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Scientific Reports

Investigation of the diagonal elements of the Wigner’s reaction matrix for networks with violated time reversal invariance

Michał Ławniczak, Leszek Sirko

Published Apr 4, 2019• 50 citations
Publisher

Abstract

The distributions of the diagonal elements of the Wigner's reaction [Formula: see text] matrix for open systems with violated time reversal T invariance in the case of large absorption are for the first time experimentally studied. The Wigner's reaction matrix links the properties of chaotic systems with the scattering processes in the asymptotic region. Microwave networks consisting of microwave circulators were used in the experiment to simulate quantum graphs with violated T invariance. The distributions of the diagonal elements of the reaction [Formula: see text] matrix were experimentally evaluated by measuring of the two-port scattering matrix [Formula: see text]. The violation of T invariance in the networks with large absorption was demonstrated by calculating the enhancement factor W of the matrix [Formula: see text]. Our experimental results are in very good agreement with the analytic ones attained for the Gaussian unitary ensemble in the random matrix theory. The obtained results suggest that the distributions P(ʋ) and P(u) of the imaginary and the real parts of the diagonal elements of the Wigner's reaction [Formula: see text] matrix together with the enhancement factor W can be used as a powerful tool for identification of systems with violated T symmetry and quantification of their absorption.

DOI
10.1038/s41598-019-42123-y

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The distributions of the diagonal elements of the Wigner's reaction [Formula: see text] matrix for open systems with violated time reversal T invariance in the case of large absorption are for the first time experimentally studied. The Wigner's reaction matrix links the properties of chaotic systems with the scattering processes in the asymptotic region. Microwave networks consisting of microwave circulators were used in the experiment to simulate quantum graphs with violated T invariance. The distributions of the diagonal elements of the reaction [Formula: see text] matrix were experimentally evaluated by measuring of the two-port scattering matrix [Formula: see text]. The violation of T invariance in the networks with large absorption was demonstrated by calculating the enhancement factor W of the matrix [Formula: see text]. Our experimental results are in very good agreement with the analytic ones attained for the Gaussian unitary ensemble in the random matrix theory. The obtained results suggest that the distributions P(ʋ) and P(u) of the imaginary and the real parts of the diagonal elements of the Wigner's reaction [Formula: see text] matrix together with the enhancement factor W can be used as a powerful tool for identification of systems with violated T symmetry and quantification of their absorption.
The present doctoral thesis describes experimentally measured properties of the resonance spectra of flat microwave billiards with partially broken timereversal invariance induced by an embedded magnetized ferrite. A vector network analyzer determines the complex scattering matrix elements. The data is interpreted in terms of the scattering formalism developed in nuclear physics. At low excitation frequencies the scattering matrix displays isolated resonances. At these the effect of the ferrite on isolated resonances (singlets) and pairs of nearly degenerate resonances (doublets) is investigated. The hallmark of time-reversal symmetry breaking is the violation of reciprocity, i.e. of the symmetry of the scattering matrix. One finds that reciprocity holds in singlets; it is violated in doublets. This is modeled by an effective Hamiltonian of the resonator. A comparison of the model to the data yields time-reversal symmetry breaking matrix elements in the order of the level spacing. Their dependence on the magnetization of the ferrite is understood in terms of its magnetic properties. At higher excitation frequencies the resonances overlap and the scattering matrix elements fluctuate irregularly (Ericson fluctuations). They are analyzed in terms of correlation functions. The data are compared to three models based on random matrix theory. The model by Verbaarschot, Weidenmüller and Zirnbauer describes time-reversal invariant scattering processes. The one by Fyodorov, Savin and Sommers achieves the same for systems with complete time-reversal symmetry breaking. An extended model has been developed that accounts for partial breaking of time-reversal invariance. This extended model is in general agreement with the data, while the applicability of the other two models is limited. The cross-correlation function between forward and backward reactions determines the time-reversal symmetry breaking matrix elements of the Hamiltonian to up to 0.3 mean level spacings. Finally the sensitivity of the elastic enhancement factor to time-reversal symmetry breaking is studied. Based on the data elastic enhancement factors below 2 are found which is consistent with breaking of time-reversal invariance in the regime of overlapping resonances. The present work provides the framework to probe for broken time-reversal invariance in any scattering data by a multitude of methods in the whole range between isolated and overlapping resonances.
The influence of direct processes on the cross-correlation function c 12 (ν) and the elastic enhancement factor W S , β was studied experimentally using microwave networks in the presence of absorption. Microwave networks simulate quantum graphs with and without time-reversal symmetry. Direct processes exist because, for example, of non-perfect coupling between a studied system and a measuring device. We show that direct processes strongly influence the cross-correlation function c 12 (ν) in contrast to the enhancement factor W S , β , which is not sensitive to these processes. It makes the enhancement factor W S , β an important measure of the chaoticity of a quantum system.
