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Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

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230 EXACT SOLUTIONS AND SCALAR FIELDS IN GRAVITY<br />

approaches a rotat<strong>in</strong>g steady state <strong>in</strong> the zoom<strong>in</strong>g space. In the ord<strong>in</strong>ary<br />

coord<strong>in</strong>ates, the central core is seen to rotate non-uniformly <strong>and</strong><br />

by it starts <strong>de</strong>form<strong>in</strong>g <strong>in</strong>to an elongated bar as a result of the<br />

growth of a non-axisymmetric <strong>in</strong>stability. Figure 1 displays equatorial<br />

<strong>de</strong>nsity contours of the central cloud portion at when a<br />

<strong>de</strong>nse bar has already formed. In Ref. [19] it is studied the mechanisms<br />

responsible for bar formation with<strong>in</strong> a collaps<strong>in</strong>g disk us<strong>in</strong>g the zoom<strong>in</strong>g<br />

coord<strong>in</strong>ates. They found that the growth of the shear component of velocity<br />

may <strong>in</strong>duce a non-uniformly rotat<strong>in</strong>g disklike core to elongate <strong>in</strong>to<br />

a barlike configuration. Subsequent collapse of the central bar is seen<br />

to proceed self-similarly. That is, the bar shr<strong>in</strong>ks faster <strong>in</strong> the direction<br />

of the cyl<strong>in</strong>drical radius than along the long axis. As a consequence the<br />

collaps<strong>in</strong>g bar becomes progressively narrower <strong>and</strong> a filamentary structure<br />

eventually forms as shown <strong>in</strong> Figure 2 at At this time, the<br />

<strong>de</strong>nsity of the filament is <strong>and</strong> because of the assumption<br />

of isothermality it will un<strong>de</strong>rgo un<strong>de</strong>f<strong>in</strong>ite collapse upon itself. This solution<br />

strongly resembles the self-similar solution for isothermal collapse<br />

first found <strong>in</strong> Ref. [15]. They predicted by l<strong>in</strong>ear analysis that when the<br />

mass per unit length of an <strong>in</strong>f<strong>in</strong>itely long cyl<strong>in</strong><strong>de</strong>r is much greater than<br />

the equilibrium value fragmentation of the cyl<strong>in</strong><strong>de</strong>r<br />

will not occur as long as the collapse rema<strong>in</strong>s isothermal. The <strong>de</strong>tails of

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