Hidden modes in open disordered media: analytical, numerical, and experimental results

Abstract

We explore numerically, analytically, and experimentally the relationship between quasi-normal modes (QNMs) and transmission resonance (TR) peaks in the transmission spectrum of one-dimensional (1D) and quasi-1D open disordered systems. It is shown that for weak disorder there exist two types of the eigenstates: ordinary QNMs which are associated with a TR, and hidden QNMs which do not exhibit peaks in transmission or within the sample. The distinctive feature of the hidden modes is that unlike ordinary ones, their lifetimes remain constant in a wide range of the strength of disorder. In this range, the averaged ratio of the number of transmission peaks ${N}_{{\rm{res}}}$ to the number of QNMs ${N}_{{\rm{mod}}},$ ${N}_{{\rm{res}}}/{N}_{{\rm{mod}}},$ is insensitive to the type and degree of disorder and is close to the value $\sqrt{2/5},$ which we derive analytically in the weak-scattering approximation. The physical nature of the hidden modes is illustrated in simple examples with a few scatterers. The analogy between ordinary and hidden QNMs and the segregation of superradiant states and trapped modes is discussed. When the coupling to the environment is tuned by an external edge reflectors, the superradiance transition is reproduced. Hidden modes have been also found in microwave measurements in quasi-1D open disordered samples. The microwave measurements and modal analysis of transmission in the crossover to localization in quasi-1D systems give a ratio of ${N}_{{\rm{res}}}/{N}_{{\rm{mod}}}$ close to $\sqrt{2/5}.$ In diffusive quasi-1D samples, however, ${N}_{{\rm{res}}}/{N}_{{\rm{mod}}}$ falls as the effective number of transmission eigenchannels M increases. Once ${N}_{{\rm{mod}}}$ is divided by M , however, the ratio ${N}_{{\rm{res}}}/{N}_{{\rm{mod}}}$ is close to the ratio found in 1D.

Keywords

• Anderson localization
• open disordered system
• transmission resonances
• quasi-normal modes