COMMISSIONING AND FIRST RESULTS OF THE NA62 RICH

Size: px
Start display at page:

Download "COMMISSIONING AND FIRST RESULTS OF THE NA62 RICH"

Transcription

1 Siena th Topical Seminar on Innova4ve Par4cle and Radia4on Detectors (IPRD16) 3-6 October 2016 Siena, Italy COMMISSIONING AND FIRST RESULTS OF THE NA62 RICH M. LENTI INFN Sezione di Firenze On behalf of the NA62 RICH WG

2 Outlook The NA62 experiment The RICH Detector ConstrucJon and Commissioning Time ResoluJon Pion-Muon separajon Conclusions 3/10/16 M. LenJ 2

3 The NA62 Experiment NA48 ( ): K L /K S beams èdirect CPV Measurement NA48/1 (2002): K S beam è K S rare decays NA48/2 (2003-4): K + /K - beams è K ± precise measurement NA62 (2007-8): K + /K - beams èlepton Universality K e2 /K µ2 NA62 (2014-8): K + beam èbr(k + π + νν), new physics, rare decays, etc NA62: 200 parjcipants, 30 InsJtutes 3/10/16 M. LenJ 3

4 The NA62 Goal FCNC loop process Very clean theorejcally SM predicjon BR( K + π + νν ) = ( 8.4 ±1.0) Experiments BR K + π + νν K + π + νν ( ) = NA62: 100 events, 10% error [ ] ( ) BNL E949 ( ) 3/10/16 M. LenJ 4

5 1 m Detectors for Secondary Beam Kaon ID (KTAG) Beam Tracker Beam guard ring (CHANTI) The NA62 Setup CHANTI Large Angle E.M. Calorimeters Hadron Calorimeters Forward E.M. Calorimeter (LKR) Momentum selecjon and collimajon KTAG Beam tracker RICH Straw Spectrometer Small Angle E.M. Calorimeters SPS protons 400 GeV p/s 3.5 s spill Secondary Beam 75 GeV, Δp/p 1% X,Y Divergence < 100 µrad K(6%),π(70%),p(23%) Total rate: 750 MHz Beam size: cm 2 Kaon Decay 5 MHz /year 60 m length 10-6 mbar vacuum Detectors for Decay Products Charged ParJcle Tracking Charged ParJcle Time stamping Photon DetecJon ParJcle ID 3/10/16 M. LenJ 5

6 The RICH Detector PMTs Mirror Mosaic (17m focal length) Beam Vessel: 17 m long, filled with Neon µ contaminajon < 1% in π sample in 15<p<35 GeV/c Time resolujon < 100 ps L0 trigger for a charged track 3/10/16 M. LenJ 6

7 The RICH Detector (since 2014) 3/10/16 M. LenJ 7

8 The Cherenkov Radiator Neon gas slightly above atmospheric pressure (n-1)= at λ = 300 nm P threshold = 12.5 GeV/c for π good light transparency Low chromajc dispersion Fresh Neon injected aler RICH container evacuated: no purificajon/recirculajon system 3/10/16 M. LenJ 8

9 The Gas Container ( Vessel ) Vacuum proof tank 17 m long in construcjon steel 4 cylindrical secjon of decreasing diameter and different lengths Beam pipe (Ø 168 mm) going through Thin Al entrance and exit windows View from inside, looking upstream towards the PMTs 3/10/16 M. LenJ 9

10 The Mirror System Mosaic of 20 spherical mirrors (18 hexagonal, 2 semi-hex close to the beam pipe) to focus Cherenkov light to the PMTs plane 2.5 cm thick glass coated with Al with dielectric film 35 cm side length Radius of curvature: (34.0±0.2) m Average reflecjvity 90% ( nm) D 0 < 4 mm (opjcal quality parameter) 3/10/16 M. LenJ 10

11 Mirrors Support and Alignment Al honeycomb support structure Each Mirror supported by a dowel inserted in the back Two thin Al ribbons keep the mirror in equilibrium and allow its orientajon A third verjcal ribbon avoid rotajon Piezo motors allow remotely controlled orientajon 3/10/16 M. LenJ 11

