Specific heat of the quantum Bragg Glass
arXiv:cond-mat/0212300 · doi:10.1209/epl/i2003-10232-x
Abstract
We study the thermodynamics of the vibrational modes of a lattice pinned by impurity disorder in the absence of topological defects (Bragg glass phase). Using a replica variational method we compute the specific heat in the quantum regime and find at low temperatures in dimension three and two. The prefactor is controlled by the pinning length. The non trivial cancellation of the linear term in arises from the so-called marginality condition and has important consequences for other mean field models.
arXiv comment5 pages, RevTex, strongly revised version
References in corpus (12)
- Elastic theory of flux lattices in presence of weak disorder
- Harmonic Vibrational Excitations in Disordered Solids and the "Boson Peak"
- Vortex-glass phases in type-II superconductors
- Quantum Fluctuations of a Nearly Critical Heisenberg Spin Glass
- Variational theory of elastic manifolds with correlated disorder and localization of interacting quantum particles
- Low Energy Quasiparticle Excitation in the Vortex State of Borocarbide Superconductor YNi_2B_2C
- The Quantum Spherical p-Spin-Glass Model
- Pinned Wigner Crystals
- Vibrational spectrum of topologically disordered systems
- A Discotic Disguised as a Smectic: A Hybrid Columnar Bragg Glass
- Statics and Dynamics of Disordered Elastic Systems
- Specific heat of classical disordered elastic systems
Cited by in corpus (5)
- Impact of jamming criticality on low-temperature anomalies in structural glasses
- Low-temperature properties of some disordered systems from the statistical properties of nearly degenerate two-level excitations
- Energy relaxation in disordered charge and spin density waves
- Two-level systems and harmonic excitations in a mean-field anharmonic quantum glass
- Specific Heat of Quantum Elastic Systems Pinned by Disorder