<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">APM</journal-id><journal-title-group><journal-title>Advances in Pure Mathematics</journal-title></journal-title-group><issn pub-type="epub">2160-0368</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/apm.2012.26054</article-id><article-id pub-id-type="publisher-id">APM-24364</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  A Note on Nilpotent Operators
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>bhay</surname><given-names>K. Gaur</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Mathematics, Duquesne University, Pittsburgh, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>gaura@duq.edu</email></corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>11</month><year>2012</year></pub-date><volume>02</volume><issue>06</issue><fpage>367</fpage><lpage>370</lpage><history><date date-type="received"><day>July</day>	<month>16,</month>	<year>2012</year></date><date date-type="rev-recd"><day>September</day>	<month>11,</month>	<year>2012</year>	</date><date date-type="accepted"><day>September</day>	<month>19,</month>	<year>2012</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  We find that a bounded linear operator T on a complex Hilbert space 
  H satisfies the norm relation |||T|
  <sup>n</sup>a|| =2q, for any vector 
  a in 
  H such that q≤（||Ta||-4
  <sup>-1</sup>||Ta||
  <sup>2</sup>)≤1.A partial converse to Theorem 1 by Haagerup and Harpe in [1] is suggested. We establish an upper bound for the numerical radius of nilpotent operators.
 
</p></abstract><kwd-group><kwd>Numerical Range; Numerical Radius; Nilpotent Operator Weighted Shift; Eigenvalues</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The motivation for this note is provided by the results obtained in [1-4]. Let T be a bounded linear operator on a complex Hilbert space H. The numerical range of T, denoted by W(T), is the subset of the complex plane and</p><p><img src="2-5300237\05d1a1b3-c6ed-4a9b-8766-ab2f199fe27a.jpg" /></p><p>The numerical radius of T is defined as,</p><p><img src="2-5300237\89dc8b62-7e40-4919-87ee-f37dd4c40ea6.jpg" /></p><p>The following lemma is known and is an easy consequence of the definitions involved.</p><p>Lemma 1.1.<img src="2-5300237\4bf75ca4-bd9e-462b-a89a-4a00dd4e33c1.jpg" />, where T<sup>*</sup> is the adjoint operator of T and <img src="2-5300237\6a081ec8-f9fd-41e4-88f4-a26bed375164.jpg" /> is the complex conjugate of<img src="2-5300237\9721eb60-b41e-4dc8-abab-e89c4801cb7b.jpg" />.</p><p>Berger and Stampfli in [<xref ref-type="bibr" rid="scirp.24364-ref2">2</xref>] have proved that if <img src="2-5300237\b9b82f78-e261-4976-be44-aa4f62d84fdc.jpg" /> and<img src="2-5300237\6036e57a-ac4d-4530-a754-99154d5bd90f.jpg" />, for some n, then<img src="2-5300237\7f46cf8a-45f6-43e2-aa84-7e0ec78f9344.jpg" />. Also, they gave an example of an operator T and an element <img src="2-5300237\a5ea2289-8dcd-4d65-9b53-49de827e9c4d.jpg" /> such that <img src="2-5300237\d7c94bc6-c6bc-4bfc-bc1e-ff65fa09a62f.jpg" /> implies that <img src="2-5300237\e172aab1-b6b0-4b83-b604-78adcc879ca3.jpg" /> and<img src="2-5300237\64523e7d-7fb2-4002-b141-033ddd6f6888.jpg" />. In Theorem 2.1, we present a different proof of their result in [<xref ref-type="bibr" rid="scirp.24364-ref2">2</xref>] and show that <img src="2-5300237\131f0ab6-08de-4526-9969-452c490500f0.jpg" /> is indeed the best constant.