12 Mirrors Alignment Preliminary Laser alignment before closing the vessel Final alignment using charged tracks during data taking (reconstructed by the spectrometer) Compare the posijon of the ring center on the PMTs plane with posijon predicted by track extrapolajon Select rings fully contained in a single mirror (Y ring -Y ref )(mm) Jura (Y ring -Y ref )(mm) Saleve All mirrors Aligned within 1 mm ( 30 µrad) With respect to The reference Each cross is one mirror (X ring -X ref )(mm) (X ring -X ref )(mm) 3/10/16 M. LenJ 12

13 The PhotoMulJpliers Cherenkov light reflected by the mirrors is collected by 1952 PMTs located in two spots Compact hexagonal packing 18 mm pixel size Hamamatsu R7400-U03 UV glass window, 16 mm Ø (8 mm acjve Ø) Custom made HV divider SensiJve range nm (420 nm peak) Gain at 900 V Q.E. 20% at peak 280 ps Jme jiuer (FWHM) Winston cones with Al mylar to opjmize light collecjon Quartz window separate Neon from air TDAQ system bastem on custom made FE boards and TEL62 3/10/16 M. LenJ 13

14 Front-End and Read-Out RICH front-end 64 Custom-made boards 8-ch NINO chip discriminators 32-ch boards (3 NINO each) RICH read-out 128-ch TDC daughter boards (TDCB) each with 4 CERN HPTDC 5 TEL62 mother boards (4 for the 1952 PMTs, 1 for the muljplicity read-out used for L0 trigger) each with 4 TDCBs 3/10/16 M. LenJ 14

15 Time ResoluJon The RICH event Jme resolujon is 70 ps Detected photons (hits) of one Cherenkov ring split in two sets Time difference of Jme average of each set is ploued Time resolujon is ½ σ Cherenkov ring average Jme compared with KTAG Jme 3/10/16 M. LenJ 15

16 RICH ParJcle ID Charged pions, muons and electrons selected with calorimetric and spectrometer info <N hits > Number of hits per Cherenkov ring vs p e + µ + Radius (mm) Cherenkov ring Radius vs p π + p(gev/c) Kaons from scauered beam p(gev/c) 3/10/16 M. LenJ 16

17 π-µ separajon For 86% π ID efficiency a 1.3% µ mis-id efficiency is observed Squared parjcle mass reconstructed using velocity (from RICH ring Radius) and momentum (from spectrometer) Pion idenjficajon efficiency vs Muon mis-idenjficajon Efficiency for π ID m 2 (GeV 2 /c 4 ) Efficiency for µ mis-id 3/10/16 M. LenJ 17

18 2016 Preliminary Results For 90% π ID efficiency a 0.8% µ mis-id efficiency is observed Efficiency for π ID 2016 Preliminary Results Beuer mirror alignment in 2016 w.r.t Efficiency for µ mis-id 3/10/16 M. LenJ 18

19 Conclusions NA62 RICH detector installed in 2014 Pilot Run in fall 2014 Commissioning run in 2015 Detector upgrade in the winter shutdown Physics Run in 2016 RICH performances fufilling expectajon NA62 running unjl (at least) end of /10/16 M. LenJ 19

20 NA62 3/10/16 M. LenJ 20

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

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 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 information

The NA62 RICH detector

The NA62 RICH detector Available online at www.sciencedirect.com Physics Procedia 37 (2012 ) 634 641 TIPP 2011 - Technology and Instrumentation for Particle Physics 2011 The NA62 RICH detector Monica Pepe a, * a INFN Sezione

More information

Progress of the NA62 RICH detector

Progress of the NA62 RICH detector Home Search Collections Journals About Contact us My IOPscience Progress of the NA62 RICH detector This content has been downloaded from IOPscience. Please scroll down to see the full text. (http://iopscience.iop.org/1748-0221/9/01/c01054)

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

New Limits on Heavy Neutrino from NA62

New Limits on Heavy Neutrino from NA62 New Limits on Heavy Neutrino from NA62 Michal Koval (CERN) michal.koval@cern.ch on behalf of the NA62 collaboration EPS HEP 2017 Venice, Italy, 5 12 July 2017 Kaon Decay Experiments at CERN Earlier: NA31

