Startseite Rogue-Wave Interaction of a Nonlinear Schrödinger Model for the Alpha Helical Protein
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Rogue-Wave Interaction of a Nonlinear Schrödinger Model for the Alpha Helical Protein

  • Hui-Xian Jia EMAIL logo , Yu-Jun Liu und Ya-Ning Wang
Veröffentlicht/Copyright: 4. November 2015

Abstract

In this article, we investigate a fourth-order nonlinear Schrödinger equation, which governs the Davydov solitons in the alpha helical protein with higher-order effects. By virtue of the generalised Darboux transformation, higher-order rogue-wave solutions are derived. Propagation and interaction of the rogue waves are analysed: (i) Coefficients affect the existence time of the first-order rogue waves; (ii) coefficients affect the interaction time of the second- and third-order rogue waves; (iii) direction of the rogue-wave propagation remain unchanged after interaction.

PACS numbers:: 47.35.Fg; 05.45.Yv; 02.30.Jr

Corresponding author: Hui-Xian Jia, Department of Basic, Shijiazhuang Post and Telecommunication Technical College, Shijiazhuang 050021, China, E-mail:

Acknowledgments

We express our sincere thanks to all the members of our discussion group for their valuable comments. This work has been supported by the Foundation of Hebei Education Department of China under Grant No. QN2015051.

Appendix A

θ^^1[2]=1480(45ieit2210eit2t28140eit2rt1080ieit2t228320ieit2rt2131040ieit2r2t2+1200eit2t3+36960eit2rt3+313920eit2r2t3+812160eit2r3t3+80ieit2t4+1920ieit2rt4+17280ieit2r2t4+69120ieit2r3t4+103680ieit2r4t432eit2t5960eit2rt511520eit2r2t569120eit2r3t5207360eit2r4t5248832eit2r5t5+30ieit2x+1200eit2tx+22560eit2rtx+2640ieit2t2x+62400ieit2rt2x+279360ieit2r2t2x320eit2t3x5760eit2rt3x34560eit2r2t3x69120eit2r3t3x160ieit2t4x3840ieit2rt4x34560ieit2r2t4x138240ieit2r3t4x207360ieit2r4t4x+120ieit2x21680eit2tx225440eit2rtx2480ieit2t2x25760ieit2rt2x217280ieit2r2t2x2+320eit2t3x2+5760eit2rt3x2+34560eit2r2t3x2+69120eit2r3t3x2240ieit2x3+320eit2tx3+1920eit2rtx3+320ieit2t2x3+3840ieit2rt2x3+11520ieit2r2t2x3+80ieit2x4160eit2tx4960eit2rtx432ieit2x5),

θ^1[2]=1480eit2(45+210it+28140irt+1080t2+28320rt2+131040r2t21200it336960irt3313920ir2t3812160ir3t380t41920rt417280r2t469120r3t4103680r4t4+32it5+960irt5+11520ir2t5+69120ir3t5+207360ir4t5+248832ir5t5+30x+1200itx+22560irtx+2640t2x+62400rt2x+279360r2t2x320it3x5760irt3x34560ir2t3x69120ir3t3x160t4x3840rt4x34560r2t4x138240r3t4x207360r4t4x120x2+1680itx2+25440irtx2+480t2x2+5760rt2x2+17280r2t2x2320it3x25760irt3x234560ir2t3x269120ir3t3x2240x3+320itx3+1920irtx3+320t2x3+3840rt2x3+11520r2t2x380x4+160itx4+960irtx432x5).

Appendix B

q^^[2]=45+360it+4464irt468t27920rt2+6192r2t2192it312672irt3131328ir2t3373248ir3t3528t49600rt458752r2t4124416r3t420736r4t4384it511520irt5138240ir2t5829440ir3t52488320ir4t52985984ir5t5+64t6+2304rt6+34560r2t6+276480r3t6+1244160r4t6+2985984r5t6+2985984r6t6180x2+576itx2+12672irtx21440t2x226496rt2x2107136r2t2x2768it3x213824irt3x282944ir2t3x2165888ir3t3x2+192t4x2+4608rt4x2+41472r2t4x2+165888r3t4x2+248832r4t4x2144x4384itx42304irtx4+192t2x4+2304rt2x4+6912r2t2x4+64x6,

q^[2]=9+396t2+11664rt2+92592r2t2+432t4+13440rt4+148608r2t4+705024r3t4+1223424r4t4+64t6+2304rt6+34560r2t6+276480r3t6+1244160r4t6+2985984r5t6+2985984r6t6+108x2288t2x212672rt2x265664r2t2x2+192t4x2+4608rt4x2+41472r2t4x2+165888r3t4x2+248832r4t4x2+48x4+192t2x4+2304rt2x4+6912r2t2x4+64x6.

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Received: 2015-7-9
Accepted: 2015-10-9
Published Online: 2015-11-4
Published in Print: 2016-1-1

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