536 research outputs found

    Auger recombination of dark excitons in WS2{\rm WS_2} and WSe2{\rm WSe_2} monolayers

    Full text link
    We propose a novel phonon assisted Auger process unique to the electronic band structure of monolayer transition metal dichalcogenides (TMDCs), which dominates the radiative recombination of ground state excitons in Tungsten based TMDCs. Using experimental and DFT computed values for the exciton energies, spin-orbit splittings, optical matrix element, and the Auger matrix elements, we find that the Auger process begins to dominate at carrier densities as low as 10910 cm210^{9-10}~{\rm cm^{-2}}, thus providing a plausible explanation for the low quantum efficiencies reported for these materials.Comment: 5 pages, 2 figure

    Four phases of angular-momentum buildup in high-z galaxies: from cosmic-web streams through an extended ring to disc and bulge

    Full text link
    We study the angular-momentum (AM) buildup in high-zz massive galaxies using high-resolution cosmological simulations. The AM originates in co-planar streams of cold gas and merging galaxies tracing cosmic-web filaments, and it undergoes four phases of evolution. (I) Outside the halo virial radius (Rv ⁣ ⁣100kpcR_{\rm v}\!\sim\!100\,{\rm kpc}), the elongated streams gain AM by tidal torques with a specific AM (sAM)  ⁣1.7\sim\!1.7 times the dark-matter (DM) spin due to the gas' higher quadrupole moment. This AM is expressed as stream impact parameters, from  ⁣0.3Rv\sim\!0.3R_{\rm v} to counter rotation. (II) In the outer halo, while the incoming DM mixes with the existing halo of lower sAM to a spin λdm ⁣ ⁣0.04\lambda_{\rm dm}\!\sim\!0.04, the cold streams transport the AM to the inner halo such that their spin in the halo is  ⁣3λdm\sim\!3\lambda_{\rm dm}. (III) Near pericenter, the streams dissipate into an irregular rotating ring extending to  ⁣0.3Rv\sim\!0.3R_{\rm v} and tilted relative to the inner disc. Torques exerted partly by the disc make the ring gas lose AM, spiral in, and settle into the disc within one orbit. The ring is observable with 30\% probability as a damped Lyman-α\alpha absorber. (IV) Within the disc, < ⁣0.1Rv<\!0.1R_{\rm v}, torques associated with violent disc instability drive AM out and baryons into a central bulge, while outflows remove low-spin gas, introducing certain sensitivity to feedback strength. Despite the different AM histories of gas and DM, the disc spin is comparable to the DM-halo spin. Counter rotation can strongly affect disc evolution.Comment: Resubmitted to MNRAS after responding to referee's comments. (27 pages, 20 figures

    Coplanar streams, pancakes and angular-momentum exchange in high-z disc galaxies

    Get PDF
    We study the feeding of massive galaxies at high redshift through streams from the cosmic web using the Mare Nostrum hydrocosmological simulation. Our statistical sample consists of 350 dark matter haloes of ≃1012 M⊙ at z= 2.5. We find that ∼70 per cent of the influx into the virial radius Rv is in narrow streams covering 10 per cent of the virial shell. On average 64 per cent of the stream influx is in one stream, and 95 per cent is in three dominant streams. The streams that feed a massive halo tend to lie in a plane that extends from half to a few Rv, hereafter ‘the stream plane' (SP). The streams are typically embedded in a thin sheet of low-entropy gas, a Zel'dovich pancake, which carries ∼20 per cent of the influx into Rv. The filaments-in-a-plane configuration about the massive haloes at the nodes of the cosmic web differs from the large-scale structure of the web where the filaments mark the intersections of slanted sheets. The SP is only weakly aligned with the angular momentum (AM) near Rv, consistent with the fact that typically 80 per cent of the AM is carried by one dominant stream. The galactic disc plane shows a weak tendency to be perpendicular to the large-scale SP, consistent with tidal-torque theory. Most interesting, the direction of the disc AM is only weakly correlated with the AM direction at Rv. This indicates a significant AM exchange at the interphase between streams and disc in the greater environment of the disc inside an ‘AM sphere' of radius ∼0.3Rv. The required large torques are expected based on the perturbed morphology and kinematics within this interaction sphere. This AM exchange may or may not require a major modification of the standard disc modelling based on AM conservation, depending on the extent to which the amplitude of the disc AM is affected, which is yet to be studie

    Fast relaxation of photo-excited carriers in 2-D transition metal dichalcogenides

    Get PDF
    We predict a fast relaxation of photo-excited carriers in monolayer transition metal dichalcogenides, which is mediated by the emission of longitudinal optical (LO) and homopolar (HP) phonons. By evaluating Born effective charges for MoS2, MoSe2, WS2, and WSe2, we find that, due to the polar coupling of electrons with LO phonons, and the HP phonons lattice deformation potential, the cooling times for hot electrons and holes from excitation energies of several hundred meV are at ps-scale

