<?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">JMP</journal-id><journal-title-group><journal-title>Journal of Modern Physics</journal-title></journal-title-group><issn pub-type="epub">2153-1196</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmp.2013.42035</article-id><article-id pub-id-type="publisher-id">JMP-28330</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>
 
 
  Wronskian Representation of Solutions of NLS Equation, and Seventh Order Rogue Wave
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ierre</surname><given-names>Gaillard</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>Université de Bourgogne, Dijon, France</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>Pierre.Gaillard@u-bourgogne.fr</email></corresp></author-notes><pub-date pub-type="epub"><day>05</day><month>02</month><year>2013</year></pub-date><volume>04</volume><issue>02</issue><fpage>246</fpage><lpage>266</lpage><history><date date-type="received"><day>November</day>	<month>28,</month>	<year>2012</year></date><date date-type="rev-recd"><day>December</day>	<month>30,</month>	<year>2012</year>	</date><date date-type="accepted"><day>January</day>	<month>8,</month>	<year>2013</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 use the representation of the solutions of the focusing nonlinear Schrodinger equation we have constructed recently, in terms of wronskians; when we perform a special passage to the limit, we get quasi-rational solutions expressed as a ratio of two determinants. We have already construct breathers of orders N = 4, 5, 6 in preceding works; we give here the breather of order seven. 
 
</p></abstract><kwd-group><kwd>Riemann Theta Functions; Fredholm Determinant; Wronskian; NLS Equation; Peregrine Breathers; Akhmediev Solutions</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>From fundamental work of Zakharov and Shabat in 1968 [1,2], a lot of research has been carried out on the nonlinear Schr&#246;dinger equation (NLS). The case of periodic and almost periodic algebro-geometric solutions to the focusing NLS equation were first constructed in 1976 by Its and Kotlyarov [<xref ref-type="bibr" rid="scirp.28330-ref3">3</xref>]. The first quasi-rational solutions of NLS equation were construted in 1983 by Peregrine [<xref ref-type="bibr" rid="scirp.28330-ref4">4</xref>]; they are nowadays called worldwide Peregrine breathers. In 1986, Eleonski, Akhmediev and Kulagin obtained the two-phase almost periodic solution to the NLS equation and obtained the first higher order analogue of the Peregrine breather [5,6]. Other families of higher order were constructed in a series of articles by Akhmediev et al. [7,8] using Darboux transformations.</p><p>In 2010, it has been shown in [<xref ref-type="bibr" rid="scirp.28330-ref9">9</xref>] that rational solutions of NLs equation can be writen as a quotient of two wronskians.</p><p>In this paper, we use a result [<xref ref-type="bibr" rid="scirp.28330-ref10">10</xref>] giving a new representation of the solutions of the NLS equation in terms of a ratio of two wronskians determinants of even order 2N composed of elementary functions; the related solutions of NLS are called of order N. When we perform the passage to the limit when some parameter tends to 0, we got families of multi-rogue wave solutions of the focusing NLS equation depending on a certain number of parameters. It allows to recognize the famous Peregrine breather [<xref ref-type="bibr" rid="scirp.28330-ref4">4</xref>] and also higher order Peregrine’s breathers constructed by Akhmediev [7,11].