</p><p>Theorem 2.1 also generalizes the result in [<xref ref-type="bibr" rid="scirp.24364-ref4">4</xref>] and provides a partial converse to Theorem 1 in [1, p. 372].</p><p>Our next main result in Theorem 2.3 gives an alternative and shorter proof of Theorem 1 in [<xref ref-type="bibr" rid="scirp.24364-ref1">1</xref>].</p><p>Applying Lemma 2 and Proposition 2 of [<xref ref-type="bibr" rid="scirp.24364-ref1">1</xref>], a new result on the numerical range of nilpotent operators on H is obtained in Theorem 2.4. This gives a restricted version of Theorem 1 in [<xref ref-type="bibr" rid="scirp.24364-ref3">3</xref>].</p><p>Finally, two examples are discussed. Example 3.1 deals with the operator<img src="2-5300237\af0fe0a9-c699-4204-9a03-79806f9f28da.jpg" />, where 1 is not the eigenvalue of <img src="2-5300237\bb780a80-dba8-40bd-8be5-95d47147ca8a.jpg" /> if<img src="2-5300237\eeda6333-ac5d-46e0-915b-bd6fdc49ff3b.jpg" />. Example 3.3 justifies why <img src="2-5300237\ca96d81a-3e0c-4f3f-8603-68dea8400947.jpg" /> fails to increase until and unless<img src="2-5300237\b7beddef-62a7-4626-a724-c0d70380ecf4.jpg" />.</p></sec><sec id="s2"><title>2. Main Results</title><p>Theorem 2.1. The following statements are true for a bounded linear operator T on a Hilbert space H with<img src="2-5300237\07b3ca8a-8ee2-451a-8b78-a60f1f14de0e.jpg" />.</p><p>1) <img src="2-5300237\8b982159-fa9c-4590-a3da-c5d31934c6ba.jpg" />such that</p><p><img src="2-5300237\43d489aa-3d94-4fb7-9fed-cafb61df79b3.jpg" />,<img src="2-5300237\219e95fd-7a1c-4d7f-a6fa-93dc78434852.jpg" />.</p><p>2) If <img src="2-5300237\2511be3c-d630-450a-a1db-2bd8d40175e7.jpg" /> for some integer n, then</p><p><img src="2-5300237\8721e5a3-bbcb-4917-bd6c-04acc0a2bd77.jpg" />and<img src="2-5300237\573bfb32-3f7f-4bfb-8217-12a47d9f7a10.jpg" />.</p><p>3) The set <img src="2-5300237\a2026233-87c9-45e8-934a-1af5f75bf8be.jpg" /> forms a nontrivial subspace of T so that its orthogonal complement is invariant.</p><p>Proof. 1) For each real number <img src="2-5300237\d10116ea-5efc-4ae1-90d9-cd1ad8997361.jpg" /> and a postive integer, n, let<img src="2-5300237\a161a135-bed4-4e1b-bd2d-2c5c7f84846b.jpg" />. Then the inner product relation <img src="2-5300237\8529e22d-9d28-43d1-bba6-9652af3f26c7.jpg" /> implies that</p><p><img src="2-5300237\41513ca8-7f74-4d8b-b147-2db732410a14.jpg" /></p><p>That is,</p><p><img src="2-5300237\bfc4a1bf-fa40-4d76-b1a7-10a15ce2b7cf.jpg" /></p><p>Hence,</p><p><img src="2-5300237\78a1c11e-c71e-423b-adeb-6af7d5aaa942.jpg" /></p><p>Since</p><p><img src="2-5300237\261d302b-3654-4ed3-9f8a-2e2b95f5ec2e.jpg" /></p><p>it follows that</p><p><img src="2-5300237\073ad77e-4698-4e22-a6a4-7b45c9af68c1.jpg" /></p><p>Dividing the above inequality by<img src="2-5300237\c60dded3-4858-4a4f-bd66-93a053b34a88.jpg" />, we have</p><p><img src="2-5300237\fd486c09-c497-4893-a21d-e34ea55b8d20.jpg" /></p><p>Let <img src="2-5300237\facb787a-1a59-45a9-ad88-870b88bca582.jpg" /> be the following block-diagonal