Abstract

Spectroscopy of atoms in Rydberg states was an object of extensive investigation (see for example [1–5] and references therein). Usually necessary population of Rydberg states is achieved by means of multi-stage pulse laser pumping. That is why useful signal of ionization current from Single Channel Electron Multiplier (CEM or channeltron) is also pulse signal. Essential temporal instability of this signal is one of the main problems during its registration. More over in order to investigate Rydberg spectra of elements with high value of ionization potential (Al, Cu, Au etc.) it is necessary to apply high-temperature source of atoms (up to 2000 – 3000K). That is why there appears effect of redistribution of population by means of black body radiation. This effect makes additional difficulties to study ionization spectra.

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