Tapered Optical Fiber Supercontinuum Generation
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Solution Overview
Problem
Existing optical measurement systems for lithography face challenges in obtaining bright, spatially coherent radiation with a broad spectral width and short coherence length, which is essential for precise alignment and measurement, but current solutions are complex and unreliable.
Innovation Solution
A tapered optical fiber is used to spectrally broaden radiation, generating output with a spectral width between 500 nm and 900 nm, providing a compact, reliable, and bright radiation source for optical measurement systems.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Illumination intensity
If conventional radiation sources (lasers, LEDs) are used, then spatial coherence and brightness can be achieved, but spectral width remains narrow and coherence length is too long
Solution Approach 1:
A tapered optical fiber is introduced as an intermediary component between the laser source and the measurement system. The fiber's tapered geometry creates nonlinear optical effects that broaden the spectral width while maintaining spatial coherence, eliminating the need for complex multi-component radiation sources
Solution Approach 2:
The optical parameters of the radiation are transformed by passing through the tapered fiber region. The intense laser field interacting with the tapered fiber structure generates supercontinuum radiation, changing the spectral width parameter from narrow to broad (500-900 nm) while maintaining other desirable properties
2Object-affected harmful factors
If spectral width is broadened to reduce coherence length, then coherence interference effects are reduced, but system complexity and reliability deteriorate
Solution Approach 1:
The potentially harmful coherence interference effects are converted into a beneficial measurement mechanism. The known coherence properties of laser radiation are preserved and utilized for precise alignment measurements, while the tapered fiber provides sufficient spectral broadening to reduce unwanted interference without compromising reliability
3Adaptability or versatility
If multiple radiation sources with different wavelengths are combined, then broad spectral coverage is achieved, but device complexity increases
Solution Approach 1:
The broad spectrum is generated by segmenting a single laser wavelength through nonlinear optical processes in the tapered fiber. Instead of combining multiple independent radiation sources, the system segments the spectral content from one coherent source, achieving 500-900 nm coverage with a single laser and tapered fiber combination
Solution Approach 2:
The tapered optical fiber serves multiple functions simultaneously: it acts as a waveguide, a nonlinear optical medium for spectral broadening, and a spatial coherence maintainer. This multi-functionality eliminates the need for multiple specialized components to achieve broad spectral coverage
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 enables the production of a bright, spectrally broadened radiation with a short coherence length, improving the reliability and simplicity of optical measurement systems while reducing coherence interference effects, thus enhancing alignment and measurement precision.
Implementation Method 1
Broad spectrum radiation by supercontinuum generation using a tapered optical fiber
Implementation Method 2
radiation from a laser with a nominal wavelength in the visible or near-infrared region is coupled to a tapered optical fiber and spectrally broadened in a nonlinear optical process
Data Source
AI summary
A measurement apparatus, including: a tapered optical fiber, the tapered optical fiber having an input to receive radiation and having an output to provide spectrally broadened output radiation toward a measurement target, the tapered optical fiber configured to spectrally broaden the radiation received at the input; and a detector system configured to receive a redirected portion of the output radiation from the measurement target.


