Научная статья на тему 'Частично центральные состояния на бесконечной симметрической группе'

Частично центральные состояния на бесконечной симметрической группе Текст научной статьи по специальности «Математика»

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Ключевые слова
INFINITE SYMMETRIC GROUP / FACTOR REPRESENTATIONS / QUASIEQUIVALENTNESS / UNITARY IRREDUCIBLE ADMISSIBLE REPRESENTATIONS

Аннотация научной статьи по математике, автор научной работы — Дудко А. В., Нессонов Николай Иванович, Вершик А. М.

Let $\mathfrak{S}_\infty$ be the group of all finite bijections $\mathbb{N}\to\mathbb{N}$. Denote by $\widehat{\mathfrak{S}}_{\infty}^2$ the set of all unitary irreducible {\it admissible} representations of $\mathfrak{S}_\infty^2=\mathfrak{S}_\infty\times \mathfrak{S}_\infty$. We study the factor representations of $\mathfrak{S}_\infty$ that are the restrictions of the representations from $\widehat{\mathfrak{S}}_{\infty}^2$ to $\mathfrak{S}_\infty\times\mathbf{e}$, where $\mathbf{e}$ is the unit element of $\mathfrak{S}_\infty$. It turn out that these representations are of type ${\rm I}$, ${\rm II}_1$ or ${\rm II}_\infty$. The full description for the classes of the quasiequivalent representations is given.

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PARTLY CENTRAL STATES ON THE INFINITE SYMMETRIC GROUP

Let $\mathfrak{S}_\infty$ be the group of all finite bijections $\mathbb{N}\to\mathbb{N}$. Denote by $\widehat{\mathfrak{S}}_{\infty}^2$ the set of all unitary irreducible {\it admissible} representations of $\mathfrak{S}_\infty^2=\mathfrak{S}_\infty\times \mathfrak{S}_\infty$. We study the factor representations of $\mathfrak{S}_\infty$ that are the restrictions of the representations from $\widehat{\mathfrak{S}}_{\infty}^2$ to $\mathfrak{S}_\infty\times\mathbf{e}$, where $\mathbf{e}$ is the unit element of $\mathfrak{S}_\infty$. It turn out that these representations are of type ${\rm I}$, ${\rm II}_1$ or ${\rm II}_\infty$. The full description for the classes of the quasiequivalent representations is given.

Текст научной работы на тему «Частично центральные состояния на бесконечной симметрической группе»

MSC 20C32, 20C30, 22D25

Partly central states on the infinite symmetric

group

© A. V. Dudko, N. I. Nessonov, A. M. Vershik

Phis.-Techn. Inst. Low Temp., Kharkiv, Ukraina;

S.-Petersburg State Univ., S.-Petersburg, Russia

Let 6 ^ be the group of all finite bijections N ^ N Denote bv 6^ the set of all unitary irreducible admissible representations of 6^ = 6^ x 6^. We study the factor representations of 6^ that are the restrictions of the representations from 63^ to 6^ x e, where e is the unit element of 6^. It turn out that these representations are of type I , IIi or II^. The full description for the classes of the quasiequivalent representations is given.

Keywords: infinite symmetric group, factor representations, quasiequivalentness, unitary irreducible admissible representations

1. Characters and traces

Let N be the set of the natural numbers. By definition, a bijeetion s : N ^ N is called finite if the set of i E N such that s(i) = i is finite. Define a group 6^ as the group of all finite bijections N ^ N. For n E N U {0} we have two subgroups: 6n consisting of s such that s(i) = i for all i > n and 6n,^ consisting of s such that s(k) = k for all k ^ n. In particular, 60 is the identity subgroup and 60,^ coincides with 6^,

Definition 2 A function 0 on the group G is called a finite character, if it has the following properties:

(a) 0 is central, that is, 0 (g1g2) = 0 (g2g1), g1,g2 E G;

(b) 0 is positive definite, that is, for all g1,g2,... ,gn the matrix (0 (g^g-1)) is nonnegative;

(c) 0 is normalized, that is, 0 (e) = 1, where e is the unit element of G.

0

of G corresponding to 0 (according to the GNS (Gelfand-Naimark-Segal) construction) is a factor representation.

