pith. sign in

Towards strange metallic holography

1 Pith paper cite this work. Polarity classification is still indexing.

1 Pith paper citing it
abstract

We initiate a holographic model building approach to `strange metallic' phenomenology. Our model couples a neutral Lifshitz-invariant quantum critical theory, dual to a bulk gravitational background, to a finite density of gapped probe charge carriers, dually described by D-branes. In the physical regime of temperature much lower than the charge density and gap, we exhibit anomalous scalings of the temperature and frequency dependent conductivity. Choosing the dynamical critical exponent $z$ appropriately we can match the non-Fermi liquid scalings, such as linear resistivity, observed in strange metal regimes. As part of our investigation we outline three distinct string theory realizations of Lifshitz geometries: from F theory, from polarised branes, and from a gravitating charged Fermi gas. We also identify general features of renormalisation group flow in Lifshitz theories, such as the appearance of relevant charge-charge interactions when $z \geq 2$. We outline a program to extend this model building approach to other anomalous observables of interest such as the Hall conductivity.

fields

hep-th 1

years

2026 1

verdicts

UNVERDICTED 1

representative citing papers

Poles-zeros duality in semi-holographic Mott insulators

hep-th · 2026-05-19 · unverdicted · novelty 5.0

A semi-holographic model couples a fermion to a holographic composite sector, yielding poles-zeros duality in the Green's function that distinguishes metallic and Mott-insulating phases through choice of quantization.

citing papers explorer

Showing 1 of 1 citing paper.

  • Poles-zeros duality in semi-holographic Mott insulators hep-th · 2026-05-19 · unverdicted · none · ref 55 · internal anchor

    A semi-holographic model couples a fermion to a holographic composite sector, yielding poles-zeros duality in the Green's function that distinguishes metallic and Mott-insulating phases through choice of quantization.