1935
DOI: 10.1007/bf01199559
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Richtungsfelder und Fernparallelismus in n-dimensionalen Mannigfaltigkeiten

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Cited by 214 publications
(101 citation statements)
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“…If in addition the cost function obeys J (W) = J (QW) for any (m × m) unitary matrix Q, then the solutions to (5) and (6) for the subspace spanned by the rows of W lie within the Grassmann manifold of orthonormal subspaces [21]. If J (W) = J (QW), then the solutions to (6) for W lie within the Stiefel manifold of orthonormal matrices [22]. For a general discussion of the geometric structures of the Grassmann and Stiefel manifolds, see [30].…”
Section: Grassmann and Stiefel Manifoldsmentioning
confidence: 99%
See 1 more Smart Citation
“…If in addition the cost function obeys J (W) = J (QW) for any (m × m) unitary matrix Q, then the solutions to (5) and (6) for the subspace spanned by the rows of W lie within the Grassmann manifold of orthonormal subspaces [21]. If J (W) = J (QW), then the solutions to (6) for W lie within the Stiefel manifold of orthonormal matrices [22]. For a general discussion of the geometric structures of the Grassmann and Stiefel manifolds, see [30].…”
Section: Grassmann and Stiefel Manifoldsmentioning
confidence: 99%
“…Although other adaptive methods could be used, gradient methods represent the simplest to implement and thus form the baseline to which others are often compared. Our algorithms are spatio-temporal extensions of gradient techniques on the Grassmann and Stiefel manifolds [21][22][23][24][25][26][27][28][29][30] and can be applied to any appropriatelydefined cost function. We prove that our algorithms in differential form preserve (2) or (4) over time, and thus they adjust W p in the impulse response space of paraunitary systems.…”
Section: Introductionmentioning
confidence: 99%
“…(M, g) admits a spin structure (see R.P. Geroch [23,24,25] and E. Stiefel [45]) and we choose one. We denote by S (or S A in the abstract index formalism) the spin bundle over M andS (or S A ′ ) the same bundle with the complex structure replaced by its opposite.…”
Section: Spin Structuresmentioning
confidence: 99%
“…Characteristic cohomology classes, defined in modulo 2 coefficients by Stiefel [26] and Whitney [28] and with integral coefficients by Pontrjagin [24], make up the primary source of first-order invariants of smooth manifolds. When their utility was first recognized, it became an obvious goal to study the ways in which they admitted extensions to other categories, such as the categories of topological or PL manifolds; perhaps a clean description of characteristic classes for simplicial complexes could even give useful computational techniques.…”
Section: Introductionmentioning
confidence: 99%