亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        Spatio-Temporal Deformation of Kink-Breather to the(2+1)-Dimensional Potential Boiti–Leon–Manna–Pempinelli Equation?

        2018-01-24 06:22:55LiLiSong宋莉莉ZhiLinPu蒲志林andZhengDeDai戴正德SchoolofMathematicsandSoftwareScienceSichuanNormalUniversityChengdu610068China
        Communications in Theoretical Physics 2017年5期
        關(guān)鍵詞:莉莉

        Li-Li Song(宋莉莉), Zhi-Lin Pu(蒲志林), and Zheng-De Dai(戴正德)School of Mathematics and Software Science,Sichuan Normal University,Chengdu 610068,China

        2School of Mathematics and Statistics,Yunnan University,Kunming 650091,China

        1 Introduction

        The nonlinear evolution equation is one of the typical models that describes the complexity of nature,and it is better to approach the essence of object things,so the nonlinear evolution equation plays an important role in the nonlinear science field.It has broad prospect and widespread application foregrounds in some realm,such as fluid mechanics,quantum field theory,nonlinear optics,life science,communication and so on.To study nonlinear evolution equation,soliton theory is one of the most important methods.With the development of soliton theory,plenty of methods of solving soliton are put forward,for instance,the Darboux transformation method,[1?3]the Hirota bilinear method,[4?6]the Lie group method,[7?9]the homogeneous balance method,[10?11]the variable separation method,[12]the inverse scattering method,[13?15]symmetry reductions,[16?17]wronskian technique[18]etc.However,solving analytical solution of soliton dynamical systems is very diffcult,especially in the higher dimensional systems.Under these circumstances,what directly analyzing and observing the behavior of solitons is a necessary method to study soliton dynamical problem.Generally,soliton’s velocities,frequency and amplitude will not change after solitons’interaction.But when it meets some conditions,velocities,frequency and amplitude will alter,and one wave can even be drowned by another wave.In the paper,[19]the interaction between kinky solitary wave and rogue wave for(2+1)-dimensional Burgers equation is disscused,and it finds soliton fusion and fission phenomenon.And the other paper,[20]it researches the completely non-elastic interaction between kink wave and rational breather wave for(3+1)-dimensional potensional Yu–Toda–Sasa–Fukuyama equation,and it is found that rational breather wave is drowned or swallowed by kink wave.

        In the paper,we consider the(2+1)-dimensional Boiti–Leon–Manna–Pempinelli(BLMP)equation as follows:

        The equation(1)was most early proposed by Boiti et al.based on the relationship of weak Lax pair,and it can be regarded as asymmetrical form of the following Nizhnik–Novikov–Veselov equation in the space{x,y}.

        Using the potentialq=uygives the(2+1)-dimensional potential Boiti–Leon–Manna–Pempinelli(PBLMP)equation:

        Some results of Eq.(4)have been released,for example,large of exact solutions have been gained by using variable separation method,[21?22]lie group method,[23]modified Clarkson–Krushal direct method[24]and so on.In the literature,[25]the conservation law and the correlation between symmetry and conservation law are given.The periodic-wave solutions for Eq.(4)appear in the literature.[26]However,spatio-temporal deformation of the solitary wave of the(2+1)-dimensional PBLMP equation have not been reported.In this paper,using the painleve analysis and Hirota bilinear method,we will gain the kink solitary wave and rational breather soliton of the(2+1)-dimensional PBLMP equation,and discuss their spatio-temporal deformation.Eventually,we find the fusion and degeneration of the kink solitary wave occur in this process.This is a very meaningful phenomena in researching soliton dynamical complexity in the higher dimensional system.

        Now,we take the following four steps:

        Step 1A transformationu=T(f)is made by Painleve analysis for some new and unknown function.

        Step 2Using the transformationu=T(f)of step 1,the initial equation can be turned into the Hirota bilinear formG(Dt,Dx,Dy,f)=0,whereD-operator is defined by

        Step 3Solving the above equation to obtain kinkbreather by selecting the test function which comprises rational function and exponential function.

        Step 4Under the condition of the non-singularity of kink-breather,we can get spatio-temporal deformation phenomenon at different times.

