<?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">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2022.105118</article-id><article-id pub-id-type="publisher-id">JAMP-117458</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>
 
 
  On Maps Preserving the Spectrum on Positive Cones of Operator Algebras
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zhiqin</surname><given-names>Dang</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>School of Mathematical Sciences, Qufu Normal University, Qufu, China</addr-line></aff><pub-date pub-type="epub"><day>07</day><month>05</month><year>2022</year></pub-date><volume>10</volume><issue>05</issue><fpage>1702</fpage><lpage>1710</lpage><history><date date-type="received"><day>3,</day>	<month>April</month>	<year>2022</year></date><date date-type="rev-recd"><day>27,</day>	<month>May</month>	<year>2022</year>	</date><date date-type="accepted"><day>30,</day>	<month>May</month>	<year>2022</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 consider the spectrum-preserving maps on positive definite cones of 
  <em>C</em>
  <sup>*</sup>-algebras or von Neumann algebras. We first introduce some basic properties of Jordan isomorphism. Then, we study the additively spectrum preserving property and the multiplicatively spectrum-preserving property, and prove that these maps can be characterized by Jordan isomorphisms between 
  <em>C</em>
  <sup>*</sup>-algebras.
 
</p></abstract><kwd-group><kwd>Jordan &lt;sup&gt;*&lt;/sup&gt;-Isomorphsim</kwd><kwd> Preserve</kwd><kwd> Spectrum</kwd><kwd> &lt;i&gt;C&lt;/i&gt;&lt;sup&gt;*&lt;/sup&gt;-Algebra</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In the research field of operator algebra, preserving problem is one of the hot research directions. Over the years, a large number of mathematicians and researchers have devoted themselves to the study of it ( [<xref ref-type="bibr" rid="scirp.117458-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.117458-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.117458-ref3">3</xref>]). There are also many works on preserves of Kubo-Ando means by M. Ga&#225;l, G. Nagy, Lei Li, Moln&#225;r L., Semrl P. and Liguang Wang ( [<xref ref-type="bibr" rid="scirp.117458-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.117458-ref12">12</xref>]). These preserves are characterized by Jordan <sup>*</sup>-isomorphisms.</p><p>We now recall the concept and properties of Jordan * -isomorphisms that will be used in this paper. We refer to [<xref ref-type="bibr" rid="scirp.117458-ref3">3</xref>] for more properties of Jordan * -isomorphisms. Suppose that A and B are C * -algebras, a bijective linear map J : A → B is a Jordan * -isomorphism if it satisfies</p><p>J ( A B + B A ) = J ( A ) J ( B ) + J ( B ) J ( A ) ,   J ( A ) ∗ = J ( A ∗ )</p><p>for all A , B ∈ A . The Jordan * -isomorphism J preserves the Jordan triple product, i.e., for any A , B ∈ A , we have that</p><p>J ( A B A ) = J ( A ) J ( B ) J ( A ) .