Abstract:A highly selective wet chemical etch process for gate recess of the GaAs power metal-semiconductor field effect transistors (MES-FETs) was developed. The power MESFETs used in this study were epitaxially grown devices with a 20 Å AlAs etch-stop layer for gate recess. The selective etch process using citric acid/potassium citrate/hydrogen peroxide solution was studied. A selectivity better than 3800:1 was achieved for GaAs/AlAs layers. This selective etch was applied both to high-power, high-voltage power MESFE… Show more
“…GaAs, the substrate was removed by a series of etches [19,20]. The final result of the processing was a 1 × 2 mm membrane less than 1 µm thick.…”
mentioning
confidence: 99%
“…For the experimental convenience of matching excitonic absorption peaks in the different samples, the band gap of the wider well was raised by adding 5% aluminum to match the 2D band gap of the narrower well. Because HSG is measured in transmission and the exciton absorption lines of the QWs are above the band gap of bulk arXiv:1309.3264v3 [cond-mat.mes-hall] 2 Jan 2014 GaAs, the substrate was removed by a series of etches [19,20]. The final result of the processing was a 1 × 2 mm membrane less than 1 µm thick.…”
Electron-hole recollisions are induced by resonantly injecting excitons with a near-IR laser at frequency fNIR into quantum wells driven by a 10 kV/cm field oscillating at fTHz = 0.57 THz. At T = 12 K, up to 18 sidebands are observed at frequencies f sideband = fNIR + 2nfTHz, with −8 ≤ 2n ≤ 28. Electrons and holes recollide with total kinetic energies up to 57 meV, well above the ELO = 36 meV threshold for longitudinal optical (LO) phonon emission. Sidebands with order up to 2n = 22 persist up to room temperature. A simple model shows that LO phonon scattering suppresses but does not eliminate sidebands associated with kinetic energies above ELO.The interaction of electrons and holes in semiconductors has long been a rich area of study in physics. In most cases, the electron and hole are treated as point particles within the effective mass approximation [1]. In this approximation, the effects of the lattice are parametrized by the dielectric constant of the semiconductor and the effective masses of the electrons and holes. Calculations based on the effective mass approximation successfully predict, for example, the binding energies and the frequencies of internal transitions of impurity-bound electrons and excitons in GaAs [2] and in GaAs/AlGaAs quantum wells [3][4][5]. The effective mass approximation, however, belies the rich complexity of the microscopic physics. In GaAs, for example, ground-state excitons are collective excitations of more than 10 5 atoms in the crystal. The advent of sources of intense terahertz electromagnetic radiation enables the study of semiconductors in a regime where time-dependent perturbation theory fails completely. Exciting new quantum coherent phenomena emerge, including the dynamical Franz-Keldysh effect [6,7], non-linear excitonic effects [8][9][10][11], and highorder sideband generation [12][13][14]. High-order sideband generation is a cousin of high-order harmonic generation from atoms in intense laser fields [15][16][17]. Excitons are created by a near-infrared laser in a semiconductor driven by an intense terahertz field. The terahertz field ionizes the exciton into an electron and a hole that it then pulls apart and smashes back together. Upon recollision, the electron and hole can recombine across the band gap with the acquired kinetic energy carried off by light with frequency above that of the near-IR laser.In this Letter, we report that the electron-hole recollision process-which, in its theoretical descriptions to date has been treated as a purely ballistic process-is surprisingly robust against scattering. We report electronhole recollisions both with kinetic energy well above the threshold for emission of a longitudinal optical (LO) phonon and at room temperature. We model our results by treating the electron-hole pair as a single particle with the appropriate reduced mass subject to dephasing and LO phonon scattering.Two quantum well (QW) samples with 20 QW repetitions were studied. Both samples were grown on semiinsulating GaAs substrates by molecular beam epitax...
