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Er 4118 x ms 3 resonator

Manufactured by Oxford Instruments

The ER 4118 X-MS-3 resonator is a laboratory instrument designed for electron paramagnetic resonance (EPR) spectroscopy. It provides a controlled environment for analyzing and characterizing the magnetic properties of materials. The resonator is a key component in the EPR spectrometer, responsible for generating and detecting the electromagnetic signals used in the spectroscopic analysis.

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2 protocols using er 4118 x ms 3 resonator

1

Pulsed EPR Spectroscopy at Cryogenic Temperatures

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Conventional EPR spectra were obtained at room temperature with a Bruker ESP 380E spectrometer operating at a modulation amplitude of 0.01 mT, with the output microwave (MW) power of 100 mW, the MW attenuation set up to 25 dB and the sweep and constant times of 60 s and 46 ms, respectively. A Bruker ER 4118 X-MD-5 dielectric resonator was used. In pulsed EPR studies, an X-band Bruker ELEXSYS E580 EPR spectrometer was used equipped with a split-ring Bruker ER 4118 X-MS-3 resonator and an Oxford Instruments CF-935 cryostat.
The three-pulse ESEEM sequence (π/2)-τ-(π/2)-t-(π/2)-τ-echo was employed, with excitation at the maximum of the echo-detected EPR spectrum. The pulse lengths were 16 ns and the time delay τ was 204 ns, and the time delay t was scanned from 300 ns to 10 μs, with a 12 or 16 ns time step. The resonator was cooled with a stream of cold nitrogen gas. The temperature was controlled with a nitrogen flow stabilized by a Bruker ER4131VT temperature controller. The sample temperature was kept near 80 K.
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2

EPR Spectroscopy Protocol for Pulsed Experiments

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Conventional EPR spectra were obtained at room temperature with an X-band EPR benchtop SPINSCAN-X spectrometer (ADANI, Minsk, Belorussia), operating at modulation amplitude of 0.01 mT, with the output microwave (MW) power of 100 mW, the MW attenuation set to −25 dB, and with sweep and constant times of 60 s and 46 ms, respectively.
In pulsed EPR studies, an X-band Bruker ELEXSYS E580 EPR spectrometer was used equipped with a split-ring Bruker ER 4118 X-MS-3 resonator and an Oxford Instruments CF-935 cryostat. A three-pulse ESEEM sequence (π/2)-τ-(π/2)-t-(π/2)-τ-echo was employed, with excitation at the maximum of the echo-detected EPR spectrum. The pulse lengths were 16 ns, time delay τ was 204 ns, the time delay t was scanned from 300 ns to 10 µs, with a 12 or 16 ns time step. The resonator was cooled with a stream of cold nitrogen gas. The temperature was controlled by a nitrogen flow stabilized by a Bruker ER4131VT temperature controller, the sample temperature was kept near 80 K.
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