1989
DOI: 10.1007/bf00659996
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Optimal conditions for generation of three-color metal-vapor ion lasers with a hollow cathode

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Cited by 2 publications
(5 citation statements)
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“…The maximum value is at the point where helium and cadmium pressures reach 20 and 0.1 Torr, respectively. This result is in good agreement with our data obtained in experiments with the 441.6 nm laser line in a HCD (Vainer et al 1983, Kalinchenko et al 1989.…”
Section: The Analysis Of Results and A Comparison With Experimentssupporting
confidence: 93%
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“…The maximum value is at the point where helium and cadmium pressures reach 20 and 0.1 Torr, respectively. This result is in good agreement with our data obtained in experiments with the 441.6 nm laser line in a HCD (Vainer et al 1983, Kalinchenko et al 1989.…”
Section: The Analysis Of Results and A Comparison With Experimentssupporting
confidence: 93%
“…Therefore, to determine the pumping rate of the wher W H e * is the rate of excitation of He, ν H e * is the frequency of elimination of excited helium atoms from the active volume due to all the various processes except the Penning ionization (the most important are diffusion and stepwise ionization). When the density of cadmium atoms increases to 10 15 cm −3 , or higher, the second term in the denominator of ( 14) becomes essentially larger than the first one (Kalinchenko et al 1989). This is possible since radiative resonance transitions to the ground state of the He atom (the shunting Penning process) are 'closed' (Ivanov et al 1972) and both upper excited states and metastable ones take part in the Penning process.…”
Section: The Penning Processmentioning
confidence: 99%
“…where v. is the frequency of elastic collisions of electrons with surrounding gas particles [10], f, and Ii are EDF for different intervals of the electron energy namely, f1 describes a highvelocity electrons when they move as a beam, f, is EDF when electrons move as diffusion cloud, e'the threshold energy ofinelastic collisions. The solutions of equations (2) and (3) are given in Appendix.…”
Section: The Methodsmentioning
confidence: 99%
“…The cross sections of metal atom excitation is ten-times more then one of ionization [10]. Meanwhile the time of EDF forming for high-speed electrons is near 1O s. Therefore the regime of excitation by microsecond's pulses is quasi-state for this EDF, and one can solve the stationary equations.…”
Section: The Methodsmentioning
confidence: 99%
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