Difference between revisions of "Bloch's Theorem"
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[[Main_Page#Electronic Band Structure of Organic Materials|Return to Band Structure Menu]] | [[Main_Page#Electronic Band Structure of Organic Materials|Return to Band Structure Menu]] | ||
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Bloch’s Theorem | |||
=== Bloch’s Theorem === | |||
As polyenes get longer and longer you could calculate and combine the wavefunctions for all the bonds, but this is not very efficient. Instead it is more powerful to consider the periodicity of repeated units. | As polyenes get longer and longer you could calculate and combine the wavefunctions for all the bonds, but this is not very efficient. Instead it is more powerful to consider the periodicity of repeated units. | ||
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Note: Polyacetylene is made from acetylene but it does not contain triple bonds. | Note: Polyacetylene is made from acetylene but it does not contain triple bonds. | ||
One can concentrate on the repeat unit cell (with cell length a) and the interactions with its neighbors. For example if you move over 2a units from point r you should find the same electron density at that point ja as point r. Because of the translation symmetry electron density r | One can concentrate on the repeat unit cell (with cell length a) and the interactions with its neighbors. For example if you move over 2a units from point r you should find the same electron density at that point ja as point r. Because of the translation symmetry electron density <math>overrightarrow{r}\,\!</math> in cell j (j equiv integer) must equal the electron density at point <math>overrightarrow{r}\,\!</math> in the origin cell. | ||
<math>\vert \Psi (\overrightarrow{r} + j \overrightarrow{a}) \vert^2 = \vert \Psi (\overrightarrow{r} ) \vert ^2\,\!</math> | <math>\vert \Psi (\overrightarrow{r} + j \overrightarrow{a}) \vert^2 = \vert \Psi (\overrightarrow{r} ) \vert ^2\,\!</math> | ||
<math>\Psi (\overrightarrow{r} + j\overrightarrow{a}) = exp (i \overrightarrow{k}j\overrightarrow{A}) (\overrightarrow{r})\,\!</math> | |||
Where | |||
<math>exp (i \overrightarrow{k}j\overrightarrow{A})\,\!</math> is the '''phase factor''' | |||
Revision as of 14:54, 20 May 2009
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Bloch’s Theorem
As polyenes get longer and longer you could calculate and combine the wavefunctions for all the bonds, but this is not very efficient. Instead it is more powerful to consider the periodicity of repeated units.
Note: Polyacetylene is made from acetylene but it does not contain triple bonds. One can concentrate on the repeat unit cell (with cell length a) and the interactions with its neighbors. For example if you move over 2a units from point r you should find the same electron density at that point ja as point r. Because of the translation symmetry electron density <math>overrightarrow{r}\,\!</math> in cell j (j equiv integer) must equal the electron density at point <math>overrightarrow{r}\,\!</math> in the origin cell.
<math>\vert \Psi (\overrightarrow{r} + j \overrightarrow{a}) \vert^2 = \vert \Psi (\overrightarrow{r} ) \vert ^2\,\!</math>
<math>\Psi (\overrightarrow{r} + j\overrightarrow{a}) = exp (i \overrightarrow{k}j\overrightarrow{A}) (\overrightarrow{r})\,\!</math>
Where
<math>exp (i \overrightarrow{k}j\overrightarrow{A})\,\!</math> is the phase factor