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On the stability of crystal lattices. I

  • Max Born (a1)
Abstract

The stability of lattices is discussed from the standpoint of the method of small vibrations. It is shown that it is not necessary to determine the whole vibrational spectrum, but only its long wave part. The stability conditions are nothing but the positive definiteness of the macroscopic deformation energy, and can be expressed in the form of inequalities for the elastic constants. A new method is explained for calculating these as lattice sums, and this method is applied to the three monatomic lattice types assuming central forces. In this way one obtains a simple explanation of the fact that the face-centred lattice is stable, whereas the simple lattice is always unstable and the body-centred also except for small exponents of the attractive forces. It is indicated that this method might be used for an improvement of the, at present, rather unsatisfactory theory of strength.

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(2) M. Born Atomtheorie des festen Zustandes (Leipzig, 1923).

(7) M. Blackman Proc. Roy. Soc. A, 148 (1935), 365; 149 (1935), 117; 159 (1937), 416; 164 (1938), 62; Proc. Cambridge Phil. Soc. 33 (1937), 94.

(8) K. Herzfeld and R. H. Lyddane Phys. Rev. 54 (1938), 846.

(9) M. Born J. Chem. Phys. 7 (1939), 591.

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Mathematical Proceedings of the Cambridge Philosophical Society
  • ISSN: 0305-0041
  • EISSN: 1469-8064
  • URL: /core/journals/mathematical-proceedings-of-the-cambridge-philosophical-society
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