More information

NA62: Ultra-Rare Kaon Decays

NA62: 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 information

THE CERN NA62 experiment [1] aims to measure the

THE CERN NA62 experiment [1] aims to measure the 1 Studies of the Effects of Oxygen and CO 2 Contamination of the Neon Gas Radiator on the Performance of the NA62 RICH Detector Evelina Gersabeck on behalf of the NA62 RICH Working Group arxiv:1111.3332v1

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

Κ+ p+νν : first NA62 results

Κ+ p+νν : first NA62 results Κ+ p+νν : first NA62 results Speaker: Radoslav Marchevski On behalf of the NA62 collaboration Moriond EW Conference, 10 17th March 2018, La Thuile, Italy, Kaon physics @ NA62 `14-`18 NA62:Κ+ π+νν 2014

More information

R. Fantechi CERN and INFN Sezione di Pisa on behalf of the NA62 Collaboration

R. Fantechi CERN and INFN Sezione di Pisa on behalf of the NA62 Collaboration Search for K + π + _ νν at NA62 R. Fantechi CERN and INFN Sezione di Pisa on behalf of the NA62 Collaboration Birmingham, Bratislava, Bristol, Bucharest, CERN, Dubna (JINR), Fairfax, Ferrara, Florence,

More information

New Limits on Heavy Neutrino from NA62

New 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 information

Jacopo Pinzino CERN HQL /05/2018

Jacopo Pinzino CERN HQL /05/2018 Search for K + π + ν ν at NA62 Jacopo Pinzino CERN HQL2018 30/05/2018 The NA62 Experiment NA62: High precision fixed-target Kaon experiment at CERN SPS Main goal: measurement of BR(K + π + υ υ) Broader

More information

The HERA-B ring imaging Cherenkov system } design and performance

The HERA-B ring imaging Cherenkov system } design and performance Nuclear Instruments and Methods in Physics Research A 446 (2000) 299}304 The HERA-B ring imaging Cherenkov system } design and performance JoK rg Pyrlik For the HERA-B RICH Collaboration University of

More information

The CNGS neutrino beam

The CNGS neutrino beam 10th Topical Seminar on Innovative Particle and Radiation Detectors (IPRD06) 1-5 October 2006 Siena, Italy ν The CNGS neutrino beam G. Sirri INFN Bologna CNGS (CERN Neutrinos to Gran Sasso) The project

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

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 NA62 Experiment. Seminar at LPNHE, Paris, France. Mathieu PERRIN-TERRIN. February 4, CERN, Geneva, Switzerland.

The NA62 Experiment. Seminar at LPNHE, Paris, France. Mathieu PERRIN-TERRIN. February 4, CERN, Geneva, Switzerland. The NA62 Experiment Seminar at LPNHE, Paris, France Mathieu PERRIN-TERRIN CERN, Geneva, Switzerland. February 4, 2016 Outline 1 Physics Case (10min) 2 The NA62 Experiment (25min) 3 Outlook of the First

More information

New limits on Heavy Neutral Lepton from Kaon CERN

New limits on Heavy Neutral Lepton from Kaon CERN New limits on Heavy Neutral Lepton from Kaon experiments @ CERN Monica Pepe INFN Perugia On behalf of the NA62 and NA48/2 Collaborations International Workshop on Baryon & Lepton Number Violation 2017

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

π 0 Dalitz Transition Form Factor and other news from NA62 Nicolas Lurkin University of Birmingham, 26/04/2017

π 0 Dalitz Transition Form Factor and other news from NA62 Nicolas Lurkin University of Birmingham, 26/04/2017 π 0 Dalitz Transition Form Factor and other news from NA62 Nicolas Lurkin University of Birmingham, 26/04/2017 Outline π 0 transition form factor slope from the π 0 Dalitz decay at NA62 2007 The K + π

More information

The LHCb Experiment II Detector XXXIV SLAC Summer Institute, July, 2006

The 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

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

Calorimetry in particle physics experiments

Calorimetry in particle physics experiments Calorimetry in particle physics experiments Unit N. 9 The NA48 ECAL example (LKR) Roberta Arcidiacono R. Arcidiacono Calorimetry 1 Lecture overview The requirements Detector layout & construction Readout

