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Dynamics of soliton propagation: bifurcation, chaos, and quantitative insights into the modified Camassa-Holm equation. [PDF]
Alam MN +5 more
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Fuzzy-based numerical analysis of Sisko hybrid nanofluid bioconvective flow over a stretched cylinder for osteoarthritis drug delivery. [PDF]
Karthik V +5 more
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Dynamical modeling of TNF-α, IL-6, and IL-10 interactions in stroke-induced inflammation. [PDF]
Arishi FAM, Rambely AS, Abdul Razak F.
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Dynamic modeling of PISA achievement scores: comparative analysis of artificial neural networks and differential equation systems approaches. [PDF]
Daşbaşi B.
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Applied Mathematics and Computation, 2007
zbMATH Open Web Interface contents unavailable due to conflicting licenses.
Biazar, J., Ghazvini, H.
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zbMATH Open Web Interface contents unavailable due to conflicting licenses.
Biazar, J., Ghazvini, H.
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An Efficient Method for Solving Systems of Linear Ordinary and Fractional Differential Equations
Bulletin of the Malaysian Mathematical Sciences Society, 2015zbMATH Open Web Interface contents unavailable due to conflicting licenses.
Didgar, Mohsen, Ahmadi, Nafiseh
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BIT Numerical Mathematics, 2008
Consider the highly oscillatory system of ordinary differential equations (ODEs) \[ y'=A_{\omega }y+f(t,y),\quad y(0)=y_o\in{\mathbb{R}}^d,\;t\geq 0, \] where \(A_{\omega}\) is a constant non-singular \(d\times d\) matrix with large eigenvalues, \(\sigma (A_{\omega })\subset\) i\({\mathbf{R}}\), \(\parallel A_{\omega}\parallel\gg 1,\omega\gg 1\) is a ...
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Consider the highly oscillatory system of ordinary differential equations (ODEs) \[ y'=A_{\omega }y+f(t,y),\quad y(0)=y_o\in{\mathbb{R}}^d,\;t\geq 0, \] where \(A_{\omega}\) is a constant non-singular \(d\times d\) matrix with large eigenvalues, \(\sigma (A_{\omega })\subset\) i\({\mathbf{R}}\), \(\parallel A_{\omega}\parallel\gg 1,\omega\gg 1\) is a ...
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