Literature DB >> 22218011

A spectrometer designed for 6.7 and 14.1 T DNP-enhanced solid-state MAS NMR using quasi-optical microwave transmission.

Kevin J Pike1, Thomas F Kemp, Hiroki Takahashi, Robert Day, Andrew P Howes, Eugeny V Kryukov, James F MacDonald, Alana E C Collis, David R Bolton, Richard J Wylde, Marcella Orwick, Kosuke Kosuga, Andrew J Clark, Toshitaka Idehara, Anthony Watts, Graham M Smith, Mark E Newton, Ray Dupree, Mark E Smith.   

Abstract

A Dynamic Nuclear Polarisation (DNP) enhanced solid-state Magic Angle Spinning (MAS) NMR spectrometer operating at 6.7 T is described and demonstrated. The 187 GHz TE(13) fundamental mode of the FU CW VII gyrotron is used as the microwave source for this magnetic field strength and 284 MHz (1)H DNP-NMR. The spectrometer is designed for use with microwave frequencies up to 395 GHz (the TE(16) second-harmonic mode of the gyrotron) for DNP at 14.1T (600 MHz (1)H NMR). The pulsed microwave output from the gyrotron is converted to a quasi-optical Gaussian beam using a Vlasov antenna and transmitted to the NMR probe via an optical bench, with beam splitters for monitoring and adjusting the microwave power, a ferrite rotator to isolate the gyrotron from the reflected power and a Martin-Puplett interferometer for adjusting the polarisation. The Gaussian beam is reflected by curved mirrors inside the DNP-MAS-NMR probe to be incident at the sample along the MAS rotation axis. The beam is focussed to a ~1 mm waist at the top of the rotor and then gradually diverges to give much more efficient coupling throughout the sample than designs using direct waveguide irradiation. The probe can be used in triple channel HXY mode for 600 MHz (1)H and double channel HX mode for 284 MHz (1)H, with MAS sample temperatures ≥85 K. Initial data at 6.7 T and ~1 W pulsed microwave power are presented with (13)C enhancements of 60 for a frozen urea solution ((1)H-(13)C CP), 16 for bacteriorhodopsin in purple membrane ((1)H-(13)C CP) and 22 for (15)N in a frozen glycine solution ((1)H-(15)N CP) being obtained. In comparison with designs which irradiate perpendicular to the rotation axis the approach used here provides a highly efficient use of the incident microwave beam and an NMR-optimised coil design.
Copyright © 2011 Elsevier Inc. All rights reserved.

Entities:  

Mesh:

Substances:

Year:  2011        PMID: 22218011     DOI: 10.1016/j.jmr.2011.12.006

Source DB:  PubMed          Journal:  J Magn Reson        ISSN: 1090-7807            Impact factor:   2.229


  12 in total

1.  Topical Developments in High-Field Dynamic Nuclear Polarization.

Authors:  Vladimir K Michaelis; Ta-Chung Ong; Matthew K Kiesewetter; Derik K Frantz; Joseph J Walish; Enrico Ravera; Claudio Luchinat; Timothy M Swager; Robert G Griffin
Journal:  Isr J Chem       Date:  2014-02-13       Impact factor: 3.333

2.  A versatile and modular quasi optics-based 200GHz dual dynamic nuclear polarization and electron paramagnetic resonance instrument.

Authors:  Ting Ann Siaw; Alisa Leavesley; Alicia Lund; Ilia Kaminker; Songi Han
Journal:  J Magn Reson       Date:  2016-03       Impact factor: 2.229

3.  Solid state nuclear magnetic resonance with magic-angle spinning and dynamic nuclear polarization below 25 K.

Authors:  Kent R Thurber; Alexey Potapov; Wai-Ming Yau; Robert Tycko
Journal:  J Magn Reson       Date:  2012-11-21       Impact factor: 2.229

4.  Simplified THz Instrumentation for High-Field DNP-NMR Spectroscopy.

Authors:  Thorsten Maly; Jagadishwar R Sirigiri
Journal:  Appl Magn Reson       Date:  2012-07-01       Impact factor: 0.831

5.  Theory for cross effect dynamic nuclear polarization under magic-angle spinning in solid state nuclear magnetic resonance: the importance of level crossings.

Authors:  Kent R Thurber; Robert Tycko
Journal:  J Chem Phys       Date:  2012-08-28       Impact factor: 3.488

6.  Dynamic Nuclear Polarization as an Enabling Technology for Solid State Nuclear Magnetic Resonance Spectroscopy.

Authors:  Adam N Smith; Joanna R Long
Journal:  Anal Chem       Date:  2015-12-17       Impact factor: 6.986

7.  A quasi-optical and corrugated waveguide microwave transmission system for simultaneous dynamic nuclear polarization NMR on two separate 14.1 T spectrometers.

Authors:  Thierry Dubroca; Adam N Smith; Kevin J Pike; Stuart Froud; Richard Wylde; Bianca Trociewitz; Johannes McKay; Frederic Mentink-Vigier; Johan van Tol; Sungsool Wi; William Brey; Joanna R Long; Lucio Frydman; Stephen Hill
Journal:  J Magn Reson       Date:  2018-01-31       Impact factor: 2.229

8.  Design and characterization of a W-band system for modulated DNP experiments.

Authors:  Mallory L Guy; Lihuang Zhu; Chandrasekhar Ramanathan
Journal:  J Magn Reson       Date:  2015-10-14       Impact factor: 2.229

9.  Multi-resonant photonic band-gap/saddle coil DNP probehead for static solid state NMR of microliter volume samples.

Authors:  Alexander A Nevzorov; Sergey Milikisiyants; Antonin N Marek; Alex I Smirnov
Journal:  J Magn Reson       Date:  2018-10-23       Impact factor: 2.229

10.  Higher order amyloid fibril structure by MAS NMR and DNP spectroscopy.

Authors:  Galia T Debelouchina; Marvin J Bayro; Anthony W Fitzpatrick; Vladimir Ladizhansky; Michael T Colvin; Marc A Caporini; Christopher P Jaroniec; Vikram S Bajaj; Melanie Rosay; Cait E Macphee; Michele Vendruscolo; Werner E Maas; Christopher M Dobson; Robert G Griffin
Journal:  J Am Chem Soc       Date:  2013-12-13       Impact factor: 15.419

View more

北京卡尤迪生物科技股份有限公司 © 2022-2023.