Design and construction of SMART Presented by Seigo Kato Nov. 12, 2005

Slides:



Advertisements
Similar presentations
Motivation Requirements Preliminary design Status Yaroslav Kalmykov Small Angle Magnet Institut für Kernphysik Technische Universität Darmstadt SFB 634.
Advertisements

Optics and magnetic field calculation for the Hall D Tagger Guangliang Yang Glasgow University.
Proposal of high-resolution eA collider spectrometer Seigo Kato Yamagata University.
Status of the Tagger Hall Background Simulation Simulation A. Somov, Jefferson Lab Hall-D Collaboration Meeting, University of Regina September
Tagger and Vacuum Chamber Design. Outline. Design considerations. Stresses and deformations. Mechanical assembly.
Magnet rotated by 5.9 degree Distance from entrance point to magnet right bottom corner m.
Tagger and Vacuum Chamber Design. Outline. Design considerations. Stresses and deformations. Mechanical assembly.
Possibility of bringing TRI  P to HIE-ISOLDE Dual magnetic Spectrometer Olof TENGBLAD ISCC Oct. 22nd 2013 There will be a presentation during the ISOLDE.
T. Horn, SHMS Optics Update SHMS Optics Update Tanja Horn Hall C Users Meeting 31 January 2009.
AWAKE Electron Spectrometer Design Simon Jolly 4 th September 2012.
Permanent Magnets Y. Iwashita Kyoto University. PMQ with saturated iron pole B=2Br (1-r 1 /r 2 ) cos 2 (π/M) sin(2π/M) /(2π/M)
Lecture 5: Electron Scattering, continued... 18/9/2003 1
Carbon Injector for FFAG
Spectroscopic Investigation of P-shell Λ hypernuclei by the (e,e'K + ) Reaction - Analysis Update of the Jlab Experiment E Chunhua Chen Hampton.
Optics and magnetic field calculation for the Hall D Tagger Guangliang Yang Glasgow University.
HYP03 Future Hypernuclear Program at Jlab Hall C Satoshi N. Nakamura Tohoku University 18 th Oct 2003, JLab.
Possible Spectrometer for eA Collider Seigo Kato Faculty of Science, Yamagata University, Yamagata , Japan Presented to the workshop "Rare-Isotope.
Medium heavy Λ hyper nuclear spectroscopic experiment by the (e,e’K + ) reaction Graduate school of science, Tohoku University Toshiyuki Gogami for HES-HKS.
HKS Analysis Status Report HKS Analysis Status Report Liguang Tang (Hampton/JLAB) Hall C User Meeting, Jan. 15, 2011 HKS has data taken in 2005 (E01-011)
SHMS Optics and Background Studies Tanja Horn Hall C Summer Meeting 5 August 2008.
Soft collective excitations in weakly bound nuclei studied with ELI-NP A.Krasznahorkay Inst. of Nuclear Research of the Hung. Acad. of Sci. (ATOMKI)
Spectrometer Optics John J. LeRose. The Basics Charged particles moving through static magnetic fields.  Magnetic Rigidity Local radius of curvature.
Neutron transfer reactions at large internuclear distances studied with the PRISMA spectrometer and the AGATA demonstrator.
W. Decking, M. Dohlus, C. Gerth, A. Krasnov, S. Lederer, T. Limberg, N. Mildner, D. Noelle FEL Beam Dynamics Meeting, XFEL Bunch Compressor.
SHMS Optics Studies Tanja Horn JLab JLab Hall C meeting 18 January 2008.
Development of the neutron counters for the Spin dipole resonance Kazuhiro Ishikawa.
RESEARCH and DEVELOPMENT for CBM (at LHE JINR) Yu.V. Zanevsky Laboratory of High Energies JINR, Dubna - NEW INFRASTRUCTURE - FAST GAS DETECTORS - DIPOLE.
The Readout Electronics for Upgrading of BESIII End-capTOF Chunyan Yin University of Science and Technology of China University of Science and Technology.
GlueX Collaboration Meeting. Jefferson Lab. September 9 – 11, Review of Tagger System.
Integrated Radiation Measurement and Radiation Protection of BES Ⅲ Zhang Qingjiang, Wu protection group, accelerator center, IHEP,
22 September 2005 Haw05 1  (1405) photoproduction at SPring-8/LEPS H. Fujimura, Kyoto University Kyoto University, Japan K. Imai, M. Niiyama Research.
Optics considerations for ERL test facilities Bruno Muratori ASTeC Daresbury Laboratory (M. Bowler, C. Gerth, F. Hannon, H. Owen, B. Shepherd, S. Smith,
Lecture 9: Inelastic Scattering and Excited States 2/10/2003 Inelastic scattering refers to the process in which energy is transferred to the target,
SHMS Spectrometer Update Hall C 2008 Users Meeting Paul Brindza January 18, 2008.
Tuesday, 02 September 2008FFAG08, Manchester Stephan I. Tzenov1 Modeling the EMMA Lattice Stephan I. Tzenov and Bruno D. Muratori STFC Daresbury Laboratory,
MEIC Detector and IR Integration Vasiliy Morozov, Charles Hyde, Pawel Nadel-Turonski MEIC Detector and IR Design Mini-Workshop, October 31, 2011.
Detector / Interaction Region Integration Vasiliy Morozov, Charles Hyde, Pawel Nadel-Turonski Joint CASA/Accelerator and Nuclear Physics MEIC/ELIC Meeting.
Present status of production target and Room design Takashi Hashimoto, IBS/RISP 2015, February.
J-Parc Neutrino Facility Primary Proton Beam Design A. K. Ichikawa(KEK), Y.Iwamoto(KEK) and K.Tanabe(Tokyo) et.al. 7 th Nov. 2003,
Ancillary/Complementary detectors for the AD at LNL.
Tagger and Vacuum Chamber Design Jim Kellie Glasgow University.
Understanding the 3 He Nuclei: Asymmetry Measurements in Quasi- Elastic Ge Jin University of Virginia For the E Collaboration.
SAMURAI magnet Hiromi SATO SAMURAI Team, RIKEN Requirements Geometry Magnetic field Superconducting coil and cooling system Present status of construction.
How to Design spectrometers Dec 15, 2012 Seigo Kato.
Status of the forward tracker design
Young Researchers Session in IFIN-HH 2016
A 3D design model of the apparatus for the Laser Wakefield Acceleration of electrons at ELI-NP S. Balascuta1 , R. Dinca1 1) “Horia Hulubei” National.
Bending crystals for magnetic and electric dipole moment measurements
Hall C Readiness Review – Small Angle SHMS Operation
▪ Issues after KOBRA review meeting
PANDA Yoke of the Magnet
IF Separator Design of RAON
Ben Cerio Office of Science, SULI Program 2006
Main magnets for PERLE Test Facility
Precision Measurement of the Electroproduction of p0 Near Threshold:
ISOLDE Workshop and Users Meeting 2017
Nathan Mertins, Michael Staib, William Bittner
1. Introduction Secondary Heavy charged particle (fragment) production
Hall “12 GeV” May 27, 2003 NAPP 2003: J.J. LeRose.
Recent Highlights and Future Plans at VAMOS
Hall C Users Meeting 31 January 2009
Hall C SHMS & Configuration Status
Cooler e-source Magnetized Beam LDRD Progress Report
Hall C SHMS & Configuration Status
RHIC Spin Flipper M. Bai, T. Roser Collider Accelerator Department
Fanglei Lin MEIC R&D Meeting, JLab, July 16, 2015
G.H. Wei, V.S. Morozov, Fanglei Lin Y. Nosochkov (SLAC), M-H. Wang
Crab Crossing Named #1 common technical risk (p. 6 of the report)
Fanglei Lin JLEIC R&D Meeting, August 4, 2016
Cooler e-source Magnetized Beam LDRD Progress Report
Presentation transcript:

