Status of RAON and LAMPS in Korea

Size: px
Start display at page:

Download "Status of RAON and LAMPS in Korea"

Transcription

1 7 th International Symposium on Nuclear Symmetry Energy (NuSYM2017) GANIL, Caen, France, September 4-7, 2017 Status of RAON and LAMPS in Korea Byungsik Hong (Korea University) September 4-7, 2017 GANIL 1

2 Location of RAON Complex RAON: Rare isotope Accelerator complex for ON-line experiments ~11 km Current RISP Office September 4-7, 2017 GANIL 2

3 Site Plan Bird s eye view Basic design was finished in Dec A construction company was selected in Sept September 4-7, 2017 GANIL 3

4 Site Preparation Construction and civil engineering for RAON has begun. The ground breaking for accelerators and experimental buildings was done on Feb. 13 th this year. Total area: 952,066 m 2 September 4-7, 2017 GANIL 4

5 Layout of RAON RISP 4.6 Neutron Science Facility Project period: Dec ~ Dec Scope: Accelerator Facility, Buildings & Utilities Budget: Total ~U$ 1.43 B Accelerator and Expt. Facility: ~U$ 0.46 B Building & Utility: ~U$ 0.97 B (including the land cost) Host: Ministry of Science, ICT and Future Planning (MSIP) RISP 4.3 High-precision Mass Measurement Facility RISP 4.4 Collinear Laser Spectroscopy High Energy Expt. Bldg. (B) RISP 4.7 Bio-medical Research Facility Low Energy Expt. Bldg. RISP 3.2 ISOL Facility RISP 4.1 Recoil Spectrometer (KOBRA) RISP 4.2 High Energy Expt. Bldg. (A) Large Acceptance Spectrometer RISP 3.3 IF Facility RISP 4.5 µ-sr September 4-7, 2017 GANIL 5

6 Layout of RAON Driver Linac Post Acc. Cyclotron Particle H + O +8 Xe +54 U +79 RI beam proton Energy (MeV/u) RISP 4.6 Neutron Science Facility Current (pμa) Power (kw) > RISP 4.3 High-precision Mass Measurement Facility RISP 4.4 Collinear Laser Spectroscopy High Energy Expt. Bldg. (B) RISP 4.7 Bio-medical Research Facility Low Energy Expt. Bldg. RISP 3.2 ISOL Facility RISP 4.1 Recoil Spectrometer (KOBRA) RISP 4.2 High Energy Expt. Bldg. (A) Large Acceptance Spectrometer RISP 3.3 IF Facility RISP 4.5 µ-sr September 4-7, 2017 GANIL 6

7 Expected RIBs at RAON 90 IFS: 238 U(200 Mev/u, 400 kw) + C 80 KOBRA: 40 Ar(30 MeV/u,12 kw) + Be Stable line Number of Proton (Z) ISOL: p(70 MeV, 70 kw)+uc x ISOL+IF: 140 Xe(222 MeV/u, 1E+07 pps)+ C KOBRA ISOL ZZ = NN Z=N <1 pps ISOL+IF Number of Neutron (N) September 4-7, 2017 GANIL 7 IFS IF KOBRA ISOL ISOL+IF 1.0E E E+11 1E E E E+10 1E E E E+09 1E E E E+08 1E E E E+07 1E E E E+06 1E E E E E E E+04 1E E E E+03 1E E E E+02 1E E E E+01 1E E E E+00 1E-10 RAON aims to provide an access to unexplored regions of nuclear chart.

8 Accelerator Systems SCL2(SSR1) SCL2(SSR2) Injector SCL1(QWR) SCL1(HWR) Bending Section Cyclotron IF System September 4-7, 2017 GANIL 8

9 Prototypes of Accelerator Components 28 GHz ECR Ion Source RFQ HTS Q-magnet QWR SC Cavity & its Cryomodule HWR SC Cavity & its Cryomodule SSR SC Cavity and its Cryomodule September 4-7, 2017 GANIL 9

10 Experimental Systems Neutron Facility HPMMS CLS Bio-medical facility Ultra-low Expt. Bldg. High Energy Expt. Bldg. (B) Low Energy Expt. Bldg. µsr KOBRA LAMPS High Energy Expt. Bldg. (A) September 4-7, 2017 GANIL 10

11 Prototypes of Experimental Systems LASER for collinear laser spectroscopy β-detection system for µsr Gamma array Time Projection Chamber ISOL beam diagnostics Beam-tracking detector (PPAC) ISOL target September 4-7, 2017 GANIL 11

12 Major Milestones System Prototype development Accelerator and Experimental System Installation and Commissioning Basic Design ECR Beam ISOL SI Beam ( 15.12) Site Building Civil Construction Tendering Process Detail Design SCL Demo Beam ( 17.12) Utility Supply ( 18.9) DAY-1 Expt. ( 20.7) ISOL RI Beam ( 20.12) IF RI Beam ( 21.12) Milestones in 2017 Cryomodule test for QWR and HWR Mass production Beam extraction from SCL demo (1 QWR) Cavity test for SSR Cryomodule test in early 2018 Construction / Facility Inspection/ Safety Management Radiation Safety Approved by KINS September 4-7, 2017 GANIL 12

13 LAMPS: Large-Acceptnce MultiPurpose Spectrometer September 4-7, 2017 GANIL 13

14 Location of LAMPS ECR (RAON) SCL1 SCL2 ISOL SCL3 ECR Si-CsI Neutron array September 4-7, 2017 GANIL 14

15 Location of LAMPS ECR (RAON) Ion beams to IF target via SCL1+SCL2 SCL1 SCL2 RIB to IF target via ISOL+SCL3+SCL2 ISOL SCL3 ECR September 4-7, 2017 GANIL 15

16 Time Projection Chamber η=-0.7 (127 o ) η=1.6 (24 o ) 400 mm Target 150 mm 500 mm 300 mm 900 mm One central Au+Au event at 250 AMeV (IQMD) September 4-7, 2017 GANIL 16

17 Prototype TPC: Design Half-dimension prototype TPC Outer field cage Triple GEM Cathode PAD 150 mm Inner field cage 490 mm September 4-7, 2017 Bottom Al 진도관리 frame NuSYM2017 중간평가 for (LAMPS) GANIL & GEM 17 17

