1980
DOI: 10.1090/s0002-9939-1980-0572296-4
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Conformal transformations and Clifford algebras

Abstract: Abstract. A spinor representation for the conformai group of the real orthogonal space /tM is given. First, the real orthogonal space RM is compactified by adjoining a (closed) isotropic cone at infinity. Then the nonlinear conformai transformations are linearized by regarding the conformai group as a factor group of a larger orthogonal group. Finally, the spin covering group of this larger orthogonal group is realized in the Clifford algebra Rx +f containing the Clifford algebra RpJt on the orthogonal space R… Show more

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Cited by 27 publications
(4 citation statements)
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“…Remark 2.4. The geometric significance of the conjugation Φ u (x) = uxu −1 is well explained in the paper by Lounesto and Latvamaa [18]. For example, when Q is the quadratic form of signature (p, q) corresponding to the Clifford algebra C p,q and uũ = 1, the following exact sequences exist:…”
Section: Clifford Operator Calculusmentioning
confidence: 92%
“…Remark 2.4. The geometric significance of the conjugation Φ u (x) = uxu −1 is well explained in the paper by Lounesto and Latvamaa [18]. For example, when Q is the quadratic form of signature (p, q) corresponding to the Clifford algebra C p,q and uũ = 1, the following exact sequences exist:…”
Section: Clifford Operator Calculusmentioning
confidence: 92%
“…The smooth composition with translations is best done in the conformal model [1,8,15,17,18,27] of Euclidean space (in the GA of R 4,1 ), which adds two null-vector dimensions for the origin e 0 and infinity e ∞ X = x + 1 2 x 2 e ∞ + e 0 , e 2 0 = e 2 ∞ = X 2 = 0, X · e ∞ = −1.…”
Section: Space Groupsmentioning
confidence: 99%
“…Intuitively all symmetry properties of crystals depend on these vectors. Indeed, the geometric product of vectors [7] combined with the conformal model of three-dimensional (3D) Euclidean space [1,8,15,17,18,27] yield an algebra fully expressing crystal point and space groups [10,13,[19][20][21]. Two successive reflections at (non-) parallel planes express (rotations) translations, etc.…”
Section: Introductionmentioning
confidence: 99%
“…The main difficulty is related to the fact that the point-wise stabilizer of a complete geodesic in Isom + (H 4 ) is isomorphic to SO(3), which is non-commutative, as opposed to the case of H 3 , where the point-wise stabilizer of a complete geodesic in Isom + (H 3 ) is isomorphic to SO(2) and is commutative. To a certain extent, this non-commutativity is reflected by the non-commutativity of A 2 , so that the representation of elements of Isom + (H 4 ) by Vahlen matrices (2 × 2 matrices with entries in A 2 satisfying certain conditions, following Vahlen [27] and more recently Ahlfors and his collaborators and several others ([1]- [6], [21], [28], [29], [30])), is particularly useful and appropriate. This is the approach adopted here.…”
Section: Introductionmentioning
confidence: 99%