Abstract:Within this review, we describe a home-built pulsed electron paramagnetic resonance (EPR) spectrometer operating at 180 GHz as well as the incorporation of two double resonance techniques, electron nuclear double resonance (ENDOR) and pulsed electron double resonance (PELDOR), along with first applications. Hahn-echo decays on a TEMPO/polystyrene sample are presented, demonstrating that the observation of anisotropic librational motions is possible in a very precise manner at high magnetic fields. Bisdiphenyle… Show more
“…The sensitivity 9,14 was measured with a 0.1% (by mass) sample of the organic radical TEMPOL (C 9 H 18 NO 2 ) in a polystyrene film. It has been suggested that TEMPOL may have a role in treating cancer 25 .…”
Section: Resultsmentioning
confidence: 99%
“…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 .…”
Section: Introductionmentioning
confidence: 99%
“…High field/high frequency EPR has the following advantages: (i) At higher fields an EPR experiment can resolve more resonances, such as those from multiple spin centres and anisotropic g-tensors 1,14 .…”
Section: Introductionmentioning
confidence: 99%
“…The microwave sources used for high frequency EPR include orotrons 12 , gyrotrons 2 , extended interaction klystrons 11 , far infra-red lasers 3,10 , Gunn diodes 1,13,14 and IMPATT phase locked oscillators 9 . The frequency and power available from amplified synthesizers with multipliers have increased in recent years, and such sources were used in the spectrometer described here, supplied by Virginia Diodes Inc. (VDI) 22 .…”
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 .
“…The sensitivity 9,14 was measured with a 0.1% (by mass) sample of the organic radical TEMPOL (C 9 H 18 NO 2 ) in a polystyrene film. It has been suggested that TEMPOL may have a role in treating cancer 25 .…”
Section: Resultsmentioning
confidence: 99%
“…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 .…”
Section: Introductionmentioning
confidence: 99%
“…High field/high frequency EPR has the following advantages: (i) At higher fields an EPR experiment can resolve more resonances, such as those from multiple spin centres and anisotropic g-tensors 1,14 .…”
Section: Introductionmentioning
confidence: 99%
“…The microwave sources used for high frequency EPR include orotrons 12 , gyrotrons 2 , extended interaction klystrons 11 , far infra-red lasers 3,10 , Gunn diodes 1,13,14 and IMPATT phase locked oscillators 9 . The frequency and power available from amplified synthesizers with multipliers have increased in recent years, and such sources were used in the spectrometer described here, supplied by Virginia Diodes Inc. (VDI) 22 .…”
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 .
“…Furthermore, In order to compensate for hysteresis effects, the sweep of the magnetic field has to start at much lower (or higher) field position than the first resonance appears. Many other experiments, such as ENDOR [11,12], PELDOR [11] or DNP [13] require fixed, reproducible and stable magnetic field values, which are difficult to achieve at high magnetic fields using only control of the magnet or sweep coil current without any feedback loops.…”
We describe a field-lock/field-sweep system for the use in superconducting magnets. The system is based on a commercially available field mapping unit and a custom designed broad-band 1 H-NMR probe. The NMR signal of a small water sample is used in a feedback loop to set and control the magnetic field to high accuracy. The current instrumental configuration allows field sweeps of ± 0.4 T and a resolution of up to 10 -5 T (0.1 G) and the performance of the system is demonstrated in a high-field electron paramagnetic resonance (EPR) application. The system should also be of utility in other experiments requiring precise and reproducible sweeps of the magnetic field such as DNP, ENDOR or PELDOR.
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