Charles Fabry and Alfred Perot coined the term etalon (a standard of weight or measure) to describe an optical cavity between two reflecting surfaces. Micron Optics has added a single segment of optical fiber within the original Fabry-Perot etalon and developed and patented a fiber Fabry-Perot (FFP) tunable filter. This all-fiber etalon contains no lenses or collimating optics and constitutes Micron Optics FFP Technology. All the powerful fundamental characteristics of the original invention is preserved, but with three critical advanced technical attributes:
These three critical innovations allow the FFP optical response to truly follow the Airy function from the top of its low-loss peak down to the very bottom of its stop band, and to be smoothly and precisely controlled over all points in between.
Why filter response is so critical
The shape of any filter response defines its performance characteristics. The high degree to which the Micron Optics FFP Technology follows the Airy Function theory means optical systems can be designed to exhibit extremely low loss, predictable cross-talk, highly accurate power measurements, high Optical Signal to Noise Ratio (OSNR), and excellent wavelength resolution.Micron Optics FFP tunable filters show distinct advantages over competitive Fabry-Perot technology, including excellent linearity and contrast characteristics as shown to the right.
Micron Optics' Fiber Fabry-Perot Technology
Swept Laser Systems Based on FFP-TF Technology
As illustrated in the figure to the right, the core of the Micron Optics' high-speed swept laser incorporates a Semiconductor Optical Amplifier (SOA,) a high-performance FFP-TF, and the associated isolators and couplers to form a uni-directional ring laser. This unique design embodies the collective advantages of the SOA's broad gain-bandwidth with direct modulation capability, and the Micron Optics FFP-TF's wide tuning ranges (i.e., free spectral range (FSR) > 200 nm), high finesse (1000 to 10,000), low loss (<2 dB), and fast scan rates reaching beyond 45 KHz to provide rapid wavelength scanning operations. As a result, the laser can sweep beyond 100 nm in micro-seconds range, output a scanning peak power in the milliwatt level, and exhibit excellent peak signal-to-spontaneous-emission ratio (SSE) >80 dB.
When configured as a seed laser followed by post amplification, the swept spectrum and power can be optimized for high-sensitivity imaging, remote sensing, and nonlinear wavelength conversion applications. Furthermore, when combined with a dispersive element, the wavelength sweep can be converted into high-speed and wide-angle spatial scanning without moving parts. Depending on applications, the laser generally needs to be optimized to meet varying combinations of requirements including the sweep range, linewidth, power, speed, and center wavelength.
Swept Laser Technology Platform Comparison
Micron Optics Technology -- Higher Imaging Performance and Commercialization Capability