        2 Kink Solitary Wave Solution

        In the part,we will search for kink solitary wave solution of the(2+1)-dimensional PBLMP equation by means of Painleve analysis and Hirota bilinear method.Meanwhile,we will select suitable test function to help in the quest.

        Using Painleve analysis in Eq.(4),let

        3 Rational Breather Soliton

        wheref(x,y,t)is unknown real function.Substituting Eq.(5)into Eq.(4),by the aid of the Hirota bilinear operatorD,we will get the following bilinear form:

        that is

        With regard to Eq.(6),we choose test function of the following form to seek for the kink solitary wave solution of(2+1)-dimensional PBLMP equation.

        wherea3,b3andc3are real constants to be determined.

        Substituting Eq.(8)into Eq.(6)we get

        Thereby,we obtain the following dispersion relation from Eq.(9),

        Meanwhile,we can also get the following solution of the(2+1)-dimensional PBLMP equation

        wherea3,b3andc3are contents related to the dispersion relation(10).Whent→ +∞,the solutionu→ ?2a3,and whent→ ?∞,the solutionu→ 0.So the solution(11)is the kink solitary wave solution(see Fig.1).

        Fig.1 The kink solitary wave as a3=1/8,b3=0,and c3=1/12.

        In the part,similarly,drawing support from the Hirota bilinear form and selecting the following test function to seek for the rational breather soliton of the(2+1)-dimensional PBLMP equation.

        Plugging(12)into(6)with the help of Maple,and equating all coeffcient of all power ofx,y,t,we get the following algebraic equations.

        Solving algebraic Eqs.(13),we choose the following set of solutions

        So we get the following rational breather soliton of the(2+1)-dimensional PBLMP equation by putting Eq.(14)and Eq.(12)into Eq.(5)

        Observing the following Fig.2,we see that the shape of soliton is one convex wave upward and one concave wave downward,which are located in both sides of horizontal plane,so this soliton is described as the rational breather soliton.Further observation on the solution(15)and Fig.2,we will also find useful properties that it is not exponentially decaying but algebraically decaying.Furthermore,whenx(ory,t)→∞,u(x,y,t)→0.

        Fig.2 The rationalbreathersoliton u(x,t) =?8x/(1+2x2+2t2)as y=t,a1=1,b1=i,c1=?i.

        In addition,in Fig.2,we can also see the similar structure of the rogue wave which is localized in bothx-andt-directions.Thus,it shows that the solution(15)is the 2D rogue wave of(2+1)-dimensional PBLMP equation.

        4 Spatio-Temporal Deformation of Kink-Breather

        In the part,we will discuss spatio-temporal deformation of kink-breather for the(2+1)-dimensional PBLMP equation,and observe the process of solitons’interaction.So we will select the test function of the following form

        wheref(x,y,t)comprises a rational function and an exponential function,andai,bi,ci(i=1,2,3),δwill be determined later.Putting Eq.(16)in Eq.(6)by means of Maple,we obtain the following algebraic equations.

        Solving Eqs.(17)we gain relations as follows

        Plugging Eqs.(18)and(16)into(5),we can achieve new exact solitary wave solution of the(2+1)-dimensional PBLMP equation

        wherea2,a3,b2andδare free.Pay attention to the solution(19),ifa3<0,the solutionu→?2a3ast→+∞,and the solutionu→ 0 ast→ ?∞. Conversely,ifa3>0,the solutionu→ 0 ast→ +∞,and the solutionu→ ?2a3ast→ ?∞.These asymptotic characteristics show that the solution(19)is the kink solitary wave solution.With further analysis of the solution(19),we notice that it is also the rational solution withx,y,so the solution(19)is the rational kink solitary wave solution.Therefore,the solution(19)is exponentially decaying and also algebraically decaying.It is the mixed exponential-algebraic solitary wave solution,[20]which has complex nature structure.Then critical parametersδ,a3will be analyzed about this complexity.In order to ensure the non-singularity of the solution(19),we assumeδ>0.

        Whenδ>0,a3<0,we observe the following Fig.3 which shows the interaction process between the kink solitary wave and the rational breather soliton.It is found that the rational breather soliton will be drowned by the kink solitary wave finally,that is,a soliton fusion take place.

        From Fig.3,we see that the rational breather soliton and the kink solitary wave are to interaction and annihilate step by step.

