J-PARC, facility for hadron physics, the present status and future T.Takahashi KEK/J-PARC Center.

Slides:



Advertisements
Similar presentations
May/27/05 Exotic Hadron WS 1 Hypothetical new scaler particle X for  + and its search by the (K +, X + ) reaction T. Kishimoto Osaka University.
Advertisements

HYPERNUCLEAR PHYSICS USING CEBAF BEAM PAST AND FUTURE Liguang Tang Hampton University/JLAB 4 th Workshop on Hadron Physics In China and Opportunities with.
Dense and Cold Nuclear Matter and Hard Exclusive ProcesssAug.24,2007 The J-PARC Hypernuclear Physics Programs - Hyperonization in dense nuclear matter.
James Ritman Univ. Giessen PANDA: Experiments to Study the Properties of Charm in Dense Hadronic Matter Overview of the PANDA Pbar-A Program The Pbar Facility.
A search for deeply-bound kaonic nuclear states by in-flight 3 He(K -,n) reaction at J-PARC Hiroaki Ohnishi RIKEN Nishina Center J-PARC E15 experiment.
J-PARC: Where is it? J-PARC (Japan Proton Accelerator Research Complex) Tokai, Japan 50 GeV Synchrotron (15  A) 400 MeV Linac (350m) 3 GeV Synchrotron.
HLab meeting 10/14/08 K. Shirotori. Contents SksMinus status –SKS magnet trouble –Magnetic field study.
HYP03 Future Hypernuclear Program at Jlab Hall C Satoshi N. Nakamura Tohoku University 18 th Oct 2003, JLab.
(Concluding) Remarks Ken Imai (JAEA/J-PARC) KEK Workshop on Hadron Physics with high-momentum beams at J-PARC
1 Hadron Physics at J-PARC Shin’ya Sawada 澤田 真也 KEK (High Energy Accelerator Research Organization, Japan) ECT*, Feb
Working Group 5 Summary David Christian Fermilab.
Medium heavy Λ hyper nuclear spectroscopic experiment by the (e,e’K + ) reaction Graduate school of science, Tohoku University Toshiyuki Gogami for HES-HKS.
June 20, 2008Shin'ya Fermilab E9061 J-PARC and Dimuon Experiments Shin’ya Sawada KEK (High Energy Accelerator Research Organization, Japan)
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.
Atsushi Tokiyasu (for LEPS collaboration) Experimental Nuclear and Hadronic Physics Laboratry, Department of Physics, Kyoto University.
Hadron Physics Experiments at J-PARC - Current Status and Future Prospects Megumi Naruki (KEK)
Possibility for hypernuclei including pentaquark,   Kiyoshi Tanida (Seoul National Univ.) 19 Sep 2009 High resolution search for   &
The search for deeply bound kaonic nuclear states at J-PARC Toshihiko Hiraiwa Kyoto University On behalf of the J-PARC E15 collaboration.
Brad Sawatzky / JLAB Acknowledgements to Liguang Tang Hampton University/JLAB MESON 2012 Krakow, Poland.
Spin at J-PARC Naohito Saito for Shoji Nagamiya. Executive Summary Spin physics at J-PARC, now The facility is starting up; Only spin physics would be.
 meson in nucleus at J-PARC Hiroaki Ohnishi RIKEN New Frontiers in QDC Exotic Hadron Systems and Dense Matter – Mini Symposium on Exotic hadrons.
1 Hypernuclear spectroscopy up to medium mass region through the (e,e’K + ) reaction in JLab Mizuki Sumihama For HKS collaboration Department of Physics.
Antiproton Physics Experiments Keith Gollwitzer -- Fermilab Antiproton Sources Accumulator Antiproton Physics Experiments –Precision measurements Method.
Particle and Nuclear Physics at J-PARC July 16, 2003 Lattice 2003 Jun Imazato KEK, IPNS.
Setup for hypernuclear gamma-ray spectroscopy at J-PARC K.Shirotori Tohoku Univ. Japan for the Hyperball-J collaboration J-PARC E13 hypernuclear  -ray.
Status of E391a Search for K L    decay G.Y.Lim IPNS, 32nd ICHEP 19 th August 2004 Beijing.
Omega meson in nucleus, experimental study K. Ozawa (Univ. of Tokyo)
Hypernuclear spectroscopy using (K - stop,  0 ) and (e,e’K + ) reactions Doc. dr. sc. Darko Androić University of Zagreb Physics Department.
Hiroaki Ohnishi RIKEN For the J-PARC E15 collaboration A search for deeply bound kaonic nuclear states by in-flight 3 He(K -,n) reaction ストレンジネスとエキゾティクス・理論の課題.
S=  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.
JLab Hypernuclear Workshop 27 th May 2014 Satoshi N Nakamura, Tohoku University HKS HES Results from Hall-C.
