning) Merits of experiments with antiprotons Physics Program Charmonium Spectroscopy ( D. Bettoni) Heavier Glueballs and

More information

PANDA FAIR. Anastasios Belias for the PANDA Collaboration GSI, Darmstadt, Germany. EXA2017, Vienna September 15th, 2017

PANDA FAIR. Anastasios Belias for the PANDA Collaboration GSI, Darmstadt, Germany. EXA2017, Vienna September 15th, 2017 PANDA Physics @ FAIR Anastasios Belias for the PANDA Collaboration GSI, Darmstadt, Germany EXA2017, Vienna September 15th, 2017 PANDA Physics @ FAIR The Facility PANDA Physics Goals Status & Outlook Facility

More information

The PANDA Experiment. Lars Schmitt, GSI on behalf of the PANDA Collaboration Open PANDA, Mainz, November 19th 2009.

The PANDA Experiment. Lars Schmitt, GSI on behalf of the PANDA Collaboration Open PANDA, Mainz, November 19th 2009. The PANDA Experiment Lars Schmitt, GSI on behalf of the PANDA Collaboration Open Charm @ PANDA, Mainz, November 19th 2009 The Facility Overview of PANDA Physics Summary and Outlook Facility for Antiproton

More information

Physics with the PANDA Detector at FAIR

Physics with the PANDA Detector at FAIR II. Physics Institute Justus-Liebig-Universität Giessen, Germany on behalf of the PANDA collaboration SPIN-Praha-2008, July 21 st 2008, Prague PANDA= AntiProton ANnihilations at DArmstadt Physics with

More information

International Workshop on Heavy Quarkonium Oct. 2007, DESY Hamburg. Prospects for Panda. Charmonium Spectroscopy

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

More information

The PANDA experiment: Antiproton physics at FAIR

The PANDA experiment: Antiproton physics at FAIR IL NUOVO CIMENTO Vol. 34 C, N. 6 Novembre-Dicembre 2011 DOI 10.1393/ncc/i2011-11089-2 Colloquia: IFAE 2011 The PANDA experiment: Antiproton physics at FAIR P. Montagna on behalf of the PANDA Collaboration

More information

The PANDA experiment at FAIR

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

More information

PANDA. antiproton Annihilation at DArmstadt

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

More information

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 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

More information

Physics Goals of PANDA

Physics Goals of PANDA Physics Goals of PANDA Introduction The PANDA Project PANDA and HESR Status of the PANDA Project Physics Program of PANDA Hadron Spectroscopy Merits of Antiproton Physics Properties of Hadrons in Matter

More information

Experimental overview of the PANDA experiment

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

More information

Kärnfysikermötet, Umeå 1-2 November 2005 Agnes Lundborg, Uppsala Universitet

Kärnfysikermötet, Umeå 1-2 November 2005 Agnes Lundborg, Uppsala Universitet Charmonium in e + e and pp Kärnfysikermötet, Umeå 1-2 November 2005 Agnes Lundborg, Uppsala Universitet Raise a whole bunch of Questions Charmonium is a good tool for QCD studies: Why we want to understand

More information

Particle Identification of the LHCb detector

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

More information

Content. Complex Detector Systems. Calorimeters Velocity Determination. Semiconductor detectors. Scintillation detectors. Cerenkov detectors

Content. Complex Detector Systems. Calorimeters Velocity Determination. Semiconductor detectors. Scintillation detectors. Cerenkov detectors Semiconductor detectors Semiconductor basics Sensor concepts Readout electronics Scintillation detectors General characteristics Organic materials Inorganic materials Light output response Calorimeters

More information

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 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

More information

MEIC Central Detector Zhiwen Zhao for JLab MEIC Study Group

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

More information

The Barrel DIRC Detector for the PANDA Experiment at FAIR

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

More information

Barrel time-of-flight (TOF) detector for the PANDA experiment at FAIR

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,

More information

Status of the LHCb RICH detector and the HPD

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

More information

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 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 information

Simulation of X(3872) Resonance Scan Using the PandaRoot Framework 1

Simulation of X(3872) Resonance Scan Using the PandaRoot Framework 1 Simulation of X(3872) Resonance Scan Using the PandaRoot Framework 1 XXXVIII. PANDA Collaboration Meeting, GSI Darmstadt Martin J. Galuska, Svende A. Braun, Wolfgang Kühn and Jens Sören Lange for the PANDA

More information

Overview of the PandaRoot Framework

Overview of the PandaRoot Framework Overview of the PandaRoot Framework for the Stefano Spataro computing group ISTITUTO NAZIONALE DI FISICA NUCLEARE Sezione di Torino Thuersday, 18th November, 2010 The Panda experiment AntiProton Annihilations

