What is the oscillator model in a generalized Snyder scheme?

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The oscillator model in a generalized Snyder scheme describes the dynamics of oscillating systems through coupled differential equations. It typically involves two states, X and Y, influenced by coefficients A and B, along with external forcing terms F(t) and G(t). The model is particularly useful for analyzing nonlinear systems across various scientific fields. The derived formula for the oscillator's behavior incorporates an exponential term and an integral that accounts for the forcing function over time. This mathematical framework aids in understanding complex oscillatory phenomena in physical, chemical, and biological contexts.
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$$H= \frac{1}{4} \sum_{\mu v}\left(\frac{\hat{\rho}_{\mu v}^{2}}{M}+M \omega^{2} \hat{x}_{\mu v}^{2}\right)+\lambda \hat{x}^{4},$$
What is the oscillator model in a generalized Snyder scheme?How to derive the formula?
 

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The oscillator model in a generalized Snyder scheme is a mathematical model that describes the dynamics of an oscillator, i.e. a system which can oscillate between two states over time. It is usually derived from a system of coupled differential equations, in which the oscillator is driven by a forcing term. The model is most commonly used to describe the behavior of nonlinear systems, such as those found in physical, chemical, and biological processes.The formula for the oscillator model in a generalized Snyder scheme can be derived by starting with the following system of coupled differential equations: \begin{alignat}{3}\frac{dX}{dt} &= A X + F(t) \\\ \frac{dY}{dt} &= B Y + G(t)\end{alignat}Where X and Y are the two states of the oscillator, A and B are the coefficients of the coupling between the two states, and F(t) and G(t) are the forcing terms. Solving the above system of equations yields the following equation for the oscillator model: \begin{equation}X(t) = X_0 e^{At} + \int_0^t e^{A(t-\tau)}F(\tau) d\tau\end{equation}Where X_0 is the initial condition of the oscillator at time t=0.
 
At first, I derived that: $$\nabla \frac 1{\mu}=-\frac 1{{\mu}^3}\left((1-\beta^2)+\frac{\dot{\vec\beta}\cdot\vec R}c\right)\vec R$$ (dot means differentiation with respect to ##t'##). I assume this result is true because it gives valid result for magnetic field. To find electric field one should also derive partial derivative of ##\vec A## with respect to ##t##. I've used chain rule, substituted ##\vec A## and used derivative of product formula. $$\frac {\partial \vec A}{\partial t}=\frac...