A new NQR method of measuring the spectral density of slow motions in
solids is proposed. It is shown that also in NQR a 90 degrees phase sh
ift of a resonant rf magnetic field following a 90 degrees pulse locks
the nuclear magnetization in a 'rotating frame' similarly as in NMR.
The spin-lattice relaxation time T-1 rho of the locked magnetization i
s calculated in general for an arbitrary spin. It is assumed that the
fluctuations of the EFG tensor dominate the spin-lattice relaxation. T
he calculations show that T-1 rho depends on the spectral density J(om
ega) of the electric quadrupole fluctuations at the NQR frequencies, a
nd also at a low frequency Omega. Here Omega approximate to gamma B-1
kHz depends on the orientation of the rf magnetic field in the princip
al-axis system of the EFG tenser. The term containing J(Omega) in the
expression for T-1 rho(-1) depends on the orientation of the rf magnet
ic field in the principal-axis system of the EFG tensor, only through
the orientation dependence of Omega. This term vanishes when the elect
ric quadrupole fluctuations do not modulate the frequency of the NQR t
ransition excited by the rf magnetic field. Two particular examples: I
= 1 and I = 3/2 are worked out in details. (C) 1997 Elsevier Science
B.V.