Development of Forward Aerogel Cherenkov Detector for the H-dibaryon search experiment (E42) at J-PARC Japan-Korea PHENIX Collaboration Meeting Minho Kim.

Slides:

Advertisements

Similar presentations

Neutrinos from kaon decay in MiniBooNE Kendall Mahn Columbia University MiniBooNE beamline overview Kaon flux predictions Kaon measurements in MiniBooNE.

Advertisements

NDVCS measurement with BoNuS RTPC M. Osipenko December 2, 2009, CLAS12 Central Detector Collaboration meeting.

1 A DIRC for GlueX Paul Mueller Oak Ridge National Laboratory and Stefan Spanier University of Tennessee, Knoxville BaBar DIRC Collaboration for the GlueX.

14 Sept 2004 D.Dedovich Tau041 Measurement of Tau hadronic branching ratios in DELPHI experiment at LEP Dima Dedovich (Dubna) DELPHI Collaboration E.Phys.J.

SUNJI KIM, H. BHANG, M. KIM, K. TSHOO, K. TANIDA, H. FUJIOKA1, Y. SADA1, and H. ASANO1 Seoul National University, 1 Kyoto University Abstract Introduction.

Mar 31, 2005Steve Kahn -- Ckov and Tof Detector Simulation 1 Ckov1, Ckov2, Tof2 MICE Pid Tele-Meeting Steve Kahn 31 March 2005.

Review of PID simulation & reconstruction in G4MICE Yordan Karadzhov Sofia university “St. Kliment Ohridski” Content : 1 TOF 2 Cerenkov.

1 KEK Beam Test Analysis Hideyuki Sakamoto 15 th MICE Collaboration Meeting 10 st June,2006.

Progress and plans on PID simulation and reconstruction Yordan Karadzhov Sofia university St. Kliment Ohridski.

Study of optical properties of aerogel

Jun 27, 2005S. Kahn -- Ckov1 Simulation 1 Ckov1 Simulation and Performance Steve Kahn June 27, 2005 MICE Collaboration PID Meeting.

27 Jun 2005S. Kahn -- Tof/Ckov Status1 Status of TOF and Ckov Sub- packages in G4Mice Steve Kahn 27 June 2005.

TOF/ACC test Overview M. Yoshida Osaka Univ.. TOF / ACC in the prototype test For the prototype test in May, we will need PID: –TOF counter Distinguish.

Update on the Gas Ring Imaging Cherenkov (GRINCH) Detector for A 1 n using BigBite Todd Averett Department of Physics The College of William and Mary Williamsburg,

The HERMES Dual-Radiator Ring Imaging Cerenkov Detector N.Akopov et al., Nucl. Instrum. Meth. A479 (2002) 511 Shibata Lab 11R50047 Jennifer Newsham YSEP.

HYP03 Future Hypernuclear Program at Jlab Hall C Satoshi N. Nakamura Tohoku University 18 th Oct 2003, JLab.

Report of the NTPC Test Experiment in 2007Sep and Others Yohei Nakatsugawa.

A Reconstruction Algorithm for a RICH detector for CLAS12 Ahmed El Alaoui RICH Workchop, Jefferson Lab, newport News, VA November th 2011.

Medium heavy Λ hyper nuclear spectroscopic experiment by the (e,e’K + ) reaction Graduate school of science, Tohoku University Toshiyuki Gogami for HES-HKS.

ハイパー核ガンマ線分光用磁気スペクトロメータ -SksMinus- 東北大学大学院理学研究科白鳥昂太郎 ATAMI.

QM2006 Shanghai, China 1 High-p T Identified Hadron Production in Au+Au and Cu+Cu Collisions at RHIC-PHENIX Masahiro Konno (Univ. of Tsukuba) for the PHENIX.

GlueX Particle Identification Ryan Mitchell Indiana University Detector Review, October 2004.

Lambda hypernuclear spectroscopy at JLab Hall-C Graduate School of Science, Tohoku University Toshiyuki Gogami for the HES-HKS collaboration 1.Introduction.

Feb 10, 2005 S. Kahn -- Pid Detectors in G4MicePage 1 Pid Detector Implementation in G4Mice Steve Kahn Brookhaven National Lab 10 Feb 2005.

Setup for hypernuclear gamma-ray spectroscopy at J-PARC K.Shirotori Tohoku Univ. Japan for the Hyperball-J collaboration J-PARC E13 hypernuclear  -ray.

Aerogel counter with a Fresnel lens

The calibration and alignment of the LHCb RICH system Antonis Papanestis STFC - RAL for the LHCb Collaboration.

