E Experimental Setup and Condition

Size: px
Start display at page:

Download "E Experimental Setup and Condition"

Transcription

1 C2C Rome E Experimental Setup and Condition Tomofumi Maruta Graduate School of Science, Tohoku Univ

2 Table of Contents Kinematics Experimental setup HKS Detector HES Detector Design Resolution Data summary 2

3 Progress of Spectroscopic by (e,e K + HallC E (2000): 12!B Splitter + SOS + Enge Resolution : 750keV(FWHM) A proof of principle E !B 440h x 0.66µA 3

4 Progress of Spectroscopic by (e,e K + HallC E (2000): 12!B Splitter + SOS + Enge Resolution : 750keV(FWHM) A proof of principle E (2005): 7!He, 12!B, 28!Al Splitter + HKS + Enge Resolution : 400keV(FWHM) Yield : 10 x E Optimization of eʼ acceptance (Tilt method) Establish the techniques E !B 440h x 0.66µA Resolution x 2 Yield x 10 S/N ratio x 4 E !B 120h x 24µA Preliminary 3

5 Progress of Spectroscopic by (e,e K + HallC E (2000): 12!B Splitter + SOS + Enge Resolution : 750keV(FWHM) A proof of principle E (2005): 7!He, 12!B, 28!Al Splitter + HKS + Enge Resolution : 400keV(FWHM) Yield : 10 x E Optimization of eʼ acceptance (Tilt method) Establish the techniques E !B 440h x 0.66µA Resolution x 2 Yield x 10 S/N ratio x 4 E !B 120h x 24µA E (2009): 7!He, 9!Li, 10!Be, 52!V New Splitter + HKS + HES Tilt method Precise study in the wide mass region Preliminary 3

6 Kinematics of the E Experiment Electron beam Momentum: 2.34GeV/c Target nucleus Scattered electron Central momentum: 0.844GeV/c Angular acceptance: 3 9! "+p#!+k + 1.5GeV "* p Coincidence measurement M.Q.Tran et al. PLB445 (1998) 20 K + Central momentum: 1.2GeV/c Angular acceptance :

7 Kinematics of (e, e K + ) programs E E E Mainz E" (GeV) W (GeV) Q 2 (GeV/c) Ebeam (GeV) 4.02/3.78/ Peʼ (GeV/c) 1.8/1.57/ θeʼ (deg) PK+ (GeV/c) θk+ (deg) M.Q.Tran et al. PLB445 (1998) 20 "+p#!+k + Q 2 (GeV/c) 2 Mainz E (E05-115: virtual photon oriented e distribution) E E

8 Continuous Electron Beam Accelerator Facility Bird view of CEBAF North Linac South Linac Accelerator specification Duty factor : 100%! comparable hypernuclear yield[/h] to ($ +,K + ) reaction (100 x σ(e,eʼk) < σ($,k)) Injector HallA HallC Beam energy spread : < 7 x 10-5 Bunch energy spread (σ) < 3 x 10-5 Energy stability (σ) < 3 x 10-5! Achievable to good energy resolution of a few 100keV Beam size (rms): < 100μm Beam configuration 0.5ps bunch in every 2ns time 2ns Δt=0.5ps CEBAF is unique facility for (e, e K + ) hypernuclear spectroscopy except for Mainz 6

9 Beamline at Hall-C E01-011:!Post-chicane configuration E05-115:!Pre-chicane configuration Merit : Combine dumps in both photon and beam. Demerit : Huge background around post-chicane area due to beam halo. Merit : Cleanly transport the beam. Demerit : Photon dump is necessary inside the Hall. To dump Target HKS HKS 2009年12月21日月曜日 New Splitter HES To beam dump Target HKS CHAPTER Photon line Beam 24 Beam The HKS Enge spectrometer Splitter 2.3 Enge The E hypernuclear spectroscopy system is establi olution for the Λ hypernuclear spectroscopy. It consists of the Enge split pole magnet (Enge) and the High resolution The incident electron ( 1.8 GeV) interacted with a target Enge Photon dump 7

10 E setup HES Introduction of Large acceptance electron spectrometer. HES detector Higher electron beam energy acceptable than Enge. e HKS New splitter K + HKS detector 2.344GeV e beam Target 8

11 E Setup HKS New SPL To Photon dump Beam To beam dump HES 9

12 HKS Spectrometer KD KQ2 KQ1 QQD configuration Momentum acceptance : 1.2GeV/c ±12.5% Solid angle : 11msr!p/p : 2 x 10-4 Angle acceptance : 1 13 deg Rate capability : 1.5MHz HKS Solid Angle Solid Angle (msr) Kaon Momentum (GeV/c) 10

13 HKS Detectors (Cherenkov Counters) HKS-D KDC1 KTF1Y KDC2 KTF2X KLC Singles Rate $ + 25 khz K + p 0.2 khz 16 khz Max. DAQ rate 2kHz 30μA, 12 C 100mg/cm 2 Based on E KTF1X KAC KWC KAC1/2/3 7-seg. Aerogel cherenkov Effective area 46 H x 169 W x 31 T (cm 3 ) Index KWC1/2 12-seg. Water cherenkov Effective area 35 H x W x 8 T (cm 3 ) Index 1.33 KLC 13-seg. Lucite cherenkov Effective area 42 H x W x 2 T (cm 3 ) Index 1.49 New New Cherenkov counters are for $/p rejection >99.9% $ rejection by AC >99.9% p rejection by WC AC WC LC $ + K + p Ncherenkov 1-1/(%n) 2 11

