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Progress in Cryogenics Jeremy Good Cryogenic Ltd 16 Tesla Cryogen Free Magnet Neutron Scattering and Beam-line systems 5-Tesla HiFi Muon Spectrometer Magnet 5 Tesla Cryogen Free Mini-Magnet 7 Tesla Fast Switching Mini Cryogen Free Magnet 17 Tesla Cryogen Free Magnet for Small Angle X-ray Scattering Cryogen Free Dilution Refrigerator down to 10mK 7 Tesla Cryogen Free SQUID Magnetometer 12 Tesla System with top loading, Variable Temperature Cryostat and Rotating Stand Cryogen Free Variable Temperature Cryostat 14 Tesla Vibrating Sample Magnetometer 5 Tesla Mini-VSM VSM data examples Measurement 3: m(H) using low-field option. A thin ferromagnetic film with a narrow hysteresis loop was measured with the magnet in low-field regime. The time constant was 10 seconds and the Cryogenic VSM preamplifier was used. The loop is shifted horizontally due to the effect of the remanent field in the magnet. In this case the remanent field was +1.5 mT. The noise level as determined by standard deviation of the data between 20 and 30 mT is 9.7 10-7 emu. moment, emu 5x10-4 0 -5x10-4 -30 -20 -10 0 10 20 Magnetic field, mT 30 40 VSM data examples Measurement 1: magnetic moment as a function of field at fixed temperatures. Measurement 2: magnetic moment as a function of continuously ramping temperature at fixed fields Palladium cylinder. Sample courtesy of Prof. M Valente, University of Aveiro µ0B = 2 T µ0B = 1 T µ0B = 0.01 T 0.04 0.2 0.0 T= 5K 10 K 50 K 100 K 150 K 200 K 250 K 270 K -0.1 -0.2 -10 -5 0 magnetic field, T 5 10 magnetic moment, emu magnetic moment, emu 0.03 0.1 0.02 0.01 1x10-3 0 50 100 150 200 250 300 0 50 100 150 200 250 300 5x10-4 0 Temperature, K AC susc. data examples Real part of AC susceptibility across an antiferromagnetic phase transition. The peak width of appox. 0.1 K is clearly resolved. AC susceptibility with sample extraction from the coils set and compensation of background signal. 1/χ, [emu/G]-1 8000 Gd2(SO4)3 8H2O AC susceptibility measured at frequency = 210.4 Hz AC field amplitude = 1 mT 6000 4000 2000 0 0 50 100 150 200 Temperature, K 250 300 350 AC susc. data examples In a spin glass the AC susceptibility is strongly affected by spin dynamics hence the position of the phase transition depends on the frequency of the excitation field. The data demonstrate a regular frequency dependence and correct discrimination between χ’ and χ’’ (i.e. the phase of the measured signal is set accurately so that the contributions due to χ’ and χ’’ are separated correctly and are not mixed). 4.0x10-4 3x10-3 2x10-3 30 Hz 60 Hz 300 Hz 600 Hz 900 Hz -3 1x10 0 60 70 80 90 100 Temperature, K 110 120 χ'', emu/G χ', emu/Oe 3.0x10-4 2.0x10-4 30 Hz 60 Hz 300 Hz 600 Hz 900 Hz -4 1.0x10 0.0 60 70 80 90 100 Temperature, K 110 120 Resistance and Hall effect Measurements of very low DC voltage is only possible by using reversing polarity. Otherwise the signal is dominated by thermal voltages rendering the measurement inaccurate. 0.20 0.15 Voltage, microVolt 0.10 Standard resistor T=2K I-V curve using reverse polarity R = 1.33 microOhms 0.05 0.00 -0.05 -0.10 -0.15 -0.20 -0.15 -0.10 -0.05 0.00 Current, Amp 0.05 0.10 0.15 Very low field option The following four graphs show successive reduction of the field steps from 10 mT to 0.01 mT using the low-current source. VSM measurements taken at 300 ms time constant without the preamplifier, hence the noise level is 10-5 emu. Sample: NIST calibration sample (YIG sphere) at 298 K. Resolution of the low-field source is 1 microTesla 50 mT The full range is typically m, emu 0.05 0.00 -0.05 -100 -50 0 B, mT 50 100 0.003 0.002 m, emu 0.001 0.000 -0.001 -0.002 -0.003 -3 -2 -1 0 B, mT 1 2 3 Heat capacity data example Magneto-caloric material Metallic sample Sample courtesy of Dr S.Ozcan, University of Cambridge and Cambridge Ltd. Heat capacity AC calorimetry method Sensor patterned on a silicon nitride membrane Ideal for small samples Record sensitivity 1 nJ/K Rotating Sample Probe Mini Magnet for NMR Baby-scan MRI magnet Delivered Cryogen Free Magnet Systems.