Differences between revisions 2 and 4 (spanning 2 versions) Back to page
Revision 2 as of 9:45AM, Oct 19, 2013
Size: 184
Editor: Sam
Comment:
Revision 4 as of 9:47AM, Oct 19, 2013
Size: 544
Editor: Sam
Comment:
Deletions are marked like this. Additions are marked like this.
Line 3: Line 3:
<<fl(T)>>he density of states is a basic quantity that students learn, when they learn how to describe free electrons in a solid. <<fl(T)>>he density of states is a basic quantity that students learn, when they learn how to describe free electrons in a solid. As the name suggests, it says how many electrons the material can accomodate at a certain energy value.

In a strongly correlated electron system such as high temperature superconductors, the equivalent quantity is the ''many body'' density of states, $\int d\vec k A(\vec k, \omega)$, where $A$ is the single particle spectral function, measured by ARPES.

Anomalous nodal many body density of states

The density of states is a basic quantity that students learn, when they learn how to describe free electrons in a solid. As the name suggests, it says how many electrons the material can accomodate at a certain energy value.

In a strongly correlated electron system such as high temperature superconductors, the equivalent quantity is the many body density of states, $\int d\vec k A(\vec k, \omega)$, where $A$ is the single particle spectral function, measured by ARPES.