More information

Early physics with the LHCb detector

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

More information

Status of the LHCb RICH and hadron particle identification

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 information

The PANDA experiment at FAIR

The PANDA experiment at FAIR The PANDA experiment at FAIR Diego Bettoni Istituto Nazionale di Fisica Nucleare, Ferrara representing the PANDA collaboration Charm 2007 Cornell University, 8 August 2007 Outline FAIR HESR PANDA Physics

More information

Hadron structure with photon and antiproton induced reactions - QCD in the non-perturbative range -

Hadron structure with photon and antiproton induced reactions - QCD in the non-perturbative range - Hadron structure with photon and antiproton induced reactions - QCD in the non-perturbative range - Introduction Present: Photoproduction of Mesons at ELSA and MAMI CB-ELSA/TAPS Experiment Crystal Ball/TAPS

More information

The Aerogel Forward RICH detector for PANDA

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,

More information

Flavor Physics beyond the SM. FCNC Processes in the SM

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

More information

HADRON PHYSICS WITH ANTI-PROTONS: The PANDA EXPERIMENT AT FAIR

HADRON PHYSICS WITH ANTI-PROTONS: The PANDA EXPERIMENT AT FAIR MENU 2007 11th International Conference on Meson-Nucleon Physics and the Structure of the Nucleon September10-14, 2007 IKP, Forschungzentrum Jülich, Germany HADRON PHYSICS WITH ANTI-PROTONS: The PANDA

More information

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 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 information

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 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 information

Aerial view of the FAIR construction site.

Aerial view of the FAIR construction site. PANDA - p Annihilation at Darmstadt N. Bianchi, A. M. Bragadireanu (Ass.), P. Dorel (Ass.), P. Gianotti (Resp. Naz.), C. Guaraldo (Ass.), V. Lucherini, E. Pace, D. Orecchini (Tec.)., L. Passamonti (Tec.),

More information

QCD aspects of the antiproton program at GSI

QCD aspects of the antiproton program at GSI QCD aspects of the antiproton program at GSI H. Koch Ruhr-Universität t Bochum Titel Organizers: Mauro Anselmino, Helmut Koch (Coordinator), Ulrich Mosel, Dan-Olof Riska All talks available: http://www.ep1.ruhr-uni-bochum.de/~dagmar/trento.htm

More information

A copy can be downloaded for personal non-commercial research or study, without prior permission or charge

A copy can be downloaded for personal non-commercial research or study, without prior permission or charge Cowie, E., Föhl, K., Glazier, D., Hill, G., Hoek, M., Kaiser, R., Keri, T., Murray, M., Rosner, G., and Seitz, B. (2009) The P ANDA focussinglightguide disc DIRC. Journal of Instrumentation, 4 (9). P09006.

More information

Simulation and event reconstruction inside the PandaRoot framework

Simulation and event reconstruction inside the PandaRoot framework Journal of Physics: Conference Series Simulation and event reconstruction inside the PandaRoot framework To cite this article: S Spataro 28 J. Phys.: Conf. Ser. 119 3235 View the article online for updates

More information

The PANDA Experiment

The PANDA Experiment High Precision Hadron Physics at FIR Lars chmitt GI, armstadt First FIR FEE Workshop, October 2005 Outline 1 PN Overview Introduction Physics Program 2 Overview Highlights PN Q and Trigger PN Overview

More information

Study of Baryon Form factor and Collins effect at BESIII

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 &

More information

PANDA at FAIR : physics goals and experimental overview. Gianluigi Boca

PANDA at FAIR : physics goals and experimental overview. Gianluigi Boca Hirschegg, January 17 th, 2011 PANDA at FAIR : physics goals and experimental overview Gianluigi Boca GSI, Darmstadt, Germany and Universita di Pavia, Italy antiproton ANnihilation at DArmstadt Experiment

More information

Antiproton Physics (Overview of the PANDA Physics Program)

Antiproton Physics (Overview of the PANDA Physics Program) Antiproton Physics (Overview of thepanda Physics Program) Diego Bettoni INFN, Ferrara, Italy International School of Nuclear Physics, From Quarks and Gluons to Hadrons and Nuclei Erice, Italy, 16-24 September

More information

Status dell esperimento PANDA

Status dell esperimento PANDA Status dell esperimento PANDA Daniela Calvo on behalf of the PANDA collaboration Sezione di Torino SIF2011, Societa Italiana di Fisica - XCVII Congresso Nazionale 26-30 Settembre 2011, L Aquila, Italy

