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I_2(B) formation in the oxygen-iodine laser medium

机译:氧碘激光介质中I_2(B)的形成

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摘要

The mechanism by which I_2(B) is excited in the chemical oxygen-iodine laser was studied by means of emission spectroscopy. Using the intensity of the O_2(b~1Σ,v'=0) → O_2(X~3Σ,v"=0) band as a reference, I_2(B) relative number densities were assessed by measuring the I_2(B,v')→ I_2(X,v") emission intensities. Vibrationally excited singlet oxygen molecules O_2(a~1Δ, v'=1) were detected using IR emission spectroscopy. The measured relative density of O_2(a~1Δ,v'=1) for the conditions of a typical oxygen-iodine laser medium amounted to ~15% of the total O_2 content. Mechanisms for I_2(B) formation were proposed for both the I_2 dissociation zone and the region downstream of the dissociation zone. Both pumping mechanisms involved electronically excited molecular iodine I_2(A', A) as an intermediate. It has been suggested that, in the dissociation zone, the I_2 A', and A states are populated in collisions with vibrationally excited singlet oxygen molecules O_2(a~1A,v'). In the region downstream of the dissociation zone the intermediate states are populated by iodine atom recombination process. I_2(B) is subsequently formed in collisions of I_2(A',A) with singlet oxygen. We also conclude that I_2(B) does not participate measurably in the I_2 dissociation process and that energy transfer from O_2(b~1 Σ) does not excite I_2(B) to a significant degree.
机译:通过发射光谱研究了化学氧碘激光器中I_2(B)激发的机理。以O_2(b〜1Σ,v'= 0)→O_2(X〜3Σ,v“ = 0)的强度为参考,通过测量I_2(B,v)评估I_2(B)相对数密度。 ')→I_2(X,v“)发射强度。利用红外光谱法检测了振动激发的单线态氧分子O_2(a〜1Δ,v'= 1)。在典型的氧碘激光介质条件下测得的O_2相对密度(a〜1Δ,v'= 1)占总O_2含量的〜15%。提出了I_2解离区和解离区下游区域的I_2(B)形成机理。两种泵送机制都涉及电子激发的分子碘I_2(A',A)作为中间体。已经提出,在解离区中,I_2A'和A状态与振动激发的单线态氧分子O_2(a〜1A,v')碰撞。在离解区下游的区域中,中间态通过碘原子重组过程填充。随后,在I_2(A',A)与单线态氧的碰撞中形成I_2(B)。我们还得出结论,I_2(B)不能显着地参与I_2的解离过程,并且从O_2(b〜1Σ)传递的能量不会明显激发I_2(B)。

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