Prospects and Limitations of Transition Metal Dichalcogenide Laser Gain Materials.

Nanolasers operate with a minimal amount of active material and low losses. In this regime, single layers of transition-metal dichalcogenides (TMDs) are being investigated as next generation gain materials due to their high quantum efficiency. We provide results from microscopic gain calculations of highly excited TMD monolayers and specify requirements to achieve lasing with four commonly used TMD semiconductors. Our approach includes band-structure renormalizations due to excited carriers that trigger a direct-to-indirect band gap transition. As a consequence, we predict a rollover for the gain that limits the excitation regime where laser operation is possible. A parametrization of the peak gain is provided that is used in combination with a rate-equation theory to discuss consequences for experimentally accessible laser characteristics.

A few-emitter solid-state multi-exciton laser.

We report on non-conventional lasing in a photonic-crystal nanocavity that operates with only four solid-state quantum-dot emitters. In a comparison between microscopic theory and experiment, we demonstrate that irrespective of emitter detuning, lasing with [Formula: see text] is facilitated by means of emission from dense-lying multi-exciton states. In the spontaneous-emission regime we find signatures for radiative coupling between the quantum dots. The realization of different multi-exciton states at different excitation powers and the presence of electronic inter-emitter correlations are reflected in a pump-rate dependence of the ß-factor.

Observation of Exciton Redshift-Blueshift Crossover in Monolayer WS2.

We report a rare atom-like interaction between excitons in monolayer WS2, measured using ultrafast absorption spectroscopy. At increasing excitation density, the exciton resonance energy exhibits a pronounced redshift followed by an anomalous blueshift. Using both material-realistic computation and phenomenological modeling, we attribute this observation to plasma effects and an attraction-repulsion crossover of the exciton-exciton interaction that mimics the Lennard-Jones potential between atoms. Our experiment demonstrates a strong analogy between excitons and atoms with respect to interparticle interaction, which holds promise to pursue the predicted liquid and crystalline phases of excitons in two-dimensional materials.

Two-Dimensional Heterojunctions from Nonlocal Manipulations of the Interactions.

We propose to create lateral heterojunctions in two-dimensional materials based on nonlocal manipulations of the Coulomb interaction using structured dielectric environments. By means of ab initio calculations for MoS2 as well as generic semiconductor models, we show that the Coulomb interaction-induced self-energy corrections in real space are sufficiently nonlocal to be manipulated externally, but still local enough to induce spatially sharp interfaces within a single homogeneous monolayer to form heterojunctions. We find a type-II heterojunction band scheme promoted by a laterally structured dielectric environment, which exhibits a sharp band gap crossover within less than 5 unit cells.

Monolithically Integrated High-ß Nanowire Lasers on Silicon.

Reliable technologies for the monolithic integration of lasers onto silicon represent the holy grail for chip-level optical interconnects. In this context, nanowires (NWs) fabricated using III-V semiconductors are of strong interest since they can be grown site-selectively on silicon using conventional epitaxial approaches. Their unique one-dimensional structure and high refractive index naturally facilitate low loss optical waveguiding and optical recirculation in the active NW-core region. However, lasing from NWs on silicon has not been achieved to date, due to the poor modal reflectivity at the NW-silicon interface. We demonstrate how, by inserting a tailored dielectric interlayer at the NW-Si interface, low-threshold single mode lasing can be achieved in vertical-cavity GaAs-AlGaAs core-shell NW lasers on silicon as measured at low temperature. By exploring the output characteristics along a detection direction parallel to the NW-axis, we measure very high spontaneous emission factors comparable to nanocavity lasers (ß = 0.2) and achieve ultralow threshold pump energies ≤11 pJ/pulse. Analysis of the input-output characteristics of the NW lasers and the power dependence of the lasing emission line width demonstrate the potential for high pulsation rates ≥250 GHz. Such highly efficient nanolasers grown monolithically on silicon are highly promising for the realization of chip-level optical interconnects.

Efficient Excitonic Photoluminescence in Direct and Indirect Band Gap Monolayer MoS2.

