High-frequency dynamic nuclear polarization in the nuclear rotating frame

Citation
Ct. Farrar et al., High-frequency dynamic nuclear polarization in the nuclear rotating frame, J MAGN RES, 144(1), 2000, pp. 134-141
Citations number
28
Categorie Soggetti
Chemistry & Analysis","Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF MAGNETIC RESONANCE
ISSN journal
10907807 → ACNP
Volume
144
Issue
1
Year of publication
2000
Pages
134 - 141
Database
ISI
SICI code
1090-7807(200005)144:1<134:HDNPIT>2.0.ZU;2-G
Abstract
A proton dynamic nuclear polarization (DNP) NMR signal enhancement (epsilon ) close to thermal equilibrium, epsilon = 0.89, has been obtained at high f ield (B-o = 5 T, nu(epr) = 139.5 GHz) using 15 mM trityl radical in a 40:60 water/glycerol frozen solution at 11 K, The electron-nuclear polarization transfer is performed in the nuclear rotating frame with microwave irradiat ion during a nuclear spin-lock pulse. The growth of the signal enhancement is governed by the rotating frame nuclear spin-lattice relaxation time (T-1 rho), which is four orders of magnitude shorter than the nuclear spin-latt ice relaxation time (T-ln), Due to the rapid polarization transfer in the n uclear rotating frame the experiment can be recycled at a rate of 1/T-1 rho and is not limited by the much slower lab frame nuclear spin-lattice relax ation rate (1/T-ln). The increased repetition rate allowed in the nuclear r otating frame provides an effective enhancement per unit time(1/2) of epsil on(t) = 197, The nuclear rotating frame-DNP experiment does not require hig h microwave power; significant signal enhancements were obtained with a low -power (20 mW) Gunn diode microwave source and no microwave resonant struct ure. The symmetric trityl radical used as the polarization source is water- soluble and has a narrow EPR linewidth of 10 G at 139.5 GHz making it an id eal polarization source for high-field DNP/NMR studies of biological system s. (C) 2000 Academic Press.