2006
DOI: 10.1063/1.2211301
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Electron-lattice coupling in bound-to-continuum THz quantum-cascade lasers

Abstract: Articles you may be interested inSubband electronic temperatures and electron-lattice energy relaxation in terahertz quantum cascade lasers with different conduction band offsets

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Cited by 40 publications
(33 citation statements)
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“…3͑b͒ shows that the most likely channel for thermal activation of electrons out of the upper laser level is into the higher lying state localized mainly in the first two wells of the miniband; previous photoluminescence studies of operating QCLs have supported the suggestion of carrier leakage into this state. 24 The measured activation energy is in reasonable agreement with the calculated position of this level ϳ7.5 meV above the upper laser level.…”
Section: Temperature Dependencesupporting
confidence: 73%
“…3͑b͒ shows that the most likely channel for thermal activation of electrons out of the upper laser level is into the higher lying state localized mainly in the first two wells of the miniband; previous photoluminescence studies of operating QCLs have supported the suggestion of carrier leakage into this state. 24 The measured activation energy is in reasonable agreement with the calculated position of this level ϳ7.5 meV above the upper laser level.…”
Section: Temperature Dependencesupporting
confidence: 73%
“…If thermalization of carriers by e-e intrasubband scattering is not significantly more efficient than intersubband scattering processes, the carriers accumulate in the subband 1 up to the kinetic energy of 9 meV, in contrast to the Fermi-Dirac or the Maxwell-Boltzmann distributions 35,36 . The relative simplicity of this device would make it a good candidate for studies of electron temperature by microprobe photoluminescence experiments 37 .…”
Section: Resultsmentioning
confidence: 99%
“…In the case of BTC devices, band-to-band transitions associated with the injector low energy miniband and upper laser level j = 2 are visible, together with the heavyhole (HH) and light-hole (LH) exciton peaks arising from level 2, as expected from the calculation of the Debye screening length [8,9]. For the line shape analysis we used as fitting function a Lorentzian on the low energy side joined with an exponential decay on the high energy side for band-to-band transitions and a Lorentzian for the exciton peaks [10,11]. The experimental data have been fitted leaving T j e , the band intensities and the full width at half maximum of the HH and LH exciton peaks as fitting parameters.…”
Section: Resultsmentioning
confidence: 99%