ADB För Folkbokföring OCH Skatteuppbörd I Sverige

Summary A governmental Swedish committee has suggested conversion to ADP for the file maintenance involved in population registration, tax accounting etc. with a tape-oriented IBM 7070 and five IBM 1401 satellite computers. Investment in hardware, building etc. >6 M$; planning, programming, and file conversion 4 M$. Estimated annual savings, taking depreciation of initial costs into account: 2 M$/yr. Reduction of clerical force more than 1,000.     

Invariante Zwischenkörper endlicher Körpererweiterungen

Let KM be a finite field extension. An intermediate field L is called invariant if there is an affine algebraic K-group acting on M with L as its invariant field. The question, which intermediate fields are invariant, was studied by Bégueri [1] for purely inseparable extensions and by Sweedler [6] for arbitrary extensions, but only for a restricted class of groups. In this paper Bégueri's result is generalized to arbitrary field extensions. Additionally it is shown that one can check whether a given intermediate field is invariant or not by computing the rank of certain matrices. As an application we get a class of invariant intermediate fields.     

Fixkörper vonp-Automorphismengruppen rein-transzendenter Körpererweiterungen vonp-Charakteristik

Ohne Zusammenfassung Karl Heinrich Weise zum 50. Geburtstag     

Gitterpunktsanzahl und Parallelkörpervolumen von Eikörpern

LetΛ={x=(x ₁,...,x _d )|x _i ∈?} be a lattice in euclideand-spaceR ^d with respect to a rectangular coordinate system with unit vectors. Then for instance the following theorem holds: The number of lattice pointsG(K)=card (K∩Λ) of an arbitrary convex bodyK?R ^d is less or equal the volumeV(K _λd) of the outer parallel bodyK _λd ofK at a distance λ _d =ω _d ^-1/d (ω _d =Volume of thed-unitsphere, 2≤d≤5). The number λ is best possible.     

Zur Wellenausbreitung im heterogen-porösen Festkörper

Summary A method is developed which allows to describe analytically the two-dimensional elastic wave-field in porous media disturbed by heterogeneities. In the first place circular inclusions are regarded, later inclusions of arbitrary contour.     

Zur Möbiusgeometrie über Alternativkörpern

Zusammenfassung Möbiusgeometrien (K, L) über nicht notwendig kommutativen KörpernKL – eine Definition dieser Geometrien findet man in [1] — sind Verallgemeinerungen der Geometrie der Kreise auf der Riemannschen Zahlenkugel (K=,L=). In der vorliegenden Note wollen wir, unter Verzicht auf die Assoziativität vonL, Möbiusgeometrien auch für den Fall betrachten, woK ein im Zentrum des AlternativkörpersL enthaltener Körper ist, und (in Abschnitt 2) die Gruppe der Kreisverwandtschaften von (K, L) angeben. Dabei benutzen wir, anders als in [1] und [5], nur den Doppelverhältniskalkül, den wir gleichwertig zu der von A. Schleiermacher in [6] vorgeschlagenen Verallgemeinerung für kollineare Punkte einer Moufarigebene definieren. Es ergibt sich damit ein neuer Beweis des Satzes über Kettenverwandtschaften von (K, L) auch im assoziativen Fall. Die Verwendung von Doppelverhältnissen beim Beweis — auch bei charL=2-wird insbesondere durch das in Abschnitt 2 bewiesene Lemma (2.4) (Verallgemeinerung des sog. von Staudtschen Theorems; vgl. [2], [3]) ermöglicht.     

Zur Möbiusgeometrie über einem Körperpaar

Ohne ZusammenfassungHerrn Professor Dr.Reinhold Baer zum 60. Geburtstag am 22. 7. 1962 gewidmet     

Zu den Lagrange'schen Lösungen des n-Körperproblems

Ohne Zusammenfassung     

Zu den Lagrange'schen Lösungen des n-Körperproblems II

Ohne Zusammenfassung     

1D Schrödinger Operators with Short Range Interactions: Two-Scale Regularization of Distributional Potentials

For real ${L_\infty(\mathbb{R})}$ -functions ${\Phi}$ and ${\Psi}$ of compact support, we prove the norm resolvent convergence, as ${\varepsilon}$ and ${\nu}$ tend to 0, of a family ${S_{\varepsilon \nu}}$ of one-dimensional Schrödinger operators on the line of the form $$S_{\varepsilon \nu} = -\frac{d^2}{dx^2} + \frac{\alpha}{\varepsilon^2} \Phi \left( \frac{x}{\varepsilon} \right) + \frac{\beta}{\nu} \Psi \left(\frac{x}{\nu} \right),$$ provided the ratio ${\nu/\varepsilon}$ has a finite or infinite limit. The limit operator S ₀ depends on the shape of ${\Phi}$ and ${\Psi}$ as well as on the limit of ratio ${\nu/\varepsilon}$ . If the potential ${\alpha\Phi}$ possesses a zero-energy resonance, then S ₀ describes a non trivial point interaction at the origin. Otherwise S ₀ is the direct sum of the Dirichlet half-line Schrödinger operators.     