</p><p>Recently, another representation of the solutions of the focusing NLS equation, as a ratio of two determinants has been given in [<xref ref-type="bibr" rid="scirp.28330-ref12">12</xref>] using generalized Darboux transform.</p><p>A new approach has been done in [<xref ref-type="bibr" rid="scirp.28330-ref13">13</xref>] which gives a determinant representation of solutions of the focusing NLS equation, obtained from Hirota bilinear method, derived by reduction of the Gram determinant representation for Davey-Stewartson system.</p><p>We have already given breathers of order N = 1 to N = 6 in [<xref ref-type="bibr" rid="scirp.28330-ref14">14</xref>]. Here, we construct the breather of order N = 7 which shows the efficiency of this method.</p></sec><sec id="s2"><title>2. Expression of Solutions of NLS Equation in Terms of Wronskian Determinant and Quasi-Rational Limit</title><sec id="s2_1"><title>2.1. Solutions of NLS Equation in Terms of Wronskian Determinant</title><p>We briefly recall results obtained in [10,14]. We consider the focusing NLS equation</p><disp-formula id="scirp.28330-formula39591"><label>(1)</label><graphic position="anchor" xlink:href="15-7501105\39d5d11f-7461-416f-8104-ee110d513d55.jpg"  xlink:type="simple"/></disp-formula><p>From [<xref ref-type="bibr" rid="scirp.28330-ref14">14</xref>], the solution of the NLS equation can be written in the form</p><disp-formula id="scirp.28330-formula39592"><label>(2)</label><graphic position="anchor" xlink:href="15-7501105\14ee2875-5e14-4796-aca8-8c80f3629210.jpg"  xlink:type="simple"/></disp-formula><p>In (2), the matrix <img src="15-7501105\a5ea19f9-ec8c-4009-9804-7b3a8498d290.jpg" /> is defined by</p><disp-formula id="scirp.28330-formula39593"><label>(3)</label><graphic position="anchor" xlink:href="15-7501105\c28757cf-f802-41b3-8fee-3d1b615bcdb0.jpg"  xlink:type="simple"/></disp-formula><p>The terms <img src="15-7501105\66c11240-03dd-4cb4-89e1-a3612a4c5792.jpg" /> and <img src="15-7501105\79ae8944-e41c-4212-b440-9bc508ad1bc1.jpg" /> are functions of the parameters <img src="15-7501105\40f91e91-9c9f-4d07-baa9-cdb9880dadb9.jpg" /> satisfying the relations</p><p><img src="15-7501105\171d7090-fe75-45a8-b7c3-3e8b430e3b78.jpg" /></p><p>They are given by the following equations,</p><p><img src="15-7501105\b9c1cbf2-a73c-46a3-abbc-dc37a9f747ef.jpg" /></p><p>and</p><p><img src="15-7501105\312bcd4e-236d-42e9-93af-e1781e4474c7.jpg" />.</p><p>The terms <img src="15-7501105\3238f81c-2502-41b1-9b47-4510dd003f84.jpg" /> are defined by</p><p><img src="15-7501105\b8d8b66f-b0aa-45a4-a888-f33096039522.jpg" /></p><p>The coefficients <img src="15-7501105\c2680a0c-868b-4670-b6a4-2e4315acd78d.jpg" /> are defined by :</p><disp-formula id="scirp.28330-formula39594"><label>(4)</label><graphic position="anchor" xlink:href="15-7501105\fccfdd1d-66fc-4de1-be76-a848dd297227.jpg"  xlink:type="simple"/></disp-formula><p>We consider the following functions</p><disp-formula id="scirp.28330-formula39595"><label>(5)</label><graphic position="anchor" xlink:href="15-7501105\3c5fe482-d3fb-4bd6-93d7-7d7fe3a23c40.jpg"  xlink:type="simple"/></disp-formula><p>We use the following notations:</p><p><img src="15-7501105\2bd8b6c4-a05e-4c95-8739-22c6962f600e.jpg" />.