matix of order n and</p><p><img src="2-5300237\960b35b4-06c6-48fb-b9d8-1b80fffeefb1.jpg" /></p><p>If γ<sub>n</sub> denotes the determinant of <img src="2-5300237\6c90583f-2a2a-474a-8e11-ecb9006fdf0b.jpg" /> such that <img src="2-5300237\b9f891b2-877b-491c-a489-095c73684843.jpg" /> then the value of γ<sub>n</sub> is positive because all principal minors of <img src="2-5300237\b6732f93-7395-407c-a05c-83ac0d6e768b.jpg" /> are nonnegative. Suppose that <img src="2-5300237\95ffb0a2-eb24-443d-913b-355075f05d68.jpg" /></p><disp-formula id="scirp.24364-formula59509"><label>(2.1)</label><graphic position="anchor" xlink:href="2-5300237\26bf9da5-14bf-4f44-8b83-a905851ecc1a.jpg"  xlink:type="simple"/></disp-formula><p>We consider the following cases:</p><p>Case 1. If<img src="2-5300237\27ee091b-7e9f-493a-9538-193b5e3140a3.jpg" />for the least<img src="2-5300237\7560ac0f-318a-49d9-91cf-98c0280cb7a8.jpg" />then</p><p><img src="2-5300237\ed0132cf-4f90-4b87-bccf-6383a11b64a5.jpg" />and <img src="2-5300237\b100c5cf-e036-4aac-8965-a31c47b7e5a6.jpg" /> converges to zero.</p><p>Case 2. Let <img src="2-5300237\fdd7bed0-5d21-4a0e-990a-95d1bcbe6a5e.jpg" /> for all<img src="2-5300237\4acae98a-9e5d-464e-854f-15cc7db59701.jpg" />. Then</p><p><img src="2-5300237\2ec480db-ce07-4499-8a46-4217b2de9363.jpg" />and by induction</p><p><img src="2-5300237\43e2b128-1f2b-4d1b-a1dd-e572fde6c2da.jpg" /></p><p>Further, the inequality</p><p><img src="2-5300237\62d67b45-282d-4e15-bd1f-b3ec860bb0e3.jpg" /></p><p>implies that <img src="2-5300237\16a232f9-4395-4303-919e-0e9d839a131a.jpg" /> converges to q as n goes to infinity for some q ≥ 0. Therefore from Equation (2.1), <img src="2-5300237\94f137d9-d21f-4217-9fba-7faf1c04359a.jpg" />as<img src="2-5300237\9b2b86c4-5f75-4125-8ba8-9f97c492e3f4.jpg" />. Thus<img src="2-5300237\6460730b-3283-4344-81d6-0ca587663640.jpg" />. Obviously, q = 1 only if<img src="2-5300237\58ca7a5f-e972-45ac-b5cc-65d2478413ea.jpg" />.</p><p>2) By the assumption, <img src="2-5300237\be6c728f-3348-4797-8cb1-36f0da2db57f.jpg" />for some positive integer n. Now fom Equation (2.1), we obtain:</p><p><img src="2-5300237\f7dafee0-919c-404a-b52e-42d8510f23be.jpg" /></p><p>and <img src="2-5300237\70818541-d38e-475d-8959-3a9747fd77ed.jpg" /> so that<img src="2-5300237\76568095-db52-4e21-a392-4888cf1f07cb.jpg" />. The equality,</p><p><img src="2-5300237\046a9115-dc4f-4206-9166-f6159b114845.jpg" />now follows from (a) and thus<img src="2-5300237\587cd65a-a6b0-45cc-a9bc-b3756033a550.jpg" />. Also, <img src="2-5300237\d2cdcea0-51f3-416a-81f0-73e33d3143ea.jpg" />which gives <img src="2-5300237\a3b44b60-b928-443d-bee4-b29071688be4.jpg" /> since<img src="2-5300237\b3b3ca1b-2714-40bc-ba23-1cf7f1915e3e.jpg" />.</p><p>3) To prove this case, we assume that if the vector <img src="2-5300237\52ecf880-e75c-4d8e-9d2c-cd27b3ce901c.jpg" /> is orthogonal to the spanning set <img src="2-5300237\9bb27b1f-b171-4dc8-a404-03090b308e08.jpg" /> then<img src="2-5300237\00386dc3-a7d0-4aeb-9935-7789de082a0b.jpg" />. Let</p><p><img src="2-5300237\721dc4a5-42ea-4ab7-9eec-2e65bff2334a.jpg" />, for<img src="2-5300237\3c4623b9-6d4d-4c39-a2e1-632ce64713b6.jpg" />. Then</p><p><img src="2-5300237\5cc23856-bdb1-4567-9091-b44e54c0256a.jpg" /></p><p>Hence, <img src="2-5300237\3de7b331-c012-489a-8fe9-0c8f6b70192e.jpg" />for <img src="2-5300237\45e3842b-e69d-497f-bc03-d57ae4a50a59.jpg" /> and the spanning set <img src="2-5300237\0469d69e-bdcf-447f-85f7-d355430472fc.jpg" /> is a non-trivial invariant subspace on T.