The optical Bloch equations which incorporate the phenomenological population $({T}_{1})$ and dipole dephasing $({T}_{2})$ times have been tested recently by optical free-induction-decay (FID) measurements on an impurity-ion crystal ${\mathrm{Pr}}^{3+}$ : ${\mathrm{La}}_{3}$ at 1.6 K. At low optical fields, the observed ${\mathrm{Pr}}^{3+}$ optical linewidth is dominated by magnetic fluctuations arising from pairs of fluorine nuclear flip-flops where the condition ${T}_{1}\ensuremath{\gg}{T}_{2}$ prevails. At elevated fields, this nuclear broadening mechanism is quenched and the Bloch equations are violated with ${T}_{2}\ensuremath{\rightarrow}{T}_{1}$. In this paper, a microscopic theory appropriate for a low-temperature impurity solid is presented which reveals the above features both for optical and radio frequencies, and a simple physical interpretation of this line narrowing phenomenon is given. Modified Bloch equations of a novel form are derived to second order and yield analytic FID solutions over the entire range of optical-field strength. A discussion of the earlier NMR theories is given, pointing out similarities and differences.The optical Bloch equations which incorporate the phenomenological population $({T}_{1})$ and dipole dephasing $({T}_{2})$ times have been tested recently by optical free-induction-decay (FID) measurements on an impurity-ion crystal ${\mathrm{Pr}}^{3+}$:${\mathrm{La}}_{3}$ at 1.6 K. At low optical fields, the observed ${\mathrm{Pr}}^{3+}$ optical linewidth is dominated by magnetic fluctuations arising from pairs of fluorine nuclear flip-flops where the condition ${T}_{1}\ensuremath{\gg}{T}_{2}$ prevails. At elevated fields, this nuclear broadening mechanism is quenched and the Bloch equations are violated with ${T}_{2}\ensuremath{\rightarrow}{T}_{1}$. In this paper, a microscopic theory appropriate for a low-temperature impurity solid is presented which reveals the above features both for optical and radio frequencies, and a simple physical interpretation of this line narrowing phenomenon is given. Modified Bloch equations of a novel form are derived to second order and yield analytic FID solutions over the entire range of optical-field strength. A discussion of the earlier NMR theories is given, pointing out similarities and differences.

Physical Review AJul 1, 198474 citations

The optical Bloch equations which incorporate the phenomenological population

({T}_{1})

and dipole dephasing

({T}_{2})

times have been tested recently by optical free-induction-decay (FID) measurements on an impurity-ion crystal

{\mathrm{Pr}}^{3+}

{\mathrm{La}}_{3}

at 1.6 K. At low optical fields, the observed

{\mathrm{Pr}}^{3+}

optical linewidth is dominated by magnetic fluctuations arising from pairs of fluorine nuclear flip-flops where the condition ${T}_{1}\ensuremath{\gg}{T}_{2}$ prevails. At elevated fields, this nuclear broadening mechanism is quenched and the Bloch equations are violated with ${T}_{2}\ensuremath{\rightarrow}{T}_{1}$. In this paper, a microscopic theory appropriate for a low-temperature impurity solid is presented which reveals the above features both for optical and radio frequencies, and a simple physical interpretation of this line narrowing phenomenon is given. Modified Bloch equations of a novel form are derived to second order and yield analytic FID solutions over the entire range of optical-field strength. A discussion of the earlier NMR theories is given, pointing out similarities and differences.