Presentation is loading. Please wait.

Presentation is loading. Please wait.

Continued Advanced Semiconductor Lab.

Similar presentations


Presentation on theme: "Continued Advanced Semiconductor Lab."— Presentation transcript:

1 continued Advanced Semiconductor Lab

2

3 New Materials Strong temperature sensitivity ← Insufficient electron confinement in the active region Insufficient variation of refraction index in InGaAs/InP ← severe problem in the formation of distributed Bragg reflectors for vertical cavity surface emitting lasers (VCSELs) Quantum well structure 로는 필요한 파장 range를 얻지 못한다.  Emerge Quantum Dot, InGaAsN, InNAsP, etc.

4 7.4 Mode power distributed feedback lasers
Solution of incident and reflection Reflectance for corrugation at z=0 Under phase matching conditions, △β Semiconductor optoelectronic devices, by P. Bhattacharya

5 Semiconductor optoelectronic devices, by P. Bhattacharya

6 7.5 Cleaved-Coupled-Cavity(C3 ) laser
Semiconductor optoelectronic devices, by P. Bhattacharya

7 Injection-locked Laser
C3 Laser Injection-locked Laser Semiconductor optoelectronic devices, by P. Bhattacharya

8 7.6 Quantum well laser Semiconductor optoelectronic devices, by P. Bhattacharya

9 Band diagram of the active region
Semiconductor optoelectronic devices, by P. Bhattacharya

10 Strained Quantum Well Lasers
Semiconductor optoelectronic devices, by P. Bhattacharya

11 7.7 Surface-Emitting Laser
Semiconductor optoelectronic devices, by P. Bhattacharya

12 7.10 Device fabrication Broad-area laser by cleaving
Ridge lasers are defined by photolithography and wet or dry etching Semiconductor optoelectronic devices, by P. Bhattacharya

13 7.11 measurement of laser characteristics
Differential gain Near-and far field patterns Usually, the fabricated laser is mounted on an efficient heat sink. For high performance operations, a feedback circuit and thermoelectric cooling are provided. It is common to determine the laser characteristics under pulsed biasing conditions. Semiconductor optoelectronic devices, by P. Bhattacharya

14 Linearity of light current characteristics
Modulated output power P(t) = P0 [1+ms(t)] Modulation index, Harmonic distortion Intermodulation distortion light-current characteristics should be as linear as possible. Semiconductor optoelectronic devices, by P. Bhattacharya

15 7.16 Long-wavelength semiconductor laser
Lead-salt or lead chalcogenide lasers Population inversion can be achieved by using resonant tunneling Tuning by changing the well and barrier parameters Semiconductor optoelectronic devices, by P. Bhattacharya


Download ppt "Continued Advanced Semiconductor Lab."

Similar presentations


Ads by Google