Showing posts with label A. Klimont. Show all posts
Showing posts with label A. Klimont. Show all posts

Tuesday, October 29, 2019

Abstract-Line-defect photonic crystal terahertz quantum cascade laser

Publisher Logo


A. Klimont, A. Ottomaniello,  R. Degl’Innocenti, L. Masini, F. Bianco, Y. Wu1,  Y. D. Shah, Y. Ren, D. S. Jessop,  A. Tredicucci, H. E. Beere,  D. A. Ritchie.

Scanning electron microscope (SEM) pictures of the line defect QCLs after reactive ion etching for three different line-defect waveguides. Figure (a) corresponds to D1, where the defects before BCB planarization are separated by one row of small pillars in the triangular PhC lattice. Figure (b) (D3) and (c) (D5) correspond to line-defect QCLs separated by three rows and five rows of small pillars, respectively. Figure (d) shows in more detail the defect area and identifies the main parameters of the PhC structure, such as the vectors on the direct triangular lattice, a1 and a2, the radius of the regular and defect pillars, r and R, respectively, as well as the line orientation. Figure (e) shows a typical line-defect QCL after the BCB planarization, leaving only the tops of ∼14 μm-tall pillars exposed.
https://aip.scitation.org/doi/full/10.1063/1.5120025

The terahertz (THz) quantum cascade laser (QCL) provides a versatile tool in a plethora of applications ranging from spectroscopy to astronomy and communications. In many of these fields, compactness, single mode frequency emission, and low threshold are highly desirable. The proposed approach, based on line defects in a photonic crystal (PhC) matrix, addresses all these features while offering unprecedented capabilities in terms of flexibility, light waveguiding, and emission directionality. Nine line-defect QCLs were realized in a triangular lattice of pillars fabricated in the laser active region (AR), centered around ∼2 THz by tuning the photonic design. A maximal 36% threshold reduction was recorded for these ultraflat dispersion line-defect QCLs in comparison to standard metal-metal QCL. The mode selectivity is an intrinsic property of the chosen fabrication design and has been achieved by lithographically scaling the dimension of the defect pillars and by acting on the PhC parameters in order to match the AR emission bandwidth. The measured line-defect QCLs emitted preferentially in the single frequency mode in the propagation direction throughout the entire dynamic range. An integrated active platform with multiple directional outputs was also fabricated as proof-of-principle to demonstrate the potential of this approach. The presented results pave the way for integrated circuitry operating in the THz regime and for fundamental studies on microcavity lasers.

Tuesday, September 29, 2015

Abstract-Efficient coupling of double-metal terahertz quantum cascade lasers to flexible dielectric-lined hollow metallic waveguides


R. Wallis, R. Degl’Iinnocenti, D. S. Jessop, Y. Ren, A. Klimont, Y. D. Shah, O. Mitrofanov, C. M. Bledt, J. E. Melzer, J. A. Harrington, H. E. Beere, and D. A. Ritchie
https://www.osapublishing.org/oe/abstract.cfm?uri=oe-23-20-26276

The growth in terahertz frequency applications utilising the quantum cascade laser is hampered by a lack of targeted power delivery solutions over large distances (>100 mm). Here we demonstrate the efficient coupling of double-metal quantum cascade lasers into flexible polystyrene lined hollow metallic waveguides via the use of a hollow copper waveguide integrated into the laser mounting block. Our approach exhibits low divergence, Gaussian-like emission, which is robust to misalignment error, at distances > 550 mm, with a coupling efficiency from the hollow copper waveguide into the flexible waveguide > 90%. We also demonstrate the ability to nitrogen purge the flexible waveguide, increasing the power transmission by up to 20% at 2.85 THz, which paves the way for future fibre based terahertz sensing and spectroscopy applications.
© 2015 Optical Society of America
Full Article  |  PDF Article