Abstract:Abstract. We consider the analogues of the Horn inequalities in finite von Neumann algebras, which concern the possible spectral distributions of sums a + b of self-adjoint elements a and b in a finite von Neumann algebra. It is an open question whether all of these Horn inequalities must hold in all finite von Neumann algebras, and this is related to Connes' embedding problem. For each choice of integers 1 ≤ r ≤ n, there is a set T n r of Horn triples (I, J, K) of r-tuples of integers, and the Horn inequaliti… Show more
“…As in the result of [3] just mentioned, we have c I J K = c I J K . The general reduction we propose can be described as follows.…”
Section: S = S(e I ) ∩ S(f J ) ∩ S(g K ) ⊂ G(r X)mentioning
confidence: 59%
“…The question arises naturally whether c I J K = 0 if c I J K = 0, so that the reduced problem is still guaranteed to have a solution. That this is indeed the case was shown by Collins and Dykema [3] who proved that in fact c I J K = c I J K .…”
Section: S = S(e I ) ∩ S(f J ) ∩ S(g K ) ⊂ G(r X)mentioning
confidence: 70%
“…This is equivalent with the puzzle description of [8]. Choose unit vectors w 1 , w 2 , w 3 in the plane such that w 1 + w 2 + w 3 = 0.…”
Section: The Littlewood-richardson Rulementioning
confidence: 99%
“…The following figure illustrates the process as applied to a measure m = m ϕ whose support is pictured below, and ν is the measure whose inflation was depicted in the preceding figure. We have oriented all the edges away from the branch point inside 3 , and completed the outline of 6 .…”
Section: Inflations and Fractured Immersionsmentioning
confidence: 99%
“…Let e 1 , e 2 , e 3 be three edges of T adjacent to a vertex V , and assume that e 1 is oriented toward V . These edges are mapped by ϕ to A j X, j = 1, 2, 3, and we must have A 1 X → m XA 2 and A 1 X → m XA 3 . It follows that the edge XB opposite A 1 X satisfies m(XB) = 0, and therefore m 1 (XB) = 0, so that this vertex V contributes nothing to Σ m 2 (m 1 ).…”
Section: Lemma 41 With the Notation Above We Havementioning
We produce a family of reductions for Schubert intersection problems whose applicability is checked by calculating a linear combination of the dimensions involved. These reductions do not alter the Littlewood-Richardson coefficient, and this fact is connected to known multiplicative properties of these coefficients.
“…As in the result of [3] just mentioned, we have c I J K = c I J K . The general reduction we propose can be described as follows.…”
Section: S = S(e I ) ∩ S(f J ) ∩ S(g K ) ⊂ G(r X)mentioning
confidence: 59%
“…The question arises naturally whether c I J K = 0 if c I J K = 0, so that the reduced problem is still guaranteed to have a solution. That this is indeed the case was shown by Collins and Dykema [3] who proved that in fact c I J K = c I J K .…”
Section: S = S(e I ) ∩ S(f J ) ∩ S(g K ) ⊂ G(r X)mentioning
confidence: 70%
“…This is equivalent with the puzzle description of [8]. Choose unit vectors w 1 , w 2 , w 3 in the plane such that w 1 + w 2 + w 3 = 0.…”
Section: The Littlewood-richardson Rulementioning
confidence: 99%
“…The following figure illustrates the process as applied to a measure m = m ϕ whose support is pictured below, and ν is the measure whose inflation was depicted in the preceding figure. We have oriented all the edges away from the branch point inside 3 , and completed the outline of 6 .…”
Section: Inflations and Fractured Immersionsmentioning
confidence: 99%
“…Let e 1 , e 2 , e 3 be three edges of T adjacent to a vertex V , and assume that e 1 is oriented toward V . These edges are mapped by ϕ to A j X, j = 1, 2, 3, and we must have A 1 X → m XA 2 and A 1 X → m XA 3 . It follows that the edge XB opposite A 1 X satisfies m(XB) = 0, and therefore m 1 (XB) = 0, so that this vertex V contributes nothing to Σ m 2 (m 1 ).…”
Section: Lemma 41 With the Notation Above We Havementioning
We produce a family of reductions for Schubert intersection problems whose applicability is checked by calculating a linear combination of the dimensions involved. These reductions do not alter the Littlewood-Richardson coefficient, and this fact is connected to known multiplicative properties of these coefficients.
We characterize in terms of inequalities the possible generalized singular numbers of a product AB of operators A and B having given generalized singular numbers, in an arbitrary finite von Neumann algebra. We also solve the analogous problem in matrix algebras M n (C), which seems to be new insofar as we do not require A and B to be invertible.
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