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

Cherenkov Detector Simulation

Cherenkov Detector Simulation Outline E.Chudakov JLab Cherenkov Detector 1 Cherenkov Detector Simulation E.Chudakov 1 1 JLab For GLUEX Collaboration Meeting, March 2007 http://www.jlab.org/~gen/gluex/gas_cher_geom.html Outline E.Chudakov

More information

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 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 information

AIRFLY: Measurement of the Air Fluorescence induced by electrons

AIRFLY: Measurement of the Air Fluorescence induced by electrons AIRFLY: Measurement of the Air Fluorescence induced by electrons Valerio Verzi INFN Sezione di Roma II For the Airfly collaboration 9 th Topical Seminar on Innovative Particle and Radiation Detectors 23-26

More information

NA62 & Kaon Experiments

NA62 & Kaon Experiments NA62 & Kaon Experiments Outline: Evgueni Goudzovski (University of Birmingham) eg@hep.ph.bham.ac.uk 1) Ultra-rare K πνν decays: theory vs experiment. 2) NA62 and other K πνν experiments. 3) UK responsibilities

More information

2017 NA62 Status Report to the CERN SPSC

2017 NA62 Status Report to the CERN SPSC 17 NA6 Status Report to the CERN SPSC Abstract The status of the analysis of the data collected in 16 by the NA6 experiment is reported. About 5 11 K + decays have been taken to study the K + π + ν ν decay.

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

Dual readout with tiles for calorimetry.

Dual readout with tiles for calorimetry. Dual readout with tiles for calorimetry. F.Lacava on behalf of the RD52 / DREAM Collaboration Cagliari Cosenza Iowa State Pavia Pisa Roma 1 Texas Tech. 13th Topical Seminar on Innovative Particle and Radiation

More information

Module of Silicon Photomultipliers as a single photon detector of Cherenkov photons

Module of Silicon Photomultipliers as a single photon detector of Cherenkov photons Module of Silicon Photomultipliers as a single photon detector of Cherenkov photons R. Pestotnik a, H. Chagani a, R. Dolenec a, S. Korpar a,b, P. Križan a,c, A. Stanovnik a,c a J. Stefan Institute, b University

More information

The Factors That Limit Time Resolution for Photon Detection in Large Cherenkov Detectors

The Factors That Limit Time Resolution for Photon Detection in Large Cherenkov Detectors The Factors That Limit Time Resolution for Photon Detection in Large Cherenkov Detectors Kate Scholberg, Duke University Chicago, April 2011 OUTLINE - Overview/physics motivation - Event reconstruction

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

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

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

Guest Lecture PHY 7361: Harnessing Cherenkov Radiation SteveSekula, 13 April 2010 (created 9 April 2010)

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

More information

PoS(KAON)059. Giuseppe Ruggiero. Scuola Normale Superiore and INFN, Pisa, Italy

PoS(KAON)059. Giuseppe Ruggiero. Scuola Normale Superiore and INFN, Pisa, Italy The π ν ν experiment at CERN Scuola Normale Superiore and INFN, Pisa, Italy E-mail: giuseppe.ruggiero@cern.ch The P326 proposal for an experiment to measure the branching ratio of the very rare kaon decay

More information

HARP a hadron production experiment. Emilio Radicioni, INFN for the HARP collaboration

HARP a hadron production experiment. Emilio Radicioni, INFN for the HARP collaboration HARP a hadron production experiment Emilio Radicioni, INFN for the HARP collaboration HARP motivations provide data for neutrino factory / muon collider design. reduce the uncertainties in the atmospheric

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

PoS(KAON)049. Testing the µ e universality with K ± l ± ν decays

PoS(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 information

NA62 status and prospects

NA62 status and prospects NA62 status and prospects Outline: Evgueni Goudzovski (University of Birmingham, eg@hep.ph.bham.ac.uk) on behalf of the NA62UK collaboration 1) Physics at kaon experiments: K decays and beyond 2) NA62

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 Jožef Stefan Institute, Ljubljana, Slovenia; currently CERN, Geneva, Switzerland November 30 December 5, 2004 for BELLE Aerogel

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

Results 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 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 information

