
Fabry-Perot (FP) laser diode is a type of laser diode that utilizes a Fabry-Perot (FP) resonant cavity to control the modes of operation and achieve wavelength stability. Fabry-Perot (FP) lasers are a foundational element in the domain of optical coherent tomography (OCT). These lasers are distinguished by their relatively simple yet highly effective architecture, making them a versatile choice for various optical applications in both research and industry. Explore the world of Fabry-Perot (FP) lasers, their working principles, and their applications in telecommunications and astronomy. Discover the advancements in Fabry-Perot (FP) laser technology with InPhenix.
InPhenix designs and manufactures cutting-edge Fabry-Perot Laser and light sources, critical for state-of-the-art applications in medical, telecom, sensing, and measurement industries. Our FP Laser technology is a foundational element in the domain of optical coherent tomography (OCT), offering reliable, stable, and cost-effective solutions for diverse optical needs.
Window (nm)
To: From: | Peak
To: Wavelength (nm) | Threshold Current (mA) | Output Power (mW) | Operation Current (mA) | Spectrum Width (rms)(nm) | Package Type | Part Number |
|---|---|---|---|---|---|---|---|
| Window (nm) | Peak Wavelength(nm) | Threshold Current(mA) | Output Power(mW) | Operation Current(mA) | Spectrum Width (rms)(nm) | Package Type | Part Number |
| 785 | 785 to 795 | 400 | 600 | 1000 | 5 | TO 8, 9Ex-Window | IPFPT0701 |
| 1310 | 1290 to 1350 | 20 | 180 | 1000 | 5 | BUT or DIL | IPFPD1302 |
| 1490 | 1450 to 1500 | 20 | 180 | 1000 | 5 | BUT or DIL | IPFPD1402 |
| 1550 | 1520 to 1580 | 20 | 180 | 1000 | 5 | BUT or DIL | IPFPD1502 |
| 1625 | 1610 to 1650 | 20 | 180 | 1000 | 7 | BUT or DIL | IPFPD1602 |
Window (nm)
To: From: | Peak
To: Wavelength (nm) | Threshold Current (mA) | Output Power (mW) | Operation Current (mA) | Slope Efficiency (mW/mA) | Spectrum Width (rms)(nm) | Package Type | Part Number |
|---|---|---|---|---|---|---|---|---|
| Window (nm) | Peak Wavelength(nm) | Threshold Current(mA) | Output Power(mW) | Operation Current(mA) | Slope Efficiency (mW/mA) | Spectrum Width (rms)(nm) | Package Type | Part Number |
| 785 | 785 to 792 | <400 | <200 | 1000 | 0.4 | 5 | BUT or DIL | IPFPD0701 |
| 785 | 785 to 792 | <400 | <400 | 1000 | 0.8 | 5 | TO 8, 9Ex-Window | IPFPT0701 |
| 1310 | 1300 to 1320 | <15 | <100 | <1000 | 0.4 | 5 | BUT or DIL | IPFPD1302 |
| 1310 | 1300 to 1320 | <15 | <100 | <1000 | 0.4 | 5 | TO 8, 9 or 56 Ex-Window | IPFPT1302 |
| 1490 | 1480 to 1500 | <15 | <100 | <1000 | 0.4 | 5 | BUT or DIL | IPFPD1402 |
| 1490 | 1480 to 1500 | <15 | <100 | <1000 | 0.4 | 5 | TO 8, 9 or 56 Ex-Window | IPFPT1402 |
| 1550 | 1540 to 1570 | <15 | <100 | <1000 | 0.4 | 5 | BUT or DIL | IPFPD1502 |
| 1550 | 1540 to 1570 | <15 | <100 | <1000 | 0.4 | 5 | TO 8, 9 or 56 Ex-Window | IPFPT1502 |
| 1625 | 1620 to 1640 | <15 | <100 | <1000 | 0.4 | 7 | BUT or DIL | IPFPD1602 |
| 1625 | 1620 to 1640 | <15 | <100 | <1000 | 0.4 | 7 | TO 8, 9 or 56 Ex-Window | IPFPT1602 |
Understanding the Fabry-Perot Laser: Structure and Operation
The Fabry-Perot Laser operates on the principle of confining a gain medium within a resonant cavity. This cavity, formed by two parallel, partially reflective mirrors, is the heart of the FP Laser. It enables the selective amplification of light through stimulated emission, ensuring coherent light output at discrete, stable wavelengths.
Key components of an InPhenix Fabry-Perot Laser include:
Gain Medium: The material responsible for light amplification. InPhenix utilizes advanced semiconductor materials, doped fibers, and solid-state crystals, tailored to dictate the wavelength range and efficiency of each FP Laser.
Mirrors: Highly reflective elements that define the resonant cavity. Their precise reflectivity and positioning are crucial for determining the Fabry-Perot Laser‘s output power and spectral characteristics.
Pump Source: Supplies the energy to initiate the lasing process. Our FP Laser designs incorporate efficient pump sources, from electrical currents to optical pumping, ensuring optimal performance.
Fabry-Perot Laser in Optical Coherence Tomography (OCT)
The Fabry-Perot Laser is integral to OCT systems, renowned for its narrow linewidth and stable output. These characteristics are essential for achieving the high spatial resolution required for detailed imaging and precise measurements in OCT.
Advantages of the Fabry-Perot Laser in OCT:
Narrow Linewidth: This characteristic is vital for high spatial resolution, enabling the differentiation of fine structures within a sample, a key advantage of the FP Laser.
Stable Output: Crucial for reliable imaging and measurement, particularly in long-term or repetitive scanning scenarios, ensuring consistent performance from our Fabry-Perot Laser.
Cost-Effectiveness: The inherent simplicity of the FP Laser design, compared to other laser types, makes it an economical choice for high-performance OCT systems.
Recent Advances in Fabry-Perot Laser Technology
InPhenix is at the forefront of Fabry-Perot Laser innovation, continuously enhancing performance and broadening application scope. These advancements leverage the essential FP Laser structure for stable light amplification, benefiting various fields.
Innovations include:
Enhanced Reflective Coatings: High-reflectivity dielectric coatings significantly improve the efficiency of our Fabry-Perot Laser products by reducing intracavity losses, leading to higher output power.
Advanced Gain Media: Research into new semiconductor materials and doped fibers has yielded gain media with broader wavelength ranges and greater tunability, enhancing the versatility of the FP Laser for diverse OCT applications.
Integration with Photonic Circuits: The integration of the Fabry-Perot Laser into photonic integrated circuits (PICs) represents a significant advancement. This makes systems more compact and efficient, especially for portable OCT devices.
Technical Improvements and Customization for your Fabry-Perot Laser Needs
The evolution of InPhenix Fabry-Perot Laser technology focuses on customization to meet specific application requirements. Adjustments in cavity length, mirror reflectivity, and gain medium composition allow for precise control over the FP Laser‘s output characteristics. This adaptability makes our Fabry-Perot Laser an indispensable tool in modern optics.
InPhenix Fabry-Perot Laser devices are increasingly integrated into complex systems, such as PICs, expanding their role in advanced optical systems. This integration reduces size and cost while enhancing overall system performance.
Furthermore, our commitment to improving the thermal and mechanical stability of the Fabry-Perot Laser has resulted in devices that maintain consistent performance under varying environmental conditions. This robustness is crucial for reliable operation in harsh or uncontrolled environments, ensuring your FP Laser always performs.
Explore the Power of Precision
with InPhenix Fabry-Perot Lasers
Ready to elevate your optical applications? Discover how InPhenix Fabry-Perot Laser technology can provide the stable, high-resolution light source you need.