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Mpms xl 5 squid magnetometer

Manufactured by Quantum Design
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The MPMS XL-5 SQUID magnetometer is a highly sensitive instrument designed to measure the magnetic properties of materials. It utilizes a Superconducting Quantum Interference Device (SQUID) technology to detect and measure extremely small magnetic fields. The MPMS XL-5 is capable of measuring magnetic moments over a wide range of temperatures and applied magnetic fields, making it a versatile tool for materials research and characterization.

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27 protocols using mpms xl 5 squid magnetometer

1

Magnetic Susceptibility of Molecules

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Temperature-dependent magnetic susceptibility measurements were carried out with a Quantum-Design MPMS-XL-5 SQUID magnetometer equipped with a 5 T magnet over the temperature range 310–385 K with a cooling and heating rate of 2 K min−1, and magnetic field of 0.5 T. Diamagnetic correction for the molecule was applied.
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2

Synthesis and Characterization of Azine Complexes

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All chemicals and solvents used for syntheses of azine compounds and Ni complexes were reagent grade and used without further purification. First, 2-pyridinecarboxaldehyde, 1H-imidazole-4-carboxaldehyde, 2-methyl-1H-imidazole-4-carboxaldehyde, nickel(II) chloride hexahydrate, and ammonium hexafluorophosphate were purchased from FUJIFILM (Tokyo, Japan). All reactions were carried out under aerobic conditions. Infrared spectra (KBr pellets; 4000–400 cm−1) were recorded on a JASCO FT-001 Fourier transform infrared spectrometer (JASCO, Tokyo, Japan). Absorption spectra were recorded on a Shimadzu UV/Vis-1650 spectrophotometer (Kyoto, Japan) in the range of 200–600 nm at room temperature in acetonitrile. The 1H NMR spectra were acquired on a Varian 400-MR spectrometer (Los Angeles, CA, USA); the chemical shifts were referenced to residual 1H NMR signals of solvents and are reported versus TMS. Elemental analyses were conducted at Advanced Science Research Center, Okayama University. Magnetic susceptibilities were measured on a Quantum Design MPMS XL5 SQUID magnetometer (Tokyo, Japan) in a 1.9–300 K temperature range under an applied magnetic field of 0.1 T at the Okayama University of Science. Corrections for diamagnetism were applied using Pascal’s constants [35 (link)].
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3

Chemical Analysis and Magnetism

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The elemental analyses were measured on a Vario ELIII elemental analyser. The magnetic susceptibility measurements were carried out on a Quantum Design MPMS-XL5 SQUID magnetometer, and diamagnetic corrections were calculated from Pascal’s constants of all components.
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4

Magnetic Susceptibility Measurements of 3

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Temperature-dependent magnetic susceptibility measurements were carried out with a Quantum-Design MPMS-XL-5 SQUID magnetometer equipped with a 5T magnet in the range from 300 to 2.0 K. The powdered samples were contained in a gel bucket and fixed in a nonmagnetic sample holder. Diamagnetic corrections of the constituent atoms for 3 were calculated from Pascal's constants51 and found to be −854.0 × 10−6 cm3 mol−1. Experimental susceptibilities were also corrected for the magnetization of the sample holder (0.0001, cm3 mol−1).
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5

Synthesis and Characterization of Fe-Pt Nanoparticles

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For the synthesis of the Fe–Pt NPs, a hemispherical heating mantle (model WiseTherm WHM 12112 from Witeg Labortechnik GmbH) connected to a temperature controller (J-KEM, model 310) with a J-type Teflon thermocouple was used. The samples were characterized using a (scanning) transmission electron microscope (TEM Jeol JEM-2010F) equipped with energy-dispersive X-ray spectroscopy (EDXS). Low-temperature magnetic measurements were performed on a Quantum Design MPMS-XL-5 SQUID magnetometer. With the thermogravimetric analyses (TG analyser NETZSCH STA 449 C/6/G Jupiter) the amount of organic matter in the sample was determined to be 30%. The magnetization values are reported for the mass of Fe–Pt in the sample after the subtraction of the organic content. Fourier-transform infrared spectroscopy (FTIR) measurements were performed using a Spectrum 400 spectrometer (Perkin Elmer, USA). The spectra were recorded on dried samples in the wavenumber range 4000–650 cm−1.
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6

