SearcharxivSearch

arXiv · astro-ph/9801057

The Hubble Deep Field and the Disappearing Dwarf Galaxies

Abstract

Several independent lines of reasoning suggest that many of the very faint (B > 24) blue galaxies are low-mass objects that experienced a short epoch of star formation at redshifts 0.5 < z < 1 and have since faded into low luminosity, low surface brightness objects. Such a scenario, which arises naturally if star formation in dwarf galaxies is delayed by photoionisation due to the metagalactic UV radiation field, provides an attractive way to reconcile the Einstein-de Sitter cosmological model to the steeply rising galaxy counts observed at blue wavelengths. The Hubble Deep Field (HDF) images provide a stringent test of this model. We compare the Babul & Ferguson (1996) model to the data by constructing using simulated images and carrying out source detection and photometry for the simulations in the same way they were carried out for the real data. We compare the model predictions for the counts, sizes, and colours of galaxies observed in the HDF, and to the predictions from a low q_0 pure-luminosity-evolution (PLE) model. Both models fail to reproduce the observations. The low q_0 model predicts far more Lyman-break ``dropouts'' than are seen in the data. The fading dwarf model predicts too many remnants: faded dwarf galaxies in the redshift range 0.2 < z < 0.5 that should be detectable in the HDF as low-surface brightness red objects but are not seen. If fading dwarf galaxies are to reconcile the Einstein-de Sitter geometry to the counts, then the dwarf population must (a) form earlier than z ~ 1, with a higher initial luminosity; (b) have an initial-mass function more heavily weighted toward massive stars than the Salpeter IMF; or (c) expand much more than assumed during the supernova wind phase.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Henry C. Ferguson, Arif Babul. 1998-01-07. The Hubble Deep Field and the Disappearing Dwarf Galaxies. https://doi.org/10.1046/j.1365-8711.1998.01371.x

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Dark Energy is the Cosmological Quantum Vacuum Energy of Light Particles-The Axion and the Lightest Neutrino

We uncover the general mechanism producing the dark energy(DE). This is only based on well known quantum physics and cosmology. We show that the observed DE originates from the cosmological quantum vacuum of light particles which provides a continuous energy distribution able to reproduce the data. Bosons give positive contributions to the DE while fermions yield negative contributions. As usual in field theory, ultraviolet divergences are subtracted from the physical quantities. The subtractions respect the symmetries of the theory and we normalize the physical quantities to be zero for the Minkowski vacuum. The resulting finite contributions to the energy density and the pressure from the quantum vacuum grow as log a(t) where a(t) is the scale factor, while the particle contributions dilute as 1/a^3(t), as it must be for massive particles. The DE equation of state P = w(z)H turns to be w(z)<-1 with w(z) asymptotically reaching the value -1 from below.A scalar particle can produce the observed DE through its quantum cosmological vacuum provided:(i)its mass is of the order of 10^{-3} eV = 1 meV,(ii) it is very weakly coupled and (iii) it is stable on the time scale of the age of the universe. The axion vacuum thus appears as a natural candidate. The neutrino vacuum (especially the lightest mass eigenstate) can give negative contributions to the DE. We find that w(z=0) is slightly below -1 by an amount ranging from [-1.5 10^{-3}] to [-8 10^{-3}] and we predict the axion mass to be in the range between 4 and 5 meV. We find that the universe will expand in the future faster than the de Sitter universe, as an exponential in the square of the cosmic time. DE arises from the quantum vacua of light particles in FRW cosmological space time in an analogous way to the Casimir effect in Minkowski spacetime with non trivial boundaries.

astro-ph

Scaling of Black Hole Accretion Discs from Gamma-Ray Bursts and Black Hole X-Ray Binaries to Active Galactic Nuclei

I consider how physical processes scale over eight orders of magnitude in black hole mass, from stellar masses in gamma-ray bursts (GRB) and black-hole X-ray binaries (BHXRB) to supermassive active galactic nuclei (AGN). Accretion rates onto stellar mass black holes range over more than sixteen orders of magnitude, from the lower luminosity BHXRB to GRB. These enormous parameter ranges correspond to qualitative as well as quantitative differences in behavior. The fundamental questions involve the balance between nonequilibrium and thermalized plasmas. When energy fluxes exceed a critical value $\sim 10^{29}$ erg/cm$^2$s, as in GRB, a black-body equilibrium pair plasma forms. At the lower fluxes found in AGN, BHXRB and microquasars, accretion power electrodynamically accelerates a small number of very energetic particles, explaining their non-thermal spectra and the high energy gamma-ray emission of blazars. Ultra-high energy cosmic rays may be accelerated by massive black holes, otherwise undetectable, with very low thermal luminosities. New-born fast high-field pulsars may be in the black-body equilibrium regime, resembling SGR in permanent outburst. I also consider the question, significant for the acceleration of nonthermal particles in GRB outflows, of whether collisionless plasmas interpenetrate rather than forming hydrodynamic shocks, and propose this as an alternative to internal shock models of GRB. A new appendix attempts to explain why AGN are, proportionally, more efficient accelerators of energetic particles than stellar mass black holes.

astro-ph