A simple model of a laser (URGENT!!!!!!!) 1. The problem statement, all variables and given/known data Need to turn this in 2 hrs from now. Yes, I'm a slacker. (a) Suppose that N evolves much more quickly than n so that we can make the quasi-static approximation N ≈ 0. Given this approximation, re-write our equations as a 1-D dynamical system for n. (b) Show that for p > pc, the "trivial" fixed point n* = 0 is unstable, and that for p < pc, n* = 0 is stable. No need to explicitly determine pc. (c) What type of bifurcation occurs as the pump strength increases past the laser threshold pc? (d) For what range in the parameters (G, k, f, p) do you expect the quasi-static approximation to be good? 2. Relevant equations "This will give some good intuition and background information on the physics involved. The problem we will consider is as follows. Let N be the number of excited atoms in our laser, and let n be the number of photons (particles of light) that ... [etc.] .... n'(t) = GnN - kn N'(t) = -GnN - fN + p, where G is the gain coefficient .... [etc.] .... 3. The attempt at a solution Part (a) is easy: I have n'(t) = Gnp/(Gn+f) - k. Note that this means n'(t) = 0 if n = 0 or n = p/k - f/g. So then (n'(t))'(n) = Gpf/(Gn+f)2 - k. Plugging in n*=0 to that gives Gp/f - k. I'm assuming that the pc in the problem means pc = kf/G ????????? Because then we have a situation where p > pc makes Gp/f - k > 0, and p < pc makes Gp/f - k < 0. I've noticed also that p = fk/g makes (n'(t))'(n) = 0 when I plug in the other fixed point, n* = p/k - f/g. I'm still trying to figure out the significance of this.