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Determinantal solutions to the (3+1)-dimensional Painlevé-type evolution equation: Higher-order rogue and soliton waves (3+1)维painlev<s:2>型演化方程的行列式解:高阶流浪波和孤子波
IF 2.5 3区 物理与天体物理 Q2 ACOUSTICS Pub Date : 2025-08-22 DOI: 10.1016/j.wavemoti.2025.103624
Majid Madadi , Mustafa Inc
We derive and characterize general rogue wave solutions (RWSs) of the (3+1)-dimensional Painlevé-type (P-type) integrable nonlinear evolution equation using the Hirota bilinear method in conjunction with the Kadomtsev–Petviashvili hierarchy reduction method (KPHRM). These solutions arise from intricate nonlinear interactions and exhibit diverse dynamical patterns, such as bright and dark triangular, pentagonal, and other structures, governed by key free parameters and the signs of system coefficients. Additionally, we address new nonlinear soliton solutions using the KPHRM in a determinantal framework. To further generalize the model, we incorporate spatiotemporal coefficients, which introduce additional nonlinear modulation. Using the Wronskian approach, another determinant-based technique, we construct N-soliton solutions for the variable-coefficient equation and analyze their nonlinear dynamics, demonstrating how parameter variation influences wave evolution and interactions.
本文利用Hirota双线性方法结合Kadomtsev-Petviashvili层次约简法(KPHRM),导出了(3+1)维painlev 型(p型)可积非线性演化方程的一般异常波解(RWSs),并对其进行了表征。这些解决方案产生于复杂的非线性相互作用,并表现出不同的动力模式,如明亮和黑暗三角形,五边形和其他结构,由关键自由参数和系统系数符号控制。此外,我们在确定性框架中使用KPHRM解决了新的非线性孤子解。为了进一步推广模型,我们引入了时空系数,这引入了额外的非线性调制。利用另一种基于行列式的方法——朗斯基方法,我们构建了变系数方程的n孤子解,并分析了它们的非线性动力学,展示了参数变化如何影响波的演化和相互作用。
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引用次数: 0
Investigation of shear wave propagation in two-dimensional systems with Lorentzian-correlated disorder 二维洛伦兹相关无序系统中横波传播的研究
IF 2.5 3区 物理与天体物理 Q2 ACOUSTICS Pub Date : 2025-08-21 DOI: 10.1016/j.wavemoti.2025.103620
M.O. Sales , L.D. da Silva , M.S.S. Junior , F.A.B.F. de Moura
In this study, we investigate the propagation of shear vibrations in a rectangular system where disorder is introduced through the compressibility term, exhibiting Lorentzian spatial correlations. Our primary objective is to understand how these correlations influence the behavior and velocity of harmonic mode packets as they travel through the system. To achieve this, we employ a finite difference formalism to accurately capture the wave dynamics. Furthermore, we analyze how the spectral composition of the incident pulse affects wave propagation, shedding light on the interplay between disorder correlations and wave transport. By systematically exploring these factors, we aim to deepen our understanding of the fundamental mechanisms governing shear vibration propagation in disordered media.