18 Prototype TPC: Components [Readout Pads] Tested pads with the two different dimensions 3 10 mm 2 : 357 Ch./Oct mm 2 : 175 Ch./Oct. Multi-layer PCB board [GEM Foil] Trapezoidal shape Thickness: 75 µm Area: mm 2 Triple layers for each plane [Field Cage] 35 µm thick and 2 mm wide Cu strips 500 µm gap between adjacent strips Mirror strips on the back 1 MΩ resistors with 0.1% var. TPC body: G10 + Aramid honeycomb September 4-7, 2017 GANIL 18

19 Prototype TPC: Assembly Inner Field Cage installed Outer Field Cage installed Prototype TPC assembled Prototype TPC: back September 4-7, 2017 GANIL 19

20 Prototype TPC: Test at ELPH ELPH: Research Center for Electron Photon Science at Tohoku University, Japan Dates: November 1-2, 2016 Beams: ee + beams at 500 MeV Gas: Ar(90%)+CH 4 (10%) (P10) Ar(90%)+CO 2 (10%) (ArCO 2 ) Purpose: To study the detailed characteristics, such as vv dddddddddd, diffusion and σσ xx, of LAMPS TPC September 4-7, 2017 GANIL 20

21 Prototype TPC: Event Displays September 4-7, 2017 GANIL 21

22 Prototype TPC: Drift Velocity Preliminary vv dddddddddd 5.3 cm/μμs for P10: Maximum distance: 512 timing bins 0.04 μμs bin 5 cm μμs 100 cm Tested P20 with cosmic muons: vv dddddddddd > 6 cm/μμs that will be suitable for LAMPS TPC if read out from only one endcap side. September 4-7, 2017 GANIL 22

23 Prototype TPC: Diffusion Preliminary 2 σσ tttttttttt = DD 2 2 zz + σσ 0 where zz: drift length σσ tttttttttt : width of hit distributions w.r.t. the fitted track DD: diffusion coefficient σσ 0 : coefficient depending on the amplification system September 4-7, 2017 GANIL 23

24 Prototype TPC: Position Resolution P10 σσ = mmmm Preliminary P10 σσ = mmmm September 4-7, 2017 GANIL 24

25 Neutron Detector Array veto Dimensions of each scintillation bar: cm 3 Construction of the real-size prototype detectors and test of their performances using Radiation-source test: 60 Co and 252 Cf Neutron-beam test at RCNP, Japan September 4-7, 2017 GANIL 25

26 NDA: Results from Source Test γ n 252 Cf Watt spectrum: dddd dddd ee aaaa sinh aa=0.88 MeV -1 and bb=2.0 MeV -1 B. Watt, Physical Review 87, 1037 (1952) September 4-7, 2017 GANIL 26 bbbb

27 NDA: Beam Test at RCNP E479 approved in B-PAC in March 2016 Date: May 29, 2016 (Visited RCNP for May 22 June 2) Beam specifications Protons on Li production target (p+ 7 Li n + 7 Be) Neutron energies: 65 and 392 MeV in N0 beamline 10 na flux 1/9 chopping Background neutron above 3MeV is less than1% [NIMA629, 43 (2011)] Chopping signals Neutron flux: n sr μμc 2 stations with 2 1 veto layer September 4-7, 2017 GANIL 27

28 NDA: RCNP-E479 D2 D1 D6 D5 D4 D3 Distance from target to the detector: 15 m Gap between stations: 60 cm Dim. of each S1 detector: cm 3 Dim. of each S2 detector: cm 3 Beam size at S1: cm 2 September 4-7, 2017 GANIL 28

29 NDA: Energy Resolution for Neutrons Preliminary 392 MeV Time resolution: Δtt = Δττ 2 + Δxx vv 2 = 0.66 ns where Δττ = FWHM of γγ peak = 0.60 ns Δxx = effective thickness of the detector = (Total thinness of Li target, veto, and neutron detector)/2 = 6.0 cm vv = neutron velocity = 21.3 cm/ns Neutron energy resolution: ΔEE Δtt = γγ γγ + 1 = 3.2% EE tt where Lorentz γγ = 1 + EE mmcc 2 = 1.42 tt = 70.4 ns Energy resolution (FWHM/EE)= 3.3 % September 4-7, 2017 GANIL 29

30 NDA: Position Resolution for Neutrons & Cosmics Preliminary 392 MeV Hit position difference between DDD For neutron and DD2 for neutrons: beams Δxx SSS xx DDD xx DDD for 10 MeV threshold and δδtt < 3 ns Relative position resolution for neutrons for one bar: Δxx SSS (m) σσ nn = σσ Δxx SSS 2 = 3.1 cm For cosmic muons Δxx SSS (m) Position difference between the projected hit position and the hit position for DD3 for cosmic muons: Δxx SSS xx DD3,pppppppp xx DD3,hiiii Relative position resolution for cosmic muons for one bar: σσ μμ = σσ Δxx SSS 1.87 = 3.1 cm September 4-7, 2017 GANIL 30

31 Summary Rare Isotope Science Project (RISP) at IBS, Korea is moving forward. The construction and civil engineering for RAON has begun: The ground breaking for accelerators and experimental buildings was done on Feb. 13 th this year. LAMPS is a dedicated spectrometer for nuclear symmetry energy at RAON. Performance tests of the prototype TPC and the neutron-detector-array modules with accelerator beams were done, and we are analyzing the data. September 4-7, 2017 GANIL 31

Introduction to RAON & Detector Systems for Nuclear Physics

Introduction to RAON & Detector Systems for Nuclear Physics 3 rd Japan-Korea PHENIX Collaboration Meeting RIKEN, Japan, 27-28 November 2014 Introduction to RAON & Detector Systems for Nuclear Physics Byungsik Hong (Korea University) Outline - Plan for RAON and

More information

Progress of RAON Heavy Ion Accelerator Project in Korea

Progress of RAON Heavy Ion Accelerator Project in Korea Progress of RAON Heavy Ion Accelerator Project in Korea Sunchan Jeong Rare Isotope Science Project (RISP) 중이온가속기 사업단 Institute for Basic Science (IBS) May 13, 2016 IPAC2016 Contents Rare Isotope Science

