Markus Führer

Demonstration of Photon Coupling in Dual Multiple-Quantum-Well Solar Cells

Multiple-quantum-well (MQW) top cells can enhance the performance of multi-junction solar cells since the absorption edge of top and middle subcells can be tuned with the MQWs to maximize the efficiency. The radiative dominance of MQW top cells can enhance photon coupling, which can potentially reduce the spectral sensitivity of the device and, thus, raise the energy harvest. We present experimental results on photon coupling in dual-junction cells with GaInP top cells containing GaInAsP quantum wells along with theoretical calculation based on a detailed balance model. It is observed that at high concentration, approximately 50% of the dark current of an MQW top cell is transferred to the photocurrent of the cell in the bottom, which is much higher than any previously reported values.

Experimental demonstration of hot-carrier photo-current in an InGaAs quantum well solar cell

An unambiguous observation of hot-carrier photocurrent from an InGaAs single quantum well solar cell is reported. Simultaneous photo-current and photoluminescence measurements were performed for incident power density 0.04–3 kW cm−2, lattice temperature 10 K, and forward bias 1.2 V. An order of magnitude photocurrent increase was observed for non-equilibrium hot-carrier temperatures >35 K. This photocurrent activation temperature is consistent with that of equilibrium carriers in a lattice at elevated temperature. The observed hot-carrier photo-current is extracted from the well over an energy selective GaAs barrier, thus integrating two essential components of a hot-carrier solar cell: a hot-carrier absorber and an energy selective contact.

Simulation of novel InAlAsSb solar cells

This work uses simulations to predict the performance of InAlAsSb solar cells for use as the top cell of triple junction cells lattice matched to InP. The InP-based material system has the potential to achieve extremely high efficiencies due the availability of lattice matched materials close to the ideal bandgaps for solar energy conversion. The band-parameters, optical properties and minority carrier transport properties are modeled based on literature data for the InAlAsSb quaternary, and an analytical drift-diffusion model is used to realistically predict the solar cell performance.

Hot carrier dynamics in InGaAs/GaAsP quantum well solar cells

A hot carrier solar cell is a device with a steady-state carrier population which is described by a higher temperature than the surrounding lattice. Thermalisation loss is reduced in such a device, offering the potential for substantial efficiency advantages over single junction solar cells. Despite clear efficiency benefits no real world device has ever been developed, partly because of the difficulty of developing a suitable absorber material with sufficiently limited interaction between excited carriers and lattice phonons. This study evaluates the suitability of strain balanced InGaAs/GaAsP quantum well structures as hot carrier absorbers. Ultrafast time resolved photoluminescence (TRPL) spectroscopy measurements are presented which demonstrate hot carrier populations beyond 2ns after excitation in a deep well sample. Continuous wave photoluminescence (CWPL) spectroscopy was used to compare steady-state carrier populations in deep and shallow well samples. In both cases hot distributions were observed under photon flux density greater than 10,000 Suns equivalent. Increasing incident photon flux density was shown to increase carrier distribution temperature, suggesting that the hot carrier effect might be enhanced in a multiple QW structure with better well region absorption. It was also found that the deep well sample achieved significantly higher carrier distribution temperatures than the shallow well sample, demonstrating that increasing quantum confinement further inhibits thermalisation pathways. This study provides a guide to the development of hot carrier solar cells as it indicates deep multiple quantum well samples might exhibit an enhanced hot carrier effect. Strain Balanced InGaAs/GaAsP is a particularly suitable material system for growing this type of structure, making it an exciting prospect for the development of a hot carrier absorber.

Enhanced Hot-Carrier Effects in InAlAs/InGaAs Quantum Wells

Hot-carrier solar cells require absorber materials with restricted carrier thermalization pathways, in order to slow the rate of heat energy dissipation from the carrier population to the lattice, relative to the rate of carrier extraction. Absorber suitability can be characterized in terms of carrier thermalization coefficient (Q). Materials with lower Q generate steady-state hot-carrier populations at lower levels of incident solar power and, therefore, are better able to perform as hot-carrier absorbers. In this study, we evaluate Q = 2.5±0.2 W·K-1 · cm-2 for a In0.52 AlAs/In0.53 GaAs single-quantum-well(QW) heterostructure using photoluminescence spectroscopy. This is the lowest experimentally determined Q value for any material system studied to date. Hot-carrier solar cell simulations, using this material as an absorber yield efficiency ~39% at 2000X, which corresponds to a >5% enhancement over an equivalent single-junction thermal equilibrium device.

