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  "body": "\n## Proof\n\nWe solve the system with the inverse matrix and read off each coordinate by a Laplace expansion.\n\n1. Let $A = (a_{kl})$ be an $n \\times n$ matrix over the [[field|0QA8CHH8MG]] $F$ with $\\det A \\ne 0$, and let $b = (b_1, \\dots, b_n) \\in F^n$.\n2. First let $n = 1$. Then $A = (a_{11})$ with $a_{11} \\ne 0$, by the [[Leibniz formula|016PE4VZ8Q]] with one term. The equation $a_{11} x_1 = b_1$ has the single solution $x_1 = b_1 / a_{11}$.\n3. For $n = 1$, $A_1 = (b_1)$ and $\\det A_1 = b_1$. So $x_1 = \\det A_1 / \\det A$, as claimed. From now on let $n \\ge 2$.\n4. In a field, the nonzero element $\\det A$ is a unit. By the [[inverse in terms of the adjugate|0ENVM493VK]], $A$ is invertible with $A^{-1} = (\\det A)^{-1} \\operatorname{adj}(A)$.\n5. Existence: let $x = A^{-1} b$. By [[associativity|073E4XC016]], $A x = (A A^{-1}) b = I_n b = b$. So $x$ is a solution of the [[linear system|0JTRMBQ1SA]] $Ax = b$.\n6. Uniqueness: if $A y = b$, then $y = (A^{-1} A) y = A^{-1} (A y) = A^{-1} b = x$, by associativity.\n7. Let $C_{kl}$ be the [[cofactors|0W2QAVJQ1W]] of $A$. By the definition of the [[adjugate|0GMPYM0NSR]] and the [[matrix product|076JGP6R3T]], $x_i = (\\det A)^{-1} \\sum_{j=1}^{n} C_{ji} b_j$.\n8. Fix $i$. The matrix $A_i$ differs from $A$ only in column $i$, and it has entry $b_j$ in position $(j, i)$.\n9. A cofactor in position $(j, i)$ deletes column $i$. So the cofactors of $A_i$ in the positions $(j, i)$ equal the cofactors $C_{ji}$ of $A$.\n10. By the [[Laplace expansion along column $i$|06AMCJMMVM]] of $A_i$ and steps 8 and 9, $\\det A_i = \\sum_{j=1}^{n} b_j C_{ji}$.\n11. By steps 7 and 10, $x_i = \\det A_i / \\det A$ for $1 \\le i \\le n$.\n\n## Idea\n\nThe solution is $x = A^{-1} b = (\\det A)^{-1} \\operatorname{adj}(A)\\, b$. Coordinate $i$ of $\\operatorname{adj}(A)\\, b$ pairs $b$ with the cofactors of column $i$. That pairing is exactly the Laplace expansion of $\\det A_i$ along its new column $i$.\n",
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