More information

Future Opportunity of Nuclear Symmetry Energy at LAMPS/RAON

Future Opportunity of Nuclear Symmetry Energy at LAMPS/RAON 9 th APCTP-BLTP JINR Joint Workshop at Kazakhstan Modern Problems of Nuclear and Elementary Particle Physics Almaty, Kazakhstan, 27 June-4 July, 2015 Future Opportunity of Nuclear Symmetry Energy at LAMPS/RAON

More information

Plan for the Nuclear Symmetry Energy Measurements at RAON, LAMPS Facility

Plan for the Nuclear Symmetry Energy Measurements at RAON, LAMPS Facility 3 rd International Symposium on Nuclear Symmetry Energy (NuSYM13) NSCL/FRIB, East Lansing, Michigan, U.S.A. 22-26 July, 2013 Plan for the Nuclear Symmetry Energy Measurements at RAON, LAMPS Facility Byungsik

More information

Activity Report on ANPhA (in place of Dong-Pil Ming)

Activity Report on ANPhA (in place of Dong-Pil Ming) 2014 WG.9 @ GSI July 11, 2014 Activity Report on ANPhA (in place of Dong-Pil Ming) H. Sakai ANPhA Observer RIKEN As of today Member countries and regions alphabetical order Australia China Ind ia Jap an

More information

Status & Plans for the TRIUMF ISAC Facility

Status & Plans for the TRIUMF ISAC Facility Status & Plans for the TRIUMF ISAC Facility P.W. Schmor APAC 07, Jan 29-Feb 2 Indore, India TRIUMF ISAC Schematic Layout of TRIUMF/ISAC with H- Driver, ISOL Production & Post Accelerators ISAC-II High

More information

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

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Available on CMS information server CMS CR -2018/225 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 27 September 2018 (v2, 19 November

More information

Preliminary Simulation of Beam Extraction for the 28 GHz ECR Ion Source

Preliminary Simulation of Beam Extraction for the 28 GHz ECR Ion Source Preliminary Simulation of Beam Extraction for the 28 GHz ECR Ion Source Bum-Sik Park*, Yonghwan Kim and Seokjin Choi RISP, Institute for Basic Science, Daejeon 305-811, Korea The 28 GHz ECR(Electron Cyclotron

More information

DEVELOPMENT OF JINR FLNR HEAVY-ION ACCELERATOR COMPLEX IN THE NEXT 7 YEARS

DEVELOPMENT OF JINR FLNR HEAVY-ION ACCELERATOR COMPLEX IN THE NEXT 7 YEARS Ó³ Ÿ. 2010.. 7, º 7(163).. 827Ä834 ˆ ˆŠ ˆ ˆŠ Š ˆ DEVELOPMENT OF JINR FLNR HEAVY-ION ACCELERATOR COMPLEX IN THE NEXT 7 YEARS G. Gulbekyan, B. Gikal, I. Kalagin, N. Kazarinov Joint Institute for Nuclear

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

ALICE Commissioning: Getting ready for Physics

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

More information

Operation of the Coupled Cyclotron Facility at Michigan State University

Operation of the Coupled Cyclotron Facility at Michigan State University Operation of the Coupled Cyclotron Facility at Michigan State University Andreas Stolz Workshop on Accelerator Operations Head, Operations Department SLAC National Accelerator Laboratory NSCL / Michigan

More information

Status and Plans of the Large TPC Prototype for the ILC

Status and Plans of the Large TPC Prototype for the ILC EUDET Status and Plans of the Large TPC Prototype for the ILC T. Behnke, R. Diener, L. Hallermann, P. Schade May 20, 2008 Abstract Within the EUDET programme, the FLC TPC Group at DESY in collaboration

More information

arxiv: v1 [nucl-ex] 3 Feb 2015

arxiv: v1 [nucl-ex] 3 Feb 2015 arxiv:1502.00703v1 [nucl-ex] 3 Feb 2015 Study of in-medium mass modification at J-PARC K. Aoki 1 for the J-PARC E16 Collaboration 1 KEK, High Energy Accelerator Research Organization, Tsukuba, Ibaraki

More information

RCNP cyclotron facility

RCNP cyclotron facility 11th International Conference on HEAVY ION ACCELERATOR TECHNOLOGY RCNP cyclotron facility K. Hatanaka hatanaka@rcnp.osaka-u.ac.jp Research Center for Nuclear Physics Osaka University HIAT09 TU9 June 9,

More information

SPIRAL-2 FOR NEUTRON PRODUCTION

SPIRAL-2 FOR NEUTRON PRODUCTION SPIRAL-2 FOR NEUTRON PRODUCTION X. Ledoux and the NFS collaboration Outline The SPIRAL-2 facility The Neutrons For Science Facility OUTLINE SPIRAL-2 The Neutrons For Science facility The SPIRAL-2 project

More information

The SPIRAL2 Project and experiments with high-intensity rare isotope beams

The SPIRAL2 Project and experiments with high-intensity rare isotope beams The SPIRAL2 Project and experiments with high-intensity rare isotope beams Marek Lewitowicz GANIL, CEA/DSM-CNRS/IN2P3, BP 55027, 14076 Caen Cedex, France Lewitowicz@ganil.fr Abstract. The SPIRAL2 facility

More information

Near detector tracker concepts. D. Karlen / U. Vic. & TRIUMF T2K ND280m meeting August 22, 2004

Near detector tracker concepts. D. Karlen / U. Vic. & TRIUMF T2K ND280m meeting August 22, 2004 Near detector tracker concepts D. Karlen / U. Vic. & TRIUMF T2K ND280m meeting August 22, 2004 Longitudinal extent of tracker modules Consensus has developed that the near detector should consist of a

More information

MuSIC- RCNP at Osaka University

MuSIC- RCNP at Osaka University Commissioning of new DC muon beam line, MuSIC- RCNP at Osaka University Dai Tomono Research Center for Nuclear Physics (RCNP), Osaka University On behalf of the MuSIC- RCNP collaboration tomono@rcnp.osaka-

