Wikipedia / Hilbert's fourth problem
Wikipedia / Hilbert's fourth problem
In mathematics, Hilbert's fourth problem in the 1900 list of Hilbert's problems is a foundational question in geometry. In one statement derived from the original, it was to find — up to an isomorphism — all geometries that have an axiomatic system of the classical geometry (Euclidean, hyperbolic and elliptic), with those axioms of congruence that involve the concept of the angle dropped, and 'triangle inequality', regarded as an axiom, added.
If one assumes the continuity axiom in addition, then, in the case of the Euclidean plane, we come to the problem posed by Jean Gaston Darboux: "To determine all the calculus of variation problems in the plane whose solutions are all the plane straight lines."
There are several interpretations of the original statement of David Hilbert. Nevertheless, a solution was sought, with the German mathematician Georg Hamel being the first to contribute to the solution of Hilbert's fourth problem.
A recognized solution was given by Soviet mathematician Aleksei Pogorelov in 1973. In 1976, Armenian mathematician Rouben V. Ambartzumian proposed another proof of Hilbert's fourth problem.
Original statement
Hilbert discusses the existence of non-Euclidean geometry and non-Archimedean geometry
...a geometry in which all the axioms of ordinary euclidean geometry hold, and in particular all the congruence axioms except the one of the congruence of triangles (or all except the theorem of the equality of the base angles in the isosceles triangle), and in which, besides, the proposition that in every triangle the sum of two sides is greater than the third is assumed as a particular axiom.
Due to the idea that a 'straight line' is defined as the shortest path between two points, he mentions how congruence of triangles is necessary for Euclid's proof that a straight line in the plane is the shortest distance between two points. He summarizes as follows:
The theorem of the straight line as the shortest distance between two points and the essentially equivalent theorem of Euclid about the sides of a triangle, play an important part not only in number theory but also in the theory of surfaces and in the calculus of variations. For this reason, and because I believe that the thorough investigation of the conditions for the validity of this theorem will throw a new light upon the idea of distance, as well as upon other elementary ideas, e. g., upon the idea of the plane, and the possibility of its definition by means of the idea of the straight line, the construction and systematic treatment of the geometries here possible seem to me desirable.
Flat metrics
Desargues's theorem, named after Girard Desargues, states that if two triangles lie on a plane such that the lines connecting corresponding vertices of the triangles meet at one point, the three points at which the prolongations of three pairs of corresponding sides of the triangles intersect lie on one line. The necessary condition for solving Hilbert's fourth problem is the requirement that a metric space that satisfies the axioms of this problem should be Desarguesian. That is:
if the space is of dimension 2, then Desargues's theorem and its inverse should hold;
if the space is of dimension greater than 2, then any three points should lie on one plane.
For Desarguesian spaces Georg Hamel proved that every solution of Hilbert's fourth problem can be represented in a real projective space if one determines the congruence of segments by equality of their lengths in a special metric for which the lines of the projective space are geodesics.
Metrics of this type are called flat or projective.
Thus, the solution of Hilbert's fourth problem was reduced to the solution of the problem of the constructive determination of all complete flat metrics.
Hamel solved this problem under the assumption of high regularity of the metric. However, as simple examples show, the class of regular flat metrics is smaller than the class of all flat metrics. The axioms of geometries under consideration imply only the continuity of the metrics. Therefore, to solve Hilbert's fourth problem completely, it is necessary to determine constructively all the continuous flat metrics.
Prehistory of Hilbert's fourth problem
Before 1900, there was known the Cayley–Klein model of Lobachevsky geometry in the unit disk, according to which geodesic lines are chords of the disk and the distance between points is defined as a logarithm of the cross-ratio of a quadruple. For two-dimensional Riemannian metrics, Eugenio Beltrami (1835–1900) proved that flat metrics are the metrics of constant curvature.
For multidimensional Riemannian metrics this statement was proved by E. Cartan in 1930.
In 1890, for solving problems on the theory of numbers, Hermann Minkowski introduced a notion of the space that nowadays is called the finite-dimensional Banach space.
Minkowski space
be a compact convex hypersurface in a Euclidean space defined by
satisfies the following conditions:
is positively definite.
The length of the vector OA is defined by:
A space with this metric is called Minkowski space.
is convex and can be irregular. The defined metric is flat.
Finsler spaces
Let M be a smooth finite-dimensional manifold and its tangent bundle is called Finsler metric if
;
is the Minkowski norm.
is Finsler space.
Hilbert's geometry
be a bounded open convex set with the boundary of class C2 is called the absolute of Hilbert's geometry.
Hilbert's distance (see fig.) is defined by
induces the Hilbert–Finsler metric on U (see fig.), we have
is an ellipsoid, then we have the Lobachevsky geometry.
