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Figure 1 shows various aspects of the ISM simulations. Figure 1a
shows the projection of the density field in z-direction. Figure 1b shows
16 cuts of the density field along the z-direction, with a
separation of 7 pixels between cuts. Figure 1c shows cuts along the
same fixed-z planes for the z-component of the velocity. Finally, figure 1d
shows the velocity channels of the corresponding position-velocity (PV)
data cube, with a resolution of 16 channels. The PV cube is obtained
assuming an optically thin gas, the z-coordinate containing
the density-weighted velocity histogram for each (x,y)-pixel.
A number of points are worth noting:
- Localized structures in the PV maps do not necessarily correspond
to localized structures in physical space, and viceversa. For example,
the structure labeled A in the 11th velocity channel in fig. 1d
is seen to result from the superposition of two density structures
also labeled A in cuts 5 and 11 of the 3D density field (fig. 1b). Conversely, expanding
shells (caused by the modeled star formation) are localized in physical
space, but extended in
PV space, such as the structures labeled B in the same figures.
- The structure seen in the velocity channels of fig. 1d
is subjectively more similar to the velocity cuts shown in fig. 1c
than to the density cuts shown in fig. 1b, or the projected density
field of fig. 1a, indicating that the
process of ``selecting'' the density by its velocity imprints features
of the velocity distribution onto that of the density. Although
further quantification of this effect is necessary, it can be
understood as a possible consequence that the structure seen in the
velocity channels actually originates from histograms of velocity, albeit weighted by the density.
Next: PRELIMINARY PCA RESULTS
Up: No Title
Previous: THE MODEL
Barbara Pichardo Silva
1999-01-30