1996
DOI: 10.1090/s0002-9947-96-01512-7
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Some New Homogeneous Einstein Metrics on Symmetric Spaces

Abstract: Abstract. We classify homogeneous Einstein metrics on compact irreducible symmetric spaces. In particular, we consider symmetric spaces with rank(M ) > 1, not isometric to a compact Lie group. Whenever there exists a closed proper subgroup G of Isom(M ) acting transitively on M we find all G-homogeneous (non-symmetric) Einstein metrics on M .

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Cited by 28 publications
(23 citation statements)
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“…for some x 1 > 0 and x 2 > 0. Note, that the subset of SO(2n)-invariant (symmetric) metrics on G/H consists of the metrics with the relation x 2 = 2x 1 [26]. As in the previous case, every SO(2n − 1)-invariant metric on SO(2n − 1)/U (n − 1) is weakly symmetric and, hence, g.o.…”
Section: Theorem 23 Implies Easily the Classification Of Transitive A...mentioning
confidence: 87%
“…for some x 1 > 0 and x 2 > 0. Note, that the subset of SO(2n)-invariant (symmetric) metrics on G/H consists of the metrics with the relation x 2 = 2x 1 [26]. As in the previous case, every SO(2n − 1)-invariant metric on SO(2n − 1)/U (n − 1) is weakly symmetric and, hence, g.o.…”
Section: Theorem 23 Implies Easily the Classification Of Transitive A...mentioning
confidence: 87%
“…There is one further inequivalent (We take the volume to be V = y 2 1 y 2 y 2 3 .) These metrics were found in [15,16], and discussed further in [14]. The first metric is just the standard SO(7)-invariant metric on the Grassmanian SO(7)/[SO(2)×SO( 5)] [14].…”
Section: G 2 /Su(2) Maxmentioning
confidence: 93%
“…We find the Einstein constant and the invariant The metric on the coset G 2 /[SU (2) L ×U (1) R ] is obtained by dividing out the y 4 terms and the last of the three y 3 terms in (5.9): subgroups of G 2 ). The resulting coset space is isomorphic to the Grassmannian G + 2 (R 7 ) = SO(7)/[SO(2)×SO( 5)] of oriented 2-planes through the origin in R 7 [14].…”
Section: G 2 /Su(2) Diagmentioning
confidence: 99%
See 1 more Smart Citation
“…in a pure-state controllable manner) on the homogeneous space SO(2d)/U(d) assuming d ≥ 3. The case d ≥ 4 is discussed in [60]. For d = 3 we have SO(6) ∼ = SU(4) and SU(4)/U(3) = CP 3 (where CP 3 denotes the complex projective space in four dimensions), and it is known that only subgroups of SU(4) isomorphic to SU(4) or Sp(2) ∼ = SO(5) can act transitively on CP 3 (see p. 168 of [61] or p. 68 of [62]; refer also to [63]).…”
Section: B Orbits and Stabilizers Of Quasifree States Under The Actimentioning
confidence: 99%