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Vibrational Autoionization in NH3 and its Isotopomers in the 10-12 eV photon energy range.

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Published in : ICPEAC Abstracts (International Conference on the Physic of Electronic and Atomic Collisions), (1991), p. 126 Status : Postprint (Author’s version)

VIBRATIONAL AUTOIONIZATION IN NH

3

AND ITS ISOTOPOMERS

IN THE 10-12 eV PHOTON ENERGY RANGE.

R. Locht* , B. Leyh* , W. Denzer+ , G. Hagenow+ , H. Baumgärtel+ . *Institut de Chimie, Université de Liège, Sart-Tilman par 4000 Liège 1, Belgium.

+

Institut fur Physikalische Chemie, FU Berlin, Takustrasse 3, D-1000 Berlin 33, FRG.

In the frame of the dissociative ionization work on NH3 , the contribution of autoionization was shown

to play an important role1 .However autoionization in this molecule has scarcely been investigated.

This phenomenon was first examined in the 10-12 eV photon energy range for NH3 and its isotopomers

NH2D, NHD2 and ND3. The abovemen-tioned energy range lying below the lowest appearance energy for

fragmentation of NH3 in the NH2 +

+H channel, photoionization mass spectrometry is a suitable method for this investigation. Synchrotron radiation provided by the electron storage ring BESSY (Berlin) has been used as a light source dispersed by a 1m NIM-monochromator. A quadrupole filter is used for mass analysis.

The photoionization efficiency curves of the four molecular ions were recorded. An abundant and fairly well resolved structure is observed. The photoion yield curves show drastic differences in shape and intensity distribution.

By proper filtering and by numerical differentiation of the photoion yield curves, simulated photoelectron spectra are obtained. Onsets, corresponding to the adiabatic ionization energies, are measured at 10.072 ± 0.010 eV for NH3, NH2D and NHD2 and at 10.083 ± 0.010 eV for ND3 . Wavenumbers and

anharmonicities could be deduced and compared to photoelectron spectroscopic data when available2,3

By subtracting the filtered photoion yield curve from the original photoionization efficiency curve, the autoionization structure could be enhanced. A typical example is shown in figure 1 in the case of ND3+. The

same procedure has been applied to NH3, NH2D +

and NHD2 +

All autoionization features could be classified into long vibrational progressions belonging to nsa1 and

npe (n=5,6,7) Rydberg series converging to the NH3 +

(X 2A1 ) state. The relative intensity of each series

markedly varies with the isotopic substitution. In the case of NH3 the results are in good agreement with those

obtained by EELS 4.

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Published in : ICPEAC Abstracts (International Conference on the Physic of Electronic and Atomic Collisions), (1991), p. 126 Status : Postprint (Author’s version)

These Rydberg states autoionize vibrationally. A close correlation is observed between the parity of the vibrational transition ∆v and the intensity of the corresponding autoionization process. Although both even and odd ∆v transitions are observed, to odd ∆v values correspond the strongest intensities. This observation can be understood by applying symmetry considerations to vibrational autoionization theory 5 .

References.

1. R.Locht, G.Hagenow, W.Denzer, H.Baumgärtel BESSY Jahresbericht 1988, p135.

2. J.W.Rabalais, L.Karlsson, L.O.Werme, T.Berg mark, K.Siegbahn, J.Chem.Phys.58(1973)3370. 3. M.J.Weiss, G.M.Lawrence, J.Chem.Phys. 53 (1970)214.

4.M.Furlan, M.J.Hubin-Franskin, J.Delwiche, D.Roy,J.E.Collin,J.Chem.Phys.82(1985)1797.

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