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On the Construction of Families of type П1 Subfactors Each Containing a Middle Subfactors
Bahman Mashood1,
, Mahmood Khoshkam1
1Former lecturer at university of Saskatchewan, San Francisco/California
Abstract
In this article we are going to construct a family of type П1 subfactors each containing a middle subfactor. As a result of the above construction we show that the set of the indices of hyperfinite irreducible subfactors contains the interval [37.0037,∞).
Keywords: subfactors, von Neumann algebras, Jones Index, lattice, relative commutants
Received January 09, 2015; Revised April 07, 2015; Accepted June 23, 2015
Copyright © 2015 Science and Education Publishing. All Rights Reserved.Cite this article:
- Bahman Mashood, Mahmood Khoshkam. On the Construction of Families of type П1 Subfactors Each Containing a Middle Subfactors. American Journal of Mathematical Analysis. Vol. 3, No. 2, 2015, pp 44-46. http://pubs.sciepub.com/ajma/3/2/4
- Mashood, Bahman, and Mahmood Khoshkam. "On the Construction of Families of type П1 Subfactors Each Containing a Middle Subfactors." American Journal of Mathematical Analysis 3.2 (2015): 44-46.
- Mashood, B. , & Khoshkam, M. (2015). On the Construction of Families of type П1 Subfactors Each Containing a Middle Subfactors. American Journal of Mathematical Analysis, 3(2), 44-46.
- Mashood, Bahman, and Mahmood Khoshkam. "On the Construction of Families of type П1 Subfactors Each Containing a Middle Subfactors." American Journal of Mathematical Analysis 3, no. 2 (2015): 44-46.
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1. Introduction and Priliminaries
In the next chapter we are going to use locally trivial subfactors to construct a set of middle subfactors. The important of locally trivial subfactos was indicated by S.Popa at [9]. The simplest locally trivial subfactors are those having only two orthogonal projections in their relative commutant. It is well known that these subfactors are isomorphic to Jones subfactors.. Also it is easy easy to show that these kind of subfactors do not posses middle subfactors. For the locally trivial subfactors that their relative commutant have dimension larger than two we believe that the above result is still valid ie’there are no middle subfactors. Suppose we are Given a pair L ⊂ M of subfactors that are limiting algebras of a tower of commuting squares.
Then using the results in [1] we can show that if the inclusion graphs of the corresponding finite C* algebras are A graphs, then the subfactors L ⊂ M do not have middle subfactors. One of the problems in the index theory, is to find the set of all the values for the indices of hyperfinite irreducible subfactors. Using the above constructions, we are going to show that the above set contains the interval (37.0037,∞).
2. Main Results
For a given pair of subfactors N ⊂ M, With [M:N] = λ-1 <∞. Let e be a projection in M that induces the expectation N onto Q = (e)′∩N. Let P1,P2 = 1-P1 be a partition of unity in Q. Using standard argu-ments as in [5], there exists an isomorphism Ф, taking NP1 onto NP2. Let L(P1) be the set of all the elements of the form L(P1) = (x +Ф(x); x∈NP1 ). Then it is well known that L(P1), is a locally trivial subfactor of N. Also by (Lemma2.2.1) [5], [N : LP ] = 1=tr(P1) + 1=tr(P2). Where tr is a unique normalized trace on M. Suppose P1, does not communicate with e0 = e. Set y = P1eP2 ≠ 0. Note that the relative commutant of L(P1), inside M is spanned by the projection P1. Since y, does not communicate with P1, we have that the algebra, H(P1) =< L(P1); Y > is a middle subfac-tor which is strictly larger than L(P1) If under certain conditions H(P1) becomes strictly smaller than M, then H(P1) becomes a proper middle sub-factor. In this case by the above arguments it is easy to see that the inclusions H(P1)⊃ L(P1) and H(P1)⊂M are irreducible inclusion of subfactors. Let us denote r1 = [ H(P1) : L(P1)] and r2 = [M : H(P1)]. Let IR, be the set of all irreducible subfactors of finite index. Let us denote by IIR, the set of indices of all subfactors in IR. Then by (Proposition2.1.15) [5] r1r2 is in IIR. It is easy to check that the set of of the elements f of the form f =∑j∈J ujgzjegwj, with g = EQ(P2), zj∈Q, uj = P1xjP1, wj = P1yjP1, xj∈N yj∈N where J is a set of indices is dense in (H(P1))P1. Let e1 be a projection in N, such that EQ(e1) = λ. Then e1 induces the expectation of Q onto the subfactor Q1 = (e)′∩Q. Next for a number r, r∈IIR, construct an irreducible subfac-tor Q2, Q2⊆Q1, with [Q1 : Q2] = r. We can define the projection e3, Using (corollary 1.8) [13], there exits a projection e3 in Q1, such that e3 induces the expectation of Q2 onto The subfactor Q3, with Q3 = (e3)′∩Q2. This process will induce the following tonnel, M⊃N ⊃ Q ⊃ Q1 ⊃ Q2 ⊃ Q3. Let us set P1 = qe1e3 with q a projection in Q3. Now we can check that the following set of elements, f of the form,
with z =
, with
as in the above and J a set of indices will be a dense subset of (H(P1))P1. In particular assuming now that H(P1) = M implies that the above set of elements are dense in MP1. Furthermore as we mentioned in the above for any number r∈IIR; e3∈Q1 can be chosen such that tr(e3) = r. For example suppose tr(e1) = tr(e0) = .5. Then it is easy to see that there exists a unitary V ∈(e3)′∩N = L, with L a type
Von Neumann algebra, such that V e1V* = 1 − e1. Then we can express the f from the above as f = λ(1 −λ)2e1e3ze1e3 + (e1e3e0V e1e3)(e1e3V*ze1e3). For a given real number S, let [S], be the largest integer which is smaller or equal to [S]. Let us set Sr = S − [S]. Let us assume now that H(P1) = M, We will get the following results.
