1970 年 29 巻 6 号 p. 1479-1490
A many-body theory for nearly-free electrons has been constructed by introducing “ Bloch-pair operators,” αk and βk, which are related to free-particle operators through the transformation
(Remark: Graphics omitted.)
where h is 2π times a reciprocal lattice vector, and θh is the sign of the relevant Fourier component, vh, of the periodic field. This theory has been then applied to the annihilation of positrons in the periodic field. The interaction between a positron and a Bloch electron, has been, for the first time, taken into account through a few simplest diagrams. The result shows that a fairly sharp break of the angular-correlation curve occurs a the hexagonal-zone-face position in copper just as expected from the experiments previously made by the present author and his collaborator.
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