14 HKS Detectors (TOF Counters, DCs) KDC1 KDC2 KTF1Y KTF2X HKS-D KLC KTF1X KAC KWC KDC1/2 Planner drift chamber Effective area 30 H x 105 W x 3.5 T (cm 3 ) Layer config 6 (xxʼ, uuʼ, vvʼ) KTF1X 17-seg. plastic scinti Effective area 30 H x 125 W x 2 T (cm 3 ) KTF1Y 9-seg. plastic scinti Effective area 27.5 H x 125 W x 2 T (cm 3 ) KTF2X 18-seg. plastic scinti. Effective area 35 H x 170 W x 2 T (cm 3 )! TOF resolution of σ=75ps is required for $ + /K + 4σ separation! flight length 1.5m (KTF1X - 2X)! 1.35GeV/c $ + /K + ΔTOF = 300ps! σ=77ps achieved at test experiment at KEK-T1 12

15 HES Spectrometer ED QQD configuration Momentum acceptance : 0.844GeV/c±17% Solid angle : 7msr Angle acceptance : 3 9 deg δp/p : 2 x 10-4 (FWHM) Rate capability : 5MHz HES Solid Angle Solid Angle (msr) EQ2 EQ e Momentum (GeV/c) 13

16 HES detector package EDC1 Honeycomb, used in 2nd EDC2 EDC1 Effective area 12 H x 100 W x 32 T (cm 3 ) Layer config 10 (xxʼ, uuʼ, xxʼ, vvʼ, xxʼ) EDC2 Planner drift chamber Effective area 30 H x 105 W x 3.5 T (cm 3 ) Layer config 6 (xxʼ, uuʼ, vvʼ) EHOD1/2 29 seg. plastic scinti. e EHOD1 HES-D Effective area 30 H x 117 W x 1 T (cm 3 ) EHOD1 EDC1 EHOD1 EHOD2 EDC2 14

17 Momentum Correlation Momentum acceptance between K+ and eʼ are HES Pe '[ GeV / c ] decided! distribution to be diagonal. 1.1 E Pe ' vs PK Beam energy GeV ΛV Σ Λ g.s PK [ GeV / c ] HKS 350 Figure 5: Momentum correlation between kaon arm and electron arm for hyperons and hypernuclei production 2009年12月21日月曜日 reaction. 15

18 Tilt Method Optimization of Scattered electron acceptance Beam Energy : 1.8"2.34GeV Background electrons go more forward Beam current # S/N ratio # Brand-new e spectrometer, HES Enlarge acceptance # Virtual Photon Yield # EQ2 EQ1 signal Splitter y (mrad) yʼ (mrad) ENGE acceptance x (mrad) Red: Signal Green: B.G. Blue : B.G. E E background xʼ (mrad) 16

19 Tilt Method Optimization of Scattered electron acceptance Beam Energy : 1.8"2.34GeV Background electrons go more forward Beam current # S/N ratio # Brand-new e spectrometer, HES Enlarge acceptance # Virtual Photon Yield # EQ2 EQ1 signal Splitter 6.5 y (mrad) yʼ (mrad) ENGE acceptance x (mrad) Red: Signal Green: B.G. Blue : B.G. E E background xʼ (mrad) 16

20 Design Energy Resolution Target 7 Li 10 B 12 C 52 Cr HKS momentum (kev) HKS angle (kev) HES momentum (kev) HES angle (kev) Beam energy (kev) 160 Target (100mg/cm 2 ) Overall (kev)

21 Parameters of JLab (e, e K + ) programs Configuration E E E E SOS+ENGE +Splitter HRS+HRS +Septum HKS+ENGE +Splitter HKS+HES +New Splitter Beam intensity (μa) Target thickness (mg/cm 2 ) Hypernuclear yield ( 12!B g.s.) ( 16) ( 40) Resolution (kev) ( 3 400) Beam energy(gev) pk (GeV/c) peʼ (GeV/c) θk (deg) θeʼ (deg) ( ): Expectation 18

22 Data summary Beamtime: Aug./21 st Nov./2 nd /2009 Target Hypernucleus Thickness (mg/cm 2 ) Average beam current (ua) Total Charge (Coulomb) CH2 Water! & ! & Li 7! He Be 9! Li B 10! Be C 12! B Cr 52! V

23 Collaboration Pictures 20

Hypernuclear spectroscopy via the (e,e K + ) reaction

Hypernuclear spectroscopy via the (e,e K + ) reaction HYP2015, Sendai, Japan 7 th September 2015 Satoshi N Nakamura, Tohoku University Hypernuclear spectroscopy via the (e,e K + ) reaction Analysis Details: T.Gogami parallel 1a-5 Future Programs at JLab L.Tang,

More information

Spectroscopic investigation of Λ hypernuclei in the wide mass region using the (e,e'k + ) reaction

Spectroscopic investigation of Λ hypernuclei in the wide mass region using the (e,e'k + ) reaction Journal of Physics: Conference Series Spectroscopic investigation of Λ hypernuclei in the wide mass region using the (e,e'k + ) reaction To cite this article: Satoshi N Nakamura and JLab E05-115 collaboration

More information

The Second Generation Hypernuclear Spectroscopy at JLab Hall C (E experiment)

The Second Generation Hypernuclear Spectroscopy at JLab Hall C (E experiment) The Second Generation Hypernuclear Spectroscopy at JLab Hall C (E01-011 experiment) A. Matsumura ( Tohoku Univ. ) for the E01-011 collaboration PANIC08 Eilat, ISRAEL 11 Nov. 2008 Motivation Investigate

More information

Study of Lambda hypernuclei with electron beams

Study of Lambda hypernuclei with electron beams Study of Lambda hypernuclei with electron beams Satoshi N Nakamura, Tohoku University JLab HKS-HES Mainz A1 hypernuclear Collaborations JLab E05-115 collaboration, 2009, JLab Hall-C Quantum Many-body System

More information

Satoshi N Nakamura Tohoku University HUGS 2010 Lecture June Jefferson Lab. Day 3 : #5 and #6

