Population inversion between I(2P1/2) and I(2P3/2) of atomic iodine generated by excitation transfer from NCl(a1 delta) to I(2P3/2)

Tientsai T. Yang; Vytas Tom Gylys; Robert D. Bower; Lawrence F. Rubin

doi:10.1117/12.145237

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6 June 1993 Population inversion between I(²P_1/2) and I(²P_3/2) of atomic iodine generated by excitation transfer from NC_l(a¹ delta) to I(²P_3/2)

Tientsai T. Yang, Vytas Tom Gylys, Robert D. Bower, Lawrence F. Rubin

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Proceedings Volume 1871, Intense Laser Beams and Applications; (1993) https://doi.org/10.1117/12.145237
Event: OE/LASE'93: Optics, Electro-Optics, and Laser Applications in Scienceand Engineering, 1993, Los Angeles, CA, United States

Abstract

Excited iodine atoms I(²P_1/2) are created when ICl is injected into a stream of NCl(a¹(Delta) ). A population inversion between the I(²P_1/2) and I(²P_3/2) states of atomic iodine was observed using an optical double-resonance technique.

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Tientsai T. Yang, Vytas Tom Gylys, Robert D. Bower, and Lawrence F. Rubin "Population inversion between I(²P_1/2) and I(²P_3/2) of atomic iodine generated by excitation transfer from NC_l(a¹ delta) to I(²P_3/2)", Proc. SPIE 1871, Intense Laser Beams and Applications, (6 June 1993); https://doi.org/10.1117/12.145237

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