Plasmonic Illumination Device Anisotropic Light Directionality
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Solution Overview
Problem
Current light emitting diode (LED) illumination devices suffer from absorption and emission losses due to the isotropic emission of wavelength converting materials and the inefficiency of photonic band gap materials in controlling emission direction, leading to reduced light output and directional issues.
Innovation Solution
A plasmonic illumination device with a periodic plasmonic antenna array and a wavelength converting layer positioned for maximum field enhancement, utilizing localized surface plasmon resonances and photonic modes to achieve anisotropic light emission and reduce losses by optimizing the spatial distribution of wavelength converting materials in relation to the antenna array.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Illumination intensity
If wavelength converting material is applied directly on the LED and made scattering, then color uniformity over angle is improved, but absorption losses in the LED increase due to blue light being scattered back
Solution Approach 1:
A scattering layer is introduced as an intermediary component between the LED and the wavelength converting material. This scattering layer is positioned at a specific distance from the LED surface, allowing it to scatter the converted light uniformly in all directions while preventing direct contact between the scattering material and the LED, thereby avoiding backscattering of blue light into the LED and reducing absorption losses.
Solution Approach 2:
The solution transitions from a two-dimensional planar arrangement (LED chip with phosphor directly on top) to a three-dimensional structure by introducing a scattering layer at a specific height above the LED. This vertical dimensionality allows the scattering function to be separated from the conversion function, enabling independent optimization of both color uniformity and efficiency.
2Device complexity
If isotropic phosphor emission is used, then simplicity of structure is maintained, but light output efficiency decreases as only a portion of light escapes through the output surface
Solution Approach 1:
A reflective layer is introduced as an intermediary between the LED and the wavelength converting material. This reflective layer redirects the downward-directed light that would otherwise be lost, bouncing it upward through the wavelength converting material. This allows the system to maintain simple isotropic phosphor emission while improving light extraction efficiency by recovering previously lost downward-directed photons.
3Illumination intensity
If photonic band gap material is used to control emission direction, then light directionality is improved, but manufacturing complexity increases due to high refractive index contrast requirements, high aspect ratio holes or pillars, strict size control, and luminescent material requirements
Solution Approach 1:
The patent replaces complex photonic band gap structures with a simple scattering layer made from conventional, inexpensive materials. Instead of requiring precise nanoscale fabrication of high aspect ratio holes or pillars in luminescent materials, the solution uses a relatively thick scattering layer that can be manufactured using standard, cost-effective techniques. This achieves comparable or superior directionality control without the manufacturing complexity.
Solution Approach 2:
The solution changes the key parameter from nanoscale structural geometry (high aspect ratio holes, precise lattice constants) to macroscopic material properties (scattering coefficient, layer thickness). This parameter transformation allows achieving similar optical effects using conventional materials and manufacturing processes rather than requiring precise nanoscale structuring.
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
The solution enhances light directionality and coupling efficiency, increasing the amount of light emitted towards a specific direction while minimizing absorption losses, resulting in improved overall efficiency and reduced losses in the illumination device.
Implementation Method 1
support a first lattice resonance at the predetermined wavelength, arising from coupling of localized surface plasmon resonances in the individual antenna elements to photonic modes
Implementation Method 2
coupling of localized surface plasmon resonances in the individual antenna elements to photonic modes supported by the system comprising the plasmonic antenna array and the photon emitting layer
Implementation Method 3
a photon emitting material configured to receive energy from an energy source and to emit light having a predetermined wavelength; said photon emitting material is a wavelength converting material configured to receive light of a first wavelength and to convert said received light from said first wavelength to a second wavelength
Data Source
AI summary
There is provided an illumination device (100) comprising: a substrate (104); an optically transmissive first layer (106) arranged on the substrate; a photon emitting layer (108), arranged on the optically transmissive first layer and comprising a photon emitting material configured to receive energy from an energy source and to emit light having a predetermined wavelength; a periodic plasmonic antenna array, arranged on the substrate and embedded within the first layer, and comprising a plurality of individual antenna elements (114) arranged in an antenna array plane, the plasmonic antenna array being configured to support a first lattice resonance at the predetermined wavelength, arising from coupling of localized surface plasmon resonances in the individual antenna elements to photonic modes supported by the system comprising the plasmonic antenna array and the photon emitting layer, wherein the plasmonic antenna array is configured to comprise plasmon resonance modes such that light emitted from the plasmonic antenna array has an anisotropic angle distribution; and wherein the photon emitting layer is arranged at a distance from the antenna array plane corresponding to a location of maximum field enhancement for light out-coupling resulting from the plasmonic-photonic lattice resonances.