1999
DOI: 10.1002/(sici)1521-3951(199901)211:1<255::aid-pssb255>3.0.co;2-w
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Quantum-Well and Cavity-Mode Resonance Effects in a Vertical-Cavity Surface-Emitting Laser Structure, Observed by Photoreflectance Using Hydrostatic Pressure and Temperature Tuning

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Cited by 21 publications
(9 citation statements)
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“…The rate at which the cavity mode changes with temperature is calculated in two ways. First, the ratio of for EEL and VCSEL is assumed to be the same as the ratio [22]. 0.34 meV K for the EEL and is calculated for the VCSEL as 0.079 meV K .…”
Section: Temperature Dependence Measurementsmentioning
confidence: 99%
“…The rate at which the cavity mode changes with temperature is calculated in two ways. First, the ratio of for EEL and VCSEL is assumed to be the same as the ratio [22]. 0.34 meV K for the EEL and is calculated for the VCSEL as 0.079 meV K .…”
Section: Temperature Dependence Measurementsmentioning
confidence: 99%
“…[1][2][3] The major challenge in achieving efficient lasing in VCSELs is strongly dependent on the wavelength alignment between the peak of the gain spectrum of the active quantum well (QW) layers and the cavity mode (CM) dip in the reflectance spectrum of the VCSEL Fabry-Perot structure. 4,5 When other effects such as self-heating and non-radiative recombination have been taken into account, achieving an optimized alignment at the desired operating temperature between the energy positions of the QW ground-state transition (E QW ) and the CM dip in the reflectance spectrum (E CM ) should give improved device performance. 6 It is thus critical to know the initial E CM /E QW alignment especially with respect to the temperature performance of devices.…”
Section: Introductionmentioning
confidence: 99%
“…The major challenge in achieving efficient lasing in VCSELs is strongly dependent on the wavelength alignment between the peak of the gain spectrum of the active quantum well (QW) layers and the cavity mode (CM) of the reflectance spectrum of the VCSEL Fabry-Perot structure. When other effects such as self-heating and non-radiative recombination is taken into account, achieving an optimized alignment at the desired operating temperature (T) between the energy positions of the QW ground-state transition (E QW ) and the CM dip in the reflectance spectrum (E CM ) should give ideal device performance [5,6]. However, even a small E QW -E CM misalignment at the desired operating T causes significant degradation in the threshold current and output power.…”
Section: Introductionmentioning
confidence: 99%