We report a numerical investigation of the recently proposed (Nature 621, 2023, 746) high-speed μ-OLED optically pumped organic laser and confirm that in this configuration the threshold for quasi-CW lasing is much easier reached than in case of a direct-electrically pumped organic laser diode. With a new model for the electrically biased OLED, we simulate the generation of pulsed and quasi-CW light. This light is fed into the organic laser where it optically pumps the emitting organic medium The model is voltage-driven and includes field-enhanced Langevin recombination in the OLED, Stoke-shifted reabsorption in both the OLED and organic laser, with an optical cavity in the latter. We numerically demonstrate 3.5 kA/cm2 laser threshold current density, 1 GHz modulation and conjecture the capability of Gb/s data transmission with this device.
We report experimental and theoretical investigations with high-speed μ-OLEDs and demonstrate promising optical pulse responses as short as 400 ps using Alq3. These observations indicate that high-speed μ-OLEDs can be used for light communication in the GHz regime. The measurements are for in-house fabricated μ-OLEDs without cavity and size of 100 μm × 100 μm. With a validated model for an electrically pumped OLED, we simulate the generation of ultra-short optical pulses. The model includes Stoke-shifted reabsorption and field-enhanced Langevin recombination rate. For the Alq3 system we compare the results with the above-mentioned measurements. The good agreement between the measurement and the simulation is the basis for further study of the prospects for ultra-short dynamics and organic laser diode operation on the ps time scale.
We have realized and characterized an optically pumped hybrid photonic crystal (PhC) L3 nanocavity made of an organic material as a gain medium and a Si3N4 two-dimensional PhC. The organic gain medium consists of a guest-host system with tris(8-hydroxyquinolinato) aluminum (Alq3) as the hosting matrix doped with 4-(dicyanomethylene)-2–t-butyl-6(1,1,7,7–tetramethyljulolidyl–9-enyl)-4H-pyran (DCJTB) as a guest. A laser emission at 662 nm with a threshold of 9.3 μJ/cm2 is experimentally observed. The impact of the organic layer thickness on the laser threshold is studied.
In this work we report optical parametric generation in two dimensional, second order periodically poled lithium tantalate crystals. We are particularly interested by angular tuning of the conversion efficiency. We experimentally demonstrate that the generated intensity can be driven by the incidence angle of the pump beam. A double circle construction, different from the conventional Ewald sphere, is adopted to explain the quasi phase matching process.
In this work, we experimentally and theoretically investigate half-wavelength-thick Organic Light Emitting Diode
(OLED) in a vertical microcavity. The latter is based on a quarter-wavelength multilayer mirror on one side and a thin
aluminum semi-transparent layer on the other side. Two key parameters are studied for an optimal design of a cavity-
OLED: the organic layer and the metallic cathode thicknesses. The experimental study shows that a 627 nm peak
emission is obtained for a 127 nm-thick OLED hetero-structure. To achieve both desired optical transmission and
effective electron injection, we investigate the influence of the Al cathode thickness on the performance of the
microcavity devices. The experimental results are compared to those obtained by simulations of the emission spectra
using the transfer matrix method and taking into account the organic emitter position inside the cavity.
In this paper, we report the investigation of two-dimensional organic photonic crystal microcavity laser (2D OPCM). The
gain medium consists of an Alq3:DCJTB layer deposited on a planar Si3N4 photonic crystal microcavity. Both H2 and
L3 photonic crystal cavities are studied in terms of quality factor and the resonance wavelength by 3D FDTD
simulations. The structures are characterized under optical pumping by using a Nd:YAG frequency-tripled laser emitting
at 355 nm with a repetition frequency of 10 Hz and a pulse duration of 6 ns. A laser peak at 652 nm is observed for both
cavities with lasing thresholds of 0.014 nJ and 0.017 nJ for the H2 and the L3 cavities, respectively.
The optical properties of two-dimensional (2D) photonic crystal (PhC) slabs based on self-assembled monolayer of
dielectric microspheres are studied. The in-plane transmission spectra of 2D array of dielectric spheres with triangular
lattice are investigated using the finite-difference-time-domain (FDTD) method. The structures studied are monolayer of
dielectric spheres infiltrated with air ('opals') and air spheres infiltrated with dielectric material ('inverse opals'), with
glass substrate sustaining the monolayer of spheres. The transmission spectra are calculated for different values of
refractive index contrasts between the spheres and the infiltrated material and for different values of filling fractions
(compactness of the spheres). As the refractive index is varied, compact spheres are assumed; and as the filling fraction
is varied, the refractive index of the dielectric spheres or the dielectric matrix is fixed to be 2.5. For compact opal
structure on glass substrate, a narrow photonic band gap (PBG) is observed in the transmission spectra for dielectric
spheres with refractive index higher than around 1.9. When the refractive index is fixed at 2.5, the PBG is observed for
more compact spherical arrangement and disappears for more separated spheres. While for inverse opal structure on
glass substrate, using non-compact spheres enlarges the width of PBG which is not observed for compact spherical
arrangement. The application of the study is to realize organic PhC microcavity laser.
Through simulations based on the rate equations for diode lasers with filtered optical feedback, we show that in the Coherence Collapse regime a large variety of dynamics is predicted such as periodic and quasiperiodic oscillations and chaos. The control of the transition through these dynamical regimes is achieved through the filter parameters : the filter's spectral width and its central frequency.
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