ar X iv : c on d - m at / 0 30 51 93 v 2 1 3 O ct 2 00 3 Weak magnetism and non - Fermi liquids near heavy - fermion critical points

ar X iv : c on d - m at / 0 30 74 20 17 J ul 2 00 3 Non - Fermi liquid normal state of the Heavy Fermion superconductor UBe 13

ar X iv : 0 81 0 . 55 74 v 1 [ he p - ph ] 3 0 O ct 2 00 8 Neutrino Mass Seesaw Version 3

The origin of neutrino mass is usually attributed to a seesaw mechanism, either through a heavy Majorana fermion singlet (version 1) or a heavy scalar triplet (version 2). Recently, the idea of using a heavy Majorana fermion triplet (version 3) has gained some attention. This is a review of the basic idea involved, its U(1) gauge extension, and some recent developments.

ar X iv : c on d - m at / 9 51 00 95 v 1 1 8 O ct 1 99 5 Metamagnetism and Fermi Surface in the Anderson Lattice Model

We investigate magnetization as functions of external magnetic field H in the U-infinite Anderson lattice model within the leading order approximation in the 1/N-expansion. At T = 0, at H = H M where the Zeeman energy is equal to a certain characteristic energy in the system, the magnetization curve has a kink and the differential susceptibility dM/dH shows a jump. At finite temperature, dM/dH ...

ar X iv : c on d - m at / 0 51 05 97 v 2 17 J an 2 00 7 Thermoelectric transport near the pair breaking quantum phase transition out of a d - wave superconductor

We study electric, thermal, and thermoelectric conductivities in the vicinity of a z = 2 superconductor-diffusive metal transition in two dimensions, both in the high and low frequency limits. We find violation of the Wiedemann-Franz law and a dc thermoelectric conductivity α that does not vanish at low temperatures, in contrast to Fermi liquids. We introduce a Langevin equation formalism to st...

ar X iv : c on d - m at / 0 20 91 44 v 3 7 M ay 2 00 3 Fractionalized Fermi liquids

In spatial dimensions d ≥ 2, Kondo lattice models of conduction and local moment electrons can exhibit a fractionalized, non-magnetic state (FL∗) with a Fermi surface of sharp electron-like quasiparticles, enclosing a volume quantized by (ρa − 1)(mod 2), with ρa the mean number of all electrons per unit cell of the ground state. Such states have fractionalized excitations linked to the deconfin...