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

ar X iv : 1 00 6 . 37 94 v 3 [ he p - th ] 10 A ug 2 01 0 Holographic metals and the fractionalized Fermi liquid

We show that there is a close correspondence between the physical properties of holographic metals near charged black holes in anti-de Sitter (AdS) space, and the fractionalized Fermi liquid phase of the lattice Anderson model. The latter phase has a ‘small’ Fermi surface of conduction electrons, along with a spin liquid of local moments. This correspondence implies that certain mean-field gapl...

ar X iv : 0 71 2 . 38 38 v 3 [ gr - q c ] 3 1 M ay 2 00 8 General Transformation Formulas for Fermi - Walker Coordinates

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

This paper is concerned with the weak-moment magnetism in heavy-fermion materials and its relation to the non-Fermi liquid physics observed near the transition to the Fermi liquid. We explore the hypothesis that the primary fluctuations responsible for the non-Fermi liquid physics are those associated with the destruction of the large Fermi surface of the Fermi liquid. Magnetism is suggested to...

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 80 3 . 44 39 v 1 [ m at h . D S ] 3 1 M ar 2 00 8 PERIODIC UNIQUE BETA - EXPANSIONS : THE SHARKOVSKIĬ ORDERING

Let β ∈ (1, 2). Each x ∈ [0, 1 β−1 ] can be represented in the form