Lemma 1 Keeping the same notations as in the above let
Then there exist unitary operators U, U2, U3 in L and projection p≤e1, such that f can be expresses as in the following,
With σ1, will be equal to 1 if
odd integer and equal to zero otherwise. Simi-larly σ2 is equal to 1 if
is not an integer and equal to zero otherwise.
Proof First suppose tr(e0)−1 = λ−1 = 2n, for some positive integer n, then let
be a partition of unity by orthogonal projections in L, such that for any odd integer k < 2n, there exists a unitary
, with
. Using our definition of f1 = e1, this implies,
Let
Then U is a unitary in L. Set
The we have,
Next for each 1 ≤ i ≤ n, there exists a unitary
such that
Hence
Next since for
Thus we get
For
let us define
Then it is easy to check
This implies that y = 0. Another useful relation that we will need later is the following equality,
that can be checked easily. Let us define the operator h, with
with, 1≤ i, k ≤ n and
. Then using the above relations we can see that h is a projection, tr(h) = tr(g), and
is orthogonal to h. Hence we get, tr(h) = tr(
) = .5. This will implies that f can be expressed as,
Suppose λ−1 = 2n+1. Then we have the following partition of unity,
. Where the above projections have equal traces. Furthermore ther exists a unitary
such that f can be expressed as,
then we have the following partition of unity by the following projections,
Where σ1 and σ2, can only take values 0 or 1, depending if the corresponding projections f2n+1 and f0 are or are not equal to zero. Furthermore for k ≠ 0, all non zero projections fk's, have equal traces and tr(f0) < λ. Hence generally f can be expressed as,
Where U and U2 are as in the above, U3 a unitary in
and p, is a sub projection of e1 and is in
. At this point note that we can extend U2 and U3 to be unitaries in L. Finally we can express f, as
![]() |
Now let us set the following notations.
and
.
Lemma 2 Keeping the same notations as in the above, and assuming that σ1 and σ2 both different from zero and without loss of generality, we have the following equalities. 
Proof Note that since
commues with all the above operators, drop-ping
from all the operations does not makes any different from the final outcome. So in the following operations we ignore the existence of
. In particular we can identify
with
. Since the proof of the above equalities are very similar, we only show some of the equalities. We have
Hence we get,
Next
Thus
. But we have,
This implies,
. But
is orthogonal
which implies that
. Fur-thermore
Hence we get,
Next
This implies,
But using the above relations,
which implies
Now let us calculate
. Now using the above relations we can show that
hence 
Assuming that Me1e3 is acting standardly on H = [Me1e3 ] and L(P1) = M, the above lemma implies that the operator identity can be spanned by at most four orthogonal projections in G each of trace less or equal to λ. Hence by Remarks(1.4) [13], we get the following Corollary,
Corollary 3 Keeping the same notations as before, for [M:N] > 4, H(P1) is a proper middle subfactor.
As before let IIR represents the set of all indices of irreducible hyperfinite subfactors.
Suppose H(P1) is a proper middle subfactor, ie' L(P1) ⊂ H(P1) ⊂ M, where the inclusions are restrict. Let us denote r1 = [H(P1):L(P1)] and r2 = [M:L(P1)]. Also using the fundamental property of the index of subfactors, r1r2 = r = [M:L(P1)] = [M : N][N : L(P1)]. But [M : N] =λ−1 and [N:L(P1)] = (tr(P1)(tr(P2))−1 Hence r = r1r2 = λ−1(tr(P1)tr(P2))−1 And by the results of [5], r∈IIR. Now notice that by the result of S.Popa in "Subfactors and classification in von Neumann algebras" Corollary(4.4) of the above article indicate the gap in IIR between the values 4 and
. In fact
corresponds to the square of the norm of Coxeter graph E10 and there exists a subfactor of such an index. By its definition P1 = qe1e3 and we had λ = tr(e1) λ1 = tr(e3). Hence tr(P1) = tr(q)λλ1. Let us set c = tr(q), and
then c can take any value in the interval [0,1]. Note also that (λ1)−1 can take any value in IIR larger than .5. Let us denote,
, then
= tr(P1). Note that
can take any value in IIR larger than or equal to
. Hence if we set
then we have
Since q can be taken to be any projection in Q3, tr(P1), can get any value in the interval
. This implies the following theorem.
Theorem 4 Keeping the same notations as in the above, suppose
and
Let N ⊃ M, [M:N]=λ−1 be a pair of irreducible subfactors and lets define a projection p = qe1e3, for some projection q in Q3. Then H(P1) =<L(P1), p1ep2> is a proper irreducible subfactor of M. In particular letting q to vary in Q3, we will get that IIR includes the interval
.
At this end note that by the above arguments there exists a function Ф, acting on the above interval
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