        Whenδ>0,a3>0,we observe the following Fig.4,which is quite different from Fig.3. It is found that the kink solitary wave will degenerate into the rational breather soliton.

        From Fig.4,we see that there is only the kink solitary wave at first.As time goes by,the rational breather soliton split offfrom the kink solitary wave.But at last,there is nothing except the rational breather soliton because of the kink solitary wave’s energy decay in the process of evolution over time.The kink solitary wave has become vestigial.The total energy is conserved,so the rational breather soliton absorb energy and exist.

        Fig.3 Spatial structure of the solution(19)at different time as a2=1,b2=1/2,a3= ?1/4,δ=16.

        Fig.4 Spatial structure of the solution(19)at different time as a2=1,b2=1/2,a3=1/4,δ=16.

        The above phenomena are necessary to study soliton dynamical complexity in the higher dimensional systems.Then,we put the focus on conditions about fusion and degeneration of soliton.At the same time,fusion and degeneration of soliton also illustrate that the solution(19)is not stable.

        The solution(19)contains rational function and exponential function.Ifδ>0,a3<0,whent→ ?∞,the solution(19)stands for the rational breather soliton and the kink solitary wave.Whilet→+∞,exponential function rises faster than rational function so that the rational breather soliton is annihilated by the kink solitary wave,and the fusion of the solitary wave take place.Ifδ>0,a3>0,whent→ ?∞,the solution(19)represents the kink solitary wave solution.While in the vicinity oft=0,the kink solitary wave starts to become weak,and the rational breather soliton begins to become strong.The kink solitary wave and the rational breather soliton keep pace with each other.Whent→ +∞,exponential function goes to zero,so the kink solitary wave degenerates except for the rational breather soliton.

        In addition,please note that the velocity of the kink solitary wave and the rational breather soliton in the solution(19)areandvr=0 on thex-axis.Thus we get the relation Δ(vr,vk)of betweenvrandvk:

        If Δ(vr,vk)=0,thenvr≡vk.At this time,a3=0,and you will find that there is no interaction of the solitary wave.They will remain the same speed along the way forward,and not affect each other.

        If Δ(vr,vk)>0,thenvr>vk.Whena3<0,the solution(19)will be divided into the kink solitary wave and the rational breather soliton ast→ ?∞,but the solitary wave’s fusion will happen until only the kink solitary wave is left ast→+∞.Whena3>0,the solution(19)represents the kink solitary wave ast→ ?∞,but the kink solitary wave will degenerate into the rational breather soliton ast→ +∞.In the above process,the fusion and degeneration of the kink solitary wave occur.This also shows that the mixed algebraic-exponential solitary wave solution is unstable,and this type of solution contains rich dynamical properties of(2+1)-dimensional PBLMP equation.

        5 Conclusion

        In the paper,the kink solitary wave solution,the rational breather soliton and the kink-breather solitary wave are gained for the(2+1)-dimensional PBLMP equation by applying the Hirota bilinear method and selecting different test functions. Then we study spatio-temporal deformation of the kink solitary wave and the rational breather soliton,and find that the fusion and degeneration of the kink solitary wave occur in the process of evolution over time from theoretical analysis and figure display.It is found that the mixed exponential-algebraic solution is very useful in researching the soliton dynamical complexity in the higher dimensional systems.In the future,we will keep on trying to construct various types of exact solutions to discover more dynamical properties of the(2+1)-dimensional PBLMP equation.

        [1]K.Kimiaki and W.Miki,Prog.Theor.Phys.53(1975)1652.

        [2]C.H.Gu,H.S.Hu,and Z.X.Zhou,Darboux Transformation in Soliton Theory and Its Geometric Applications,Shanghai Science and Technology Press,Shanghai(2005).

        [3]A.K.Pogrebkov,Theor.Math.Phys.181(2014)1585.

        [4]R.Hirota and J.Satsuma,Phys.Lett.A 85(1981)407.

        [5]H.W.Tam,W.X.Ma,X.B.Hu,and D.L.Wang,J.Phys.Soc.Jpn.69(2000)45.

        [6]X.B.Hu,J.Phys.A:Math.Gen.30(1998)8225.

        [7]G.Z.Tu,Sci.China(Serries A)32(1989)142.

