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41.
首先讨论了约束离散KP可积方程族一种等价形式:差分算子的商.接下来,利用这种新的描述形式,构造了约束离散KP方程族的完全Virasoro对称. 相似文献
42.
In this paper, the squared eigenfunction symmetries for the BTL and CTL hierarchies are explicitly constructed with the suitable modification of the ones for the TL hierarchy, by considering the BTL and CTL constraints. Also the connections with the corresponding additional symmetries are investigated: the squared eigenfunction symmetry generated by the wave function can be viewed as the generating function for the additional symmetries. 相似文献
43.
We discuss a modified Wadati-Konno-Ichikawa(m WKI) equation,which is equivalent to the WKI equation by a hodograph transformation.The explicit formula of degenerated solution of m WKI equation is provided by using degenerate Darboux transformation with respect to the eigenvalues,which yields two kinds of smooth solutions possessing the vanishing and nonvanishing boundary conditions respectively.In particular,a method for the decomposition of modulus square is operated to the positon solution,and the approximate orbits before and after collision of positon solutions are displayed explicitly. 相似文献
44.
The N-fold Darboux transformation(DT) T_n~([N]) of the nonlinear self-dual network equation is given in terms of the determinant representation. The elements in determinants are composed of the eigenvalues λ_j(j = 1, 2..., N)and the corresponding eigenfunctions of the associated Lax equation. Using this representation, the N-soliton solutions of the nonlinear self-dual network equation are given from the zero "seed" solution by the N-fold DT. A general form of the N-degenerate soliton is constructed from the determinants of N-soliton by a special limit λ_j →λ_1 and by using the higher-order Taylor expansion. For 2-degenerate and 3-degenerate solitons, approximate orbits are given analytically,which provide excellent fit of exact trajectories. These orbits have a time-dependent "phase shift", namely ln(t~2). 相似文献
45.
本文首先根据Mizrahi构造不变量的方法建立了在一维变化磁场中自旋j系统的不变量,然后利用自旋1/2和自旋1系统不变量的简明矩阵形式直接求解不变量的本征波函数,由此给出了该系统含时Schrodinger方程的精确解,进而根据Lewis相讨论了此系统的Aharonov-Anandan相。 相似文献
46.
本文给出了双参数形变量子代数SUqs(2)和SUqs(1,1)的Holstein-Primakoff实现的明显形式。此外,通过引入广义qs-玻色算符,得到了Holstein-Primakoff实现的多qs-玻色子形式。 相似文献
47.
本文明显构造了双参数形变谐振子湮灭算符二次幂的本征态,并利用qs-积分给出了其完备性的证明。 相似文献
48.
本文引入了qs-费米振子的概念,然后构造了qs-超对称振子,并给出其相应的qs-超代数的实现.此外,我们给出了双参数形变量子代数SU_(qs)(2)的qs-费米振子实现. 相似文献
49.
明显构造了双参数qs-形变谐振子湮灭算符高次幂的本征态,并利用qs-积分给出了其完备性证明。 相似文献
50.
利用Kadomtsev-Petviashvili(KP)系列约束方法和双线性方法,构造了空间位移宇称-时间反演(PT)对称非局域非线性薛定谔方程的高阶怪波解.任意N阶怪波解的解析表达式是通过舒尔多项式表示的.首先通过分析一阶怪波解的动力学行为,发现怪波的最大振幅可以大于背景平面三倍的任意高度.分析了对称非局域非线性薛定谔方程中的空间位移因子x0在一阶怪波解中的影响,结果表明其仅改变怪波中心的位置.另外,研究了二阶怪波解的动力学行为以及怪波模式,然后给出了N阶怪波模式与N阶怪波解的解析表达式中参数之间的关系,进一步展示了高阶怪波的不同模式. 相似文献