Satoshi N Nakamura Tohoku University HUGS 2010 Lecture June Jefferson Lab. Day 3 : #5 and #6 Satoshi N Nakamura Tohoku University HUGS 2010 Lecture 14-17 June 2010 @ Jefferson Lab Day 3 : #5 and #6 g-ray spectroscopy Weak-decay p spectroscopy Produce HY by (p,k) or (K, p) reaction : Resolution

More information

E COLLABORATION

E COLLABORATION E94-107 COLLABORATION A.Acha, H.Breuer, C.C.Chang, E.Cisbani, F.Cusanno, C.W.de Jager, R. De Leo, R.Feuerbach, S.Frullani, F.Garibaldi, D.Higinbotham, M.Iodice, L.Lagamba, J.LeRose, P.Markowitz, S.Marrone,

More information

Hypernuclear spectroscopy program at JLab Hall C

Hypernuclear spectroscopy program at JLab Hall C Nuclear Physics A 804 (2008) 125 138 www.elsevier.com/locate/nuclphysa Hypernuclear spectroscopy program at JLab Hall C O. Hashimoto a,, S.N. Nakamura a,a.acha c, A. Ahmidouch g, D. Androic f,a.asaturyan

More information

E Analysis status Mass and cross section evaluation Comments on physics interpretation

E Analysis status Mass and cross section evaluation Comments on physics interpretation E01-011 Analysis status Mass and cross section evaluation Comments on physics interpretation Based on Ph.D presentation of A. Matsumura Y.Fujii Tohoku University HKS-HES collaboration meeting at JLab,

More information

Spectroscopic study of Λ hypernuclei in the medium-heavy mass region and p-shell region using the (e,e K + ) reaction

Spectroscopic study of Λ hypernuclei in the medium-heavy mass region and p-shell region using the (e,e K + ) reaction Spectroscopic study of Λ hypernuclei in the medium-heavy mass region and p-shell region using the (e,e K + ) reaction ( Additional beamtime request of the approved E05-115 experiment) O. Hashimoto (Spokesperson),

More information

! Hypernuclear spectroscopy in Hall A. ! Experimental issues. ! Prospectives (Hall A & Hall C collaboration)

! Hypernuclear spectroscopy in Hall A. ! Experimental issues. ! Prospectives (Hall A & Hall C collaboration) High-Resolution Hypernuclear Spectroscopy ElectronScattering at JLab, Hall A F. Garibaldi HYP2012 - Barcelona - October 2012! Hypernuclear spectroscopy in Hall A! 12 C, 16 O, 9 Be, H! E-07-012! Experimental

More information

Table of Contents. References... 21

Table of Contents. References... 21 Table of Contents Introduction and Experimental Overview 2 production cross sections: e + p ν e + Λ Λ > p + π decay particle detection target luminosity considerations backgrounds Physics Motivation 5

More information

High-Resolution Hypernuclear Physics at Jlab

High-Resolution Hypernuclear Physics at Jlab High-Resolution Hypernuclear Physics at Jlab F. Garibaldi Mainz and beyond - 02 April 209 8 Electroproduction E r pr u n of f hypernuclei yp rnu Experimental challenges The experimental Program at Jefferson

More information

Hypernuclear Physics in the S=-1 sector

Hypernuclear Physics in the S=-1 sector Hypernuclear Physics in the S=-1 sector O. Hashimoto Department of Physics, Tohoku University, Sendai 980-8578, Japan (Dated: June 1, 2003) Hypernuclear physics in the S=-1 sector, particularly its spectroscopic

More information

Present Status and Future Plans of Hypernuclear experiments -- S = -1 sector --

Present Status and Future Plans of Hypernuclear experiments -- S = -1 sector -- KEK Nuclear Theory WS Aug. 2, KEK 2006WS Aug. 2, 2006 Present Status and Future Plans of Hypernuclear experiments -- S = -1 sector -- 2006.6 2005.1 Dept. of Physics, Tohoku University H. Tamura SKS @KEK

More information

Production of neutron-rich Λ hypernuclei by the (π,k + ) double-charge-exchange reaction

Production of neutron-rich Λ hypernuclei by the (π,k + ) double-charge-exchange reaction HYP2003@Jlab Production of neutron-rich Λ hypernuclei by the (π,k + ) double-charge-exchange reaction P. K. SAHA for KEK-PS-E521 collaboration Osaka E-C. University, Japan. Osaka E-C Univ., KEK, Tokyo

More information

Electron scattering experiment off proton at ultra-low Q 2

Electron scattering experiment off proton at ultra-low Q 2 Electron scattering experiment off proton at ultra-low Q 2 Toshimi Suda Research Center for Electron-Photon Science, Tohoku University, Sendai Proton Radius Puzzle NEUROSCIENCE People Who Remember Everything

More information

APEX: Goals and Strategy

APEX: Goals and Strategy APEX: Goals and Strategy Natalia Toro (Perimeter Institute) e 2 10-4 10-5 10-6 10-7 10-8 E141 A' Æ Standard Model a m, 5 s E774 a m,±2 s favored a e DarkLight WASA Phenix HPS 2015 KLOE MAMI APEX BaBar

More information

LEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration

LEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration LCS2014 International Workshop LEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration Outline Overview of the LEPS&LEPS2 beamlines Recent results from LEPS Search

More information

Proposal Title: Proposal Physics Goals Indicate any experiments that have physics goals similar to those in your proposal.

