English

$1/f^\alpha$ noise and generalized diffusion in random Heisenberg spin systems

Disordered Systems and Neural Networks 2015-11-30 v1

Abstract

We study the `flux noise' spectrum of random-bond quantum Heisenberg spin systems using a real-space renormalization group (RSRG) procedure that accounts for both the renormalization of the system Hamiltonian and of a generic probe that measures the noise. For spin chains, we find that the dynamical structure factor Sq(f)S_q(f), at finite wave-vector qq, exhibits a power-law behavior both at high and low frequencies ff, with exponents that are connected to one another and to an anomalous dynamical exponent through relations that differ at T=0T = 0 and T=T = \infty. The low-frequency power-law behavior of the structure factor is inherited by any generic probe with a finite band-width and is of the form 1/fα1/f^\alpha with 0.5<α<10.5 < \alpha < 1. An analytical calculation of the structure factor, assuming a limiting distribution of the RG flow parameters (spin size, length, bond strength) confirms numerical findings. More generally, we demonstrate that this form of the structure factor, at high temperatures, is a manifestation of anomalous diffusion which directly follows from a generalized spin-diffusion propagator. We also argue that 1/f1/f-noise is intimately connected to many-body-localization at finite temperatures. In two dimensions, the RG procedure is less reliable; however, it becomes convergent for quasi-one-dimensional geometries where we find that one-dimensional 1/fα1/f^\alpha behavior is recovered at low frequencies; the latter configurations are likely representative of paramagnetic spin networks that produce 1/fα1/f^\alpha noise in SQUIDs.

Keywords

Cite

@article{arxiv.1506.00643,
  title  = {$1/f^\alpha$ noise and generalized diffusion in random Heisenberg spin systems},
  author = {Kartiek Agarwal and Eugene Demler and Ivar Martin},
  journal= {arXiv preprint arXiv:1506.00643},
  year   = {2015}
}

Comments

22 pages, 21 figures

R2 v1 2026-06-22T09:45:17.567Z