Abstract
A microscopic molecular theory is developed for dielectric behavior at molecular crystal surfaces. Since dipolar interactions between layers of molecules decrease rapidly with separation, only layers within a short distance of the surface are affected by it. Algebraic results are obtained relating the local electric field and the macroscopic electric field in a surface layer to an applied uniform electric field, and hence to one another. These lead to expressions for the linear electric susceptibility of a layer and of an assembly of layers. The results provide a basis for calculations of various surface-induced and surface-modified properties.
Original language | English |
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Pages (from-to) | 4532-4535 |
Number of pages | 4 |
Journal | The Journal of chemical physics |
Volume | 97 |
Issue number | 6 |
Publication status | Published - 1992 |