在这项研究中,我们研究了剪切振动在矩形系统中的传播,其中通过压缩率项引入无序,表现出洛伦兹空间相关性。我们的主要目标是了解这些相关性如何影响谐波模包在系统中传播时的行为和速度。为了实现这一点,我们采用有限差分形式来准确地捕捉波动动力学。此外,我们分析了入射脉冲的光谱组成如何影响波的传播,揭示了无序相关和波输运之间的相互作用。通过系统地探索这些因素,我们的目标是加深我们对无序介质中剪切振动传播的基本机制的理解。
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引用次数: 0
Non-autonomous positon and breather molecule for the variable-coefficient Kundu-nonlinear Schrödinger equation 变系数kundu -非线性Schrödinger方程的非自治位置和呼吸分子
IF 2.5 3区 物理与天体物理 Q2 ACOUSTICS Pub Date : 2025-08-19 DOI: 10.1016/j.wavemoti.2025.103623
Yanan Wang , Minghe Zhang
We construct novel non-autonomous positons, breather-positons, and breather molecules for the variable-coefficient Kundu-nonlinear Schrödinger equation —a key model for pulse propagation in optical fibers. Through degenerate Darboux transformation, we reveal intricate dynamics previously unattainable. For non-autonomous positon solution, generalized asymptotic analysis method yields exact expressions of asymptotic solitons with logarithmic trajectories. Arising from the different non-autonomous breather-positon, we give the non-autonomous rogue wave generation process and other results. For the non-autonomous breather molecule, the related dynamic behaviors under the periodic, exponential and hyperbolic function parameters are explored by the characteristic line analysis. This work provides a unified framework for investigating degenerate complex waves in inhomogeneous optical media.
我们为变系数kundu非线性Schrödinger方程(光纤中脉冲传播的关键模型)构建了新的非自治位、呼吸位和呼吸分子。通过简并达布变换,我们揭示了以前无法实现的复杂动力学。对于非自治位置解,广义渐近分析方法给出了具有对数轨迹的渐近孤子的精确表达式。在不同的非自主呼吸位置下,给出了非自主异常波的产生过程和其他结果。对于非自主呼吸分子,通过特征线分析,探讨了周期函数、指数函数和双曲函数参数下的相关动力学行为。这项工作为研究非均匀光学介质中的简并复波提供了一个统一的框架。
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引用次数: 0
Guided modes of helical waveguides 螺旋波导的导模
IF 2.5 3区 物理与天体物理 Q2 ACOUSTICS Pub Date : 2025-08-19 DOI: 10.1016/j.wavemoti.2025.103621
Jay Gopalakrishnan, Michael Neunteufel
This paper studies guided transverse scalar modes propagating through helically coiled waveguides. Modeling the modes as solutions of the Helmholtz equation within the three-dimensional (3D) waveguide geometry, a propagation ansatz transforms the mode-finding problem into a 3D quadratic eigenproblem. Through an untwisting map, the problem is shown to be equivalent to a 3D quadratic eigenproblem on a straightened configuration. Next, exploiting the constant torsion and curvature of the Frenet frame of a circular helix, the 3D eigenproblem is further reduced to a two-dimensional (2D) eigenproblem on the waveguide cross section. All three eigenproblems are numerically treated. As expected, significant computational savings are realized in the 2D model. A few nontrivial numerical techniques are needed to make the computation of modes within the 3D geometry feasible. They are presented along with a procedure to effectively filter out unwanted non-propagating eigenfunctions. Computational results show that the geometric effect of coiling is to shift the localization of guided modes away from the coiling center. The variations in modes as coiling pitch is changed are reported considering the example of a coiled optical fiber.
