Optical Characterization of OMT-Coupled TES Bolometers for LiteBIRD
A hybrid map-$C_\ell$ component separation method for primordial CMB $B$-mode searches
A novel approach to correcting $T_e$-based mass-metallicity relations
Two modes of LyC escape from bursty star formation: implications for [C II] deficits and the sources of reionization
Abstract:
We use the SPHINX20 cosmological radiation hydrodynamics simulation to study how Lyman continuum (LyC) photons escape from galaxies and the observational signatures of this escape. We define two classes of LyC leaker: Bursty Leakers and Remnant Leakers, based on their star formation rates (SFRs) that are averaged over 10 Myr (SFR10) or 100 Myr (SFR100). Both have fesc>20 per cent and experienced an extreme burst of star formation, but Bursty Leakers have SFR10 > SFR100, while Remnant Leakers have SFR10 < SFR100. The maximum SFRs in these bursts were typically ∼100 times greater than the SFR of the galaxy prior to the burst, a rare 2σ outlier among the general high-redshift galaxy population. Bursty Leakers are qualitatively similar to ionization-bounded nebulae with holes, exhibiting high ionization parameters and typical H II region gas densities. Remnant Leakers show properties of density-bounded nebulae, having normal ionization parameters but much lower H II region densities. Both types of leaker exhibit [C II]158μm deficits on the [C II]–SFR100 relation, while only Bursty Leakers show deficits when 10 is used. We predict that [C II] luminosity and SFR indicators such as Hα and M1500Å can be combined to identify both types of LyC leaker and the mode by which photons are escaping. These predictions can be tested with [C II] observations of known z = 3–4 LyC leakers. Finally, we show that leakers with fesc>20 per cent dominate the ionizing photon budget at z ≳ 7.5 but the contribution from galaxies with fesc<5 per cent becomes significant at the tail-end of reionization.
An active convective 4He heat switch
Abstract:
The design and experimental demonstration are reported of an active convective heat switch suitable for use at cryogenic temperatures. The switch is mechanically simple, relatively inexpensive, and requires no moving parts, instead being operated entirely using heaters. The working gas used is <4> He in a closed cycle and, as such, the switch requires no external gas connections. Closed conductances on the order of 50 mW/K have been demonstrated with residual open conductances on the order of 0.4 mW/K. Novel modelling is presented which shows excellent agreement with the experimental data and significant improvement over existing models.