Funk metric
In 1930, Funk introduced a non-symmetric metric. It is defined in a domain bounded by a closed convex hypersurface and is also flat.
σ-metrics
Sufficient condition for flat metrics
Georg Hamel was first to contribute to the solution of Hilbert's fourth problem. He proved the following statement.
Theorem is flat if and only if it satisfies the conditions:
Crofton formula
is an angle between the line and the x. Crofton proved this statement in 1870.
A similar statement holds for a projective space.
Blaschke–Busemann measure
In 1966, in his talk at the International Mathematical Congress in Moscow, Herbert Busemann, which satisfies the following conditions:
is a set of straight lines passing through a point P;
is a set of straight lines passing through some set X that contains a straight line segment;
is finite.
, then condition 3) should be replaced by the following: for any set H such that H and the closure of H, the inequality
holds.
is defined by
.
The triangle inequality for this metric follows from Pasch's theorem.
Theorem is flat, i.e., the geodesics are the straight lines of the projective space.
-metrics exhaust all flat metrics. He wrote, "The freedom in the choice of a metric with given geodesics is for non-Riemannian metrics so great that it may be doubted whether there really exists a convincing characterization of all Desarguesian spaces".
Two-dimensional case
Pogorelov's theorem
The following theorem was proved by Pogorelov in 1973
Theorem. -metric.
Thus Hilbert's fourth problem for the two-dimensional case was completely solved.
A consequence of this is that you can glue boundary to boundary two copies of the same planar convex shape, with an angle twist between them, you will get a 3D object without crease lines, the two faces being developable.
Ambartsumian's proofs
In 1976, Ambartsumian proposed another proof of Hilbert's fourth problem.
His proof uses the fact that in the two-dimensional case the whole measure can be restored by its values on biangles, and thus be defined on triangles in the same way as the area of a triangle is defined on a sphere. Since the triangle inequality holds, it follows that this measure is positive on non-degenerate triangles and is determined on all Borel sets. However, this structure can not be generalized to higher dimensions because of Hilbert's third problem solved by Max Dehn.
In the two-dimensional case, polygons with the same volume are scissors-congruent. As was shown by Dehn this is not true for a higher dimension.
Three-dimensional case
For three-dimensional case, Pogorelov proved the following theorem.
Theorem. -metric.
to be flat are the following three conditions:
on any plane equals zero,
in any cone is non-negative,
is positive if the cone contains interior points.
-metrics.
Thus Pogorelov could prove the following statement.
Theorem. -metric in generalized meaning.
Busemann, in his review to Pogorelov’s book "Hilbert’s Fourth Problem" wrote, "In the spirit of the time Hilbert restricted himself to n = 2, 3 and so does Pogorelov. However, this has doubtless pedagogical reasons, because he addresses a wide class of readers. The real difference is between n = 2 and n>2. Pogorelov's method works for n>3, but requires greater technicalities".
Multidimensional case
The multi-dimensional case of the Fourth Hilbert problem was studied by Szabo. In 1986, he proved, as he wrote, the generalized Pogorelov theorem.
Theorem. Each n, is generated by the Blaschke–Busemann construction.
-measure that generates a flat measure has the following properties:
-measure of hyperplanes passing through a fixed point is equal to zero;
-measure of the set of hyperplanes intersecting two segments [x, y], [y, z], where x, y та z are not collinear, is positive.
There was given the example of a flat metric not generated by the Blaschke–Busemann construction. Szabo described all continuous flat metrics in terms of generalized functions.
Hilbert's fourth problem and convex bodies
Hilbert's fourth problem is also closely related to the properties of convex bodies. A convex polyhedron is called a zonotope if it is the Minkowski sum of segments. A convex body which is a limit of zonotopes in the Blaschke – Hausdorff metric is called a zonoid. For zonoids, the support function is represented by is an even positive Borel measure.
is even and not necessarily of positive Borel measure. The bodies bounded by such hypersurfaces are called generalized zonoids.
is not generated by the Blaschke–Busemann construction.
Generalizations of Hilbert's fourth problem
There was found the correspondence between the planar n.
There were considered periodic solutions of Hilbert's fourth problem :
Let (M, g Finsler metric on M with the same geodesics as in the metric g is given. Then the Finsler metric is the sum of a locally Minkovski metric and a closed 1-form.
Let (M, g) be a compact symmetric Riemannian space of rank greater than one. If F Finsler metric whose geodesics coincide with geodesics of the Riemannian metric g, then (M, g) is a symmetric Finsler space. The analogue of this theorem for rank-one symmetric spaces has not been proven yet.
Another exposition of Hilbert's fourth problem can be found in work of Paiva.
Unsolved problems
Hilbert's fourth problem for non-symmetric Finsler metric has not yet been solved.
for which k-planes minimize the k-area has not been given (Busemann).
References
Further reading