Kelvinox®TLM, Top-loading into liquid dilution refrigerator

Top-loading into liquid dilution refrigerator

The KelvinoxTLM is a high performance dilution refrigerator with a base temperature of less than 15 mK and cooling power of more than 400 µW.

  • Top loading of the sample directly into the 3He/4He mixing chamber via a vacuum lock arrangement ensures good sample thermalisation, high stability of the thermal environment and guarantee of operation in high magnetic field.
  • Multiple service, multi-user access : unique design which can be used with a range of sample probes such as Swedish rotator or high frequency co-axial lines.
  • Quick and easy sample change : no need to remove the mixture during sample change, giving quicker experiment turnaround times and reducing the risk of leaks.
  • Non metallic sample environment : ideal for experiments such as solid state NMR when removing metallic material surrounding the pickup coil resonant circuit is key to accurate measurements. Typically, field sweeps of up to 2T / min leave the temperature of the mixture unaffected.
  • The KelvinoxTLM is covered by US patent No. 6202439.
  • Specification 
  • System components/options 
  • Operation 
  • Applications 
  • Images 
Base temperature ≤ 15 mK
Base temperature stability ± 1 mK
Maximum temperature 1 K
Continuous operation Standard
Sample environment Liquid
Cooling power at 100 mK ≥ 400 µW
Cooling power at 120 mK ≥ 580 µW
3He/4He mixture

Key:   = Included with system

Every KelvinoxTLM is made up from three main components:

Dilution unit - providing ≥ 400 µW at 100 mK measured at the He mixture phase boundary.

Insert - featuring still pumping line, 1 K pot, diagnostic wiring and inner vacuum can.

Top loading probe - ease of access to samples with a range of experimental services.

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
    • CAPV/CAP : Capillary line with or without valve
    • KELMSWR : Swedish rotator - manual
    • KELMSRWA : Swedish rotator - automation
    • 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 tube
    • TLMP3 : Spare top loading probe, 34 mm access - tested with system
    • TLMP4 : Spare top loading probe, 34 mm access - supplied untested at a later date
    • HE3F : 3He flow meter
    • VIN : Valves in pumping lines

To load the sample, the probe along with any electrical services and/or sample positioning mechanisms is lowered into the cold 3He/4He mixture via a vacuum lock arrangement.  This can be undertaken with the mixture condensed or circulating.  The mixing chamber tail is formed from concentric non-metallic tubes, with the outer tube forming the mixing chamber vessel.  The inner tube promotes the flow of 3He atoms mixture around the sample region, eliminating temperature gradients.  The refrigerator is fitted with a continuous heat exchanger and a stack of sintered silver heat exchangers for optimum base temperature performance.  The non-metallic tail construction allows the whole mixing chamber assembly to be inserted into the bore of a high field magnet if desired.  Typically, field sweeps of up to 2 T/min leave the temperature of the mixture unaffected.

Top-loading into liquid dilution refrigerator

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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