Photolytic spectroscopy of simple molecules. I. The production of 5 2D atoms from Cs2
摘要:
A two-photon technique is reported for the measurement of relative cross sections for the selective photolysis of simple molecules into particular product channels. In a demonstration of this method two independently tunable dye lasers were used to sequentially dissociate molecules of Cs2 for wavelengths in the visible range and then to excite the resulting products to Rydberg states which could be readily ionized for detection. With this system the spectra were determined for the selective photolysis of Cs2 into product atoms in the 5 2D3/2 and 5 2D5/2 states. Two relatively broad absorption bands were found, each of which led to the preferential population of a different fine structure components of the 5 2D products. Analysis of the photolysis spectra indicated that both dissociation and predissociation mechanisms were responsible and led to the identification of a new 1Σu and 3Σu state correlated with the 5 2D atomic states.
Measurement of the absolute third-order rate constant for the reaction between Cs + I + He by time-resolved atomic resonance fluorescence monitoring of iodine atoms in the vacuum ultraviolet region {I[6s(<sup>2</sup>P<sub>J</sub>)]–I[5p<sup>5</sup>(<sup>2</sup>P<sub>3/2</sub>)]} coupled with steady atomic resonance fluorescence on atomic caesium [Cs(7<sup>2</sup>P<sub>J</sub>)– Cs(6<sup>2</sup>S<sub>1/2</sub>)] in the visible region
作者:David Husain、John M. C. Plane、Chen Cong Xiang
DOI:10.1039/f29858101675
日期:——
nm I[5p46s(2P3/2)]–I[5p5(2P3/2)]} using photon counting in the vaccum ultraviolet region. Cs(62S1/2) was monitored by steadyatomicresonancefluorescence of the Rydberg doublet at λ= 457 nm [Cs(72PJ)–Cs(62S1/2)] using phase-sensitive detection. We report a measured absolutethird-orderrateconstant of k1(T= 491 K)=(7.9 ± 1.2)× 10–31 cm6 atom–2 s–1, which we believe to be the first measurement of
我们提出了反应Cs + I + He→CsI + He的绝对三阶速率常数的直接动力学测量。(1)I(5 2 P 3/2)是通过在流动系统中由CH 3 I在来自热管炉的过量原子铯存在下的反应中对CsI进行重复脉冲辐照而产生的。通过时间分辨的原子共振荧光在λ= 178.3 nm I [5 p 4 6 s(2 P 3/2)] – I [5 p 5(2 P 3/2)]监测基态碘原子。}在真空紫外线区域使用光子计数。铯(6 2 S 1/2)通过相变检测在λ= 457 nm [Cs(7 2 P J)–Cs(6 2 S 1/2)]上通过Rydberg doublet的稳定原子共振荧光进行监测。我们报告了测得的绝对三阶速率常数k 1(T = 491 K)=(7.9±1.2)×10 –31 cm 6原子–2 s –1,我们认为这是此类的首次测量。我们还报告了反应I + Cs 2 →CsI + Cs(3)为k
Raman Spectroscopic Investigation of Matrix Isolated Rubidium and Cesium Molecules: Rb<sub>2</sub>, Rb<sub>3</sub>, Cs<sub>2</sub>, and Cs<sub>3</sub><sup>,</sup><sup>1</sup>
作者:Andreas Kornath、Anja Zoermer、Ralf Ludwig
DOI:10.1021/ic990506m
日期:1999.10.1
The rubidiummolecules Rb(2) and Rb(3) and the cesiummolecules Cs(2) and Cs(3) were isolated in argonmatrixes and characterized for the first time by Raman spectroscopy. The fundamental frequencies of the dimers were observed at 59.1 cm(-)(1) for the rubidium dimer and 45.8 cm(-)(1) for the cesium dimer. The Raman lines of the rubidium trimer appeared at 38.3 and 53.9 cm(-)(1), and the lines of the
Optically pumped atomic spin orientation and the law of mass action for 2Cs⇄Cs<sub>2</sub>
作者:J. J. Ho、Chongye Wang、R. A. Bernheim
DOI:10.1063/1.455013
日期:1988.9
The effect of optically pumped atomic spin orientation on the atom–dimer equilibrium in cesium vapor has been observed. Such a shift in equilibrium was predicted over two decades ago and is due to the redistribution of spin-determined bonding and antibonding collision trajectories. Orientation of the total spin angular momentum of 6 2S1/2 ground state Cs atoms in the vapor phase was produced by optical pumping with a tunable cw dye laser. A decrease in the equilibrium molecular density resulted and was measured using laser induced fluorescence from the B 1Πu state. The shift in equilibrium is a function of the degree of atomic orientation and could be observed in the temperature range 383–421 K for cesium vapor in a glass cell which also contained a He–N2 buffer gas mixture with a composition ratio of 9:1.
High resolution laser spectroscopy of the Cs2 C 1Πu state: Perturbation and predissociation
High resolution spectra of the C 1Πu(v′,J′)−X 1Σg+(v″,J″) transitions of the Cs2 molecule were measured by the technique of Doppler-free optical–optical double resonance polarization spectroscopy. A number of C 1Πu(v⩾13,J) levels were found to be strongly perturbed. Transitions to the perturbing levels were observed, and the energy shifts of e and f levels of the C 1Πu state were studied and identified as originating from perturbations between the C 1Πu and (2)3Π1u states. Molecular constants of the C 1Πu(v=7–18) and (2)3Π1u(v=v0–v0+6) levels were determined. Line splittings were observed for the transitions to the C 1Πu(v=13 and 14,Jf) levels which were identified as hyperfine splittings originating from additional interaction with the (2)3Σu+ state. Remarkable line broadenings were observed in the transitions to the C 1Πu(v>15,Je and f) levels, and were identified as originating from the predissociation through the dissociative (2)3Σu+ state. The repulsive potential curve of the (2)3Σu+ state was estimated to cross that of the C 1Πu state around the outer turning point of the C 1Πu(v=16 or 17) level.
Study of the chemiluminescent reaction between alkali dimers and oxygen atoms
作者:H. Figger、R. Straubinger、H. Walther
DOI:10.1063/1.441820
日期:1981.7
The reaction of alkali dimers with oxygen atoms has been studied in a crossed beam experiment. Strong chemiluminescence of the reaction products was observed. It is shown that the luminescence was emitted by alkali atoms from the reaction M2+O→MO+M (M alkali atom). M can be excited up to the exoergicity of this reaction at least in the cases M = Cs and Na. For M = Cs, detailed rate constants for the excitation of the different excited states have been determined using both laser induced fluorescence and chemiluminescence. The rates decrease nearly exponentially as a function of the excitation energy. They partly follow the expectation of statistical theories. Absolute reaction cross sections have been determined for all of the reactions investigated. They agree partially with those predicted by the harpoon model.