3,537 research outputs found
H-alpha features with hot onsets. I. Ellerman bombs
Ellerman bombs are transient brightenings of the wings of the Balmer lines
that uniquely mark reconnection in the solar photosphere. They are also bright
in strong Ca II and ultraviolet lines and in ultraviolet continua, but they are
not visible in the optical continuum and the Na I D and Mg I b lines. These
discordant visibilities invalidate all published Ellerman bomb modeling. I
argue that the assumption of Saha-Boltzmann lower-level populations is
informative to estimate bomb-onset opacities for these diverse diagnostics,
even and especially for H-alpha, and employ such estimates to gauge the
visibilities of Ellerman bomb onsets in all of them. They constrain Ellerman
bomb formation to temperatures 10,000 - 20,000 K and hydrogen densities around
10^15 cm^-3. Similar arguments likely hold for H-alpha visibility in other
transient phenomena with hot and dense onsets.Comment: Accepted by Astronomy & Astrophysic
Radial Velocity Jitter in Stars from the California and Carnegie Planet Search at Keck Observatory
I present an empirical model for predicting a star's radial velocity jitter
from its B-V color, activity level, and absolute magnitude. This model is based
on observations of 450 well- observed stars from Keck Observatory for the
California and Carnegie Planet Search Program. The model includes noise from
both astrophysical sources and systematic errors, and describes jitter as
generally increasing with a star's activity and height above the main sequence.Comment: 16 pages, 7 figures, PASP in pres
Non-equilibrium hydrogen ionization in 2D simulations of the solar atmosphere
The ionization of hydrogen in the solar chromosphere and transition region
does not obey LTE or instantaneous statistical equilibrium because the
timescale is long compared with important hydrodynamical timescales, especially
of magneto-acoustic shocks. We implement an algorithm to compute
non-equilibrium hydrogen ionization and its coupling into the MHD equations
within an existing radiation MHD code, and perform a two-dimensional simulation
of the solar atmosphere from the convection zone to the corona. Analysis of the
simulation results and comparison to a companion simulation assuming LTE shows
that: a) Non-equilibrium computation delivers much smaller variations of the
chromospheric hydrogen ionization than for LTE. The ionization is smaller
within shocks but subsequently remains high in the cool intershock phases. As a
result, the chromospheric temperature variations are much larger than for LTE
because in non-equilibrium, hydrogen ionization is a less effective internal
energy buffer. The actual shock temperatures are therefore higher and the
intershock temperatures lower. b) The chromospheric populations of the hydrogen
n = 2 level, which governs the opacity of Halpha, are coupled to the ion
populations. They are set by the high temperature in shocks and subsequently
remain high in the cool intershock phases. c) The temperature structure and the
hydrogen level populations differ much between the chromosphere above
photospheric magnetic elements and above quiet internetwork. d) The hydrogen n
= 2 population and column density are persistently high in dynamic fibrils,
suggesting that these obtain their visibility from being optically thick in
Halpha also at low temperature.Comment: 10 pages, 4 figure
The Quiet-Sun Photosphere and Chromosphere
The overall structure and the fine structure of the solar photosphere outside
active regions are largely understood, except possibly important roles of a
turbulent near-surface dynamo at its bottom, internal gravity waves at its top,
and small-scale vorticity. Classical 1D static radiation-escape modelling has
been replaced by 3D time-dependent MHD simulations that come closer to reality.
The solar chromosphere, in contrast, remains ill-understood although its
pivotal role in coronal mass and energy loading makes it a principal research
area. Its fine structure defines its overall structure, so that hard-to-observe
and hard-to-model small-scale dynamical processes are the key to understanding.
However, both chromospheric observation and chromospheric simulation presently
mature towards the required sophistication. The open-field features seem of
greater interest than the easier-to-see closed-field features.Comment: Accepted for special issue "Astrophysical Processes on the Sun" of
Phil. Trans. Royal Soc. A, ed. C. Parnell. Note: clicking on the year in a
citation opens the corresponding ADS abstract page in the browse
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