150 research outputs found
Diverse Structural Evolution at z > 1 in Cosmologically Simulated Galaxies
From mock Hubble Space Telescope images, we quantify non-parametric
statistics of galaxy morphology, thereby predicting the emergence of
relationships among stellar mass, star formation, and observed rest-frame
optical structure at 1 < z < 3. We measure automated diagnostics of galaxy
morphology in cosmological simulations of the formation of 22 central galaxies
with 9.3 < log10 M_*/M_sun < 10.7. These high-spatial-resolution zoom-in
calculations enable accurate modeling of the rest-frame UV and optical
morphology. Even with small numbers of galaxies, we find that structural
evolution is neither universal nor monotonic: galaxy interactions can trigger
either bulge or disc formation, and optically bulge-dominated galaxies at this
mass may not remain so forever. Simulated galaxies with M_* > 10^10 M_sun
contain relatively more disc-dominated light profiles than those with lower
mass, reflecting significant disc brightening in some haloes at 1 < z < 2. By
this epoch, simulated galaxies with specific star formation rates below 10^-9.7
yr^-1 are more likely than normal star-formers to have a broader mix of
structural types, especially at M_* > 10^10 M_sun. We analyze a cosmological
major merger at z ~ 1.5 and find that the newly proposed MID morphology
diagnostics trace later merger stages while G-M20 trace earlier ones. MID is
sensitive also to clumpy star-forming discs. The observability time of typical
MID-enhanced events in our simulation sample is less than 100 Myr. A larger
sample of cosmological assembly histories may be required to calibrate such
diagnostics in the face of their sensitivity to viewing angle, segmentation
algorithm, and various phenomena such as clumpy star formation and minor
mergers.Comment: 23 pages, 16 figures, MNRAS accepted versio
Cotunneling through quantum dot with even number of electrons
We study an influence of a finite magnetic field on a small spin-degenerate
quantum dot with even number of electrons, attached to metallic leads. It is
shown that, under certain conditions, the low energy physics of the system can
be described by the S=1/2 antiferromagnetic Kondo model.Comment: Contribution to LT-22; to be published in Physica
Cosmological Implications of Lyman-Break Galaxy Clustering
We review our analysis of the clustering properties of ``Lyman-break''
galaxies (LBGs) at redshift z~3, previously discussed in Wechsler et al (1998).
We examine the likelihood of spikes found by Steidel et al (1998) in the
redshift distribution of LBGs, within a suite of models for the evolution of
structure in the Universe. Using high-resolution dissipationless N-body
simulations, we analyze deep pencil-beam surveys from these models in the same
way that they are actually observed, identifying LBGs with the most massive
dark matter halos. We find that all the models (with SCDM as a marginal
exception) have a substantial probability of producing spikes similar to those
observed, because the massive halos are much more clumped than the underlying
matter -- i.e., they are biased. Therefore, the likelihood of such a spike is
not a good discriminator among these models. The LBG correlation functions are
less steep than galaxies today (gamma~1.4), but show similar or slightly longer
correlation lengths. We have extened this analysis and include a preliminary
comparison to the new data presented in Adelberger et al (1998). We also
discuss work in progress, in which we use semi-analytic models to identify
Lyman-break galaxies within dark-matter halos.Comment: 4 pages, 2 figures, Latex, uses aipproc.sty; to appear in the
proceedings of the 9th Annual October Maryland Astrophysics Conference,
"After the Dark Ages: When the Galaxies Were Young (the Universe at 2<z<5)
Equilibrium Current and Orbital Magnetization in a Quantum Hall Fluid
We present a general theory for the equilibrium current distribution in an
interacting two-dimensional electron gas subjected to a perpendicular magnetic
field, and confined by a potential that varies slowly on the scale of the
magnetic length. The distribution is found to consist of strips or channels of
current, which alternate in direction, and which have universal integrated
strength.Comment: 13 pages, Revtex, to appear in the proceedings of the "Workshop on
Novel Physics in Low-Dimensional Electron Systems" held in Madra
Wet Compaction to a Blue Nugget: a Critical Phase in Galaxy Evolution
We utilize high-resolution cosmological simulations to reveal that
high-redshift galaxies tend to undergo a robust `wet compaction' event when
near a `golden' stellar mass of . This is a gaseous
shrinkage to a compact star-forming phase, a `blue nugget' (BN), followed by
central quenching of star formation to a compact passive stellar bulge, a `red
nugget' (RN), and a buildup of an extended gaseous disc and ring. Such nuggets
are observed at cosmic noon and seed today's early-type galaxies. The
compaction is triggered by a drastic loss of angular momentum due to, e.g., wet
mergers, counter-rotating cold streams, or violent disc instability. The BN
phase marks drastic transitions in the galaxy structural, compositional and
kinematic properties. The transitions are from star-forming to quenched
inside-out, from diffuse to compact with an extended disc-ring and a stellar
envelope, from dark matter to baryon central dominance, from prolate to oblate
stellar shape, from pressure to rotation support, from low to high metallicity,
and from supernova to AGN feedback. The central black hole growth, first
suppressed by supernova feedback when below the golden mass, is boosted by the
compaction, and the black hole keeps growing once the halo is massive enough to
lock in the supernova ejecta.Comment: 33 pages, 26 figures in the main body (49 pages, 45 figures including
appendix
Dependence of Galaxy Quenching on Halo Mass and Distance from its Centre
We study the dependence of star-formation quenching on galaxy mass and
environment, in the SDSS (z~0.1) and the AEGIS (z~1). It is crucial that we
define quenching by low star-formation rate rather than by red colour, given
that one third of the red galaxies are star forming. We address stellar mass
M*, halo mass Mh, density over the nearest N neighbours deltaN, and distance to
the halo centre D. The fraction of quenched galaxies appears more strongly
correlated with Mh at fixed M* than with M* at fixed Mh, while for satellites
quenching also depends on D. We present the M*-Mh relation for centrals at z~1.