More information

Developments of the RCNP cyclotron cascade

Developments of the RCNP cyclotron cascade CYCLOTRONS 2007 The 18th International Conference on Cyclotrons and Their Applications Developments of the RCNP cyclotron cascade K. Hatanaka,, M. Fukuda, T. Saito, T. Yorita,, H. Tamura, M. Kibayashi,

More information

Introduction to REX-ISOLDE concept and overview of (future) European projects

Introduction to REX-ISOLDE concept and overview of (future) European projects Introduction to REX-ISOLDE concept and overview of (future) European projects Thanks to: Y. Blumenfeld, P. Butler, M. Huyse, M. Lindroos, K. Riisager, P. Van Duppen Energetic Radioactive Beam Facilities

More information

Review of ISOL-type Radioactive Beam Facilities

Review of ISOL-type Radioactive Beam Facilities Review of ISOL-type Radioactive Beam Facilities, CERN Map of the nuclear landscape Outline The ISOL technique History and Geography Isotope Separation On-Line Existing facilities First generation facilities

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

Betty Tsang, NSCL/MSU 曾敏兒. collaboration

Betty Tsang, NSCL/MSU 曾敏兒. collaboration Science of the SpRIT Time Projection Chamber From Earth to Heavens: Femto-scale nuclei to Astrophysical objects SAMURAI International Collaboration Meeting, Sept 8-9, 2014 Sendai, Japan 曾敏兒 for Betty Tsang,

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

two-proton radioactivity discovery of two-proton radioactivity experimental results with TPC s future studies

two-proton radioactivity discovery of two-proton radioactivity experimental results with TPC s future studies two-proton radioactivity discovery of two-proton radioactivity experimental results with TPC s future studies Bertram Blank CEN Bordeaux-Gradignan EPS European Nuclear Physics Conference 2009 Spring meeting

More information

Hadron Physics at LEPS2

Hadron Physics at LEPS2 Hadron Physics at LEPS2 and next-term LEPS Masaru Yosoi RCNP, Osaka Univ. We have decided to continue LEPS and the extension proposal has recently been approved. LEPS2 overview Θ + @LEPS2 solenoid spectrometer

More information

Investigation of nuclear Equation of State (EoS) is an attractive subject not only for nuclear

Investigation of nuclear Equation of State (EoS) is an attractive subject not only for nuclear First Experiment of SπRIT-TPC at SAMURAI in RIKEN-RIBF for SπRIT Collaboration RIKEN, Nishina Center, RIKEN, Japan E-mail: mizuki@riken.jp Investigation of nuclear Equation of State (EoS) is an attractive

More information

Accelerators for the Advanced Exotic Beam Facility

Accelerators for the Advanced Exotic Beam Facility Accelerators for the Advanced Exotic Beam Facility Peter N. Ostroumov Physics Division Content Facility for Radioactive Ion Beams (FRIB) Short introduction to the current status Major differences from

More information

The Accelerator System for ReA3 the New Re-accelerated RIBs Facility at MSU

The Accelerator System for ReA3 the New Re-accelerated RIBs Facility at MSU The Accelerator System for ReA3 the New Re-accelerated RIBs Facility at MSU Xiaoyu Wu National Superconducting Cyclotron Laboratory Michigan State University on behalf of the NSCL ReA3 team X. Wu, Cyclotrons

More information

Development of a Time Projection Chamber with GEM technology in IMP. Herun yang Gas detector group

Development of a Time Projection Chamber with GEM technology in IMP. Herun yang Gas detector group Development of a Time Projection Chamber with GEM technology in IMP Herun yang Gas detector group Outline Introduction TPC prototype based on GEM performance test based cosmic ray Beam test Summary Gas

More information

Status and Challenges of CEPC Time Projection Chamber Detector. Huirong On behalf of CEPC Tracking Subgroup

Status and Challenges of CEPC Time Projection Chamber Detector. Huirong On behalf of CEPC Tracking Subgroup Status and Challenges of CEPC Time Projection Chamber Detector Huirong On behalf of CEPC Tracking Subgroup 015.01.1 Content Status of GEM and TPC Detector Requirements and Concept design Preliminary Simulation

More information

The NFS project. Part of the SPIRAL-2 project built on the GANIL site, Caen, France. NFS is one of the two facilities of the LINAG Experimental Area

The NFS project. Part of the SPIRAL-2 project built on the GANIL site, Caen, France. NFS is one of the two facilities of the LINAG Experimental Area The NFS project Part of the SPIRAL-2 project built on the GANIL site, Caen, France NFS is one of the two facilities of the LINAG Experimental Area Neutron beam between 100 kev and 40 MeV Irradiation station

More information

Status of KEK-E391a and Future Prospects on K L π 0 νν at KEK. GeiYoub Lim IPNS, KEK

Status of KEK-E391a and Future Prospects on K L π 0 νν at KEK. GeiYoub Lim IPNS, KEK Status of KEK-E391a and Future Prospects on K L π 0 νν at KEK GeiYoub Lim IPNS, KEK E391a Collaboration Joint Institute for Nuclear Research (Dubna), Russia High Energy Accelerator Research Organization,

More information

PoS(HCP2009)042. Status of the ALICE Experiment. Werner Riegler. For the ALICE Collaboration. CERN

PoS(HCP2009)042. Status of the ALICE Experiment. Werner Riegler. For the ALICE Collaboration. CERN Status of the ALICE Experiment CERN E-mail: Werner.Riegler@cern.ch For the ALICE Collaboration ALICE is a general-purpose heavy-ion experiment designed to study the physics of strongly interacting matter

More information

Detectors in Nuclear and High Energy Physics. RHIG summer student meeting June 2014

Detectors in Nuclear and High Energy Physics. RHIG summer student meeting June 2014 Detectors in Nuclear and High Energy Physics RHIG summer student meeting June 2014 Physics or Knowledge of Nature Experimental Data Analysis Theory ( application) Experimental Data Initial Conditions /

