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Lorenz KL, Mousa MS. Effects of hot electron emission on a low-conductivity tetracyanoethylene polymer layer including studies of the corrugation of the film surface. Ultramicroscopy. 2003;95(1):113-7doi: 10.1016/s0304-3991(02)00305-4.
Lorenz, K. L., & Mousa, M. S. (2003). Effects of hot electron emission on a low-conductivity tetracyanoethylene polymer layer including studies of the corrugation of the film surface. Ultramicroscopy, 95(1), 113-7. https://doi.org/10.1016/s0304-3991(02)00305-4
Lorenz, K L, and Mousa, M S. "Effects of hot electron emission on a low-conductivity tetracyanoethylene polymer layer including studies of the corrugation of the film surface." Ultramicroscopy vol. 95,1 (2003): 113-7. doi: https://doi.org/10.1016/s0304-3991(02)00305-4
Lorenz KL, Mousa MS. Effects of hot electron emission on a low-conductivity tetracyanoethylene polymer layer including studies of the corrugation of the film surface. Ultramicroscopy. 2003 May-Jun;95(1):113-7. doi: 10.1016/s0304-3991(02)00305-4. PMID: 12535553.
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Ultramicroscopy. 2003 May-Jun;95(1):113-7. doi: 10.1016/s0304-3991(02)00305-4.

Effects of hot electron emission on a low-conductivity tetracyanoethylene polymer layer including studies of the corrugation of the film surface.

Ultramicroscopy

K L Lorenz, M S Mousa

Affiliations

  1. Institut fuer Physikalische und Theoretische Chemie, Universitaet Bonn, Wegelerstrasse 12, D-53115, Bonn, Germany.

PMID: 12535553 DOI: 10.1016/s0304-3991(02)00305-4

Abstract

The effect of strong field electron emission (FEE) on a tetracyanoethylene (TCNE) polymer layer was studied by Field Ion Microscopy (FIM) using TCNE and Ne as the imaging gases. The TCNE polymer was formed on each tungsten tip by radical polymerisation before FEE. The FIM images show field emission spots all over the surface of the tip. The FEM images show a random distribution of several field emission areas at the onset of FEE. After sometime at a current of about microA, there is a transition to higher currents at the same voltage, in which the electron emission pattern changes to have only one emitting area. After this transition, two different types of FIM images were observed, depending on the imaging gas that was used. Neon FIM images at low tip voltages show spots in the areas where the electron emission current was greatest, and at much higher voltages these images show emission from other areas with lower surface corrugation. However, the FIM images with TCNE as the imaging gas do not show any differences between the areas with and without electron emission. The FIM images remain as before FEE, which can be explained by the formation of a new polymer by the reaction of the surface layer with the imaging gas. It is assumed that chemically reactive fragments at the polymer/vacuum interface, which are needed for the polymerisation reaction, are formed by pyrolysis and sputtering processes during FEE.

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