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Near-infrared emission silicates

Figure 9.1 Examples of spectral energy distributions from young Sun-like stars with circumstellar dust disks. Optically thick dust disks (solid line) have excess emission relative to the stellar photosphere over a broad wavelength range, from near-infrared to millimeter wavelengths. Transition disks (dashed line) lack near-infrared excess emission, but have large mid- and far-infrared emission. Debris disks (dotted line) have small excess emission starting at wavelengths typically longer than 10 pm. Primordial and transition disks often show a prominent 10 pm silicate emission feature from warm dust grains in the disk atmosphere. Figure 9.1 Examples of spectral energy distributions from young Sun-like stars with circumstellar dust disks. Optically thick dust disks (solid line) have excess emission relative to the stellar photosphere over a broad wavelength range, from near-infrared to millimeter wavelengths. Transition disks (dashed line) lack near-infrared excess emission, but have large mid- and far-infrared emission. Debris disks (dotted line) have small excess emission starting at wavelengths typically longer than 10 pm. Primordial and transition disks often show a prominent 10 pm silicate emission feature from warm dust grains in the disk atmosphere.
While orrly a few in-situ observatiorts of dust are available, nttmerous remote observations of the above-mentioned bodies have been performed. Observation of emitted light, mostly in the infrared for solar system dust, provides information about temperatrrre and compositiorr, with the silicate emission feature near 11 pm. Observation of solar light scattered by dust, mostly in the optical and near infrared domains, provides clues to dust physical properties. [Pg.394]

One of the main spectroscopic properties that differentiate fluoride glasses from silica-based glasses is the low multiphonon emission rate. These non-radiative relaxations that may strongly compete with radiative processes in rare-earth ions are nearly three orders of magnitude lower in ZBLAN glass than in silicate, as shown in Fig. 2. This property is directly related to the fundamental vibration modes of the host and, therefore, varies basically in the same manner as the infrared absorption edge. [Pg.243]


See other pages where Near-infrared emission silicates is mentioned: [Pg.415]    [Pg.42]    [Pg.668]    [Pg.90]    [Pg.69]    [Pg.325]    [Pg.398]    [Pg.1442]    [Pg.58]    [Pg.83]    [Pg.386]    [Pg.274]    [Pg.153]    [Pg.93]    [Pg.415]    [Pg.110]    [Pg.6]   
See also in sourсe #XX -- [ Pg.359 , Pg.360 ]




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Emission infrared

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