Abstract

We have studied the charge exchange and compositional dependence of the sandwich thickness of stage-1 alkali-ammonia ternary graphite intercalation compounds K(${\mathrm{NH}}_{3}$${)}_{\mathrm{x}}$${\mathrm{C}}_{\mathrm{y}}$, 0\ensuremath{\le}x\ensuremath{\le}4.33, 12\ensuremath{\le}y\ensuremath{\le}24. A model of the sandwich energy is presented which explicitly accounts for x-dependent charge exchange and size or stiffness effects and is in excellent agreement with experimental measurements of the dependence of the (00l) x-ray diffraction patterns on ammonia vapor pressure. From this model we find that for the stage-1 compound K(${\mathrm{NH}}_{3}$${)}_{4.33}$${\mathrm{C}}_{24}$, f=0.95 and that the ${\mathrm{NH}}_{3}$ molecules solvate some of the electron charge which was originally donated to the carbon layers in the ${\mathrm{KC}}_{24}$ starting material. In addition, the ${\mathrm{NH}}_{3}$ molecules form planar fourfold-coordinated K(${\mathrm{NH}}_{3}$${)}_{4}$ clusters and hence also solvate the ${\mathrm{K}}^{+}$ ions in graphite galleries. We suggest that the K(${\mathrm{NH}}_{3}$${)}_{4}$ clusters together with ``spacer'' ${\mathrm{NH}}_{3}$ molecules constitute the two-dimensional structural analog of the well-studied bulk, three-dimensional metal-ammonia solutions.

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