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A method combining laser-induced fluorescence and injection of a neutral beam was employed to determine a time-varying electron-density in a conical theta-pinch plasma. The method consists of measuring the electron excitation rate relative to the spontaneous emission coefficient. An expression for the electron density in terms of the measured fluorescence and collision-induced emission signals has been formulated, taking into account the appreciable population of the excited level, as well as incomplete laser saturation. Neutral atomic beams (Li and Mg) were produced using laser ablation. A low-density hydrogen plasma was produced using a conical theta-pinch to simulate tokamak edge-plasma conditions. Using a Langmuir double-probe and emission spectroscopic methods, a time-varying electron density and an electron temperature. Measuring the electron excitation of the atomic beams with laser-induced fluorescence (LIF), the rapidly varying electron density could be deduced using either the Li 670 nm or the Mg 285 nm transition.
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Breger et al. (1991) studied this question.
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