Download e-book for kindle: Complex Spaces in Finsler, Lagrange and Hamilton Geometries by Gheorghe Munteanu

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By Gheorghe Munteanu

ISBN-10: 1402022050

ISBN-13: 9781402022050

From a historic perspective, the speculation we undergo the current examine has its origins within the well-known dissertation of P. Finsler from 1918 ([Fi]). In a the classical inspiration additionally traditional type, Finsler geometry has along with a couple of generalizations, which use an identical paintings approach and which are thought of self-geometries: Lagrange and Hamilton areas. Finsler geometry had a interval of incubation lengthy sufficient, in order that few math­ ematicians (E. Cartan, L. Berwald, S.S. Chem, H. Rund) had the endurance to penetrate right into a universe of tensors, which made them examine it to a jungle. To aU folks, who research these days Finsler geometry, it's noticeable that the qualitative jump used to be made within the 1970's via the crystallization of the nonlinear connection inspiration (a inspiration that is virtually as outdated as Finsler area, [SZ4]) and via work-skills into its tailored body fields. the implications acquired by way of M. Matsumoto (coUected later, in 1986, in a monograph, [Ma3]) aroused curiosity not just in Japan, but additionally in different nations comparable to Romania, Hungary, Canada and america, the place faculties of Finsler geometry are based and are shortly broadly recognized.

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Extra info for Complex Spaces in Finsler, Lagrange and Hamilton Geometries

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Finite Mobius Groups and a symmetry of the octahedron that interchanges t he tetrahedron with its dual. An exampl e for th e lat ter is the quarter-turn around the vertical axis. This quarter-turn corresponds to the linear fraction al transformat ion ( f-t i( characterized by z = ei t and w = O. / ( - i ( f-t t ( ,( , t ( _ I ,t (+I , t ( _i,t ( +i' l=0 ,1 ,2 ,3. Finally, we work out th e icosahedral Mobius group I. We inscribe the icosahedron in S 2 such th at th e north and south poles become vertices.

Hence 2d I d(l + 1), and l must be odd . Inspecting the ranges of j and m , we see that 1m - 2j l :::; 2d so that l = ±1. We have 2j = m ± d so that m and d have the same parity, j = (m ± d)/2 . 3. Invariant Forms 41 for l = -1, m :::; d. , the same m) exist iff m = d, and, in this case, the general form is a linear combination of zd and wd. Since ( = z/w , the general Cd-invariant rational function q is a quotient of two linearly independent forms. We obtain that the most general Cd-invariant rational function is a linear fractional transformation applied to (d .

Remark. If K / H is a homogeneous space then H acts on the tangent space To(KI H) at 0 = {H} by the isotropy representation. ) Wolf [1] classified all homogeneous spaces K I H, where the action of the identity component H 0 of H on To(K/H) is irreducible (no invariant linear subspace). Wang and Ziller [2] classified those homogeneous spaces K / H in which the action of H on the tangent space To(KI H) is irreducible, but the action of H o is not. The simplest examples are 80(3)/G, where G are the symmetry groups of the Platonic solids (K = 80(3) and H = G with H o trivial).

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Complex Spaces in Finsler, Lagrange and Hamilton Geometries by Gheorghe Munteanu


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