[Article] On the Essence of Physical Relativity by Larmor J. PDF

By Larmor J.

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14), which gives

2) k with k = 2nn/L, n being a posItive or negative integer, since the Fourier coefficient, Yo, being the spatial average of the height variations, vanishes according to our assumptions. The other Fourier coefficients satisfy Y-k = Y: since y(x) is a real function. On the other hand, k has a cut-off at n/~ since, due to the finite thickness of the line, it is impossible to have an oscillation with a wavelength shorter than 2~. 1 and 2) we have L\E 1 = - - Po L 2 L kk'YkYk' J ei(k+k')xdx k L k' 0 The function under the integral has a period L/(n + n') (n, n' positive or negative integers) so that the integral vanishes unless k + k' = O.

The configuration of the step is given by the set of lengths of the N + 1 close packed surface atomic rows ending at the step edge numbered from left to right (see 30 2. Thermodynamical a nd Statistical Properties of Clean Surfaces Fig. 10. Simple cubic crystal with an arbitrary number of atoms at T = 0 K 0 0 0 0 0 0 0 0 0 0 0 ? ' • ~ I I ~ I I (a) • I ·\... Overhang • • • • • • • • • Island •• • • • • • • • • • • • • • • Adatom • • • • • • • • • • • • • • • • • • (b) Fig. 11a, b. Configurations of a step edge on a sq uare surface lattice (full circles are occupied sites): a configurations allowed in the model.

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[Article] On the Essence of Physical Relativity by Larmor J.


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