New Traveling Wave Solutions for the (2 + 1)-Dimensional Heisenberg Ferromagnetic Spin Chain Equation

The principal objective of this article is to construct new exact soliton solutions of the (2+1)-dimensional Heisenberg ferromagnetic spin chain equation which investigates the nonlinear dynamics of magnets. Through using the complete discrimination system method, the traveling wave solutions are obtained. As a result, we get the traveling wave solutions of the Heisenberg ferromagnetic spin chain equation, which include rational function solutions, Jacobian elliptic function solutions, hyperbolic function solutions, trigonometric function solutions, inverse trigonometric function, logarithmic function. Some graphical representations of the problems and that of comparison are also provided.


Introduction
In this paper, we are devoted to studying the traveling wave solutions for (2 + 1)-dimensional nonlinear equation describing nonlinear wave propagation in Heisenberg ferromagnetic spin chain equation(HFSC) which was derived by Latha and Christal Vasanthi [1], where α 1 c 4 (J + J 2 ), α 3 2c 4 J 2 , and α 4 2c 4 Ω. In (1), u(x, y, t) is the complex function of the normalized spatial variables x and y and temporal variable t and represents the appropriate continuum approximation of the coherent magnetism amplitude to the bosonic operators at spin-lattice sites; c is lattice parameter; J and J 1 correspond to the coe cients of bilinear exchange interactions along the x and y directions, respectively; J 2 refer to the neighboring interaction along the diagonal; and Ω is the uniaxial crystal eld anisotropy parameter.
Traveling wave solution is an important research content of nonlinear partial di erential equations. It is di cult to nd the traveling wave solution of nonlinear partial di erential equations (PDE), but in recent years, many methods of spherical traveling wave solution have been studied. A large number of reports show that researchers have obtained traveling wave solutions of partial di erential equations involving many elds, such as nuclear physics, chemical reaction, signal processing, optical ber, hydrodynamics, plasma, nonlinear optics, and ecology. Traveling wave solutions play an important role in revealing the properties of these nonlinear partial di erential equations and predicting the trend of these phenomena [2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21].
Heisenberg ferromagnetic spin chain equation is used to describe the nonlinear wave propagation in a ferromagnetic spin chain system. It is also a generalization of (2 + 1)-dimensional nonlinear Schrödinger equation. With the development of technology, the transistor size is reduced to the nanometer scale. How to develop electronic components with higher density and faster storage speed is the practical reason why the HFSC equation is valued [22][23][24][25].
Since the traveling wave solution is helpful to explain many physical properties of magnetic materials, many scholars are attracted to the study of the traveling wave solution of the HSFC equation. In reference [1], equation (1) was derived by using the coherent state ansatz connected to a Holstein-Primakoff bosonic representation of spin operators. en, the multisoliton solution is constructed by the Darboux transform, and the modulation instability is discussed. ree kinds of traveling wave solutions of equation (1) are obtained by using traveling wave transformation [26]. e bilinear form and dark soliton solution of equation (1) are derived by the auxiliary function method, and the soliton interaction is studied.
ere are two types of elastic and inelastic collisions between these solitons [27]. In references [28,29], dark multiple solitons are derived, and then, the propagation, interaction, and linear stability analysis of solitons are discussed, respectively. Some complex solutions were obtained by the auxiliary ordinary differential equation method in [30]. In [31], a series of new solutions are constructed by the improved F-expansion method combined with the Jacobian ellipse method.
ey are exported to understand the constraints that exist. ese solutions include periodic wave solutions, double periodic wave solutions, dark soliton solutions, and bright soliton solutions. Lax pair and generalized Darboux transform are used in equation (1) to construct a class of n-order strange waves [32]. In reference [33], the bifurcation of the solution of equation (1) and some traveling wave solutions are obtained by using the dynamic system method. In [34], the authors find the soliton solutions for equation (1) by considering the Bäcklund transformation. By using the Hirota bilinear method, the one-order rogue waves solutions are obtained in [35], and the interaction behaviors between breather and rogue wave are studied in [36]. By applying the bilinear method, the lump wave solution is constructed in [37]. Recently, Li studied a (2 + 1)-dimensional nonlinear ferromagnetic spin chain system with variable coefficients in [38] and obtained the breather and rogue wave by using the algebraic iteration method. e scholars mentioned above have obtained different traveling wave solutions by different transformations, so they have obtained the properties of HFSC from different directions. Although many traveling wave solutions of the HFSC equation have been obtained in the above literature, there are few studies on the classification of all possible traveling wave solutions. Driven by the above reasons, we will use the complete discrimination system method to find more traveling wave solutions of HFSC to enrich the research results of HFSC. e rest of this continuing article is methodized as follows: in Section 2, we propound the formation of the polynomial complete discrimination system. In Section 3, we implement this technique to find traveling wave solutions to the HFSC equation. In Section 4, with the help of Maple, the graphical illustration of the modulus of the traveling wave solutions is described by using 2-dimensional and 3-dimensional plots. Finally, some conclusions are given in Section 5.