More information

An Overview of RICH Detectors From PID to Velocity Spectrometers

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

More information

GlueX Capabilities for Nuclear Photoproduction

GlueX Capabilities for Nuclear Photoproduction GlueX Capabilities for Nuclear Photoproduction A. Somov, Jefferson Lab Nuclear Photoproduction with GlueX April 28 29, 2016 Physics Topics with Nuclear Targets Considered for GlueX Photoproduction of vector

More information

Heavy Hadron Production and Spectroscopy at ATLAS

Heavy 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 information

VO Detector and detector systems for particle and nuclear physics I. Friday

VO Detector and detector systems for particle and nuclear physics I.   Friday VO 260 066 Detector and detector systems for particle and nuclear physics I E-mail: johann.zmeskal@oeaw.ac.at Friday 9.1.2015 Detector 1 PARTICLE DETECTION Particle cannot be seen or measured directly

More information

Particle Detectors A brief introduction with emphasis on high energy physics applications

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

More information

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 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 information

The PANDA experiment: physics goals and experimental setup

The PANDA experiment: physics goals and experimental setup PJ Web of Conferences 72, 00002 ( 2014) DOI: 10.1051/ epjconf/ 20147200002 C Owned by the authors, published by DP Sciences, 2014 The PANDA experiment: physics goals and experimental setup Gianluigi Boca,

More information

Development and Applications of Tracking of Pellet Streams. Andrzej Pyszniak

Development and Applications of Tracking of Pellet Streams. Andrzej Pyszniak Development and Applications of Tracking of Pellet Streams Andrzej Pyszniak Dissertation presented at Uppsala University to be publicly examined in Polhemsalen, Ångströmlaboratoriet, Lägerhyddsvägen 1,

More information

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 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 information

PANDA Hardware - Status and Developments

PANDA Hardware - Status and Developments PANDA Hardware - Status and Developments Introduction K. Peters, The Physics of PANDA PANDA at FAIR: Hardware EMC in detail H.-G. Zaunick Status and Recent Developments Kai-Thomas Brinkmann, BelINP Minsk,

More information

PANDA Experiment. Nordic Winter Meeting on FAIR Björkliden Department of Physics and Astronomy Uppsala University

PANDA Experiment. Nordic Winter Meeting on FAIR Björkliden Department of Physics and Astronomy Uppsala University Department of Physics and Astronomy Uppsala University Nordic Winter Meeting on Phyics @ FAIR Björkliden 1-3-6 1 3 pp Λ c Λ + c 4 5 pp ȲY What are the relevant degrees of freedom to describe a process?

More information

Studies of charmonium production in e + e - annihilation and B decays at BaBar

Studies of charmonium production in e + e - annihilation and B decays at BaBar Studies of charmonium production in e + e - annihilation and B decays at BaBar I. Garzia, INFN Sezione di Ferrara On behalf of the BaBar Collaboration XVI International Conference on Hadron Spectroscopy

More information

PANDA Muon System Prototype

PANDA Muon System Prototype PANDA Muon System Prototype Victor Abazov 1, Gennady Alexeev 1, Maxim Alexeev 2, Vladimir Frolov 1, Georgy Golovanov 1, Sergey Kutuzov 1, Alexei Piskun 1, Alexander Samartsev 1, Valeri Tokmenin 1, Alexander

More information

CLAS12 at Jefferson Lab

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

More information

and Charmonium Prospects at FAIR

and Charmonium Prospects at FAIR PANDA and Charmonium Prospects at FAIR Klaus Peters, GSI and Ruhr-University Bochum χ c2 (2 3 P 2 ) ψ(3 ψ(1 3 D 3 ) η 3 S 1 ) D*D* c (3 1 S 0 ) χ ψ(1 3 c1 (2 3 P 1 ) h D 2 ) 1c (2 1 P 1 ) χ DD* ψ(1 1 c0

More information

Charm with ZEUS HERA-II data

Charm with ZEUS HERA-II data Charm with ZEUS HERA-II data Falk Karstens on behalf of the ZEUS collaboration University of Freiburg/ Germany Outline: DIS 26 21th April 26 HF-2 D ± mesons in deep inelastic

More information

Reconstruction of. events in LHCb. Benjamin Carron

Reconstruction 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 information

Particle identification at LHC: Alice and LHCb

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

More information

High resolution spectroscopy of hypernuclei with γ-ray detectors

High resolution spectroscopy of hypernuclei with γ-ray detectors High resolution spectroscopy of hypernuclei with γ-ray detectors multi- hypernuclei H-particle Alessandro Feliciello I.N.F.N. - Sezione di Torino Contents 2 Discovery potential of the strangeness nuclear

