Research Interests
Strong Correlations in Layered Materials
My research on strong correlations began with investigations of heavy fermions, transition metal oxides and layered organic charge transfer salts, and the value of the Kadowaki-Woods ratio in these materials. The Kadowaki-Woods ratio is the ratio of the electron-electron scattering contribution to resistivity to the square of the electronic contribution to heat capacity. This ratio is constant for most heavy fermion materials, and for transition metals, taking different values in each. However, layered materials do not have a constant value, and many exotic reasons have been posited, including proximity to a quantum critical point or a strange temperature dependence of electron-phonon interactions in low dimensions. Some less exotic possibilities have also been discussed, for example using volumetric (rather than molar) units in the heat capacity (to be consistent with the units of resistivity) reduces the variation in the KWR in layered transition metal oxides. If one of these arguments were correct, then the Kadowaki-Woods ratio would be a useful identifying feature of one of these unusual physical properties. I, together with Ben Powell and John Fjærestad, investigated a simple phenomenological Fermi liquid theory. We found that:- The KWR is not constant, in general.
- The reason that it appears constant in the heavy fermions and transition metals is due to other (material dependent) factors being constant.
- By correctly including these material-dependent factors one can formulate an new ratio which is universal in Fermi liquids.
I have used density functional theory to parameterise model Hamiltonians for low-dimensional strongly correlated materials such as the Fabre salts and Pd(dmit)2 derivatives. I applied exact diagonalisation and other many-body techniques to solve these model Hamitonials and study the interplay of frustration and anisotropy with correlations in low dimensions. In a recent preprint, I showed that there are important qualitative differences between t-t' triangular lattices and fully anisotropic triangular lattices (FATL). This work was done in the context of Pd(dmit)2 materials, whose electronic structure is fairly well approximated by a t-t' model. However, we show that the relatively small deviation from t-t' seen in these materials is enough to greatly enhance the transition to the spin-liquid phase.