More information

Development of a new MeV gamma-ray camera

Development of a new MeV gamma-ray camera Development of a new MeV gamma-ray camera ICEPP Symposium February 16, 2004 Hakuba, Nagano, Japan Kyoto University Atsushi Takeda H. Kubo, K. Miuchi, T. Nagayoshi, Y. Okada, R. Orito, A. Takada, T. Tanimori,

More information

DEVELOPMENT OF FFAG AT KYUSYU UNIVERSITY

DEVELOPMENT OF FFAG AT KYUSYU UNIVERSITY FFAG11, Sept.13-17, 2011, Oxford DEVELOPMENT OF FFAG AT KYUSYU UNIVERSITY N.Ikeda, Y.Yonemura, Y.Mori* Kyusyu University *invited FFAG11, Sept.13-17, 2011, Oxford DEVELOPMENTS OF FFAG IN JAPAN Osaka,RCNP

More information

Advantages / Disadvantages of semiconductor detectors

Advantages / Disadvantages of semiconductor detectors Advantages / Disadvantages of semiconductor detectors Semiconductor detectors have a high density (compared to gas detector) large energy loss in a short distance diffusion effect is smaller than in gas

More information

A PRELIMINARY ALIGNMENT PLAN FOR RIA AT MSU

A PRELIMINARY ALIGNMENT PLAN FOR RIA AT MSU IWAA2004, CERN, Geneva, 4-7 October 2004 A PRELIMINARY ALIGNMENT PLAN FOR RIA AT MSU D. P. Sanderson, NSCL-MSU, 1 Cyclotron Lab, East Lansing, MI 48824, USA 1. INTRODUCTION The Rare Isotope Accelerator

More information

Utilization of Intense Rare Isotope Beam at KoRIA

Utilization of Intense Rare Isotope Beam at KoRIA KIAS Workshop Nuclear and Particle Physics in KoRIA and BSI Utilization of Intense Rare Isotope Beam at KoRIA 2011. 9. 17 Yong-Kyun Kim (Hanyang University) On behalf of KoRIA User Community 초신성의 관측 1

More information

In-Flight Fragment Separator and ISOL Cyclotron for RISP

In-Flight Fragment Separator and ISOL Cyclotron for RISP In-Flight Fragment Separator and ISOL Cyclotron for RISP Jong-Won Kim Daejeon, May 9, 2012 Scope of Presentation in the RI Science Project Area of the IF Separator and ISOL cyclotron Two kinds of beam

More information

NSCL Operations and ReAcclerator Facility at MSU. Daniela Leitner Michigan State University

NSCL Operations and ReAcclerator Facility at MSU. Daniela Leitner Michigan State University NSCL Operations and ReAcclerator Facility at MSU Daniela Leitner Michigan State University CCF Operations In Perspective NSCL is funded by NSF in support of a versatile user program with a historical average

More information

Appendix A2. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France.

Appendix A2. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France. Appendix A. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France. Prepared by: Arash Akbari-Sharbaf Why Build Accelerators? Probe deeper From

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

Particle Energy Loss in Matter

Particle Energy Loss in Matter Particle Energy Loss in Matter Charged particles, except electrons, loose energy when passing through material via atomic excitation and ionization These are protons, pions, muons, The energy loss can

More information

Design of a Sector Magnet for High Temperature Superconducting Injector Cyclotron

Design of a Sector Magnet for High Temperature Superconducting Injector Cyclotron MOA2C01 13th Intl. Conf. on Heavy Ion Accelerator Technology Sep. 7, 2015 Design of a Sector Magnet for High Temperature Superconducting Injector Cyclotron Keita Kamakura Research Center for Nuclear Physics

More information

Performance of the Gamma-ray Imaging Detector with Micro-TPC

Performance of the Gamma-ray Imaging Detector with Micro-TPC Performance of the Gamma-ray Imaging Detector with Micro-TPC Cosmic-Ray Group Dept. of Physics, Graduate School of Science, Kyoto University R.Orito Orito,H.Kubo,K.,H.Kubo,K.Miuchi,T.Nagayoshi, A.Takada,A.Takeda,T.Tanimori

More information

Photons in the universe. Indian Institute of Technology Ropar

Photons in the universe. Indian Institute of Technology Ropar Photons in the universe Photons in the universe Element production on the sun Spectral lines of hydrogen absorption spectrum absorption hydrogen gas Hydrogen emission spectrum Element production on the

More information

PANDA-X A New Detector for Dark Matter Search. Karl Giboni Shanghai Jiao Tong University

PANDA-X A New Detector for Dark Matter Search. Karl Giboni Shanghai Jiao Tong University PANDA-X A New Detector for Dark Matter Search Karl Giboni Shanghai Jiao Tong University Seminar at KEK, Tsukuba Japan 3 February, 2011 Jin Ping Laboratory Newly constructed deep underground lab In the

More information

Cascade Spectroscopy at CLAS

Cascade Spectroscopy at CLAS Cascade Spectroscopy at CLAS D.P. Weygand Thomas Jefferson National Accelerator Facility 12/1/2005 D.P. Weygand Cascade Workshop 1 Outline: Ξ* Resonances at CLAS Ghosts of Ξ s Past Ξ(1620), High Mass Ξ*

More information

Heavy Ion Accelerators for RIKEN RI Beam Factory and Upgrade Plans. Upgrade Injector

Heavy Ion Accelerators for RIKEN RI Beam Factory and Upgrade Plans. Upgrade Injector Heavy Ion Accelerators for RIKEN RI Beam Factory and Upgrade Plans RI Beam Factory (1997-) Heavy Ion Beams (2007-) Low intensity Beam now (2008) (Goal: 1pμA U-ion beam) Upgrade Injector H. Okuno, et. al.