</p><p>In [2, p. 1052], an example of an operator T on <img src="2-5300237\1ba7db1c-a95c-47a2-a781-a16b073bf305.jpg" /> and an element x in H with<img src="2-5300237\babb8b98-91e0-47f0-b82a-d4bf864068b7.jpg" />, is given where</p><p><img src="2-5300237\5b3cfecb-d8ca-4cbd-818e-cbd54b5c1954.jpg" />. Theorem 2.1 above establishes that <img src="2-5300237\6e7142de-3d76-4a47-9c1d-280fc067aac5.jpg" /> is the best constant in this case.</p><p>Remark 2.2. An operator A on H is hyponormal if</p><p><img src="2-5300237\9e2d0657-9a43-4ad7-b36b-5b46fe06e3cf.jpg" />. Let <img src="2-5300237\70dcf3c3-8186-4404-b9ec-cf4edf40e9dd.jpg" /> then<img src="2-5300237\93f07b7d-4ebd-453f-97b1-7cdc2674a2fc.jpg" />if A is a hyponormal operator. Hence, <img src="2-5300237\bf295b58-6aeb-42bf-b7b6-a0b6b2e5a7cd.jpg" />, <img src="2-5300237\2708da40-1a50-4574-94c2-bb6d9027e3e5.jpg" />and the set of vectors <img src="2-5300237\9ce1f491-de84-40d0-b8ba-97a8a9ade78c.jpg" /> forms a reducing subspace of A.</p><p>A natural connection between Feijer’s inequality and the numerical radius of a nilpotent operator was estaplished by Haagerup and Harpe in [<xref ref-type="bibr" rid="scirp.24364-ref1">1</xref>]. They proved, using positive definite kernals, that for a bounded linear operator T on a Hilbert space H such that <img src="2-5300237\b2dd79bf-ff4b-4b3d-a9c9-2355f2c8189e.jpg" /> and<img src="2-5300237\e6faa13c-89c1-4ede-968a-979eaafcee05.jpg" />then<img src="2-5300237\ef33e384-d29a-4637-9758-493a2347b217.jpg" />. The external operator is shown to be a truncated shift with a suitable choice of the vector in H. The inequality is related to a result from Feijer about trigonometric polynomials of the form</p><p><img src="2-5300237\a754ba04-9c0c-40d5-86ba-c4db7060449d.jpg" />with<img src="2-5300237\58534fb2-102c-46f8-8ee4-3c016a09450c.jpg" />. Such a polynomial is positive if <img src="2-5300237\6a817ba1-105d-47d9-bdff-b28adf8bec72.jpg" /> for all<img src="2-5300237\b93efa27-4c85-4588-8b17-7abb6a55fa4a.jpg" />. Here, we present a simplified proof of Theorem 1 in [<xref ref-type="bibr" rid="scirp.24364-ref1">1</xref>].</p><p>Theorem 2.3. For an operator N on H with <img src="2-5300237\380ce0d5-e5f9-46ca-ae1a-add865123625.jpg" /> and<img src="2-5300237\7cc45763-9246-467a-a04d-49d0eed16a21.jpg" />, we have<img src="2-5300237\28e1f62e-df63-4ff1-929f-367fcc0da626.jpg" />.</p><p>Proof. We will follow the notations of Theorem 1 in [<xref ref-type="bibr" rid="scirp.24364-ref1">1</xref>]. Let S be the operator on <img src="2-5300237\74581d47-6fee-444d-804b-4b98f3be2b87.jpg" /> and<img src="2-5300237\edd447d8-8c7d-4766-9fda-4bbf02442732.jpg" />, <img src="2-5300237\a99864f0-9946-43d3-ac80-184bd586dee2.jpg" />be the basis in<img src="2-5300237\0569a015-be8a-4367-9bc2-97677cb7c47a.jpg" />. We define the operator S as follows:</p><p><img src="2-5300237\f0f796ae-5b98-4ef7-9e2e-34d72a400db4.jpg" />and <img src="2-5300237\623feffd-eb4b-4e7d-91f3-c087392069ea.jpg" /> for <img src="2-5300237\74b68237-2211-40f4-80f9-b6bb6f2e3238.jpg" /></p><p>The matrix for S gives a dialation for T. Let A be the matrix for S and</p><p><img src="2-5300237\453a4516-2517-4298-a451-421fe02b2184.jpg" /></p><p>If <img src="2-5300237\2771b218-3757-4c8a-a65c-4310b42953ec.jpg" /> is a unitary operator on <img src="2-5300237\ceb4a4d1-e814-4863-b4f3-99d659603b67.jpg" /> with diagonal <img src="2-5300237\0a93686d-2dd7-4703-a530-28194afee468.jpg" /> then<img src="2-5300237\8914fbc9-0b48-43eb-9afa-2ed287663009.jpg" />. By Lemma 1, we have:</p><p><img src="2-5300237\087469d7-fd09-4548-890c-da4a2ee2292e.jpg" /></p><p>This helps to define the characteristic function of a contraction.</p><p>For the operator N on H, let <img src="2-5300237\9c1ad12b-7255-4554-aeb6-65e175e9f1ae.jpg" /> then</p><p><img src="2-5300237\75c12c9f-c46c-4881-8e02-1330f752ff6c.jpg" />is a positive operator and <img src="2-5300237\beb6897e-cab1-423b-994c-26f0b238d992.jpg" /> depends on N. Let the range of <img src="2-5300237\3ab9742c-3be4-48be-a761-2dc4de51f8e1.jpg" /> be denoted by<img src="2-5300237\d24a533d-a049-4e60-b510-13d591647bfe.jpg" />. Then the tensor product, <img src="2-5300237\ca48dcfc-6d31-4890-a36c-acbb6db1314c.jpg" />, is a Hilbert space. We define the map <img src="2-5300237\c80cedf2-0f33-4b8d-a765-aae9ce291bea.jpg" /> so that F is an isometry.</p><p>For λ, let <img src="2-5300237\5a2c0dad-929f-43a8-bfd0-b520b888889b.jpg" /> where <img src="2-5300237\526c79ac-a642-4e1c-87fd-ae3a2594d5b3.jpg" /> I is the identity operator, and <img src="2-5300237\64a8e087-594d-4798-83d4-95ea9b68bb66.jpg" /> is an operator on<img src="2-5300237\5e3e42e8-3e39-477b-8b4a-4d31a8e4f5b1.jpg" />.</p><p>Therefore <img src="2-5300237\4ad074db-c90b-45e7-a345-3cca9ceb213e.jpg" /> and<img src="2-5300237\04354699-f886-41df-a8ec-34785e3420a3.jpg" />.</p><p>Now, we claim that<img src="2-5300237\380fbd4f-028d-4d95-9682-8299a371c123.jpg" />, for we hope that <img src="2-5300237\f2f20732-2073-4c7e-b2f1-04cbd6df3cd8.jpg" /> By Lemma 1.1</p><p><img src="2-5300237\a153c579-8b93-4363-80ec-d496c574d05b.jpg" /></p><p>That is,<img src="2-5300237\13d8c1d1-512b-427f-a3e3-e64623a4f5de.jpg" />.</p><p>Since<img src="2-5300237\4bf1de09-7749-4af3-9b3a-33ebcd551a66.jpg" />, we have:</p><p><img src="2-5300237\f7741965-7ff6-4094-8386-0416d75facb8.jpg" /></p><p>and</p><p><img src="2-5300237\77256940-c09a-4d13-9ee2-be3a08a4147a.jpg" /></p><p>where <img src="2-5300237\a0c03486-b3c9-4927-bbc9-9cde30086090.jpg" /> is the spectral radius of<img src="2-5300237\76852ea6-02f3-4e20-a8bb-e6d322747ecd.jpg" />. By the definition of the spectral radius, we have the characteristic polynomial f such that <img src="2-5300237\c18f1e75-9e0d-4da2-bcf7-1c3851ffb8f7.jpg" /> by [5, p. 179, Example 9], the roots of <img src="2-5300237\b990c040-7d92-4af9-ad1f-57400b721cfa.jpg" /> are given by</p><p><img src="2-5300237\ca36ed0c-3740-43d3-972b-6f48cf9d0fc0.jpg" />,<img src="2-5300237\aedd31b4-112a-4192-9f30-16d074c2e9e4.jpg" /> and <img src="2-5300237\421f9b88-d7ad-45a8-83a9-273f324c5ba1.jpg" /> and</p><p><img src="2-5300237\462d1e56-4ee2-4839-bb8d-71ccbd71bd1e.jpg" />.