PoS(DIS 2010)058. ATLAS Forward Detectors. Andrew Brandt University of Texas, Arlington

PoS(DIS 2010)058. ATLAS Forward Detectors. Andrew Brandt University of Texas, Arlington University of Texas, Arlington E-mail: brandta@uta.edu A brief description of the ATLAS forward detectors is given. XVIII International Workshop on Deep-Inelastic Scattering and Related Subjects April

More information

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

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland. Commissioning of the CMS Detector Available on CMS information server CMS CR -2009/113 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 15 May 2009 Commissioning of the CMS

More information

EP228 Particle Physics

EP228 Particle Physics EP8 Particle Physics Topic 4 Particle Detectors Department of Engineering Physics University of Gaziantep Course web page www.gantep.edu.tr/~bingul/ep8 Oct 01 Page 1 Outline 1. Introduction. Bubble Chambers

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

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

Likelihood Methods for Beam Particle Identification at the COMPASS Experiment

Likelihood 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 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

Likelihood Methods for Beam Particle Identification at the COMPASS Experiment

Likelihood Methods for Beam Particle Identification at the COMPASS Experiment EPJ manuscript No. (will be inserted by the editor) Likelihood Methods for Beam Particle Identification at the COMPASS Experiment Tobias Weisrock 1,2,a on behalf of the COMPASS Collaboration 1 Johannes

More information

MINOS. Physics Program and Construction Status. Karol Lang The University of Texas at Austin. YITP: Neutrinos and Implications for Physics Beyond

MINOS. Physics Program and Construction Status. Karol Lang The University of Texas at Austin. YITP: Neutrinos and Implications for Physics Beyond MINOS Physics Program and Construction Status Karol Lang The University of Texas at Austin YITP: Neutrinos and Implications for Physics Beyond YITP Conference: Neutrinos and Implications The Standard for

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

LHCb Calorimetry Impact

LHCb 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 information

PoS(KAON09)023. Beam Hole Photon Veto For J-PARC K O TO experiment. Yosuke Maeda Kyoto University

PoS(KAON09)023. Beam Hole Photon Veto For J-PARC K O TO experiment. Yosuke Maeda Kyoto University Beam Hole Photon Veto For J-PARC K O TO experiment Kyoto University E-mail: maeda_y@scphys.kyoto-u.ac.jp The Beam Hole Photon Veto counter (BHPV) for the J-PARC K O TO experiment was designed by MC simulation.

More information

SciBar and future K2K physics. F.Sánchez Universitat Aútonoma de Barcelona Institut de Física d'altes Energies

SciBar and future K2K physics. F.Sánchez Universitat Aútonoma de Barcelona Institut de Física d'altes Energies SciBar and future K2K physics F.Sánchez Universitat Aútonoma de Barcelona Institut de Física d'altes Energies ICRR, 29 th October 2003 Outline Introduction: K2K SciBar detector: Physics goals Design Electron

More information

The HARP Experiment. G. Vidal-Sitjes (INFN-Ferrara) on behalf of the HARP Collaboration

The 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 information

Calorimetry in QGP studies at RHIC

Calorimetry in QGP studies at RHIC E.Kistenev Calorimetry in QGP studies at RHIC Siena, Italy, October 2008 Innovative Particle and Radiation Detectors 1 Collider facility at BNL : RHIC RHIC and Its Experiments RHIC relativistivic-heavy

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

Performance of New and Upgraded Detectors for Luminosity and Beam Condition Measurement at CMS

Performance of New and Upgraded Detectors for Luminosity and Beam Condition Measurement at CMS Performance of New and Upgraded Detectors for Luminosity and Beam Condition Measurement at CMS Jessica Leonard On behalf of CMS BRIL EPS 2015, Vienna July 24, 2015 1 CMS BRIL: Beam Radiation Instrumentation

More information

7. Particle identification

7. Particle identification 7. Particle identification in general, momentum of a particle measured in a spectrometer and another observable is used to identity the species velocity time-of-flight Cherenkov threshold transition radiation

More information

First neutrino beam and cosmic tracks. GDR neutrino

First neutrino beam and cosmic tracks. GDR neutrino Magali Besnier T2K status tt of the experiment First neutrino beam and cosmic tracks GDR neutrino 28 04 09 T2K Tokai 2 Kamiokande Main goals : 1) Measurement of 13 mixing angle studying the e oscillation