Overview of the Complete Discrimination System
To show the basic idea of our method, consider the following nonlinear differential equation: where u is an unknown function and P is a polynomial of u and its partial fractional derivatives. Using the traveling wave transformation, where c is a nonzero velocity of the traveling wave in (3). We get an ordinary differential equation of the polynomial form where Q is a polynomial in u and its derivatives and notation ( ′ ) is the derivative with respect to ξ. Equation (4) can be written as where θ 1 , θ 2 , . . . , θ m are parameters. en, integrating the above formula once, we have where G(u) is a polynomial function. According to the complete discrimination system for G(u), the roots of G(u) can be classified, and the detailed classification will be given in Section 3.

Traveling Wave Solution of the (2 + 1)-Dimensional HFSC
To find the traveling wave solutions of equation (1), we assume that where where ξ is the traveling coordinate, φ(ξ) is the real amplitude function to be determined, and ρ(x, y, t) is the phase of the envelope. e parameters η 1 and η 2 represent the wavenumbers in the x and y directions, respectively, c is the wave velocity, and μ is the frequency of the pulse.
Utilizing the wave transformation (8) into equation (1), separating the real part and the imaginary part, respectively, we obtain that and Letting It follows We can see that systems (12) and (13) will be compatible in the case C � 0. We always assume that B ≠ 0, otherwise equation (13) is not a differential equation. Multiply both sides of equation (13) by φ ′ (ξ) and integrate once, we get where C 0 is the integration constant. Let a 4 � α 4 /2B, a 2 � − A/B, a 0 � C 0 . Equation (14) can be written as Taking Equation (15) can be written as follows: Equation (17) becomes the following integration form: where F(w) � w 2 + b 1 w + b 0 , and noting Δ � b 2 1 − 4b 0 .
Case 1. Δ � 0. Since w > 0, we obtain that If b 1 < 0, the solution of equation (19) is e traveling wave solutions of equation (17) are If b 1 > 0, the traveling wave solution of (17) is If b 1 � 0, the traveling wave solution of equation (17) is at is to say, when Δ � 0, we get the following solutions of equation (17): (23) is the rational function solution of the equation. (19) can be written as

solution (21) is the solitary wave solution, solution (22) is the hyperbolic function solution, solution (23) is the trigonometric function solution, and solution
If b 1 > 0, then, equation (25) is e solutions of equation (17) are If b 1 < 0, then, the solution of equation (25) is So, the solution of (17) is Case 3. Δ > 0, b 0 ≠ 0. Suppose α 1 < α 2 < α 3 , and one of them is zero, and the other two are the roots of F(w).
With the help of (7) and (16), we get the classification of all single traveling wave solutions of (1) as follows: Mathematical Problems in Engineering

Numerical Simulation
is section contains the 2-dimensional and 3-dimensional solution graph of some of the obtained traveling wave solutions of the HFSC equation. Here, the numerical simulation has been performed in Figures 1-5 for showing the nature of the obtained solution.

Concluding Remarks
In this paper, the (2 + 1)-dimensional Heisenberg ferromagnetic spin chain equation has been investigated via the complete discriminant system method. A range of new traveling wave solutions is obtained, such as periodic solutions, rational wave solutions, Jacobi elliptic solutions, triangular functions solutions, and hyperbolic function solutions. By selecting appropriate parameters, some representative solutions are drawn. ese solutions may help us to explore new phenomena which appear in equation (1). is paper gives a new idea to study the dispersive traveling wave solutions of the Heisenberg ferromagnetic spin chain equation. In addition, these results are also helpful to understand the dynamics of nonlinear waves in optics, hydrodynamics and magnetic materials. is method can solve the single wave solutions of more types of PDE, such as fractional or random terms.

Data Availability
No data are required for this article.

Conflicts of Interest
e authors declare that they have no conflicts of interest.