Kelvinox®VT, Dilution refrigerator, sample in vacuum, no 1 K pot

Dilution refrigerator, sample in vacuum, no 1 K pot

KelvinoxVT is a sample-in-vacuum dilution refrigerator that provides a simple means of cooling samples below 25mK. It is designed to fit into any Oxford Instruments variable temperature inserts (VTI) with 50mm access.

As it uses the cold gas environment of the VTI, there is no need for a 1K pot on the insert. This provides key benefits:

  • the temperature range of a new or existing VTI can be extended to 25 mK or less
  • appropriate use of exchange gas allows measurements up to 300 mK
  • there is no liquid helium in the sample horizontal plane making the Kelvinox®VT ideal for neutron or X-ray scattering experiments
  • Specifications 
  • System components/options 
  • Operation 
  • Applications 
  • Images 
Base temperature ≤ 25 mK
Base temperature stability ± 1 mK
Maximum temperature 300 K
Continuous operation Standard
Sample environment Vacuum (no liquid He in horizontal sample path)
Cooling power at 100 mK ≥ 15 µW
Cooling power at 120 mK ≥ 20 µW
Sliding seal assembly Included
3He/4He mixture Included

   

A KelvinoxVT system includes :

  • Integrated sliding seal and insert for loading into the VTI
  • A 'pot-less' condensing stage
  • A dilution unit equipped with one step heat exchanger

Automation and control of your dilution refrigerator using the KelvinoxIGH - Intelligent Gas Handling system :

  • All systems are delivered with a KelvinoxIGH which is a fully automated system which enables complete operation of a dilution refrigerator using sophisticated software and virtual instrument drivers for National Instruments'LabVIEWTM.

    Options:

    • PT100: 24-way copper/supercon loom wired to the mixing chamber
    • PT200 : 2 x S1 co-axial cables wired to the mixing chamber
    • PT210 : 4 x S1 co-axial cables wired to the mixing chamber
    • PT300 : 2 x UT85-SS-SS coaxial cables wired to the mixing chamber
    • LE100 : LECSH low eddy current sample holder
    • CS100 : ROTH1, 30 point calibrated RuO2 sensor to 50 mK
    • CS200 : ROTH2, generic calibration RuO2 sensor
    • RB100 : AVS47 resistance bridge with rf filtering, cables & IEEE interface
    • TS530 : Temperature controller for use with AVS47 resistance bridge
    • IPC : Isobus Picobus converter
    • HTC: Helium cold trap
    • Transfer tubes
    • HE3F : 3He flow meter
    • VIN : Valves in pumping lines

     

    Solutions to helium rising costs  :

    The KelvinoxVT is compatible the IntegraAC, recondensing liquid helium cryostat.

    This product has been developed to significantly reduce the consumption of liquid helium by recondensing helium gas evaporated within the system, which would other wise be vented from the cryostat. This decreases the frequency of helium refills. Cryogenic systems can be kept cold continuously, even when in stand by mode, leading to greater freedom to schedule experimental time.

    IntegraAC recondensing dewar compability sketch

     

    Prior to circulating the 3He/4He mixture, the KelvinoxVT is cooled to below 2 K by the variable temperature insert exchanging stage and the appropriate volume of exchange gas.  This heat exchanger is a continuous-flow type that is fed through a needle valve and capillary from the helium bath, located well above the horizontal beamline.  Once the dilution refrigerator has been cooled down to below 2 K, the mixture is then condensed and circulated as in a conventional dilution refrigerator.  Once circulating, the returning 3He is condensed by heat exchange to the VTI (at ~1.5 K) providing a 'pot-less' condensing stage.

    This compact system can be cooled down to base temperature in around three hours from loading.  Temperature control can be achieved when circulating up to a temperature of approximately 3 K.  The VTI temperature control can be used for higher temperatures up to 300 K.

     This compact system can be cooled from room to base temperature in about 6 hours.

    Kelvinox VT dilution refrigerator mode of operation

    Research areas

    Applications

    Experimental techniques
    Semiconductors Quantum Hall Effect
    Quantum dots
    Single electron tunneling
    Quantum computing
    Magneto-resistance
    Hall effect
    RF transport
    High frequency conductivity
    Solid State Physics Heavy fermions systems
    Metal insulator transition
    Spin glass
    Mesoscopic systems
    Giant magnetic resistance
    Specific heat
    DeHaas-van Alphen Oscillations
    Solid state NMR
    Electrical resistivity
    Magneto-resistance
    Neutron scattering
    Superconductivity Low Tc superconductors
    Quantum computing  
    Josephson junctions
    Flux vortices
    Quantum initial phenomema
    Electrical resistivity
    Scanning spectroscopy(STM/AFM)
    Squids
    AC susceptibility
    Astrophysics & Cosmology Low temperature detectors Superconducting tunnel junctions
    Ge bolometers
    Electrothermal measurements
    Voltage biased measurements
    Low energy photon detection
    Metrology Quantum Hall Effect
    Voltage standards
    Current standards
    Magneto-resistance
    DC & AC low frequency transport and magnetic measurements
    Single electron tunneling
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