本文研究了在螺旋螺旋波导中传播的波导横向标量模。将模式建模为三维波导几何结构中的亥姆霍兹方程的解,将寻模问题转换为三维二次特征问题。通过解扭曲映射,表明该问题等价于一个三维二次特征问题。接下来,利用螺旋结构的恒定扭转和曲率,将三维特征问题进一步简化为波导截面上的二维特征问题。所有三个特征问题都进行了数值处理。正如预期的那样,在2D模型中实现了显著的计算节省。为了使三维几何中的模态计算可行,需要一些重要的数值技术。它们与有效滤除不需要的非传播特征函数的过程一起提出。计算结果表明,卷取的几何效应是使导模的定位偏离卷取中心。本文以卷绕式光纤为例,报道了卷绕式光纤模式随螺距变化的变化规律。
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引用次数: 0
Cauchy–Poisson problem in a homogeneous liquid layer over a magnetoelastic half-space 磁弹性半空间上均匀液体层的Cauchy-Poisson问题
IF 2.5 3区 物理与天体物理 Q2 ACOUSTICS Pub Date : 2025-08-18 DOI: 10.1016/j.wavemoti.2025.103625
Selina Hossain , Koushik Nandi , Soumen De
The present work investigates the generation and propagation of wave motion produced by initial disturbances in a finite-depth ocean with an elastic bottom, influenced by a constant magnetic field acting in the normal direction of wave propagation. The objective is to derive an analytical solution to the Cauchy–Poisson problem for an ocean over an elastic bottom, modeled as an elastic solid medium, in presence of a uniform magnetic field. The fluid is assumed to be incompressible and is bounded above by a free surface and below by a homogeneous magnetoelastic half-space. By applying linear theory of water waves and linear elasticity theory for solids, the physical problem is formulated as an initial boundary value problem. The Laplace–Fourier integral transform method is employed to obtain analytical expressions for the free surface elevation and the vertical displacement of the seabed in the form of multiple infinite integrals. The method of steepest descent approximation is then applied to evaluate these integrals asymptotically. The results, illustrated through figures, highlight the effects of various key physical parameters on wave behavior. The dispersion relation governing the wave motion is also derived and analyzed. The findings reveal that the magnetic field significantly alters wave characteristics and mitigates wave impact. Additionally, variations in pressure and shear wave velocities are found to have a notable influence on wave propagation. Validation is carried out by comparing the results with existing literature for the special case of a rigid seabed.
本文研究了在具有弹性底的有限深度海洋中,在恒定磁场作用于波传播法向的影响下,由初始扰动产生的波浪运动的产生和传播。目标是推导出弹性海底海洋的柯西-泊松问题的解析解,模拟为均匀磁场存在下的弹性固体介质。假定流体是不可压缩的,上面有一个自由表面,下面有一个均匀的磁弹性半空间。应用水波线性理论和固体线性弹性理论,将该物理问题表述为初始边值问题。采用拉普拉斯-傅立叶积分变换方法,以多次无穷积分的形式得到海床自由表面高程和垂直位移的解析表达式。然后应用最陡下降逼近法对这些积分进行渐近求值。结果通过图表说明,突出了各种关键物理参数对波浪行为的影响。推导并分析了控制波动的色散关系。研究结果表明,磁场显著改变了波的特性,减轻了波的冲击。此外,发现压力和横波速度的变化对波的传播有显著的影响。在刚性海床的特殊情况下,通过与现有文献的比较进行了验证。
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引用次数: 0
Ultrasonic field estimation for random P -and S-wavenumbers in isotropic solids using DPSM 用DPSM估计各向同性固体中随机P波数和s波数的超声场
IF 2.5 3区 物理与天体物理 Q2 ACOUSTICS Pub Date : 2025-08-16 DOI: 10.1016/j.wavemoti.2025.103628
Ayush Thakur , Nur M.M. Kalimullah , Amit Shelke , Budhaditya Hazra , Tribikram Kundu
The measurement of elastic constants often shows randomness, which consequently affects the propagation of P- and S-waves in a solid material. In the theory of wave propagation, longitudinal and transverse waves are characterised using P-and-S wavenumbers (kp and ks), which can be modelled as a random variable to simulate random ultrasonic fields. In this research work, an efficient and accurate solution technique to model random wave propagation due to random wavenumbers using Distributed point source method (DPSM) is developed. DPSM is a semi-analytical method that requires Green’s function (GF) solution for producing ultrasonic fields in homogeneous or heterogeneous solids and near the fluid-solid interface. The generation of ultrasonic fields at higher frequencies and in complex structures requires a large number of distributed point sources, thereby leading to the computation of a greater number of GFs. Therefore, the numerical calculation of random wavefields increases the computational complexity. An analytical model to approximate first-order and second-order moments of the displacement GF solutions for isotropic solid corresponding to randomly distributed P- and S-wavenumbers is proposed. The statistical moments (mean and variance) of ultrasonic fields (stresses and displacement fields) near the fluid-solid interface and in the solid half-space are calculated using the proposed theoretical model. The efficacy and accuracy of the proposed model for normally distributed wavenumbers are illustrated through two numerical analyses. Initially, the mean ultrasonic fields such as displacement and stress fields are evaluated using both the proposed analytical model and Monte Carlo (MC) simulation for 1 MHz excitation frequency. Mean and standard deviations of the total scattered wavefields are computed near the interface and along the solid medium. Further, to check the robustness of the proposed analytical model ultrasonic fields for 2.25 MHz excitation frequency are computed for the same problem configuration and the mean fields are compared with the MC simulation. The computed mean displacement GF solutions and ultrasonic fields using the proposed model for normally distributed wavenumbers match precisely with the MC simulation. Further, the standard deviation of the ultrasonic fields for normally distributed wavenumbers is estimated for different transducer frequencies.