More information

Status / Hadron Spectroscopy at COMPASS

Status / Hadron Spectroscopy at COMPASS Status / Hadron Spectroscopy at COMPASS Johannes Bernhard 1 Institut für Kernphysik Mainz January 22 nd 2010 1 johannes.bernhard@cern.ch Outline 1 Introduction 2 Recoil Proton Detector 3 Trigger 4 Analysis

More information

LHCb: From the detector to the first physics results

LHCb: 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 information

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 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

More information

ISOSPIN RESOLVED DOUBLE PION PRODUCTION AT CELSIUS

ISOSPIN RESOLVED DOUBLE PION PRODUCTION AT CELSIUS Vol. 29 (1998) ACTA PHYSICA POLONICA B No 11 ISOSPIN RESOLVED DOUBLE PION PRODUCTION AT CELSIUS M. Andersson a, Chr. Bargholtz a, E. Fumero a, K. Fransson a L. Holmberg a, K. Lindh a, L. Mårtensson a,

More information

Scintillators for photon detection at at medium energies

Scintillators for photon detection at at medium energies Scintillators for photon detection at at medium energies R.Novotny II.Physics II.Physics Institute, Institute, University University Giessen, Giessen, Germany Germany and and for for the the TAPS TAPS

More information

The PANDA Experiment at FAIR

The PANDA Experiment at FAIR The PANDA Experiment at FAIR Diego Bettoni INFN, Ferrara, Italy Hadrons from Quarks and Gluons Hirschegg, Kleinwalsertal, Austria, January 12-18, 2014 Outline Introduction The FAIR facility Experimental

More information

Design of the Central Tracker of the PANDA experiment

Design of the Central Tracker of the PANDA experiment Scientifica Acta 4, No. 1, Ph 3-8 (21) Design of the Central Tracker of the PANDA experiment S. Costanza 1 1 Istituto Nazionale di Fisica Nucleare, Sezione di Pavia, via Bassi 6, 271 Pavia, Italy susanna.costanza@pv.infn.it

More information

Muon reconstruction performance in ATLAS at Run-2

Muon 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 information

On a Hydrogen Pellet Target for Antiproton Physics with PANDA

On a Hydrogen Pellet Target for Antiproton Physics with PANDA Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 219 On a Hydrogen Pellet Target for Antiproton Physics with PANDA ÖRJAN NORDHAGE ACTA UNIVERSITATIS UPSALIENSIS

More information

Cherenkov light imaging in particle and nuclear physics experiments

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

More information

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) 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 information

Identification of Central Production in the π + π π + π Channel at COMPASS

Identification of Central Production in the π + π π + π Channel at COMPASS Identification of Central Production in the π + π π + π Channel at COMPASS ASI-Spin-Praha-009 Johannes Bernhard for the COMPASS collaboration Institut für Kernphysik Mainz July 8 th Outline 1 Introduction

More information

Particle Identification with Disc DIRC at PANDA

Particle Identification with Disc DIRC at PANDA Particle Identification with Disc DIRC at PANDA Mustafa Schmidt, Simon Bodenschatz, Michael Düren, Erik Etzelmüller, Klaus Föhl, Avetik Hayrapetyan, Julian Rieke TIPP 217 May 23, 217 Mustafa Schmidt Particle

More information

Benjamin Carron Mai 3rd, 2004

Benjamin 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 information

Tracking at the LHC. Pippa Wells, CERN

Tracking 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 information

The ALICE Experiment Introduction to relativistic heavy ion collisions

The ALICE Experiment Introduction to relativistic heavy ion collisions The ALICE Experiment Introduction to relativistic heavy ion collisions 13.06.2012 Introduction to relativistic heay ion collisions Anna Eichhorn 1 Facts about ALICE ALICE A Large Ion Collider Experiment

More information

LABORATORI NAZIONALI DI FRASCATI SIS-Pubblicazioni

LABORATORI NAZIONALI DI FRASCATI SIS-Pubblicazioni LABORATORI NAZIONALI DI FRASCATI SIS-Pubblicazioni LNF-06/22 (P) 29 August 2006 HADRON PROPERTIES IN THE NUCLEAR MEDIUM THE PANDA PROGRAM WITH pa REACTIONS Olaf N. Hartmann INFN, Laboratori Nazionali di

More information

Exploring dense matter at FAIR: The CBM Experiment

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

More information

arxiv: v1 [hep-ex] 30 Oct 2007

arxiv: v1 [hep-ex] 30 Oct 2007 Proceedings of the CHARM 2007 Workshop, Ithaca, NY, August 5-8, 2007 1 The PANDA Experiment at FAIR Diego Bettoni Istituto Nazionale di Fisica Nucleare, 44100 Ferrara, Italy The physics program of the

