<?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.2017.54068</article-id><article-id pub-id-type="publisher-id">JAMP-75355</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>
 
 
  Nonlinear Super Integrable Couplings of Super Yang Hierarchy and Its Super Hamiltonian Structures
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Sixing</surname><given-names>Tao</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yunling</surname><given-names>Ma</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Mathematics and Statics, Shangqiu Normal University, Shangqiu, China</addr-line></aff><pub-date pub-type="epub"><day>12</day><month>04</month><year>2017</year></pub-date><volume>05</volume><issue>04</issue><fpage>792</fpage><lpage>800</lpage><history><date date-type="received"><day>March</day>	<month>5,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>April</month>	<year>9,</year>	</date><date date-type="accepted"><day>April</day>	<month>12,</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>
 
 
   
   Nonlinear super integrable couplings of the super Yang hierarchy based upon an enlarged matrix Lie super algebra were constructed. Then its super Hamiltonian structures were established by using super trace identity. As its reduction, nonlinear integrable couplings of Yang hierarchy were obtained. 
  
 
</p></abstract><kwd-group><kwd>Lie Super Algebra</kwd><kwd> Nonlinear Super Integrable Couplings</kwd><kwd> Super Yang Hierarchy</kwd><kwd> Super Hamiltonian Structures</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>With the development of soliton theory, super integrable systems associated with Lie superalgebra have aroused growing attentions by many mathematicians and physicists. It was known that super integrable systems contained the odd variables, which would provide more prolific fields for mathematical researchers and physical ones. Several super integrable systems including super AKNS hierarchy, super KdV hierarchy, super KP hierarchy etc., have been studied in [<xref ref-type="bibr" rid="scirp.75355-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.75355-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.75355-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.75355-ref4">4</xref>]. There are some interesting results on the super integrable systems, such as Darboux transformation [<xref ref-type="bibr" rid="scirp.75355-ref5">5</xref>], super Hamiltonian structures in [<xref ref-type="bibr" rid="scirp.75355-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.75355-ref7">7</xref>], binary nonlinearization [<xref ref-type="bibr" rid="scirp.75355-ref8">8</xref>] and reciprocal transformation [<xref ref-type="bibr" rid="scirp.75355-ref9">9</xref>] and so on.</p><p>There search of integrable couplings of the well known integrable hierarchy has received considerable attention [<xref ref-type="bibr" rid="scirp.75355-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.75355-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.75355-ref12">12</xref>]. A few approaches to construct linear integrable couplings of the classical soliton equation are presented by permutation, enlarging spectral problem, using matrix Lie algebra [<xref ref-type="bibr" rid="scirp.75355-ref12">12</xref>] constructing new loop Lie algebra and creating semi-direct sums of Lie algebra. Zhang [<xref ref-type="bibr" rid="scirp.75355-ref13">13</xref>] once employed two kinds of explicit Lie algebra F and G to obtain the nonlinear integrable couplings of the GJ hierarchy and Yang hierarchy, respectively. Recently, You [<xref ref-type="bibr" rid="scirp.75355-ref14">14</xref>] presented a scheme for constructing nonlinear super integrable couplings for the super integrable hierarchy.</p><p>Inspired by Zhang [<xref ref-type="bibr" rid="scirp.75355-ref13">13</xref>] and You [<xref ref-type="bibr" rid="scirp.75355-ref14">14</xref>], we hope to construct nonlinear super integrable couplings of the super Yang hierarchy through enlarging matrix Lie super algebra. We take the Lie algebra <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x2.png" xlink:type="simple"/></inline-formula> as an example to illustrate the approach for extending Lie super algebras. Based on the enlarged Lie super algebra<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x3.png" xlink:type="simple"/></inline-formula>, we work out nonlinear super integrable Hamiltonian couplings of the super Yang hierarchy. Finally, we will reduce the nonlinear super Yang integrable Hamiltonian couplings to some special cases.</p></sec><sec id="s2"><title>2. Enlargement of Lie Super Algebra</title><p>Consider the Lie super algebra<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x4.png" xlink:type="simple"/></inline-formula>. Its basis is</p><disp-formula id="scirp.75355-formula644"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x5.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x6.png" xlink:type="simple"/></inline-formula> are even element and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x7.png" xlink:type="simple"/></inline-formula> are odd elements. Their non- zero (anti) commutation relations are</p><disp-formula id="scirp.75355-formula645"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x8.png"  xlink:type="simple"/></disp-formula><p>Let us enlarge the Lie super algebra <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x9.png" xlink:type="simple"/></inline-formula> to the Lie super algebra <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x10.png" xlink:type="simple"/></inline-formula> with a basis</p><disp-formula id="scirp.75355-formula646"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x11.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x12.png" xlink:type="simple"/></inline-formula> are even, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x13.png" xlink:type="simple"/></inline-formula> are odd.</p><p>The generator of Lie super algebra<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x14.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x15.png" xlink:type="simple"/></inline-formula>satisfy the following (anti) commutation relations:</p><disp-formula id="scirp.75355-formula647"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x16.png"  xlink:type="simple"/></disp-formula><p>Define a loop super algebra corresponding to the Lie super algebra gl(6, 2), denote by</p><disp-formula id="scirp.75355-formula648"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x17.png"  xlink:type="simple"/></disp-formula><p>The corresponding (anti) commutative relations are given as</p><disp-formula id="scirp.75355-formula649"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x18.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. Nonlinear Super Integrable Couplings of Super Yang Hierarchy</title><p>If Let us start from an enlarged spectral problem associated with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x19.