791 research outputs found

    Fabrication methods for a quantum cascade photonic crystal surface emitting laser

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    Conventional quantum cascade (QC) lasers are intrinsically edge-emitting devices with mode confinement achieved via a standard mesa stripe configuration. Surface emission in edge emitting QC lasers has therefore necessitated redirecting the waveguided laser emission using a second order grating. This paper describes the methods used to fabricate a 2D photonic crystal (PC) structure with or without a central defect superimposed on an electrically pumped QC laser structure with the goal of achieving direct surface emission. A successful systematic study of PC hole radius and spacing was performed using e-beam lithography. This PC method offers the promise of a number of interesting applications, including miniaturization and integration of QC lasers

    Transport and percolation in a low-density high-mobility two-dimensional hole system

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    We present a study of the temperature and density dependence of the resistivity of an extremely high quality two-dimensional hole system grown on the (100) surface of GaAs. For high densities in the metallic regime (p\agt 4 \times 10^{9} cm2^{-2}), the nonmonotonic temperature dependence (50300\sim 50-300 mK) of the resistivity is consistent with temperature dependent screening of residual impurities. At a fixed temperature of TT= 50 mK, the conductivity vs. density data indicates an inhomogeneity driven percolation-type transition to an insulating state at a critical density of 3.8×1093.8\times 10^9 cm2^{-2}.Comment: accepted for publication in PR

    Fabrication technologies for quantum cascade photonic-crystal microlasers

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    In this paper we describe the technological and fabrication methods necessary to incorporate both photonic and electronic-band engineering in order to create novel surface-emitting quantum cascade microcavity laser sources. This technology offers the promise of several innovative applications such as the miniaturization of QC lasers, and multi-wavelength two-dimensional laser arrays for spectroscopy, gas-sensing and imaging. This approach is not limited to light-emitting devices, and may be efficiently applied to the development of mid- and far-infrared normal-incidence detectors

    Quantum cascade photonic crystal surface emitting injection laser

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    A surface emitting quantum cascade injection laser is presented. Direct surface emission is obtained by using a 2D photonic-band-gap structure that simultaneously acts as a microcavity. The approach may allow miniaturization and on-chip-integration of the devices

    Bias-Dependent Generation and Quenching of Defects in Pentacene

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    We describe a defect in pentacene single crystals that is created by bias stress and persists at room temperature for an hour in the dark but only seconds with 420nm illumination. The defect gives rise to a hole trap at Ev + 0.38eV and causes metastable transport effects at room temperature. Creation and decay rates of the hole trap have a 0.67eV activation energy with a small (108 s-1) prefactor, suggesting that atomic motion plays a key role in the generation and quenching process.Comment: 10 pages, 3 figure

    Acoustic phonon scattering in a low density, high mobility AlGaN/GaN field effect transistor

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    We report on the temperature dependence of the mobility, μ\mu, of the two-dimensional electron gas in a variable density AlGaN/GaN field effect transistor, with carrier densities ranging from 0.4×1012\times10^{12} cm2^{-2} to 3.0×1012\times10^{12} cm2^{-2} and a peak mobility of 80,000 cm2^{2}/Vs. Between 20 K and 50 K we observe a linear dependence μac1=α\mu_{ac}^{-1} = \alphaT indicating that acoustic phonon scattering dominates the temperature dependence of the mobility, with α\alpha being a monotonically increasing function of decreasing 2D electron density. This behavior is contrary to predictions of scattering in a degenerate electron gas, but consistent with calculations which account for thermal broadening and the temperature dependence of the electron screening. Our data imply a deformation potential D = 12-15 eV.Comment: 3 pages, 2 figures, RevTeX. Submitted to Appl Phys Let

    Large Bychkov-Rashba spin-orbit coupling in high-mobility GaN/AlGaN heterostructures

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    We present low temperature magnetoconductivity measurements of a density-tunable and high mobility two-dimensional electron gas confined in the wide bandgap GaN/AlGaN system. We observed pronounced anti-localization minima in the low-field conductivity, indicating the presence of strong spin-orbit coupling. Density dependent measurements of magnetoconductivity indicate that the coupling is mainly due to the Bychkov-Rashba mechanism. In addition, we have derived a closed-form expression for the magnetoconductivity, allowing us to extract reliable transport parameters for our devices. The Rashba spin-orbit coupling constant is αso\alpha_{so} \sim 6×\times 1013^{-13}eVm, while the conduction band spin-orbit splitting energy amounts to Δso\Delta_{so} \sim 0.3meV at ne_e=1×1016\times10^{16}m2^{-2}.Comment: Accepted for publication in PR

    Impact of spin-orbit coupling on quantum Hall nematic phases

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    Anisotropic charge transport is observed in a two-dimensional (2D) hole system in a perpendicular magnetic field at filling factors nu=7/2, nu=11/2, and nu=13/2 at low temperature. In stark contrast, the transport at nu=9/2 is isotropic for all temperatures. Isotropic hole transport at nu=7/2 is restored for sufficiently low 2D densities or an asymmetric confining potential. The density and symmetry dependences of the observed anisotropies suggest that strong spin-orbit coupling in the hole system contributes to the unusual transport behavior.Comment: 4 pages, 4 figure

    Lasing mode pattern of a quantum cascade photonic crystal surface-emitting microcavity laser

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    The identification of the lasing mode within a quantum cascade photonic crystal microcavity laser emitting at λ ~8 µm is presented. The symmetry of the lasing mode is determined by the position of nodal lines within micro-bolometer camera measurements of its polarized spatial distribution. Full three-dimensional finite-difference time-domain simulations are also performed, and the resulting vertically emitted radiation field pattern is seen to follow the experimental results closely
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