Using time‐resolved photoluminescence spectroscopy on GaInN/GaN multiple quantum well structures, we analyze the radiative and nonradiative processes contributing to the “green gap” in GaN‐based light emitting devices. We observe that it is only partly caused by a reduced oscillator strength due to the Quantum Confined Stark Effect (QCSE) which becomes stronger with increasing indium concentration and well width. As the dominant effect we observe a reduction of nonradiative lifetimes when the indium concentration is increased. For higher indium concentrations, we find an additional nonradiative recombination path that might be attributed to an increased generation of defects like misfit dislocations, nitrogen vacancies and/or indium clusters within the optically active region. (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)

The origin of the green gap for GaInN/GaN quantum wells is investigated via temperature-dependent time-resolved photoluminescence spectroscopy. A strong correlation between nonradiative lifetimes and total strain energy is observed, although the wells are almost fully strained. We discuss this observation in terms of nonradiative recombination at defects which contribute to a beginning partial relaxation. The formation energy of a defect is likely reduced by the amount of its released strain energy. We therefore expect an exponential dependence of the defect density on this released strain energy. Our measured nonradiative lifetimes are consistent with a cumulative strain driven generation of defects.

Nonradiative loss processes are a major concern in nitride-based light emitting devices. Utilizing optical gain measurements on GaInN/GaN/AlGaN laser structures, we have studied the dependence of the total recombination rate on excess carrier density, up to rather high densities. From a detailed quantitative analysis, we find a room-temperature Auger recombination coefficient of 1.8 ± 0.2 × 10−31 cm6/s in the bandgap range 2.5 − 3.1 eV, considerably lower than previous experimental estimates. Thus, Auger recombination is expected to be significant for laser diodes, while it is not likely to be a major factor for the droop observed in light-emitting diodes.

We have studied the growth of GaInN/GaN quantum wells on various polar, nonpolar and semipolar planes. From a detailed x-ray diffraction analysis, we derive the strain state and the composition of the quantum wells. The optical emission energy is obtained from photoluminescence spectra and modelled taking into account the deformation potentials and the Stark shifts. Both x-ray and optical data consistently show that indium incorporation is identical on the polar, nonpolar and semipolar planes within the experimental uncertainty.

The optical gain of single quantum well laser structures on semipolar (1122)-GaN in dependence of the optical polarization and the resonator orientation has been studied by variable stripe length method. The c'-[1123] resonator shows maximum gain in TE mode, followed by the m-[1100]-resonator with extraordinary polarization. The anisotropic gain behaviour is explained by valence sub-band ordering and birefringence of the wurtzite crystal, resulting in a modification of the transition matrix element for stimulated emission. Measurements are accompanied by 6 x 6 k . p band structure calculations and gain analysis

Introduction:The Cassini mission revealed gas plumes associated with surface features called "tiger stripes" at the south pole of Saturn's moon Enceladus. The composition of plume particles and local cryovolcanism suggested as a possible cause for the activity are typically considered in the context of hydrothermal circulation in the rocky core within a differentiated core-ocean-ice crust structure. We model the internal evolution and differentiation of Enceladus heated by radioactive nuclides and tidal dissipation. Calculating the core formation, we investigate its compaction by modeling the evolution of porosity, thereby varying the rock rheology based on different assumptions on the composition, such as grain size, creep activation energy, degree of hydration, and oxygen fugacity. We obtained "successful" final structures with a core radius of 185-205 km, a porous core layer of 4-70 km, an ocean of ≈10-27 km, and an ice crust layer of ≈30-40 km, that are largely consistent with the current estimates for Enceladus. By fitting the model results to these observations, we determined an accretion time of 1.3-2.3 Ma after Ca-Al-rich inclusions for Enceladus. Our models produce a porous outer core for wet and dry olivine rock rheologies supporting the hypothesis of hydrothermal circulation of oceanic water in the core. No porosity is retained for an antigorite rheology, implying that the core of Enceladus is not dominated by this mineral.Model: For model calculations we adapted a 1D thermal evolution code used previously for Ceres [1] to Enceladus. The updated model [2] calculates heating by the short-and long-lived radioactive isotopes, latent heat, compaction of initially porous rock, continuous water-rock separation, redistribution of radionuclides, tidal heating, and convection in the water ocean.A crucial aspect of the model is the calculation of the melt porosity in the rocky core during its formation and subsequent evolution (i.e., the change of the pore space filled with water). The core forms by the redistribution of water and silicate rock particles in a two-phase system after melting of ice. The melting front proceeds from the center upward. The rock particles in the H 2 O-rich layer below the melting front settle and form an agglomerate with water-filled pores, while atop that a water layer forms. This agglomerate is a high-porosity core that grows along with the water layer while the melting front moves further upward. Deformation of the core can lead to a reduction of the

The efficiency droop in nitride LEDs is currently attributed to either carrier-density-dependent nonradiative recombination or to carrier leakage, both being discussed in terms of a single-particle picture. Our time-resolved photoluminescence results show that the radiative lifetime is independent of carrier density, while the nonradiative lifetime scales with the inverse of the carrier density. This can not be understood in a single-particle model. By means of a many-particle theory approach we obtain a consistent picture with both radiative and Auger recombination enhanced by excitonic electron-hole correlation. In the high carrier density limit single-particle radiative and Auger recombination are recovered.

<p><strong>Introduction:</strong> The Cassini mission revealed gas plumes at the south pole of Enceladus that are considered in the context of hydrothermal circulation in the rocky core. We model the internal evolution and differentiation of Enceladus heated by radioactive nuclides and tidal dissipation and investigate core compaction by modeling the evolution of porosity, thereby varying the rock rheology based on different assumptions on the composition.</p> <p><strong>Model:</strong> The model<sup>[2]</sup> calculates heating by short- and long-lived radionuclides, latent heat, compaction of porous rock, continuous water-rock separation, redistribution of radionuclides, tidal heating, and water ocean convection. A crucial aspect is the calculation of the core porosity. The core forms by the redistribution of water and silicate particles in a two-phase system after melting of ice. An initial particle agglomerate with interstitial water grows along with an overlying water layer during Enceladus' bottom-up melting. Deformation of the core can lead to a reduction of the pores. The water displaced from them supplies the water layer, while the rock is displaced downward according to the evolution of the porosity. With time it can deform further by creep processes on a geologic timescale. This is modeled by calculating the evolution of the porosity from the change of the strain rate. Here, we use the creep law from [3] that can describe diffusion creep of both “dry” (models A1-A4) and “wet” (models B1-B4) olivine for different values of water fugacity. For a phyllosilicate-rich composition (models C1-C2) supported by plume and E-ring spectral analyses<sup>[4]</sup>, we use the creep law from [5].</p> <p><strong>Results:</strong> Figure 1 shows the evolution of the structural layers over 4,5 Ga for the model A2 (accretion time of 1,7 Ma), representing successful calculations with the dry olivine rheology. A strong initial temperature increase leads to the onset of melting. The ocean formation starts at ≈3 Ma, with a significant differentiation phase from ≈4 Ma resulting in the formation of an ocean atop a core, finalized by ≈5 Ma after CAIs. During this process, compacting proto-core squeezes a part of the interstitial water through the porous rock into the water layer. The radionuclides are concentrated in the central part of the moon, bringing the central temperature to ≈800 K.</p> <p><img src="data:image/png;base64, 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