Stability results for the N-dimensional Schiffer conjecture via a perturbation method

Given a eigenvalue $\mu _{0m}^2$ of $-\Delta $ in the unit ball $B_1$ , with Neumann boundary conditions, we prove that there exists a class $\mathcal{D}$ of $C^{0,1}$ -domains, depending on $\mu _{0m} $ , such that if $u$ is a no trivial solution to the following problem $ \Delta u+\mu u=0$ in $\Omega , u=0$ on $\partial \Omega $ , and $ \int \nolimits _{\partial \Omega }\partial _{\mathbf{n}}u=0$ , with $\Omega \in \mathcal{D}$ , and $\mu =\mu _{0m}^2+o(1)$ , then $\Omega $ is a ball. Here $\mu $ is a eigenvalue of $-\Delta $ in $\Omega $ , with Neumann boundary conditions.     

Sharp energy estimates for nonlinear fractional diffusion equations

We study the nonlinear fractional equation $(-\Delta )^su=f(u)$ in $\mathbb R ^n,$ for all fractions $0<s<1$ and all nonlinearities $f$ . For every fractional power $s\in (0,1)$ , we obtain sharp energy estimates for bounded global minimizers and for bounded monotone solutions. They are sharp since they are optimal for solutions depending only on one Euclidian variable. As a consequence, we deduce the one-dimensional symmetry of bounded global minimizers and of bounded monotone solutions in dimension $n=3$ whenever $1/2\le s<1$ . This result is the analogue of a conjecture of De Giorgi on one-dimensional symmetry for the classical equation $-\Delta u=f(u)$ in $\mathbb R ^n$ . It remains open for $n=3$ and $s<1/2$ , and also for $n\ge 4$ and all $s$ .     

Collapsibility and Vanishing of Top Homology in Random Simplicial Complexes

Let $\Delta _{n-1}$ denote the $(n-1)$ -dimensional simplex. Let $Y$ be a random $d$ -dimensional subcomplex of $\Delta _{n-1}$ obtained by starting with the full $(d-1)$ -dimensional skeleton of $\Delta _{n-1}$ and then adding each $d$ -simplex independently with probability $p=\frac{c}{n}$ . We compute an explicit constant $\gamma _d$ , with $\gamma _2 \simeq 2.45$ , $\gamma _3 \simeq 3.5$ , and $\gamma _d=\Theta (\log d)$ as $d \rightarrow \infty $ , so that for $c < \gamma _d$ such a random simplicial complex either collapses to a $(d-1)$ -dimensional subcomplex or it contains $\partial \Delta _{d+1}$ , the boundary of a $(d+1)$ -dimensional simplex. We conjecture this bound to be sharp. In addition, we show that there exists a constant $\gamma _d< c_d <d+1$ such that for any $c>c_d$ and a fixed field $\mathbb{F }$ , asymptotically almost surely $H_d(Y;\mathbb{F }) \ne 0$ .     

Singular perturbation method for inhomogeneous nonlinear free boundary problems

In this paper, we study solutions of one phase inhomogeneous singular perturbation problems of the type: $ F(D^2u,x)=\beta _{\varepsilon }(u) + f_{\varepsilon }(x) $ and $ \Delta _{p}u=\beta _{\varepsilon }(u) + f_{\varepsilon }(x)$ , where $\beta _{\varepsilon }$ approaches Dirac $\delta _{0}$ as $\varepsilon \rightarrow 0$ and $f_{\varepsilon }$ has a uniform control in $L^{q}, q>N.$ Uniform local Lipschitz regularity is obtained for these solutions. The existence theory for variational (minimizers) and non variational (least supersolutions) solutions for these problems is developed. Uniform linear growth rate with respect to the distance from the $\varepsilon -$ level surfaces are established for these variational and nonvaritional solutions. Finally, letting $\varepsilon \rightarrow 0$ basic properties such as local Lipschitz regularity and non-degeneracy property are proven for the limit and a Hausdorff measure estimate for its free boundary is obtained.     

Regularity of semi-stable solutions to fourth order nonlinear eigenvalue problems on general domains

We examine the fourth order problem $\Delta ^2 u = \lambda f(u) $ in $ \Omega $ with $ \Delta u = u =0 $ on $ {\partial \Omega }$ , where $ \lambda > 0$ is a parameter, $ \Omega $ is a bounded domain in $\mathbb{R }^N$ and where $f$ is one of the following nonlinearities: $ f(u)=e^u$ , $ f(u)=(1+u)^p $ or $ f(u)= \frac{1}{(1-u)^p}$ where $ p>1$ . We show the extremal solution is smooth, provided $$\begin{aligned} N < 2 + 4 \sqrt{2} + 4 \sqrt{ 2 - \sqrt{2}} \approx 10.718 \text{ when} f(u)=e^u, \end{aligned}$$ and $$\begin{aligned} N < \frac{4p}{p-1} + \frac{4(p+1)}{p-1} \left( \sqrt{ \frac{2p}{p+1}} + \sqrt{ \frac{2p}{p+1} - \sqrt{ \frac{2p}{p+1}}} - \frac{1}{2} \right) \end{aligned}$$ when $ f(u)=(u+1)^p$ . New results are also obtained in the case where $ f(u)=(1-u)^{-p}$ . These are substantial improvements to various results on critical dimensions obtained recently by various authors. To do that, we derive a new stability inequality satisfied by minimal solutions of the above equation, which is more amenable to estimates as it allows a method of proof reminiscent of the second order case.     

