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Magnetic property measurement system mpms 3

Manufactured by Quantum Design

The Magnetic Property Measurement System (MPMS-3) is a versatile laboratory instrument designed to measure the magnetic properties of a wide range of materials. The MPMS-3 utilizes a superconducting quantum interference device (SQUID) technology to provide highly sensitive and accurate measurements of magnetization, susceptibility, and other magnetic phenomena across a wide range of temperatures and magnetic fields.

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4 protocols using magnetic property measurement system mpms 3

1

Characterization of Polycrystalline Materials

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Powder x-ray diffraction was performed at room temperature using a PANalytical x-ray diffractometer (model EMPYREAN) with monochromatic Cu Kα1 radiation. The DC magnetic properties of the polycrystals were conducted by using a Quantum Design magnetic property measurement system (MPMS-3). The electrical resistivity was measured on sintered pellets by a Quantum Design physical property measurement system (PPMS).
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2

Magnetic Characterization of Iron Oxide Nanoparticles

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A Quantum Design magnetic property measurement system (MPMS 3) superconducting quantum inference device (SQUID) magnetometer was used to analyze the magnetic properties of the particles. Magnetization curves at room temperature were obtained for liquid samples in a polytetrafluoroethylene sample holder with 100 μL of the iron oxide nanoparticle suspension in hexane/water. The volume-weighted median magnetic diameter (Dmv) and geometric deviation of the magnetic nanoparticle samples were determined by fitting the superparamagnetic equilibrium magnetization curve to the Langevin function, weighted using a log-normal size distribution.
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3

Transport and Specific Heat Measurements

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Transport and specific heat were measured by a conventional four-probe method and a relaxation method, respectively, in a Physical Property Measurement System equipped with a rotator and 3He insert (Quantum Design). In the transport measurements Au wires were attached to the sample with Ag paste (DuPont 4922 N). The typical dimensions were 1.2 mm × 0.5 mm × 0.1 mm (shown in the inset of Fig. 2), which enable us to thoroughly measure the transport properties for both longitudinal and transverse configurations. The magnetic field dependence of resistivity (Hall resistivity) is obtained after the symmetrization (antisymmetrization) with respect to the positive and negative field. Magnetization was measured with a Magnetic Property Measurement System MPMS3, equipped with a 3He insert (Quantum Design).
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4

Single Crystal Growth and Magnetic Characterization of TbMn6Sn6

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Single crystals of TbMn6Sn6 were grown via a standard tin flux method29 . Magnetic measurements on TbMn6Sn6 were performed in a Quantum Design magnetic property measurement system (MPMS-3). When the field was applied along the c axis, a sharp transition could be observed in the M(T) profile at around 313 K (TSR) in Supplementary Fig. S1, corresponding to the spin-reorientation transition. A magnetic anomaly occurs at around 100 K as indicated by the hump in the temperature derivative of the susceptibility, which suggest possible spin excitations in the kagome lattices43 (link),44 (link) and is beyond our current scope of research.
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