J-PARC Accelerators Masahito Tomizawa KEK Acc. Lab. Outline, Status, Schedule of J-PARC accelerator MR Beam Power Upgrade.
Cross section of elementally process [5] The  -ray spectroscopy of light hypernuclei at J-PARC (E13) K. Shirotori for the Hyperball-J collaboration Department.
Recent Studies of Hypernuclei Formation with Electron Beams at MAMI Patrick Achenbach U Mainz Sept. 2o13.
Prospects for Hadron Physics in Asia H. Shimizu Laboratory of Nuclear Science Tohoku University,
A search for deeply-bound kaonic nuclear states in (in-flight K -, N) reaction Hiroaki Ohnishi RIKEN.
Hadron Spectroscopy with high momentum beam line at J-PARC K. Ozawa (KEK) Contents Charmed baryon spectroscopy New experiment at J-PARC.
Study of Neutron-Rich  Hypernuclei Tomokazu FUKUDA Osaka Electro-Communication University 2013/09/091EFB 22.
22 September 2005 Haw05 1  (1405) photoproduction at SPring-8/LEPS H. Fujimura, Kyoto University Kyoto University, Japan K. Imai, M. Niiyama Research.
SksMinus status Hyperball collaboration meeting 2009/3/11 K. Shirotori.
J-PARC Heavy ion program and related topics K. Ozawa (KEK)
G-2, EDM, COMET muon particle physics programmes at J-PARC Mu_01 Satoshi MIHARA IPNS, KEK FKPPL-FJPPL workshop, Yonesei Univ.
Magnetic Moment of a  in a Nucleus H. Tamura Tohoku University 1. Introduction 2.  -ray spectroscopy of  hypernuclei and spin-flip B(M1) 3. Experiments.
(F.Cusanno, M.Iodice et al,Phys. Rev. Lett (2009). 670 keV FWHM  M. Iodice,F.Cusanno et al. Phys.Rev.Lett. 99, (2007) 12 C ( e,e’K )
Dec7,2007 ie-FP7 Test Beams for detector R&D at CERN The PS East Area The SPS North Area Irradiation facilities.
Dec. 1, 2005S. Sawada / J-PARC-HS051 Dimuon measurement at J-PARC (LoI-15: Physics of high-mass dimuon production at the 50-GeV Proton Synchrotron) Shin’ya.
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.
Master thesis 2006 Shirotori1 Hypernuclear gamma-ray spectroscopy at J-PARC K1.8 beam line 東北大学大学院理学研究科 原子核物理 白鳥昂太郎.
Status of facility design Activities of the IPNS Nuclear/Particle Physics group Basic information for the working sessions Activities of Nuclear and Particle.
1 Status of the T2K long baseline neutrino oscillation experiment Atsuko K. Ichikawa (Kyoto univeristy) For the T2K Collaboration.
Study of Light  -Hypernuclei by Spectroscopy of Two Body Weak Decay Pions Liguang Tang Department of Physics, Hampton University Jefferson National Laboratory.
Study of light hypernuclei by the (e,e’K + ) reaction Graduate school of science, Tohoku Univ. Toshiyuki Gogami JLab E collaboration, 2009, JLab.
J-PARC における 4  He の生成と構造の研究 東北大学 大学院理学研究科 白鳥昂太郎 for the Hyperball-J Collaboration.
Hypernuclear gamma-ray spectroscopy at J-PARC K1.8 Beam line Tohoku Univ. K.Shirotori 東北大学 大学院理学研究科 白鳥昂太郎.
December 1, 2005Shin'ya Hadron Structure at J-PARC 1 Japan Proton Accelerator Research Complex J-PARC - Nuclear and Particle Physics Facility.
1 Heavy-Ion Physics at J-PARC Shoji Nagamiya RIKEN / KEK / JAEA January 20, 2016 Tokai 1) Motivation 2) J-PARC vs. FAIR.
Experimental Activities at University of Tokyo K. Ozawa (University of Tokyo) (University of Tokyo)
Search for the K  pp bound state via the in-flight 3 He(K ,n) reaction MESON2014 Yuta Sada for the E15 collaboration RCNP, Osaka Univ & RIKEN 1.
Past Fermilab Accumulator Experiments Antiproton Source Accumulator Ring (Inner Ring) Debuncher Ring (Outer Ring) AP50 Experiment Area PRECISION Precision.
Stopped K beam at J-PARC Designed by J.Doornbos 1)Optics design of a K0.8 branch 2)Performance 3)Pion contamination 4)Comments on K1.1 Nov. 4, 2005 Korea.
Cascade Baryon Spectroscopy with Kaon Beams M. Naruki (Kyoto Univ) 2016/5/17, Tallahassee, Baryon
Hypernuclear Spectroscopy with Electron Beams
Florida International University, Miami, FL
Hadron experimental facility at J-PARC
The First
Kaon beam at K1.1BR KEK Jun Imazato.
平岩聡彦 京都大学 On behalf of the J-PARC E15 collaboration
Progress on J-PARC hadron physics in 2016
Search for Exotic Hadrons, H-dibaryon resonance and Pentaquark
高強度高分解能2次ビームラインを用いたハイパー核研究
Presentation transcript:

