A nested hybridizable discontinuous Galerkin method for computing second-harmonic generation in three-dimensional metallic nanostructures
- 1. Department of Aeronautics and Astronautics, Massachusetts Institute of Technology, Cambridge, MA 02139 (United States)
- 2. Center for Biomolecular Nanotechnologies, Istituto Italiano di Tecnologia, Via Barsanti 14, 73010 Arnesano (LE) (Italy)
- 3. Department of Electrical and Computer Engineering, University of Minnesota, Minneapolis, MN 55455 (United States)
Description
Highlights: • A nested HDG method to economize the solution of traditional HDG systems. • A computational framework combining nested HDG with the structure of the problem for additional computational savings. • Model order reduction strategy to identify geometries that lead to resonances at ω, 2ω. • Ability to simulate nonlocal second harmonic generation plasmonic phenomena on realistic 3-D nanostructures. We develop a nested hybridizable discontinuous Galerkin (HDG) method to numerically solve the Maxwell's equations coupled with a hydrodynamic model for the conduction-band electrons in metals. The HDG method leverages static condensation to eliminate the degrees of freedom of the approximate solution defined in the elements, yielding a linear system in terms of the degrees of freedom of the approximate trace defined on the element boundaries. This article presents a computational method that relies on a degree-of-freedom reordering such that the HDG linear system accommodates an additional static condensation step to eliminate a large portion of the degrees of freedom of the approximate trace, thereby yielding a much smaller linear system. For the particular metallic structures considered in this article, the resulting linear system obtained by means of nested static condensations is a block tridiagonal system, which can be solved efficiently. We apply the nested HDG method to compute second harmonic generation on a triangular coaxial periodic nanogap structure. This nonlinear optics phenomenon features rapid field variations and extreme boundary-layer structures that span a wide range of length scales. Numerical results show that the ability to identify structures which exhibit resonances at ω and 2ω is essential to excite the second harmonic response.
Availability note (English)
Available from http://dx.doi.org/10.1016/j.jcp.2020.110000Additional details
Identifiers
- DOI
- 10.1016/j.jcp.2020.110000;
- PII
- S0021999120307749;
Publishing Information
- Journal Title
- Journal of Computational Physics (Print)
- Journal Volume
- 429
- Journal Page Range
- vp.
- ISSN
- 0021-9991
- CODEN
- JCTPAH
INIS
- Country of Publication
- Netherlands
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 54001869
- Subject category
- S71: CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; S77: NANOSCIENCE AND NANOTECHNOLOGY;
- Descriptors DEI
- BOUNDARY LAYERS; DEGREES OF FREEDOM; ELECTRODYNAMICS; ELECTRONS; GEOMETRY; HARMONIC GENERATION; HARMONICS; HYDRODYNAMIC MODEL; HYDRODYNAMICS; NANOSTRUCTURES; THREE-DIMENSIONAL LATTICES
- Descriptors DEC
- CRYSTAL LATTICES; CRYSTAL STRUCTURE; ELEMENTARY PARTICLES; FERMIONS; FLUID MECHANICS; FREQUENCY MIXING; LAYERS; LEPTONS; MATHEMATICAL MODELS; MATHEMATICS; MECHANICS; OSCILLATIONS; PARTICLE MODELS; STATISTICAL MODELS; THERMODYNAMIC MODEL
Optional Information
- Copyright
- Copyright (c) 2020 Elsevier Inc. All rights reserved.