May 18, 2006 Examiners: Sergiu Klainerman, Janos Kollar, Robert Gunning Topics: PDE, Harmonic analysis Time: roughly 3 hours. Preamble: I got there five minutes early. Kollar arrived a few minutes after I did. Gunning came right on time. We stood outside waiting, me fidgeting and extremely nervous. Finally Klainerman shows up and let us into the office. Klainerman and Gunning each pulled up a chair. I stood. Kollar proceeded to layout a foam padding and reclined on his back, explaining he has lower back problem. They asked me what topic I want to start with, having really no preference, I told them to start with Harmonic. Klainerman then decided that prior to Harmonic we should ask a bit about real, which he deferred to Gunning. Real Analysis. Gunning: Suppose we have a sequence of integrable functions on the interval [0,1], tell me about convergence. Me: Fatou's lemma. Gunning: What would be a converse that would "make sense" for Limit inferiors? Is it true? Me: You change the sign in the inequality, and it is not true. Gunning: Counter example? Me: The sequence of functions f_n defined by n times the characteristic function of 1/n. The liminf of the integrals is 1, but the integral of the liminf is 0. Gunning: How about pointwise convergence? Me: I stated Egarov's theorem and stated that outside a set of epsilon measure, the convergence would be uniform. Gunning: But if a sequence converges in L1, must the sequence converge pointwise? Me: Yes? (saw Gunning shake his head) No... Gunning: Give an example. Me: (after much thought) The sequence of functions f_n defined by f_1 = 1. f_2 is characteristic function of [0,1/2]. f_3 is that of [1/2,1], f_4 is characteristic of [0,1/4] and so on. Gunning: Does it contradict Egarov's theorem? Me: hmmmmm perhaps Egarov's theorem requires a.e. convergence? (apparently I left that part out in the initial statement.) Gunning: How about the other way around, if a sequence of functions converges, does it necessarily converge in L1. Me: No. You need to assume uniform convergence. Gunning: okay, let's change the subject, how about fundamental theorem of calculus for Lebesgue measures. Me: give the theorem in both directions (for absolutely continuous functions the derivative exists a.e. and integrates to it). Gunning: what is the corresponding theorem for measures. Me: Give Radon-Nikodym. Klainerman: What is the differentiability/continuity of Lebesgue integrable functions. Me: I had no idea what he was asking about. After getting cues from Klainerman a bit, I finally realized he was asking about Lebesgue Differentiation Theorem. Then he asked me for a proof. While I was hestitating, he told me to consider the Maximal function. So we talked a bit about that: the definition, the fact that it is L1->weak L1, and L^p to L^p for p up to infinity. Then he asked me for a proof ot the L.D.T. using the maximal function, but I still have no idea. So he asked me whether the theorem is obvious for continuous functions, I said yes, and sketched the proof. He then asked about how to show that C0 is dense in L1, and, for some bizarre reason, I blanked out (which will happen quite a lot during the next three hours). So he hinted me at C^infty functions, and finally I caught on and gave the mollifier construction. At which point, we moved to Harmonic/PDE. Part I Klainerman: Time for some Harmonic analysis. What can you say about Calderon-Zygmund theory? Me: I defined a C-Z operator, and said that it would take L^p to L^p, 1
0). [On hindsight, that is completely, utterly, obvious.]
And here comes the really humiliating parts.
Harmonic/PDE. Part II
Klainerman: tell me about the Maximal principle.
Me: gave the strong one.
Klainerman: how does this relate to the maximal principle in complex
analysis?
Me: I gave some other things and he wasn't too happy. Finally I
figured out he only wanted that the real and imaginary parts of an
analytic function each is a harmonic function.
Klainerman: explain ellipticity. (simple.)
Klainerman: How about the Dirichlet problem?
Me: I wrote out the problem, and mentioned that on special domains
(half plane or disk) we have Poisson's formula.
Klainerman: What makes those two special.
Me: No idea.
Klainerman: How about for arbitrary domains.
Me: I blanked out. For a whole 5 minutes. I was just about to say
somthing about energy methods when Klainerman told me that "If you
don't know just say so, no need to waste our time." And he was
obviously unhappy about my really, really despictable performance on
PDEs.
Klainerman: that was rather unacceptable. What do you actually know?
Me: So I told him that maybe we can switch to harmonic again and do
Littlewood Paley theory.
Klainerman: okay, fine, give us a short lecture on what you know about
Littlewood-Paley theory.
Me: I gave the basic construction, wrote down the properties (cheap
littlewood-paley, square function estimate, finite band, almost
orthogonality, and Bernstein. Didn't get a chance to do commutator
estimates before he interrupted).
Klainerman: But this is just a tool, what is it good for?
Me: Started doing Sobolev multiplication estimates. (fg) in H^s can be
bounded be f in H^r and g in H^t if s