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Zhurnal Eksperimentalnoi i Teoreticheskoi Fiziki

Resonance ionization of atoms in the mode of adiabatic inversion of levels

Mikhail Vladimirovich Fedorov

Published Dec 1, 1979• 0 citations
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Resonant ionization of atoms under conditions of adiabatic level inversion

Mikhail Vladimirovich Fedorov

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Characteristics of ionization probability with adiabatic inversion by stochastic fields

Shuichi Hasegawa, Hitoshi Maeda, Takafumi Kakudoh +1 more

Adiabatic inversion in two- and three-level systems excited by stochastic fields is investigated. The stochastic electric fields, which are called the chaotic field and the phase-diffusion field, can invert the population of a two-level atom. In a three-level system, we compare the method of sweeping the laser frequency with that of the resonance excitation by lasers that have bandwidths appropriate to the width of Doppler broadening. When the Doppler shift is taken into account, bandwidths of the electric fields are effective to ionize atoms efficiently. When sweeping the first exciting laser frequency, the delay of the second laser pulse increases the ionization probability. If the half width at half maximum of Doppler broadening is narrow and two lasers irradiate atoms simultaneously, the finite bandwidths of the lasers ionize more atoms than sweeping the laser frequency. On the other hand, if the Doppler broadening is large or the second laser irradiates the atoms properly after the first laser, sweeping the first laser frequency is efficient for ionization. Sweeping the laser frequency is not suitable for the system where the intermediate state's spontaneous-decay constant is short. For that system it is efficient to ionize the atoms by lasers that have the finite bandwidth appropriate for the Doppler broadening.

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Inversion of the resonance line of Sr^+ produced by optically pumping Sr atoms

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We report inversion and lasing on the optically pumped resonance line of Sr+. A mode-locked frequency-doubled dye laser was tuned to excite the dipole-allowed two-electron transition, 5S(2) (1)S(0)-4d5p (3)P1(0), in Sr vapor. The same laser then ionized the excited atoms, selectively producing ions in the Sr+ 5p (2)p(3/2)(0) excited level. The inversion density with respect to the Sr+ ground level was approximately 10(13) cm(-3).

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Mechanism of the resonant ionization of atoms under nonresonant excitation

С. А. Бахрамов, Konstantin N. Drabovich, А. М. Коххаров +2 more

Журнал технической физики•Jul 1, 1987•0 citations
Adiabatic inversion in two- and three-level systems excited by stochastic fields is investigated. The stochastic electric fields, which are called the chaotic field and the phase-diffusion field, can invert the population of a two-level atom. In a three-level system, we compare the method of sweeping the laser frequency with that of the resonance excitation by lasers that have bandwidths appropriate to the width of Doppler broadening. When the Doppler shift is taken into account, bandwidths of the electric fields are effective to ionize atoms efficiently. When sweeping the first exciting laser frequency, the delay of the second laser pulse increases the ionization probability. If the half width at half maximum of Doppler broadening is narrow and two lasers irradiate atoms simultaneously, the finite bandwidths of the lasers ionize more atoms than sweeping the laser frequency. On the other hand, if the Doppler broadening is large or the second laser irradiates the atoms properly after the first laser, sweeping the first laser frequency is efficient for ionization. Sweeping the laser frequency is not suitable for the system where the intermediate state's spontaneous-decay constant is short. For that system it is efficient to ionize the atoms by lasers that have the finite bandwidth appropriate for the Doppler broadening.