Quasinormal mode representation of radiating resonators in open phononic systems
arXiv:2211.12823 · doi:10.1103/PhysRevB.107.144301
Abstract
Open phononic systems including resonators radiating inside an unbounded medium support localized phonons characterized by a complex frequency. In this context, the concept of elastic quasinormal mode (QNM) arises naturally, as in the cases of nanophotonic and plasmonic open systems. Based on a complex, unconjugated form of reciprocity theorem for elastodynamics, the eigenfunction expansion theorem expressed on the elastic QNM basis yields an accurate approximation to the response function, for an arbitrary excitation. The description of the elastic Purcell effect then requires defining a complex-valued modal volume for each QNM. For validation, we first consider the case a vibrating nylon rod radiating in water. As a second test example, we consider a slender nickel ridge on the surface of a fused silica substrate, before extending our attention to a nanoscale tuning fork composed of two such ridges. In all cases, the response estimated from only a few elastic QNMs agrees with the solution to the elastodynamic equation.
References in corpus (6)
- Resonant state expansion applied to three-dimensional open optical systems
- Shape deformation of nanoresonator: a quasinormal-mode perturbation theory
- Nonlocal quasinormal modes for arbitrarily shaped three-dimensional plasmonic resonators
- Quasi-normal mode theory of the scattering matrix, enforcing fundamental constraints for truncated expansions
- Multiple Extremal Eigenpairs by the Power Method
- Quasinormal mode theory of elastic Purcell factors and Fano resonances of optomechanical beams