弹性常数的测量往往表现出随机性,从而影响了纵波和横波在固体材料中的传播。在波传播理论中,纵波和横波用p波数和s波数(kp和ks)来表征,p波数和s波数可以建模为随机变量来模拟随机超声场。在本研究中,提出了一种利用分布式点源法(DPSM)求解随机波数引起的随机波传播的高效、准确的方法。DPSM是一种半解析方法,需要格林函数(GF)解来产生均匀或非均匀固体和流固界面附近的超声场。在高频率和复杂结构中产生超声场需要大量的分布点源,从而导致计算更多的GFs。因此,随机波场的数值计算增加了计算复杂度。提出了各向同性固体随机分布P波数和s波数对应的位移GF解的一阶和二阶矩近似解析模型。利用所提出的理论模型计算了流固界面附近和固体半空间内超声场(应力场和位移场)的统计矩(均值和方差)。通过两个数值分析说明了该模型对正态分布波数的有效性和准确性。首先,利用所提出的解析模型和蒙特卡罗(MC)仿真计算了1 MHz激励频率下的平均超声场,如位移场和应力场。计算了界面附近和沿固体介质的总散射波场的均值和标准差。进一步,为了验证所提解析模型的鲁棒性,对相同问题配置计算了2.25 MHz激励频率下的超声场,并将平均场与MC仿真进行了比较。采用正态分布波数模型计算的平均位移GF解和超声场与MC模拟结果吻合较好。此外,估计了不同换能器频率下正态分布波数的超声场的标准偏差。
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引用次数: 0
Eulerian contributions to the particle velocity in Stokes and Gerstner waves 欧拉对斯托克斯波和格斯纳波中粒子速度的贡献
IF 2.5 3区 物理与天体物理 Q2 ACOUSTICS Pub Date : 2025-08-15 DOI: 10.1016/j.wavemoti.2025.103627
Jan Erik H. Weber
For inviscid periodic wave motion, we derive a novel expression in Lagrangian variables for the Stokes drift, which is valid for rotational as well as irrotational waves. The derivation confirms that the Lagrangian mean velocity can be expressed as the sum of the Eulerian mean velocity and the Stokes drift. However, from the Stokes drift part of this expression, we find that the rotational Gerstner wave has a non-zero Stokes drift. Since the Lagrangian mean velocity is zero for this particular wave, we obviously must have a non-zero Eulerian mean velocity in this case, cancelling the Stokes drift. To discuss this problem in detail, we return to the basic kinematics of periodic wave motion in fluids. We avoid time averaging and consider the classic problem of how the Lagrangian particle velocity develops in time, resulting in a Eulerian velocity (expressed in Lagrangian variables) plus the Stokes velocity. We discuss the implication for irrotational deep-water Stokes waves and rotational Gerstner waves. It is demonstrated that the Eulerian velocity, expressed in Lagrangian variables, is different for the two wave types. This explains why the Lagrangian mean velocity in the Stokes wave is equal to the Stokes drift, while it is zero for the Gerstner wave.