</p><p>For any A ∈ A , A is invertible if and only if J ( A ) is invertible and, moreover,</p><p>J ( A ) − 1 = J ( A − 1 ) .</p><p>In particular, J preserves the spectrum of the elements, i.e.,</p><p>σ ( J ( A ) ) = σ ( A )</p><p>for any A ∈ A . We also have</p><p>J ( f ( A ) ) = f ( J ( A ) )</p><p>for any A ∈ A s and continuous real function f on its spectrum. Moreover, J preserves commutativity in both directions, i.e., for any A , B ∈ A , we have</p><p>A B = B A ⇔ J ( A ) J ( B ) = J ( B ) J ( A ) .</p><p>Finally, for any A , B ∈ A s we have</p><p>A ≤ B ⇔ J ( A ) ≤ J ( B ) ,</p><p>and J is an isometry,</p><p>‖ J ( A ) ‖ = ‖ A ‖ ,     A ∈ A + − 1 .</p><p>Let A , B be C * -algebras with the set of all self-adjoint A s , B s respectively. Suppose ϕ : A s → B s be a surjective map. Moln&#225;r in [<xref ref-type="bibr" rid="scirp.117458-ref13">13</xref>] considered the map that satisfies</p><p>σ ( ϕ ( a ) + ϕ ( b ) ) = σ ( a + b ) ,     a , b ∈ A s (1.1)</p><p>and</p><p>σ ( ϕ ( a ) ϕ ( b ) ) = σ ( a b ) ,     a , b ∈ A s . (1.2)</p><p>He showed that these maps are characterized by Jordan <sup>*</sup>-isomorphism.</p><p>In this paper, we would like to consider when there are two maps in (1.1) and (1.2). The results obtained in this generalize Moln&#225;r’s works in [<xref ref-type="bibr" rid="scirp.117458-ref13">13</xref>]. Suppose ϕ : A s → B s and ψ : A s → B s be surjective maps. Now we consider the following structures</p><p>σ ( ϕ ( a ) + ψ ( b ) ) = σ ( a + b ) ,   a , b ∈ A s</p><p>and</p><p>σ ( ϕ ( a ) ψ ( b ) ) = σ ( a b ) ,     a , b ∈ A s .</p><p>In the process of proving the theorem, we describe some lemmas, and then give the results and proofs.</p></sec><sec id="s2"><title>2. Main Results</title><p>Now we first give fives lemmas that will use in the proving theorems.</p><p>Lemma 2.1. ( [<xref ref-type="bibr" rid="scirp.117458-ref14">14</xref>]) Let A , B be C * -algebras. If <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/20-1722787x48.png" xlink:type="simple"/></inline-formula> is a surjective linear isometry, then it of the form</p><p>ϕ ( a ) = u J ( a ) ,     a ∈ A ,</p><p>where u ∈ B is a unitary element and <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/20-1722787x51.png" xlink:type="simple"/></inline-formula> is a Jordan * -isomorphism.</p><p>Lemma 2.2. ( [<xref ref-type="bibr" rid="scirp.117458-ref7">7</xref>]) Let A , B be C * -algebras and let ϕ : A → B be a bijective linear map which preserves the order in both direction, i.e., satisfies</p><p>a ≤ b ⇔ ϕ ( a ) ≤ ϕ ( b ) ,     a , b ∈ A s .</p><p>Then ϕ is of the form</p><p>ϕ ( a ) = t J ( a ) t * ,     a ∈ A ,</p><p>where t ∈ B is an invertible element and J : A → B is a Jordan * -isomorphism.</p><p>Lemma 2.3. ( [<xref ref-type="bibr" rid="scirp.117458-ref13">13</xref>]) Let A be a von Neumann algebra. Assume a ∈ A is a symmetry such that for every symmetry t ∈ A , the spectrum σ ( s t ) contains only real numbers. Then s is a central symmetry in A .