We have measured proton Zeeman relaxation rates R in the 2,4- and 2,5-isomers of di tert-butylhydroxybenzene (DTHB) in the solid state. R was measured as a function of temperature T at proton Larmor frequencies of (j)/21T = 8.50,22.5, and 53.0 MHz. The Tranges were from 78 K to just below the melting points of 2,4- and 2,5-DTHB, 385 and 323 K, respectively. The 2,5- DTHB R vs T and (j) can be interpreted qualitatively in terms of three Bloembergen-PurcellPound (BPP) spectral densities, one for each of the three types of rotors in the molecule. The quantitative agreement is poor but a good fit is obtained using either a Davidson-Cole (DC) or Frolich spectral density, still preserving the three rotor types. The implications of this are discus...
Proton spin-lattice relaxation times have been measured at 16, 31, and 59 MHz in 4-methyl-2,6-ditert...
Deuterium nuclear magnetic resonance (NMR) spectra and spin-lattice relaxation times were determined...
We have investigated the dynamics of methyl group reorientation in solid methyl‐substituted phenan...
We have measured proton Zeeman relaxation rates R in the 2,4- and 2,5-isomers of di tert-butylhydrox...
We have measured the temperature T dependence of the proton Zeeman relaxation rate R in polycrystall...
We reinterpret proton spin-lattice relaxation measurements in solid 1,4-di-t-butylbenzene (1,4-DTB) ...
We have measured the temperature T and Larmor frequency ω/2π dependence of the proton spin‐lattice r...
We investigate proton spin-lattice relaxation in two powdered organic molecular solids with reorient...
There are two solid phases which either have a large hysteresis of at least 90 K, or are both stable...
We have determined the molecular and crystal structure of 4,5-dibromo-2,7-di-t-butyl-9,9-dimethylxan...
We have investigated the dynamics of the ethyl groups and their constituent methyl groups in polycry...
We have measured the solid state nuclear magnetic resonance (NMR) 1H spin-lattice relaxation rate fr...
Proton spin-lattice relaxation rates R = T1−1 have been measured in powdered samples of 4-methyl-2,6...
We have used the solid state proton spin relaxation technique to investigate the barriers for methyl...
We report proton Zeeman relaxation rates R as a function of temperature T at 8.5 and 53 MHz in polyc...
Proton spin-lattice relaxation times have been measured at 16, 31, and 59 MHz in 4-methyl-2,6-ditert...
Deuterium nuclear magnetic resonance (NMR) spectra and spin-lattice relaxation times were determined...
We have investigated the dynamics of methyl group reorientation in solid methyl‐substituted phenan...
We have measured proton Zeeman relaxation rates R in the 2,4- and 2,5-isomers of di tert-butylhydrox...
We have measured the temperature T dependence of the proton Zeeman relaxation rate R in polycrystall...
We reinterpret proton spin-lattice relaxation measurements in solid 1,4-di-t-butylbenzene (1,4-DTB) ...
We have measured the temperature T and Larmor frequency ω/2π dependence of the proton spin‐lattice r...
We investigate proton spin-lattice relaxation in two powdered organic molecular solids with reorient...
There are two solid phases which either have a large hysteresis of at least 90 K, or are both stable...
We have determined the molecular and crystal structure of 4,5-dibromo-2,7-di-t-butyl-9,9-dimethylxan...
We have investigated the dynamics of the ethyl groups and their constituent methyl groups in polycry...
We have measured the solid state nuclear magnetic resonance (NMR) 1H spin-lattice relaxation rate fr...
Proton spin-lattice relaxation rates R = T1−1 have been measured in powdered samples of 4-methyl-2,6...
We have used the solid state proton spin relaxation technique to investigate the barriers for methyl...
We report proton Zeeman relaxation rates R as a function of temperature T at 8.5 and 53 MHz in polyc...
Proton spin-lattice relaxation times have been measured at 16, 31, and 59 MHz in 4-methyl-2,6-ditert...
Deuterium nuclear magnetic resonance (NMR) spectra and spin-lattice relaxation times were determined...
We have investigated the dynamics of methyl group reorientation in solid methyl‐substituted phenan...