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Overview
- Spitzer will be able to study star and planet formation.
- Star formation is ongoing in dark interstellar clouds. Most if not
all stars are believed to have a circumstellar disk at some point in the
star formation process. Planet formation, if it occurs for any given
star, is thought to occur in these circumstellar disks, which are best
seen in infrared light. Spitzer can study the evolution of disks in the key
phase of planet formation.
Even when a planet itself is too faint to see directly, its gravitational
influence on its star's dust disk can still be visible, either directly,
just as small moons sculpt Saturn's rings, or indirectly, via structure
in the observed spectral energy distribution. Spitzer will provide the
first images of many nearby circumstellar disks, and spectral energy
distributions for many more. Holes, clumps, or sharp edges in these disks
may betray the presence of planets.
Spitzer will be able to study the interstellar medium in our Galaxy,
including things such as:
- The structure of our Galaxy as mapped in gas and dust clouds.
- Supernova remnants interacting with the interstellar medium.
- Planetary nebulae.
Spitzer will be able to find and study brown dwarfs. There are now several
hundred known; Spitzer is expected to find thousands of them.
Images and Plots
Note:
Note: This Compendium is a work in progess. We have used the best information available, including data
from other missions, and will update these pages as soon as possible with
the new information.
Representations of star formation process:
 Click for
larger image
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Mid-IR spectra of several stages of star formation, with major molecular
species marked; PAH=Polycyclic Aromatic Hydrocarbons. Plot courtesy the
c2d Legacy
team. |
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Orginal plots of IRAS data indicating standard stars (left column) and
stars with (then) newly-discovered far-IR excesses (right column). (This
copy of these plots from Backman and Paresce, 1993, "Protostars and
Planets III"; originally from a paper by Fred Gillett, 1986, in "Light on
Dark Matter" volume.)
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 Click for
full-size complete image
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Representation of model spectral energy distributions of stars with debris
disks as a function of spectral type. The model has 0.1 Mmoon of
30-micron size dust grains in a disk from 30-60 AU. The bars are 3
sigma limits. (The model is based on disks around A stars.) Plot courtesy
D. Koerner, NAU.
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Sensitivity to Evolution of Circumstellar Dust at 30 pc for IRAS, ISO, and
Spitzer (approximate levels). Plot courtesy D. Backman, M. Meyer, and the
FEPS Legacy team.
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Spectral Energy Distributions (SED) for star with disk as a function of
time, with IRAS, ISO, and Spitzer sensitivity levels indicated. Plot
courtesy D. Backman, M. Meyer, and the FEPS Legacy team.
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Simulated MIPS 70 micron observations of (left to right) Vega (which is
known to have a remnant dust disk), 1/10th as much dust as Vega, and a
point source. All are on a logarithmic brightness scale. Simulations
courtesy N. Wright, UCLA. |
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Simulated MIPS 24 micron observations of (left to right) Vega (which is
known to have a remnant dust disk), and the difference of 1/100th as much
dust as Vega and a point source. Both are on a logarithmic brightness
scale. Simulations courtesy N. Wright, UCLA. |
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Approximate size of a Spitzer pixel at the distance of
alpha Cen. (Image from JPL image library.)
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 Click
for larger image
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Approximate size of a Spitzer pixel at the distance of
Vega. (Image from JPL image library.)
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Click for larger
version of plot
Click for larger
version of plot
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As is the case in the far-red and near-IR, the brightness temperature,
Tbr, of brown dwarfs varies strongly with wavelength due to the high
contrast between opacity windows and molecular absorption bands. This is
still true in the mid-IR up to about 11 microns. Thereafter, Tbr gradually
decreases to stabilize at ~75% of the effective temperature, Teff, beyond
18 microns. Only near 6 and near 10 microns does Tbr become as large as
the effective temperature. Exposure times should be calculated
appropriately.
The attached figures present a model mid-infrared spectral sequence of
brown dwarfs with Teff ranging from 600 to 2400 K (from bottom to top) in
steps of 200 K. All models have solar metallicity, log g = 5, include the
effect of iron and silicate clouds, and are shown at a spectral resolution
of 200. The bandpasses of the four IRAC filters are shown by thick solid
lines at the top of the first figure. Additional details can be found in
Saumon, Marley, and
Lodders (2003).
Figures courtesy Didier Saumon and Mark Marley.
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As brown dwarfs age and cool, their molecular bands become very prominent.
The IRAC 3.6 and 4.5 micron filters are tuned to methane-dominated brown
dwarf spectra. Here are predicted spectral energy distribution of two
brown dwarfs and Jupiter at different distances; red dots are IRAC
sensitivities (5 sigma in 12 sec exposure). Plot courtesy N. Wright, UCLA.
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Left: Image of Gl229B from Hubble.
Right: Image of Jupiter at 5 microns (from J. L. Ortiz, et al. 1998.
Evolution and persistence of 5-um hot spots at the Galileo Probe entry
latitude, J. Geophys. Res. 103, 23051 - 23069).
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