</p><p>Lemma 2.4. ( [<xref ref-type="bibr" rid="scirp.117458-ref13">13</xref>]) Let A be a von Neumann algebra. Pick a , b ∈ A s . If σ ( a t ) = σ ( b t ) holds for all t ∈ A + − 1 , then we have a = b .</p><p>Lemma 2.5. ( [<xref ref-type="bibr" rid="scirp.117458-ref9">9</xref>]) Let A be a C * -algebra and pick ∀ a , b ∈ A + − 1 , then</p><p>a ≤ b ⇔ ‖ x a x ‖ ≤ ‖ x b x ‖ ,     x ∈ A + − 1 .</p><p>The following are the main results obtained in this paper.</p><p>Theorem 2.1. Suppose A and B are C * -algebras and ϕ , ψ : A s → B s are surjective maps. Then</p><p>σ ( ϕ ( a ) + ψ ( b ) ) = σ ( a + b ) ,     a , b ∈ A s ,</p><p>and</p><p>ϕ ( 0 ) = ψ ( 0 )</p><p>if and only if there is a Jordan isomorphism J : A → B such that ϕ = φ = ϕ | A s .</p><p>Proof. ( ⇒ ) Assume that</p><p>σ ( ϕ ( a ) + ψ ( b ) ) = σ ( a + b ) ,     a , b ∈ A s .</p><p>Then we have</p><p>σ ( ϕ ( a ) + ψ ( − a ) ) = σ ( a − a ) = σ ( 0 ) = { 0 } ,     a ∈ A s .</p><p>i.e., ϕ ( a ) + ψ ( − a ) = 0 and ϕ ( 0 ) = ψ ( 0 ) = 0 . Hence ψ ( − a ) = − ϕ ( a ) . For any a , b ∈ A s , we have</p><p>σ ( ϕ ( a ) − ϕ ( b ) ) = σ ( ϕ ( a ) + ψ ( − b ) ) = σ ( a − b ) ,     a , b ∈ A s .</p><p>Thus ‖ ϕ ( a ) − ϕ ( b ) ‖ = ‖ a − b ‖ for all a , b ∈ A s and ϕ : A s → B s is a surjective isometry. It follows from Mazur-Ulam theorem ( [<xref ref-type="bibr" rid="scirp.117458-ref15">15</xref>]) that ϕ is a linear surjective isometry. Then by Lemma 2.1 there exist a Jordan isomorphism J : A → B and a center symmetry s ∈ B such that</p><p>ϕ ( a ) = s J ( a ) ,     a ∈ A s .</p><p>By the spectrum-preserving property of ϕ , put a = 1 , b = 0 , we infer</p><p>σ ( ϕ ( 1 ) + ψ ( 0 ) ) = σ ( 1 ) = σ ( ϕ ( 1 ) )</p><p>and therefore ϕ ( 1 ) = 1 . Since J ( 1 ) = 1 , we have s = 1 . Hence</p><p>ϕ ( a ) = J ( a ) ,     a ∈ A s .</p><p>Since</p><p>ψ ( a ) = − ϕ ( − a ) = − J ( − a ) = J ( a ) ,     a ∈ A s .</p><p>we have ψ ( a ) = J ( a ) = ϕ ( a ) for a ∈ A s .</p><p>( ⇐ ) If a , b ∈ A s , then we have</p><p>σ ( ϕ ( a ) + ψ ( b ) ) = σ ( J ( a ) + J ( b ) ) = σ ( a + b ) .</p><p>This completes the proof. □</p><p>In the proof of next theorem we also need the concept of the Thompson metric (see [<xref ref-type="bibr" rid="scirp.117458-ref16">16</xref>]) which we denote by d T . Define</p><p>d T ( a , b ) = log max { M ( a / b ) , M ( b / a ) } ,     a , b ∈ A + − 1 ,</p><p>where M ( x / y ) = inf { λ &gt; 0 : x ≤ λ y } for a , y ∈ A + − 1 . It also holds:</p><p>d T ( a , b ) = ‖ log ( a − 1 2 b a − 1 2 ) ‖ ,     a , b ∈ A + − 1 .</p><p>By Theorem 9 in [<xref ref-type="bibr" rid="scirp.117458-ref16">16</xref>], for every such isometry ϕ : A + − 1 → B + − 1 , there is a Jordan * -isomorphism J : A → B , a center projection p ∈ B and a positive invertible element c ∈ B such that</p><p>ϕ ( a ) = c ( p J ( a ) + ( 1 − p ) J ( a − 1 ) ) c ,     a ∈ A + − 1 .