The Localization Transition in the Ultrametric Ensemble\addtokomafont
author \minisecAbstract We study the hierarchical analogue of power-law random band matrices, a symmetric ensemble of random matrices with independent entries whose variances decay exponentially in the metric induced by the tree topology on . We map out the entirety of the localization regime by proving the localization of eigenfunctions and Poisson statistics of the suitably scaled eigenvalues. Our results complement existing works on complete delocalization and random matrix universality, thereby proving the existence of a phase transition in this model.
One-dimensional lattice Hamiltonians with random long-range hopping provide a useful and simplified testing ground for the Anderson metal-insulator transition in more complicated systems. Two prominent examples of such models are the random band matrices [4, 13], whose entries are zero outside some band , and the power-law random band matrices (PRBM) [12, 19], whose entries have variances decaying according to some power of the Euclidean distance . Even for these models, the mathematically rigorous understanding is far from complete, although there has been some progress; see [22, 9, 2, 6, 10, 21] and references therein. This article is concerned with a further simplification, the ultrametric ensemble of Fyodorov, Ossipov and Rodriguez , which is essentially obtained by replacing the Euclidean distance in the definition of the PRBM with the metric induced by the tree topology.
The index space of the ultrametric ensemble is endowed with the metric
where is the nested sequence of partitions defined by
The basic building blocks of the ultrametric ensemble are the matrices whose entries are independent (up to the symmetry constraint) centered real Gaussian random variables with variance
Thus is a direct sum of random matrices drawn independently from the Gaussian Orthogonal Ensemble (GOE) of size . The ultrametric ensemble with parameter refers to the random matrix
where and are independent for . We choose the normalizing constant such that
which means that grows exponentially in in case and is asymptotically constant in case . The original definition in  contains an additional parameter governing the relative strengths of the diagonal and off-diagonal disorder, but this parameter does not significantly alter our analysis and so we omit it altogether. Moreover, the authors of  constructed the block matrices from the Gaussian Unitary Ensemble (GUE), and our results apply to both GOE and GUE blocks with only slight changes.
The ultrametric ensemble is a hierarchical analogue of the PRBM in a sense which was first introduced to statistical mechanical models by Dyson , and studied rigorously in the context of quantum hopping systems with only diagonal disorder in [3, 15, 16, 17, 20, 24]. Thus, one expects the core features of the PRBM phase transition to be present in the ultrametric ensemble as well. Indeed, the authors of  present arguments at a theoretical physics level of rigor as well as numerical evidence for a localization-delocalization transition in the eigenfunctions of as the parameter changes from to . The effect of the Gaussian perturbations on the spectrum of can be described dynamically by Dyson Brownian motion  and, in this sense, the critical point is natural because it governs whether the evolution passes the local equilibration time of this system or not.
In this article we establish the localized phase by proving that the eigenfunctions remain localized and the level statistics converge to a Poisson point process if . Both statements are improvements over the rigorous results for band matrices, where the only localization result is due to Schenker  and no proof of Poisson statistics is known. For the first main result in this paper, we recall that, by the Wegner estimate , the infinite-volume density of states measure defined through
has a bounded Radon-Nikodym derivative, the density of states, whose values we denote by .
Theorem 1.1 (Poisson statistics).
Suppose and let be a Lebesgue point of . Then, the random measure
converges in distribution to a Poisson point process with intensity as .
The second main result of this paper says that if an eigenfunction of in some mesoscopic energy interval has any mass at some , then actually all but an exponentially small amount of the total mass is carried in an exponentially vanishing fraction of the volume near with high probability. We formulate this result in terms of the eigenfunction correlator
which in completely delocalized regimes is typically given by
Thus, since grows very large for mesoscopic spectral windows, it is a signature of localization if the eigenfunction correlator asymmptotically vanishes for small enough mesoscopic intervals , as is proved in the following theorem.
Theorem 1.2 (Eigenfunction localization).