Proposal Title: Proposal Physics Goals Indicate any experiments that have physics goals similar to those in your proposal. JLAB USER GROUP Jefferson Lab PAC19 Proposal Cover Sheet This document must be received by close of business Thursday, Experimental Hall: Days Requested for Approval: December 14, 2000 at: Jefferson Lab

More information

Future gamma-ray spectroscopic experiment (J-PARC E63) on 4 ΛH

Future gamma-ray spectroscopic experiment (J-PARC E63) on 4 ΛH Future gamma-ray spectroscopic experiment (J-PARC E63) on ΛH 2018/6/26 T. O. Yamamoto KEK IPNS (Japan) for the E63 collaboration Contents CSB in s-shell hypernuclear system studied via γ-ray spectroscopy

More information

Atsushi Sakaguchi (Osaka University) for the J-PARC E10 Collaboration

Atsushi Sakaguchi (Osaka University) for the J-PARC E10 Collaboration Atsushi Sakaguchi (Osaka University) for the J-PARC E10 Collaboration Study of Λ hypernuclei and ΛN interaction Λ hypernucleus System made of a Λ hyperon and a nucleus(a) ΛN interaction strong enough to

More information

T.Takahashi (KEK) K1.8 Exp. Group. Status of Apparatus. Run Plan

T.Takahashi (KEK) K1.8 Exp. Group. Status of Apparatus. Run Plan Status Report on K1.8/SKS Experiments T.Takahashi (KEK) K1.8 Exp. Group. The 9 th PAC Meeting on 2010 Jan. 15 Introduction Status of Apparatus Available Beam Condition Run Plan Approved Experiments K1.8

More information

GMp Experiment. M. Eric Christy. Hall A/C Summer Meeting For the GMp Collaboration

GMp Experiment. M. Eric Christy. Hall A/C Summer Meeting For the GMp Collaboration GMp Experiment M. Eric Christy For the GMp Collaboration Hall A/C Summer Meeting 2017 Overview of GMp Experiment Performed measurements of elastic e-p cross section over a Q2 range of 2-16 GeV2 Improve

More information

Polarimetry. POSIPOL 2011 Beijing Peter Schuler (DESY) - Polarimetry

Polarimetry. POSIPOL 2011 Beijing Peter Schuler (DESY) - Polarimetry Polarimetry Overview Compton Transmission Polarimetry at source energy Bhabha Polarimetry at 400 MeV Compton Polarimetry at 5 GeV Compton Polarimetry at full energy 1 Suitable Processes Compton Transmission

More information

Hadron Physics with Photon Beam at LEPS/ LEPS2 Takashi Nakano (RCNP, Osaka Univ.) HHIQCD2015, March 3rd, 2015

Hadron Physics with Photon Beam at LEPS/ LEPS2 Takashi Nakano (RCNP, Osaka Univ.) HHIQCD2015, March 3rd, 2015 Hadron Physics with Photon Beam at LEPS/ LEPS2 Takashi Nakano (RCNP, Osaka Univ.) HHIQCD2015, March 3rd, 2015 1 Outline LEPS Overview Some recent results LEPS2 Physics Motivation Overview First experiment

More information

Electron Beam Polarimetry: Status and Prospects. DIS 2005, Madison, April 2005 E. Chudakov (JLab)

Electron Beam Polarimetry: Status and Prospects. DIS 2005, Madison, April 2005 E. Chudakov (JLab) Electron Beam Polarimetry: Status and Prospects DIS 2005, Madison, April 2005 E. Chudakov (JLab) Motivation: what accuracy is required for various experiments Methods in use: Optical methods Mott scattering

More information

Max. Central Momentum 11 GeV/c 9 GeV/c Min. Scattering Angle 5.5 deg 10 deg Momentum Resolution.15% -.2% Solid Angle 2.1 msr 4.

Max. Central Momentum 11 GeV/c 9 GeV/c Min. Scattering Angle 5.5 deg 10 deg Momentum Resolution.15% -.2% Solid Angle 2.1 msr 4. Hall C - 12 GeV pcdr Max. Central Momentum 11 GeV/c 9 GeV/c Min. Scattering Angle 5.5 deg 10 deg Momentum Resolution.15% -.2% Solid Angle 2.1 msr 4.4 msr Momentum Acceptance 40% Target Length Acceptance

More information

C NS. Direct reactions of Borromean nuclei FM50. S. Shimoura CNS, University of Tokyo

C NS. Direct reactions of Borromean nuclei FM50. S. Shimoura CNS, University of Tokyo C NS Direct reactions of Borromean nuclei S. Shimoura CNS, University of Tokyo FM50 Introduction 3N force in neutron-rich nuclei U1X IL2/4 B.E. Importance of T=3/2 3N force in the PRC 64 014001 (2001)

More information

Study of Hypernuclei with Heavy Ion (HypHI collaboration)

Study of Hypernuclei with Heavy Ion (HypHI collaboration) Study of Hypernuclei with Heavy Ion Beams @GSI (HypHI collaboration) Tomokazu Fukuda Osaka Electro-Communication Univ. Take R. Saito, S. Minami, S. Ajimura, Y. Mizoi, A. Sakaguchi et al. GSI, Mainz, Osaka

More information

Study of Light Hypernuclei by Pionic Decay at JLab

Study of Light Hypernuclei by Pionic Decay at JLab Study of Light Hypernuclei by Pionic Decay at JLab M. Christy, C. Keppel, M. Kohl, Liguang Tang (spokesperson), L. Yuan (spokesperson), L. Zhu Department of Physics, Hampton University, VA 23668, U.S.A.

More information

A Measurement of the Induced polarization of electro-produced Λ(1116) with CLAS

A Measurement of the Induced polarization of electro-produced Λ(1116) with CLAS A Measurement of the Induced polarization of electro-produced Λ(1116) with CLAS Marianna Gabrielyan Florida International University HUGS 2008 Why study electromagnetic production of kaons? Formalism.