</p><p><img src="15-7501105\75760f2b-6fcb-4971-83e2-76b92839da35.jpg" />is the wronskian</p><disp-formula id="scirp.28330-formula39596"><label>(6)</label><graphic position="anchor" xlink:href="15-7501105\77876d7c-d203-41ea-b128-037135f138a6.jpg"  xlink:type="simple"/></disp-formula><p>We consider the matrix <img src="15-7501105\3e06ca2b-d9bb-47ca-8b30-f72e29fe8030.jpg" /> defined by</p><p><img src="15-7501105\31926c1c-427e-4481-a763-608d12fc7b7e.jpg" /></p><p>Then we get the following link between Fredohlm and Wronskian determinants [<xref ref-type="bibr" rid="scirp.28330-ref14">14</xref>]</p><sec id="s2_1_1"><title>Theorem 2.1</title><disp-formula id="scirp.28330-formula39597"><label>(7)</label><graphic position="anchor" xlink:href="15-7501105\b7561079-4f78-42b2-94ea-5543317c02da.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="15-7501105\253cedfc-17da-44c7-ba72-8fb0967d744d.jpg" /></p><p>It can be deduced the following result:</p><p>Theorem 2.2 The function v defined by</p><disp-formula id="scirp.28330-formula39598"><label>(8)</label><graphic position="anchor" xlink:href="15-7501105\aac68882-359f-4439-a8c8-7d0f5c42b9b6.jpg"  xlink:type="simple"/></disp-formula><p>is solution of the NLS Equation (1)</p><p><img src="15-7501105\948128c2-5227-42ad-a4a0-0d4d3db96263.jpg" /></p></sec></sec><sec id="s2_2"><title>2.2. Quasi-Rational Solutions of NLS Equation</title><p>In the following, we take the limit when the parameters <img src="15-7501105\884b20e5-580b-455d-b414-3c481f59e062.jpg" /> for <img src="15-7501105\8a49daa3-7979-4e4b-a350-8be01ef28fd1.jpg" /> and <img src="15-7501105\64ac1f9a-00f1-4987-99f8-adaaede6f07e.jpg" /> for <img src="15-7501105\5cb1e082-dcf9-4ab8-b089-660e1354c35e.jpg" />.</p><p>For simplicity, we denote <img src="15-7501105\61ff385b-666a-45f6-8530-6f8096b8c31e.jpg" /> the term<img src="15-7501105\3fa9371e-a371-4596-948f-01c17b40ad84.jpg" />.</p><p>We consider the parameter <img src="15-7501105\a1142d38-f3c8-4813-9aa3-85f75f379ef5.jpg" /> written in the form</p><disp-formula id="scirp.28330-formula39599"><label>(9)</label><graphic position="anchor" xlink:href="15-7501105\80fad1cf-caa3-4e27-a383-f4113cf15cfc.jpg"  xlink:type="simple"/></disp-formula><p>When <img src="15-7501105\57f8b7d6-299e-4b86-a63f-0367c76cd5eb.jpg" /> goes to 0, we realize limited expansions at order p, for<img src="15-7501105\ec8eae13-e5ea-4547-a0af-c92d20c2cf9e.jpg" />, of the terms</p><p><img src="15-7501105\91b656d4-b5f1-4e26-bff8-7d06e1b4e610.jpg" /></p><p><img src="15-7501105\61dd4fd4-bd07-4201-80fd-bb5b1a3f8610.jpg" /></p><p><img src="15-7501105\8dfe0889-587a-4815-bca8-88c3fc3527bb.jpg" /></p><p><img src="15-7501105\22e72415-506c-4558-a78e-5afcfad4ab80.jpg" /></p><p><img src="15-7501105\81cc4727-a606-4fbe-87d6-f9013deb9a9c.jpg" /></p><p><img src="15-7501105\42360597-12e2-443f-9c2e-a8f29838ae56.jpg" /></p><p><img src="15-7501105\60846924-020c-4b3a-b8c1-643ff8a7aaa5.jpg" /></p><p><img src="15-7501105\a2dafebd-ad46-4d17-a3fe-e9a637460e79.jpg" /></p><p>We have the central result formulated in [<xref ref-type="bibr" rid="scirp.28330-ref14">14</xref>] :</p><p>Theorem 2.3 The function v defined by</p><disp-formula id="scirp.28330-formula39600"><label>(10)</label><graphic position="anchor" xlink:href="15-7501105\e09117d9-a0b6-4692-86d4-e0bb2d027bb1.jpg"  xlink:type="simple"/></disp-formula><p>is a quasi-rational solution of the NLS Equation (1)</p><p><img src="15-7501105\efc299e1-0493-45c5-a9c4-cdd42df1ea15.jpg" /></p><p>Proof: Let <img src="15-7501105\bea0242a-03bc-4bdb-af03-8c653d97a949.jpg" /> be the complex number</p><p><img src="15-7501105\56bab548-80c6-4f78-80d9-d09aa0c69033.jpg" />, <img src="15-7501105\52806c78-ed5d-4b1e-8a1f-d2c0fd47bdd0.jpg" />,<img src="15-7501105\384eba7f-283a-4967-8b73-e432eb489832.jpg" />. We use the following functions:</p><disp-formula id="scirp.28330-formula39601"><label>(11)</label><graphic position="anchor" xlink:href="15-7501105\37290cea-c1c7-427d-94ea-4fb4eb75b40a.jpg"  xlink:type="simple"/></disp-formula><p>for<img src="15-7501105\fdf992b8-9187-4d3c-85b0-3de2bc099a7a.jpg" />, and</p><disp-formula id="scirp.28330-formula39602"><label>(12)</label><graphic position="anchor" xlink:href="15-7501105\7baa17c9-04fd-401c-aebf-0b379a03bd70.jpg"  xlink:type="simple"/></disp-formula><p>for<img src="15-7501105\6d2e4353-619a-4a4b-aab2-2c5430e26b46.jpg" />.