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A fundamental result of representation theory for Єis a complete description of finite indecomposable characters. To state it we need some notation,

(а, в)

positive numbers а = {а1 ^ а2 ^ ...} and в = {в1 ^ в2 ^ ...} such that

<^k + вk ^ 1.

kk

Denote by А the set of all such pairs (а, в)■

Let us write a permutation s є as a product of disjoint cycles:

S = C1 c2 . . . ct

with lengths l1,l2 ..., lt respectively greater than 1, To any (а, в) є А we assign a function хав on Є^>:

хав (s) = Ц I 3 (аАk - (-вk)lk)

m=1 \ k

In 1964 E, Thoma proved the next important statement

Theorem 3 The functions хав> where (а, в) ranges over А, are exactly the finite indecomposable characters of the group Єте.

The full description of the properly semifinite (non finite) traces on C* (&&,) was obtained by A, M, Vershik and S, V, Kerov [2]. The next proposition contains the corresponding result.

Proposition 4 Let \ be a partition of n є N and 7Л the corresponding irreducible representation of &n. Let (а, в) be Thoma parameters, denote by пав the GNS-representation of &n,^ corresponding to the finite character хав- F°r g є Єп and h є &n,™ pu t Tл а в (gh) = ^(g) ® Пав (h) • Let both sgqugїісєз а and в be finite and

3 <^k + 3 вk = 1, kk

then we have the following two properties:

(i) the representation ПЛав of induced by the representation ^ав of the subgroup &n ■ &n ^ is a ІІте-factor representation of

(ii) the faithful semi-finite trace т on factor ПЛав (&<х)" defines, by the formula т (ПЛав (A)) = тЛав(A), where A є C* (&^)\ semifinite trace тЛав on C* (&x).

The converse of this statement is true. Namely, for any semifinite trace x on C* (&^) there exist n є N a partition X of n and Thoma parameters (а, в) with

x = тЛ а в

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§ 2. Admissible representations of the group ©TO x ©TO

The theory of finite characters on ©O is a special case of a general theory of admissible representations of the group ©O x ©O developed bv G, I, Olshanski and A, Yu, Okounkov,

Let us consider a countable group G and its subgroup K. Denote by SP the set of positive definite functions p on G with p (e) = 1 that are K-biinvariant, This means that p (k\gk2) = p (g) for all g G G and k\,k2 G K, If is a GNS-representation corresponding to p G S^^d is a unit cyclic vector such that p(g) = (nv(g)£v, £p), then nv(k)£v = for all k G K. The set SP is convex.

The following properties are equivalent

p SP

(b) the representation is irreducible.

Let n be a unitary representation of G acting on a Hilbert space H Denote by HK

the subspace of vectors fixed for K, If dim HK = 1, the irreducible representation n

pG

as p(g) = (n(g)£,£), where n is a spherical representation, £ G HK. Hence spherical

SP

Proposition 5 There exists a natural one-to-one correspondence between the set of spherical functions of the pair (©O x ©O, diag ©O) and the set of finite characters on ©o-

G, I, Olshanski [3] initiated the study of a more general class of representations for the group ©O x ©O, To state it we need some notation.

Definition 6 Let n be a unitary representation of G acting on a Hilbert space H

CO

If U H©nTC is dense in H then n is called tame [1],

n=l

Definition 7 A unitary representation n of ©O x ©O is called admissible if its restriction to diag ©O is tame.

Obviously, a spherical representation of a pair (©O x ©O, diag ©O) is admissible,

©O x ©O

©O

gave a construction of examples admissible representations and a conjectural full classification. A, Yu, Okounkov proved Olshanski’s conjecture. We notice that a

©O x e

or e x ©O gives new examples of factor representations for ©O which are dilferent from discussed in Theorem 3 and Proposition 4,

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3. The results

Let n be a factor representation of ©O. We say that n is associated with an admissible irreducible representation n(2) of ©O x ©O if n arises as the restriction of n(2) to the subgroup ©O x e of the group ©O x ©O, Denote by FA the class of all such representations n of ©O,

Let B (H) be the algebra of all bounded operators in a Hilbert space H For a subset S of B (H), its commutant S1 consists of operators T G B (H) such that AT = TA for all A G S, Denote S" = (S')'.

Definition 8 Unitary representations n1 and n2 of a group G are called quasiequivalent, if there exists isomorphism a : n1 (G)" ^ n2 (G)" such that a (n1 (g)) = n2 (g) gGG

P(G) G

p(e) = 1 p G P(G)

GNS-representation is a factor representation. Let PF(G) be the set of all

indecomposable functions from P(G). Let M* stand for the space of all a-weakly continuous functionals on a W*-algebra M. The next important statement is well known.

