Multi-step phase-cycling in a free-electron laser-powered pulsed electron paramagnetic resonance spectrometer. Issue 26 (25th June 2018)

• Record Type: Journal Article
• Authors: Wilson, C. Blake; Aronson, Samuel; Clayton, Jessica A.; Glaser, Steffen J.; Han, Songi; Sherwin, Mark S.
• Is Part Of: Physical chemistry chemical physics. Volume 20:Issue 26(2018)
• Page Start: 18097
• Page End: 18109
• Publication Date: 2018-06-25
• Subjects: Chemistry, Physical and theoretical -- Periodicals; 541.3
• DOI: 10.1039/c8cp01876f
• Languages: English
• ISSNs: 1463-9076

Abstract

Abstract : Optomechanical multi-step phase cycling enables free electron laser-powered 240 GHz pulsed electron paramagnetic resonance electron spin relaxation measurements. Abstract : Electron paramagnetic resonance (EPR) is a powerful tool for research in chemistry, biology, physics and materials science, which can benefit significantly from moving to frequencies above 100 GHz. In pulsed EPR spectrometers driven by powerful sub-THz oscillators, such as the free electron laser (FEL)-powered EPR spectrometer at UCSB, control of the duration, power and relative phases of the pulses in a sequence must be performed at the frequency and power level of the oscillator. Here we report on the implementation of an all-quasioptical four-step phase cycling procedure carried out directly at the kW power level of the 240 GHz pulses used in the FEL-powered EPR spectrometer. Phase shifts are introduced by modifying the optical path length of a 240 GHz pulse with precision-machined dielectric plates in a procedure we call phase cycling with optomechanical phase shifters (POPS), while numerical receiver phase cycling is implemented in post-processing. The POPS scheme was successfully used to reduce experimental dead times, enabling pulsed EPR of fast-relaxing spin systems such as gadolinium complexes at temperatures above 190 K. Coherence transfer pathway selection with POPS was used to perform spin echo relaxation experiments to measure the phase memory time of P1 centers in diamond in the presence of a strong unwanted FID signal in the background. The large excitation bandwidth of FEL-EPR, together with phase cycling, enabled the quantitative measurement of instantaneous electron spectral diffusion, from which the P1 center concentration was estimated to within 10%. Finally, phase cycling enabled saturation-recovery measurements of T 1 in a trityl-water solution at room temperature – the first FEL-EPR measurement of electron T 1 .