We discuss the photoluminescence (PL) of semiconducting transition metal dichalcogenides on the basis of experiments and a microscopic theory. The latter connects ab initio calculations of the single-particle states and Coulomb matrix elements with a many-body description of optical emission spectra. For monolayer MoS2, we study the PL efficiency at the excitonic A and B transitions in terms of carrier populations in the band structure and provide a quantitative comparison to an (In)GaAs quantum well-structure. Suppression and enhancement of PL under biaxial strain is quantified in terms of changes in the local extrema of the conduction and valence bands. The large exciton binding energy in MoS2 enables two distinctly different excitation methods: above-band gap excitation and quasi-resonant excitation of excitonic resonances below the single-particle band gap. The latter case creates a nonequilibrium distribution of carriers predominantly in the K-valleys, which leads to strong emission from the A-exciton transition and a visible B-peak even if the band gap is indirect. For above-band gap excitation, we predict a strongly reduced emission intensity at comparable carrier densities and the absence of B-exciton emission. The results agree well with PL measurements performed on monolayer MoS2 at excitation wavelengths of 405 nm (above) and 532 nm (below the band gap).

Influence of excited carriers on the optical and electronic properties of MoS2.

We study the ground-state and finite-density optical response of molybdenum disulfide by solving the semiconductor Bloch equations, using ab initio band structures and Coulomb interaction matrix elements. Spectra for excited carrier densities up to 10(13) cm(-2) reveal a redshift of the excitonic ground-state absorption, whereas higher excitonic lines are found to disappear successively due to Coulomb-induced band gap shrinkage of more than 500 meV and binding-energy reduction. Strain-induced band variations lead to a redshift of the lowest exciton line by ∼110 meV/% and change the direct transition to indirect while maintaining the magnitude of the optical response.

Emission properties and photon statistics of a single quantum dot laser.

A theoretical description for a single quantum-dot emitter in a microcavity is developed.We analyze for increasing steady-state pump rate the transition from the strong-coupling regime with photon antibunching to the weak-coupling regime with coherent emission. It is demonstrated how Coulomb interaction of excited carriers and excitation-induced dephasing can strongly modify the emission properties. Our theoretical investigations are based on a direct solution of the Liouville-von Neumann equation for the coupled carrier-photon system. We include multiple carrier excitations in the quantum dot, their Coulomb interaction, as well as excitation-induced dephasing and screening. Similarities and differences to atomic systems are discussed and results in the regime of recent experiments are interpreted.

Direct observation of correlations between individual photon emission events of a microcavity laser.

Lasers are recognized for coherent light emission, the onset of which is reflected in a change in the photon statistics. For many years, attempts have been made to directly measure correlations in the individual photon emission events of semiconductor lasers. Previously, the temporal decay of these correlations below or at the lasing threshold was considerably faster than could be measured with the time resolution provided by the Hanbury Brown/Twiss measurement set-up used. Here we demonstrate a measurement technique using a streak camera that overcomes this limitation and provides a record of the arrival times of individual photons. This allows us to investigate the dynamical evolution of correlations between the individual photon emission events. We apply our studies to micropillar lasers with semiconductor quantum dots as the active material, operating in the regime of cavity quantum electrodynamics. For laser resonators with a low cavity quality factor, Q, a smooth transition from photon bunching to uncorrelated emission with increasing pumping is observed; for high-Q resonators, we see a non-monotonic dependence around the threshold where quantum light emission can occur. We identify regimes of dynamical anti-bunching of photons in agreement with the predictions of a microscopic theory that includes semiconductor-specific effects.

Photon statistics of semiconductor microcavity lasers.

We present measurements of first- and second-order coherence of quantum-dot micropillar lasers together with a semiconductor laser theory. Our results show a broad threshold region for the observed high-beta microcavities. The intensity jump is accompanied by both pronounced photon intensity fluctuations and strong coherence length changes. The investigations clearly visualize a smooth transition from spontaneous to predominantly stimulated emission which becomes harder to determine for high beta. In our theory, a microscopic approach is used to incorporate the semiconductor nature of quantum dots. The results are in agreement with the experimental intensity traces and the photon statistics measurements.

Renal response to infusion of dopamine precursors in anaesthetized rats.

