Mai wa Laser Diode?
Takaitaccen Laser Diode
Laser diode na nufin diod da zan iya gina laser light idan an sanya da karamin current. Yana cikin p-n junction tare da wurin intrinsic layer a kan bayan, wanda yake tsakiyar p-i-n. Wurin intrinsic layer shine wurin aktif da inda light ta shafi da recombination daga electrons da holes.
P-type da n-type regions suna sauran da impurities don samun carriers, amma wurin intrinsic layer ba'a undoped ko lightly doped don allow for optical amplification. Afafin intrinsic layer suna kasa da reflective materials, daya fully reflective da daya partially reflective, don form optical cavity wanda yake shiga light da kuma enhance stimulated emission.
Stimulated emission ya faru idan photon mai inganta ya fa excited electron a drop to a lower energy level da kuma emit another photon wanda yake mafi so kuɗi da incoming one a frequency, phase, polarization, and direction. Haka, number of photons a cavity ya zama exponentially, creating coherent beam of light wanda yake shiga through the partially reflective end.
Wavelength of laser light ya bambanta da band gap of the semiconductor material and the optical cavity’s length, enabling emission across the electromagnetic spectrum, from infrared to ultraviolet.
Mechanism of Operation
Laser diode ya yi aiki tare da applying a forward bias voltage across the p-n junction, which causes current to flow through the device. The current injects electrons from the n-type region and holes from the p-type region into the intrinsic layer, where they recombine and release energy in the form of photons.
Some of these photons are spontaneously emitted in random directions, while others are stimulated by existing photons in the cavity to emit in phase with them. The stimulated photons bounce back and forth between the reflective ends, causing more stimulated emission and creating a population inversion, where there are more excited electrons than non-excited ones.
When the population inversion reaches a threshold level, steady-state laser output is achieved, where the rate of stimulated emission equals the rate of photon loss due to transmission or absorption. The output power of the laser diode depends on the input current and the efficiency of the device.
Output power hinges on device temperature; higher temperatures decrease efficiency and raise the threshold current, necessitating cooling systems for optimal performance.
Types of Laser Diodes
Laser diodes are classified into different types based on their structure, mode of operation, wavelength, output power, and application. Some of the common types are:
Single-mode laser diodes
Multi-mode laser diodes
Master oscillator power amplifier (MOPA) laser diodes
Vertical cavity surface emitting laser (VCSEL) diodes
Distributed feedback (DFB) laser diodes
External cavity diode lasers (ECDLs)

Applications of Laser Diodes
Optical storage
Optical communication
Optical scanning
Optical sensing
Optical display
Optical surgery
Advantages of Laser Diodes
Compact size
Low power consumption
High efficiency
Long lifetime
Versatility
Disadvantages of Laser Diodes
Temperature sensitivity
Optical Feedback
Mode hopping
Cost
Summary
Laser diode na nufin semiconducting device wanda yake produce coherent light through a process of stimulated emission. Yana ciki da light-emitting diode (LED), amma yana da structure masu kyau da kuma faster response time.
Laser diode na nuna p-n junction tare da wurin intrinsic layer a kan bayan, wanda yake tsakiyar p-i-n. Wurin intrinsic layer shine wurin aktif da inda light ta shafi da recombination daga electrons da holes.
Laser diode ya yi aiki tare da applying a forward bias voltage across the p-n junction, which causes current to flow through the device. The current injects electrons from the n-type region and holes from the p-type region into the intrinsic layer, where they recombine and release energy in the form of photons.
Some of these photons are spontaneously emitted in random directions, while others are stimulated by existing photons in the cavity to emit in phase with them. The stimulated photons bounce back and forth between the reflective ends, causing more stimulated emission and creating a population inversion, where there are more excited electrons than non-excited ones.
When the population inversion reaches a threshold level, steady-state laser output is achieved, where the rate of stimulated emission equals the rate of photon loss due to transmission or absorption. The output power of the laser diode depends on the input current and the efficiency of the device.
The wavelength of the laser light depends on the band gap of the semiconductor material and the length of the optical cavity. Laser diodes can produce light in different regions of the electromagnetic spectrum, from infrared to ultraviolet.
Laser diodes are classified into different types based on their structure, mode of operation, wavelength, output power, and application. Some of the common types are single-mode laser diodes, multi-mode laser diodes, master oscillator power amplifier (MOPA) laser diodes, vertical cavity surface emitting laser (VCSEL) diodes, distributed feedback (DFB) laser diodes, external cavity diode lasers (ECDLs), etc.
Laser diodes have a wide range of applications in various fields due to their advantages such as compact size, low power consumption, high efficiency, long lifetime, and versatility. Some of their applications are optical storage, optical communication, optical scanning, optical sensing, optical display, and optical surgery.
Despite their benefits, laser diodes have drawbacks including temperature sensitivity, optical feedback, mode hopping, and high costs.