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Physical Review

Selective Absorption of Circularly Polarized Light in Broad Bands by the Zeeman Components of Divalent Thulium in Calcium Fluoride

Charles H. Anderson, Herbert A. Weakliem, Edward S. Sabisky

Published Mar 4, 1966• 43 citations
Publisher

Abstract

The paramagnetic circular dichroism of the $4f\ensuremath{-}5d$ absorption bands of Ca${\mathrm{F}}_{2}$:${\mathrm{Tm}}^{2+}$ was investigated at 2.0\ifmmode^\circ\else\textdegree\fi{}K and 9.0kG. Using group theory it is shown that the bands can be separated into ${E}_{\frac{5}{2}}$ and ${G}_{\frac{3}{2}}$ character. Experimentally it was found that in this case the bands are primarily ${G}_{\frac{3}{2}}$ in character. Optical pumping experiments were performed where changes as large as \ifmmode\pm\else\textpm\fi{}20% were easily observed in the electron-paramagnetic-resonance absorption signal at $X$-band frequencies and 1.5\ifmmode^\circ\else\textdegree\fi{}K by changing the polarization of the pump light from right to left circular. A method for optically monitoring the difference in the population of the two Zeeman components of the ground state is also reported on.

DOI
10.1103/physrev.143.223

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Microwave absorption in the spin levels of the excited state of an ionic system can modulate the circularly polarized fluorescence from the state at right angles to an applied, static magnetic field. This modulation is detected in the broad, vibronic, sideband fluorescence of the Eu2+{\mathrm{Eu}}^{2+}Eu2+ ion in CaF2{\mathrm{F}}_{2}F2​ for a modulation frequency of 9.5 GHz.
Change in polarization produced by circularly polarized D(1) + D(2) radiation and destroyed by the resonance can be observed by monitoring the intensity of the radiation transmitting the vapor. The polarization and intensity of the absorption signal (change in absorption of the radiation produced by the resonance) are calculated from the solutions of equations governing the rate at which the populations of Zeeman sublevels of the ground state change. The result shows that the polarization increases as the disorientation mixing in the excited state decreases, and that the signal intensity is nearly equal to that when the D(1) radiation was used alone. Signal representation derived by Bell and Bloom based on Bloch's equations is modified so as to be applied to the experiment using D(1) + D(2) radiation as well as to that using D(1) radiation alone. The calculated result from the representation shows that the amplitude of the modulation signal (rf light modulation at the resonance) for D(1) + D(2) radiation is also nearly equal to that for D(1) radiation alone.
We report our study of the magneto-optical effect in a strictly linear regime on spin-polarized cold cesium atoms. Due to the low intensity and the short illumination period of the probe beam, less than 7.5% of the sample atoms change their states by absorbing probe photons. We produce a medium of atoms at rest in either the 6S1∕2,F=3,mF=06{S}_{1∕2},F=3,{m}_{F}=06S1∕2​,F=3,mF​=0 or 6S1∕2,F=3,mF=36{S}_{1∕2},F=3,{m}_{F}=36S1∕2​,F=3,mF​=3 state by optically pumping atoms trapped in a magneto-optical trap. We use the D1D1D1 resonance with large lower and upper state hyperfine splittings as a probe transition to avoid hyperfine mixing from the Zeeman interaction. Under this idealized situation we measure the Stokes parameters in order to find the polarization rotation and circular dichroism experienced by the probe light. We find that there are qualitative differences between the results for the mF=0{m}_{F}=0mF​=0 and mF=3{m}_{F}=3mF​=3 cases. While dispersion and consequent Faraday rotation play a dominant role when the atoms are in the mF=0{m}_{F}=0mF​=0 state, it is dissipation and circular dichroism that are important when they are in the mF=3{m}_{F}=3mF​=3 state. Similarly, while the size of the Faraday rotation and the circular dichroism for the mF=0{m}_{F}=0mF​=0 case scales linearly with the applied magnetic field, for the mF=3{m}_{F}=3mF​=3 case it is the shift of the probe polarization change versus frequency that is linearly proportional to the magnetic field strength.