At z~1, the dependence of quenching on M* at fixed Mh is somewhat more
pronounced than at z~0, but the quenched fraction is low (10%) and the haloes
are less massive. For satellites, M*-dependent quenching is noticeable at high
D, suggesting a quenching dependence on sub-halo mass for recently captured
satellites. At small D, where satellites likely fell in more than a few Gyr
ago, quenching strongly depends on Mh, and not on M*. The Mh-dependence of
quenching is consistent with theoretical wisdom where virial shock heating in
massive haloes shuts down accretion and triggers ram-pressure stripping,
causing quenching. The interpretation of deltaN is complicated by the fact that
it depends on the number of observed group members compared to N, motivating
the use of D as a better measure of local environment.Comment: 23 pages, 13 figures, accepted by MNRA
Implications of Spikes in the Redshift Distribution of Galaxies
We address the high peaks found by Steidel et al (1997) in the redshift
distribution of ``Lyman-break'' objects (LBOs) at redshift z~3. The highest
spike represents a relative overdensity of 2.6 in the distribution of LBOs in
pixels of comoving size ~10Mpc/h. We examine the likelihood of such a spike in
the redshift distribution within a suite of models for the evolution of
structure in the Universe, including models with Omega=1 (SCDM and CHDM) and
with Omega=0.4-0.5 (LCDM and OCDM). Using high-resolution dissipationless
N-body simulations, we analyze deep pencil-beam surveys from these models in
the same way that they are actually observed, identifying LBOs with the most
massive dark matter halos. We find that all the models (with SCDM as a marginal
exception) have a substantial probability of producing spikes similar to those
observed, because the massive halos are much more clumped than the underlying
matter -- i.e., they are biased. Therefore, the likelihood of such a spike is
not a good discriminator among these models. We find in these models that the
mean biasing parameter b of LBOs with respect to dark matter varies within a
range b ~2-5 on a scale of ~10Mpc/h. We also compute the two-body correlation
functions of LBOs predicted in these models. The LBO correlation functions are
less steep than galaxies today (gamma ~1.4), but show similar or slightly
longer correlation lengths.Comment: 12 pages, 7 EPS inlined figures, 1 inlined table, LaTex + emulateapj,
multicol and graphics macro packages. Accepted for publication in the ApJ.
Revised version includes new appendix, table, updated references. A version
with higher quality inlined figures is available at
http://fozzie.gsfc.nasa.gov/wgpbd97/spikes.htm
Current-Carrying Ground States in Mesoscopic and Macroscopic Systems
We extend a theorem of Bloch, which concerns the net orbital current carried
by an interacting electron system in equilibrium, to include mesoscopic
effects. We obtain a rigorous upper bound to the allowed ground-state current
in a ring or disc, for an interacting electron system in the presence of static
but otherwise arbitrary electric and magnetic fields. We also investigate the
effects of spin-orbit and current-current interactions on the upper bound.
Current-current interactions, caused by the magnetic field produced at a point
r by a moving electron at r, are found to reduce the upper bound by an amount
that is determined by the self-inductance of the system. A solvable model of an
electron system that includes current-current interactions is shown to realize
our upper bound, and the upper bound is compared with measurements of the
persistent current in a single ring.Comment: 7 pager, Revtex, 1 figure available from [email protected]
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