J-PARC, facility for hadron physics, the present status and future T.Takahashi KEK/J-PARC Center

Contents Brief Introduction of J-PARC Hadron Facility  Results of Commissioning and Physics Programs at each beamline K1.8/K1.8BR/K1.1BR  Beamlines to be constructed in future High-p/K1.1 Summary

J-PARC at Tokai Village

ML F RCS LIN AC 50GeV-PS (MR) Hd Bird’s eye photo in Feb. 2008

High-power & multi-purpose accelerator IPNS Energy (GeV) AGS CERN-PS FNAL-MI U70 SPS ISIS TRIUMF PSI (CW) KEK- 12GeV PS Tevatron This Project 3 GeV Existing Under construction Power KEK-500MeV Booster Current (  A) SNS Proposed Materials-Life Sciences 1 MW 0.1 MW ESS Nuclear-Particle Physics This Project 50 GeV J-PARC = 1MW-class high-power accelerators 10-times beam power of any existing accelerators

Pions (  ) Kaons (K) Anti-proton ( p) Neutron (n) High-power & multi-purpose accelerator proton(p) Target nucleus neutron(n) Muon (  ) Neutrino( ) Particle & Nuclear 50(30) GeV Materials & Life Nuclear Proton beam (p) 3GeV/50(30)GeV

Hadron Experimental Hall Photo was taken in Oct Hadron Experimental Hall

Hadron Facility Hadron Hall Switch Yard (SY) Tunnel Beam Dump MR Tunnnel Production Target (T1) Primary Beam LineSlow extraction point Main Ring (MR) SY ( ~ 250m) Hadron Hall (56m) MR Main Ring to Hadron Hall 60m

Nuclear & Hadron Physics at Hadron Hall  multi-strangeness hypernuclei  6  He double-  K − Meson X-ray Nucleus kaonic atom kaonic nuclei  d u u d s Pentaquark  + Hypernuclear Physics Exotic Hadrons Origin of Hadron Mass  -ray spectroscopy K N Interaction K1.8 K1.8BR KL K1.1 K1.1BR High-P

Beam lines in Hadron Hall p max = 1.1 GeV/c I K ~ GeV/c p max = 2.0 GeV/c I K ~ GeV/c Double stages Electrostatic Separators K  /(   +   )  p max = 0.8 GeV/c I K ~ GeV/c as Kaon Factory (2x10 14 ppp, 30GeV-9  A) p mean ~2 GeV/c I KL = 1.8x10 7 ppp pencil-beam of 7.8  sr Ni Target K L    bar rare-decay exp.