</p><p>We define the functions <img src="15-7501105\6bc4264e-7287-422a-bc37-b590a5c56426.jpg" /> for<img src="15-7501105\d4f1f3fb-e1af-4dfe-90ca-87cf2a870b0f.jpg" />, <img src="15-7501105\d94c5958-24cc-43c4-961b-4b4293ab6afe.jpg" /> in the same way, where the term <img src="15-7501105\ce1c23fd-66c0-4479-8752-33bcf3147fb2.jpg" /> in <img src="15-7501105\421a98a8-b731-445a-bba3-18ad70396478.jpg" /> is replaced by<img src="15-7501105\0a757d06-5cd2-47e2-a708-8f061a6fc230.jpg" />.</p><p>Then it is clear that</p><disp-formula id="scirp.28330-formula39603"><label>(13)</label><graphic position="anchor" xlink:href="15-7501105\5ca89668-1bd5-47a1-ac37-d4710254b32e.jpg"  xlink:type="simple"/></disp-formula><p>All the functions <img src="15-7501105\04028f33-fce7-45c4-a795-ea321d401cf2.jpg" /> and <img src="15-7501105\662b6973-083c-4a0d-b40d-90fc977da27e.jpg" /> and their derivatives depend on <img src="15-7501105\41fe820d-6210-4135-b804-a1d3d4279e0b.jpg" /> and can all be prolonged by continuity when<img src="15-7501105\1de57fea-a590-44ca-85e2-745a568336c9.jpg" />.</p><p>For simplicity we denote <img src="15-7501105\16dad1a5-7df8-4281-a976-d720f55d5aff.jpg" /> the term</p><p><img src="15-7501105\9f1f099f-aefa-4761-84e9-62aab5355bed.jpg" />, <img src="15-7501105\a13e953e-5c02-4330-af4c-9a480d19b4bd.jpg" />and <img src="15-7501105\4e75d24a-4d1d-4b72-a586-59ab7ba3ea86.jpg" /> the term<img src="15-7501105\e3ae2cbd-b641-4f2e-9da6-1b9db0cb0b71.jpg" />.</p><p>Then we use the expansions</p><p><img src="15-7501105\567edbbe-d4fe-4589-98d3-4f7789311225.jpg" /></p><p><img src="15-7501105\6741ecd0-356d-4ac1-b22f-e7b64ec40ed9.jpg" /></p><p>We have the same expansions for the functions<img src="15-7501105\644eb236-211a-4764-b403-3115ae413e3c.jpg" />.</p><p><img src="15-7501105\025f0b39-f6ac-4c8a-8688-e61e56792e6a.jpg" /></p><p><img src="15-7501105\8f9208cf-d7f4-42a2-89fd-c410d659f22a.jpg" /></p><p>The components j of the columns 1 and N + 1 are respectively equal by definition to <img src="15-7501105\9cfffada-48bd-4130-b4b3-dd117c6a1fee.jpg" /> for<img src="15-7501105\0123c15f-28e2-4011-b6e7-44b9e23bb865.jpg" />, <img src="15-7501105\a9e6beda-76cd-4296-ad87-fce356583b96.jpg" />for <img src="15-7501105\652c88ad-168e-44c5-adfd-ad1161f1e6ac.jpg" /> of<img src="15-7501105\59f6a829-a06d-47cb-a75b-52540bbc8a80.jpg" />, and <img src="15-7501105\19720c5e-d4b9-489b-acee-1f627bf6db6b.jpg" /> for<img src="15-7501105\9cdd69a9-e917-4476-a69f-f1d8590e3a5e.jpg" />, <img src="15-7501105\db933b38-7fe5-4205-8800-b20bd53f7843.jpg" />for <img src="15-7501105\a4b6d3e6-f90b-43ab-b221-1a98bebffa5f.jpg" /> of<img src="15-7501105\25014217-1b0a-4a13-9564-46f1419b80ae.jpg" />.