More information

Light Meson Decays at BESIII

Light Meson Decays at BESIII Light Meson Decays at BESIII Liqing QIN (for the Collaboration ) Shandong University XVI International Conference on Hadron Spectroscopy Sep. 13-18, 2015, Newport News, VA OUTLINE n Introduction n Recent

More information

Simulation of J/ψ detection via electron-positron decay

Simulation of J/ψ detection via electron-positron decay 1 Simulation of J/ψ detection via electron-positron decay Goran Kružić Faculty of Science, University of Zagreb, Croatia 6 th Austrian Croatian Hungarian meeting Summer workshop for theoretical physics

More information

Impact of the Belle II Pixel Detector on CP-Violation Measurements

Impact of the Belle II Pixel Detector on CP-Violation Measurements Impact of the Belle II Pixel Detector on CP-Violation Measurements Fernando Abudinén September 6, 216 1 SuperKEKB and Belle II 2 CP-Violation Measurements 3 Belle II Pixel Vertex Detector 4 B-Meson Vertex

More information

B 0 s physics at LHCb

B 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 information

Measurement of the baryon number transport with LHCb

Measurement 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 information

Detectors & Beams. Giuliano Franchetti and Alberica Toia Goethe University Frankfurt GSI Helmholtzzentrum für Schwerionenforschung

Detectors & Beams. Giuliano Franchetti and Alberica Toia Goethe University Frankfurt GSI Helmholtzzentrum für Schwerionenforschung Detectors & Beams Giuliano Franchetti and Alberica Toia Goethe University Frankfurt GSI Helmholtzzentrum für Schwerionenforschung Pro-seminar Winter Semester 2015-16 DPG Spring Meeting Giuliano Franchetti

More information

Photon and neutral meson production in pp and PbPb collisions at ALICE

Photon and neutral meson production in pp and PbPb collisions at ALICE Photon and neutral meson production in pp and PbPb collisions at ALICE Dieter Roehrich University of Bergen, Norway for the ALICE Collaboration Nuclear collisions at the LHC Photons as a probe for the

More information

Testing the m-e universality with ±

Testing the m-e universality with ± Testing the m-e universality with ± ± K l n decays Venelin Kozhuharov University of Sofia St. Kl. Ohridski / JINR Dubna Neutrino Oscilation Workshop 2006 on behalf of the NA48/2 collaboration Cambridge,

More information

Physics with Hadron Beams at COMPASS

Physics with Hadron Beams at COMPASS Physics with Hadron Beams at COMPASS Bernhard Ketzer Technische Universität München MAMI and Beyond 2009 International Workshop on Hadron Structure and Spectroscopy 2009 30 March 2009 The Goal Understand

More information

High-intensity anti-proton beam on internal pellet/cluster target.

High-intensity anti-proton beam on internal pellet/cluster target. THE DIRC DETECTORS FOR THE PANDA EXPERIMENT AT FAIR J h Schwiening Jochen S h i i for the PANDA Cherenkov Group PANDA Experiment DIRC Concept Barrel & Disk DIRC Design g Prototypes and R&D PANDA EXPERIMENT

More information

RICH detectors for LHCb

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

More information

Measurements of the Masses, Mixing, and Lifetimes, of B Hadrons at the Tevatron

Measurements of the Masses, Mixing, and Lifetimes, of B Hadrons at the Tevatron Measurements of the Masses, Mixing, and Lifetimes, of B Hadrons at the Tevatron Mike Strauss The University of Oklahoma The Oklahoma Center for High Energy Physics for the CDF and DØ Collaborations Outline

More information

Results from BABAR/PEP-II - One Year of Operations

Results from BABAR/PEP-II - One Year of Operations SLAC-PUB-9158 March 22 Results from /PEP-II - One Year of Operations Paul C. Bloom Representing the Collaboration Presented at the 4th International Conference on Hyperons, Charm and Beauty Hadrons, 6/27/2

More information

The BES-III experiment

The BES-III experiment The BES-III experiment Igor Denysenko for the BES-III collaboration JINR Dubna on leave from BITP, Kiev Hadron Structure and QCD July 4-8, 2012, Gatchina, Russia BEPCII/BESIII at IHEP(Beijing) 2004: start

More information

CLEO Results From Υ Decays

CLEO Results From Υ Decays CLEO Results From Υ Decays V. Credé 1 2 1 Cornell University, Ithaca, NY 2 now at Florida State University Tallahassee, FL Hadron 05 Outline 1 Introduction The Υ System CLEO III Detector CLEO III Υ Data

More information