“…GaAs, the substrate was removed by a series of etches [19,20]. The final result of the processing was a 1 × 2 mm membrane less than 1 µm thick.…”
mentioning
confidence: 99%
“…For the experimental convenience of matching excitonic absorption peaks in the different samples, the band gap of the wider well was raised by adding 5% aluminum to match the 2D band gap of the narrower well. Because HSG is measured in transmission and the exciton absorption lines of the QWs are above the band gap of bulk arXiv:1309.3264v3 [cond-mat.mes-hall] 2 Jan 2014 GaAs, the substrate was removed by a series of etches [19,20]. The final result of the processing was a 1 × 2 mm membrane less than 1 µm thick.…”
Electron-hole recollisions are induced by resonantly injecting excitons with a near-IR laser at frequency fNIR into quantum wells driven by a 10 kV/cm field oscillating at fTHz = 0.57 THz. At T = 12 K, up to 18 sidebands are observed at frequencies f sideband = fNIR + 2nfTHz, with −8 ≤ 2n ≤ 28. Electrons and holes recollide with total kinetic energies up to 57 meV, well above the ELO = 36 meV threshold for longitudinal optical (LO) phonon emission. Sidebands with order up to 2n = 22 persist up to room temperature. A simple model shows that LO phonon scattering suppresses but does not eliminate sidebands associated with kinetic energies above ELO.The interaction of electrons and holes in semiconductors has long been a rich area of study in physics. In most cases, the electron and hole are treated as point particles within the effective mass approximation [1]. In this approximation, the effects of the lattice are parametrized by the dielectric constant of the semiconductor and the effective masses of the electrons and holes. Calculations based on the effective mass approximation successfully predict, for example, the binding energies and the frequencies of internal transitions of impurity-bound electrons and excitons in GaAs [2] and in GaAs/AlGaAs quantum wells [3][4][5]. The effective mass approximation, however, belies the rich complexity of the microscopic physics. In GaAs, for example, ground-state excitons are collective excitations of more than 10 5 atoms in the crystal. The advent of sources of intense terahertz electromagnetic radiation enables the study of semiconductors in a regime where time-dependent perturbation theory fails completely. Exciting new quantum coherent phenomena emerge, including the dynamical Franz-Keldysh effect [6,7], non-linear excitonic effects [8][9][10][11], and highorder sideband generation [12][13][14]. High-order sideband generation is a cousin of high-order harmonic generation from atoms in intense laser fields [15][16][17]. Excitons are created by a near-infrared laser in a semiconductor driven by an intense terahertz field. The terahertz field ionizes the exciton into an electron and a hole that it then pulls apart and smashes back together. Upon recollision, the electron and hole can recombine across the band gap with the acquired kinetic energy carried off by light with frequency above that of the near-IR laser.In this Letter, we report that the electron-hole recollision process-which, in its theoretical descriptions to date has been treated as a purely ballistic process-is surprisingly robust against scattering. We report electronhole recollisions both with kinetic energy well above the threshold for emission of a longitudinal optical (LO) phonon and at room temperature. We model our results by treating the electron-hole pair as a single particle with the appropriate reduced mass subject to dephasing and LO phonon scattering.Two quantum well (QW) samples with 20 QW repetitions were studied. Both samples were grown on semiinsulating GaAs substrates by molecular beam epitax...
“…The technology of the substrate removal after the assembly of the FPA consisted of the successive processes of the mechanical grinding aimed at removing the main thickness of the GaAs substrate, chemical mechanical polishing and chemical dynamic polishing, in order to obtain a mirror-smooth surface of the array crystal. The processes of the chemical selective etching of the GaAs and heterostructure layers were applied to remove the GaAs substrate from the FPA surface completely (Figure 15) [20][21][22].…”
Section: The Gaas Substrate Removal From the Fpa Assemblymentioning
In this article, we present an overview of a focal plane array (FPA) with 640 Â 512 pixels based on the AlGaAs quantum well infrared photodetector (QWIP). The physical principles of the QWIP operation and their parameters for the spectral range of 8-10 μm have been discussed. The technology of the manufacturing FPA based on the QWIP structures with the pixels 384 Â 288 and 640 Â 512 has been demonstrated. The parameters of the manufactured 640 Â 512 FPA with a step of 20 μm have been given. At the operating temperature of 72 K, the temperature resolution of QWIP focal plane arrays is less than 35 mK. The number of defective elements in the matrix does not exceed 0.5%. The stability and uniformity of the FPA have been demonstrated.
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