</p><p>At the first step of the reduction, we replace the columns <img src="15-7501105\e0968339-2f21-4a3a-9f98-e1cff94dac78.jpg" /> by <img src="15-7501105\1fc843d2-0399-47bf-8ac0-c2242817e7db.jpg" /> and <img src="15-7501105\6b04ba24-0d52-4bbc-a9ba-b38726e4a444.jpg" /> by <img src="15-7501105\e1bc4f4d-c642-4fb8-ae17-9992a63a0591.jpg" /> for<img src="15-7501105\01e727db-298c-49d4-817d-f9ab8fd58733.jpg" />, for<img src="15-7501105\d2e35e6d-0f28-4097-86b9-a27567b12b85.jpg" />; we do the same changes for<img src="15-7501105\08397453-4780-4279-93bd-6ad304795512.jpg" />. Each component j of the column <img src="15-7501105\033b9ce1-e041-44d3-bae9-1ed49243cde4.jpg" /> of <img src="15-7501105\e5a1f223-a18d-41a2-9b14-f3896e192b06.jpg" /> can be rewritten as</p><p><img src="15-7501105\ff302858-b002-4318-a1da-b12d3c270248.jpg" /></p><p>and the column <img src="15-7501105\035bb93c-3add-4026-867e-771a6d068f56.jpg" /> replaced by</p><p><img src="15-7501105\e766a5a5-1a8e-49a3-b6db-33699416b42d.jpg" /></p><p>for<img src="15-7501105\93af6a53-0bd7-4a29-a2df-58f84ed35393.jpg" />. For<img src="15-7501105\d98084c9-3c1f-4204-b828-b23565ebb10c.jpg" />, we have the same reductions, each component j of the column <img src="15-7501105\e6dfdf7e-024b-49bf-b507-86dba7ca1527.jpg" /> of can be rewritten as</p><p><img src="15-7501105\24d594e7-de69-4242-8f30-ff5b56c8fb98.jpg" /></p><p>and the column <img src="15-7501105\59b52809-2ac5-4f29-a46c-3a18b9d2e0b9.jpg" /> replaced by</p><p><img src="15-7501105\1a28dcc7-e190-4f57-bfee-b1e95fa5f533.jpg" /></p><p>for<img src="15-7501105\5cb92147-7954-4c12-b862-2c1bf99ffa9f.jpg" />.</p><p>We can factorize in D<sub>3</sub> and D<sub>1</sub> in each column k and <img src="15-7501105\c3bcb8c1-e548-4f49-a905-090b5ac8f3a3.jpg" /> the term <img src="15-7501105\d22aa4de-85bb-46a8-934c-c3ecf6b931d7.jpg" /> for<img src="15-7501105\e5f10d90-e797-469e-b9b7-e48008149fec.jpg" />, and so simplify these common terms in numerator and denominator.</p><p>If we restrict the developments at order 1 in columns 2 and<img src="15-7501105\6438f42c-f951-4e77-b585-08bebc72ce4e.jpg" />, we get respectively <img src="15-7501105\21235fb4-d9c0-4b5a-afb4-bbaa1951adc0.jpg" /> for the component j of D<sub>2</sub>, <img src="15-7501105\bd5cf888-be52-4709-bbec-03f1df238c40.jpg" />for the component j of <img src="15-7501105\e43b9b79-472a-4f15-8d02-c372b501c4b8.jpg" /> of D<sub>3</sub>, and <img src="15-7501105\693ab3a5-81da-46d8-a52e-3565fe879b43.jpg" /> for the component j of<img src="15-7501105\36ea5b16-d18c-4d28-a4e6-87646ddc5790.jpg" />, <img src="15-7501105\54e5913b-c78f-4b18-bf1f-712c662a3252.jpg" />for the component j of <img src="15-7501105\ced40eff-7793-42b1-8213-dcf2c9a7aca4.jpg" /> of D<sub>1</sub>. This algorithm can be continued until the columns C<sub>N</sub>, C<sub>2N</sub> of D<sub>3</sub> and<img src="15-7501105\202050a6-3922-4407-b09e-e01632861616.jpg" />, <img src="15-7501105\625dd294-bc63-4f9a-9632-bfd21951d418.jpg" />of D<sub>1</sub>.</p><p>Then taking the limit when <img src="15-7501105\d047c9cc-41d5-47f6-b6ce-b77d0755d64b.jpg" /> tends to 0, <img src="15-7501105\8a0a9c2b-d43f-4515-80ce-65ad3a90035d.jpg" />can be replaced by <img src="15-7501105\a583131a-b599-4c97-84cf-df978c6c819e.jpg" /></p><disp-formula id="scirp.28330-formula39604"><label>(14)</label><graphic position="anchor" xlink:href="15-7501105\8329b417-8c59-4346-9062-3a636a1cfeb2.jpg"  xlink:type="simple"/></disp-formula><p>Each element of these determinants is a polynomial in x and t. So the solution of the NLS equation takes the form <img src="15-7501105\038eed8e-80d3-4d85-bbb4-215863e6b44c.jpg" /> with <img src="15-7501105\c2fa222d-4748-46ce-879b-befa26c762b9.jpg" /> a rational function in x and t, and which ends the proof.