More information

Spatial resolution of a MPGD TPC using the charge dispersion signal

Spatial resolution of a MPGD TPC using the charge dispersion signal Spatial resolution of a MPGD TPC using the charge dispersion signal Madhu Dixit Carleton University & TRIUMF Carleton University University of Montreal LAL Orsay CEA Saclay A. Bellerive, K. Boudjemline,

More information

Lise Meitner, Otto Hahn. Nuclear Fission Hans-Jürgen Wollersheim

Lise Meitner, Otto Hahn. Nuclear Fission Hans-Jürgen Wollersheim Lise Meitner, Otto Hahn Nuclear Fission Hans-Jürgen Wollersheim Details of the 252 Cf decay α s: 96.9% SF: 3.1% T 1/2 = 2.647 a Q α = 6.217 MeV E α = 6.118 MeV α α α α α-decay of 252 Cf Mass data: nucleardata.nuclear.lu.se/database/masses/

More information

Study of GEM-TPC for ILC in Japan

Study of GEM-TPC for ILC in Japan Study of GEM-TPC for ILC in Japan Akira Sugiyama (Saga Univ.) japanese LC-TPC group KEK-TUAT-Kogakuin-Kinki-Saga Requirements @ILC ILC-TPC results of small prototype test GEM endplate for Large Prototype

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

for the HARPO Collaboration: *

for the HARPO Collaboration: * Polarimetry and high-angular-resolution gamma-ray observations in the MeV regime using a novel detector concept for the HARPO Collaboration: * * Author list from recent publication: https://arxiv.org/abs/1706.06483

More information

Motivation Electron-Tracking Compton Telescope 1 st Flight of SMILE Preparation for next step summary

Motivation Electron-Tracking Compton Telescope 1 st Flight of SMILE Preparation for next step summary A. Takada (ISAS/JAXA), T. Tanimori, H. Kubo, K. Miuchi, S. Kabuki, H. Nishimura, K. Hattori, K. Ueno, S. Kurosawa, C. Ida, S. Iwaki, M. Takahashi (Kyoto Univ.) Motivation Electron-Tracking Compton Telescope

More information

Korea RI Accelerator

Korea RI Accelerator Korea RI Accelerator Seoul National University On behalf of KoRIA Project Team International Symposium on Nuclear Physics in Asia 2010 10 15 KoRIA in Short RI Accelerator in Korea ISOL and In-Flight method

More information

Beam diagnostics: Alignment of the beam to prevent for activation. Accelerator physics: using these sensitive particle detectors.

Beam diagnostics: Alignment of the beam to prevent for activation. Accelerator physics: using these sensitive particle detectors. Beam Loss Monitors When energetic beam particles penetrates matter, secondary particles are emitted: this can be e, γ, protons, neutrons, excited nuclei, fragmented nuclei... Spontaneous radiation and

More information

COMET muon conversion experiment in J-PARC

COMET muon conversion experiment in J-PARC Institute for Basic Science, Daejeon, Korea E-mail: myeongjaelee@ibs.re.kr COMET is an experiment at J-PARC, Japan, which will search for neutrinoless conversion of muons into electrons in the field of

More information

HARPO: Measurement of polarised gamma rays (1.7 to 72MeV) with the HARPO TPC

HARPO: Measurement of polarised gamma rays (1.7 to 72MeV) with the HARPO TPC HARPO: Measurement of polarised gamma rays (1.7 to 72MeV) with the HARPO TPC Philippe Gros for the HARPO collaboration 1/39 Gamma Astronomy HARPO project Setup at the NewSUBARU photon beam Gas monitoring

More information

pp physics, RWTH, WS 2003/04, T.Hebbeker

pp physics, RWTH, WS 2003/04, T.Hebbeker 3. PP TH 03/04 Accelerators and Detectors 1 pp physics, RWTH, WS 2003/04, T.Hebbeker 2003-12-16 1.2.4. (Inner) tracking and vertexing As we will see, mainly three types of tracking detectors are used:

More information

The Silicon-Tungsten Tracker of the DAMPE Mission

The Silicon-Tungsten Tracker of the DAMPE Mission The Silicon-Tungsten Tracker of the DAMPE Mission Philipp Azzarello, DPNC, University of Geneva for the DAMPE-STK collaboration 10th International Hiroshima Symposium on the Development and Application

More information

Chung-Yao Chao Fellowship Interview

Chung-Yao Chao Fellowship Interview Chung-Yao Chao Fellowship Interview Shaobo WANG Shanghai Jiao Tong University, China April 24, 2017 Supervisor: Prof. Xiangdong JI Dr. Ke HAN 1 Outlines Resume: Education Internship Previous Work and Achievements:

More information

Physics with stopped beams at TRIP-TRAP Facility. P.D. Shidling Cyclotron Institute, Texas A&M University

Physics with stopped beams at TRIP-TRAP Facility. P.D. Shidling Cyclotron Institute, Texas A&M University Physics with stopped beams at TRIP-TRAP Facility P.D. Shidling Cyclotron Institute, Texas A&M University Physics with stopped beams Experiments require high purity low energy ions for studying various

More information

Construction of time-projection chambers to probe the symmetry energy at high density. R. Shane, for the SAMURAI-TPC collaboration

Construction of time-projection chambers to probe the symmetry energy at high density. R. Shane, for the SAMURAI-TPC collaboration Construction of time-projection chambers to probe the symmetry energy at high density R. Shane, for the SAMURAI-TPC collaboration Constraints on the Nuclear Symmetry Energy Nuclear EOS: Impacts heavy-ion

More information

Longitudinal stacking and electron cooling of ion beams in the ESR as a proof of principle for FAIR. C. Dimopoulou

Longitudinal stacking and electron cooling of ion beams in the ESR as a proof of principle for FAIR. C. Dimopoulou Longitudinal stacking and electron cooling of ion beams in the ESR as a proof of principle for FAIR C. Dimopoulou B. Franzke, T. Katayama, D. Möhl, G. Schreiber, M. Steck DESY Seminar, 20 November 2007

More information

Particle Energy Loss in Matter

Particle Energy Loss in Matter Particle Energy Loss in Matter Charged particles loose energy when passing through material via atomic excitation and ionization These are protons, pions, muons, The energy loss can be described for moderately

More information

ECOS-LINCE PROJECT: A highintensity light- and heavy-ion facility for nuclear structure and reactions

ECOS-LINCE PROJECT: A highintensity light- and heavy-ion facility for nuclear structure and reactions ECOS-LINCE PROJECT: A highintensity light- and heavy-ion facility for nuclear structure and reactions Ismael Martel & Muhsin N. Harakeh For the ECOS collaboration NuPECC Meeting, 10-11 October 2014; Edinburgh,

