Pulsed NMRON oscillatory free induction decay signals in the angular distribution of gamma radiation from plated60Co Fe

Results for an inhomogeneously broadened60Co Fe NMRON sample have been obtained for gamma detected single pulse (nutation) and two pulse (free induction decay) experiments in the region of intermediate-to-low R(=ω1/Δ). Here ω1 is the angular frequency measure of the strength of the ferromagnetically enhanced RF field at the nucleus and Δ is the HWHM of the inhomogeneously broadened line. Comparisons of the oscillatory FID signals obtained are made with the theoretical predictions of the following paper [6]. © 1993 J.C. Baltzer AG, Science Publishers

Pulsed NMRON oscillatory free induction decay signals in the angular distribution of gamma radiation from plated60Co Fe

Results for an inhomogeneously broadened60Co Fe NMRON sample have been obtained for gamma detected single pulse (nutation) and two pulse (free induction decay) experiments in the region of intermediate-to-low R(=ω1/Δ). Here ω1 is the angular frequency measure of the strength of the ferromagnetically enhanced RF field at the nucleus and Δ is the HWHM of the inhomogeneously broadened line. Comparisons of the oscillatory FID signals obtained are made with the theoretical predictions of the following paper [6]. © 1993 J.C. Baltzer AG, Science Publishers

Pulsed NMRON oscillatory free induction decay signals in the angular distribution of gamma radiation from plated60Co Fe

Results for an inhomogeneously broadened60Co Fe NMRON sample have been obtained for gamma detected single pulse (nutation) and two pulse (free induction decay) experiments in the region of intermediate-to-low R(=ω1/Δ). Here ω1 is the angular frequency measure of the strength of the ferromagnetically enhanced RF field at the nucleus and Δ is the HWHM of the inhomogeneously broadened line. Comparisons of the oscillatory FID signals obtained are made with the theoretical predictions of the following paper [6]. © 1993 J.C. Baltzer AG, Science Publishers