Single-chip electron spin resonance detectors operating at 50GHz, 92GHz, and 146GHz

[Display omitted] •Single-chip ESR detectors operating at 50GHz, 92GHz, and 146GHz.•Spin sensitivity down to 2×107spins/Hz1/2 at 146GHz with BDPA at 300K.•Experiments up to 360GHz using the higher harmonics of the 92GHz oscillator. We report on the design and characterization of single-chip electron...

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Veröffentlicht in:Journal of magnetic resonance (1997) 2017-05, Vol.278, p.113-121
Hauptverfasser: Matheoud, Alessandro V., Gualco, Gabriele, Jeong, Minki, Zivkovic, Ivica, Brugger, Jürgen, Rønnow, Henrik M., Anders, Jens, Boero, Giovanni
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container_title Journal of magnetic resonance (1997)
container_volume 278
creator Matheoud, Alessandro V.
Gualco, Gabriele
Jeong, Minki
Zivkovic, Ivica
Brugger, Jürgen
Rønnow, Henrik M.
Anders, Jens
Boero, Giovanni
description [Display omitted] •Single-chip ESR detectors operating at 50GHz, 92GHz, and 146GHz.•Spin sensitivity down to 2×107spins/Hz1/2 at 146GHz with BDPA at 300K.•Experiments up to 360GHz using the higher harmonics of the 92GHz oscillator. We report on the design and characterization of single-chip electron spin resonance (ESR) detectors operating at 50GHz, 92GHz, and 146GHz. The core of the single-chip ESR detectors is an integrated LC-oscillator, formed by a single turn aluminum planar coil, a metal-oxide-metal capacitor, and two metal-oxide semiconductor field effect transistors used as negative resistance network. On the same chip, a second, nominally identical, LC-oscillator together with a mixer and an output buffer are also integrated. Thanks to the slightly asymmetric capacitance of the mixer inputs, a signal at a few hundreds of MHz is obtained at the output of the mixer. The mixer is used for frequency down-conversion, with the aim to obtain an output signal at a frequency easily manageable off-chip. The coil diameters are 120μm, 70μm, and 45μm for the U-band, W-band, and the D-band oscillators, respectively. The experimental frequency noises at 100kHz offset from the carrier are 90Hz/Hz1/2, 300Hz/Hz1/2, and 700Hz/Hz1/2 at 300K, respectively. The ESR spectra are obtained by measuring the frequency variations of the single-chip oscillators as a function of the applied magnetic field. The experimental spin sensitivities, as measured with a sample of α,γ-bisdiphenylene-β-phenylallyl (BDPA)/benzene complex, are 1×108spins/Hz1/2, 4×107spins/Hz1/2, 2×107spins/Hz1/2 at 300K, respectively. We also show the possibility to perform experiments up to 360GHz by means of the higher harmonics in the microwave field produced by the integrated single-chip LC-oscillators.
doi_str_mv 10.1016/j.jmr.2017.03.013
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We report on the design and characterization of single-chip electron spin resonance (ESR) detectors operating at 50GHz, 92GHz, and 146GHz. The core of the single-chip ESR detectors is an integrated LC-oscillator, formed by a single turn aluminum planar coil, a metal-oxide-metal capacitor, and two metal-oxide semiconductor field effect transistors used as negative resistance network. On the same chip, a second, nominally identical, LC-oscillator together with a mixer and an output buffer are also integrated. Thanks to the slightly asymmetric capacitance of the mixer inputs, a signal at a few hundreds of MHz is obtained at the output of the mixer. The mixer is used for frequency down-conversion, with the aim to obtain an output signal at a frequency easily manageable off-chip. The coil diameters are 120μm, 70μm, and 45μm for the U-band, W-band, and the D-band oscillators, respectively. 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LC-oscillator
title Single-chip electron spin resonance detectors operating at 50GHz, 92GHz, and 146GHz
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