Dynamic nuclear polarization enhanced NMR at 187 GHz/284 MHz using an extended interaction Klystron amplifier

<p>A Dynamic Nuclear Polarisation (DNP) enhanced solid-state Magic Angle Spinning (MAS) NMR spectrometer which uses a 187 GHz (corresponding to 1H NMR frequency of 284 MHz) Extended Interaction Klystron (EIK) amplifier as the microwave source is briefly described. Its performance is demonstrat...

Full description

Bibliographic Details
Main Authors: Watts, A, Kemp, T, Dannatt, H, Barrow, N, Brown, S, Newton, M, Dupree, R
Format: Journal article
Published: Elsevier 2016
_version_ 1797083301671862272
author Watts, A
Kemp, T
Dannatt, H
Barrow, N
Brown, S
Newton, M
Dupree, R
author_facet Watts, A
Kemp, T
Dannatt, H
Barrow, N
Brown, S
Newton, M
Dupree, R
author_sort Watts, A
collection OXFORD
description <p>A Dynamic Nuclear Polarisation (DNP) enhanced solid-state Magic Angle Spinning (MAS) NMR spectrometer which uses a 187 GHz (corresponding to 1H NMR frequency of 284 MHz) Extended Interaction Klystron (EIK) amplifier as the microwave source is briefly described. Its performance is demonstrated for a biomolecule (bacteriorhodopsin), a pharmaceutical, and surface functionalised silica. The EIK is very compact and easily incorporated into an existing spectrometer. The bandwidth of the amplifier is sufficient that it obviates the need for a sweepable magnetic field, once set, for all commonly used radicals.</p> <p>The variable power (CW or pulsed) output from the EIK is transmitted to the DNP-NMR probe using a quasi-optic system with a high power isolator and a corrugated waveguide which feeds the microwaves into the DNP-NMR probe. Curved mirrors inside the probe project the microwaves down the axis of the MAS rotor, giving a very efficient system such that maximum DNP enhancement is achieved with less than 3 W output from the microwave source. The DNP-NMR probe operates with a sample temperature down to 90 K whilst spinning at 8 kHz. Significant enhancements, in excess of 100 for bacteriorhodopsin in purple membrane (bR in PM), are shown along with spectra which are enhanced by ≈25 with respect to room temperature, for both the pharmaceutical furosemide and surface functionalised silica. These enhancements allow hitherto prohibitively time consuming experiments to be undertaken. The power at which the DNP enhancement in bR in PM saturates does not change significantly between 90 K and 170 K even though the enhancement drops by a factor of ≈11. As the DNP build up time decreases by a factor 3 over this temperature range, the reduction in T1n is presumably a significant contribution to the drop in enhancement.</p>
first_indexed 2024-03-07T01:39:49Z
format Journal article
id oxford-uuid:96780316-ab88-419d-9dae-23435e9003bf
institution University of Oxford
last_indexed 2024-03-07T01:39:49Z
publishDate 2016
publisher Elsevier
record_format dspace
spelling oxford-uuid:96780316-ab88-419d-9dae-23435e9003bf2022-03-26T23:53:13ZDynamic nuclear polarization enhanced NMR at 187 GHz/284 MHz using an extended interaction Klystron amplifierJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:96780316-ab88-419d-9dae-23435e9003bfSymplectic Elements at OxfordElsevier2016Watts, AKemp, TDannatt, HBarrow, NBrown, SNewton, MDupree, R<p>A Dynamic Nuclear Polarisation (DNP) enhanced solid-state Magic Angle Spinning (MAS) NMR spectrometer which uses a 187 GHz (corresponding to 1H NMR frequency of 284 MHz) Extended Interaction Klystron (EIK) amplifier as the microwave source is briefly described. Its performance is demonstrated for a biomolecule (bacteriorhodopsin), a pharmaceutical, and surface functionalised silica. The EIK is very compact and easily incorporated into an existing spectrometer. The bandwidth of the amplifier is sufficient that it obviates the need for a sweepable magnetic field, once set, for all commonly used radicals.</p> <p>The variable power (CW or pulsed) output from the EIK is transmitted to the DNP-NMR probe using a quasi-optic system with a high power isolator and a corrugated waveguide which feeds the microwaves into the DNP-NMR probe. Curved mirrors inside the probe project the microwaves down the axis of the MAS rotor, giving a very efficient system such that maximum DNP enhancement is achieved with less than 3 W output from the microwave source. The DNP-NMR probe operates with a sample temperature down to 90 K whilst spinning at 8 kHz. Significant enhancements, in excess of 100 for bacteriorhodopsin in purple membrane (bR in PM), are shown along with spectra which are enhanced by ≈25 with respect to room temperature, for both the pharmaceutical furosemide and surface functionalised silica. These enhancements allow hitherto prohibitively time consuming experiments to be undertaken. The power at which the DNP enhancement in bR in PM saturates does not change significantly between 90 K and 170 K even though the enhancement drops by a factor of ≈11. As the DNP build up time decreases by a factor 3 over this temperature range, the reduction in T1n is presumably a significant contribution to the drop in enhancement.</p>
spellingShingle Watts, A
Kemp, T
Dannatt, H
Barrow, N
Brown, S
Newton, M
Dupree, R
Dynamic nuclear polarization enhanced NMR at 187 GHz/284 MHz using an extended interaction Klystron amplifier
title Dynamic nuclear polarization enhanced NMR at 187 GHz/284 MHz using an extended interaction Klystron amplifier
title_full Dynamic nuclear polarization enhanced NMR at 187 GHz/284 MHz using an extended interaction Klystron amplifier
title_fullStr Dynamic nuclear polarization enhanced NMR at 187 GHz/284 MHz using an extended interaction Klystron amplifier
title_full_unstemmed Dynamic nuclear polarization enhanced NMR at 187 GHz/284 MHz using an extended interaction Klystron amplifier
title_short Dynamic nuclear polarization enhanced NMR at 187 GHz/284 MHz using an extended interaction Klystron amplifier
title_sort dynamic nuclear polarization enhanced nmr at 187 ghz 284 mhz using an extended interaction klystron amplifier
work_keys_str_mv AT wattsa dynamicnuclearpolarizationenhancednmrat187ghz284mhzusinganextendedinteractionklystronamplifier
AT kempt dynamicnuclearpolarizationenhancednmrat187ghz284mhzusinganextendedinteractionklystronamplifier
AT dannatth dynamicnuclearpolarizationenhancednmrat187ghz284mhzusinganextendedinteractionklystronamplifier
AT barrown dynamicnuclearpolarizationenhancednmrat187ghz284mhzusinganextendedinteractionklystronamplifier
AT browns dynamicnuclearpolarizationenhancednmrat187ghz284mhzusinganextendedinteractionklystronamplifier
AT newtonm dynamicnuclearpolarizationenhancednmrat187ghz284mhzusinganextendedinteractionklystronamplifier
AT dupreer dynamicnuclearpolarizationenhancednmrat187ghz284mhzusinganextendedinteractionklystronamplifier