<img src="15-7501105\14d2ed93-368e-4841-a6ee-09132178fa7a.jpg" /></p></sec></sec><sec id="s3"><title>3. Seventh-Order Breather Solution of NLS Equation</title><sec id="s3_1"><title>3.1. Fiber-Optics Case</title><p>To get solutions of NLS equation written in the context of fiber optics</p><disp-formula id="scirp.28330-formula39605"><label>(15)</label><graphic position="anchor" xlink:href="15-7501105\638c6e96-42a0-47d7-a818-a51d01de7d2e.jpg"  xlink:type="simple"/></disp-formula><p>from these of (1), we can make the following changes of variables</p><disp-formula id="scirp.28330-formula39606"><label>(16)</label><graphic position="anchor" xlink:href="15-7501105\c4fe3dcb-705b-468b-95b4-10ee9aedf01c.jpg"  xlink:type="simple"/></disp-formula><p>Equation (15) plays a fundamental role in optics and is the object of active research as recent work [<xref ref-type="bibr" rid="scirp.28330-ref8">8</xref>] attests it where the solutions of the two-breathers are studied.</p></sec><sec id="s3_2"><title>3.2. Case of the Initial Conditions</title><p>In the case of order N = 7, we make an expansion at order 13. Taking the limit when <img src="15-7501105\9d399f72-18fa-4188-bf1c-73e4b7da014c.jpg" /> with d<sub>j</sub> = j, 1 ≤ j ≤ N, the solution of NLS Equation (15) takes the form</p><p><img src="15-7501105\9041cec1-e908-4bda-9dbb-2ba8795d2a15.jpg" /></p><p>Because of the length of the complete analytical expression, we only give it in the appendix.</p><p>We give here the expression of the solution in the form</p><p><img src="15-7501105\814d0b7b-903d-4670-8ea2-149f0d6a0374.jpg" /></p><p>in the case t = 0:</p><p>Remark 3.1 The expressions of <img src="15-7501105\306ea6bc-014a-4b76-98f2-72a8003b14b9.jpg" /> and <img src="15-7501105\8022f6c0-4fc9-4572-b1d4-34807bace9a6.jpg" /> can be easily verified from the recursive formulae given in [<xref ref-type="bibr" rid="scirp.28330-ref11">11</xref>].</p></sec><sec id="s3_3"><title>3.3. Plot in the (x, t) Coordinates</title><p>Please see <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>The method described in the present paper provides a powerful tool to get explicitly solutions of the NLS equation.</p><p>To the best of my knowledge, it is the first time that the breather of order seven solution of the NLS equation is presented.</p><p>It confirms the conjecture about the shape of the rogue wave in the <img src="15-7501105\f752ac7d-c96c-4421-93c5-b2cc3362f598.jpg" /> coordinates, the maximum of amplitude equal to 2N + 1 = 15 and the degree of polynomials in x and t here equal to 56 as already formulated in [<xref ref-type="bibr" rid="scirp.28330-ref7">7</xref>]. This new formulation gives the possibility, by introduction of parameters in the arguments of preceding functions defined in the text, to create an infinite set of non singular solutions of NLS equation. It will be the next step of the work which will open a large way to future researches in this domain.</p></sec><sec id="s5"><title>REFERENCES</title></sec><sec id="s6"><title>Appendix</title><p>Rather than to give the analytical expression in the form<img src="15-7501105\587891cb-2f18-4c54-9707-efd0eee661a4.jpg" />, to shorten the formulation one prefers to give that inspired by Akhmediev et al. in [<xref ref-type="bibr" rid="scirp.28330-ref11">11</xref>].</p><p>The solution of NLS equation takes the form, with N = 7</p><p><img src="15-7501105\9df6dd26-d5b5-451a-9d4f-f692ded26634.jpg" /></p><p>with</p><p><img src="15-7501105\159256cf-9851-4c38-aae6-be21185b3c00.jpg" /></p><p><img src="15-7501105\e8b40621-a366-4a17-a3fe-92128522e0d1.jpg" /></p><p><img src="15-7501105\ca84c523-5c25-49a3-a566-6c87cab2a68e.jpg" /></p><p><img src="15-7501105\ac1f4f58-321f-48e3-ae6a-2732a3300051.jpg" /></p><p><img src="15-7501105\8673e906-6d2b-4ccb-a3ec-95f710dfec62.jpg" /></p><p><img