Motivated by the normal state of the cuprates in which the integrated spectral weight of the optical conductivity or optical sum increases faster than a linear function of the particle density, we derive an f-sum rule for a system in which the kinetic-energy operator in the Hamiltonian is a general function of the momentum squared. Such a kinetic energy arises in scale invariant theories and can be derived within the context of holography. Our derivation of the f-sum rule is based on the gauge couplings of a nonlocal Lagrangian in which the kinetic operator is a fractional Laplacian of order α. We find that the f-sum rule in this case deviates from the standard linear dependence on the particle density. We find two regimes. At high temperatures and low densities, the optical sum is proportional to nTα-1α where T is the temperature. At low temperatures and high densities, the optical sum is proportional to n1+2(α-1)d with d being the number of spatial dimensions. The result in the low-temperature and high-density limit, when α<1, can be used to qualitatively explain the behavior of the effective number of charge carriers in the cuprates at various doping concentrations.
|Original language||English (US)|
|Journal||Physical Review B|
|State||Published - May 9 2017|
ASJC Scopus subject areas
- Electronic, Optical and Magnetic Materials
- Condensed Matter Physics