首页> 外文期刊>The Journal of Chemical Physics >TWO-DIMENSIONAL PHOTOELECTRON SPECTROSCOPY OF ACETYLENE - RYDBERG-VALENCE INTERACTION BETWEEN THE (3-SIGMA(G))(-1)(3P-SIGMA(U))(1) AND (3-SIGMA(G))(-1)(3-SIGMA(U))(1) STATES
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TWO-DIMENSIONAL PHOTOELECTRON SPECTROSCOPY OF ACETYLENE - RYDBERG-VALENCE INTERACTION BETWEEN THE (3-SIGMA(G))(-1)(3P-SIGMA(U))(1) AND (3-SIGMA(G))(-1)(3-SIGMA(U))(1) STATES

机译:(3-SIGMA(G))(-1)(3P-SIGMA(U))(1)和(3-SIGMA(G))(-1)之间乙炔-莱德伯格相互作用的二维光电子能谱(3-SIGMA(U))(1)状态

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Two-dimensional photoelectron spectroscopy is performed for studying autoionization of acetylene in the Franck-Condon gap between the X(2) Pi(u) and A(2)A(g) states of C2H2+. The photoelectron spectrum in the photon energy range from 12.8 to 13.6 eV shows exclusive vibrational excitation of the symmetric C-H stretching mode nu(1) of C2H2+(X(2) Pi(u)), which results from autoionization of the valence state (3 sigma(g))(-1)(3 sigma(u))(1). Vibrational frequencies with anharmonicities of the nu(1) and nu(2) (the symmetric C-C stretch) modes are determined by a least-squares fit of the ionization energies of the observed peaks to a second order expansion. At the photon energy of 14.120 eV, autoionization of the Rydberg state (3 sigma(g))(-1)(3p pi(u))(1) leads to a complicated photoelectron spectrum where probably the trans-bending mode nu(4) of C2H2+ (X(2) Pi(u)) as well as nu(1) is excited, reflecting a substantial metrical change during autoionization. Furthermore, a similar excitation of the nu(4) mode is observed at similar to 13.8 eV. An excellent agreement in positions of the vibrational levels between the spectra at 13.821 and 14.120 eV suggests the presence of the Rydberg stare (3 sigma(g))(-1)(3p sigma(u))(1) at similar to 13.8 eV which has not been identified previously in the photoabsorption or photoionization cross section curves. The constant-ionic-state spectra for the nu(1) = 0-4 levels of C2H2+ (X(2) Pi(u)) show two spectral features: (a) a weak shoulder (upsilon(1) = 0) or a small maximum (nu(1) = 1-4) at 13.8 eV and (b) two groups of peaks in the range of 14.0-14.4 eV. The ratio of the integrated intensity of the 13.8 eV maximum to that of the two groups differs from level to level. This observation is interpreted in terms of a strong interaction between the Rydberg (3 sigma(g))(-1)(3p sigma(u))(1) and valence (3 sigma(g))(-1)(3 sigma(u))(1) states. (C) 1997 American Institute of Physics. [References: 18]
机译:进行二维光电子能谱研究C2H2 +的X(2)Pi(u)和A(2)A(g)态之间的Franck-Condon间隙中乙炔的自电离。光子能量范围为12.8至13.6 eV的光电子谱显示C2H2 +(X(2)Pi(u))的对称CH拉伸模式nu(1)的专有振动激发,这是由价态的自电离引起的(3 sigma(g))(-1)(3 sigma(u))(1)。 nu(1)和nu(2)模式(对称C-C拉伸)的非谐振动频率由观察峰的电离能的最小二乘拟合确定。在14.120 eV的光子能量下,里德堡态(3 sigma(g))(-1)(3p pi(u))(1)的自电离导致复杂的光电子谱,其中可能存在反弯弯曲模式nu(4 )的C2H2 +(X(2)Pi(u))以及nu(1)都被激发,反映出自电离过程中的实质性度量变化。此外,在类似于13.8 eV处观察到nu(4)模式的相似激发。在13.821和14.120 eV处的频谱之间的振动水平位置极佳的一致性表明存在Rydberg凝视(3 sigma(g))(-1)(3p sigma(u))(1)与13.8 eV相似以前在光吸收或光电离截面曲线中尚未确定。 nu(1)= 0-4级C2H2 +(X(2)Pi(u))的恒定离子态光谱显示出两个光谱特征:(a)弱肩(upsilon(1)= 0)或在13.8 eV处有一个小的最大值(nu(1)= 1-4),并且(b)在14.0-14.4 eV范围内的两组峰。最大值的13.8 eV的积分强度与两组的积分强度之比在各级之间有所不同。根据Rydberg(3 sigma(g))(-1)(3p sigma(u))(1)和化合价(3 sigma(g))(-1)(3 sigma)之间的强相互作用来解释此观察结果(u))(1)所述。 (C)1997美国物理研究所。 [参考:18]

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