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Semiconductor Laser

  • Output Wavelength: 405nm,450nm,488nm,520nm,638nm
  • Power: 5~100mW
  • Noise (20‒2MHz): <0.25%(RMS Noise);<1.00%(P-P Noise)
  • Power Stability: <2.00%

Technical Parameters

BIOFOCUS
Technical Specifications Minimum Typical Maximum
Output Wavelength 405nm,450nm,488nm,
520nm,638nm
Power 5~100mW
Noise (20‒2MHz) <0.25%(RMS Noise);
<1.00%(P-P Noise)
Power Stability <2.00%
Beam Spot Size@ 1/e2 0.7mm(Horizontal/Vertical)
M2 <1.3
Output Mode TM00
Polarization Ratio >100:1
Warm-up Time 5min
Static Emission Height 19mm
Static Beam Collimation <±2.5mrad(Angle);
<±0.5mm(Position)
Spot Pointing Stability <30urad(8hrs, <±3℃);
<10urad/℃(8hrs, 15~35℃)
Laser Base Temperature During Operation 10℃ 40℃
Laser Base Temperature During Non-operation -10℃ 65℃
Shock Resistance During Operation (11ms) 1g
Shock Resistance During Non-operation (11ms) 25g
Vibration Resistance During Operation (5Hz‒500Hz) 0.3g
Vibration Resistance During Non-operation (5Hz‒500Hz) 2g
Non-operating Humidity (Non-condensing) 10% 90%
Input Voltage/Current @ 12V 11.8V , / 12V , / 12.2V , 0.5V
Input Voltage/Current @ 5V 4.8V , / 5V , / 5.2V , 2V
Heat Sink Power Consumption 4W
Drive Control Interface(DB 9 pin) J30J-9ZKS

Application

Semiconductor lasers areapplicable in fields such as laser guidance, laser ranging, optical communication, lidar, and laser sensing.

 

Product Description

Semiconductor lasers, also known as Laser Diodes (LDs) , are the most widely produced and utilized type of laser in the world. They use semiconductor materials as the gain medium and typically generate laser light through electrical injection. Their main advantages include compact size, high efficiency, long lifespan, and ease of integration.

To provide a comprehensive understanding, the following sections cover their working principle, core structure, main types, key components, and cutting-edge developments.

Working Principle and Core Structure

The operation of a semiconductor laser is based on stimulated emission. To achieve stable laser output, three fundamental conditions must be met, and the core structure is designed around these requirements:

Three Conditions Core Structure Function Description
Gain Condition Active Region To achieve population inversion. When current is injected into a semiconductor P-N junction, electrons and holes recombine in the active region, releasing photons. This is the material basis for light generation.
Resonance Condition Resonant Cavity To provide optical feedback. Typically, the natural cleaved facets of the semiconductor crystal (e.g., in Fabry-Perot cavities) act as mirrors, causing photons to oscillate back and forth and be amplified.
Threshold Condition Current Injection To overcome losses. Only when the injected current is high enough to reach the threshold current does the optical gain exceed the total losses, leading to stable laser oscillation and output.

Main Types

Through technological advancements, semiconductor lasers have evolved into various types to suit different applications. Below is a comparison of the mainstream types and their characteristics:

Type Characteristics Typical Applications
Edge-Emitting Laser Laser light is emitted from the side of the chip; the beam spot is elliptical and can achieve very high power. Industrial cutting, pump sources for fiber lasers.
Vertical-Cavity Surface-Emitting Laser (VCSEL) Laser light is emitted perpendicular to the chip surface; the beam spot is circular, has low power consumption, and is easy to fabricate in 2D arrays. Smartphone face recognition, short-reach data communication.
Distributed Feedback Laser (DFB) An integrated grating within the cavity ensures single-longitudinal-mode, narrow-linewidth, and wavelength-stable output. Long-haul fiber optic communication, gas sensing.
Quantum Cascade Laser (QCL) Based on intersubband transitions of electrons within quantum wells, covering the mid-to-far infrared and even terahertz bands. Trace gas detection, terahertz imaging.
Tunable Laser The output wavelength can be continuously tuned over a certain range using an external grating or filter. Dense wavelength-division multiplexing (DWDM) systems, optical spectrum analysis.

Key Optical Components

The performance of a semiconductor laser relies not only on the chip itself but also on the synergy of various precision optical components.

  • Optical Window:** Acts as a barrier between the chip and the environment. It must ensure high transmittance while withstanding damage from high-power lasers. Sapphire or diamond windows are often used in high-power devices to enhance heat dissipation.

  • Mirror:** Forms the core of the resonant cavity. It can be a natural cleaved facet of the semiconductor or a Distributed Bragg Reflector (DBR) with a reflectivity exceeding 99.9%.

  • Lens:** Used to correct the inherent high divergence angle of semiconductor lasers, enabling beam collimation or focusing.

  • Diffractive Optical Element (DOE) : By shaping the beam, DOEs can convert a Gaussian spot into a flat-top distribution or generate structured light patterns used in 3D sensing.

Cutting-Edge Developments

Current research in semiconductor laser technology is moving towards tighter integration and extreme performance.

  • On-Chip Integration:** Integrating lasers with other photonic components on a single silicon chip is a core requirement for optical interconnects and quantum technologies. Researchers are exploring techniques like heterogeneous integration (e.g., bonding III-V materials onto silicon) or monolithic integration (e.g., growing quantum dot lasers directly on silicon) to achieve low-cost, high-performance on-chip light sources.

  • Performance Breakthroughs:** Novel structures like Quantum Dot Lasers demonstrate excellent high-temperature performance and long operational life. Meanwhile, External Cavity Diode Lasers (ECDLs) can achieve high power, high beam quality, and even generate ultrashort pulses.

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