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ASTR 610 Theory of Galaxy Formation Lecture 16

ASTR 610 Theory of Galaxy Formation Lecture 16

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Dutton, vdBosch, Dekel & Courteau, 2007, ApJ, 654, 27<br />

Adiabatic Contraction<br />

Note: r M(r) is only an adiabatic invariant for spherical systems with circular orbits.<br />

In reality disk growth results in halo contraction that is slightly different. This can<br />

be parameterized by stating that r f =Γ ν r i , where Γ=r f /r i in the simplified AC<br />

case discussed above, and ν is a `free parameter’.<br />

standard AC<br />

Simulations suggest that ν 0.8<br />

ν =1<br />

ν =0<br />

ν V max , which is simply due<br />

to the self-gravity <strong>of</strong> the disk<br />

Model predictions for the ratio V 2.2 /V vir for<br />

disk galaxies embedded in NFW haloes. Results<br />

are shown as function <strong>of</strong> the halo concentration<br />

parameter, c. Here V 2.2 is the rotation velocity<br />

<strong>of</strong> the disk measured at 2.2 disk scale-lengths.<br />

Results are shown for different `forms’ <strong>of</strong><br />

adiabatic contraction (different values <strong>of</strong> ν ).<br />

For comparison, the green curve shows the<br />

ratio V max /V vir .<br />

<strong>ASTR</strong> <strong>610</strong>: <strong>Theory</strong> <strong>of</strong> <strong>Galaxy</strong> <strong>Formation</strong> © Frank van den Bosch: Yale 2012

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