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Dissociative Ionization of N2 by Electron Impact.

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Published in: Electronic and Atomic Collisions: Abstracts of Papers: VIII ICPEAC, Beograd, 1973 (1973), pp. 426-427 Status: Postprint (Author’s version)

DISSOCIATIVE IONIZATION OF N

2

BY ELECTRON IMPACT

R. LOCHT and J. SCHOPMAN

Institut de Chimie, Université de Liège, Sart-Tilman par 4000 Liège I (Belgique)

In the recent years much attention has been paid to the N2+ molecular ion. In most experiments, one has

studied the radiative transitions in N2 +

or the translational spectroscopy of N+ fragments of N2 +

spontaneously dissociated or collision induced. Nevertheless there still remain questions regarding the concerned electronic states of N2

+

. In order to extend the available information, we have studied the kinetic energy distributions of the N+ fragments from the dissociative ionization of N2 by electron impact.

In an ion-source, N2 is excited by an electron beam of energies ranging from 0 eV to 80 ev:

less probable

The kinetic energy of the charged fragments,analyzed with a quadrupole mass spectrometer, can be studied at 90 degrees with respect to the electron beam by means of a retarding grid. Using a retarding lens with a reasonable energy resolution (the FWHM of the N2

+

peak is 80 mV)new information could be obtained. Fig.l shows an example of the measured kinetic energy distributions. The kinetic energy values corresponding to the observed maxima are given in Table I. For each maximum the appearance potentials have been measured.

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Published in: Electronic and Atomic Collisions: Abstracts of Papers: VIII ICPEAC, Beograd, 1973 (1973), pp. 426-427 Status: Postprint (Author’s version)

Table I Kinetic energies corresponding to the maxima in the energy distribution of N+ from N2 at an electron

energy of 60 eV.

Band or peak maxima (eV)

0.75 (0.27 - l.0l) 2.29 3.32 5.55

1.15 (1.12 - 1.49) 2.57 3.67 8.28

1.92 (1.65 - 2.02) 2.75 4.03

in brackets: substructure.

The analysis of the retarding curves suggests the existence of vibrational structures which could not yet be completely resolved. From these results it is likely that the maxima(0.27-1·01 eV) correspond to a

predissociation of N2 +

to the first dissociation limit (1-4).The structure observed in several other peaks indicate that there might be more predissociating processes involved.

Figure

Table I Kinetic energies corresponding to the maxima in the energy distribution of N +  from N 2  at an electron  energy of 60 eV

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