<?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">ALAMT</journal-id><journal-title-group><journal-title>Advances in Linear Algebra &amp; Matrix Theory</journal-title></journal-title-group><issn pub-type="epub">2165-333X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/alamt.2017.71001</article-id><article-id pub-id-type="publisher-id">ALAMT-74143</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>
 
 
  Two Nonzero Component Lemma and Matrix Trigonometry
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Morteza</surname><given-names>Seddighin</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>Indiana University East, Richmond, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>mseddigh@iue.edu</email></corresp></author-notes><pub-date pub-type="epub"><day>15</day><month>02</month><year>2017</year></pub-date><volume>07</volume><issue>01</issue><fpage>1</fpage><lpage>6</lpage><history><date date-type="received"><day>December</day>	<month>20,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>February</month>	<year>12,</year>	</date><date date-type="accepted"><day>February</day>	<month>15,</month>	<year>2017</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>
 
 
  In this paper we show that the author’s Two Nonzero Lemma (TNCL) can be applied to present a simple proof for a very useful equality which was first proved by Karl Gustafson in 1968. Gustafson used Hilbert space methods, including convexity of the Hilbert space norm, to prove this identity which was the basis of his matrix trigonometry. By applying TNCL, we will reduce the problem to a simple problem of ordinary calculus.
 
</p></abstract><kwd-group><kwd>Matrix Trigonometry</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Given a positive matrix<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x2.png" xlink:type="simple"/></inline-formula>, in 1968 Gustafson proved</p><disp-formula id="scirp.74143-formula30"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x3.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.74143-formula31"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x4.png"  xlink:type="simple"/></disp-formula><p>are eigenvalues of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x5.png" xlink:type="simple"/></inline-formula> such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x6.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x7.png" xlink:type="simple"/></inline-formula> are the largest and the smallest eigenvalues of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x8.png" xlink:type="simple"/></inline-formula> respectively. Please see [<xref ref-type="bibr" rid="scirp.74143-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.74143-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.74143-ref3">3</xref>] .</p><p>The equality (1) played an important role in establishing what Gustafson calls “operator trigonometry”. In fact, for a positive matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x9.png" xlink:type="simple"/></inline-formula> he defined <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x10.png" xlink:type="simple"/></inline-formula> to be</p><disp-formula id="scirp.74143-formula32"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x11.png"  xlink:type="simple"/></disp-formula><p>He proved (1) by using the convexity of the Hilbert space norm and other Hilbert space properties.</p><p>Later, in his investigation on problems of antieigenvalue theory, this author discovered a useful lemma which he calls the Two Nonzero Component Lemma or TNCL, for short (see [<xref ref-type="bibr" rid="scirp.74143-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.74143-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.74143-ref6">6</xref>] ). The antieigenvalue of an accretive operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x12.png" xlink:type="simple"/></inline-formula> acting on a complex Hilbert space is defined to be</p><disp-formula id="scirp.74143-formula33"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x13.png"  xlink:type="simple"/></disp-formula><p>For positive matrices, there is a relationship between the antieigenvalue of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x14.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x15.png" xlink:type="simple"/></inline-formula>. In a series of papers this author applied his TNCL to compute antieigenvalues of different types of operators, including normal operators. He also applied TNCL to compute other types of antieigenvalue quantities such as total antieigenvalues, higher order antieigenvalues,and joint antieigenvalues. Furthermore, he applied TNCL to solve some optimization problems in statistics, econometrics, and resource allocations. Please see [<xref ref-type="bibr" rid="scirp.74143-ref5">5</xref>] - [<xref ref-type="bibr" rid="scirp.74143-ref11">11</xref>] . Although this Lemma is implicitly used in all of the author's earlier papers up to 2008, it was not until 2008 that he stated a formal description of the Lemma in his paper titled, “Antieigenvalue Techniques in Statistics.” Below is the statement of the lemma. For an early proof of the lemma please see the author’s work in [<xref ref-type="bibr" rid="scirp.74143-ref5">5</xref>] .</p><p>Lemma 1 (The Two Nonzero Component Lemma) Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x16.png" xlink:type="simple"/></inline-formula> be the set of all sequences with nonnegative terms in the Banach Space<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x17.png" xlink:type="simple"/></inline-formula>. That is, let</p><disp-formula id="scirp.74143-formula34"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x18.png"  xlink:type="simple"/></disp-formula><p>Let</p><disp-formula id="scirp.74143-formula35"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x19.png"  xlink:type="simple"/></disp-formula><p>be a function from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x20.png" xlink:type="simple"/></inline-formula> to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x21.png" xlink:type="simple"/></inline-formula>. Assume <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x22.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x23.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x24.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x25.png" xlink:type="simple"/></inline-formula>. Then the minimizing vectors for the function</p><disp-formula id="scirp.74143-formula36"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x26.png"  xlink:type="simple"/></disp-formula><p>on the convex set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x27.png" xlink:type="simple"/></inline-formula> have at most two nonzero components.