More information

China high-intensity accelerator technology developments for Neutron Sources & ADS

China high-intensity accelerator technology developments for Neutron Sources & ADS AT/INT-04 China high-intensity accelerator technology developments for Neutron Sources & ADS J. Wei, Tsinghua University, China S.N. Fu, IHEP, CAS, China International Topical Meeting on Nuclear Research

More information

Technical Specifications and Requirements on Direct detection for Dark Matter Searches

Technical Specifications and Requirements on Direct detection for Dark Matter Searches Technical Specifications and Requirements on Direct detection for Dark Matter Searches Jin Li THU/IHEP Symposium of the Sino-German GDT Cooperation 04/08/2013 Tübingen Outline Introduction Direct detection

More information

Nuclear Physics New Projects at IMP

Nuclear Physics New Projects at IMP ANPhA Symposium Nuclear Physics New Projects at IMP Institute of Modern Physics Guoqing Xiao 2013.4.25-28, 28, Taipei Cancer Therapy Outline 1.Brief introduction of IMP 2.Recent Results of Nuclear Physics

More information

Il progetto SPES: produzione di fasci di ioni radioattivi ai Laboratori Nazionali di Legnaro.

Il progetto SPES: produzione di fasci di ioni radioattivi ai Laboratori Nazionali di Legnaro. Il progetto SPES: produzione di fasci di ioni radioattivi ai Laboratori Nazionali di Legnaro. Alberto Andrighetto LNL-INFN Congresso SIF 2012 - Napoli Talk Overview -Introduction - The SPES layout & devices.

More information

Performance of a triple-gem detector for high-rate particle triggering

Performance of a triple-gem detector for high-rate particle triggering Performance of a triple-gem detector for high-rate particle triggering G. Bencivenni 1, W. Bonivento 2,4,A.Cardini 2,C. Deplano 2, P. de Simone 1, G. Felici 1, D. Marras 2, F.Murtas 1, D.Pinci 2,3, M.

More information

Status and Performance of the ATLAS Experiment

Status and Performance of the ATLAS Experiment Status and Performance of the ATLAS Experiment P. Iengo To cite this version: P. Iengo. Status and Performance of the ATLAS Experiment. 15th International QCD Conference (QCD 10), Jun 2010, Montpellier,

More information

Prompt gamma measurements for the verification of dose deposition in proton therapy. Contents. Two Proton Beam Facilities for Therapy and Research

Prompt gamma measurements for the verification of dose deposition in proton therapy. Contents. Two Proton Beam Facilities for Therapy and Research Prompt gamma measurements for the verification of dose deposition in proton therapy Two Proton Beam Facilities for Therapy and Research Ion Beam Facilities in Korea 1. Proton therapy facility at National

More information

HIGH INTENSITY ION BEAMS AT GANIL F. Chautard, September 6th, Cyclotron 2010 Lanzhou, China, september F. Chautard

HIGH INTENSITY ION BEAMS AT GANIL F. Chautard, September 6th, Cyclotron 2010 Lanzhou, China, september F. Chautard HIGH INTENSITY ION BEAMS AT GANIL F. Chautard, September 6th, 2010 OUTLINE Operation modes at GANIL Statistics Stable beams Exotic beams ISOL In Flight Beam developments Stable beams Exotic beams Machine

More information

2. Acceleration Scheme

2. Acceleration Scheme 2. Acceleration Scheme Accelerators in the RIBF consist of three existing accelerators and three ring cyclotrons under construction. The existing accelerators are the RIKEN Linear Accelerator (RILAC),

More information

A Triple-GEM Telescope for the TOTEM Experiment

A Triple-GEM Telescope for the TOTEM Experiment A Triple-GEM Telescope for the TOTEM Experiment Giuseppe Latino (Siena University & Pisa INFN) IPRD06 Siena October 4, 2006 TOTEM Experiment @ LHC T2 Telescope 3-GEM Technology Detailed Detector Simulation

More information

NSRRC Current Status and the TPS Project

NSRRC Current Status and the TPS Project NSRRC Current Status and the TPS Project Chien-Te Chen July 21, 2005 1-1 Milestones 1981 Dec. Feasibility study began 1983 Jul. SRRC Project approved by the government 1986 Mar. Preparatory Office of SRRC

More information

Motivation Electron-Tracking Compton Telescope 1 st Flight of SMILE Preparation for next step summary

Motivation Electron-Tracking Compton Telescope 1 st Flight of SMILE Preparation for next step summary A. Takada (ISAS/JAXA), T. Tanimori, H. Kubo, K. Miuchi, S. Kabuki, Y. Kishimoto, J. Parker, H. Nishimura, K. Hattori, K. Ueno, S. Kurosawa, S. Iwaki, C. Ida, M. Takahashi, T. Sawano, K. Taniue, K. Nakamura,

More information

THE DESIGN AND COMMISSIONING OF THE ACCELERATOR SYSTEM OF THE RARE ISOTOPE REACCELERATOR ReA3 AT MICHIGAN STATE UNIVERSITY*

THE DESIGN AND COMMISSIONING OF THE ACCELERATOR SYSTEM OF THE RARE ISOTOPE REACCELERATOR ReA3 AT MICHIGAN STATE UNIVERSITY* THE DESIGN AND COMMISSIONING OF THE ACCELERATOR SYSTEM OF THE RARE ISOTOPE REACCELERATOR ReA3 AT MICHIGAN STATE UNIVERSITY* X. Wu#, B. Arend, C. Compton, A. Facco, M. Johnson, D. Lawton, D. Leitner, F.