</p><p>Theorem 2.2. Let A and B be von Neumann algebras. Suppose ϕ , ψ : A s → B s be surjective maps. Then</p><p>σ ( ϕ ( a ) ψ ( b ) ) = σ ( a b ) ,     a , b ∈ A s</p><p>and</p><p>ϕ ( 1 ) = ψ ( 1 )</p><p>if and only if there exists a Jordan isomorphism J : A → B such that</p><p>ϕ ( a ) = ψ ( a ) = J ( a ) ,     a ∈ A S .</p><p>Proof. ( ⇒ ) Suppose ϕ and ψ satisfy σ ( ϕ ( a ) ψ ( b ) ) = σ ( a b ) and ϕ ( 1 ) = ψ ( 1 ) . Let a = b = 1 and we have</p><p>σ ( ϕ ( 1 ) ψ ( 1 ) ) = σ ( ϕ ( 1 ) 2 ) = σ ( 1 2 ) = { 1 } .</p><p>This implies that ϕ ( 1 ) = ψ ( 1 ) = 1 . By Lemma 2.3, ϕ ( 1 ) is a central symmetry. Then it follows that ϕ and ψ preserve the spectrum. In particular, we obtain that ϕ and ψ maps A + − 1 onto B + − 1 . For any a ∈ A + − 1 , we have</p><p>{ 1 } = σ ( 1 ) = σ ( a a − 1 ) = σ ( ϕ ( a ) ψ ( − a ) ) = σ ( ϕ ( a ) 1 2 ψ ( a − 1 ) ϕ ( a ) 1 2 )</p><p>and this implies that ϕ ( a ) 1 2 ψ ( a − 1 ) ϕ ( a ) 1 2 = 1 , i.e., ψ ( a − 1 ) = ϕ ( a ) . If a , b ∈ A + − 1 , we get</p><p>σ ( ϕ ( a ) − 1 2 ϕ ( b ) ϕ ( a ) − 1 2 ) = σ ( ϕ ( b ) ϕ ( a ) − 1 ) = σ ( ϕ ( b ) ψ ( a − 1 ) ) = σ ( b a − 1 ) = σ ( a − 1 2 b a − 1 2 ) .</p><p>By the definition of Thompson metric, this implies that ϕ is a surjective Thompson isometry from A + − 1 onto B + − 1 .</p><p>Since for all a , b ∈ A + − 1 and all real numbers λ , we have</p><p>σ ( ( λ ϕ ( a ) ) ψ ( b ) ) = λ σ ( ϕ ( a ) ψ ( b ) ) = λ σ ( a b ) = σ ( ( λ a ) b ) = σ ( ϕ ( λ a ) ψ ( b ) ) .</p><p>It follows from Lemma 2.4 that ϕ is also homogeneous. Hence ϕ is a Thompson isometry. By Theorem 9 in [<xref ref-type="bibr" rid="scirp.117458-ref16">16</xref>] that there exist a Jordan isomorphism J : A → B such that ϕ ( a ) = J ( a ) holds for all a ∈ A + − 1 . We need to show that ϕ ( a ) = J ( a ) for all a ∈ A s .</p><p>If b ∈ A + − 1 , then we have</p><p>ψ ( b ) = ϕ ( b − 1 ) − 1 = J ( b − 1 ) − 1 = J ( b ) .</p><p>For any a ∈ A s and arbitrary b ∈ A + − 1 , we have</p><p>σ ( J − 1 ( ϕ ( a ) ) b ) = σ ( J − 1 ( ϕ ( a ) ) J − 1 ψ ( b ) ) = σ ( a b ) ,</p><p>and then Lemma 2.4 implies that J − 1 ( ϕ ( a ) ) = a , i.e., ϕ ( a ) = J ( a ) , a ∈ A s . For any b ∈ A + − 1 and a ∈ A s , we have</p><p>σ ( J − 1 ( ψ ( a ) ) b ) = σ ( J − 1 ( ψ ( a ) ) J − 1 ( ϕ ( b ) ) ) = σ ( ψ ( a ) ϕ ( b ) ) = σ ( ϕ ( b ) ψ ( a ) ) = σ ( b a ) = σ ( a b ) .</p><p>Hence J − 1 ∘ ψ ( a ) = a and ψ ( a ) = J ( a ) for all a ∈ A s .</p><p>( ⇐ ) For a , b ∈ A s , we have</p><p>σ ( ϕ ( a ) ψ ( b ) ) = σ ( J ( a ) J ( b ) ) = σ ( a b ) .</p><p>This completes the proof. □</p><p>Let A be a standard C * -algebra acting on a Hilbert space H . Suppose a , b ∈ A s , such that σ ( a t ) = σ ( b t ) holds for all t ∈ A + − 1 . Pick p ∈ A and ( λ n ) → 0 , we have σ ( a ( λ n ⋅ 1 + p ) ) = σ ( b ( λ n ⋅ 1 + p ) ) . By the Corollary 3.4.5 in [<xref ref-type="bibr" rid="scirp.117458-ref17">17</xref>], σ ( a p ) = σ ( b p ) holds for every rank-one projective p . Then for every unit vector ξ in H , we have 〈 a ξ , ξ 〉 = 〈 b ξ , ξ 〉 and therefore a = b . Now we can prove the following result.