More information

J-PARC E07 Ξ - Junya Yoshida (Advanced Science Research Center, JAEA) On behalf of J-PARC E07 Collaboration K + K - X -

J-PARC E07 Ξ - Junya Yoshida (Advanced Science Research Center, JAEA) On behalf of J-PARC E07 Collaboration K + K - X - J-PARC E07 Systematic study of double strangeness nuclei with Hybrid emulsion method LL hypernucleus K - 1.8GeV/c Target SSD X - K + nλ p p Λ n X hypernucleus n p p Ξ - n Ge detector X-ray X-ray from X

More information

Experimental hypernuclear physics

Experimental hypernuclear physics Experimental hypernuclear physics p n n p n n p p Λ p p n Alessandro Feliciello I.N.F.N. - Sezione di Torino Outline strangeness nuclear physics: interest discovery potential experimental results high

More information

Measurement of the lifetime and of weak decay partial widths of mirror p-shell Λ-hypernuclei

Measurement of the lifetime and of weak decay partial widths of mirror p-shell Λ-hypernuclei Measurement of the lifetime and of weak decay partial widths of mirror p-shell -hypernuclei International Workshop on Physics at the extended Hadron Experimental Facility of J-PARC March 5-6, 2016, J-PARC,

More information

Yoshikazu Maeda RCNP For LEPS collaboration

Yoshikazu Maeda RCNP For LEPS collaboration LEPS2 detector Yoshikazu Maeda RCNP For LEPS collaboration LEPS2 project Higher intensity and energy photon beam General purposed detector Detector design based on E949 detector Nagoya 08/12/7 Key words

More information

M.Battaglieri Istituto Nazionale di Fisica Nucleare Genova - Italy. A Forward Photon Tagging Facility for CLAS12

M.Battaglieri Istituto Nazionale di Fisica Nucleare Genova - Italy. A Forward Photon Tagging Facility for CLAS12 A Forward Photon Tagging Facility for CLAS12 M.Battaglieri Istituto Nazionale di Fisica Nucleare Genova - Italy 1) From CEBAF at 6 GeV 2) From CEBAF at 6 GeV to CEBAF at 12 GeV add Hall D (and beam line)

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

The APEX Experiment and Test Run

The APEX Experiment and Test Run The APEX Experiment and Test Run Natalia Toro (Perimeter Institute) for the APEX Collaboration S. Abrahamyan, A. Afanasev, Z. Ahmed, E. Aliotta, K. Allada, D. Anez, D. Armstrong, T. Averett, A. Barbieri,

More information

J-PARC (Japan Proton Accelerator Research Complex)

J-PARC (Japan Proton Accelerator Research Complex) J-PARC Tokai, Japan (Japan Proton Accelerator Research Complex) Material and Biological Science Facility 50 GeV Synchrotron (15 ma) 400 MeV Linac (350m) 3 GeV Synchrotron (333 ma) Neutrino Facility World-highest

More information

Electroproduction of Strangeness on 3,4 He

Electroproduction of Strangeness on 3,4 He Electroproduction of Strangeness on 3,4 He Motivation 1H(e,e K)L A(e,e K), A=2,3,4 Bound Λ Hypernuclei: 3 ΛH, 4 ΛH Outlook HYP2003, Jefferson Lab Frank Dohrmann, Forschungszentrum Rossendorf, Dresden !

More information

Meson spectroscopy at CLAS and CLAS12: the present and the future. Raffaella De Vita INFN Genova for the CLAS Collaboration

Meson spectroscopy at CLAS and CLAS12: the present and the future. Raffaella De Vita INFN Genova for the CLAS Collaboration Meson spectroscopy at CLAS and CLAS12: the present and the future Raffaella De Vita INFN Genova for the CLAS Collaboration Why hadron spectroscopy? QCD is responsible for most of the visible mass in the

More information

E (GMp) Precision Measurement of the Proton Elastic Cross Section at High Q 2. Thir Gautam Hampton University

E (GMp) Precision Measurement of the Proton Elastic Cross Section at High Q 2. Thir Gautam Hampton University E12-07-108 (GMp) Precision Measurement of the Proton Elastic Cross Section at High Q 2 Thir Gautam Hampton University On behalf of the GMp Collaboration Hall A Collaboration Meeting January 18, 2017 GMp

More information

Threshold photoproduction of J/y with the GlueX experiment. Lubomir Pentchev Jefferson Lab for the GlueX collaboration

Threshold photoproduction of J/y with the GlueX experiment. Lubomir Pentchev Jefferson Lab for the GlueX collaboration Threshold photoproduction of J/y with the GlueX experiment Lubomir Pentchev Jefferson Lab for the GlueX collaboration 7 th Workshop of the APS Topical Group on Hadron Physics, Washington, DC February 1-3

More information

Theory English (Official)

Theory English (Official) Q3-1 Large Hadron Collider (10 points) Please read the general instructions in the separate envelope before you start this problem. In this task, the physics of the particle accelerator LHC (Large Hadron

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

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

Low-Energy Accelerators for High Precision Measurements Sebastian Baunack

Low-Energy Accelerators for High Precision Measurements Sebastian Baunack Low-Energy Accelerators for High Precision Measurements Sebastian Baunack Johannes Gutenberg-Universität Mainz EINN 2017, Oct. 31 - Nov 4, 2017 Paphos, Cyprus 1 Outline New type of accelerators: ERL High

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

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

Hypernuclear magnetic moments

Hypernuclear magnetic moments The HypHI HI project at GSI/FAIR Hypernuclear spectroscopy with heavy ion collisions ons Progress Report Take R. Saito for the HypHI collaboration Helmholtz-University Young Investigators Group VH-NG-239

More information

GMp Experiment (E ): An update

GMp Experiment (E ): An update GMp Experiment (E12-07-108): An update Kalyan Allada MIT Hall A/C Summer Meeting, Jefferson Lab 17th July 2015 Motivation Accurately measure e-p elastic cross section in kinematics similar to other JLab

