1994
DOI: 10.1007/bf01895313
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On third order rotatability

Abstract: Bi-axial rotations, finite matrix groups, information surfaces, invariant subspaces of symmetric matrices, orthogonal groups, permutation groups, response surface designs, tensor representations of classical matrix groups,

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Cited by 18 publications
(5 citation statements)
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“…However, the associated technicalities are not identical, due to the fact that the moment matrices MK, Ms, Mull of the Kronecker, Schliiflian, or Box-Hunter representations differ. It is precisely because of these technical differences that the eigenvalue decomposition of the Kronecker representation moment matrix MK takes an almost explicit form, as in (3.27) of Draper and Pukelsheim (1994). The same could also be achieved under the Sehl/iflian calculus, but we find the details less transparent.…”
Section: Introductionmentioning
confidence: 91%
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“…However, the associated technicalities are not identical, due to the fact that the moment matrices MK, Ms, Mull of the Kronecker, Schliiflian, or Box-Hunter representations differ. It is precisely because of these technical differences that the eigenvalue decomposition of the Kronecker representation moment matrix MK takes an almost explicit form, as in (3.27) of Draper and Pukelsheim (1994). The same could also be achieved under the Sehl/iflian calculus, but we find the details less transparent.…”
Section: Introductionmentioning
confidence: 91%
“…The moment matrix of boundary nucleus designs is given by equation (3.27) in Draper and Pukelsheim (1994). From this we can obtain the eigenvalues as functions of the weight c~ and the radius r, for dimension m _> 3, as follows: …”
Section: Boundary Nucleus Designsmentioning
confidence: 99%
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