16th Crystal Ball Meeting October, 11-13, 2010, Dubrovnik Grigory Gurevich, Yuri Usov Dubna-Mainz Dilution Cryostat of the New Frozen-Spin Target.

Slides:



Advertisements
Similar presentations
Participants: C-1:Cryogenic last-stage suspensions (interferometers) (F.Ricci-G.Frossati) Objectives: -Design new suspension elements for the last stage.
Advertisements

The Use of Small Coolers for Hydrogen and Helium Liquefaction
Patricia Aguar Bartolomé Institut für Kernphysik, Universität Mainz PSTP 2013 Workshop, Charlottesville 11th September 2013.
A polarized solid state target for photon induced double polarization experiments at ELSA H. Dutz TR16 Bommerholz Hartmut Dutz, S. Goertz, A.
Mauricio Martínez Fabregate Dubrovnik, April 8th 2008 Crystal Ball Meeting 7th -9th April, Dubrovnik Status of the Mainz Frozen Spin Target Institut für.
Zian Zhu Superconducting Solenoid Magnet BESIII Workshop Zian Zhu Beijing, Oct.13,2001.
HD group LEPS RCNP C. Morisaki. ① Development of NMR measurement system for the polarized HD target ② Development of single crystal HD target.
Guenther Rosner FAIR Design Study, PANDA 3, GSI, 19/1/06 1 PANDA3: Magnet design and integration of detectors Tasks & participants Progress Milestones.
Institut für Kernphysik Bosen th August 2010 Andreas Thomas Polarised Targets for Photoproduction Experiments.
Available thin solenoids with dimensions of about 1 m  X 1 mL with field about 1 tesla in KEK/IPNS KEK/IPNS Y.Makida 2005/March/28.
Status of the Polarized 3He Target
Vacuum, Surfaces & Coatings Group Technology Department Vacuum tests for CLIC module prototypes 6 November 2013 C. Garion2 Outline: Reminder: specification.
ILC Main Linac Superconducting Cryogen Free Splittable Quadrupole Progress Report V. Kashikhin for Superconducting Magnet Team.
Superconducting Large Bore Sextupole for ILC
1 Cryostat assembly, integration and commissioning procedures M.Olcese Version: 07 May 2008.
Progress on the MuCool and MICE Coupling Coils * L. Wang a, X. K Liu a, F. Y. Xu a, A. B. Chen a, H. Pan a, H. Wu a, X. L. Guo a, S. X Zheng a, D. Summers.
Possible HTS wire implementation Amalia Ballarino Care HHH Working Meeting LHC beam-beam effects and beam-beam interaction CERN, 28 th August 2008.
CD meeting R.Yamada1 Thoughts on 4CD (4 th Concept Detector) Solenoid System based on Alex Mikhailchenko’s Basic Design Ryuji Yamada October 20,
Future activities of the COMPASS polarized target N. Doshita University of Bochum, Germany.
26 April 2013 Immanuel Gfall (HEPHY Vienna) Belle II SVD Overview.
Motivation Polarized 3 He gas target Solenoid design and test 3 He feasibility test Summary and outlook Johannes Gutenberg-Universit ä t Mainz Institut.
Overview installation of Polarized Target 14th Crystal Ball Meeting
Study of Pion Capture Solenoids for PRISM H.Ohnishi AB M. Aoki C, Y. Ajima A, N. Fukasawa AD, K. Ishibashi B, Y. Kuno C, T. Miura A, K. Nakahara C, T.
HD target.
Focusing Lens for the SSR1 Section of PXIE Preliminary analysis of main options 3/13/2012I. Terechkine1.
Zian Zhu Magnet parameters Coil/Cryostat/Support design Magnetic field analysis Cryogenics Iron yoke structure Mechanical Integration Superconducting Magnet.
Preliminary Design for the Coupling Coil Cryostat in MICE
CMS FPIX Cooling System Studies Joe Howell, Fermilab for the FPIX Upgrade Mechanical Working Group CMS Upgrade Workshop April 27,
9 th Crystal Ball Meeting Basel October Andreas Thomas Transversely Polarized Target 1.-Possible Physics Experiments 2.-Frozen Spin Target 3.-Technical.
Spectrometer Solenoid Fabrication Status and Schedule Steve Virostek Lawrence Berkeley National Lab MICE RAL October 20, 2008.
1 G9a -FROST. 2 Experiments FROST New generation of CLAS photoproduction experiments with FROzen Spin Polarized Target (FROST) E02-112: γp→KY (K + Λ,
CONSTRUCTION AND TEST OF A TRANSVERSE SUPERCONDUCTING HOLDING MAGNET 15th CB Meeting Mainz March 8th, 2010 Henry G. Ortega Spina.
Recent Developments in Polarized Solid Targets H. Dutz, S. Goertz Physics Institute, University Bonn J. Heckmann, C. Hess, W. Meyer, E. Radke, G. Reicherz.
He3 dilution refrigerator
Removal of 3 He from 4 He (R&D) David Haase, Franklin Dubose, Travis McCaw and Paul Huffman North Carolina State University.
9/17/07IRENG071 Cryogenic System for the ILC IR Magnets QD0 and QF1 K. C. Wu - BNL.
EDMEDM LANL Review of EDM Cost and Schedule Jan Boissevain, P-25 February 11, 2005, Los Alamos National Laboratory EDM Reference Design Tour of the Reference.
Restoring Komag Yasuhiro Makida Consideration of restoring and modifying Komag for a stand alone operation without the refrigerator. Contents 1.Magnet.
17th Crystal Ball Meeting
Dilution Refrigerators with Superconducting Magnets
The integration of 420 m detectors into the LHC
ILC Main Linac Superconducting Quadrupole V. Kashikhin for Superconducting Magnet Team.
Preliminary result of the target polarization 2004 Kaori Kondo COMPASS target team.
Exercises for Q1. Insulated copper tube A thin walled 10 mm copper tube is used to transport a low-temperature refrigerant with a temperature that is.
ILC Main Linac Superconducting Cryogen Free Splittable Quadrupole Technical Design V. Kashikhin for Superconducting Magnet Team.
Present status of production target and Room design Takashi Hashimoto, IBS/RISP 2015, February.
8/29/07K. C. Wu - Brookhaven National Lab1 Major Components in ILC IR Hall Interchangeable Detectors.
QXF Reaction / Impregnation Fixtures J. Schmalzle 4/9/13.
Cryogenics for SuperB IR Magnets J. G. Weisend II SLAC National Accelerator Lab.
24 June 2013 GSI, Darmstadt Helmholtz Institut Mainz Bertalan Feher, PANDA EMP First Measurements for a Superconducting Shield for the PANDA Polarized.
CLAS12 Longitudinally Polarized Target R&D Update CLAS Collaboration, October 20, 2015 Chris Keith.
HTS and LTS Magnet Design and Prototyping for RAON
Initial Tests of the JLab Frozen Spin Target Chris Keith Target Group Jefferson Lab September 13, 2007 Brookhaven National Lab.
CBM Dipole Conceptional Design Review
CBM magnet overview of the BINP work
Status of the PANDA Magnet mechanics (yoke & cryostat)
Hervé Allain, R. van Weelderen (CERN)
Cryogenic behavior of the cryogenic system
Ti/SS transitions A.Basti INFN-PISA*
Status of the CLIC DR wiggler design and production at BINP
Cedric Garion, TE-VSC-DLM, WP12
Hervé Allain, R. van Weelderen (CERN)
Status of the PANDA Magnet
CHEN, Fusan KANG, Wen November 5, 2017
Yingshun Zhu Accelerator Center, Magnet Group
Challenges for FCC-ee MDI mechanical design
I. Bogdanov, S. Kozub, V. Pokrovsky, L. Shirshov,
Updated concept of the CBM dipole magnet
Measurement and Characterization of a 5T Solenoid Field
IR Beam Transport Status
Presentation transcript:

16th Crystal Ball Meeting October, 11-13, 2010, Dubrovnik Grigory Gurevich, Yuri Usov Dubna-Mainz Dilution Cryostat of the New Frozen-Spin Target

Main technical requirements Horizontal Dilution Refrigerator to fit in the CB detector geometry Beam along cryostat axis φ symmetric, θ>160 0 Thin internal holding coil 0.4 T on 1.5 K radiation shield (longitudinal, transverse) Target material loading along the cryostat axis Base temperature in the frozen spin mode ≈ 30 mK

1.5 K radiation shield 25 K radiation shield Separator (3K) and Evaporator (1.2K) precooling stages ( 4 He) 80 K radiation shield 3 He/ 4 He Dilution stage T min ≈ 23 mK Polarization ≈ 94% Relaxation ≈ 1500 hours ≈≈

High-temperature heat exchanger (7 stages: from room to 10 K)

Intermediate tube-in-tube heat exchanger: (seven 3-mm capillaries inside a 10-mm tube: from 10 K to 4 K)

Low-temperature heat exchanger (4 stages: from 4 to ~2 K)

4 He Evaporator bath (surrounds and thermally isolates the still bath)

Still bath of the dilution unit

Preliminary heat exchanger of 3 He/ 4 He dilution stage (geometric impedance ≈ 2×10 8 cm -3 )

Sintered copper heat exchanger of the dilution unit (10 stages, total area 5 m 2 on each side)

Vacuum C 4 H 10 O – 60% 30mm 3He/4He – 6%

Loading of the target material into the cryostat

First variant of the insert Although T~30 mK was reached with this insert, its installation required using of critically large loads, while the thermal contacts turned out to be ineffective and unreliable. In spite of high power of the heater it was impossible to reach sufficiently high temperature of the indium gasket for reliable sealing, which resulted in appearing superleaks. The re-cooling line inside the insert was found to be insufficiently effective. The waveguide of a stainless steel tube had too large attenuation. NMR cables were not completely vacuum-tight.

Second variant of the insert Two-part insert has important advantages: i) a difficult procedure of introducing and vacuum-sealing of the outer insert can be performed at room temperature in usual atmosphere; ii) mounting of the inner insert with the cooled butanol sample inside the cold cryostat can be accomplished very easy, without effort, and do not require the hermetic seal (an indium gasket placed into a slot was used).

Internal longitudinal Holding coil ( solenoid coil manufactured of μm multifilamental NbTi cable and consisting of four layers, each having 600 turns wound around a 0.3-mm thick copper holder, T ≈ 1.5 K)

Internal transverse Holding coil

SUMMARY Working parameters of the dilution cryostat are in agreement with the technical requirements: - T min ≈ 23 mK; - polarization relaxation time ≈ 1500 hours (at T=30 mK); - time to cool from room temperature ≈ 5 hours; - LHe consumption in the frozen spin mode ≈ 2 l/hour Internal holding coils provide longitudinal/ transverse field 0.4 Tesla at 30 A Any combinations of beam and target polarizations are possible Two-part insert makes the sample loading operation easy and convenient Future development: New insert, containing light-guides, for active polarized target

Participants JINR (Dubna): N.Borisov, A.Fedorov, V.Kolomiets, L.Kutuzova, A.Lazarev, S.Mironov, A.Neganov, V.Pavlov, Yu.Usov INR RAS (Moscow): G.Gurevich, R.Kondratiev, Yu.Vorobiev IKPh (Mainz): A.Thomas, M.Martinez