</p><p>What make the proof of the Lemma possible are the following two facts: First, the convexity of the set</p><disp-formula id="scirp.74143-formula37"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x28.png"  xlink:type="simple"/></disp-formula><p>Second, a special property that the functions</p><disp-formula id="scirp.74143-formula38"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x29.png"  xlink:type="simple"/></disp-formula><p>involved possess. If we set</p><disp-formula id="scirp.74143-formula39"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x30.png"  xlink:type="simple"/></disp-formula><p>then all restrictions of the form</p><disp-formula id="scirp.74143-formula40"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x31.png"  xlink:type="simple"/></disp-formula><p>of</p><disp-formula id="scirp.74143-formula41"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x32.png"  xlink:type="simple"/></disp-formula><p>have the same algebraic form as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x33.png" xlink:type="simple"/></inline-formula> itself. For example if</p><disp-formula id="scirp.74143-formula42"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x34.png"  xlink:type="simple"/></disp-formula><p>then we have</p><disp-formula id="scirp.74143-formula43"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x35.png"  xlink:type="simple"/></disp-formula><p>which has the same algebraic form as</p><disp-formula id="scirp.74143-formula44"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x36.png"  xlink:type="simple"/></disp-formula><p>Indeed, for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x37.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x38.png" xlink:type="simple"/></inline-formula>; all restrictions of the function</p><disp-formula id="scirp.74143-formula45"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x39.png"  xlink:type="simple"/></disp-formula><p>obtained by setting an arbitrary set of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x40.png" xlink:type="simple"/></inline-formula> components of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x41.png" xlink:type="simple"/></inline-formula> equal to zeros have the same algebraic form as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x42.png" xlink:type="simple"/></inline-formula>. Obviously, not all functions have this property. For instance, for the function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x43.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x44.png" xlink:type="simple"/></inline-formula>, which does not have the same algebraic form as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x45.png" xlink:type="simple"/></inline-formula>.</p><p>In the next section we prove that Gustafson’s identity (1) can be obtained using this author’s the Two Nonzero Component Lemma or TNCL. Our proof is elementary (comparing to Gustafson’s proof) in the sense that we use only TNCL and techniques of calculus.</p></sec><sec id="s2"><title>2. A Proof of (1) Based on TNCL</title><p>Theorem 2 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x46.png" xlink:type="simple"/></inline-formula> be a positive matrix where</p><disp-formula id="scirp.74143-formula46"><graphic  xlink:href="http://html.scirp.org/file/1-2230123x47.png"  xlink:type="simple"/></disp-formula><p>are eigenvalues of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x48.png" xlink:type="simple"/></inline-formula> such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x49.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x50.png" xlink:type="simple"/></inline-formula> are the largest and the smallest eigenvalues of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x51.png" xlink:type="simple"/></inline-formula>, then</p><disp-formula id="scirp.74143-formula47"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x52.png"  xlink:type="simple"/></disp-formula><p>Proof. Note that if we square the left hand side of (17) we get</p><disp-formula id="scirp.74143-formula48"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x53.png"  xlink:type="simple"/></disp-formula><p>Thus, we need to show</p><disp-formula id="scirp.74143-formula49"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x54.png"  xlink:type="simple"/></disp-formula><p>Now to follow notations usually used in differential calculus, let’s substitute <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x55.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x56.png" xlink:type="simple"/></inline-formula> and consider</p><disp-formula id="scirp.74143-formula50"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x57.png"  xlink:type="simple"/></disp-formula><p>instead. With this change of notation. now we apply spectral theorem to the positive matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x58.png" xlink:type="simple"/></inline-formula> and assume</p><disp-formula id="scirp.74143-formula51"><graphic  xlink:href="http://html.scirp.org/file/1-2230123x59.png"  xlink:type="simple"/></disp-formula><p>are components of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x60.png" xlink:type="simple"/></inline-formula> with respect to an orthogonal basis corresponding to</p><disp-formula id="scirp.74143-formula52"><graphic  xlink:href="http://html.scirp.org/file/1-2230123x61.png"  xlink:type="simple"/></disp-formula><p>Therefore, we can rewrite (20) as</p><disp-formula id="scirp.74143-formula53"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x62.png"  xlink:type="simple"/></disp-formula><p>Applying TNCL we can assume any optimizing vector</p><disp-formula id="scirp.74143-formula54"><graphic  xlink:href="http://html.scirp.org/file/1-2230123x63.png"  xlink:type="simple"/></disp-formula><p>is so that only two of its components, say <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x64.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x65.png" xlink:type="simple"/></inline-formula> are nonzero and the rest of them are zero. Keeping that in mind, for such optimizing vectors <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x66.png" xlink:type="simple"/></inline-formula> (21) will be reduced to</p><disp-formula id="scirp.74143-formula55"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x67.png"  xlink:type="simple"/></disp-formula><p>To compute (22), let’s do some change of variables first. Substitute <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x68.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x69.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x70.png" xlink:type="simple"/></inline-formula>for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x71.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x72.