        [8]M.Jimbo and T.Miwa,Publications of the Research Institude for Mathematical Sciences Kyato University 19(1983)943.

        [9]Z.H.Zhao and Z.D.Dai,Int.J.Nonl.Sci.Numer.Simulation 11(2010)679.

        [10]X.Zhao,L.Wang,and W.Sun,Chaos,Solitons and Fractals 28(2006)448.

        [11]M.Senthilvelan,Appl.Math.Comp.123(2001)381.

        [12]J.H.He,Phys.Lett.A 335(2005)182.

        [13]A.V.Mikhailov.Phys.D 3(1981)73.

        [14]M.J.Ablowitz and P.A.Clarkson,Solitons,Nonlinear Evolution Equations and Inverse Scattering,Cambridge University Press,Cambridge(1991).

        [15]V.O.Vakhnenko,E.J.Parkes,and A.J.Morrison,Chaos,Solitons and Fractals 17(2003)683.

        [16]B.Ren,J.Yu,and X.Z.Liu,Commun.Theor.Phys.65(2016)341.

        [17]L.Wang,S.F.Tian,Z.T.Zhao,and X.Q.Song,Commun.Theor.Phys.66(2016)35.

        [18]D.S.Wang,X.G.Li,C.K.Chan,and J.Zhou,Commun.Theor.Phys.65(2016)259.

        [19]C.J.Wang,Z.D.Dai,and C.F.Liu,Mediter.J.Math.(2015)1.

        [20]W.Tan and Z.D.Dai,Nonlinear Dyn.85(2016)817.

        [21]X.Y.Tang,Phys.Lett.A 314(2003)286.

        [22]F.Z.Lin and S.H.Ma,Adv.Mater.Res.912–914(2014)1303.

        [23]C.Tian,The Lie Group and Its Applications in Differential Equation,Science Press,Beijing(2001).

        [24]Y.Li and D.Li,Appl.Math.Sci.6(2012)579.

        [25]N.Liu and X.Q.Liu,Chin.J.Quant.Electr.25(2008)546.

        [26]Y.N.Tang and W.J.Zai,Nonlinear Dyn.81(2015)249.

        猜你喜歡
        莉莉
        雪娃娃莉莉
        誰(shuí)在悄悄幫助莉莉呢?
        With you at that moment
        今年 11 歲
        不倒自行車(chē)
        機(jī)器人“小K”
        天上飛車(chē)
        Look from the Anglo—American jury system of jury system in our country
        Differentiation of recurrence rectal cancer and benign pelvic lesions after curative rectal operation with 3.0 T magnatic resonance
        新年的6個(gè)祝愿
        意林(2012年4期)2012-05-30 03:06:54
        av毛片亚洲高清一区二区| 国产亚洲精品bt天堂| 久久青草国产免费观看| 亚洲国产大胸一区二区三区| 亚洲av中文无码乱人伦在线观看| 99国产精品无码| 天天综合天天色| av在线男人的免费天堂| 极品人妻少妇av免费久久 | 久久精品国产色蜜蜜麻豆| 国产91中文| 国产av一区网址大全| 麻豆视频在线播放观看| 国产亚洲日韩在线一区二区三区| 911精品国产91久久久久| 久久久精品亚洲懂色av| 中文字幕精品一区二区三区 | 韩国19禁无遮挡啪啪无码网站| 日本a在线免费观看| 精品蜜桃av免费观看| 99在线精品免费视频| 国产自国产在线观看免费观看 | 水野优香中文字幕av网站| 亚洲一区二区三区中文字幂| 国产xxxxx在线观看免费| 亚洲熟女av一区少妇| 国产无套乱子伦精彩是白视频| 久久久精品人妻一区二区三区四 | 国产欧美亚洲另类第一页| 综合久久精品亚洲天堂| 成人影院yy111111在线| 欧美日韩国产成人高清视| 丰满人妻无奈张开双腿av| 日韩av一区二区网址| 疯狂撞击丝袜人妻| 四虎精品国产一区二区三区 | 亚洲最大中文字幕在线| 久久亚洲色www成人欧美| 国产精品系列亚洲第一| 蕾丝女同一区二区三区| 无遮挡呻吟娇喘视频免费播放|