Design and construction of SMART Presented by Seigo Kato Nov. 12,

Characteristics of a fixed-angle spectrometer Advantages cascade mode selectable resolution future extension (3-rd dipole) zero-degree measurement (beam stop at first stage) trace back to the target by double position detection no need of rotation mechanism and space heavy shield for detectors neutron TOF Disadvantages need of beam swinger need of arbitrary-angle twister beam dump to be discussed in this report

Layout of the experimental halls The concrete is not strong here.

Layout of SMART

Selectable resolution 41 % 20 msr 1/ % 10 msr 1/13000

Possible extension: a super-high-resolution mode

Ray-tracing

Beam swinger For the angular dependence measurements, the incoming beam direction is changed instead of the outgoing particle direction. pre-assembling at manufacturer’s factory configuration: DQQD bending: - 45 and +135 deg designed by H. Shimizu

Arbitrary-angle beam twister Because the direction of the dispersion in the beam swinger has to be within the median plane, we need a beam image rotator for arbitrary angles. effect of rotator S(  ) invert-rotator T(  )

before inversion after inversion Graphical understanding of the invert-rotator T(  ) is easy to obtain and is not inferior toas a rotator.

vertical inverter Trotation matrix R of the reference system invert-rotator T(  ) Calculation

Q-triplet is an incomplete inverter because we cannot specify * ’s. A Q-septet rotated by  /2 can rotate the beam image by  after vertical inversion. Q-septet is a complete inverter. reference: S. Kato, Nucl. Instr. & Meth. A254(1987)487 How to make a vertical inverter

Asymmetric quadrupole magnets between horizontal and vertical directions Bottom yokes of Q 1 and Q 2 are open for the beam dump. Q1Q1 Q2Q2 Q3Q3 left halves: field line curves right halves: field strength contours (convenient for Q-magnets)

Quadrupole magnets before installation Q 1 magnet being painted Q 3 (left) and Q 2 (right)

Total system installed

reference: T. Ichihara et al, Nucl. Phys. A569(1994)287c Performances

What was SMART for me from technical viewpoint? A big challenge to overcome many problems Hints to subsequent spectrometers QQD spectrometers such as BBS, HKS, HES fixed spectrometer proposed for GSI eA-collider Farewell to SMART I would like to express my thanks to the collaborators