57 research outputs found
Measurement of the earthshine polarization in the B, V, R, and I band as function of phase
The characterization of the polarimetric properties of the planet Earth is
important for the interpretation of expected observations and the planning of
future instruments. We present a multi-wavelengths and multi-phase set of
benchmark values for the polarization signal of the integrated light from the
planet Earth derived from new polarimetric observations of the earthshine
back-scattered from the Moon's dark side. Using a new, specially designed wide
field polarimeter we measured the fractional polarization of the earthshine in
the B, V, R and I filters for Earth phase angles alpha between 30{\deg} and
110{\deg}. The phase dependence of the earthshine polarization is fitted by a
function p x sin(alpha)^2. To determine the polarization of the planet Earth we
correct our earthshine measurements by a polarization efficiency function for
the lunar surface derived from measurements of lunar samples from the
literature. The polarization of the earthshine decreases towards longer
wavelengths and is about a factor 1.3 lower for the higher albedo highlands.
For mare regions the measured maximum polarization is about 13 % at quadrature
in the B band. The resulting fractional polarizations for Earth are 24.6 % for
the B band, 19.1 % for the V band, 13.5 % for the R band, and 8.3 % for the I
band. Together with literature values for the spectral reflectivity of Earth we
obtain a contrast between the polarized flux of the Earth and the (total) flux
of the Sun with an uncertainty of less than 20 % and we find that the best
phase to detect an Earth twin is around an Earth phase alpha=65{\deg}. The
polarimetric models of Earth-like planets from Stam (2008) are in qualitative
agreement with our results but there are also significant differences which
might guide more detailed computations.Comment: 14 pages, 14 figures, accepted for publication in Astronomy &
Astrophysic
Disentangling Morphology, Star Formation, Stellar Mass, and Environment in Galaxy Evolution
We present a study of the spectroscopic and photometric properties of
galaxies in six nearby clusters. We perform a partial correlation analysis on
our dataset to investigate whether the correlation between star formation rates
in galaxies and their environment is merely another aspect of correlations of
morphology, stellar mass, or mean stellar age with environment, or whether star
formation rates vary independently of these other correlations. We find a
residual correlation of ongoing star formation with environment, indicating
that even galaxies with similar morphologies, stellar masses, and mean stellar
ages have lower star formation rates in denser environments. Thus, the current
star formation gradient in clusters is not just another aspect of the
morphology-density, stellar mass-density, or mean stellar age-density
relations. Furthermore, the star formation gradient cannot be solely the result
of initial conditions, but must partly be due to subsequent evolution through a
mechanism (or mechanisms) sensitive to environment. Our results constitute a
true ``smoking gun'' pointing to the effect of environment on the later
evolution of galaxies.Comment: 31 pages, including 5 figures; accepted for publication in Ap
Spatial variations of the SrI 4607\AA scattering polarization signals at subgranular scale observed with ZIMPOL at GREGOR telescope
Sr I 4607\AA spectral line shows one of the strongest scattering polarization
signals in the visible solar spectrum. The amplitudes of these signals are
expected to vary at granular spatial scales. This variation can be due to
changes in the magnetic field intensity and orientation (Hanle effect) as well
as due to spatial and temporal variations in the plasma properties. Measuring
the spatial variation of such polarization signal would allow us to study the
properties of the magnetic fields at subgranular region. But, the observations
are challenging since both high spatial resolution and high spectropolarimetric
sensitivity are required at the same time. To the aim of measuring these
spatial variations at granular scale, we carried out a spectro-polarimetric
measurement with the Zurich IMaging POLarimeter (ZIMPOL), at the GREGOR solar
telescope at different limb distances on solar disk. Our results show a spatial
variation of scattering linear polarization signals in Sr I 4607\AA line at the
granular scale at every , starting from 0.2 to 0.8. The correlation
between the polarization signal amplitude and the continuum intensity imply
statistically that the scattering polarization is higher at the granular
regions than in the intergranular lanes.Comment: 4 pages, 3 figures, Proceeding of Third Meeting of the Italian Solar
and Heliospheric Community, OCTOBER 28-31, 2018 - TURI
Signatures of Interstellar-Intracluster Medium Interactions: Spiral Galaxy Rotation Curves in Abell 2029
We investigate the rich cluster Abell 2029 (z~0.08) using optical imaging and
long-slit spectral observations of 52 disk galaxies distributed throughout the
cluster field. No strong emission-line galaxies are present within ~400 kpc of
the cluster center, a region largely dominated by the similarly-shaped X-ray
and low surface brightness optical envelopes centered on the giant cD galaxy.
