| Ytterbium-Doped Fiber Laser Pump | ≈ n.d. | 808 nm or 980 nm direct-emitting pump diode | CW Quasi-CW | Approximately 1–20 W per emitter; higher power is commonly achieved with bars or stacked modules | Stable continuous current or millisecond-scale quasi-CW pulses; low ripple is important for pump stability | Low-noise constant-current source, soft start, over-current protection, current monitoring, and controlled output rise time | Efficient heat sinking, copper-based submounts, thermoelectric control where wavelength stability is important, and reliable optical coupling | Choose 980 nm when efficient in-band pumping and good absorption in ytterbium-doped fiber are priorities. Choose 808 nm when the gain medium and pump architecture are designed for that absorption band. |
| Erbium-Doped Fiber Amplifier or Fiber-Laser Pump | ≈ 980 nm | 980 nm pump diode, often fiber-coupled | CW Low-noise modulation | Typically hundreds of milliwatts to several watts, depending on the pump module and coupling configuration | Usually continuous operation; current modulation is normally limited to avoid excess intensity noise and thermal wavelength drift | Highly stable current regulation, low electrical noise, current limit, fault shutdown, monitor-photodiode input, and enable control | Thermal resistance, wavelength stabilization, fiber-coupling alignment, and protection against optical feedback are key considerations | Use a driver with tight current stability and slow-start behavior. The selected diode wavelength should match the absorption peak and operating temperature of the doped fiber. |
| Short-Range or Automotive LiDAR | ≈ 905 nm | 905 nm edge-emitting pulsed laser diode or multi-emitter array | Nanosecond pulse Low duty cycle | Peak optical power commonly ranges from tens of watts to several hundred watts for pulsed emitters; average power is much lower | Typically about 1–10 ns pulse widths, with pulse repetition frequency determined by range, frame rate, and eye-safety limits | Very fast current pulse loop, low-inductance layout, controlled peak current, precise trigger timing, overshoot suppression, and rapid recovery | Short thermal transients, low parasitic inductance, robust die attach, optical-axis control, and protection from repetitive electrical overstress | Choose 905 nm for mature, cost-sensitive time-of-flight systems. Size the driver by peak current, pulse width, repetition rate, and junction-temperature rise rather than average current alone. |
| Longer-Range or Eye-Safer LiDAR | ≈ 1550 nm | 1550 nm pulsed laser diode, semiconductor optical amplifier, or fiber-laser source | Nanosecond pulse High peak power | System-dependent; pulsed sources can provide high peak power while remaining within applicable eye-safety limits | Often nanosecond-scale pulses with tightly controlled timing, repetition rate, and pulse-to-pulse energy | High-speed pulsed-current driver, accurate trigger synchronization, low jitter, fast turn-off, peak-current limiting, and electromagnetic-noise control | Thermal management remains important at high repetition rates; optical isolation and wavelength-compatible coatings are also required | 1550 nm can permit higher permissible exposure levels than 905 nm under applicable safety standards, but detector sensitivity, source efficiency, cost, and atmospheric losses must be evaluated together. |
| 1310 nm Fiber-Optic Telecom | ≈ 1310 nm | 1310 nm Fabry–Pérot or distributed-feedback laser diode | Continuous bias Direct modulation | Typically a few milliwatts to tens of milliwatts at the fiber output for access and short-to-medium-reach links | High-speed intensity modulation; required bandwidth depends on the link standard and transceiver design | Low-noise bias current, modulation-current control, automatic power control, monitor-photodiode feedback, and controlled laser turn-on | Temperature compensation, stable fiber coupling, low relative-intensity noise, and protection from electrostatic discharge and optical reflection | 1310 nm is associated with low chromatic dispersion in standard single-mode fiber, making it useful for many access and moderate-distance links. |
| 1550 nm Fiber-Optic Telecom | ≈ 1550 nm | 1550 nm distributed-feedback laser diode or tunable laser | Continuous bias High-speed modulation | Commonly a few milliwatts to tens of milliwatts per channel before amplification; long-haul systems may use optical amplifiers | High-speed modulation or coherent modulation; narrow linewidth and frequency stability may be required for coherent links | Low-noise bias and modulation control, automatic power control, monitor-photodiode feedback, thermal tuning, and protection against optical feedback | Precise temperature control, low frequency drift, stable wavelength tuning, optical isolation, and high-quality fiber coupling are priorities | 1550 nm aligns with the low-loss region of silica fiber and supports optical amplification. Select the driver according to direct-detection or coherent operation, modulation bandwidth, and linewidth requirements. |
| Industrial Heating, Sensing, or Medical Pumping | 808 nm or 980 nm | High-power broad-area laser diode or diode array | CW Quasi-CW | Several watts to hundreds of watts at module level, depending on emitter count, beam-combining method, and cooling system | Continuous operation or controlled millisecond-to-second pulses; repetition rate is usually application-specific | High-current constant-current regulation, programmable ramping, current sharing, fault interlock, output monitoring, and emergency shutdown | Liquid or forced-air cooling may be required; mechanical stability, uniformity across emitters, and protection against condensation are important | Prioritize wall-plug efficiency, thermal resistance, beam uniformity, allowable current range, and lifetime at the intended duty cycle. |