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Mpms xl squid

Manufactured by Quantum Design
Sourced in United States

The MPMS-XL SQUID (Magnetic Property Measurement System) is a highly sensitive instrument used for measuring the magnetic properties of materials. It employs a Superconducting Quantum Interference Device (SQUID) technology to detect and analyze the magnetic signals from samples. The MPMS-XL SQUID provides precise measurements of a material's magnetization, susceptibility, and other magnetic characteristics.

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7 protocols using mpms xl squid

1

Magnetic and Spectroscopic Characterization

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Quattro II triple quadrupole mass spectrometer. Methanol was used as the solvent for the electrospray ionization (positive ion, full scan mode). Capillary voltage was maintained at 2 kV, and cone voltage was kept at 31 kV. Variable-temperature EPR spectra of compounds 2-4 in powdered were recorded at 5K and 10K using a Bruker spectrometer operating at Q-band (35 GHz) frequency, and the EPR simulation was performed with Easyspin software (version 5.0.0). The dc magnetic susceptibility measurements were performed on solid polycrystalline samples (the microcrystallites were immobilized in pellets) with a Quantum Design MPMS-XL SQUID magnetometer between 2 and 300 K in applied magnetic field of 2 kOe in the 2-20 K temperature range and 10 kOe above 20 K. All the measurements were corrected for the diamagnetic contribution as calculated with Pascal's constants. The ac magnetic susceptibility measurements were performed on both Quantum Design MPMS-XL SQUID and Quantum Design PPMS magnetometers.
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2

Magnetic Characterization of Samples

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Magnetic measurements were performed using a Quantum Design SQUID MPMS-XL magnetometer through the Physical Measurements unit of the Servicio de Apoyo a la Investigación-SAI, Universidad de Zaragoza. All data were corrected for the sample holders and grease contributions, determined empirically as well as for the intrinsic diamagnetism of the sample, estimated using Pascal constants.
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3

Characterization of Nanomaterials via XRD, TEM, XPS, and Magnetometry

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XRD (X-ray diffraction) patterns give information on the phase and crystallinity of the as-prepared materials, which were collected on a Rigaku D/Max-2550 diffractometer (Tokyo, Japan) equipped with Cu-Ka radiation (λ = 0.15418 nm) at a scanning range of 20–80° and scanning speed of 5°/min. HRTEM images were obtained using a Tecnai G220S-Twin transmission electron microscope (Hillsboro, OR, USA) at an accelerating voltage of 120 kV, and the images were observed at 200 kV instead of 120 kV. XPS spectra were performed on a Thermo ESCALAB 250 (Waltham, MA, USA) with Al Kα radiation at θ = 90° for the X-ray sources; the binding energies were calibrated using the C 1s peak at 284.8 eV. UV-Visible solid absorbances of the samples were obtained using a PerkinElmer Lambda950 UV-Visible solid spectrometer (Waltham, MA, USA) using BaSO4 as a reference. The magnetic properties were investigated with a Quantum Design SQUID-MPMS-XL (San Diego, CA, USA). Magnetic hysteresis loops were measured at 300 K under a magnetic field up to 2 T.
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4

SQUID Magnetometry of Solid Samples

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Magnetic measurements were conducted on Quantum Design MPMS‐XL SQUID magnetometers with magnets capable of applying DC fields up to either 5 T or 7 T. DC susceptibility measurements were carried out under an applied field of 1000 Oe. AC measurements used an oscillating field of 3 Oe together with DC fields as described in the text. The samples were immobilised in eicosane and the data were corrected for the diamagnetic contributions of the eicosane. The sample and the sample holder based on Pascal constants.
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5

Polycrystalline Magnetic Susceptibility Measurements

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The DC magnetic susceptibility measurements were performed on a solid polycrystalline sample with a Quantum Design MPMS-XL SQUID magnetometer between 2 and 300 K in an applied magnetic field of 0.02 T for temperatures of 2–20 K, 0.2 T for temperatures of 20–80 K and 1 T for temperatures of 80–300 K. AC magnetic susceptibility measurements were performed using a Quantum Design MPMS-XL SQUID for frequencies between 1 and 1000 Hz and a Quantum Design PPMS magnetometers for frequencies between 50 and 10 000 Hz. These measurements were all corrected for diamagnetic contribution, as calculated with Pascal's constants.
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6

Magnetic Susceptibility Measurements

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The dc magnetic susceptibility measurements were performed on a solid polycrystalline sample with a Quantum Design MPMS-XL SQUID magnetometer between 2 and 300 K in an applied magnetic field of 0.02 T for temperatures of 2–20 K, 0.2 T for temperatures of 20–80 K and 1T for temperatures of 80-300 K. AC magnetic susceptibility measurements were performed using a Quantum Design MPMS-XL SQUID for frequencies between 1 and 1000 Hz and a Quantum Design PPMS magnetometers for frequencies between 50 and 10 000 Hz. These measurements were all corrected for diamagnetic contribution, as calculated with Pascal's constants.
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7

Magnetic Properties of Complex 1

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The magnetic
properties of a
polycrystalline sample of complex 1 were measured using
a Quantum Design MPMS XL SQUID instrument. The molar magnetic susceptibility
multiplied by the temperature (χMT) as a function of temperature of a polycrystalline sample of complex 1 was used to follow the temperature-dependent magnetic susceptibility
in cooling and warming sequences in 2 K steps between 4 and 350 K
with an applied magnetic field of 0.1 T. Diamagnetic corrections were
calculated using Pascal’s constants and applied to all data.
The calculated χMT vs T data are given in Tables S1 and S2 for
cooling and warming cycles, respectively.
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