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By Hans Sachs

Der allgemeine Begriff der m-dimensionalen isotropen Mannigfaltigkeit Vm eines kom plexen euklidischen Rn wurde von J. LENSE gepragt und fiihrte zu einer Reihe aufier ordentlich interessanter Untersuchungen (vgl. [92J - [104]). Spater hat M. PINL (vgl. [138J - [160]) diese Thematik unter Aspekten der Riemannschen Geometrie konsequent weiterentwickelt. 1st x = x( Ul, U2, . ., u ) eine m-dimensionale Riemannsche Mannig m faltigkeit Vm, die in einem komplexen eukHdischen Rn(Xl;.. ., xn) eingebettet ist und bezeichnet 8x (0. 1) 8u{3 ihren Mafitensor, so heifit Vm isotrop vom Rang r, wenn Rang (gcx{3) = r m gerne Vm als (m-r)-fach isotrop bezeich internet. Speziell fiir r = zero, d. h. g"'{3 == zero liegen sogenannnte vollisotrope Mannigfaltigkeiten vor, denn fiir das allgemeine Bogenelementquadrat (0. 2) 2 gilt hier ds == o. Diese vollisotropen Mannigfaltigkeiten wurden nicht nur von J. LENSE und M. PINL sondern auch von E. BOMPIANI (vgl. [13J - [17]) studiert. Allgemeine Einbettungsprobleme isotroper Mannigfaltigkeiten in regulare Riemannsche Raume hat vor allem W. O. VOGEL behandelt (vgl. [250J - [254]). Eine zusammen fassende Darstellung iiber den bisher angesprochenen Themenkomplex wird unabhangig von diesem Buch in shape einer Monographie von W. O. VOGEL publiziert werden.

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This e-book by way of Jakob Nielsen (1890-1959) and Werner Fenchel (1905-1988) has had
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Extra resources for Isotrope Geometrie des Raumes

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Ll,y = ~} eine Fixgerade ist. 7) zu erstellen, die z-Achse des zugrundegelegten Koordinatensystems in diese Fixgerade legen; dann folgt ao = Po = O. 7) ist. OX3 = O. Nun kann man durch eine einfach isotrope Bewegung erreichen, daB l* in die Ferngerade der Horizontalstellung faUt, also dutch Xo = X3 = 0 beschtieben witd. Dies bedeutet, daB im zugrundegelegten Koordinatensystem 1'1 = 1'2 = 0 gilt. 9) { i = x cos u - y sin u u y = x sin u + y cos Z = PoU + z 30 an, wobei Po := "(0 'Po gesetzt wurde ..

8 - q3 Pa v'q~ + q~ - v'p~ + p~ 46 einfach isotrope Invarianten. a wird als Abstand und s als Sperrung der beiden Geraden bezeichnet. 22) eine einfach isotrope Invariante, genannt Abstand der beiden Geraden. 23) eine einfach isotrope Invariante, genannt Abstand der beiden vollisotropen Geraden. Beweis: (a): Es seien p und q zwei eigentliche, nichtisotrope Geraden des I~I), beschrieben dureh ihre Plucker-Koordinaten p(Pj), q( qj)(j = 1, ... ,6). Da die Geraden p, q vom Typ a) sind, sind die durch p und q legbaren isotropen Ebenen €p und €q nicht parallel und es existiert somit ihre eigentliche vollisotrope Schnittgerade h := €p n €q.

Hier sind Y£ und YR die Cliffordschen Links- und Rechtsschiebungen (vgl. [230,160m; es gilt U = Ps . 2) Die 6-parametrige Bewegungsgruppe des dreidimensionalen quasielliptischen Raumeso Wieder sind Y£ und YR die entsprechenden Cliffordschen Schiebungsgruppen [230, 177f] und es gilt U = Ps \ g, wobei g eine Gerade in Ps ist. 5. 5 angegebenen Zerlegung in CliffordSchiebungen noch weitere(vgl. [203,142]). Nach CR. 26) die einzige zerlegbare mit ma:vimalem Transitivitiitsgebiet U = As der Faktoren Y£ und YR.

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