对于无粘周期波动,我们导出了一个新的斯托克斯漂移的拉格朗日变量表达式,该表达式适用于旋转波和无旋转波。推导证实了拉格朗日平均速度可以表示为欧拉平均速度和斯托克斯漂移之和。然而,从表达式的Stokes漂移部分,我们发现旋转Gerstner波具有非零Stokes漂移。由于这个波的拉格朗日平均速度为零,在这种情况下,我们显然必须有一个非零的欧拉平均速度,来抵消斯托克斯漂移。为了详细讨论这个问题,我们回到流体周期波动的基本运动学。我们避免时间平均,并考虑经典的拉格朗日粒子速度如何随时间发展的问题,导致欧拉速度(以拉格朗日变量表示)加上斯托克斯速度。讨论了非旋转深水Stokes波和旋转Gerstner波的含义。证明了用拉格朗日变量表示的欧拉速度对于两种波类型是不同的。这就解释了为什么斯托克斯波的拉格朗日平均速度等于斯托克斯漂移,而格斯纳波的拉格朗日平均速度为零。
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引用次数: 0
Hybrid finite difference WENO schemes for the ten-moment Gaussian closure equations with source term 带源项的十矩高斯闭包方程的混合有限差分WENO格式
IF 2.5 3区 物理与天体物理 Q2 ACOUSTICS Pub Date : 2025-08-13 DOI: 10.1016/j.wavemoti.2025.103614
K.R. Arun , Rakesh Kumar , Asha Kumari Meena
A hybrid weighted essentially non-oscillatory (WENO) finite difference scheme is proposed for computing discontinuous solutions of the ten-moment Gaussian closure equations. A salient feature of the proposed scheme is the use of low-cost component-wise reconstruction of the numerical fluxes in smooth regions and non-oscillatory characteristic-wise reconstruction in the vicinity of discontinuities. A troubled-cell indicator which measures the smoothness of the solution, and built on utilising the smoothness indicators of the underlying WENO scheme, is employed to effectively switch between the two reconstructions. The resulting hybrid WENO scheme is simple and efficient, is independent of the order and type of the WENO reconstruction, and it can be used as an effective platform to construct finite difference schemes of any arbitrary high-order accuracy. For demonstration, we have considered the fifth order WENO-Z reconstruction. We have performed several 1D and 2D numerical experiments to illustrate the efficiency of the proposed hybrid algorithm and its performance compared to the standard WENO-Z scheme. Numerical case studies shows that the present algorithm achieves fifth order accuracy for smooth problems, resolves discontinuities in a non-oscillatory manner and takes 25%–50% less computational time than the WENO-Z scheme while retaining many of its advantages.
提出了一种计算十矩高斯闭包方程不连续解的混合加权基本非振荡有限差分格式。该方案的一个显著特点是在光滑区域使用低成本的分量重建数值通量,在不连续区域附近使用非振荡特征重建。一个故障单元指示器用来测量解决方案的平滑性,并建立在利用底层WENO方案的平滑性指标的基础上,用于有效地在两个重建之间切换。所得到的混合WENO格式简单高效,与WENO重构的阶数和类型无关,可作为构建任意高阶精度有限差分格式的有效平台。为了证明这一点,我们考虑了五阶WENO-Z重建。我们进行了几个一维和二维数值实验,以说明所提出的混合算法的效率及其与标准WENO-Z方案的性能比较。数值算例研究表明,该算法对光滑问题达到五阶精度,以非振荡方式解决不连续问题,计算时间比WENO-Z格式减少25%-50%,同时保留了WENO-Z格式的许多优点。
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引用次数: 0
The soliton solutions for an integrable nonlocal reverse space–time fifth-order nonlinear Schrödinger equation by the inverse scattering transform 用逆散射变换求可积非局部逆时空五阶非线性Schrödinger方程的孤子解
IF 2.5 3区 物理与天体物理 Q2 ACOUSTICS Pub Date : 2025-08-12 DOI: 10.1016/j.wavemoti.2025.103619
Huanhuan Lu
This paper begins by deducing a reverse space–time nonlocal fifth-order nonlinear Schrödinger (NLS) equation, which arises from a simple yet significant symmetry reduction of the corresponding local system. Following this, the determinant form of N soliton solutions is thoroughly constructed based on established Gelfand–Levitan–Marchenko(GLM) equation. As a typical application, some exact solutions are derived, including one-soliton, two-soliton, and three-soliton solutions. The dynamical properties of these solutions are further explored and visualized through graphical analysis. Moreover, the integrability of the equation is established by presenting an infinite set of conserved densities. It is particularly noteworthy that we also present the expression for the three-soliton solution, which represents an unprecedented achievement in this field.