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.75355-formula650"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x20.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x21.png" xlink:type="simple"/></inline-formula> are even potentials, but <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x22.png" xlink:type="simple"/></inline-formula> are odd ones.</p><p>In order to obtain super integrable couplings of super Yang hierarchy, we solve the adjoint representation of (7),</p><disp-formula id="scirp.75355-formula651"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x23.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.75355-formula652"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x24.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x25.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x26.png" xlink:type="simple"/></inline-formula> are commuting fields, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x27.png" xlink:type="simple"/></inline-formula> are anti-com- muting fields.</p><p>Substituting</p><disp-formula id="scirp.75355-formula653"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x28.png"  xlink:type="simple"/></disp-formula><p>into previous equation gives the following recursive formulas</p><disp-formula id="scirp.75355-formula654"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x29.png"  xlink:type="simple"/></disp-formula><p>From previous equations, we can successively deduce</p><disp-formula id="scirp.75355-formula655"><graphic  xlink:href="http://html.scirp.org/file/75355x30.png"  xlink:type="simple"/></disp-formula><p>Equation (11) can be written as</p><disp-formula id="scirp.75355-formula656"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x31.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.75355-formula657"><graphic  xlink:href="http://html.scirp.org/file/75355x32.png"  xlink:type="simple"/></disp-formula><p>Then, let us consider the spectral problem (7) with the following auxiliary problem</p><disp-formula id="scirp.75355-formula658"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x33.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.75355-formula659"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x34.png"  xlink:type="simple"/></disp-formula><p>From the compatible condition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x35.png" xlink:type="simple"/></inline-formula> according to (7) and (13), we get the zero curvature equation</p><disp-formula id="scirp.75355-formula660"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x36.png"  xlink:type="simple"/></disp-formula><p>which gives a nonlinear Lax super integrable hierarchy</p><disp-formula id="scirp.75355-formula661"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x37.png"  xlink:type="simple"/></disp-formula><p>The super integrable hierarchy (16) is a nonlinear super integrable couplings for the Yang hierarchy in [<xref ref-type="bibr" rid="scirp.75355-ref15">15</xref>]</p><disp-formula id="scirp.75355-formula662"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x38.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Super Hamiltonian Structures</title><p>A direct calculation reads</p><disp-formula id="scirp.75355-formula663"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x39.png"  xlink:type="simple"/></disp-formula><p>Substituting above results into the super trace identity [<xref ref-type="bibr" rid="scirp.75355-ref7">7</xref>]</p><disp-formula id="scirp.75355-formula664"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x40.png"  xlink:type="simple"/></disp-formula><p>Comparing the coefficients of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x41.png" xlink:type="simple"/></inline-formula> on both side of (19). From the initial values in (11), we obtain<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x42.png" xlink:type="simple"/></inline-formula>. Thus we have</p><disp-formula id="scirp.75355-formula665"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x43.png"  xlink:type="simple"/></disp-formula><p>It then follows that the nonlinear super integrable couplings (16) possess the following super Hamiltonian form</p><disp-formula id="scirp.75355-formula666"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x44.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.75355-formula667"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x45.png"  xlink:type="simple"/></disp-formula><p>is a super Hamiltonian operator and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x46.png" xlink:type="simple"/></inline-formula> are Hamiltonian functions.</p></sec><sec id="s5"><title>5. Reductions</title><p>Taking <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x47.png" xlink:type="simple"/></inline-formula> (16) reduces to a nonlinear integrable couplings of the Yang hierarchy in [<xref ref-type="bibr" rid="scirp.75355-ref13">13</xref>].</p><p>When <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x48.png" xlink:type="simple"/></inline-formula> in (16), we obtain the nonlinear super integrable couplings of the second order super Yang equations</p><disp-formula id="scirp.75355-formula668"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x49.png"  xlink:type="simple"/></disp-formula><p>Especially, taking <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x50.png" xlink:type="simple"/></inline-formula> in (23), we can obtain the nonlinear integrable couplings of the second order Yang equations in [<xref ref-type="bibr" rid="scirp.75355-ref13">13</xref>]</p><disp-formula id="scirp.75355-formula669"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x51.png"  xlink:type="simple"/></disp-formula><p>If setting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/75355x52.png" xlink:type="simple"/></inline-formula> in (23), we obtain the second order super Yang equations of (17) in [<xref ref-type="bibr" rid="scirp.75355-ref15">15</xref>]</p><disp-formula id="scirp.75355-formula670"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/75355x53.png"  xlink:type="simple"/></disp-formula></sec><sec id="s6"><title>6. Remarks</title><p>In this paper, we introduced an approach for constructing nonlinear integrable couplings of super integrable hierarchy. The method in this paper can be applied to other super integrable systems for constructing their integrable couplings. How to obtain the soliton solutions about equations deduced in this paper is worth considering for our future work.</p></sec><sec id="s7"><title>Acknowledgements</title><p>This work work was supported by the Natural Science Foundation of Henan Province (No. 162300410075), the Science and Technology Key Research Foundation of the Education Department of Henan Province (No.14A110010).</p></sec><sec id="s8"><title>Cite this paper</title><p>Tao, S.X. and Ma, Y.L. (2017) Nonlinear Super Integrable Couplings of Super Yang Hierarchy and Its Super Hamiltonian Structures. 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