Stark effects in C13H3f: Passive Q switching of the CO2 laser using C13 enriched methyl fluoride

Eric Weitz; George Flynn; A. M. Ronn

doi:10.1063/1.1659917

Stark effects in C¹³H₃f: Passive Q switching of the CO₂ laser using C¹³ enriched methyl fluoride

Eric Weitz^*, George Flynn, A. M. Ronn

^*Corresponding author for this work

Chemistry

Research output: Contribution to journal › Article › peer-review

15 Scopus citations

Abstract

Stark modulated absorption of CO₂ laser radiation at 1035.462 cm^-1 [P(32), 9.6 μ] by methyl fluoride shows that C ¹³H₃F is the absorbing species. The approximate absorption coefficient of C¹³H₃F at the laser frequency is 0.25 cm^-1 Torr^-1. Passive Q switching of the P(32) 9.6-μ laser transition has been achieved using 50% C¹³ enriched samples and a wide range of CH₃F pressures depending on the gain of the laser cavity.

Original language	English (US)
Pages (from-to)	5187-5190
Number of pages	4
Journal	Journal of Applied Physics
Volume	42
Issue number	12
DOIs	https://doi.org/10.1063/1.1659917
State	Published - Dec 1 1971

ASJC Scopus subject areas

Physics and Astronomy(all)

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10.1063/1.1659917

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title = "Stark effects in C13H3f: Passive Q switching of the CO2 laser using C13 enriched methyl fluoride",

abstract = "Stark modulated absorption of CO2 laser radiation at 1035.462 cm-1 [P(32), 9.6 μ] by methyl fluoride shows that C 13H3F is the absorbing species. The approximate absorption coefficient of C13H3F at the laser frequency is 0.25 cm-1 Torr-1. Passive Q switching of the P(32) 9.6-μ laser transition has been achieved using 50% C13 enriched samples and a wide range of CH3F pressures depending on the gain of the laser cavity.",

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year = "1971",

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T2 - Passive Q switching of the CO2 laser using C13 enriched methyl fluoride

AU - Weitz, Eric

AU - Flynn, George

AU - Ronn, A. M.

PY - 1971/12/1

Y1 - 1971/12/1

N2 - Stark modulated absorption of CO2 laser radiation at 1035.462 cm-1 [P(32), 9.6 μ] by methyl fluoride shows that C 13H3F is the absorbing species. The approximate absorption coefficient of C13H3F at the laser frequency is 0.25 cm-1 Torr-1. Passive Q switching of the P(32) 9.6-μ laser transition has been achieved using 50% C13 enriched samples and a wide range of CH3F pressures depending on the gain of the laser cavity.

AB - Stark modulated absorption of CO2 laser radiation at 1035.462 cm-1 [P(32), 9.6 μ] by methyl fluoride shows that C 13H3F is the absorbing species. The approximate absorption coefficient of C13H3F at the laser frequency is 0.25 cm-1 Torr-1. Passive Q switching of the P(32) 9.6-μ laser transition has been achieved using 50% C13 enriched samples and a wide range of CH3F pressures depending on the gain of the laser cavity.

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Stark effects in C¹³H₃f: Passive Q switching of the CO₂ laser using C¹³ enriched methyl fluoride

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