Status of GlueX Particle Identification Ryan Mitchell September 10, 2004.

PID for super Belle (design consideration) K. Inami (Nagoya-u) - Barrel (TOP counter) - Possible configuration - Geometry - Endcap (Aerogel RICH) - Photo.

A search for deeply-bound kaonic nuclear states in (in-flight K -, N) reaction Hiroaki Ohnishi RIKEN.

Electron and identified hadron v 2 to look for hadronic or partonic origin of elliptic flow Shingo Sakai for the PHENIX Collaboration Univ. of Tsukuba.

Background Subtraction and Likelihood Method of Analysis: First Attempt Jose Benitez 6/26/2006.

22 September 2005 Haw05 1  (1405) photoproduction at SPring-8/LEPS H. Fujimura, Kyoto University Kyoto University, Japan K. Imai, M. Niiyama Research.

Nov Beam Catcher in KOPIO (H. Mikata Kaon mini worksyop1 Beam Catcher in the KOPIO experiment Hideki Morii (Kyoto Univ.) for the KOPIO.

KEK beam test in May 2005 Makoto Yoshida Osaka Univ. MICE Frascati June 27 th, 2005.

SksMinus status Hyperball collaboration meeting 2009/3/11 K. Shirotori.

HES HKS collaboration meeting 3/11/2010 T.Gogami.

KEK Test Beam Phase I (May 2005) Makoto Yoshida Osaka Univ. MICE-FT Daresbury Aug 30th, 2005.

Beam test of low index sillica aerogel Yukiyoshi Kon RCNP, Osaka University Collaboration 2008/5/2.

Search for the  + in photoproduction experiments at CLAS APS spring meeting (Dallas) April 22, 2006 Ken Hicks (Ohio University) for the CLAS Collaboration.

J-PARC でのハイパー核ガンマ線分光実験用散乱粒子磁気スペクトロメータ検出器の準備状況東北大理, 岐阜大教 A, KEK B 白鳥昂太郎, 田村裕和, 鵜養美冬 A, 石元茂 B, 大谷友和, 小池武志, 佐藤美沙子, 千賀信幸, 細見健二, 馬越, 三輪浩司, 山本剛史, 他 Hyperball-J.

Aerogel Cherenkov Counters for the ALICE Detector G. Paić Instituto de Ciencias Nucleares UNAM For the ALICE VHMPID group.

Radia Sia Syracuse Univ. 1 RICH 2004 Outline:  The CLEO-III RICH Detector  Physics Requirements  CLEO-III RICH at work… Performance of the CLEO-III.

Lambda hypernuclear spectroscopy up to medium heavy mass number at JLab Hall-C Graduate School of Science, Tohoku University Toshiyuki Gogami for the HES-HKS.

Il Ring Imaging CHerenkov (RICH) detector a Jefferson Lab – Hall A.

Particle identification by energy loss measurement in the NA61 (SHINE) experiment Magdalena Posiadala University of Warsaw.

RICH studies for CLAS12 L. Pappalardo1 Contalbrigo Marco Luciano Pappalardo INFN Ferrara CLAS12 RICH Meeting – JLab 21/6/2011.

Aerogel detector revisited Sokolov Oleksiy, UNAM, progress report, 20 Sept 2006 E int = M – wall reflectivity є – PMT relative area Belle geometry (traditional):

QM2002 (July / / Nantes / France)Susumu SATO (JSPS) for the PHENIX collaboration page 1 Susumu SATO Japan Society for the Promotion of Science,

CKOV1 design status 1. Generation of muon and pion beam files 2. PID performances with water radiator 3. Does it help with fluorocarbon FC72 ? 4. Conclusion.

Aerogel Čerenkov Requirements for the SHMS ( e,e’K + ) Program Hall C User’s Workshop, August 7, Garth Huber.

PhD thesis: Simulation & Reconstruction for the PANDA Barrel DIRC Official name: Open charm analysis tools Supervisor: Prof. Klaus Peters Maria Patsyuk.