Singular limits for Liouville-type equations on the flat two-torus

We consider the problem $$\begin{aligned} -\Delta u=\varepsilon ^{2}e^{u}- \frac{1}{|\Omega |}\int _\Omega \varepsilon ^{2} e^{u}+ {4\pi N\over |\Omega |} - 4 \pi N\delta _p, \quad \text{ in} {\Omega }, \quad \int _\Omega u=0 \end{aligned}$$ in a flat two-torus $\Omega $ with periodic boundary conditions, where $\varepsilon >0,\,|\Omega |$ is the area of the $\Omega $ , $N>0$ and $\delta _p$ is a Dirac mass at $p\in \Omega $ . We prove that if $1\le m<N+1$ then there exists a family of solutions $\{u_\varepsilon \}_{\varepsilon }$ such that $\varepsilon ^{2}e^{u_\varepsilon }\rightharpoonup 8\pi \sum _{i=1}^m\delta _{q_i}$ as $\varepsilon \rightarrow 0$ in measure sense for some different points $q_{1}, \ldots , q_{m}$ . Furthermore, points $q_i$ , $i=1,\dots ,m$ are different from $p$ .     

A generalized min–max theorem for functionals of strongly indefinite sign

We consider non-linear Schrödinger equations of the following type: $$\begin{aligned} \left\{ \begin{array}{l} -\Delta u(x) + V(x)u(x)-q(x)|u(x)|^\sigma u(x) = \lambda u(x), \quad x\in \mathbb{R }^N \\ u\in H^1(\mathbb{R }^N)\setminus \{0\}, \end{array} \right. \end{aligned}$$ where $N\ge 1$ and $\sigma >0$ . We will concentrate on the case where both $V$ and $q$ are periodic, and we will analyse what happens for different values of $\lambda $ inside a spectral gap $]\lambda ^-,\lambda ^+[$ . We derive both the existence of multiple orbits of solutions and the bifurcation of solutions when $\lambda \nearrow \lambda ^+$ . Thereby we use the corresponding energy function ${I_\lambda }$ and we derive a new variational characterization of multiple critical levels for such functionals: in this way we get multiple orbits of solutions. One main advantage of our new view on some specific critical values $c_0(\lambda )\le c_1(\lambda )\le \cdots \le c_n(\lambda )\le \cdots $ is a multiplicity result telling us something about the number of critical points with energies below $c_n(\lambda )$ , even if for example two of these values $c_i(\lambda )$ and $c_j(\lambda )$ ( $0\le i<j\le n$ ) coincide. Let us close this summary by mentioning another main advantage of our variational characterization of critical levels: we present our result in an abstract setting that is suitable for other problems and we give some hints about such problems (like the case corresponding to a Coulomb potential $V$ ) at the end of the present paper.     

Remarks on the existence of solutions to some quasilinear elliptic problems involving the Hardy-Leray potential

We study the solvability of the quasilinear problem $$\begin{aligned} -\Delta _p u =\frac{u^q }{|x|^p}+g(\lambda , x, u) \quad u>0 \quad \text{ in}\;\Omega , \end{aligned}$$ with $u=0$ on $\partial \Omega $ , where $-\Delta _p(\cdot )$ is the $p$ -Laplacian operator, $q>0, 1<p<N$ and $\Omega $ a smooth bounded domain in $\mathbb R ^N$ . We consider the following cases:

1. $g(\lambda ,x,u)\equiv 0$ ;
2. $g(\lambda ,x,u)=\lambda f(x)u^r$ , with $\lambda >0$ and $f(x) \gneq 0$ belonging to $L^{\infty }(\Omega )$ and $0 \le r<p-1$ .

In the case $(i)$ , the existence of solutions depends on the location of the origin in the domain, on the geometry of the domain and on the exponent $q$ . On the other hand, in the case $(ii)$ , the existence of solutions only depends on the position of the origin and on the coefficient $\lambda $ , but does not depend either on the exponent $q$ or on the geometry of $\Omega $ .     

Liouville theorems for stable solutions of biharmonic problem

We prove some Liouville type results for stable solutions to the biharmonic problem $\Delta ^2 u= u^q, \,u>0$ in $\mathbb{R }^n$ where $1 < q < \infty $ . For example, for $n \ge 5$ , we show that there are no stable classical solution in $\mathbb{R }^n$ when $\frac{n+4}{n-4} < q \le \left(\frac{n-8}{n}\right)_+^{-1}$ .