Download presentation

Presentation is loading. Please wait.

Published byNigel Bigby Modified over 2 years ago

1
Reciprocal lattice and the metric tensor Concept of a metric and the dual space is known from the theory of relativity -line element ds measuring the distance between 2 neighboring events in space time reads metric tensorcoordinate differentials -in flat space time with coordinates In 3D real space we can represent a vectorby its coordinates x i according to basis vectors

2
Changing the basis to changes the coordinates Matrix A and B are related according to -quantities with a subscript transform like the basis vectors and are called covariant -quantities with a superscript transform like the coordinates are called countervariant Now we construct a new set of basis vectors, the countervariant basis, which is identical to the basis of the reciprocal space Consider the scalar product metric tensor where -as we know from relativity

3
The new reciprocal basis reads Let’s show that theform really a set of basis vectors coordinates with respect to the reciprocal basis Note: in the lecture we introduced reciprocal basis vectors so that Application in solid state physics -we have basis vectors (not necessarily orthogonal) Metric tensor Reciprocal lattice vectors

4
As an example let’s consider the reciprocal lattice of the bcc lattice in real space -We know from the conventional approach bcc: a 1 =a(½, ½,-½), a 2 =a(-½, ½,½) and a 3 =a(½,- ½,½) and -Now we use the metric tensor etc.

Similar presentations

© 2016 SlidePlayer.com Inc.

All rights reserved.

Ads by Google