$ \newcommand{\braket}[1]{\langle #1 \rangle} \newcommand{\abs}[2][]{\left\lvert#2\right\rvert_{\text{#1}}} \newcommand{\ket}[1]{\left\lvert#1 \right.\rangle} \newcommand{\bra}[1]{\langle\left. #1\right\rvert} \newcommand{\braket}[1]{\langle #1 \rangle} \newcommand{\dd}{\text{d}} \newcommand{\dv}[2]{\frac{\dd #1}{\dd #2}} \newcommand{\pdv}[2]{\frac{\partial}{\partial #1}} $
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A vecot $x$ in a field $\mathbb{F}^n$ is written $$\begin{align*} x=\begin{bmatrix}x_1 \\ \dots \\ x_n \end{bmatrix}\in\mathbb{F}^n \end{align*}$$

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A vecot $x$ in a field $\mathbb{F}^n$ is written $$\begin{align*} x=\begin{bmatrix}x_1 \\ \dots \\ x_n \end{bmatrix}\in\mathbb{F}^n \end{align*}$$

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definition
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FullPage
definition
concepts
used in
hypothesis
results
A vecot $x$ in a field $\mathbb{F}^n$ is written $$\begin{align*} x=\begin{bmatrix}x_1 \\ \dots \\ x_n \end{bmatrix}\in\mathbb{F}^n \end{align*}$$

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A vecot $x$ in a field $\mathbb{F}^n$ is written $$\begin{align*} x=\begin{bmatrix}x_1 \\ \dots \\ x_n \end{bmatrix}\in\mathbb{F}^n \end{align*}$$

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