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PhD Thesis (PDF) - Department of Astronomy - University of Virginia

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LMXBs has an effective radius <strong>of</strong> 129 ′′ . Both fits indicate that there are more X-ray<br />

sources at larger radii than expected from the optical light distribution. Radial fits<br />

from circular isophotes yield similar results. Since NGC 4382 is an S0 galaxy, this<br />

disagreement may reflect the contribution <strong>of</strong> X-ray sources associated with the disk<br />

<strong>of</strong> the galaxy. However, this would not explain the difference between the LMXB<br />

distribution and the optical light distribution in NGC 4365.<br />

We note that a significant fraction <strong>of</strong> the LMXBs in NGC 4365 are associated<br />

with globular clusters (§ 2.4.2), as is generally true <strong>of</strong> elliptical galaxies (Angelini,<br />

Loewenstein, & Mushotzky 2001; Sarazin et al. 2000). In elliptical galaxies (including<br />

NGC 4365), the globular cluster population is more broadly distributed than that<br />

<strong>of</strong> the optical light and field stars (e.g., Harris 1991). This might help to explain<br />

the broader distribution <strong>of</strong> the LMXBs. Figure 2.8 suggests that there may be two<br />

populations <strong>of</strong> LMXBs, one with a small effective radius perhaps consistent with the<br />

optical distribution, and one with a larger effective radius. It is possible that these<br />

two distributions represent the LMXBs formed in globular clusters and those formed<br />

from field binary star systems. However, we note that in NGC 4697, the LMXBs<br />

followed the optical light distribution (Sarazin et al. 2001). More elliptical galaxies<br />

need to be observed to resolve this question.<br />

To test whether the LMXBs in these galaxies could discriminate between such<br />

models, we added either a second de Vaucouleurs model or an exponential model to the<br />

optical light distribution. For either additional component, there were only minimal<br />

improvements to the fits (∆χ 2 −0.6 for NGC 4365 and −0.8 for NGC 4382,<br />

with one less d<strong>of</strong> compared to the single pr<strong>of</strong>ile), indicating that the current data<br />

cannot statistically discriminate between single de Vaucouleurs distributions with<br />

large effective radii or multiple component distributions.<br />

41

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