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Superconducting magnet

Manufactured by Oxford Instruments
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Superconducting magnets are high-strength electromagnets that utilize superconducting materials to generate a powerful, stable magnetic field. They are designed to operate at extremely low temperatures, typically below the critical temperature of the superconducting material, in order to maintain the superconducting state and maximize the magnetic field strength.

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6 protocols using superconducting magnet

1

Structural Characterization of Sit Derivatives

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The structures of the Sit derivatives were established by IR and NMR analysis. The NMR spectra were recorded on a Varian Mercury 300 MHz NMR spectrometer equipped with an Oxford Instruments Ltd. superconducting magnet (Palo Alto, CA, USA). FTIR analysis was performed in a WGH-30A double beam infrared spectrophotometer (Gangdong Sci. & Tech. development Co., Ltd. Tianjin, China). The specific conclusion is described in detail in the Results section.
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2

Structural Identification of Er and Derivatives

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The molecular structures of Er and its derivatives were identified by IR and NMR. NMR spectra were recorded on a Varian Mercury 300 MHz NMR spectrometer equipped with an Oxford Instruments Ltd. superconducting magnet (Palo Alto, CA, USA). CDCl3 was used as a solvent to dissolve samples and tetramethylsilane was used as the internal standard for NMR analysis. FTIR analysis was performed in a WGH-30A double-beam infrared spectrophotometer (Gangdong Sci. & Tech. development Co., Ltd. Tianjin, China).
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3

Electrical Resistance Measurements of Ho2Ir2O7

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Measurements of the electrical resistance of a single crystal of Ho2Ir2O7 of approximate size 0.2 × 0.2 × 0.25 mm3 were made using a four-wire technique with an 855 μA ac current applied along the [010] direction. We chose to show the experimentally measured resistance of the sample instead of resistivity as the conversion to resistivity is complicated by the small size and the geometry of the samples. An order-of-magnitude estimate of the resistivity for a typical low-temperature, zero-field sample resistance of 35 mΩ is 10−5Ω m (a more detailed discussion can be found in Supplementary Note 7). Magnetic fields were applied using an Oxford Instruments superconducting magnet equipped with a 3He insert and were swept at a rate of 1 T/min.
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4

Superconducting Magnet NMR Spectroscopy

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NMR spectra were obtained with a Tecmag Apollo spectrometer and a standard sample probe from NMR Service GmbH. The magnetic field has been applied by a 16 T Oxford Instruments superconducting magnet. Temperatures were regulated by a 4He variable temperature insert (VTI). Temperatures below 4.2 K were achieved by pumping on the VTI. At high temperatures and small fields, Fourier transformations (FFT) of the spin echo covered the whole spectral width. At lower temperatures, we swept the frequency and summed up the FFT’s to obtain the complete spectrum. The spectra at 15 T below 10 K have been obtained by field sweeps, and converting into frequency sweeps. This is easily possible due to the negligible quadrupole interaction. We have confirmed the correctness of this procedure at higher temperatures. The spin lattice relaxation rate, T11 , has been measured by standard saturation recovery at the peak of the spectra. The nuclear magnetization, M0, has been saturated by a train of radio frequency pulses, before measuring the recovered nuclear magnetization, M(τ), depending on the time τ between the saturation train and the spin echo sequence.
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5

Temperature-Dependent NMR Spectroscopy

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Temperature dependence measurements were performed on a 380 MHz Oxford Instruments superconducting magnet equipped with a home-built spectrometer at the Larmor frequency of 58.336 MHz for deuterons. The NMR spectra were recorded by the ((p/2) x À t À (p/2) y À t 2 -ACQ) ''solid echo'' pulse sequence with the ''exorcycle'' quadrature detection pulse scheme with a pulse length of 12 ms. Echo delay time t was set to 50 ms and the t 2 delay was set to 20 ms. Dwell time was set to 0.1 ms resulting in an spectral window of 5 MHz. Recycle delay between consecutive acquisitions was 50 ms and at each measurement 1000 scans were performed. The temperature was controlled by using an Oxford Instruments continuous flow cryostat into which a custom-built goniometer probe head holding the sample was inserted. This setup allowed for regulation of temperature with accuracy of 0.1 K in the whole region of interest, i.e., between 200 K and 440 K. Temperature scans
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6

Magnetic Susceptibility and High-Field EPR Characterization

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Magnetic susceptibility measurements over the temperature range 1.8-300 K were performed at a magnetic field of 0.5 T using a Quantum Design SQUID MPMSXL-5 magnetometer.
Correction for the sample holder, as well as the diamagnetic correction χ D , which was estimated from the Pascal constants, 22 was applied.
High-field, high-frequency EPR spectra at temperatures ranging from ca. 3 K to 290 K were recorded on a home-built spectrometer at the EMR facility of the NHMFL 23 with the microwave frequencies 52-416 GHz. The instrument is a transmission-type device and uses no resonance cavity. The microwaves were generated by a phase-locked Virginia Diodes source, generating frequency of 13 ± 1 GHz, and equipped with a cascade of frequency multipliers to generate higher harmonic frequencies. A superconducting magnet (Oxford Instruments) capable of reaching a field of 17 T was employed. Additionally, X-band and Q-Band spectra were recorded on a Bruker ElexSys E500 instrument equipped with an NMR teslameter ER 036TM and a frequency counter E 41 FC (Faculty of Chemistry, Wroclaw University).
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