More information

Observation of the rare B 0 s µ + µ decay

Observation 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 information

A beam line for schools

A beam line for schools A beam line for schools Great things can happen when high schools get involved with cutting edge science, and that s exactly what CERN is proposing with its new beam line for schools competition, which

More information

The SHiP experiment. Colloquia: IFAE A. Paoloni( ) on behalf of the SHiP Collaboration. 1. Introduction

The SHiP experiment. Colloquia: IFAE A. Paoloni( ) on behalf of the SHiP Collaboration. 1. Introduction IL NUOVO CIMENTO 40 C (2017) 54 DOI 10.1393/ncc/i2017-17054-1 Colloquia: IFAE 2016 The SHiP experiment A. Paoloni( ) on behalf of the SHiP Collaboration INFN, Laboratori Nazionali di Frascati - Frascati

More information

A gas-filled calorimeter for high intensity beam environments

A gas-filled calorimeter for high intensity beam environments Available online at www.sciencedirect.com Physics Procedia 37 (212 ) 364 371 TIPP 211 - Technology and Instrumentation in Particle Physics 211 A gas-filled calorimeter for high intensity beam environments

More information

V0 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 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 information

PERFORMANCE OF THE ATLAS MUON TRIGGER IN RUN 2

PERFORMANCE OF THE ATLAS MUON TRIGGER IN RUN 2 PERFORMANCE OF THE ATLAS MUON TRIGGER IN RUN 2 M.M. Morgenstern On behalf of the ATLAS collaboration Nikhef, National institute for subatomic physics, Amsterdam, The Netherlands E-mail: a marcus.matthias.morgenstern@cern.ch

More information

The LHCf experiment at LHC

The LHCf experiment at LHC The LHCf experiment at LHC CALOR 2006 Chicago, 5-9 June 2006 University and INFN Firenze On behalf of the LHCf Collaboration The LHCf collaboration O. Adriani,, L. Bonechi, M. Bongi, P. Papini,, R. D AlessandroD

More information

PoS(TIPP2014)093. Performance study of the TOP counter with the 2 GeV/c positron beam at LEPS. K. Matsuoka, For the Belle II PID group

PoS(TIPP2014)093. Performance study of the TOP counter with the 2 GeV/c positron beam at LEPS. K. Matsuoka, For the Belle II PID group Performance study of the TOP counter with the 2 GeV/c positron beam at LEPS, For the Belle II PID group KMI, Nagoya University E-mail: matsuoka@hepl.phys.nagoya-u.ac.jp The TOP (Time-Of-Propagation) counter

More information

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

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,

More information

ALICE A Large Ion Collider Experiment

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

More information

THE AMS RICH COUNTER

THE AMS RICH COUNTER THE AMS RICH COUNTER G. BOUDOUL ISN Grenoble ISN-GRENOBLE 1 The AMS RICH collaboration: Bologna, Grenoble, Lisbon, Madrid, Maryland, Mexico 2 The AMS collaboration UNAM S.C.C. TING (MIT), PI 3 AMS Scientific

More information

PoS(KAON13)012. R K Measurement with NA62 at CERN SPS. Giuseppe Ruggiero. CERN

PoS(KAON13)012. R K Measurement with NA62 at CERN SPS. Giuseppe Ruggiero. CERN CERN E-mail: giuseppe.ruggiero@cern.ch A precision measurement of the ratio R K of the rates of kaon leptonic decays K e ν and K µ ν with the full minimum bias data sample collected with low intensity

More information

NA62 & Kaon Experiments

NA62 & Kaon Experiments NA62 & Kaon Experiments Outline: Evgueni Goudzovski (University of Birmingham) eg@hep.ph.bham.ac.uk 1) Ultra-rare K πνν decays: theory vs experiment. 2) NA62 experiment and NA62UK. 3) Planned K πνν measurements

More information

A RICH Photon Detector Module with G-APDs

A RICH Photon Detector Module with G-APDs A RICH Photon Detector Module with G-APDs S. Korpar a,b, H. Chagani b, R. Dolenec b, P. Križan b,c, R. Pestotnik b, A. Stanovnik b,c a University of Maribor, b J. Stefan Institute, c University of Ljubljana

