“…Electron paramagnetic resonance (EPR) experiments have realized new opportunities as magnetic fields have been increased 1,2,3,4,5,6,7 and pulsed capabilities have been added 8,9,10,11,12,13,14 .…”
We describe a pulsed multi-frequency electron paramagnetic resonance spectrometer operating at several frequencies in the range of 110-336 GHz. The microwave source at all frequencies consists of a multiplier chain starting from a solid state synthesizer in the 12-15 GHz range. A fast PIN-switch at the base frequency creates the pulses. At all frequencies a FabryPérot resonator is employed and the π/2 pulse length ranges from ~100 ns at 110 GHz to ~600 ns at 334 GHz. Measurements of a single crystal containing dilute Mn 2+ impurities at 12 T illustrate the effects of large electron spin polarizations. The capabilities also allow for pulsed electron nuclear double resonance experiments as demonstrated by Mims ENDOR of 39 K nuclei in Cr:K 3 NbO 8 .
“…Electron paramagnetic resonance (EPR) experiments have realized new opportunities as magnetic fields have been increased 1,2,3,4,5,6,7 and pulsed capabilities have been added 8,9,10,11,12,13,14 .…”
We describe a pulsed multi-frequency electron paramagnetic resonance spectrometer operating at several frequencies in the range of 110-336 GHz. The microwave source at all frequencies consists of a multiplier chain starting from a solid state synthesizer in the 12-15 GHz range. A fast PIN-switch at the base frequency creates the pulses. At all frequencies a FabryPérot resonator is employed and the π/2 pulse length ranges from ~100 ns at 110 GHz to ~600 ns at 334 GHz. Measurements of a single crystal containing dilute Mn 2+ impurities at 12 T illustrate the effects of large electron spin polarizations. The capabilities also allow for pulsed electron nuclear double resonance experiments as demonstrated by Mims ENDOR of 39 K nuclei in Cr:K 3 NbO 8 .
“…Obviously, the dimensions decrease as the frequency increases, and its mechanical construction becomes proportionally challenging. Currently, the record is set at 275 GHz, as demonstrated by Schmidt et al [39,82]. The single-mode resonator has the highest possible power conversion ratio.…”
“…A convenient way to adjust the coupling is by rotating the resonator around the waveguide coupling to the iris hole in the cylinder wall. This mode allows a large iris hole, which facilitates the scaling up to higher frequencies [20,28,82]. A specific challenge is to combine the resonator with an ENDOR coil enabling pulse ENDOR applications.…”
“…To allow the RF field to penetrate the resonator, slits are machined in the resonator body. These slits also can serve as optical access [20,82]. At lower frequencies , it has been demonstrated that the resonator cylinder itself can be formed from a ''ribbon coil'' [58].…”
“…This concept will complicate the layout of the bridge considerably, since both RF and LO signals need separate quasi-optical paths. This principle was applied in the pulsed EPR bridge at 275 GHz by Schmidt et al [39,82]. Similar schemes were employed in the multi-frequency bridges operating at 120 and 240 GHz developed by van Tol et al [41,81] and Reijerse et al [42].…”
An overview of the most recent developments in high-frequency highfield electron paramagnetic resonance (EPR) instrumentation is given. In particular, the practical choices concerning sources, detectors, resonators, propagation systems as well as magnet technology are discussed in the light of various possible applications. Examples of particular homodyne and heterodyne quasi-optic EPR systems illustrate the potential for future developments in EPR technology.
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