Suppose and let . Then, there exist , , and a sequence with such that for every the -normalized eigenfunctions satisfy
Our results gain additional interest upon noting that, when , the ultrametric ensemble has an essential mean field character and techniques originally developed for Wigner matrices show that the energy levels agree asymptotically with those of the GOE and that the eigenfunctions are completely delocalized. We will now roughly sketch how to apply these results in the present situation and state the corresponding theorems. The key observation is that the normalizing factor , which scales the spectrum to , is given by
so that the spread
grows like a positive power of the system size when . The results of  then show that the semicircle law (i.e. ) is valid on scales of order even for the matrices
with a small part of the final Gaussian component removed. We set with . The validity of the local semicircle law already implies the complete delocalization of the eigenfunctions in mesoscopic windows in the bulk of the spectrum (see [9, Thm. 2.21]).
For any compact interval there exist such that for all the -normalized eigenfunctions of in satisfy
with probability .
Random matrix universality of the local statistics may be expressed by saying that the -point correlation functions
the -th marginals of the symmetrized eigenvalue density , locally agree with the corresponding objects for the GOE asymptotically. For this, we employ the work of Landon, Sosoe and Yau [18, Thm. 2.2] concerning the universality of Gaussian perturbations for
For the statement of the theorem, let
where is the -point correlation function of the GOE and is the density of the semicircle law.
Summing up, these results rigorously prove the existence of a metal-insulator transition in the ensemble of ultrametric random matrices. In particular, our results allow an approach all the way to the critical point from the localized side , which greatly improves upon the best known corresponding result for random band matrices . However, the above arguments do not cover the regime , in which the local eigenvalue statistics are still expected to be of Wigner-Dyson-Mehta type as in the case .
2 Proof of Poisson Statistics
When , the limit exists. Thus, we may drop the normalizing constant from the definition of in the remainder of this paper without any loss of generality. The goal of this section is to prove Theorem 1.1 by approximating with the truncated Hamiltonian
which has the property that, for any ,
where each is an independent copy of . Therefore
consists of independent components, a fact whose relevance to Theorem 1.1 is contained in the following characterization of Poisson point processes.
Let be a collection of point processes such that:
The point processes are independent for all .
If is a bounded Borel set, then
There exists some such that if is a bounded Borel set with , then
Then, converges in distribution to a Poisson point process with intensity .
We recall  that a sequence of point processes converges in distribution to whenever
for all , where is the rescaled Poisson kernel
for all .
The difference is a Gaussian perturbation with time parameter . Therefore, Theorem 1.1 of  shows that there exists such that for all we have
in an iterative fashion.
There exist and such that
for all .
There exists a sequence with and such that
for all .
Since , there exists a sequence with , and . By applying Theorem 2.2 with , we obtain
with independent . If is a bounded Borel set, the theorem of Combes-Germinet-Klein  asserts that and hence for any :
Since , the first hypothesis of Proposition 2.1 follows. Writing
when . In particular, and the last hypothesis of Proposition 2.1 is satisfied. It remains to prove the remaining hypothesis of Proposition 2.1, which is the second important consequence of Theorem 2.2 and is contained in the following theorem.
Let be a bounded Borel set. Then,
This shows that the measures satisfy
and Corollary 2.3 implies that also
For any bounded Borel set , the indicator is in the -closure of the finite linear combinations from the set and the measures are absolutely continuous with uniformly bounded densities by the Wegner estimate. Together, these two observations yield that (2.9) is valid for any bounded Borel set . Moreover, since is a Lebesgue point of ,
and hence we have shown that
Since takes values in the non-negative integers
3 Proof of Eigenfunction Localization
In this section, we prove Theorem 1.2 by comparing the eigenfunctions of with the obviously localized eigenfunctions of . As in Section 2, we drop the normalizing constant from the definition of . The core of this argument again consists of resolvent bounds for Gaussian perturbations, and thus we consider the Green functions
If for some , Theorem 1.2 of  proves that there exists such that
with whenever . Iterating this result, we see that
Since , we can choose , , and such that
Thus, setting and
and using that if show that
Applying Markov’s inequality, we arrive at
with probability .
We thank Y. V. Fyodorov for introducing us to the ultrametric ensemble. This work was supported by the DFG (WA 1699/2-1).
Per von Soosten Zentrum Mathematik, TU München Boltzmannstraße 3, 85747 Garching, Germany
firstname.lastname@example.orgSimone Warzel Zentrum Mathematik, TU München Boltzmannstraße 3, 85747 Garching, Germany
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