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

Time of Flight measurements with MCP-PMT

Time of Flight measurements with MCP-PMT International Symposium on the Development of Detectors, 2006/4 at SLAC Time of Flight measurements with MCP-PMT - Very high resolution TOF counter - Lifetime of MCP-PMTs T.Ohshima, K.Inami, N.Kishimoto,

More information

Overview on Compton Polarimetry

Overview on Compton Polarimetry General Issues O spin motion & alignment tolerances O beam-beam effects & upstream vs. Downstream Compton Polarimetry Basics O beam parameters & Compton detection methods O kinematics, cross sections &

More information

Electron Beam Polarimetry at JLab Hall C Dave Gaskell PST 2009 September 7, 2009

Electron Beam Polarimetry at JLab Hall C Dave Gaskell PST 2009 September 7, 2009 Electron Beam Polarimetry at JLab Hall C Dave Gaskell PST 2009 September 7, 2009 1. Møller Polarimeter 2. Compton Polarimeter 3. Summary JLab Polarimetry Techniques Three different processes used to measure

More information

Polarimetry in Hall A

Polarimetry in Hall A Outline E.Chudakov Moller-12 Workshop, Aug 2008 Polarimetry in Hall A 1 Polarimetry in Hall A E.Chudakov 1 1 Hall A, JLab Moller-12 Workshop, Aug 2008 Outline E.Chudakov Moller-12 Workshop, Aug 2008 Polarimetry

More information

The Jefferson Lab 12 GeV Program

The Jefferson Lab 12 GeV Program The Jefferson Lab 12 GeV Program The Jefferson Lab facilities have undergone a substantial upgrade, both of accelerator, CEBAF, and of the experimental installations. We will discuss the progress to completion

More information

MTV - S1183 Beam Time Summary. Performance test of MTV new detector : CDC. Yumi Totsuka. Department of Physics, Rikkyo University, Tokyo, Japan

MTV - S1183 Beam Time Summary. Performance test of MTV new detector : CDC. Yumi Totsuka. Department of Physics, Rikkyo University, Tokyo, Japan MTV - S1183 Beam Time Summary Performance test of MTV new detector : CDC Yumi Totsuka Department of Physics, Rikkyo University, Tokyo, Japan TRIUMF-ISAC Science Forum (30. Nov. 2011) Schedule: Beam Time

More information

Achim Denig Institute for Nuclear Physics Johannes Gutenberg University Mainz. Dark Photon Searches at MAMI and MESA

Achim Denig Institute for Nuclear Physics Johannes Gutenberg University Mainz. Dark Photon Searches at MAMI and MESA Achim Denig Institute for Nuclear Physics Johannes Gutenberg University Mainz Dark Photon Searches at MAMI and MESA / Mainz Achim Denig Dark Photon New massive force carrier of extra U(1) d gauge group;

More information

Particle and Nuclear Physics Facilities A summary of approved experiments. K. Nishikawa KEK June 5, 2008

Particle and Nuclear Physics Facilities A summary of approved experiments. K. Nishikawa KEK June 5, 2008 Particle and Nuclear Physics Facilities A summary of approved experiments K. Nishikawa KEK June 5, 2008 1 Two stage aapproval The stage-1 approval This will be given by the IPNS director based on the recommendation

More information

Large Acceptance High Luminosity Detector at 12 GeV

Large Acceptance High Luminosity Detector at 12 GeV Outline Large Acceptance High Luminosity Detector at 12 GeV E.Chudakov 1 1 Hall A, JLab For June 2006 Hall A Meeting Outline Outline 1 Motivation for a Large Acceptance at High Luminosity DIS Parity Violation

More information

Electroproduction of p-shell hypernuclei

Electroproduction of p-shell hypernuclei Electroproduction of p-shell hypernuclei ASTRA workshop Petr Bydžovský Nuclear Physics Institute, Řež, Czech Republic in collaboration with D.J. Millener (BNL), F. Garibaldi and G.M. Urciuoli (Rome) Outline:

More information

arxiv: v2 [nucl-ex] 13 Aug 2014

arxiv: v2 [nucl-ex] 13 Aug 2014 The experiments with the High Resolution Kaon Spectrometer at JLab Hall C and the new spectroscopy of ΛB hypernuclei arxiv:146.233v2 [nucl-ex] 13 Aug 214 L. Tang, 1, 2, C. Chen, 1 T. Gogami, 3 D. Kawama,

More information

Strangeness nuclear physics at J-PARC

Strangeness nuclear physics at J-PARC KEK-HN-2017 2017. 1. 10 Strangeness nuclear physics at J-PARC Tohoku University H. Tamura Contents 1. Introduction 2. S = -1 systems --- Charge symmetry breaking in LN interaction 3. S = -2 systems ---

More information

DETERMINATION OF THE LINEAR POLARIZATION FOR THE HALL-B PHOTON BEAM AT JLAB

DETERMINATION OF THE LINEAR POLARIZATION FOR THE HALL-B PHOTON BEAM AT JLAB DETERMINATION OF THE LINEAR POLARIZATION FOR THE HALL-B PHOTON BEAM AT JLAB Arthur A. Sabintsev For the CLAS Collaboration The George Washington University Washington, DC U.S.A. 1 Background Information

More information

DIS and SIDIS measurements with BigBite & Super Bigbite Spectrometer and 11 GeV beam in Hall A

DIS and SIDIS measurements with BigBite & Super Bigbite Spectrometer and 11 GeV beam in Hall A DIS and SIDIS measurements with BigBite & Super Bigbite Spectrometer and 11 GeV beam in Hall A B. Wojtsekhowski, JLab 23 Sep 2009 B. Wojtsekhowski INT 12 GeV JLab 1 One- and Two-Arm experiments (O&TA)

