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Journal Article
ACCEPTED MANUSCRIPT
Ghulam Abbass and others
IMA Journal of Applied Mathematics, hxaf009, https://doi.org/10.1093/imamat/hxaf009
Published: 25 April 2025
Journal Article
ACCEPTED MANUSCRIPT
Baoquan Zhou and others
IMA Journal of Applied Mathematics, hxaf008, https://doi.org/10.1093/imamat/hxaf008
Published: 16 April 2025
Journal Article
ACCEPTED MANUSCRIPT
R Bustamante and others
IMA Journal of Applied Mathematics, hxaf010, https://doi.org/10.1093/imamat/hxaf010
Published: 14 April 2025
Journal Article
ACCEPTED MANUSCRIPT
Stephen L Strickland and others
IMA Journal of Applied Mathematics, hxaf006, https://doi.org/10.1093/imamat/hxaf006
Published: 10 April 2025
Journal Article
Manasa Bhat and Santanu Manna
IMA Journal of Applied Mathematics, hxaf007, https://doi.org/10.1093/imamat/hxaf007
Published: 29 March 2025
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Published: 29 March 2025
Geometry of the problem.
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Published: 29 March 2025
Dispersion curves for non-local elastic Rayleigh waves in an isotropic layered medium.
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Published: 29 March 2025
Dispersion curves for non-local elastic Love waves in an isotropic layered medium.
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Published: 21 March 2025
Phase portraits for the second-order equation ( 10 ). Since we found numerically that , we use for the case (left), and for (right). In both panels, the green vertical lines indicate the singularities at , and the black curves are the level curves for .
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Published: 21 March 2025
Complex plane for eigenvalues of the spectral stability problem ( 12 ), for values near the first eigenvalue crossing. As increases, the non-zero eigenvalue pair moves towards the origin, crossing through onto the real axis around .
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Published: 21 March 2025
The same as Fig. 8 but for the transition in Fig. 7 .
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Published: 21 March 2025
Phase portrait for the second-order equation ( 10 ) with . Two homoclinic orbits correspond to the smooth profiles with values in .
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Published: 21 March 2025
Bright soliton profiles for various values of the frequency .
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Published: 21 March 2025
Top: square of the bifurcating unstable eigenvalue for the spectral stability problem ( 12 ). Bottom: the map . In the top panel, the dashed horizontal line is drawn at and the solid green curve is the function , which is the boundary of the continuous spectrum. In both panels, the das
Image
Published: 21 March 2025
Initial and final frequencies shown in the plane for the numerical simulations. The point represents the bright soliton with the peaked profile. The dashed line indicates the unstable branch, while the other two branches are stable.
Journal Article
P G Kevrekidis and others
IMA Journal of Applied Mathematics, hxaf005, https://doi.org/10.1093/imamat/hxaf005
Published: 21 March 2025
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Published: 21 March 2025
The function vs. . The unique zero of for positive occurs at .
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Published: 21 March 2025
Left: the initial and final solution profiles of the computations for the transition in Fig. 7 together with the final soliton profile. Right: oscillations near the stable profile for the final segment of numerical computations.
Journal Article
Penny J Davies
IMA Journal of Applied Mathematics, hxaf004, https://doi.org/10.1093/imamat/hxaf004
Published: 18 February 2025
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Published: 18 February 2025
Plot of calculated (red solid line) obtained using the frequency domain NN method with a stacked system of submatrices with when with no added noise (top) and added noise-level (bottom). The exact value is shown as a black dotted line and the blue dashed line shows calcul