</p><p>Karaev in [<xref ref-type="bibr" rid="scirp.24364-ref3">3</xref>] has proved, using Theorem 1 in [<xref ref-type="bibr" rid="scirp.24364-ref1">1</xref>] and the Sz.-Nagy-Foias model in [<xref ref-type="bibr" rid="scirp.24364-ref6">6</xref>] that the numerical range <img src="2-5300237\ef057bc1-0714-44b7-ae84-e0c45636e838.jpg" /> of an arbitrary nilpotent operator N on a complex Hilbert space H is an open or closed disc centered at zero with radius less than or equal to<img src="2-5300237\869ccb53-95b1-47f7-b9f5-39910b95a4cf.jpg" />, <img src="2-5300237\296ca24b-8af4-4403-a3b8-b98dcd5d0376.jpg" /></p><p>Using Theorem 2 and the assumption that</p><p><img src="2-5300237\716f1df7-43cd-47bf-9e6b-6b9b94850001.jpg" />, <img src="2-5300237\e979b300-3dd4-448f-a4f6-63b56b970e59.jpg" />, we have <img src="2-5300237\781cbfbd-b7f5-407b-81e3-f3b535272d00.jpg" /> as a closed or an open disc centered at zero with radius equal to<img src="2-5300237\e989a8f2-7f92-41c8-9b6f-ec209dfedbff.jpg" />. In fact, we have the following theorem.</p><p>Theorem 2.4. For a nilpotent operator N on H with<img src="2-5300237\8d96aa47-7c00-48fc-81a1-f991ff9ea07f.jpg" />, <img src="2-5300237\df606c06-51fa-48a6-b3d3-658e106c38e7.jpg" />and<img src="2-5300237\0cf1cb98-9d8e-4afc-acea-3bf49f5daebc.jpg" />, the numerical range <img src="2-5300237\1946477c-f3f7-468f-bb6b-17eb50d78e6b.jpg" /> is a disc centered at zero with radius<img src="2-5300237\27f4f7fc-1401-443e-8998-dcc57dceaca9.jpg" />.</p><p>Proof. For any <img src="2-5300237\b8e4cb6e-5043-478d-b013-b08221e50cd7.jpg" /> we must claim that<img src="2-5300237\2f8af649-45cd-497a-85ad-668e3e15f3ea.jpg" />, for <img src="2-5300237\405c83fe-9a24-47ec-90b2-3390c2296f1b.jpg" /> and <img src="2-5300237\92426ba3-35fb-4325-a1e5-6fc007fe75a2.jpg" /> is a vector in<img src="2-5300237\4f5e0f75-86ae-4713-b5f4-c04ddad1c962.jpg" />.</p><p>From [1, p. 374, Proposition 2], we have<img src="2-5300237\e7e90886-049f-44b8-8205-c24ec04bc28e.jpg" />. Also, for some<img src="2-5300237\3591aefd-8049-42ba-9302-e99b4a6fc9cd.jpg" />,</p><p><img src="2-5300237\c3150e8c-0c79-4f9b-b9e3-777c13b4b3ec.jpg" />. Now by [<xref ref-type="bibr" rid="scirp.24364-ref1">1</xref>] [P.375, Lemma 2], we obtain:</p><p><img src="2-5300237\8980c10c-89db-4d9a-802c-e0d7a4cf410d.jpg" /></p><p>and</p><p><img src="2-5300237\73948073-be81-4df8-8825-3506187bdf22.jpg" /></p><p>Let<img src="2-5300237\2626090e-ca0a-48b0-ba86-a8698e602fae.jpg" />. Then:</p><p><img src="2-5300237\b8c8d244-ed60-485a-ac72-edd29fa8b589.jpg" /></p><p>and the theorem follows from above since <img src="2-5300237\28b59dc3-8ad1-45a3-88ae-44c1a249b06b.jpg" /> is arbitrarily chosen.</p></sec><sec id="s3"><title>3. An Application</title><p>An operator A is a unilateral weghted shift if there is an orthonormal basis <img src="2-5300237\8590d736-b593-4a88-ac1f-bd6bd58d7801.jpg" /> and a sequence of scalers <img src="2-5300237\647a7a11-4723-49c1-9cf2-768dd5a98ee4.jpg" /> such that <img src="2-5300237\4cb9b0ff-5dc6-4445-99f9-e5ae035e69b7.jpg" /> for all<img src="2-5300237\a17f243e-a6a3-4b28-b858-cb1010811460.jpg" />. It is easy to see that <img src="2-5300237\f3891226-d402-411a-a99e-7cb5f56a3e5c.jpg" /> where S is the unilateral shift and D is the diagonal operator with<img src="2-5300237\8b296303-8054-40a4-b655-81aad1e1ea4e.jpg" />, for all n.