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18th International Conference on Operator Theory
June 27 - July 1, 2000
University of the West
Timisoara, Romania

Organizers
Dumitru Gaspar, Traian Ceausu, Aurelian Craciunescu, Aurelian Gheondea, Radu-Nicolae Gologan, Ciprian Pop, Dan Popovici, Nicolae Suciu, Alexandru Terescenco, Dan Timotin, Flavius Turcu

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Classes of regular Dilations
by
Dan Popovici
University of the West, Timisoara

As shown by Douglas and Foia s (A Classification of Multi-Isometries, to appear) every completely non-unitary (c.n.u.) bi-isometry V=(V1, V2) is ``modelled'' by a certain isometric pair on H2(E) in terms of two operators on the same Hilbert space E, U unitary and P orthogonal projection, called its unitary invariants. It is our aim in this paper to obtain structure results relative to this model for the minimal regular (respectively *-regular) isometric dilation (introduced by Brehmer and Sz.-Nagy) VT=(VT(1), VT(2)) (respectively VT*) of a given bi-contraction T=(T1, T2) (respectively T*) on a Hilbert space H.


Remark firstly that a minimal isometric dilation of T is c.n.u. iff T1T2 in C·0 (C\alpha, \beta,  \alpha, \beta in {·, 0, 1} represent the Sz.-Nagy-Foia s classes of contractions defined in terms of punctual convergence). Consider contractions ST(i) in L(DT3-i), ST(i)DT3-ih:=DT3-iTih and unitary operators RT(i) in L(D, DST(i)),  RT(i)\DeltaT1/2h=DST(i)DT3-ih,  h in H,  i=1, 2 (\DeltaT:=I-T1*T1-T2*T2+T1*T2*T1T2, D=[`(\DeltaTH)], DZ=(I-Z*Z)1/2 the defect operator and DZ=[`(DZH)] the defect space of a contraction Z). The unitary invariants of VT* are given by the formulas U=A1+A2*, Ai=(Ajk(i))j, k in Z, A10(i)=DST(i)RT(i),  A11(i)=ST(i)*,  A20(i)=-ST(i)RT(i),  A21(i)=DST(i)*,  Aj j-1(i)=IDST(i)* (j >= 3),  Ajk(i)=0 (for other (j, k)), i=1, 2 and P=(Pjk)j, k in Z, Pjj=IDST(2)* (j <= -2), P-1 -1=IDT1,  Pjk=0 (for other (j, k)) on l2Z-*(DST(2)*)\oplusDT1\oplusD\oplusDT2 \oplusl2Z+*(DST(1)*). Having as a starting point a paper of D.Ga spar and N.Suciu (On the geometric structure of regular dilations, Op.Theory: Adv. and Appl., 103(1998), 105-120) we can obtain corresponding results for VT.


Finally, as applications, we characterize the membership of VT and VT* to some special classes of bi-isometries in terms of T. Thus VT(i) is unitary iff Ti,  ST(i) are co-isometries and VT(i) is pure iff Ti,  ST(i) in C·0,  i=1, 2. Moreover VT* is bi-shift, VT is unitary iff Ti are backward shifts and ST(i) co-isometries i=1, 2, VT* is bi-shift, VT(1) is unitary and VT(2) is shift iff T1 is backward shift, T2 in C00,  ST(1) co-isometry, ST(2) in C·0. Similar characterizations are obtained for other remarkable parts of VT and VT*.

Date received: June 15, 2000


Copyright © 2000 by the author(s). The author(s) of this document and the organizers of the conference have granted their consent to include this abstract in Atlas Conferences Inc. Document # caeo-70.