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 共查询到19条相似文献,搜索用时 372 毫秒
1.
袁德荣  乔灵芝 《物理学报》2001,50(3):394-397
阻尼和外电场的作用使得带有非对称双阱势的氢键链存在扭结孤子激发.计算了孤子的迁移率,它包含了φ4链的结果 关键词: 氢键链 非对称双阱势 扭结孤子 迁移率  相似文献   

2.
考虑非对称势和阻尼下,研究庞小峰教授提出的氢键系统质子传递理论模型,其模型存在扭结孤子激发,给出孤子传递的精确解及质子传递的速度.  相似文献   

3.
考虑非对称势和阻尼下。研究庞小峰教授提出的氢键系统质子传递理论模型。其模型存在扭结孤子激发,给出孤子传递的精确解及质子传递的速度.  相似文献   

4.
运用二分量孤子的振子模型,研究了氢键分子系统中在外场与阻尼存在情况下,质子子晶格与重离子子晶格中扭结孤子形成的孤子对的运动特性,讨论了重离子运动对孤子对迁移率的影响和孤子对的核化特性,得到了孤子对迁移率表达式和平均核化率  相似文献   

5.
石玉仁  张娟  杨红娟  段文山 《物理学报》2010,59(11):7564-7569
基于双曲函数法的思想,通过选择新的展开函数,得到了modified Korteweg-de Vries(mKdV)方程的几类精确解,其中一类为具有扭结—反扭结状结构的双扭结单孤子解.在不同的极限情况下,该解分别退化为mKdV方程的扭结状或钟状孤波解.文中对双扭结型孤子解的稳定性进行了数值研究,结果表明:在长波和短波简谐波扰动、钟型孤立波扰动与随机扰动下,该孤子均稳定.  相似文献   

6.
运用二分量孤子的振子模型,研究了氢键分子系统中在外场与阻尼存在情况下,质子子晶格与重离子子晶格中扭结孤子形成的孤子对的运动特性,讨论了重离子运动对孤子对迁移率的影响和孤子对的核化特性,得到了孤子对迁移率表达式和平均核化率 关键词:  相似文献   

7.
石玉仁  张娟  杨红娟  段文山 《物理学报》2011,60(2):20402-020402
利用扩展的双曲函数法得到了combined KdV-mKdV (cKdV)方程的几类精确解,其中一类为具有扭结—反扭结状结构的双扭结单孤子解.在不同的极限情况下,该解分别退化为cKdV方程的扭结状或钟状孤波解.理论分析表明,cKdV方程既有传播型孤立波解,也有非传播型孤立波解.文中对双扭结型孤立波解的稳定性进行了数值研究,结果表明,cKdV方程既存在稳定的双扭结型孤立波,也存在不稳定的双扭结型孤立波. 关键词: cKdV方程 双扭结单孤子 稳定性  相似文献   

8.
阻尼作用下带对称双阱势的原子链中的洞孤子   总被引:1,自引:1,他引:0  
徐海清  钟红伟  胡柯 《计算物理》2009,26(4):629-632
采用多重尺度法,研究弱阻尼作用下带有对称双阱势的原子链,导出耗散型的非线性薛定谔方程,并对方程进行解析求解,给出阻尼作用下在链中传播的耗散型的洞孤子解.  相似文献   

9.
采用双曲函数展开法得到Modified Benjamin-Bona-Mahony(mBBM)方程的一类扭结-反扭结状的双扭结孤立波解,在不同的极限情况下,此孤立波分别退化为mBBM方程的扭结状和钟状孤立波解.对双扭结型单孤子的结构特征进行分析,构造有限差分格式对其动力学稳定性进行数值研究.有限差分格式为两层隐式格式,在线性化意义下无条件稳定.数值结果表明mBBM方程的双扭结型单孤子在不同类型的扰动下均具有很强的稳定性.对双孤立波的碰撞进行数值模拟,发现既存在弹性碰撞也存在非弹性碰撞.  相似文献   

10.
利用函数展开法求解修正耦合KdV(Coupled KdV,cKdV)方程组,得到几类孤立波解,包括扭结型-钟型、双扭结型、双钟型以及双扭结-双钟型结构的单孤子解.在不同的极限情况下,这些解分别退化为修正cKdV方程的扭结状或钟状孤波解.对孤立波的稳定性进行了数值研究,结果表明:修正cKdV方程既存在稳定的孤立波解,也存在不稳定的孤立波解.  相似文献   

11.
We discuss the nonlinear excitations and the motion of kink in hydrogen-bonded chain with asymmetric double-well potential, in presence of an external force and damping using a new two-component soliton model. We obtain the kink soliton solution using the phase-plane method, we study soliton velocity and find the expression of the mobility of the kink soliton.  相似文献   

12.
In hydrogen-bonded systems with a symmetric double-well potential, using the variational method, we study the nonlinear excitations and motion of the solitons in the presence of the optical mode of the heavy ion sublattice, based on a new two-component soliton model. We give the equations of motion and soliton-solutions in such a case. Based on these results we calculate further the energy, the momentum and the effective mass of the kink pair.  相似文献   

