Tunable Dielectric Resonators for Free-Space Light Modulation

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Solution Overview

Problem

Existing dielectric resonators struggle to modulate freespace radiation effectively due to symmetry-protected bound states in the continuum, which lack radiative coupling channels, limiting their Q-factor and light-matter interaction capabilities.

Innovation Solution

Incorporating a planar dielectric slab with a periodic grating and an electronically or thermally gated absorber material, the resonator breaks symmetry, enabling radiative coupling and modulating the qBIC resonance by adjusting the absorption properties at the qBIC resonant frequency, thereby controlling the transmission and reflection of radiation.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If symmetry-protected bound states in the continuum are used in dielectric resonators, then the Q-factor is improved (theoretically infinite), but radiative coupling channels are absent preventing effective light-matter interaction

Engineering Contradiction:
ImproveQ-factorVSAvoidlack of radiative coupling channels
Core Design Contradiction:
ReliabilityVSObject-generated harmful factors

Solution Approach 1:

The patent introduces symmetry breaking through a perturbation element (such as a nanoparticle or structural distortion) placed on or near the dielectric resonator. This asymmetry disrupts the symmetry protection of the BIC mode, opening radiative coupling channels while maintaining high Q-factor. The broken symmetry allows the resonator to interact with free-space radiation, enabling light-matter interaction while preserving the high-Q resonance characteristic.

Inventive Principle:
Principle #4Asymmetry

2Object-generated harmful factors

If oblique light illumination is used to access symmetry protected BIC, then radiative coupling channels are opened, but the Q-factor decreases due to increased scattering rate

Engineering Contradiction:
Improveradiative coupling channelsVSAvoidQ-factor
Core Design Contradiction:
Object-generated harmful factorsVSReliability

Solution Approach 1:

Instead of using oblique illumination (changing the angular dimension), the patent introduces a spatial perturbation in the transverse dimension by placing a nanoparticle or structural feature on the resonator surface. This dimensional approach to symmetry breaking opens radiative channels while maintaining normal incidence illumination, thereby preserving the high Q-factor associated with normal-incidence excitation.

Inventive Principle:
Principle #17Another dimension (Dimensionality change)

3Adaptability or versatility

If graphene is used as electro-optic material for active light modulation, then electrical modulation of optical conductivity is achieved, but the modulation depth is limited by graphene quality and absorption losses

Engineering Contradiction:
Improveelectrical modulation capabilityVSAvoidabsorption losses
Core Design Contradiction:
Adaptability or versatilityVSLoss of energy

Solution Approach 1:

The patent uses the high-Q qBIC resonance as an intermediary that enhances the interaction between light and the electro-optic material. The resonant field enhancement at the resonator surface amplifies the effect of the electro-optic material's conductivity modulation, allowing for deeper modulation with lower loss. The resonator acts as a mediator that concentrates light energy in the interaction region, making the modulation more efficient and reducing the required material quality.

Inventive Principle:
Principle #24Intermediary (Mediator)

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

This approach achieves high-Q resonances with tunable absorption, enabling nearly perfect modulation of light intensity and reflection, suitable for applications in telecommunications and other frequency bands, independent of graphene quality.

Implementation Method 1

The waveguide supports a vertical Fabry-Perot resonance

Methodology Applied
Scientific EffectFabry-Perot resonance: Fabry-Perot Interferometer

Implementation Method 2

the periodic grating supports a qBIC resonance, wherein the supported qBIC resonance has a qBIC resonant frequency corresponding to a peak in the transmission spectrum of the Fabry-Perot resonance

Methodology Applied
Scientific EffectQuasi-bound states in the continuum (qBIC): Resonance

Implementation Method 3

The electronically gated absorber has an electrically or thermally tunable absorption at the qBIC resonant frequency

Methodology Applied
Scientific EffectElectrical gating of absorption: Electro-Optic Effects

Implementation Method 4

The electronically gated absorber has an electrically or thermally tunable absorption at the qBIC resonant frequency

Methodology Applied
Scientific EffectThermal gating of absorption: Thermal Radiation

Implementation Method 5

the lateral guided mode resonance and the vertical Fabry Perot resonance couple to produce a Fano resonance having a Lorentzian line shape with a minimum transmittance and a maximum reflectance at the qBIC resonant frequency

Methodology Applied
Scientific EffectFano resonance: Interference

Data Source

PatentUS11966144B2Tunable dielectric resonators for freespace light intensity modulation
Publication Date: 2024.04.23 WISCONSIN ALUMNI RES FOUND
  • US11966144B2 patent drawing
  • US11966144B2 patent drawing
  • US11966144B2 patent drawing

AI summary

Tunable dielectric resonators for the modulation of freespace radiation and methods of using the resonators are provided. The dielectric resonators include a planar waveguide that supports a vertical Fabry-Perot resonance, a grating that supports a qBIC resonance, and a radiation absorbing material having an electronically or thermally tunable absorption at the qBIC resonant frequency. Using this resonator design, the intensity of the transmission and reflection of the qBIC resonance can be modulated by modulating the absorption properties of the absorbing material at the qBIC resonant frequency.