More information

Particle Identification at a super B Factory. FRASCATI WORKSHOP DISCUSSION ON PID

Particle Identification at a super B Factory. FRASCATI WORKSHOP DISCUSSION ON PID Particle Identification at a super B Factory. FRASCATI WORKSHOP DISCUSSION ON PID Do no harm! ( The Hippocratic oath of detector designers, especially for those outside you ). Keep a minimum thickness

More information

The Angular Dependence of 16 O(e, e K + ) 16 ΛN and. (Proposal to JLab PAC-31)

The Angular Dependence of 16 O(e, e K + ) 16 ΛN and. (Proposal to JLab PAC-31) The Angular Dependence of 16 O(e, e K + ) 16 ΛN and H(e, e K + )Λ (Proposal to JLab PAC-31) E. Cisbani, F. Cusanno, S. Frullani, F. Garibaldi (spokesperson and contact person), M.L. Magliozzi Istituto

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

Study of Light Hypernuclei by Pionic Decay at JLab

Study of Light Hypernuclei by Pionic Decay at JLab Study of Light Hypernuclei by Pionic Decay at JLab N. Grigoryan, S. Knyazyan, A. Margaryan (spokesperson), G. Marikyan, L. Parlakyan, S. Zhamkochyan, H. Vardanyan Yerevan Physics Institute, 375036 Yerevan,

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

2007/11/11 J-PARC ハドロン実験施設ビームライン整備拡充に向けて S= 2 原子核実験. T.Takahashi (KEK)

2007/11/11 J-PARC ハドロン実験施設ビームライン整備拡充に向けて S= 2 原子核実験. T.Takahashi (KEK) 2007/11/11 S= 2 原子核実験 T.Takahashi (KEK) Contents Introduction Motivation to Study S=-2 System Experiments at Early Stage Spectroscopy of Ξ-Nucleus Future Plans Summary 2007/11/11 Motivation to Study S=

More information

Simulation for Proton Charge Radius (PRad) Experiment at Jefferson Lab1 Li Ye Mississippi State University For the PRad Collaboration The Proton Charg

Simulation for Proton Charge Radius (PRad) Experiment at Jefferson Lab1 Li Ye Mississippi State University For the PRad Collaboration The Proton Charg Simulation for Proton Charge Radius (PRad) Experiment at Jefferson Lab1 Li Ye Mississippi State University For the PRad Collaboration The Proton Charge Radius Puzzle refers to 7 σ discrepancy between the

More information

Upgrade of the Proximity Focusing RICH at JLab

Upgrade of the Proximity Focusing RICH at JLab Upgrade of the Proximity Focusing RICH at JLab E. Cisbani Istituto Superiore di Sanità and INFN Roma, Sanità group RICH2007 15-20 October 2007, Trieste - Italy E. Cisbani (ISS - INFN Rome) RICH Upgrade

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

Experiment of the 30 cm-cube ETCC under the Intense Radiations with Proton Beam

Experiment of the 30 cm-cube ETCC under the Intense Radiations with Proton Beam Experiment of the 30 cm-cube ETCC under the Intense Radiations with Proton Beam Contents Y. Matsuoka T. Tanimori, H. Kubo, A. Takada, J. D. Parker, T. Mizumoto, Y. Mizumura, S. Sonoda, D. Tomono, S. Iwaki,

More information

Hall C Users Meeting. January 22-23, 2010

Hall C Users Meeting. January 22-23, 2010 Hall C Users Meeting January 22-23, 2010 Experiments completed in last year Exp Title Spin Asymmetries of the Nucleon Experiment E07-003 (SANE) Spokespersons S. Choi, M. Jones, Z. E. Meziani, O. Rondon

More information

SEARCHING FOR DARK PHOTONS WITH POSITRONS AT JEFFERSON LAB

SEARCHING FOR DARK PHOTONS WITH POSITRONS AT JEFFERSON LAB SEARCHING FOR DARK PHOTONS WITH POSITRONS AT JEFFERSON LAB Luca Marsicano INFN Genova,Università Di Genova International Workshop on Physics with Positrons at Jefferson Lab September 12-15, 2017 Thomas

More information

Beam Polarimetry (for Future Experiments at JLab)

Beam Polarimetry (for Future Experiments at JLab) Outline E.Chudakov June 24, 2009, PAVI-09 Beam Polarimetry 1 Beam Polarimetry (for Future Experiments at JLab) E.Chudakov 1 1 JLab PAVI-09 Outline E.Chudakov June 24, 2009, PAVI-09 Beam Polarimetry 2 Outline

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 Mainz Microtron MAMI

The Mainz Microtron MAMI The Mainz Microtron MAMI Hans-Jürgen Arends Institut für Kernphysik Johannes Gutenberg-Universität Mainz Race-Track-Mikrotron D E out =z E L i+1 L i L 1 E λ coherence condition: (for lowest possible energy

More information

Hall-D Update. Eric Pooser. Joint Hall A/C Summer Collaboration Meeting 07/18/2015

Hall-D Update. Eric Pooser. Joint Hall A/C Summer Collaboration Meeting 07/18/2015 1 Hall-D Update Joint Hall A/C Summer Collaboration Meeting 07/18/2015 Current Hall-D Physics Program 2 Slide Courtesy of E. Chudakov Hybrid & Exotic Hybrid Mesons 3 Conventional light mesons (π, K, η,

More information

E : Ratio of the electric form factor in the mirror nuclei 3 He and 3 H (The 3 He 3 H Charge Radius Difference)