More information

ANURIB Advanced National facility for Unstable and Rare Ion Beams

ANURIB Advanced National facility for Unstable and Rare Ion Beams PRAMANA c Indian Academy of Sciences Vol. 85, No. 3 journal of September 2015 physics pp. 505 515 ANURIB Advanced National facility for Unstable and Rare Ion Beams ARUP BANDYOPADHYAY, V NAIK, S DECHOUDHURY,

More information

Photofission of 238-U Nuclei

Photofission of 238-U Nuclei Photofission of 238-U Nuclei International Thorium Energy Conference - ThEC18, 29-31st of October 2018, Belgium İsmail Boztosun This research has been supported by TÜBİTAK with grant number 114F220 Motivations

More information

TPC-like analysis for thermal neutron detection using a GEMdetector

TPC-like analysis for thermal neutron detection using a GEMdetector Bernhard Flierl - LS Schaile TPC-like analysis for thermal neutron detection using a GEMdetector Triple GEM Detector B-Cathode 6 mm drift space 2 mm GEMs 2 mm 2 mm APV25 readout 2 µm B-converter cathode

More information

HIRFL STATUS AND HIRFL-CSR PROJECT IN LANZHOU

HIRFL STATUS AND HIRFL-CSR PROJECT IN LANZHOU HIRFL STATUS AND HIRFL-CSR PROJECT IN LANZHOU J. W. Xia, Y. F. Wang, Y. N. Rao, Y. J. Yuan, M. T. Song, W. Z. Zhang, P. Yuan, W. Gu, X. T. Yang, X. D. Yang, S. L. Liu, H.W.Zhao, J.Y.Tang, W. L. Zhan, B.

More information

EBSS: Hands-on Activity #8. Operation of an electromagnetic isotope separator (EMIS) Dan Stracener Jon Batchelder

EBSS: Hands-on Activity #8. Operation of an electromagnetic isotope separator (EMIS) Dan Stracener Jon Batchelder EBSS: Hands-on Activity #8 Operation of an electromagnetic isotope separator (EMIS) Dan Stracener Jon Batchelder Schematic of RIB Production at the HRIBF ISOL: Isotope Separation On-Line 2 Managed by UT-Battelle

More information

The Facility for Rare Isotope Beams

The Facility for Rare Isotope Beams The Facility for Rare Isotope Beams This material is based upon work supported by the U.S. Department of Energy Office of Science under Cooperative Agreement DE-SC0000661, the State of Michigan and Michigan

More information

GANIL STATUS REPORT. B. Jacquot, F. Chautard, A.Savalle, & Ganil Staff GANIL-DSM/CEA,IN2P3/CNRS, BP 55027, Caen Cedex, France.

GANIL STATUS REPORT. B. Jacquot, F. Chautard, A.Savalle, & Ganil Staff GANIL-DSM/CEA,IN2P3/CNRS, BP 55027, Caen Cedex, France. GANIL STATUS REPORT B. Jacquot, F. Chautard, A.Savalle, & Ganil Staff GANIL-DSM/CEA,IN2P3/CNRS, BP 55027, 4076 Caen Cedex, France Abstract The GANIL-Spiral facility (Caen, France) is dedicated to the acceleration

More information

The heavy ion irradiation facility at KVI-CART

The heavy ion irradiation facility at KVI-CART The heavy ion irradiation facility at KVI-CART Brian N. Jones 1, Marc-Jan van Goethem 1,2, Rob Kremers 1, Harry Kiewiet 1, Emiel van der Graaf 1, Sytze Brandenburg 1 1 University of Groningen, KVI-Center

More information

Hybrid Gaseous Detector Module for CEPC-TPC

Hybrid Gaseous Detector Module for CEPC-TPC Hybrid Gaseous Detector Module for CEPC-TPC Huirong QI Institute of High Energy Physics, CAS June 15 th, 2016, Tsinghua University, Beijing - 1 - Outline Requirements of CEPC-TPC Occupancy and simulation

More information

Opportunities to study the SHE production mechanism with rare isotopes at the ReA3 facility

Opportunities to study the SHE production mechanism with rare isotopes at the ReA3 facility Opportunities to study the SHE production mechanism with rare isotopes at the ReA3 facility Zach Kohley National Superconducting Cyclotron Laboratory Department of Chemistry Michigan State University,

More information

The BoNuS Detector. A Radial-Drift GEM TPC. Howard Fenker TPC R&D Meeting LBL, March 24, 2005

The BoNuS Detector. A Radial-Drift GEM TPC. Howard Fenker TPC R&D Meeting LBL, March 24, 2005 The BoNuS Detector A Radial-Drift GEM TPC Howard Fenker TPC R&D Meeting LBL, March 24, 2005 Barely Off-shell Nucleon Structure This work was partially supported by DOE Contract No. DE-AC05-84ER40150 under

More information

TAMU-TRAP facility for Weak Interaction Physics. P.D. Shidling Cyclotron Institute, Texas A&M University

TAMU-TRAP facility for Weak Interaction Physics. P.D. Shidling Cyclotron Institute, Texas A&M University TAMU-TRAP facility for Weak Interaction Physics P.D. Shidling Cyclotron Institute, Texas A&M University Outline of the talk Low energy test of Standard Model T =2 Superallowed transition Facility T-REX

More information

discovery of two-proton radioactivity future studies Bertram Blank, CEN Bordeaux-Gradignan Hirschegg, january 2008

discovery of two-proton radioactivity future studies Bertram Blank, CEN Bordeaux-Gradignan Hirschegg, january 2008 two-proton radioactivity discovery of two-proton radioactivity Experimental results with TPC future studies Bertram Blank, CEN Bordeaux-Gradignan Hirschegg, 14-18 january 2008 alpha emission of 4 He 2

More information

NSCL and Physics and Astronomy Department, Michigan State University Joint Institute for Nuclear Astrophysics

NSCL and Physics and Astronomy Department, Michigan State University Joint Institute for Nuclear Astrophysics National Superconducting Cyclotron Laboratory An overview Ana D. Becerril NSCL and Physics and Astronomy Department, Michigan State University Joint Institute for Nuclear Astrophysics University of North

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

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

Study of the HARPO TPC for a high angular resolution g-ray polarimeter in the MeV-GeV energy range. David Attié (CEA/Irfu)

Study of the HARPO TPC for a high angular resolution g-ray polarimeter in the MeV-GeV energy range. David Attié (CEA/Irfu) Study of the HARPO TPC for a high angular resolution g-ray polarimeter in the MeV-GeV energy range David Attié (CEA/Irfu) Outline Motivation of an MeV-GeV polarimeter Scientific case and expected performance

More information