The insulating state of matter is characterized by the excitation spectrum, but also by qualitative features of the electronic ground state. The insulating ground wave function in fact (i) sustains macroscopic polarization, and (ii) is localized. We give a sharp definition of the latter concept and we show how the two basic features stem from essentially the same formalism. Our approach to localization is exemplified by means of a two-band Hubbard model in one dimension. In the noninteracting limit, the wave function localization is measured by the spread of the Wannier orbitals
With the aid of functional-integral technique, we show that the strongly correlated electron system ...
The most direct signature of electron localisation is the tendency of an electron in a many-body sys...
A simple relation between the local energy spectrum and the time evolution of a wavepacket diffusing...
At variance with what happens in metals, the electronic charge in insulators cannot flow freely und...
Materials are traditionally classified accordind to their conduction properties. In quantum mechanic...
Electrons, electron holes, or excitations in finite or infinite 'multimer systems' may be localized ...
The qualitative difference between insulators and metals stems from the nature of the low-lying exci...
An insulator differs from a metal because of a different organization of the electrons in their grou...
The extent of electron localization and delocalization in molecular and condensed phases has been th...
We consider the combined influence of disorder, electron-electron interactions and quantum hopping o...
Density functional and quantum Monte Carlo methods are used to examine the behaviour of the many-ele...
539-549A theory which describes behaviour of excess electrons in a liquid-like medium is reviewed. T...
The deexcitation probability of localized electronic states in metals has been studied regarding the...
The localization properties of a two-dimensional electron system in the presence of a random magneti...
We study numerically the time evolution of the coupled system of an electron, described by a tight-b...
With the aid of functional-integral technique, we show that the strongly correlated electron system ...
The most direct signature of electron localisation is the tendency of an electron in a many-body sys...
A simple relation between the local energy spectrum and the time evolution of a wavepacket diffusing...
At variance with what happens in metals, the electronic charge in insulators cannot flow freely und...
Materials are traditionally classified accordind to their conduction properties. In quantum mechanic...
Electrons, electron holes, or excitations in finite or infinite 'multimer systems' may be localized ...
The qualitative difference between insulators and metals stems from the nature of the low-lying exci...
An insulator differs from a metal because of a different organization of the electrons in their grou...
The extent of electron localization and delocalization in molecular and condensed phases has been th...
We consider the combined influence of disorder, electron-electron interactions and quantum hopping o...
Density functional and quantum Monte Carlo methods are used to examine the behaviour of the many-ele...
539-549A theory which describes behaviour of excess electrons in a liquid-like medium is reviewed. T...
The deexcitation probability of localized electronic states in metals has been studied regarding the...
The localization properties of a two-dimensional electron system in the presence of a random magneti...
We study numerically the time evolution of the coupled system of an electron, described by a tight-b...
With the aid of functional-integral technique, we show that the strongly correlated electron system ...
The most direct signature of electron localisation is the tendency of an electron in a many-body sys...
A simple relation between the local energy spectrum and the time evolution of a wavepacket diffusing...