TL;DR: Experimental and theoretical evidence is presented for the existence of quantum droplets in an electron–hole plasma created in a gallium arsenide quantum well by ultrashort optical pulses.
Abstract: Fast optical pulses create a plasma of electrons and holes in a semiconductor in which excitons (pairs of holes and electrons) and combinations of two excitons emerge; now a stable liquid-like droplet of electrons and holes has been detected and called a ‘dropleton’. Excitons, plasmons and phonons are some of the better known quasiparticles — exotic entities that act in some respects like ordinary particles. New types do not come along all that often but here is one — a fundamentally new many-body particle named the 'dropleton'. Mackillo Kira and colleagues have identified this new quantum entity, a quantum droplet created when four or more electrons and holes (electronic vacancies) form a tiny correlation bubble via the Coulomb attraction, in direct-gap semiconductors such as gallium arsenide. The cover illustrates the pair-correlation function g(r) of quantum droplets — the central peak of the correlation function shows that electrons and holes are likely to be co-located and the ripples show that otherwise they form regularly spaced shells. Interacting many-body systems are characterized by stable configurations of objects—ranging from elementary particles to cosmological formations1,2,3—that also act as building blocks for more complicated structures. It is often possible to incorporate interactions in theoretical treatments of crystalline solids by introducing suitable quasiparticles that have an effective mass, spin or charge4,5 which in turn affects the material’s conductivity, optical response or phase transitions2,6,7. Additional quasiparticle interactions may also create strongly correlated configurations yielding new macroscopic phenomena, such as the emergence of a Mott insulator8, superconductivity or the pseudogap phase of high-temperature superconductors9,10,11. In semiconductors, a conduction-band electron attracts a valence-band hole (electronic vacancy) to create a bound pair, known as an exciton12,13, which is yet another quasiparticle. Two excitons may also bind together to give molecules, often referred to as biexcitons14, and even polyexcitons may exist15,16. In indirect-gap semiconductors such as germanium or silicon, a thermodynamic phase transition may produce electron–hole droplets whose diameter can approach the micrometre range17,18. In direct-gap semiconductors such as gallium arsenide, the exciton lifetime is too short for such a thermodynamic process. Instead, different quasiparticle configurations are stabilized dominantly by many-body interactions, not by thermalization. The resulting non-equilibrium quantum kinetics is so complicated that stable aggregates containing three or more Coulomb-correlated electron–hole pairs remain mostly unexplored. Here we study such complex aggregates and identify a new stable configuration of charged particles that we call a quantum droplet. This configuration exists in a plasma and exhibits quantization owing to its small size. It is charge neutral and contains a small number of particles with a pair-correlation function that is characteristic of a liquid. We present experimental and theoretical evidence for the existence of quantum droplets in an electron–hole plasma created in a gallium arsenide quantum well by ultrashort optical pulses.
TL;DR: In this paper, the electron-hole two-stream instability in a quantum semiconductor plasma has been studied including electrons and holes quantum recoil effects, exchange-correlation potentials, and degenerate pressures of the plasma species.
TL;DR: In this article, the authors investigate the mechanism of quasiparticle poisoning in devices subjected to local quasipharm injection and find that poisoning is dominated by the propagation of pair-breaking phonons across the chip.
Abstract: Nonequilibrium quasiparticles represent a significant source of decoherence in superconducting quantum circuits Here we investigate the mechanism of quasiparticle poisoning in devices subjected to local quasiparticle injection We find that quasiparticle poisoning is dominated by the propagation of pair-breaking phonons across the chip We characterize the energy dependence of the time scale for quasiparticle poisoning Finally, we observe that incorporation of extensive normal metal quasiparticle traps leads to a more than order-of-magnitude reduction in quasiparticle loss for a given injected quasiparticle power
TL;DR: In this paper, a detailed account of the propagation of quasiparticles and phonons in bulk, superconducting lead is presented, together with a theoretical description of the pulse propagation characteristics in the diffusive regimes.
Abstract: We present a detailed account of our work on the propagation of quasiparticles and phonons in bulk, superconducting lead. Time-of-flight techniques combined with tunnel junction detection (for quasiparticle) and bolometer detection (for phonons) are used. A transition from quasiparticle diffusion (and ballistic phonon propagation) to diffusion in the combined gas of qasiparticles and phonons is observed as the temperature is increased. We give a theoretical description of the pulse propagation characteristics in the diffusive regimes. The theoretical line-shape fits to the data yield a measure of the quasiparticle recombination time and their number decay time as a function of temperature.
TL;DR: In this article, the authors used quasiparticle tunneling between two identical superconductors at voltages less than 2Δ to measure the superconducting energy gap Δ.