InGaAs/GaAsP strain balanced multi-quantum wires grown on misoriented GaAs substrates for high efficiency solar cells

Quantum wires (QWRs) form naturally when growing strain balanced InGaAs/GaAsP multi-quantum wells (MQW) on GaAs [100] 6° misoriented substrates under the usual growth conditions. The presence of wires instead of wells could have several unexpected consequences for the performance of the MQW solar cells, both positive and negative, that need to be assessed to achieve high conversion efficiencies. In this letter, we study QWR properties from the point of view of their performance as solar cells by means of transmission electron microscopy, time resolved photoluminescence and external quantum efficiency (EQE) using polarised light. We find that these QWRs have longer lifetimes than nominally identical QWs grown on exact [100] GaAs substrates, of up to 1 μs, at any level of illumination. We attribute this effect to an asymmetric carrier escape from the nanostructures leading to a strong 1D-photo-charging, keeping electrons confined along the wire and holes in the barriers. In principle, these extended lifetim...

Controlling radiative loss in quantum well solar cells

The inclusion of quantum well layers in a solar cell provides a means for extending the absorption and therefore increasing the photocurrent of the cell. In 2009, a single-junction GaAsP/InGaAs quantum well solar cell attained a peak efficiency of 28.3% under solar concentration. Since then InGaP/MQW/Ge quantum well devices have attained efficiencies in excess of 40% under concentration and over 30% under AM0. The principle motivation for incorporating a quantum well stack into a multi-junction solar cell is to increase the photocurrent delivered by the middle junction over the conventional In0.01GaAs bulk junction. This enables additional current to flow through the top and middle cells, resulting in a sharp rise in efficiency. However, quantum wells also provide some freedom to manipulate the radiative recombination in the quantum well solar cell. We show that under radiatively dominated, anisotropic emission, strong radiative coupling between sub-cells takes place, resulting in a multi-junction solar cell that is tolerant to daily and seasonal changes to the solar spectrum.

Practical Limits of Multijunction Solar Cell Performance Enhancement From Radiative Coupling Considering Realistic Spectral Conditions

III-V multijunction solar cells (MJSCs) operate close to the radiative limit under solar concentration. In this regime, radiative losses from the semiconductor material in one junction of the solar cell can be absorbed by a subsequent junction, thereby transferring charge from one subcell to another. Under blue-rich solar spectra, radiative coupling can improve the electrical performance by lifting constraints imposed by a series connection of subcells. We calculate the practical limit of performance enhancement due to the radiative coupling effect for MJSCs under a wide range of atmospheric conditions encountered in potential sites for concentrator photovoltaic systems. Three-junction and four-junction solar cells with current matched and current mismatched designs under the AM1.5D spectrum were considered. Under realistic atmospheric conditions, the relative enhancement to power due to radiative coupling is found to be 1% or less for current-matched triple-junction solar cells. Enhancement of up to 21% can be expected for noncurrent-matched quad-junction devices. The energy yield improvement over an annual period is shown to be up to 5% for the best combinations of devices and sites.

Drift-diffusion modeling of InP-based triple junction solar cells.

In this work, we use an analytical drift-diffusion model, coupled with detailed carrier transport and minority carrier lifetime estimates, to make realistic predictions of the conversion efficiency of InP-based triple junction cells. We evaluate the possible strategies for overcoming the problematic top cell for the triple junction, and make comparisons of the more realistic charge transport model with incumbent technologies grown on Ge or GaAs substrates.

GaNAsSb 1-eV solar cells for use in lattice-matched multi-junction architectures

Photovoltaic devices made from a dilute nitride material, GaAsNSb, with band-gap close to 1eV have been developed and characterised. Homojunction devices of n-on-p and p-on-n type as well as an n-on-p GaAs/GaNAsSb heterojunction have been grown by molecular beam epitaxy. Optical and electrical characteristics are reported and a one-dimensional drift-diffusion model of internal quantum efficiency is used to estimate minority carrier diffusion lengths. The GaAs/GaNAsSb heterostructure produced AM1.5G short-circuit current of 23.6 mA/cm2, open-circuit voltage of 0.44V and fill factor of 67%. The model suggests that this performance is limited by both diffusion length and surface recombination.