The Mini Cryogen-Free Magnet System from Cryogenic Limited company is a physical device used for production of strong magnetic field created by a superconducting coil. The system combines the latest cryogen-free technology with sophisticated measurement techniques. It provides a versatile, powerful investigative device achieving low temperatures and high magnetic fields without the direct use of liquid helium or nitrogen. Closed loop system uses helium gas for refrigeration of the superconducting magnet and the sample. The instrument is designed for the measurement of magnetic properties using Vibrating Sample Magnetometer - VSM (magnetic moment and AC susceptibility) and electrical properties (resistivity and Hall effect). Measurement range is for magnetic field from –9 T to 9 T and for temperature from 1.6 K to 400 K.
The Cryogenic VSM (Vibrating Sample Magnetometer) module is designed to measure DC magnetic moment. It allows the measurements of magnetic hysteresis loops or temperature dependencies of magnetic moment (B = –9 T – +9 T, T = 1.6 K – 400 K). In this system, materials in various form can be analysed (bulk, thin films, powders or liquids). Orientation of the magnetic field can be parallel or perpendicular to the sample. VSM probe can be used also for AC susceptibility measurements. Since June 2017 our system contains upgraded VSM setup which has more stable adjustment.
The Cryogenic Resistivity module provides the capability to perform DC resistance and Hall voltage measurements. Samples with resistance in the range from 1 μΩ to 1 MΩ can be measured with variable temperature (T = 1.6 K – 400 K) and magnetic field (B = –9 T – +9 T). Orientation of the magnetic field can be parallel or perpendicular to the sample.
Instrument is comprised of the following components:
Cooling materials to cryogenic temperatures has traditionally used liquid cryogens (usually helium and nitrogen). The same results may be achieved more simply by mechanical means, using a cryocooler. Cryocoolers operate using a helium compressor, which requires just mains power and a source of cooling water. The cryocooler high pressure helium circuit is completely independent to the rest of the measurement system. However, it provides the cooling to both the magnet and the variable temperature insert (VTI). The cryostat is a vacuum insulated chamber whose primary function is to support and thermally shield the superconducting magnet and VTI.
The magnet in our system is a vertically oriented solenoid wound from copper stabilised filamentary niobium titanium (NbTi) superconducting wire. The coil is cooled by the cryocooler to an operating temperature of 3–4 K.
|Magnet type||NbTi solenoid with persistent mode switch|
|Central field homogeneity||0.1% over 10mm diameter x 10mm long cylinder|
|Decay rate in persistent mode (ppm/hr)||10|
|Magnet inductance (Henries)||5.3 H|
|Maximum Operating Field (Tesla)||9 T|
|Nominal operating current (amps)||108.3 A|
|Radial stray field 5 gauss contour (m)||1.3 (from centre of magnet)|
|Vertical stray field 5 gauss contour (m)||1.6 (from centre of magnet)|
|Initial magnet energisation rate||0.3 T/min|
|Maximum subsequent energisation rate||1.0 T/min|
|Magnet power supply||Cryogenic SMS120C (120A, +/-5V)|
|Low field option +/=300mA (24 mT)|
|Type||Sumitomo 1 W Pulse Tube Cryocooler|
|Compressor mains requirements||410 V, 3 phase, 16A or 32A|
|Compressor cooling water minimum flow rate (l/min)||7|
|Static compressor gas pressure (bar)||17.0|
|Working compressor gas pressure (bar)||21|
|Typical cooldown time (hrs)||11|
|Temperature range (K)||1.6–400|
|Temperature stability (K)||+/- 0.05|
|Internal diameter (mm)||25|
|Normal operating pressure (mbar)||5–15|
|Dump vessel pressure with system at room temperature||Atmosphere plus 0.25 bar (approx)|
|Dump vessel pressure with VTI at base temperature||Atmosphere minus 0.5 bar (approx)|
|Variable temperature insert without VSM coils inserted||Circulating helium gas 25 mm inner diameter|
|With VSM coils inserted||Static exchange gas 14 mm inner diameter|