2005
DOI: 10.1063/1.2149371
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Gain and carrier losses of (GaIn)(NAs) heterostructures in the 1300–1550 nm range

Abstract: A microscopic model is used to analyze gain and loss properties of (GaIn)(NAs)∕GaAs quantum wells in the 1.3–1.55μm range, including Auger and radiative recombination. The calculations show that, as long as good material quality can be achieved, growing highly compressively strained samples is preferable due to their specific band structure properties. Optimum laser operation is possible slightly above a peak gain of 1000cm−1.

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Cited by 14 publications
(10 citation statements)
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“…Although the auger recombination is considered to be negligible in wide band gap material, some reports show that for some devices it is known to be of greater importance due to spontaneous emission [25]. So, Auger recombination is also included in this device simulation.…”
Section: Device Structure and Simulation Settingsmentioning
confidence: 99%
“…Although the auger recombination is considered to be negligible in wide band gap material, some reports show that for some devices it is known to be of greater importance due to spontaneous emission [25]. So, Auger recombination is also included in this device simulation.…”
Section: Device Structure and Simulation Settingsmentioning
confidence: 99%
“…The Silvaco Atlas 2‐D drift‐diffusion simulator was used to model the device response. The traps were modeled by using the Shockley–Read–Hall recombination . Polarization models were taken into account due to the strong spontaneous and piezoelectric polarization effects of nitride semiconductors .…”
Section: Optimizing the Device Structurementioning
confidence: 99%
“…The traps were modeled by using the Shockley-Read-Hall recombination. [25] Polarization models were taken into account due to the strong spontaneous and piezoelectric polarization effects of nitride semiconductors. [26] A low field mobility model and a nitride-specific high field dependent mobility model were used considering various types of scattering mechanisms.…”
Section: Optimizing the Device Structurementioning
confidence: 99%
“…Our microscopic model allows us to consider the gain and loss properties of (GaIn)(NAs) in the entire 1.3–1.55 µm range independent of any growth issues 56, addressing the question whether the degrading of optical properties at higher wavelengths is an intrinsic‐ or a material‐quality‐related phenomenon. Figure 14 shows the intensity gain at 1.3 µm (solid lines) and 1.55 µm (dotted lines) in a quantum‐well structure containing 40% indium.…”
Section: (Gain)(nas)‐based Materials Systemmentioning
confidence: 99%