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kolosovpetro committed Sep 16, 2024
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1 change: 0 additions & 1 deletion src/sections/abstract.tex
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For every $t\in\mathbb{T}_1$ and $x,b\in \Lambda^2$
\[
\frac{\Delta t^{2m+1}}{\Delta t} =
% \frac{\partial P(m,b,x)}{\Delta x} \bigg |_{x = t, \; b = \sigma(t)} +
\frac{\partial P(m,b,x)}{\Delta x} (m, \sigma(t), t) +
\frac{\partial P(m,b,x)}{\Delta b} (m, t, t)
\]
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2 changes: 1 addition & 1 deletion src/sections/introduction.tex
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In context of Computer Science, namely object oriented programming paradigm, the time scale calculus may be thought
as unified interface of derivative operator.
Furthermore, the idea of time-scale calculus was slightly extended
in~\cite{bayour2017truly,benkhettou2016conformable,caputo2009time,martins2009calculus}.
in~\cite{bayour2017truly,benkhettou2016conformable,caputo2009time,martins2009calculus}.
32 changes: 16 additions & 16 deletions src/sections/main-results.tex
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@@ -1,31 +1,31 @@
Time scale derivative of the polynomial $t^{2m+1}$ may be expressed as follows
Timescale derivative of the polynomial $t^{2m+1}$ may be expressed as follows
\begin{thm}
\label{main_theorem}
Let $\polynomialP{m}{b}{x}$ be a $2m+1-$degree integer-valued polynomial defined by~\eqref{eq:polynomial_p}.
Let be a two-dimensional time scale
$\Lambda^2 = \mathbb{T}_1 \times \mathbb{T}_2 = \{t=(x, b) \colon \; x\in\mathbb{T}_1, \; b\in\mathbb{T}_2 \}$.
Let be $\mathbb{T}_1 = \mathbb{T}_2$.
For every $t\in\mathbb{T}_1, \; x,b\in \Lambda^2, \; m\in\mathbb{N}, \; m = const$
Let $P(m,b,x)$ be a $2m+1$-degree polynomial in $x,b$.
Let be a two-dimensional timescale
$\Lambda^2 = \mathbb{T}_1 \times \mathbb{T}_2 = \{t=(x, b) \colon \; x\in\mathbb{T}_1, \; b\in\mathbb{T}_2 \}$
such that $\mathbb{T}_1 = \mathbb{T}_2$.
For every $t\in\mathbb{T}_1$ and $x,b\in \Lambda^2$
\[
(t^{2m+1})^{\Delta} =
\frac{\partial \polynomialP{m}{b}{x}}{\Delta x} \bigg |_{x = t, \; b = \sigma(t)}+
\frac{\partial \polynomialP{m}{b}{x}}{\Delta b} \bigg |_{x = t, \; b = t},
\frac{\Delta t^{2m+1}}{\Delta t} =
\frac{\partial P(m,b,x)}{\Delta x} (m, \sigma(t), t) +
\frac{\partial P(m,b,x)}{\Delta b} (m, t, t)
\]
where
\begin{itemize}
\setlength\itemsep{1em}
\item $\sigma(t) > t$ is forward jump operator,
\item $\sigma(t) > t$ -- is forward jump operator

\item $\frac{\partial \polynomialP{m}{b}{x}}{\Delta x} \bigg |_{x = t, \; b = \sigma(t)}$
\item $\frac{\partial \polynomialP{m}{b}{x}}{\Delta x} (m, \sigma(t), t)$ --
is the value of the partial derivative on time scales of
$\polynomialP{m}{b}{x}$ with respect to the variable $x$, evaluated at $x = t, \; b = \sigma(t)$,
$\polynomialP{m}{b}{x}$ with respect to the variable $x$ evaluated in point $x = t, \; b = \sigma(t)$

\item $\frac{\partial \polynomialP{m}{b}{x}}{\Delta b} \bigg |_{x = t, \; b = t}$
\item $\frac{\partial \polynomialP{m}{b}{x}}{\Delta b} (m, t, t)$ --
is the value of the partial derivative on time scales of
$\polynomialP{m}{b}{x}$ with respect to the variable $b$, evaluated at $x = t, \; b = t$.
$\polynomialP{m}{b}{x}$ with respect to the variable $b$, evaluated at $x = t, \; b = t$
\end{itemize}
\end{thm}
In other words, theorem ~\ref{main_theorem} says
In simpler words, the theorem ~\ref{main_theorem} says
\begin{center}
\begin{quotation}
For every odd-exponent polynomial $t^{2m+1}$, its derivative on time scales equals to the sum
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^{\Delta}_{t} =
\frac{\partial}{\Delta x} \left( \sum_{k=0}^{b-1} \sum_{r=0}^{m} \coeffA{m}{r} k^r(x-k)^r \right) \Bigg |_{x = t, \; b = \sigma(t)}
+ \frac{\partial}{\Delta b} \left( \sum_{k=0}^{b-1} \sum_{r=0}^{m} \coeffA{m}{r} k^r(x-k)^r \right) \Bigg |_{x = t, \; b = t}
\end{align*}
\end{align*}

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