使用InGaAs InGaAsP材料进行EDFA泵浦方案的1480nm半导体激光器功率比较

Satyo Pradana, A. Syahriar, Ahmad H. Lubis, S. Rahardjo
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引用次数: 1

摘要

远程光通信受到许多问题的影响;信号丢失就是其中之一。掺铒光纤放大器是解决这一问题的关键。利用半导体激光器作为EDFA的抽运源,可以使信号恢复到正常状态。EDFA在1480nm处具有良好的波长操作。为了实现选定的波长,必须构造适合于1480nm波长的半导体激光器。在这种情况下,InGaAs和InGaAsP是构建半导体激光器的基础材料。在1480nm波长处,使用的材料是InGaAs和InGaAsP。原因是它适合波长选择。通过选择合适的波长和材料,可以制作出合适的半导体激光器。同时,参数的确定也是激光器结构的重要组成部分。利用速率方程对InGaAs和InGaAsP在1480nm波长处的输出功率进行比较,得到了四种结果。它们是注入电流vs电压,载流子密度,光子密度和输出功率vs注入电流。
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Comparison Power of Semiconductor Lasers at wavelength 1480nm using InGaAs InGaAsP Materials for EDFA Pumping Scheme
Long distance Optical Communications are affected by many problems; loss of signal is one of them. Erbium Doped Fiber Amplifier (EDFA) is the key to solve it. By using Semiconductor Laser as pumping source for EDFA, the signal can be brought back to it is normal condition. EDFA has a good wavelength operation at 1480nm. To achieve selected wavelength, we must construct the Semiconductor Laser that suitable in 1480nm. In that case, InGaAs and InGaAsP are the base materials to construct the Semiconductor Laser. At wavelength of 1480nm the materials that used are InGaAs and InGaAsP. The reason is it is suitable for wavelength selection. By using selected wavelength and materials, the Semiconductor Laser can be produced properly. Also, determining the parameter is the important thing to construct the Laser. By using Rate Equation, comparison of output power for InGaAs and InGaAsP at wavelength of 1480nm based on rate equation and can obtained four result. Those are injection current vs voltage, carrier density, photon density and output power vs injection current.
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