Effect of light polarization on multi-photon ionization of the one-electron atom

1973 ◽  
Vol 8 (1) ◽  
pp. 79-81 ◽  
Author(s):  
R. Parzyński
1988 ◽  
Vol 66 (1) ◽  
pp. 1-6
Author(s):  
K. R. Mah ◽  
F. W. Dalby ◽  
C. W. Barnard

The polarization dependences of some resonant multiphoton ionizations in atomic mercury have been measured with a broadband (bandwidth ≈ 1.5 cm−1) multimode dye laser at moderate light intensities (≈ 500 MW∙cm−2). The multiphoton processes studied were the absorption of four photons to a resonant 1S0, 1D2, or 3D2 level by one-photon ionization. Complete saturation of the one-photon ionization step results in the ionization of all atoms excited to the resonant level. Because of the saturation of the ionization step, the polarization dependence of the four-photon excitation to the resonant level is measured. The theory developed by Dalby et al. is shown to give good agreement with the experiment when it is used to calculate the polarization dependence of the multiphoton transition to the resonant level. For the 6d1D2 resonance, distortions in the polarization dependence and an unusual linewidth dependence on the light polarization were observed. We relate these observations to the alternating current Stark effect and to the production of the third harmonic of the laser light in the focal volume.


2015 ◽  
Vol 17 (5) ◽  
pp. 053011 ◽  
Author(s):  
Lukas Medišauskas ◽  
Felipe Morales ◽  
Alicia Palacios ◽  
Alberto González-Castrillo ◽  
Lev Plimak ◽  
...  

1984 ◽  
Vol 62 (12) ◽  
pp. 1806-1833 ◽  
Author(s):  
Michael N. R. Ashfold ◽  
J. Mark Bayley ◽  
Richard N. Dixon

Two new electronic states of H2O and D2O have been identified in the energy range 84 000–88 000 cm−1 as three-photon resonances in four-photon ionization spectroscopy. Simulations of the rotational intensity distributions using asymmetric top three-photon line strength theory, and rotational analyses, characterize the states as B1 and A2. These Rydberg states are assigned to the excitations 4sa1 ← 1b1[Formula: see text] and 3d2 ← 1b1[Formula: see text] on the basis of equilibrium geometries, quantum defects, and the polarization dependence of their three-photon transition probabilities. The identification of the one-photon forbidden 1A2–1A1 transition, together with published vacuum ultraviolet (VUV) absorption spectra, permits a consistent assignment for all five members of the 3d ← 1b1 complex.The [Formula: see text] and [Formula: see text] states arc predissociatcd via both homogeneous and heterogeneous mechanisms. The homogeneous channel from the [Formula: see text] state shows a dramatic isotope effect, being about two orders of magnitude faster in H2O than from equivalent levels of D2O. The heterogeneous predissociation exhibits irregular vibronic and isotopic dependencies, which can be rationalized in terms of the intercessional role of accidental near resonances with levels of the heavily predissociated [Formula: see text] state. The (000) levels of the [Formula: see text] states of H2O and D2O show contrasting heterogeneous predissociation behaviour, which can be interpreted with a knowledge of the relevant potential energy surfaces and the electronic–rotational Coriolis interactions that couple the states.


2011 ◽  
Vol 60 (6) ◽  
pp. 064209
Author(s):  
Zhang Er-Feng ◽  
Dai Hong-Yi

1990 ◽  
Vol 169 (3) ◽  
pp. 209-212 ◽  
Author(s):  
Jun Yoshinobu ◽  
Xingcai Guo ◽  
John T. Yates

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