In this work several aspects of quantum chaos are studied in the time domain. The wave equation for flat microwave cavities is equivalent to the Schrödinger equation in quantum mechanics. Therefore microwave measurements provide an experimental approach to quantum chaos. The experiments are described in terms of scattering theory, to take the coupling of the antennas to the system as well as the dissipation in the cavity walls into account. In the first part the scattering matrix of several microwave cavities is analyzed in the regime of overlapping resonances. The difference between regular and chaotic systems can be observed both in the autocorrelation functions of the same S-matrix elements, and in the cross-correlation functions of different S-matrix elements. In accordance with literature, this difference is more pronounced in the cross-correlation functions. To describe the experimental correlation functions, the absorption in the cavity walls is modeled by an infinite number of weak decay channels. In the second part the focus is shifted to the stability of quantum time-evolution. The fidelity amplitude is a standard benchmark for the stability of a quantum system against a change of the Hamiltonian. It is defined as the overlap of the perturbed and unperturbed time-evolution of the same initial state. Exact theoretical results for a random matrix model are compared with numerical simulations and the linear-response results. For strong perturbations a partial recovery of the fidelity amplitude is found, and an intuitive explanation for this behavior is given in terms of a spectral Debye-Waller factor. Further, in the third part, experimental results for the fidelity amplitude are presented for two microwave cavities with classically chaotic dynamics. The perturbation of the systems is realized by applying small changes to their geometry. The results are well described by the linear-response expression, and the perturbation strength can be related to the change of the geometry of the cavities. In the fourth part microwave measurements on dielectric quadrupole billiards with mixed phase space are discussed. The internal dynamics is analyzed by means of Husimi distributions, while for the outer region the Poynting vector is determined to obtain the emission pattern. The emission pattern of the quadrupole billiard is strongly influenced by the structures of its mixed phase space.
Am agnetic flux through a mesoscopic metallic ring gives rise to a persistent current which can be detected via characteristic oscillations of the magnetization depending on the applied field (Let al 1990 Phys. Rev. Lett. 64 2074). In this paper a direct visualization of such persistent currents in am icrowave analogue experiment is reported, making use of the analogy between the probability density current in the quantum-mechanical system and the Poynting vector in the corresponding electromagnetic one. To break time-reversal symmetry, a small ring of a ferrite material in a static external magnetic field was introduced into the resonator. In our analysis of the experimental data we employ the off-diagonal elements of the scattering matrix. Due to the small size of the ferrite compared to the resonator size the symmetry was partially broken in the sense that the real and the imaginary parts of the wavefunctions are not equally large on average. The statistical properties of the wavefunction's real and imaginary parts Re(ψ) ,I m(ψ) ,r espectively, as well as the distributions of the total wavefunction's amplitudes |ψ| and the statistical properties of the probability density currents were also examined and compared to the theoretical predictions.
We show the emergence of random matrix theory (RMT) spectral correlations in the chaotic phase of generic, periodically kicked, interacting, quantum many-body systems by analytically calculating the spectral form factor (SFF), K ( t ) , up to two leading orders in time, t . We explicitly consider the presence or absence of time-reversal ( T ) symmetry to investigate all three Dyson symmetry classes, namely, the circular orthogonal ensemble (COE) for T -invariant systems with T 2 = 1 , the circular unitary ensemble (CUE) in the absence of T symmetry, and the circular symplectic ensemble (CSE) for T -invariant systems with T 2 = − 1 . Our derivation applies the random phase approximation to perform ensemble averages, and we give its justification for generic many-body interactions. We express the SFF as a sum of contributions of certain diagrams. While the number of diagrams that contribute to the SFF in the first and second orders in t for the COE and CUE classes is finite, the number of such diagrams is exponentially large in t for the CSE class. Thus, we have developed a new diagrammatic technique that uses reduced diagrams to incorporate contributions from many diagrams. For the COE class, we show that beyond Thouless time t * , the SFF takes the form K ( t ) ≃ 2 t − 2 t 2 / N up to second order in time, where N is the Hilbert space dimension. For the CUE class, we show that K ( t ) ≃ t beyond t * , and there is no universal term in the second order, unlike the COE case. For the CSE class, we show that K ( t ) ≃ 2 t + 2 t 2 / N up to two orders in time beyond t * . The above findings of the SFF up to second order in time are in agreement with the RMT predictions for these classes. In all three cases, the scaling of t * with system size L is determined by the eigenvalues of a doubly stochastic matrix M . For strongly interacting fermionic chains, M is S U ( 2 ) invariant in all three cases, leading to t * ∝ L 2 in the presence of U ( 1 ) symmetry. In the absence of U ( 1 ) symmetry, we find t *