However, two-thirds of the galaxies observed outside the cluster core exhibit
line emission. H-alpha rotation curves of 14 cluster members are used in
conjunction with a deep I band image to study the environmental dependence of
the Tully-Fisher relation. The Tully-Fisher zero-point of Abell 2029 matches
that of clusters at lower redshifts, although we do observe a relatively larger
scatter about the Tully-Fisher relation. We do not observe any systematic
variation in the data with projected distance to the cluster center: we see no
environmental dependence of Tully-Fisher residuals, R-I color, H-alpha
equivalent width, and the shape and extent of the rotation curves.Comment: 22 pages, 6 figures, 3 tables; to appear in the August 2000
Astronomical Journa
A method of incorporating general relativity in electromagnetic particle-in-cell code
An algorithm is presented that incorporates the tensor form of Maxwell's
equations in a general relativistic electromagnetic particle-in-cell code. The
code simplifies to Schwartzschild space-time for a non-spinning central mass.
The particle advance routine uses a fourth-order Runge-Kutta algorithm to
integrate the four-velocity form of Lorentz force. The current density is
calculated using the curved space-time of the metric.Comment: 17 pages, 8 figure
Wide-Field Chandra X-Ray Observations of AGN in Abell 85 & Abell 754
To better understand the mechanism or mechanisms that lead to AGN activity
today, we measure the X-ray AGN fraction in a new sample of nearby clusters and
examine how it varies with galaxy properties, projected cluster-centric radius,
and cluster velocity dispersion. We present new wide-field Chandra X-ray
Observatory observations of Abell 85, Abell 754 and the background cluster
Abell 89B out to their virial radii. Out of seventeen X-ray sources associated
with galaxies in these clusters, we classify seven as X-ray AGN with L_{X,B} >
10^{41} erg/s. Only two of these would be classified as AGN based on their
optical spectra. We combine these observations with archival data to create a
sample of X-ray AGN from six z < 0.08 clusters and find that 3.4+1.1/-0.8% of
M_R 10^{41} erg/s. We find that
more X-ray AGN are detected in more luminous galaxies and attribute this to
larger spheriods in more luminous galaxies and increased sensitivity to lower
Eddington-rate accretion from black holes in those spheroids. At a given X-ray
luminosity limit, more massive black holes can be accreting less efficiently,
yet still be detected. If interactions between galaxies are the principal
drivers of AGN activity, then the AGN fraction should be higher in lower
velocity dispersion clusters and the outskirts of clusters. However, the
tendency of the most massive and early-type galaxies to lie in the centers of
the richest clusters could dilute such trends. While we find no variation in
the AGN fraction with projected cluster-centric radius, we do find that the AGN
fraction increases significantly from 2.6+1.0/-0.8% in rich clusters to
10.0+6.2/-4.3% in those with lower velocity dispersions.Comment: Accepted by Astrophysical Journal, 17 pages using emulateapj.cls, 10
B & W Figures (degraded): Full resolution paper available at
http://www.astronomy.ohio-state.edu/~sivakoff/AGN/XAGN_A85_A754.pd
Observations on spatial variations of the Sr~{\sc i} 4607~\AA~scattering polarization signals at different limb distances with ZIMPOL
The Sr~{\sc i} 4607~\AA\ spectral line shows one of the strongest scattering
polarization signals in the visible solar spectrum. The amplitude of this
polarization signal is expected to vary at granular spatial scales, due to the
combined action of the Hanle effect and the local anisotropy of the radiation
field. Observing these variations would be of great interest because it would
provide precious information on the small-scale activity of the solar
photosphere. At present, few detections of such spatial variations have been
reported. This is due to the difficulty of these measurements, which require
combining high spatial ( 0.1"), spectral ( 20 m\AA), and temporal
resolution (< 1 min) with increased polarimetric sensitivity (
10). Aims. We aim to detect spatial variations at granular scales of
the scattering polarization peak of the Sr~{\sc i} 4607~\AA\ line at different
limb distances, and to study the correlation with the continuum intensity.
Methods.Using the Zurich IMaging POLarimeter (ZIMPOL) system mounted at the
GREGOR telescope and spectrograph in Tenerife, Spain, we carried out
spectro-polarimetric measurements to obtain the four Stokes parameters in the
Sr~{\sc i} line at different limb distances, from to , on
the solar disk. Results.Spatial variations of the scattering polarization
signal in the Sr~{\sc i} 4607~\AA\ line, with a spatial resolution of about
0.66", are clearly observed at every . The spatial scale of these
variations is comparable to the granular size. A statistical analysis reveals
that the linear scattering polarization amplitude in this Sr~{\sc i} spectral
line is positively correlated with the intensity in the continuum,
corresponding to the granules, at every .Comment: 8 pages, 6 figures, accepted for publication in A&
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