More information

Precise Measurement of the Absolute Yield of Fluorescence Photons in Atmospheric Gases

Precise Measurement of the Absolute Yield of Fluorescence Photons in Atmospheric Gases Precise Measurement of the Absolute Yield of Fluorescence Photons in Atmospheric Gases Paolo Privitera 5th Fluorescence Workshop 7 th Air Fluorescence El Escorial Workshop - Madrid, Spain September 22-24,

More information

A 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 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 information

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Available on CMS information server CMS NOTE 1996/005 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Performance of the Silicon Detectors for the

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

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

K + Physics at J-PARC

K + Physics at J-PARC Takeshi K. Komatsubara (KEK-IPNS) 1 K + Physics at J-PARC K + Physics at J-PARC Takeshi K. Komatsubara (KEK-IPNS) 2005.May.26 K - RARE Meeting at INFN, Frascati Takeshi K. Komatsubara (KEK-IPNS) 2 K +

More information

B-Physics Potential of ATLAS, CMS, LHCb and BTeV

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

More information

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 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

More information

D 0 -D 0 mixing and CP violation at LHC

D 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 information

Expected Performance of the ATLAS Inner Tracker at the High-Luminosity LHC

Expected Performance of the ATLAS Inner Tracker at the High-Luminosity LHC Expected Performance of the ATLAS Inner Tracker at the High-Luminosity LHC Matthias Hamer on behalf of the ATLAS collaboration Introduction The ATLAS Phase II Inner Tracker Expected Tracking Performance

More information

The Fast Interaction Trigger Upgrade for ALICE

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

More information

(Towards) First Physics with LHCb

(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 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

on behalf of CAST Collaboration

on behalf of CAST Collaboration S. Cenk YILDIZ Dogus University/Istanbul on behalf of CAST Collaboration 13th Topical Seminar on Innovative Particle and Radiation Detectors (IPRD13) 7-10 October 2013 Siena, Italy Axions and CAST Experiment

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

FYST17 Lecture 6 LHC Physics II

FYST17 Lecture 6 LHC Physics II FYST17 Lecture 6 LHC Physics II 1 Today, (tomorrow) & Next week The LHC accelerator Challenges The experiments (mainly CMS and ATLAS) Important variables Preparations Soft physics minímum bias, underlying

More information

The LHCf experiment at LHC

The LHCf experiment at LHC The LHCf experiment at LHC Measurement of π 0 production cross section in the very forward region at LHC Equivalent laboratory energy 10 17 ev LHCf physics Description of the experiment Some results on

More information

PRELIMINARY RESULT ON DIRECT CP VIOLATION FROM NA DATA. DAPNIA-SPP / CEA-Saclay, Gif/Yvette cedex, France. Abstract

PRELIMINARY RESULT ON DIRECT CP VIOLATION FROM NA DATA. DAPNIA-SPP / CEA-Saclay, Gif/Yvette cedex, France. Abstract PRELIMINARY RESULT ON DIRECT CP VIOLATION FROM NA48 1998 DATA Raphael Granier de Cassagnac DAPNIA-SPP / CEA-Saclay, 91191 Gif/Yvette cedex, France on behalf of the NA48 collaboration 1 Abstract We present

More information

HARP (Hadron Production) Experiment at CERN

HARP (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 information

Design of the new ATLAS Inner Tracker for the High Luminosity LHC era

Design of the new ATLAS Inner Tracker for the High Luminosity LHC era Design of the new ATLAS Inner Tracker for the High Luminosity LHC era Trevor Vickey on behalf of the ATLAS Collaboration University of Sheffield, United Kingdom July 3, 2017 19th iworid Krakow, Poland

More information

Overview and Status of Measurements of F 3π at COMPASS

Overview and Status of Measurements of F 3π at COMPASS g-2 workshop Mainz: Overview and Status of Measurements of F 3π at COMPASS D. Steffen on behalf of the COMPASS collaboration 19.06.2018 sponsored by: 2 Dominik Steffen g-2 workshop Mainz 19.06.2018 Contents

More information