</p><p>Thus, <img src="2-5300237\5485cf46-7733-4de1-8efb-a1e8e0700042.jpg" />and <img src="2-5300237\38ecb2bb-c8d3-4e33-b0d3-cfbf38239736.jpg" /> for all n. So <img src="2-5300237\6773d52b-f958-46a3-be95-5ec9e20f4c07.jpg" /> is the basis of eigenvectors for<img src="2-5300237\919e2ca3-91f6-4069-8e10-b2fde3c02f23.jpg" />. Also, note that A is bounded if <img src="2-5300237\a112531a-1907-4184-b6d9-7a63a21ebe68.jpg" /> is bounded.</p><p>If A is a unilateral shift then <img src="2-5300237\a231a92d-ec32-43c2-80fa-e2ff6098a4eb.jpg" /> and <img src="2-5300237\fc81115c-87a2-4b61-97b3-49c1a7d025d6.jpg" /> for<img src="2-5300237\9e146a3a-cd7f-42f0-b05c-bcf8d13873c5.jpg" />. Consequently, for a hyponormal operator A, <img src="2-5300237\7bafe406-e089-4a0b-a7d8-7155d4ca82d8.jpg" />and <img src="2-5300237\3c3e51d2-1330-47af-96fd-5a1fdb6fa24c.jpg" /> for<img src="2-5300237\d25d2d37-85a1-4526-a9aa-ade9806bd928.jpg" />. A wighted shift is hyponormal if and only if its weight sequence is increasing.</p><p>Example 3.1. Let <img src="2-5300237\e707a5b1-22d7-4118-80fa-7ca7c72f9af1.jpg" /> be an operator on <img src="2-5300237\572e8c6c-3a02-4503-b80a-982d680b6b23.jpg" /> such that <img src="2-5300237\934c402b-17cc-4a60-b08f-91ce7d74dbe5.jpg" /> and <img src="2-5300237\e548dbda-a027-461c-b1e4-29f7793687fe.jpg" /> for <img src="2-5300237\6d219819-9641-48ba-a69b-274c64cb57ba.jpg" /> and<img src="2-5300237\be9b9082-4a3e-4a26-a855-24d7c15e70b2.jpg" />. Here, we show that <img src="2-5300237\94df3b8b-74b8-4f24-a6e5-05f65a884c33.jpg" /> is not an eigenvalue of <img src="2-5300237\3904b5dd-ecb3-4d2f-a4ef-0995efbb350f.jpg" /> if</p><p><img src="2-5300237\09cca1d0-bc77-43d9-9d15-77cbb705642b.jpg" />. We prove our claim by contradiction Let <img src="2-5300237\b90d7883-7d32-435d-ae27-4cdd547f59f5.jpg" /> be an eigenvalue of<img src="2-5300237\9b5ba5dc-892e-48d1-a024-f5fe8031cf9f.jpg" />. Then, there exists <img src="2-5300237\2edf1cc2-3b2a-4f8d-8665-9055692b8cd7.jpg" /> with <img src="2-5300237\cfea85a4-53a4-4ed3-a124-3a66a2aea015.jpg" /> and<img src="2-5300237\a327d6fc-e186-453a-a80d-84c21a356ed1.jpg" />, n = 2, 3, &#183;&#183;&#183;. It is not hard to see that:</p><p><img src="2-5300237\ee08af08-bf5c-4c07-8cfa-7a4b429693ef.jpg" /></p><p>For<img src="2-5300237\c034cdd4-309e-42b4-8f09-7c8d9e7550a4.jpg" />, we have <img src="2-5300237\7075b8ee-abe4-462a-8bd5-2c27560e9904.jpg" /> and thus<img src="2-5300237\472305d9-bc10-43cc-a880-40746b25fdaf.jpg" />, which shows that<img src="2-5300237\2c0d77dc-f234-47ae-b033-71d730449685.jpg" />, contrary to our assumption. Thus, <img src="2-5300237\1832453b-3088-4c0a-8747-1b276ad0c048.jpg" />is not an eigenvalue of <img src="2-5300237\53a8fe50-7543-4121-970c-e6f7463a2317.jpg" /> if</p><p><img src="2-5300237\e3c36cb1-584f-41db-9bad-d71f6427082e.jpg" />.</p><p>Remark 3.2. Following [<xref ref-type="bibr" rid="scirp.24364-ref2">2</xref>], if <img src="2-5300237\03062437-c0fd-49bc-8983-abf1bbb438f7.jpg" /> then</p><p><img src="2-5300237\25fb5633-131c-4652-8025-c116f79ab219.jpg" /></p><p>Therefore, the numerical radius, <img src="2-5300237\a61375d3-fe00-4ba2-b42c-60630a2808e2.jpg" />is equal to 1.