首页> 外文期刊>The Journal of Chemical Physics >Absorption and fluorescence of OClO (A)over-tilde (2)A(2)-(X)over-tilde B-2(1) in solid Ne, Ar, and Kr. I. Vibrationally unrelaxed (A)over-tilde ->(X)over-tilde emission
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Absorption and fluorescence of OClO (A)over-tilde (2)A(2)-(X)over-tilde B-2(1) in solid Ne, Ar, and Kr. I. Vibrationally unrelaxed (A)over-tilde ->(X)over-tilde emission

机译:OClO(A)叠峰(2)A(2)-(X)叠峰B-2(1)在固体Ne,Ar和Kr中的吸收和荧光。一,无松弛振动(A)波浪->(X)波浪

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Dispersed laser-induced fluorescence of the (A) over tilde (2)A(2)-->(X) over tilde B-2(1) transition of OClO in solid Ne in the spectral range 500-770 nm was recorded when the origin at 20 991 cm(-1) was excited. Progressions with spacings near 939 and 446 cm(-1) are associated with vibrational modes nu(1) and nu(2) of the (X) over tilde state. A simultaneous fit of bath modes yields omega(1)" = 957.1+/-1.4, omega(2)" = 452.6+/-0.4, x(11)" = 4.47+/-0.04, x(22)" = 0.54+/-0.05, and x(12)" = 4.00+/-0.05 cm(-1). When the 1(0)(1) line of the (A) over tilde-(X) over tilde system at 21 699 cm(-1) was excited, vibrationally unrelaxed emission was observed in the spectral region 480-600 nm. Excitation of the 2(0)(1) line at 21 284 cm(-1) generated weak vibrationally unrelaxed progressions. The visible absorption spectrum of OClO in solid Ne in the region 415-488 nm was recorded with a Fourier-transform spectrometer, yielding nu(00) = 20 991.3, nu(1)' = 707.9, nu(2)' = 292.5, and 2 nu(3)' = 887.6 cm(-1) for the (A) over tilde state. Simultaneous fits considering either only nu(1) and nu(2) modes or all three modes yield corresponding spectral parameters. Similar experiments were performed with OClO in solid Ar and Kr. Pronounced increases in nu(1)' (716.0 cm(-1) in Ar and 712.5 cm(-1) in Kr) and nu(2)' (302.3 cm(-1) in Ar and 303.0 cm(-1) in Kr) and a decrease in nu(00) (188 cm(-1) and 331 cm(-1) red-shifted, respectively) from that in the gas phase indicate substantial perturbation of the A state in solid Ar and Kr. An absorption continuum underlying the A-X system is attributed to absorption to the (1) over tilde(2)A(1) State above the predissociation barrier. The phonon interaction increases and the threshold of the continuum decreases as the matrix host is altered from Ne to Ar to Kr. (C) 1998 American Institute of Physics. [References: 48]
机译:当在500-770 nm光谱范围内记录固体Ne中OClO的(A)在波浪线(2)A(2)->(X)在波浪线B-2(1)上的分散激光诱导的荧光激发了20991 cm(-1)的原点。间距接近939和446 cm(-1)的级数与在波浪号状态下(X)的振动模式nu(1)和nu(2)相关。沐浴模式的同时拟合产生omega(1)“ = 957.1 +/- 1.4,omega(2)” = 452.6 +/- 0.4,x(11)“ = 4.47 +/- 0.04,x(22)” = 0.54 +/- 0.05,并且x(12)“ = 4.00 +/- 0.05 cm(-1)。当(A)在波浪线上的(A)的1(0)(1)线在波浪线系统上的(X)在21699激发了cm(-1),在480-600 nm的光谱范围内观察到了无振动松弛的发射;在21284 cm(-1)处的2(0)(1)线的激发产生了无振动的无松弛振动。用傅立叶变换光谱仪记录415-488 nm区域固体Ne中OClO的光谱,得到nu(00)= 20 991.3,nu(1)'= 707.9,nu(2)'= 292.5和2 nu (3)'= 887.6 cm(-1),适用于波浪线状态下的(A),同时拟合仅考虑nu(1)和nu(2)模态或所有三个模态都可产生相应的光谱参数,使用OClO进行了类似的实验固体Ar和Kr中的nu(1)'(Ar中716.0 cm(-1)和Kr中712.5 cm(-1))和nu(2)'(Ar中302.3 cm(-1)和303.0)明显增加厘米( -1)(以Kr计)和nu(00)的减少(分别为188 cm(-1)和331 cm(-1)红移)都比气相中的低,这表明固体Ar中的A态有很大的扰动和K A-X系统的吸收连续体归因于在预分解势垒上方的波浪线(2)A(1)上的(1)吸收。随着基质主体从Ne变为Ar到Kr,声子相互作用增加,连续谱阈值减小。 (C)1998美国物理研究所。 [参考:48]

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