Schweitzer 2019
Read the problems at the official link. The 2019 Schweitzer problems are © the János Bolyai Mathematical Society, so we don't reproduce them here. Open the 2019 problems (PDF) from the University of Szeged page.
The topic labels, hints and solutions below are our own, written from scratch: our solutions, not official ones. If you spot a mistake, please use “Report a problem” at the bottom of the page.
P5 Geometry: halfspaces cutting out a convex body, with margin
- Hint 1. Fix balls $B(c,r)\subseteq S\subseteq B(c,R)$. Any $\alpha<r/R$ will do.
- Hint 2. If every halfspace nearly reaches the outside point $P$, each one contains a cone from the small ball toward a point near $P$. Find a point outside $S$ that lies in all of these cones.
Our solution (not official)
Since $S$ is compact with nonempty interior, choose a point $c$ and radii $0<r\le R$ with $B(c,r)\subseteq S\subseteq B(c,R)$. We show that any $\alpha<r/R$ works.
Let $P$ be a point; if $P\in S$ there is nothing to prove. So let $d=\operatorname{dist}(P,S)>0$, and suppose, for contradiction, that $\operatorname{dist}(P,H_i)<\alpha d$ for every $i$.
A test point. Choose $s\in(0,1)$ with $\dfrac{s}{1-s}=\dfrac{\alpha d}{r}$, and let $Y=(1-s)P+sc$, a point on the segment from $P$ toward the center.
$Y$ lies in every $H_i$. Each $H_i$ contains $S$, hence the ball $B(c,r)$, and it contains a point $P_i$ with $|P-P_i|<\alpha d$. Write $$Y=(1-s)P_i+s\Big(c+\tfrac{1-s}{s}(P-P_i)\Big).$$ The second point is within $\frac{1-s}{s}\alpha d=r$ of $c$, so it lies in $B(c,r)\subseteq H_i$. As $H_i$ is convex, $Y\in H_i$. Therefore $Y\in\bigcap_iH_i=S$.
But $Y$ is outside $S$. If $Y\in S$, then $d\le|P-Y|=s\,|P-c|$. The nearest point of $S$ to $P$ lies within $R$ of $c$, so $|P-c|\le d+R$, and $$d\le s(d+R)\ \Longrightarrow\ d\le\frac{s}{1-s}R=\frac{\alpha dR}{r}\ \Longrightarrow\ r\le\alpha R,$$ which contradicts $\alpha<r/R$. So some $H_i$ has $\operatorname{dist}(P,H_i)\ge\alpha\operatorname{dist}(P,S)$.
P7 Complex analysis: critical points inside a one-piece level curve
- Hint 1. Show first that the inside of the curve is exactly the set where $|P|<1$, and that every zero of $P$ is there.
- Hint 2. On the inside, $P$ is a proper map onto the unit disc. The Riemann–Hurwitz formula counts its critical points.
Our solution (not official)
Let $n=\deg P$. A constant $P$ cannot give a Jordan curve, and for $n=1$ there are no critical points, so let $n\ge2$. By the Jordan curve theorem, the complement of $L$ has two components: a bounded inside $\Omega$ and an unbounded outside $E$.
Step 1: $\Omega$ is exactly where $|P|<1$. Neither component meets $L$, so $|P|\ne1$ on each, and each is connected; hence $|P|<1$ on all of it or $|P|>1$ on all of it. On $E$, $|P|\to\infty$ at infinity, so $|P|>1$ there. If also $|P|>1$ on $\Omega$, then $P$ would have no zeros at all (a zero is not on $L$ either). So $|P|<1$ on $\Omega$, and all $n$ zeros of $P$ lie in $\Omega$.
Step 2: a proper map. $P$ maps $\Omega$ into the unit disc $D$. If points of $\Omega$ leave every compact subset of $\Omega$, they approach $L$ (as $\Omega$ is bounded), so $|P|\to1$ along them. Thus $P:\Omega\to D$ is proper. A proper nonconstant holomorphic map has a degree: every point of $D$ has the same number of preimages, counted with multiplicity. Counting the preimages of $0$, the degree is $n$.
Step 3: Riemann–Hurwitz. For a proper holomorphic map of degree $n$ between plane domains, $\chi(\Omega)=n\,\chi(D)-b$, where $b$ is the number of critical points in $\Omega$ counted with multiplicity. The inside of a Jordan curve is simply connected, so $\chi(\Omega)=\chi(D)=1$ and $b=n-1$. But $P'$ has only $n-1$ zeros in the whole plane, counted with multiplicity. Hence all of them lie in $\Omega$, the interior of $L$.
P8 Analysis: integrable differences force an integrable function
- Hint 1. The shifts $t\in[-1,1]$ with $\int_{-2}^{2}|f(x+t)-f(x)|\,dx\le N$ form a measurable set, and for some $N$ it has positive measure.
- Hint 2. Steinhaus: $E-E$ contains an interval around $0$. Then average the differences over small shifts and choose a good base point.
Our solution (not official)
The hypothesis doesn’t change if we translate $f$, so it is enough to show that $f$ is integrable on some interval around $0$.
Step 1: many good shifts. The function $(x,t)\mapsto f(x+t)-f(x)$ is measurable on the plane. By Tonelli’s theorem, $\Phi(t)=\int_{-2}^{2}|f(x+t)-f(x)|\,dx$ is a measurable function of $t$, finite for every $t$ by hypothesis. The sets $E_N=\{t\in[-1,1]:\Phi(t)\le N\}$ increase to $[-1,1]$, so some $E=E_N$ has positive measure. By Steinhaus’ theorem, $E-E$ contains an interval $(-\delta,\delta)$.
Step 2: all small shifts are good. Let $s=t-t'$ with $t,t'\in E$. For every $x$, $$f(x+s)-f(x)=\big[f(x-t'+t)-f(x-t')\big]-\big[f(x)-f(x-t')\big].$$ For $x\in[-1,1]$, the point $x-t'$ lies in $[-2,2]$, so $$\int_{-1}^{1}|f(x+s)-f(x)|\,dx\le\Phi(t)+\Phi(t')\le2N\qquad(|s|<\delta).$$
Step 3: a good base point. Integrate over $s\in(0,\delta)$ and swap the integrals: $$\int_{-1}^{1}\Big(\int_0^\delta|f(x+s)-f(x)|\,ds\Big)dx\le2N\delta .$$ So for almost every $x_0\in[-1,1]$ the inner integral is finite, and since $f(x_0)$ is a real number, $\int_{x_0}^{x_0+\delta}|f|<\infty$. The same argument with $s\in(-\delta,0)$ gives $\int_{x_0-\delta}^{x_0}|f|<\infty$ for almost every $x_0$. Pick one $x_0$ with $|x_0|<\delta/2$ that is good for both. Then $f$ is integrable on $(x_0-\delta,x_0+\delta)$, which contains $(-\delta/2,\delta/2)$.