Tunability of silicon clathrate film properties by controlled guest-occupation of their cages.

Type I and type II silicon clathrates are guest-host structures made of silicon polyhedral cages large enough to contain atoms that can be either inserted or evacuated with only a slight volume change of the structure. This feature is of interest not only for batteries or storage applications but also for tuning the properties of the silicon clathrate films. The thermal decomposition process can be tuned to obtain Na8Si46 and Na2 View Article and Find Full Text PDF

First principles study of the electric polarization and of its switching in the multiferroic GaFeO3 system.

The electric polarization in the multiferroic GaFeO(3) system is determined from its electronic structure using first principles methods and the modern theory of polarization. By carefully following the electric polarization on a path connecting the polar and centrosymmetric structures, it is found to be -25 μC cm(-2), which is ten times larger than a previous estimation given in the literature a few years ago and two times smaller than the value obtained in a recent similar study. The switching of this electric polarization through a centrosymmetric structure is discussed in terms of the total energy barrier.

Ab initio study of the electronic and magnetic properties of Sr(2-x)La(x)Fe(1+y/2)Mo(1-y/2)O6 double perovskites.

Using the first-principles full potential linearized augmented plane wave method, the electronic structure of Sr(2-x)La(x)Fe(1+y/2)Mo(1-y/2)O6 (SLFMO) double-perovskite systems is investigated for x = 1/2 and 1 and for y = +1 and -1. Substituting Sr atoms by La atoms allows one to tune the electrons added into the minority spin band and enhances the half-metal feature--according to the rigid band shift model--even if the magnetization decreases with increasing La concentration. By taking into account the chemical disorder on the Fe and Mo sites, resulting from the introduction of La as shown experimentally, it is shown (i) that a supplemental magnetization reduction occurs because the magnetic moment on the Fe antisite is opposite to the one on the Fe regular sites and (ii) that the half-metal feature is preserved in SLFMO for x = 1/2 and 1 contrary to the case for SFMO.