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首页> 外文期刊>The Journal of Chemical Physics >VIBRONIC ANALYSIS OF FLUORESCENCE SPECTRUM OF NO2 (D)OVER-TILDE(2)B(2)(0,0,0) IN THE REGION OF 250-550 NM
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VIBRONIC ANALYSIS OF FLUORESCENCE SPECTRUM OF NO2 (D)OVER-TILDE(2)B(2)(0,0,0) IN THE REGION OF 250-550 NM

机译:250-550 NM区NO2(D)波浪(2)B(2)(0,0,0)荧光光谱的虚拟分析

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The dispersed fluorescence spectrum of NO2 (D) over tilde(2)B(2)(0,0,0) was measured and analyzed in the spectral range of 250-550 nm. The strong fluorescence bands in 250-350 nm correspond to (D) over tilde(2)B(2)(0,0,0)-->(X) over tilde(2)A(1)(n(1)=0-9, n(2)=0-5, n(3)=0) with a Franck-Condon maximum at n(1)=4 and n(2)=0. The weak and broad bands in 350-410 nm are built on a progression of bending frequency, 710 cm(-1). The lower state responsible for this fluorescence was interpreted as admixture B-ev(2) levels generated by a vibronic coupling between a(1)-vibrational levels on (A) over tilde(2)B(2) and highly excited b(2) (X) over tilde(2)A(1). The medium-intensity bands in 410-550 nm were assigned to (D) over tilde(2)B(2)(0,0,0)-->(C) over tilde(2)A(2)(n(1)=0-2, n(2)=0-5, n(3)=0-2) with a Franck-Condon maximum at n(1)=0, n(2)=2, and n(3)=0. The vibrational frequencies of (C) over tilde(2)A(2) are 1010 cm(-1) for symmetric stretch (omega(1)), 740 cm(-1) for bending (omega(2)), and 250 cm(-1) for antisymmetric stretch (omega(3)). The simple Franck-Condon calculation for (D) over tilde(2)B(2)(0,0,0)-->(C) over tilde(2)A(2)(n(1),n(2),n(3)) gives the approximate geometry of the (C) over tilde(2)A(2) State as r(N-O)similar to 134 pm and theta similar to 108 degrees. The partial rotational structure of (C) over tilde(2)A(2)(0,0,0) was analyzed using an optical-optical double resonance measurement, which confirms the A(2) vibronic symmetry. The origin of NO2 (C) over tilde(2)A(2) (T-0) was determined to be around 16 234 cm(-1). (C) 1996 American Institute of Physics. [References: 22]
机译:在250-550 nm的光谱范围内,测量并分析了在tilde(2)B(2)(0,0,0)上NO2(D)的分散荧光光谱。 250-350 nm处的强荧光带对应于在tilde(2)B(2)(0,0,0)上的(D)(在tilde(2)A(1)(n(1))上) = 0-9,n(2)= 0-5,n(3)= 0),弗兰克-康登最大值为n(1)= 4,n(2)= 0。在350-410 nm的弱带和宽带建立在710 cm(-1)弯曲频率上。负责此荧光的较低状态被解释为混合物B-ev(2)的水平,它是由在波浪号(2)B(2)上的(A)上的a(1)-振动水平和高度激发的b(2)之间的振动耦合产生的)(X)在波浪号(2)A(1)上。在tilde(2)B(2)(0,0,0)->(C)上在tilde(2)A(2)(n( 1)= 0-2,n(2)= 0-5,n(3)= 0-2),弗兰克-康登最大值在n(1)= 0,n(2)= 2和n(3 )= 0。波浪线(2)A(2)上的(C)振动频率分别为1010 cm(-1)(对称拉伸(omega(1)),740 cm(-1)弯曲(omega(2))和250) cm(-1)用于反对称拉伸(omega(3))。在波浪号(2)B(2)(0,0,0)上的(D)的简单Franck-Condon计算-在波浪号(2)A(2)(n(1),n(2)上的(C) ),n(3))给出在tilde(2)A(2)状态下(C)的近似几何形状,其中r(NO)近似于134 pm,θ近似于108度。使用光学双共振测量分析了波浪号(2)A(2)(0,0,0)上(C)的部分旋转结构,这证实了A(2)的振动对称性。代名词(2)A(2)(T-0)上的NO2(C)的起源被确定为大约16234 cm(-1)。 (C)1996年美国物理研究所。 [参考:22]

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