2000
DOI: 10.1070/qe2000v030n03abeh001691
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Stimulated IR emission in an optically pumped cesium vapour

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Cited by 3 publications
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“…Moreover, a sharp increase in efficiency of stimulated JR radiation on the 62P312-52D5 transition(3,49 .tm) was achieved under resonance conditions 62P3 -fl2Sjt and 62P3j -m2D512, whereas similar phenomenon for IR-line 3,01 pm ( 62P112-52D3,) is observed by coincidence of w,. Note that 'JR sharply increases when L S tuned in the vicinity ofresonances with frequencies of atomic transitions from the first excited 6P state to situated higher S or D levels.…”
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confidence: 61%
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“…Moreover, a sharp increase in efficiency of stimulated JR radiation on the 62P312-52D5 transition(3,49 .tm) was achieved under resonance conditions 62P3 -fl2Sjt and 62P3j -m2D512, whereas similar phenomenon for IR-line 3,01 pm ( 62P112-52D3,) is observed by coincidence of w,. Note that 'JR sharply increases when L S tuned in the vicinity ofresonances with frequencies of atomic transitions from the first excited 6P state to situated higher S or D levels.…”
mentioning
confidence: 61%
“…As a result, the molecules are excited to upper electronic states that leads to either direct formation of inverse population with respect lower lying electron-vibrational levels, which is accompanied by generation in visible or near IR spectrum region, or results in the decay of excited molecules into atoms , one of which is also excited, and inverse population occurs between two upper atomic levels in this case [1,3]. As a result, the molecules are excited to upper electronic states that leads to either direct formation of inverse population with respect lower lying electron-vibrational levels, which is accompanied by generation in visible or near IR spectrum region, or results in the decay of excited molecules into atoms , one of which is also excited, and inverse population occurs between two upper atomic levels in this case [1,3].…”
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confidence: 99%
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