Magnetic Susceptibility of Molecule 2a

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Temperature-dependent magnetic susceptibility measurements for 2a were carried out with a Quantum-Design MPMS-XL-5 SQUID magnetometer equipped with a 5-Tesla magnet in the range from 295 to 2.0 K at a magnetic field of 0.5 T. The powdered sample was contained in a Teflon bucket and fixed in a non-magnetic sample holder. Each raw data file for the measured magnetic moment was corrected for the diamagnetic contribution of the Teflon bucket according to Mdia(bucket) = χg × m × H, with an experimentally obtained gram susceptibility of the Teflon bucket. The molar susceptibility data were corrected for the diamagnetic contribution using Pascal’s constants56 (link). Experimental data were modeled with the julX program57 using a fitting procedure to the spin Hamiltonian Ĥ=-2JŜ1Ŝ2+gμBBS1+S2 . A slightly better fit quality was obtained using an additional diamagnetic contribution (–140×10–6 cm3 mol–1) and some weak intermolecular interactions (–0.12 K). The latter were considered in a mean field approach by using a Weiss temperature Θ58 . The Weiss temperature Θ (defined as Θ = zJinterS(S + 1)/3k) relates to intermolecular interactions zJinter, where Jinter is the interaction parameter between two nearest neighbor magnetic centers, k is the Boltzmann constant (0.695 cm–1 K–1), and z is the number of nearest neighbors.
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7

Growth and Characterization of Ce15Au65Ge20 Alloy

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The source material was an alloy Ce15Au65Ge20 (in atom %), produced by arc melting under
an Ar
atmosphere. The obtained button was annealed at 700 °C for 14
days. From this alloy, a crystal was grown by the Czochralski technique
using a Cyberstar apparatus. The detailed description of the instrument
and the procedure used for single-crystal growth can be found in our
recent paper.21 (link)The single-crystal
XRD data were collected on a Bruker Kappa Apex
II diffractometer equipped with a mirror monochromator and a Mo Kα
IμS (λ = 0.71073 Å). The Apex2 program
package was used for cell refinement and data reduction. The structure
was solved by using direct methods and refined with the SHELXL-2013 program. Semiempirical absorption correction (SADABS) was applied to the data.
Magnetic measurements were conducted
on a Quantum Design MPMS XL-5
SQUID magnetometer equipped with a 5 T magnet, operating in the temperature
range 1.9–400 K. The specific heat was measured on a Quantum
Design Physical Property Measurement System (PPMS 9T), equipped with
a 9 T magnet and a 3He cryostat, operating in the temperature
range 0.35–400 K.
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8

Magnetic Susceptibility Characterization

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All the samples were fixed by eicosane and parafilm to avoid movement during the measurements and were sealed in a glass tube to avoid reaction with moisture and oxygen. Direct current susceptibility and alternative current susceptibility measurements with frequencies ranging from 1 to 997 Hz were performed on a Quantum Design MPMS XL-5 SQUID magnetometer for the polycrystalline samples. All the dc susceptibilities were corrected for the diamagnetic contributions from the sample holder, eicosane and from the molecule, using Pascal's constants.11
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9

Magnetic Measurements of Crystalline Samples

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Magnetic measurements
were performed
on crystalline samples (20–40 mg) with a Quantum Design MPMS-XL-5
SQUID magnetometer working in the 2–400 K temperature range
(temperature scan rate 2 K min–1) with an applied
magnetic field 1 T. Experimental susceptibilities
were corrected for diamagnetism of the constituent atoms by the use
of Pascal’s constants.
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10

Synthesis and Characterization of Tris(4'-carboxybiphenyl)amine

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Tris(4′-carboxybiphenyl)amine was synthesized following reported procedures29 (link). Other chemicals and solvents were obtained commercially and used as received. The elemental analyses (C, H, N) were accomplished on a Vario ELIII elemental analyser. The FT-IR spectra were determined on a Bruker/Tensor-27 spectrophotometer with pressed KBr pellets in the range 4000–400 cm−1. The fluorescence spectra, the fluorescence lifetime and the absolute emission quantum yield were measured on an Edinburgh Analytical Instruments FLS980. Both the dc and ac magnetic susceptibility measurements were carried out on a Quantum Design MPMS-XL5 SQUID magnetometer using Pascal’s constants diamagnetic corrections.
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