Seoul National University On behalf of J-PARC E18 Collaboration

SHMS Aerogel Detector Construction is complete

“Performance test of a lead glass

E.A.Kravchenko Budker INP, Novosibirsk, Russia

High-pT Identified Hadron Production in Au+Au and Cu+Cu Collisions

Central detector for CLAS12: CTOF and Neutron detector

坂井　真吾　for the PHENIX Collaboration Shingo Sakai 　 Univ. of Tsukuba

Particle Identification in LHCb

Tatsuya Chujo for the PHENIX collaboration

K+ Identification in CERN experiment NA62

LHCb Particle Identification and Performance

High-pT Identified Charged Hadrons in √sNN = 200 GeV Au+Au Collisions

Identified Charged Hadron

Search for the onset of baryon anomaly at RHIC-PHENIX

Identified Charged Hadron Production at High pT

E19 result Ryuta Kiuchi (SNU)

Performance test of a RICH with time-of-flight information

Reconstruction and calibration strategies for the LHCb RICH detector

Presentation transcript:

Development of Forward Aerogel Cherenkov Detector for the H-dibaryon search experiment (E42) at J-PARC Japan-Korea PHENIX Collaboration Meeting Minho Kim Korea Univ.

Signal : p(K -, K + )Ξ - Background: p(K -, π + )Σ - H-Dibaryon Search Experiment, E42 KUNPL 2 KURAMA magnet ToF wall TPC Helmholtz magnet “AC detector” 1.7 GeV/c K - beam Drift chamber “H-dibaryon” Six quarks J π = 0 +

Forward Aerogel Cherenkov Detector 3 KUNPL π, K Fine-mesh PMT Strong to B field Parabolic reflector Light box Thin Al plate Aerogel n=1.04, 110×110×20 mm 3 Will be installed at the exit of Helmholtz magnet. Contents 1. Aerogel 2. Fine-mesh PMT 3. SPring-8 beam test

FAC Aerogel 4 Refractive index should be smaller than KUNPL Pion emits Cherenkov light. Kaon emits Cherenkov light. p min FAC can reject is about 0.48 GeV/c.

FAC PMT, fine-mesh PMT 5 KUNPL mean Npe = 1 Let’s assume one photoelectron  mean ADC, +Q. Bad resolution for photon counting. Mesh type dynode  Not Gaussian shaped amplification.

FAC Test Experiment at SPring-8 6 KUNPL 1. Parabola FAC 2. Teflon FAC 3. Winston cone FAC Installed at the very end of LEPS spectrometer.

FAC Setup KUNPL 7 PMT2 PMT16 Drawn by S.H. Kim W.S. Jung PMT1 PMT17 PMT1 PMT2 6/9~7/4 run 7/15~ 7/24 run PMT17 PMT16 Same |x|, |y| position. Similar pion momentum range with similar statistics.

FAC Installation KUNPL 8 480<x<700 mm 115<y<225 mm 480<x<700 mm -225<y<-115 mm Turned off

Particles which passed through FAC 9 KUNPL Momentum (GeV/c) Mass*charge(GeV/c 2 ) Below 3.0 GeV/c for protons. Above 0.5 GeV/c for pions. Mass*charnge (GeV/c 2 ) Counts π+π+ π-π- P K+K+ P K+K+ π+π+ Particle identification with ± 2σ tolerance. Kaon study  Pion study Wide range of momenta pions.

Pion Efficiency KUNPL Parabola FAC ADC threshold: Proton misidentification is less than 5 %. Pion efficiency = (Events which pion leaves ADC bigger than threshold) / (All pion events in specific momentum range) 10 Considered as pions. Considered as kaons.

Pion Efficiency 11 KUNPL Parabola FAC shows better performance. Maximum efficiency on average with neutron bar cut condition(>0.7 GeV/c). Teflon FAC Parabola FAC Pion momentum (GeV/c) Pion efficiency Pion momentum (GeV/c) Pion efficiency Winston FAC Parabola FAC Without nbar cut condition With nbar cut condition

Position Dependence of Efficiency 12 KUNPL Exterior Cherenkov light goes towards surrounding plane surface first. Perfect fit (to aerogel area) light box is not good. Parabola FAC Central Inclusive Boundary Maximum on average. Pion efficiency (GeV/c)

Npe Study 13 KUNPL Total (>0.7 GeV/c)0.7~0.8 GeV/c0.8~0.9 GeV/c 0.9~1.0 GeV/c1.0~1.1 GeV/c1.1~1.2 GeV/c 1.2~1.3 GeV/c 1.3~1.4 GeV/c1.4~1.5 GeV/c Npe Counts

Npe Study 14 KUNPL sin 2 θ1/β 2 mean Npe Since Cherenkov angle is smaller than 15 °, cosθ ≈ 1.

Summary & Plan 15 KUNPL We tested three types of FAC and studied corresponding pion efficiency. We’re checking pion efficiency and Npe again. From middle of November, we will start the test of full size FAC mockup.