Dec 9, 2008 - The theory of quantum graphs, i.e. Schrödinger or Dirac operators .... It is easy to see that the characteristic function satisfies ..... Theorem 3.4.
Sep 1, 2010 - arXiv:1009.0298v1 [math.FA] 1 Sep 2010. FUNCTIONS OF ...... and K = clos span{Unh : h â H }. Since 1 is not an eigenvalue of T, it follows that ...
Oct 4, 2016 - of OKN in the stimulus direction allows us to estimate contrast .... calibrated using a photometer (LS100, Konica Minolta, Japan). ..... may have been pooling evidence before responding, driving the average latency up. 0. 0.5. 1.
Sep 5, 2005 - arXiv:math/0509094v1 [math. .... The standard multishift S = (S1,...,Sn) on H is defined by Sif = zif. Again .... (2) T is of class C1 iff θT is outer. ..... The involutive automorphisms of the unit ball Bn are defined [12] by ..... [1
Apr 27, 2015 - A in terms of the quasi-analytic extension of the function f, which has become known ... trace trg(Sα) with a non-smooth function g, as α â â.
Dec 29, 2015 - [29] M.R.James, A quantum Langevin formulation of risk-sensitive optimal ... [49] I.R.Petersen, V.Ugrinovskii, and M.R.James, Robust stability of ...
On the other hand, dyadic Green functions corresponding to different boundary conditions in simple isotropic media have been thoroughly treated in the famous ...
In R the elementary arithmetic is the usual: ▫ + addition. ▫ − subtraction. ▫ *
multiplication. ▫ / division. ▫ ^ raising to a power and operators are used as in a ...
Aug 25, 2009 - FA] 25 Aug 2009. FUNCTIONS OF OPERATORS UNDER PERTURBATIONS OF. CLASS Sp. A.B. ALEKSANDROV AND V.V. PELLER.
Apr 10, 2009 - M. Frazier observed that actually L is the TriebelâLizorkin space F1. â1. Note that ...... ian processes, the problem of majorizing operators), Mat.
with a right hand side with second and third derivative of Dirac delta. There is shown that their solution are influence lines of moments and transverse forces.
Apr 1, 2009 - Bulletin of the Australian Mathematical Society. Article. Article. Aa; Aa .... [27]A.M. Rubinov , Abstract convexity and global optimization (Kluwer, ...
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Edward B Rockowert and N B Abraham$ i. Ketron, Inc., Valley Forge Executive Mall Building 10, Wayne, PA 19087, USA. $ Department of Physics, Swarthmore ...
Feb 4, 2008 - Equivalently, in terms of z = cosh θ and the formal power series expansions of the exponentials, ..... (cosh θⲠâ coshθ)λ+1 ...... John Wiley and.
Oct 16, 2013 - arXiv:1310.4318v1 [math-ph] 16 Oct 2013. Operators versus functions: from quantum dynamical semigroups to tomographic semigroups.
SeeChain, SeeCommerce, SeeRisk, Teradata Decision Experts, Teradata
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Jul 21, 1999 - compact in the case that U is a Behrens roadrunner domain. 1. ...... So fix z0 â U and such a g, and let {fn} be a bounded sequence in. H ...... MR. 43:2482. [14] T. W. Gamelin, Uniform algebras on plane sets, in Approximation ...
Dec 5, 2013 - that there is a joint sample space for all quantum observables, ..... Consider the event representing the random variable A having values.
denote by U the minimal /-unitary dilation of T and by U+ the minimal J- ... circle. Then there exist bounded operators X, Y, Z, W acting on the appropriate.
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume
59, Number
1, August 1976
CHARACTERISTIC FUNCTIONS OF OPERATORS SIMILAR TO UNITARY OPERATORS P. GHATAGE1 Abstract. Suppose T denotes an operator which is similar to a unitary operator and 9T denotes its characteristic function-considered as an operator on H2(DT). It is proved that BTis a bounded operator if and only if it is the inverse of a bounded operator.
In this note we study characteristic functions of operators which are similar to unitary operators. As seen earlier [3], invertibility of the characteristic function is a sufficient condition for a power-bounded operator to be similar to a unitary operator. Now we prove that if an operator is similar to unitary, then being bounded and being invertible are equivalent conditions for its characteristic function. Corollaries showing ways in which the conditions may fail are easily derived. Following the notation in [1] we denote the characteristic function of Fby
8T. Specifically
0T(X)= [-TJT+ \QT*(1 - XT*yxQT]\Q^% where JT = sgn (/ — T* T) and QT = positive square root of |/ — T* T\. We denote by U the minimal /-unitary dilation of T and by U+ the minimal Jisometric dilation of T. The residual space R and the shift-space M are defined in close analogy with the dilation theory for contractions. For explicit definitions and details see [1]. Lemma 1. Suppose T is an operator whose spectrum is contained in the unit circle. Then there exist bounded operators X, Y, Z, W acting on the appropriate
defect spaces such that for \X\ < 1,
(i) tV,(X) = X0TX(X)*Yand (ii) 6jXiX) = Z0T-i(\)*W. For proof see [3, Lemma 2]. Proposition 1. Suppose supu^, ||(>Y(/\)|| < oo and T is similar to a unitary operator. Then supm^, ||0f (A)|| < oo.
Proof.
Following the notation in [1] we denote the residual space of U by
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OPERATORS SIMILAR TO UNITARY OPERATORS
R and the projection
63
onto it by PR. We first prove that PR\H is invertible.
Suppose {hn) C H, \\hn\\ = 1 and ||^A
|| -* 0, i.e., \\hn- JPMthn\\ -> 0. If
s\ipk>0\\T* k\\ = 1/c and say s\ipk>0\\U+ || = a, then let 0 < e < c/2a. For the proof of power-boundedness of U+ see [1, p. 137]. Let n0 be such that \\h„ —JPMth„o\\ < e, and let k„g G M* be a finite sum of the form k„
= 2^0 Un+*h{-Vsuch that ||/>WX - k„o\\N*+l u;kjkn=p+u*kj