    Four phases of angular-momentum buildup in high-z galaxies: from cosmic-web streams through an extended ring to disc and bulge

    Get PDF
    We study the angular-momentum (AM) buildup in high-z massive galaxies using high-resolution cosmological simulations. The AM originates in co-planar streams of cold gas and merging galaxies tracing cosmic-web filaments, and it undergoes four phases of evolution. (I) Outside the halo virial radius (Rv∼100 kpc), the elongated streams gain AM by tidal torques with a specific AM (sAM) ∼1.7times the dark matter (DM) spin due to the gas' higher quadrupole moment. This AM is expressed as stream impact parameters, from ∼0.3Rv to counter rotation. (II) In the outer halo, while the incoming DM mixes with the existing halo of lower sAM to a spin λdm∼0.04, the cold streams transport the AM to the inner halo such that their spin in the halo is ∼3λdm. (III) Near pericentre, the streams dissipate into an irregular rotating ring extending to ∼0.3Rv and tilted relative to the inner disc. Torques exerted partly by the disc make the ring gas lose AM, spiral in, and settle into the disc within one orbit. The ring is observable with 30 per cent probability as a damped Lyman α absorber. (IV) Within the disc, <0.1Rv, torques associated with violent disc instability drive AM out and baryons into a central bulge, while outflows remove low-spin gas, introducing certain sensitivity to feedback strength. Despite the different AM histories of gas and DM, the disc spin is comparable to the DM-halo spin. Counter rotation can strongly affect disc evolutio

    Collaborative Housing in Scandinavia and Western Europe

    Full text link
    Special Studies Experience, Summer 2011 -- Oslo, Norway; Stockholm, Sweden; Utrecht, Rotterdam and Delft, Netherlands; Rennes and Angers, France; London, Englandhttp://deepblue.lib.umich.edu/bitstream/2027.42/110143/1/Poster_Danovich.pd

    On the effect of cosmological inflow on turbulence and instability in galactic discs

    Full text link
    We analyse the evolution of turbulence and gravitational instability of a galactic disc in a quasi-steady state governed by cosmological inflow. We focus on the possibility that the coupling between the in-streaming gas and the disc is maximal, e.g., via dense clumps, and ask whether the streams could be the driver of turbulence in an unstable disc with a Toomre parameter Q~1. Our fiducial model assumes an efficiency of ~0.5 per dynamical time for the decay of turbulence energy, and ~0.02 for each of the processes that deplete the disc gas, i.e., star formation, outflow, and inflow within the disc into a central bulge. In this case, the in-streaming drives a ratio of turbulent to rotation velocity sigma/V~0.2-0.3, which at z~2 induces an instability with Q~1, both as observed. However, in conflict with observations, this model predicts that sigma/V remains constant with time, independent of the cosmological accretion rate, because mass and turbulence have the same external source. Such strongly coupled cosmological inflow tends to stabilize the disc at low z, with Q ~ a few, which may be consistent with observations. The instability could instead be maintained for longer, with a properly declining sigma/V, if it is self-regulated to oscillations about Q~1 by a duty cycle for disc depletion. However, the 'off' phases of this duty cycle become long at low z, which may be hard to reconcile with observations. Alternatively, the coupling between the in-streaming gas and the disc may weaken in time, reflecting an evolving nature of the accretion. If, instead, that coupling is weak at all times, the likely energy source for self-regulated stirring up of the turbulence is the inflow within the disc down the potential gradient (studied in a companion paper).Comment: 14 pages, 1 table. Accepted for publication in Monthly Notices of the Royal Astronomical Society. Minor changes to match accepted versio

    Gas Accretion in Star-Forming Galaxies

    Full text link
    Cold-mode gas accretion onto galaxies is a direct prediction of LCDM simulations and provides galaxies with fuel that allows them to continue to form stars over the lifetime of the Universe. Given its dramatic influence on a galaxy's gas reservoir, gas accretion has to be largely responsible for how galaxies form and evolve. Therefore, given the importance of gas accretion, it is necessary to observe and quantify how these gas flows affect galaxy evolution. However, observational data have yet to conclusively show that gas accretion ubiquitously occurs at any epoch. Directly detecting gas accretion is a challenging endeavor and we now have obtained a significant amount of observational evidence to support it. This chapter reviews the current observational evidence of gas accretion onto star-forming galaxies.Comment: Invited review to appear in Gas Accretion onto Galaxies, Astrophysics and Space Science Library, eds. A. J. Fox & R. Dav\'e, to be published by Springer. This chapter includes 22 pages with 7 Figure

    Dissociation of two-dimensional excitons in monolayer WSe<sub>2</sub>

    Get PDF
    In two-dimensional semiconductors excitons are strongly bound, suppressing the creation of free carriers. Here, the authors investigate the main exciton dissociation pathway in p-n junctions of monolayer WSe2 by means of time and spectrally resolved photocurrent measurements
    corecore