2018
DOI: 10.1016/j.jmr.2018.09.003
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Improved signal fidelity in 4-pulse DEER with Gaussian pulses

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Cited by 49 publications
(45 citation statements)
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“…Q‐band DEER measurements were performed at 50 K on a Bruker ELEXSYS E580 with a separate electron–electron double resonance (ELDOR) source or an arbitrary waveform generator (AWG) with a 150 W traveling wave tube (TWT) amplifier and a homemade resonator. A 4‐pulse DEER sequence with 100 MHz separation between the pulses was applied with 12 ns rectangular pulses (for T4 lysozyme) or 14 ns full width at half maximum Gaussian pulses (for Bid) for both observer and pump frequencies . Additional artefacts in the DEER trace from the coherent AWG generated pulses were removed by 16‐step phase cycling.…”
Section: Methodsmentioning
confidence: 99%
“…Q‐band DEER measurements were performed at 50 K on a Bruker ELEXSYS E580 with a separate electron–electron double resonance (ELDOR) source or an arbitrary waveform generator (AWG) with a 150 W traveling wave tube (TWT) amplifier and a homemade resonator. A 4‐pulse DEER sequence with 100 MHz separation between the pulses was applied with 12 ns rectangular pulses (for T4 lysozyme) or 14 ns full width at half maximum Gaussian pulses (for Bid) for both observer and pump frequencies . Additional artefacts in the DEER trace from the coherent AWG generated pulses were removed by 16‐step phase cycling.…”
Section: Methodsmentioning
confidence: 99%
“…The sidebands of the sinc-shaped excitation profile of 15 rectangular pulses increase the overlap of the observer and pump pulse in DEER, resulting in so called '2+1' artefacts at the end of the DEER trace. It has recently been shown that those artefacts can be reduced by replacing the rectangular pulses with Gaussian pulses (Teucher and Bordignon, 2018). Gaussian pulses also have a frequency function of ( ) = 0 but an amplitude function:…”
Section: Open Accessmentioning
confidence: 99%
“…20 FWHM describes the full width at half maximum of the pulse in the time domain (Teucher and Bordignon, 2018). During a rectangular or Gaussian pulse the magnetisation vector is rotated around the 1 field with an angle that is independent of the initial orientation of the magnetisation vector.…”
Section: Open Accessmentioning
confidence: 99%
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