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x73.png" xlink:type="simple"/></inline-formula>. (22) then becomes</p><disp-formula id="scirp.74143-formula56"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x74.png"  xlink:type="simple"/></disp-formula><p>For a fixed <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x75.png" xlink:type="simple"/></inline-formula> we compute the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x76.png" xlink:type="simple"/></inline-formula> in (23) with respect to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x77.png" xlink:type="simple"/></inline-formula> first. Consider the expression</p><disp-formula id="scirp.74143-formula57"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x78.png"  xlink:type="simple"/></disp-formula><p>We next find the derivative of (24) with respect to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x79.png" xlink:type="simple"/></inline-formula> and set it equal to zero</p><disp-formula id="scirp.74143-formula58"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x80.png"  xlink:type="simple"/></disp-formula><p>and then solve it for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x81.png" xlink:type="simple"/></inline-formula>. The solution is</p><disp-formula id="scirp.74143-formula59"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x82.png"  xlink:type="simple"/></disp-formula><p>Assume <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x83.png" xlink:type="simple"/></inline-formula> and note that the second derivative of (24) is</p><disp-formula id="scirp.74143-formula60"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x84.png"  xlink:type="simple"/></disp-formula><p>which is positive. This shows</p><disp-formula id="scirp.74143-formula61"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x85.png"  xlink:type="simple"/></disp-formula><p>is indeed a minimizing value. If we substitute <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x86.png" xlink:type="simple"/></inline-formula> from (26) in 24) and simplify we get</p><disp-formula id="scirp.74143-formula62"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x87.png"  xlink:type="simple"/></disp-formula><p>The derivative of (29) with respect to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x88.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.74143-formula63"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x89.png"  xlink:type="simple"/></disp-formula><p>To find the optimizing value<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x90.png" xlink:type="simple"/></inline-formula>, we solve the following equation with respect to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x91.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.74143-formula64"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x92.png"  xlink:type="simple"/></disp-formula><p>The solution of (31) is</p><disp-formula id="scirp.74143-formula65"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x93.png"  xlink:type="simple"/></disp-formula><p>If we substitute the value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x94.png" xlink:type="simple"/></inline-formula> from (32) in (29) and simplify we get</p><disp-formula id="scirp.74143-formula66"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x95.png"  xlink:type="simple"/></disp-formula><p>The second derivative of (29) is</p><disp-formula id="scirp.74143-formula67"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x96.png"  xlink:type="simple"/></disp-formula><p>which is negative, under our assumption that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x97.png" xlink:type="simple"/></inline-formula>. This indicates that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x98.png" xlink:type="simple"/></inline-formula> given by (32) is indeed a maximizing vector. Thus we have proved</p><disp-formula id="scirp.74143-formula68"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x99.png"  xlink:type="simple"/></disp-formula><p>Finally, we show that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x100.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x101.png" xlink:type="simple"/></inline-formula>. To show this note that</p><disp-formula id="scirp.74143-formula69"><label>(36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x102.png"  xlink:type="simple"/></disp-formula><p>Now define</p><disp-formula id="scirp.74143-formula70"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x103.png"  xlink:type="simple"/></disp-formula><p>and notice that</p><disp-formula id="scirp.74143-formula71"><label>(38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2230123x104.png"  xlink:type="simple"/></disp-formula><p>Hence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x105.png" xlink:type="simple"/></inline-formula> is decreasing and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x106.png" xlink:type="simple"/></inline-formula> has the largest value when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x107.png" xlink:type="simple"/></inline-formula> takes the smallest value. That is when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x108.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x109.png" xlink:type="simple"/></inline-formula>.</p><p>Remark 3 The equality (35) is valid even if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x110.png" xlink:type="simple"/></inline-formula> is an infinite dimensional positive operator acting on a separable Hilbert space. The reason is that TNCL is valid both when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x111.png" xlink:type="simple"/></inline-formula> has a finite or infinite number of components. However, in the case of an infinite dimensional positive operator, we do not know for what pair of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x112.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2230123x113.png" xlink:type="simple"/></inline-formula> (35) holds.</p></sec><sec id="s3"><title>3. Conclusion</title><p>We showed that TNCL can be used to prove an identity which was proved by Karl Gustafson in 1968. This identity was part of his min-max theorem. The identity was the basis of operator trigonometry. The original proof was based on Hilbert space techniques and convexity of operator norm. Using TNCM we reduced the problem to a very simple problem in elementary calculus. This indeed shows the power of this dimension reducing optimization lemma which is used by this author in many of his previous work. The lemma not only proved equality (1) but, as we noted in the remark above, it extended it to the case of positive operators on an infinite dimensional Hilbert space.</p></sec><sec id="s4"><title>Acknowledgement</title><p>The author wishes to thank the referee of this paper for his helpful suggestions.</p></sec><sec id="s5"><title>Cite this paper</title><p>Seddighin, M. (2017) Two Nonzero Component Lemma and Matrix Trigonometry. 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