本文首先推导了一个逆时空非局部五阶非线性Schrödinger (NLS)方程,该方程由相应的局部系统的一个简单而重要的对称约简而产生。在此基础上,基于已建立的Gelfand-Levitan-Marchenko (GLM)方程,构造了N孤子解的行列式。作为典型应用,导出了一些精确解,包括单孤子解、双孤子解和三孤子解。通过图形分析,进一步探讨了这些解的动力学性质,并将其可视化。此外,通过提出一个无限的守恒密度集,建立了方程的可积性。特别值得注意的是,我们还提出了三孤子解的表达式,这是该领域前所未有的成就。
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引用次数: 0
Detecting high-order rogue waves in two-component Bose–Einstein condensates via a convolutional neural network-based framework 基于卷积神经网络的框架检测双组分玻色-爱因斯坦凝聚体中的高阶异常波
IF 2.5 3区 物理与天体物理 Q2 ACOUSTICS Pub Date : 2025-08-11 DOI: 10.1016/j.wavemoti.2025.103618
Zhihao Zhang , Shunhong Lin , Tiantian Li , Xiao-Dong Bai , Jie Peng
Deep learning has successfully enabled the identification of first-order rogue waves in single-component Bose–Einstein condensates. However, the prediction of rogue waves and identification of high-order rogue waves in two-component coupled Bose–Einstein condensates remain unresolved challenges. In this paper, we extend the application of deep convolutional neural network to the detection of high-order rogue waves in two-component coupled Bose–Einstein condensates by interpreting the spatiotemporal evolution of wave functions as image data. The method successfully learns the complex dynamic behaviors of rogue waves in two-component coupled Bose–Einstein condensates governed by multiple parameters. Moreover, we efficiently locate a narrow, irregular region within the three-dimensional parameter space where second-order-like rogue waves arise. Compared with the tedious iterative processes of numerical methods, this approach significantly reduces computational time—a critical advantage given that time grows exponentially with the number of control parameters. This work provides a scalable tool for exploring complex behaviors in high-dimensional parameter spaces, with potential applications in nonlinear optics, plasma physics, and ocean engineering, where the rapid prediction of extreme waves is critical.
深度学习已经成功地识别了单组分玻色-爱因斯坦凝聚体中的一阶异常波。然而,在双组分耦合玻色-爱因斯坦凝聚体中异常波的预测和高阶异常波的识别仍然是未解决的挑战。本文通过将波函数的时空演化解释为图像数据,将深度卷积神经网络扩展到双组分耦合玻色-爱因斯坦凝聚体中高阶异常波的检测中。该方法成功地学习了多参数双组分耦合玻色-爱因斯坦凝聚体中异常波的复杂动力学行为。此外,我们在三维参数空间中有效地定位了一个狭窄的不规则区域,其中二阶类异常波出现。与数值方法的繁琐迭代过程相比,该方法显著减少了计算时间——考虑到时间随着控制参数的数量呈指数增长,这是一个关键优势。这项工作为探索高维参数空间中的复杂行为提供了一种可扩展的工具,在非线性光学、等离子体物理和海洋工程中具有潜在的应用前景,在这些领域,对极端波浪的快速预测至关重要。
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引用次数: 0
期刊
Wave Motion
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