The following experimental features of ultra-soft X-ray absorption molecular spectra [l], [2] are discussed : 1. Existence of strong absorption maxima on the high energy side of ionization thresholds (in continuum) of inner shells of atoms in molecules. 2. Similarity of the fine structure of K (1 S) spectrum of fluorine and L (2 p) spectrum of sulphurin the number of maxima and their energy position with respect to ionization threshold in molecule SF6. 3. Absence of sharp rise in absorption coefficient at the ionization threshold of inner shells of the central atom surrounded by electronegative atoms in high symmetrical molecules (SF6, SiF4 and others). [l] ZIMKINA (T. M.), FOMICHEV (V. A.), Dokladi ANSSSR, 1966, 169, 1304. [2] ZIMKINA (T. M.), VINOGRADOV (A. S.) (c X-ray spectra and electronic structure of matter )) 11, I. M. F. AN USSR, Kiev, 1969. At present we have studied the ultrasoft X-ray absorption spectra of several complex inorganic molecules (SF6, SiF,, SiC14, BF,, BCl,, NF, and the others). All these spectra show a large difference of the fine structure near the absorption edges of the inner atomic shells from the well known fine structure of X-ray spectra of atoms and simple molecules. The latter consists of several discret lines lying before the absorption edge and their intensity and energy separation decrease rapidly with approach to the edge. The appearance of these lines in X-ray absorption spectra is attributed to the exciton mechanism. If the electron ejected from the inner shell moves in a CoulomL field the lines of the fine structure can be represented as a_Rydberg series of absorption lines. One of the specific feature of the ultrasoft X-ray absorption spectra of molecules consists in existence of several strong absorption lines extending over 10-20 eV. Some of these discret lines were found to be behind the absorption edge in continuum. The fine structure in these spectra cannot be attributed to transition of inner atomic electrons to a Rydberg series of excited states neither in intensity nor in the energy position before the ionization threshold. Therefore the hydrogenic model cannot be used to interpretation the ultrasoft molecular spectra. The second feature consists of absence of any detectable jump ratio at the ionization thresholds of the inner electrons of central atom in symmetrical molecules (SF,, SiF,, SiCI,, BF,, NF,, BCI,). Let's consider for a example the ultrasoft X-ray absorption spectra of SF, molecule. It is known, the X-ray absorption spectra of sulphur in SF, have unusual fine structure near the K and the LI,,,,I absorption edges [l], [2]. Recently the K fluorine absorption spectrum in this molecule has been studied [3]. Besides, the energy of l S fluorine and 2 p sulphur atomic levels in SF, molecule have been measured by photoelectron spectrometry [4]. Using these data we can compare the sulphur and fluorine spectra in the same energy scale and receive the additional information about the nature of the fine structure of SF,
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