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首页> 外文期刊>The Journal of Chemical Physics >Raman and absorption spectrum of mass-selected lutetium dimers in argon matrices
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Raman and absorption spectrum of mass-selected lutetium dimers in argon matrices

机译:氩基质中质量选择的dim二聚物的拉曼光谱和吸收光谱

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We report on the absorption, resonance Raman, and Raman excitation profile spectra of mass selected lutetium dimersin argon matrices. Two.broad absorption regions were found between 415 and 545 nfi with peaks at418, 433, 452,472,505,540 nm, and between 635 and 660nmwith peaks at 640 and 652 nm. ResbnanceRaman spectra were obtained by excitation into one of these regions with the visible light of an Ar ion laser between 458 and 514 nm. Two progressions were assigned to lutetium dimmers. We interpret them to represent two distinct electronic states: A grotind-state X and an excited state A. For the ground (X) state, w~ obtain We= 121.6~0.8cm-l with WeXe =0.16::!:0.10cm-l, leading to a spectroscopic dissociation ene;gy of 2.9::!: 1.8eV, and force constant ke=0:76::!: 0.01 mdyne/A.. The lowest excited electronic state (A) has an origin at 210,7 cm -1 and almost identical vibrational parameters. C()fuparison of spectroscopic properties of lanthanide dimmers is disc.ussed, and evidence is presented that lutetium should occupy the position normally given to lanthanum in the periodic table.
机译:我们报告了mass选择的二聚体氩基体中质量的吸收,共振拉曼和拉曼激发曲线。在415和545 nfi之间发现两个宽吸收区,峰值在418、433、452,472,505,540 nm处,在635和660nm之间,峰值在640和652 nm之间。通过用458至514nm之间的Ar离子激光的可见光激发到这些区域之一中而获得ResbnanceRaman光谱。调光器分为两个级数。我们将它们解释为代表两种不同的电子状态:固位态X和激发态A。对于基态(X),w〜得到We = 121.6〜0.8cm-1,WeXe = 0.16 ::!:0.10cm -l,导致光谱解离烯gy为2.9 ::!:1.8eV,力常数ke = 0:76 ::!:0.01 mdyne / A。最低激发电子态(A)的起源为210,7 cm -1和几乎相同的振动参数。讨论了镧系元素二聚体的光谱性质的C()fuparison,并提供了证据表明应占据元素周期表中通常赋予镧的位置。

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