K1.8 & SKS SKS K1.8 Beam Spectrometer

K1.8 beam line P max =2.0 GeV/c 46m Length double stage of Electrostatic Separators 75kV/cm,6m x 2 High-resolution beam spectrometer (K1.8BS)  p/p =3.3x10  (FWHM) ESS#1 ESS#2 ESS#1 BS(QQDQQ) 2.0x10 14 ppp, Ni K   Intensity: 1.4x10 6 K  /(     )=3.5  IFV =4.0mm  MS1=4.5mm  MS2=4.8mm design value

Kaon Yield at K1.8 w/o fine tune ESS1 ON ESS2 ON K 2009 Nov.26 Separators ±200kV IFH ± 100mm IFV 0/+4mm Mom ± 60mm MS1 ± 2.35mm MS2 ± 2.5mm ← 1/3 of full ESS1 OFF ESS2 OFF 6.2x10 11 ppp (500W) Ni Target 3.6k/spill K Separators ±200kV (±375kV) IFV opening 2.0 mm (4.0mm) MS1 opening 4.7mm (4.5mm) MS2 opening 5.0mm (4.8mm) 2010 Oct x10 12 ppp (1kW) Pt Target  KK K-trigger p bar All charged particles K-trigger 12k/spill

Trouble 1/6 of coil was lost due to earth fault Beam & SKS Spectrometer - Performance - SKS from Tsukuba to Tokai for High-resolution Spectroscopy of Hypernuclei, etc.. Large solid angle of 100msr High resolution of  p/p ~ 0.1%(FWHM) 300W refrigerator for Liq-He Small refrigerator system GM-JT refrigerator x 3 GM cryocooler for GM-JT shield GM cryocooler for HiTC current leads A Measured field map Calcurated field map at 1.25GeV/c

Approved Experiments at K1.8 Exotic Hadron/Hadron system  E19   Search via the H(  ,K  )X  E27 Kaonic nuleus via the D(  ,K + )”ppK  ” Hypernuclei of S=-1  E10 n-rich  hypernuclei via the (  ,K + ) reaction ( 6  H, 9  He)  E13  -ray spectroscopy ( 4  He, 7  Li, 10  B, 11  B, 19  F )  E18/E22 weak decays ( 4  H/ 4  He, 12  C ) Hypernuclei of S=-2  E05  -hypernucleus, via the 12 C(K ,K + ) 12  Be  E07 Counter-emulsion hybrid experiment  E03 Measurement of  -Atom X-rays (  -Fe Atom) Others  E08 Pion double charge exchange  E26  in nuclei by A(  ,n) reaction and   

E19: Search for penta-quark,  , via the p+   → K  X reaction The First PHYSICS EXPERIMENT at Hadron Hall. u ー s u d d To confirm the bump-sructure observed in the previous E522 experiment with much improved resolution better than 2MeV/c 2 S/N using Liq-H 2 target statistics with high-intensity beam 7.8x10 10    on 12cm-long Liq-H 2 at 1.92GeV/c Step-1 data taking was successfully finished in this autumn. M.Naruki on Dec.10 E522 CH 2 (  ,K  ) GeV/c 2

Hypernuclear Physics N Z ,  Hypernuclei ,  Hypernuclei Strangeness    N-N int. by Lattice QCD Baryon-Baryon interaction through the hypernuclear structure   N and  interaction   N interaction in n-rich enviroment Hadron property in nuclear medium  g-factor of  by B(M1) measurement Change of nuclear property by additon of hyperon(s)  change of nuclear size etc..