In the present study the renal response to intravenous infusion of the catecholamine precursors L-dihydroxyphenylalanine (L-DOPA) or L-tyrosine was investigated in thiopentone sodium-anaesthetized Sprague-Dawley rats. Glomerular filtration rate (GFR) was assessed by renal clearance of inulin, urinary concentration of dopamine (U(DA)V) by HPLC and sodium excretion (U(Na)V) by flame photometry. We found that basal U(DA)V was 6.5 +/- 0.5 pmol/min per 100 g body weight (mean +/- SEM). Intravenous infusion of L-tyrosine at 0. 1-3.0 micromol/min dose dependently enhanced U(DA)V (17 +/- 3 to 144 +/- 14 pmol/min respectively) with higher doses of L-tyrosine resulting in no further increase in U(DA)V. Compared with L-tyrosine administration significantly lower doses of L-DOPA (0.07 to 35 nmol/min) caused increases in U(DA)V which were orders of magnitude higher (18 +/- 1 to 7800 +/- 470 pmol/min, respectively) and did not show saturation characteristics. GFR did not change in response to L-tyrosine or L-DOPA infusion. No variations in urinary flow rate or in U(Na)V could be observed which were significantly correlated to changes in U(DA)V. In contrast, intravenous infusion of dopamine at a dose of 6 nmol/min significantly increased GFR by 35 +/- 6.2% and urinary flow rate by over 2-fold. Immunohistochemistry with light microscopy revealed no tyrosine hydroxylase in the kidney. Therefore, dopamine synthesis in the tubular cells mainly depends on the renal supply of L-DOPA. The unchanged GFR and U(Na)V in spite of large variations of U(DA)V argue against the hypothesis that intratubular dopamine plays a functional role in the regulation of hemodynamics or sodium transport in the kidney. Renal dopamine excretion may rather represent an effective pathway for the elimination of catecholamine precursors from the plasma.

Characterization of the isolated rat flexor digitorum brevis for the study of skeletal muscle phosphorylase kinase phosphorylation.

The flexor digitorum brevis skeletal muscle, a nearly homogeneous fast-twitch oxidative glycolytic fiber type, has been examined for its suitability to explore the regulation of phosphorylase kinase by multisite phosphorylation. A characterization of the adrenergic response of glycogenolytic enzymes, together with the previous data on contractile properties (Carlsen, R. C., Larson, D. B., and Walsh, D. A. (1985) Can. J. Physiol. Pharm. 63, 958-965), has demonstrated that this muscle is stably maintained for the several hours necessary for phosphorylation studies. The phosphorylase kinase in this muscle is primarily the alpha' isozyme, suggesting that the alpha versus alpha' isozyme distribution in muscle is related more to oxidative capacity than to fiber contractile characteristics. Using this muscle system, beta-adrenergic activation of phosphorylase kinase was observed to occur with concomitant phosphorylation of both the alpha' and beta subunits, with the total in the alpha' subunit being approximately 3-fold greater. Similarly, deactivation, following initial adrenergic activation, occurred concomitantly with the dephosphorylation of the two subunits. These results are compatible with the conclusions drawn from previous studies of the isolated enzyme and of the enzyme in perfused rat cardiac muscle, that both alpha' (or alpha) and beta subunit phosphorylation regulate phosphorylase kinase activity.

Subunit phosphorylation and activation of skeletal muscle phosphorylase kinase by the cAMP-dependent protein kinase. Divalent metal ion, ATP, and protein concentration dependence.

This report provides a characterization of the effects of varying the concentrations of Mg2+, ATP, phosphorylase kinase, and the cAMP-dependent protein kinase on the activation and phosphorylation of phosphorylase kinase. The results show the following. (a) The Km for MgATP2- for the cAMP-dependent protein kinase-catalyzed phosphorylation is decreased by increasing Mg2+, probably as a consequence of decreasing the free ATP:MgATP2- ratio and increasing free Mg2+. (b) Whereas beta subunit phosphorylation of phosphorylase kinase plays a prominent role in determining its activity, alpha subunit phosphorylation can also modulate activity. (c) The phosphorylation of the alpha subunit, which occurs following the initial cAMP-dependent phosphorylation of the beta subunit, is catalyzed by the cAMP-dependent protein kinase and is not a consequence of EGTA-insensitive (or EGTA-sensitive) autophosphorylation occurring as a result of the enhanced phosphorylase kinase activity. (d) The relationship between subunit phosphorylation and phosphorylase kinase activation is complex and particularly dependent upon concentrations of cAMP-dependent protein kinase and phosphorylase kinase in the activation reaction. The data suggest the possibilities that the pathway of phospho-intermediates involved in the activation process probably varies with the activation conditions, that the efficacy of a specific site to be covalently modified is dependent upon the phosphorylation status of other sites, and that the effect of phosphorylation in regulating activity may also be dependent on the phosphorylation status of other sites. It is clear from the data that the activation process for phosphorylase kinase can be very complex, and it is possible that this complexity might have significant physiological ramifications.