</p><p>The example below shows that there exists an operator <img src="2-5300237\3777a52a-aaac-45cb-9599-c1861c6edb9c.jpg" /> such that <img src="2-5300237\4e0c1277-bea8-4c35-9d14-34a6466ffe50.jpg" /> for<img src="2-5300237\e63057a8-f83f-419b-a9bb-6be21cc423b2.jpg" />.</p><p>Example 3.3. Let <img src="2-5300237\504a4200-9b8d-42c5-84c6-dc42ad36e7f2.jpg" /> be a unilateral shift. If <img src="2-5300237\b8a7a357-f5d4-406d-898e-fd0c2a8ea6dd.jpg" /> is the orthogonal projection of <img src="2-5300237\b36f512e-25f8-4142-8fd4-42167d10eb0a.jpg" /> onto the spanning set of vectors <img src="2-5300237\825dc991-f5f7-4708-bb3d-ba13fc4558c1.jpg" /> then <img src="2-5300237\3c7b4451-6487-4915-b35d-4dd0db988692.jpg" /> and <img src="2-5300237\6df75a8e-be50-4ac3-a9ed-d0f4fb1fa313.jpg" /> has the usual matrix representation. Let</p><p><img src="2-5300237\d7cc00ff-cbdd-4333-a127-fef108389445.jpg" /></p><p>Then the characteristic polynomial of <img src="2-5300237\bba8bad3-4279-4c91-a687-38ab99447c4a.jpg" /> is given by a Chebyshev polynomial <img src="2-5300237\2f3b57d9-5643-4195-9d33-1148e5879295.jpg" /> of the first kind. Let <img src="2-5300237\5b4ba00e-079a-4d5f-a62e-206dee650809.jpg" /> where<img src="2-5300237\152f41f2-3a77-4977-86ac-f0059fc89c46.jpg" />. Then:</p><p><img src="2-5300237\b79e42d5-1b7a-4e60-9451-6d4448da72ab.jpg" /></p><p>(easily proven by trigonometric identities) and <img src="2-5300237\948020e4-e0a0-4960-be2f-941ecbd84fcd.jpg" /> for <img src="2-5300237\f3055566-e919-41c7-8e8f-38dff573b06f.jpg" /> is a linear combination of powers of x<sup>k</sup>. Also, det<img src="2-5300237\0975074a-8e88-46ce-a300-a01b9f78ccf6.jpg" />. If <img src="2-5300237\e6c0a386-752e-4975-9d25-14eba6051b1b.jpg" /> then the roots are given by the Chebyshev polynomial of the first kind. The roots can be found by finding the eigenvalues of matrix B. By [2, p. 179, Example 9], the eigenvalues of B are given by</p><p><img src="2-5300237\6a3513d9-0e75-48f3-888d-0ae54ffdd32a.jpg" />, for<img src="2-5300237\846a6de4-eb5d-400b-ae89-23ec9a6a6887.jpg" />.</p><p>Suppose that</p><p><img src="2-5300237\5e5cf6f7-f222-4cc6-8c63-13cf2a81f155.jpg" /></p><p>then<img src="2-5300237\0cbbcff5-3761-48f5-92d2-714e311b8ff7.jpg" />. Hence, <img src="2-5300237\146e6dc7-49a6-464b-b657-a42bfe0bd3ba.jpg" />if<img src="2-5300237\4286fd3c-85ba-4af3-97ac-293118355730.jpg" />.</p></sec><sec id="s4"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.24364-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">U. Haagerup and P. de la Harpe, “The Numerical Radius of a Nilpotent Operator on a Hilbert Space,” Proceedings of the American Mathematical Society, Vol. 115, 1999, pp. 371-379.</mixed-citation></ref><ref id="scirp.24364-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">C. A. Berger and J. G. Stampi, “Mapping Theorems for the Numerical Range,” American Journal of Mathematics, Vol. 89, 1967, pp. 1047-1055. </mixed-citation></ref><ref id="scirp.24364-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">M. T. 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