Proposition 9 Let n be a factor representation of a group G and let u" be a state from n(G)*. Denote u(g) = u"(n(g)). Then u G PF(G) and n is quasiequivalent to the GNS-representation of G.

For a C^^^^bra M denote by Aut M the group of its automorphisms.

Definition 10 Let H be a subgroup of Aut M, A state p on M is called H-central if p(h(m)) = p(m) for all h G H and m G M.

For a unitary u G M define Adu G Aut M by (Adu)(m) = um«*, m G M.

Let n ^e a factor-representation of ©O Define the central depth cd(n) of n as the minimal number n G N U {0} for that there exists an Ad n (©nO)-central state

p G n (©o)*-

Remark 1. If cd(n) = 0 then ^ ^ ^^^^^^ratation of the type IIi,

Proposition 11 If factor representations n1 and n2 of ©O are quasiequivalent, then cd (n1) = cd (n2).

The next statement follows immediately from Definition 7,

Proposition 12 Let n(2) be an admissible irreducible representation of ©O x ©O, and let n1 and n2 be its restrictions to ©O x e and e x ©O respectively. Then n1 and n2 are factor representations with a finite central depth.

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We state here the next important result.

Theorem 13 Let n be a factor-representation of ©O with n = cd(n) < ro, and let u G n (©O)'l be an Ad n (©nO)-central -state. For m G n (©O)'' put

Let E denote the support of u and Eg = Ad n (g) (E). Then

i) for each pair (g, h) G ©O x ©O, we have Eg = Eh or Eg^Eh;

ii) {g G ©o : Eg = E} = {g G ©o : g(i) ^ i for all i ^ n} = ©n ■ ©no/

Theorem 14 The representation nXa^ of ©O, defined in the same manner as in Proposition 4, is a factor representation.

§ 4. Quasiequivalence in the case aj + Y1

fa <1

Here we have the next surprising result.

Theorem 15 If (aj + faj) < 1, then for any partition X the representation

n\a/3 is quasiequivalent to Thoma’s representation nap. In particular, the w*-algebra nXap (©o)” is a IIi-factor.

Let Y be the set of all Young diagrams. Denote bv A1 the subset of Thoma’s parameters (a, fa) such that J2aj + faj = 1-

Theorem 16 If (X, (a, fa)) and (^, (j, 5)) belonging to Y x A1 do not coincide, then the representations n\ap and n^Ys are not quasiequivalent.

Corollary 17 The central depth of the factor representation n\a/3 is equal to |X|.

iii) the algebra En (©O)'' E is a finite factor.

5. The case J^aj + faj = 1

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§ 6. Restriction of the normal semifinite traces to C* (©ro)

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We suppose that J2ai + fai = 1 and |X| ^ 1. Then, bv Theorems 14 and 16,

i i

w*-algebra nXap (©O)'' is a semifinite factor of type IO or IIO, We notice that nXap has the type IO if and only if the total amount of numbers in the collection a U fa is equal to one. In this case the representation nXap is tame [1], Further we assume that nXap has tvpe IIO,

F

factor of type IIO. Let Tr be a normal semifinite trace on F,

Since for any {X a fa} the factors nXap (©O)'' are isomorphic to F, we can assume nXali (©o)'' = F.

Theorem 18 Suppose that '^2ai + fai = 1 |X| ^ 1 and the set a U fa contains

ii

more than one elements. Then the following conditions are equivalent: i) there exists a self-adjoint projection p G C* (©O) such that

0 < Tr (nxa/3(a)) < ro;

aUfa

References

1, A, Lieberman, The structure of certain unitary representations of infinite symmetric group, Trans, Amer, Math, Soe,, 1972, vol. 164, 189-198,

2, A, M, Vershik and S, V, Kerov, Asymptotic theory of characters of the symmetric groups, Funct, Anal, and its Appl,, 1981, vol. 15, No. 4, 15-27.

(G, K)

infinite symmetric group S(ro), Algebra i Analiz, 1989, vol. 1, No. 4, 178-209. Engl, transl.: Leningrad Math. J,, 1990, vol. 1, No. 4, 983-1014.

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