</p><p>Theorem 2.3. Let A , B be standard C ∗ -algebras. Suppose A is acting on the Hilbert space H and B is acting on the Hilbert space K . Let ϕ , ψ : A s → B s be surjective maps. Then</p><p>σ ( ϕ ( a ) ψ ( b ) ) = σ ( a b ) ,     a , b ∈ A s</p><p>and</p><p>ϕ ( 1 ) = ψ ( 1 )</p><p>if and only if there exist a constant λ ∈ { − 1,1 } and either a unitary or an antiunitary operator u : H → K such that</p><p>ϕ ( a ) = ψ ( a ) = λ u a u ∗ ,     a ∈ A s .</p><p>Proof. ( ⇒ ) Suppose that ϕ , ψ : A s → B s are surjective maps with</p><p>σ ( ϕ ( a ) ψ ( b ) ) = σ ( a b ) ,     a , b ∈ A s .</p><p>For vectors ξ , η in H , we denote the rank one operator ξ ⊗ η defined by ( ξ ⊗ η ) ( v ) = 〈 v , η 〉 ξ , v ∈ H . We show that ϕ is injective. If a , b ∈ A s , such that ϕ ( a ) = ϕ ( b ) . Then for every c ∈ A s that</p><p>σ ( a c ) = σ ( ϕ ( a ) ψ ( c ) ) = σ ( ϕ ( b ) ϕ ( c ) ) = σ ( b c ) .</p><p>For ∀ c ∈ ξ ⊗ ξ , where ξ ∈ H is an arbitrary vector and ‖ ξ ‖ = 1 , then we have</p><p>σ ( a ( ξ ⊗ ξ ) ) = σ ( b ( ξ ⊗ ξ ) ) .</p><p>Thus 〈 a ξ , ξ 〉 = 〈 b ξ , ξ 〉 and therefore a = b . For the self-adjoint element ϕ ( 1 ) , we have</p><p>σ ( ϕ ( 1 ) 2 ) = σ ( 1 ) = { 1 } ,</p><p>thus ϕ ( 1 ) 2 = 1 and s = ϕ ( 1 ) is a symmetry.</p><p>Now we show that s = &#177; 1 . Since</p><p>σ ( s ψ ( b ) ) = σ ( ϕ ( 1 ) ψ ( b ) ) = σ ( b ) ,     b ∈ A s ,</p><p>so σ ( s t ) is real for every t ∈ B s . Suppose s ≠ &#177; 1 . Then there is a basis { ξ α , η β } in the Hilbert space H such that</p><p>s = ∑ α     ξ α ⊗ ξ α − ∑ β     η β ⊗ η β ,</p><p>where neither of these sums is zero. Pick ξ ∈ { ξ α } and η ∈ { η β } . Define</p><p>t = i ( ξ ⊗ η − η ⊗ ξ ) .</p><p>Then t ∈ B s and σ ( s t ) = { − i , i } , that’s a contradiction. It follows that ϕ ( 1 ) = &#177; 1 . If ϕ ( 1 ) = 1 , we have σ ( ϕ ( a ) ) = σ ( ϕ ( a ) ϕ ( 1 ) ) = σ ( a ) for every a ∈ A s , and ϕ maps A + − 1 onto B + − 1 . Thus ϕ is a surjective Thompson isomorphism from A + − 1 onto B + − 1 . It follows that there is a Jordan * -isomorphism J : A → B such that</p><p>ϕ ( a ) = J ( a ) ,     a ∈ A s .</p><p>By the result of Herstein [<xref ref-type="bibr" rid="scirp.117458-ref10">10</xref>], J is either a * -isomorphism or a * -antiisomorphism. And from [<xref ref-type="bibr" rid="scirp.117458-ref3">3</xref>], we have either a unitary operator u : K → H such that</p><p>J ( a ) = u a u * ,     a ∈ A ,</p><p>or an antiunitary operator u : K → H such that</p><p>J ( a ) = u a * u * ,     a ∈ A .</p><p>The map J − 1 ∘ ϕ : A → A satisfies</p><p>σ ( ϕ ( a ) ψ ( b ) ) = σ ( a b ) ,     a , b ∈ A s ,</p><p>and it equals the identity on A + − 1 . If a ∈ A s , b ∈ A s − 1 , we have</p><p>σ ( J − 1 ( ϕ ( a ) ) b ) = σ ( J − 1 ( ϕ ( a ) ) J − 1 ( ψ ( b ) ) ) = σ ( ϕ ( a ) ψ ( b ) ) = σ ( a b ) .</p><p>So J − 1 ( ϕ ( a ) ) = a , i.e., J ( a ) = ϕ ( a ) . For any a ∈ A s , we get</p><p>σ ( ψ ( b ) ϕ ( a ) ) = σ ( a b ) ,     a , b ∈ A s .</p><p>Therefore, ψ ( a ) = J ( a ) .