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| | [No title] (Site not responding. Last check: 2007-10-25) |
 | | Content: a very detailed discussion of the simple model of interaction based on the equation array: % d^2 q(t)/dt^2 =-\Omega^2(q(t)-Q(t))+f_0(t), % d^2 u(t,x)/t^2=c^{2}d^2 u(t,x)/dx ^2 % -4\gamma c\delta(x-x_0)(Q(t)-q(t))+f_1(t,x), % Q(t) = u(t,x_0). |
 | | , x> 0, \gamma t >> 1 \\ \end{array} \right\} \end{eqnarray*} \addvspace{\bigskipamount} We see, in the case of $$ k^2=\Omega^2 \,,\, \frac{\partial q(t)}{\partial t}\Big_{t=0}=0 \,,\, \gamma t >> 1 $$ the incident wave is essentially completely reflected by the oscillator!!! |
 | | This phenomenon can also be referred to as a kind of {\bf resonance}. |
| www.ma.utexas.edu /mp_arc/papers/03-33 (2194 words) |
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