13.
We show how to improve the dilute-gas expansion by including terms that correct double counting erros. The 1D double-well system is studied in detail. The effective correction potential diverges as the kink-antikink distance goes to zero and in this way provides a repulsive core to cut off the kink-gas density. Comparisons with the kink mass give limits to the applicability of the uncorrected kink gas.  相似文献   

14.
We report on the dynamics of semi-localized nonlinear optical modes supported by an interface separating a uniform defocusing saturable medium and an imprinted semi-infinite photonic lattice. Out-of-phase and in-phase kink solitons composed by dark-soliton-like pedestals and oscillatory tails are found. Two branches of out-of-phase kink solitons exist in shallow lattices. Saturable nonlinearity enhances the pedestal height and renormalized energy flow of kink solitons evidently. While in-phase kink solitons are always unstable, out-of-phase kink solitons will be completely stable provided that lattice depth exceeds a critical value. Furthermore, stable kink solitons in the higher band gaps are also possible. Our results may give a helpful hint for understanding the dynamics of kink solitons with high pedestals in other fields.  相似文献   

15.
We show analytically that addition of a quintic term to the positive Kerr-type nonlinearity offers a unique type of kink soliton-like solution with Fermi-Dirac profile. This type of optical kink allows, in contrast to other optical kinks discovered so far, stationary kink formation not only in the time domain but in the spatial domain. The latter could admit of a route for the first time to our knowledge to spatial kink solitons of intensified laser beams. The underlying principle of the optical kink propagation is described.  相似文献   

16.
We report the oscillating propagation of kink in a nondissipative Frenkel-Kontorova (FK) chain driven by external DC force, which is different from the usual propagation of localized modes with equal speed. When the kink moves in the opposite direction of the external DC force, the kink will be accelerated and the potential of the FK chain in the external force field is transformed to be the kinetic energy of the kink. If the kink reaches the boundary of the FK chain, the kink will be bounced back and moves in the opposite direction, then the kink will be decelerated gradually and the kinetic energy of the kink & transformed to be the potential of the FK chain in the external force field. If the speed of the kink reaches zero, the kink will move in the opposite direction again driven by the external DC force, and a new oscillating cycle begins. Simulation result demonstrates exactly the transformation between the kinetic energy of the kink and the potential of the FK chain in the external force field. The interesting energy exchange is induced by the special topology of kinks, and other localized modes, such as breathers and envelope solitons, have no the interesting phenomenon.  相似文献   

17.
We study kink dynamics in a very discrete sine-Gordon system where the kink width is of the order of the lattice spacing. Numerical simulations exhibit new properties of kinks in this case: they lose the memory of their initial velocity and propagate preferentially at well-defined velocities which correspond to quasi-steady states, while a kink moving at other velocities suffers relatively high rates of radiation of small amplitude oscillations. When a small external driving force is applied to the system, the same velocities appear as plateus in the strongly nonlinear mobility of the kink. The energy radiated by the kink is calculated for a simple model that preserves the discrete character of the system, and the preferential velocities for the kink are obtained to good accuracy. Similar results may be expected to be valid for other discrete systems manifesting topological solitons. The numerical simulations reveal also new stable “multiple-kink” excitations which can propagate almost freely in extremely discrete systems where “ordinary” simple kinks are pinned to the lattice by discreteness. The stability of the “multiple-kinks” is discussed.  相似文献   

18.
The prime objective of this paper is to explore the new exact soliton solutions to the higher-dimensional nonlinear Fokas equation and(2+1)-dimensional breaking soliton equations via a generalized exponential rational function(GERF) method. Many different kinds of exact soliton solution are obtained, all of which are completely novel and have never been reported in the literature before. The dynamical behaviors of some obtained exact soliton solutions are also demonstrated by a choice of appropriate values of the free constants that aid in understanding the nonlinear complex phenomena of such equations. These exact soliton solutions are observed in the shapes of different dynamical structures of localized solitary wave solutions, singular-form solitons, single solitons,double solitons, triple solitons, bell-shaped solitons, combo singular solitons, breather-type solitons,elastic interactions between triple solitons and kink waves, and elastic interactions between diverse solitons and kink waves. Because of the reduction in symbolic computation work and the additional constructed closed-form solutions, it is observed that the suggested technique is effective, robust, and straightforward. Moreover, several other types of higher-dimensional nonlinear evolution equation can be solved using the powerful GERF technique.  相似文献   

19.
一维分子链中激子与声子的相互作用和呼吸子解   总被引:1,自引:0,他引:1       下载免费PDF全文
徐权  田强 《物理学报》2004,53(9):2811-2815
运用连续极限近似,求解声子与激子相互作用的运动方程,得到了简谐分子链和 非简谐分子链中晶格振动的孤子解,在考虑三次非简谐势的情况下,一维分子链晶格振动具 有扭结孤子解,在考虑具有四次非简谐势的情况下,得到一维分子链晶格振动具有呼吸子解 . 关键词: 一维分子链 激子 声子 孤子 呼吸子 非线性效应  相似文献   

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