Differences between revisions 3 and 6 (spanning 3 versions) Back to page
Revision 3 as of 9:46AM, Oct 19, 2013
Size: 289
Editor: Sam
Comment:
Revision 6 as of 10:38AM, Oct 19, 2013
Size: 1064
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. As the name suggests, it says how many electrons the material can accomodate at a certain energy value. L<<fl(T)>>he density of states (DOS) is a basic quantity, e.g., for describing 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 (MBDOS), $\int d\vec k A(\vec k, \omega)$, where $A$ is the single particle spectral function, measured by ARPES. Even when the DOS is predicted to be finite at the Fermi energy (&ldquo;band metal&rdquo;), strong correlation can lead to a vanishing MBDOS (&ldquo;Mott-Hubbard insulator&rdquo;).

A very important question that has been very tough to answer so far is &ldquo;does the Mott insulator physics have a distinctive signature in near the optimally doped high temperature superconductor?&rdquo;

=== Links ===

 * <<ln("http://arxiv.org/abs/1310.4668", "The manuscript")>>
 * [[pECFL|Phenomenological ECFL]]
 * [[sECFL|Simple ECFL]]

Anomalous nodal many body density of states

LThe density of states (DOS) is a basic quantity, e.g., for describing 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 (MBDOS), $\int d\vec k A(\vec k, \omega)$, where $A$ is the single particle spectral function, measured by ARPES. Even when the DOS is predicted to be finite at the Fermi energy (“band metal”), strong correlation can lead to a vanishing MBDOS (“Mott-Hubbard insulator”).

A very important question that has been very tough to answer so far is “does the Mott insulator physics have a distinctive signature in near the optimally doped high temperature superconductor?”