E : Ratio of the electric form factor in the mirror nuclei 3 He and 3 H (The 3 He 3 H Charge Radius Difference) E12 14 009: Ratio of the electric form factor in the mirror nuclei 3 He and 3 H (The 3 He 3 H Charge Radius Difference) Luke Myers Hall A Winter Meeting December 9, 2014 Measuring r 2 Absolute methods

More information

arxiv: v1 [nucl-ex] 2 Apr 2009

arxiv: v1 [nucl-ex] 2 Apr 2009 1 arxiv:0904.0298v1 [nucl-ex] 2 Apr 2009 PRODUCTION OF NEUTRON-RICH LAMBDA HYPERNUCLEI AT J-PARC A. SAKAGUCHI a, S. AJIMURA b, H. BHANG c, L. BUSSO d,e, M. ENDO a, D. FASO d,e, T. FUKUDA f, T. KISHIMOTO

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

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

Mukesh Saini. Florida State University, Tallahassee, FL. February 26, FSU Nuclear Physics Seminar. February 26

Mukesh Saini. Florida State University, Tallahassee, FL. February 26, FSU Nuclear Physics Seminar. February 26 C o l u m n 3 Mukesh Saini Florida State University, Tallahassee, FL, 2010 1 OUTLINE Introduction Meson Spectroscopy Strangeonia Experiment CEBAF & CLAS HyCLAS & g12 Calibrations Analysis Summary 2 QCD

More information

NEPTUN-A Spectrometer for measuring the Spin Analyzing Power in p-p elastic scattering at large P~ at 400 GeV (and 3 TeV) at UNK.

NEPTUN-A Spectrometer for measuring the Spin Analyzing Power in p-p elastic scattering at large P~ at 400 GeV (and 3 TeV) at UNK. NEPTUN-A Spectrometer for measuring the Spin Analyzing Power in p-p elastic scattering at large P~ at 400 GeV (and 3 TeV) at UNK. 1 All M. T. Lin Randall [.aboratory of Physics The University of Michigan,

More information

Isospin symmetry structure of J π =1 + states in 58 Ni and 58 Cu studied by high-resolution 58 Ni( 3 He,t) and 58 Ni(p,p ) measurements

Isospin symmetry structure of J π =1 + states in 58 Ni and 58 Cu studied by high-resolution 58 Ni( 3 He,t) and 58 Ni(p,p ) measurements Workshop at ECT*, Torento, 27/09/09-02/10/09 Strong, Weak and Electromagnetic Interactions to probe Spin-Isospin Excitations Isospin symmetry structure of J π =1 + states in 58 Ni and 58 Cu studied by

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

High-t Meson Photoproduction: Experimental Capabilities

High-t Meson Photoproduction: Experimental Capabilities High-t Meson Photoproduction: Experimental Capabilities Yordanka Ilieva University of South Carolina Workshop on Probing Small-Size Configurations in High-t Photo/Electroproduction Jefferson Lab March

More information

Møller Polarimetry for PV Experiments at 12 GeV

Møller Polarimetry for PV Experiments at 12 GeV Outline E.Chudakov Jan 15, 2010, MOLLER Review Møller Polarimetry 1 Møller Polarimetry for PV Experiments at 12 GeV E.Chudakov 1 1 JLab MOLLER Review Outline E.Chudakov Jan 15, 2010, MOLLER Review Møller

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

Decay-Pion Spectroscopy of Λ-Hypernuclei at MAMI

Decay-Pion Spectroscopy of Λ-Hypernuclei at MAMI Decay-Pion Spectroscopy of Λ-Hypernuclei at MAMI for the A1 Collaboration at MAMI Outline Experimental setup Pioneering run 2011 Experimental run 2012 Kaon identification Preliminary results This project

More information

September 20-21, 2010 JLAB, Newport News, USA. Achim Denig Institut für Kernphysik Johannes Gutenberg-Universität Mainz

September 20-21, 2010 JLAB, Newport News, USA. Achim Denig Institut für Kernphysik Johannes Gutenberg-Universität Mainz 1 September 20-21, 2010 JLAB, Newport News, USA Institut für Kernphysik Johannes Gutenberg-Universität Mainz 2 Outline Brief Introduction MAMI accelerator, experiments Experiences from Pilot Run (A1 Spectrometers)

More information

The intense, pulsed positron source EPOS at the Research Centre Dresden-Rossendorf

The intense, pulsed positron source EPOS at the Research Centre Dresden-Rossendorf The intense, pulsed positron source EPOS at the Research Centre Dresden-Rossendorf The EPOS Team and R. Krause-Rehberg Martin-Luther University, Halle-Wittenberg, Dept. of Physics, 06099 Halle / Germany

More information

Hypernuclear experiments at K1.1 in future. Tohoku University H. Tamura

Hypernuclear experiments at K1.1 in future. Tohoku University H. Tamura Hypernuclear experiments at K1.1 in future Tohoku University H. Tamura Contents 1. Gamma-ray spectroscopy of Λ hypernuclei at K1.1 2. Light Σ hypernuclei by (K -,π ±,0 ) at K1.1 3. γ decay of Σ hypernuclei

More information

The Aʹ Experiment (APEX)

The Aʹ Experiment (APEX) The Aʹ Experiment (APEX) Searching for New Gauge Bosons in the Aʹ Experiment at Jefferson Laboratory Natalia Toro (Perimeter Institute) for the APEX Collaboration S. Abrahamyan, Z. Ahmed, K. Allada, D.

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

Beam Asymmetry measurement in Pion Photoproduction on the neutron using CLAS

Beam Asymmetry measurement in Pion Photoproduction on the neutron using CLAS Beam Asymmetry measurement in Pion Photoproduction on the neutron using CLAS University of Glasgow, UK on behalf of the CLAS Collaboration MENU2013, Rome, Italy 1st October 2013 Meson Photoproduction Meson

More information