K1.8BR CDS detector 3 He target

K1.8BR beamline P max =1.1 GeV/c 31.3m Length Electrostatic Separator (50kV/cm,6m) 2.0x10 14 ppp, Ni target K  intensity 7.5x10 1.1GeV/c 1.0x10 0.8GeV/c 8.4x10 0.6GeV/c SlitNiPt K/  (Pt)  IFV=4mm,  MS1=4.7mm %  IFV=4mm,  MS1=9.2mm % K Yield (Measured ) 1.5x10 12 ppp, 40kV/cm (design)

Approved Experiments at K1.8BR Kaonic nuclei, K bar -N interaction  E17 Measurement of Kaonic 3 He 3d  2p X-rays  E15 Kaon deeply bound state, “ppK  ” via the 3 He(K ,n)X and X  (  p)  pp    P28 ( 3 He(K ,p/n)X )  E31 Hyperon resonance below KN threshold via the D(K ,n) reaction

E17:Strong-interaction Shift and Width of Kaonic Helium 3 Last orbit of Kaonic atoms is sensitive to K - -nucleus strong-interaction. Nucleus absorption 2p (Strong-interaction) 2p 3d 2p (Coulomb-only) 2p  E 2p : Shift  2p : Width Atomic orbits of Kaonic Helium 3 3d 2p X-rays Slide by Dr. M. Iio T.Hashimoto on Dec.10

+ K-K-K-K- 3 He NC 15 m + K - pp n Reaction Missing mass spectroscopy K - pp search with TOF measurement of neutron  pp ---- Decay Decay particle measurement K - pp search with exclusive decay particle measurement E15: Next to E17 M. iio, Slide for PANIC08 Y.Sada on Dec.10

K1.1BR

Actual layout of K1.1BR T1 D1 Q1 Q2 D2Q3 Q4ESSQ5 Q6 MS D3 Q7 Q8 IFX IFY SX1SX2 HFOC FF Proton beam Shorter length (2.0 m) of ESS instead of optics design (2.5 m) - old K5 ESS is reused - Smaller D3 bending angle (40°) than beam optics (45°) - performance limit of the recycled D3 magnet - Longer Q8-FF distance (3.3 m) than the beam optics (1.5 m) - a thick iron wall necessary for radiation safety -

Beam envelop (K1.1BR)  = 3.3 msr %  HFOC = ± 6 mm; I K + = 5.4 x 10 4  = 5.0 msr %  HFOC = ±20 mm; I K + = 8.2 x 10 4 (with Pt 1.0 GeV/c L = 21.5 m ESS Beam Analyzer D3 Q7 Q8

Measured K + Yield & 0.8GeV/c 4.5x10 12 ppp (3.6kW) Normal Vertical Slit Opening Test beamline for test exp. (for a while) TREK (Time-reversal Exp.) (future)

Other ( Approved ) Experiments Meson in nuclei, In-medium modification of mesons  E16 Chiral symmetry of QCD (  in High-P beamline  E29  -meson bound state via the A(p bar,  K1.1 beamline (deferred status)  P04 High-mass dimuon Primary (High-P) beamline

Beam lines in Hadron Hall K1.8 K1.8BR KL K1.1 K1.1BR High-P

E16: In-medium mass modification of vector meson R.Muto et al,PRL98 (07) KEK-E325 electron-pair spectrometer collect 10 4 ~10 5   ee for each target 10~100 times as large as the previous E325 data velocity dependence target (size) dependence  (1020)

Location of E16 : High-p beam line SM1: branched by 5° 2% beam loss is allowed 3.9° 5.8°x3 beam dump Experimental Area Vertical Bend Beam dump and shields are for protons/s 30 Already the spectrometer magnet has been moved to Hadron Hall. Budget being requested. R&D for the actual beam line is underway.

Summary J-PARC has started its operational era! 4 beam lines, K1.8, K1.8BR, KL, and K1.1BR, are completed.  K1.8 & SKS: Hypernuclear Physics Experiments E19 has finished the step-1 data-taking.  K1.8BR: E17/E15 are being started.  KL: K rare decay experiment (K L   bar ) started its engineering run.  K1.1BR: Commissioning and some test exp. started. We are requesting to construct K1.1 and High-p lines

People at J-PARC Hadron Experimental Hall Graduate Students, Professors, Researchers, Engineers…, all over the world First Beam to Hd Hall First beam to K1.8 KOTO (E15) Experimental Team (K L Rare Decay Search) Start up of K1.8 Counting Hat Front end circuits at K1.8BR New comers and a senior Line marking at K1.8 area Our TOF wall is ready! Midnight in KL Counting Hat Background survey before construction of KL! My beautiful TOF counters!