</p><p>( ⇐ ) For a , b ∈ A s , we have</p><p>σ ( ϕ ( a ) ψ ( b ) ) = σ ( λ u a u ∗ λ u b u ∗ ) = σ ( λ 2 u a b u ∗ ) = σ ( u a b u ∗ ) = σ ( a b ) .</p><p>This completes the proof. □</p><p>The following characterization of the order of operators is needed in the proof of Theorem 2.4.</p><p>Theorem 2.4. Let A and B be two C * -algebras and ϕ : A + − 1 → A + − 1 be a surjective map. Then</p><p>σ ( ϕ ( a ) ϕ ( b ) ϕ ( a ) ) = σ ( a b a ) ,     a , b ∈ A + − 1 ,</p><p>if and only if there is a Jordan * -isomorphism J : A → B such that ϕ ( a ) = J ( a ) for every a ∈ A + − 1 .</p><p>Proof. ( ⇒ ) Suppose ϕ : A + − 1 → A + − 1 is a surjective map satisfies</p><p>σ ( ϕ ( a ) ϕ ( b ) ϕ ( a ) ) = σ ( a b a ) ,     a , b ∈ A + − 1 .</p><p>First we prove that ϕ preserves the order in both directions. From the Lemma 2.5, for ∀ a , b ∈ A + − 1 , we have</p><p>a ≤ b ⇔ ‖ x a x ‖ ≤ ‖ x b x ‖ ,     ∀ x ∈ A + − 1                 ⇔ sup λ ∈ σ ( x a x ) | λ | ≤ sup μ ∈ σ ( x b x ) | μ |                 ⇔ sup λ ∈ σ ( ϕ ( x ) ϕ ( a ) ϕ ( x ) ) | λ | ≤ sup μ ∈ σ ( ϕ ( x ) ϕ ( b ) ϕ ( x ) ) | μ |                 ⇔ ‖ ϕ ( x ) ϕ ( a ) ϕ ( x ) ‖ ≤ ‖ ϕ ( x ) ϕ ( b ) ϕ ( x ) ‖                 ⇔ ϕ ( a ) ≤ ϕ ( b ) .</p><p>Thus ϕ is an order isomorphism.</p><p>Next to prove that ϕ is positive homogeneous. If t &gt; 0 , a ∈ A + − 1 , then for every x ∈ A + − 1 , we have</p><p>‖ ϕ ( x ) ϕ ( t a ) ϕ ( x ) ‖ = sup { | λ | : λ ∈ σ ( ϕ ( x ) ϕ ( t a ) ϕ ( x ) ) } = sup { | λ | : λ ∈ σ ( x t a x ) } = t sup { | μ | : μ ∈ σ ( x a x ) } = t ‖ x a x ‖ = t ‖ ϕ ( x ) ϕ ( a ) ϕ ( x ) ‖ = ‖ ϕ ( x ) ( t ϕ ( a ) ) ϕ ( x ) ‖ .</p><p>i.e., ϕ ( t a ) = t ϕ ( a ) . Since σ ( ϕ ( 1 ) 3 ) = σ ( 1 ) = { 1 } , we have ϕ ( 1 ) = 1 . Therefore by Lemma 2.2, there is a Jordan * -isomorphism J : A → B such that</p><p>ϕ ( a ) = J ( a ) ,     a ∈ A + − 1 .</p><p>( ⇐ ) For a , b ∈ A + − 1 , we have</p><p>σ ( ϕ ( a ) ϕ ( b ) ϕ ( a ) ) = σ ( J ( a ) J ( b ) J ( a ) ) = σ ( J ( a b a ) ) = σ ( a b a ) .</p><p>This completes the proof. □</p></sec><sec id="s3"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s4"><title>Cite this paper</title><p>Dang, Z.Q. (2022) On Maps Preserving the Spectrum on Positive Cones of Operator Algebras. Journal of Applied Mathematics and Physics, 10, 1702-1710. https://doi.org/10.4236/jamp.2022.105118</p></sec></body><back><ref-list><title>References</title><ref id="scirp.117458-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Kubo, F. and Ando, T. (1980) Means of Positive Linear Operators. Mathematische Annalen, 246, 205-224. https://doi.org/10.1007/BF01371042</mixed-citation></ref><ref id="scirp.117458-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Li, C.K. and Tsing, N.K. (1992) Linear Preserver Problems: A Brief Introduction and Some Special Techniques. Linear Algebra and Its Applications, 162-164, 217-235. https://doi.org/10.1016/0024-3795(92)90377-M</mixed-citation></ref><ref id="scirp.117458-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Molnár, L. 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