src="15-7501105\dfe068c4-38ca-4fcf-b9a4-cfcae697f070.jpg" /></p><p><img src="15-7501105\45cc7c99-1336-4526-9628-7e35e69b6b16.jpg" /></p><p><img src="15-7501105\df43d4d7-b880-44d8-ac5d-aafd5d85eea0.jpg" /></p><p><img src="15-7501105\86305494-1b9d-454f-8e98-ef4f6872b07e.jpg" /></p><p><img src="15-7501105\67204a81-60f0-4706-a1d9-c596021f0d7f.jpg" /></p><p><img src="15-7501105\2f7a542f-53d0-4f4b-bfd9-1c80a2d9da1f.jpg" /></p><p><img src="15-7501105\a4f1392a-08c0-407b-bcc3-65ed5aa79d30.jpg" /></p><p><img src="15-7501105\68ecae55-8d5a-4b25-b2a5-4744f5187a13.jpg" /></p><p><img src="15-7501105\0be4f6e3-19ef-4b28-bc4a-99303b08b0c2.jpg" /></p><p><img src="15-7501105\f1492229-de34-4005-9b8b-cf1e1f3fb3fe.jpg" /></p><p><img src="15-7501105\a0d78254-b287-46aa-8e61-401e2ce69f29.jpg" /></p><p><img src="15-7501105\3635f94a-7c62-4046-b5b6-0dbcf680f45e.jpg" /></p><p><img src="15-7501105\e4803b3c-d27f-4378-b1e8-6f9c37704067.jpg" /></p><p><img src="15-7501105\7d368b7a-9476-4b53-95e7-e0215fbfb763.jpg" /></p><p><img src="15-7501105\0b0cfa47-7cc3-4776-a935-71ba492454a5.jpg" /></p><p><img src="15-7501105\b276f4b1-ae0c-4687-8bac-5d4ae94b4c8b.jpg" /></p><p><img src="15-7501105\07ea653b-301c-4508-b375-6fef03441219.jpg" /></p><p><img src="15-7501105\93ac24cd-458f-4669-9b1c-58eeb4bde631.jpg" /></p><p><img src="15-7501105\067bf851-8af8-42dc-b2e5-fd099f22a5f5.jpg" /></p><p><img src="15-7501105\c0de5201-9e8b-498f-a07c-fef8efcd5f9a.jpg" /></p><p><img src="15-7501105\ed12ac24-be7e-4d3a-a8a4-b2fefc7ff469.jpg" /></p><p><img src="15-7501105\54dc8243-80bf-481d-bbeb-f93dba8c7460.jpg" /></p><p><img src="15-7501105\3b38e0ee-41f6-41eb-96b7-4e6e7f0a4ed7.jpg" /></p><p><img src="15-7501105\f416b433-743e-4f42-a799-c5528c4d9294.jpg" /></p><p><img src="15-7501105\6c0df648-44d6-4ad9-ba0a-0b2d51efdeeb.jpg" /></p><p><img src="15-7501105\41297950-9756-450b-a0fc-26958d3a949f.jpg" /></p><p><img src="15-7501105\dc90bb36-d3c1-4286-98e4-f052b9bad277.jpg" /></p><p><img src="15-7501105\96aa341b-490f-44e8-a8fc-75fb0829c1ac.jpg" /></p><p><img src="15-7501105\f718db83-1eb2-48db-9346-826b48fc9d36.jpg" /></p><p><img src="15-7501105\028239ee-608a-45a4-8b1e-51002f6f4ca1.jpg" /></p><p><img src="15-7501105\c21f46e4-a526-448d-aaeb-65e795be8799.jpg" /></p><p><img src="15-7501105\1d54d408-b750-47f9-bebf-3dd9cdecd52a.jpg" /></p><p><img src="15-7501105\6966b32c-b2a6-4cc9-85f2-9607bd46b431.jpg" /></p><p><img src="15-7501105\65f37351-d01f-4fad-98ac-140263838982.jpg" /></p><p><img src="15-7501105\74c1dd54-fb4d-458a-9ca3-1aa63b7c6c8f.jpg" /></p><p><img src="15-7501105\9fe09227-3767-4a06-ae89-8064a34ed52a.jpg" /></p><p><img src="15-7501105\bdc21534-9cfc-4ad2-a41f-64d44320b521.jpg" /></p><p><img src="15-7501105\8932c247-d5a4-4f2a-bd2c-339cfdcdd927.jpg" /></p><p><img src="15-7501105\b63e9fa5-2f2a-4dbe-abee-b906f44bfaa1.jpg" /></p><p><img src="15-7501105\2141660d-61aa-4e1b-a9f9-2e418eb927e1.jpg" /></p><p><img src="15-7501105\a881f132-ded5-4351-8e06-b543448928fb.jpg" 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src="15-7501105\3fbe0d2d-e5d3-4b59-9fbf-6096825451df.jpg" /></p><p><img src="15-7501105\2709f72b-f1e5-4ea0-91af-b6c6893cd456.jpg" /></p><p><img src="15-7501105\90e93753-1985-43c8-b056-a976a89f55ed.jpg" /></p><p><img src="15-7501105\2df6341e-b5de-4244-86da-b89bb08b6696.jpg" /></p><p><img src="15-7501105\cd2d4601-e52e-4f32-8e48-c8900f54eecf.jpg" /></p><p><img src="15-7501105\3a2f92e6-1218-4092-a84d-586495c13f75.jpg" /></p><p><img src="15-7501105\e08fb138-528b-4928-b566-0ce02372de35.jpg" /></p><p><img src="15-7501105\74fe96ef-4d4d-4afd-b80d-52684abfff09.jpg" /></p><p><img src="15-7501105\f8ed603c-83e1-4a96-bcef-3c14953e4674.jpg" /></p><p><img src="15-7501105\d8a4ab75-86d4-41a3-92ef-2f0e8734c92c.jpg" /></p><p><img src="15-7501105\c5d28f82-131c-428a-92e0-ade2d32677e3.jpg" /></p><p><img src="15-7501105\6f5b6956-8a39-442c-9534-75c0dc19043e.jpg" /></p><p><img src="15-7501105\dff79bcb-dfee-4251-b191-b5ded77baeaa.jpg" /></p><p><img src="15-7501105\6a004baf-5fce-4c1d-8be2-77b3115eed91.jpg" 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src="15-7501105\fe005f85-025a-46ca-9ba7-aacbc0d5e76e.jpg" /></p><p><img src="15-7501105\9db72e74-8af7-471e-b975-10f2a1eda520.jpg" /></p><p><img src="15-7501105\03766171-70d6-4f87-bd40-717a08bf0b08.jpg" /></p><p><img src="15-7501105\19ba7be0-43b2-40a2-be60-bb878af2513e.jpg" /></p><p><img src="15-7501105\4aef6074-63c3-422b-bd7a-27877a0d0a32.jpg" /></p><p><img src="15-7501105\652d82ee-631b-4dcf-a6dd-be01a38f1a5e.jpg" /></p><p><img src="15-7501105\4c474312-8aab-4d9e-bd12-13bdbe094bb6.jpg" /></p><p><img src="15-7501105\e480bd73-893f-495e-a5d4-a7aead71ea79.jpg" /></p><p><img src="15-7501105\03ba0445-8915-4e39-a603-5f756620c88d.jpg" /></p><p><img src="15-7501105\6e8003a7-8b66-43e6-9499-12075d689b3b.jpg" /></p><p><img src="15-7501105\194a5172-af96-4778-8fc1-33d77d177616.jpg" /></p><p><img src="15-7501105\b10a353b-dabb-49d1-84b7-2cc4f37aeff9.jpg" /></p><p><img src="15-7501105\a007a7a5-939d-4ece-a50c-b0c73785d120.jpg" /></p><p><img src="15-7501105\4cc5af89-9376-4e12-9a04-2d2070847079.jpg" 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src="15-7501105\13c9023c-79a2-479e-a1bf-4958671da75c.jpg" /></p><p><img src="15-7501105\70f6570e-c6a1-4606-9a45-03659c7f192c.jpg" /></p><p><img src="15-7501105\422bce8b-cc4b-42a9-b5e5-4f101a4b34c4.jpg" /></p><p><img src="15-7501105\8dbc401a-c0bc-4a16-9699-6872d720eaaa.jpg" /></p><p><img src="15-7501105\901b5ae9-117f-40a7-a89e-e26ef82fccb9.jpg" /></p><p><img src="15-7501105\c53ec20d-d516-414f-8c06-96b3f6a80b14.jpg" /></p><p><img src="15-7501105\af02a209-6ff8-4410-8371-7c933139127b.jpg" /></p><p><img src="15-7501105\ace90c4f-8683-452f-9bfe-9e4c3092d8dd.jpg" /></p><p><img src="15-7501105\b3a75d15-d793-4b7f-92e7-21fbaf96729f.jpg" /></p><p><img src="15-7501105\341eb82c-89b3-4889-9a80-6b15f34f7321.jpg" /></p><p><img src="15-7501105\a6f512d5-9de5-4936-99c7-a2c8e78d1fb6.jpg" /></p><p><img src="15-7501105\d23f4bda-c4c9-404f-9664-8bf95eaaf527.jpg" /></p><p><img src="15-7501105\03f3a966-b806-49b8-8c19-2243aa3d5a9e.jpg" /></p><p><img src="15-7501105\f02e0919-89f7-457f-bede-9dce91a2bded.jpg" 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src="15-7501105\dadea074-df7f-4767-a883-b0fa5b7350ad.jpg" /></p><p><img src="15-7501105\e4176f77-6a8a-4008-822d-dbc210b86181.jpg" /></p><p><img src="15-7501105\a88c9c73-fde7-4df7-b9e0-9a7284798a5c.jpg" /></p><p><img src="15-7501105\1b7f9b97-4c3c-4541-9e20-0012d477e3bf.jpg" /></p><p><img src="15-7501105\5e5762e7-e4e4-4304-8c6c-fa6fea8c8a02.jpg" /></p><p><img src="15-7501105\0b88426c-96e2-4fa4-bf8d-62ebf3ab65d9.jpg" /></p><p><img src="15-7501105\ee1aeaf7-44ca-4cbf-9551-beec6453761f.jpg" /></p><p><img src="15-7501105\0e9846fc-541f-4c73-a3d2-8e297ee0b0f0.jpg" /></p><p><img src="15-7501105\784335f0-d5a7-465d-95ac-6ea6ba2c42e7.jpg" /></p><p><img src="15-7501105\f4262304-a8a3-43f4-867f-5e5e1e72935f.jpg" /></p><p><img src="15-7501105\7aae1f82-cc05-44d8-b0fb-07e46a15f362.jpg" /></p><p><img src="15-7501105\e20b604a-f49f-432f-a756-4644ee49f746.jpg" /></p><p><img src="15-7501105\d7ff2257-819e-46dc-a0c2-6f706cc6f3b2.jpg" /></p></sec></body><back><ref-list><title>References</title><ref 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