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  "body": "\n## Proof\n\n1. Let $u, v : I \\to \\R$ be $n$ times differentiable and $\\alpha, \\beta \\in \\R$. By [[linearity of differentiation|0M0TKFRX2A]], applied $k$ times, $(\\alpha u + \\beta v)^{(k)} = \\alpha u^{(k)} + \\beta v^{(k)}$ for $k \\le n$.\n2. Multiplying by $a_k$ and adding over $k$ gives $L(\\alpha u + \\beta v) = \\alpha L u + \\beta L v$ on $I$. This is the computation of the [[superposition principle|0F2VBPXNP9]].\n3. Let $S$ be the set of solutions of the [[homogeneous equation|0EQZSAB9EC]] $L y = 0$ on $I$. Since $(y_1, \\dots, y_n)$ is a [[fundamental system|0H4KNNCHPY]], it is a basis of $S$.\n4. Assume $y$ is a solution of the [[linear equation|0PB7K8M7FG]] $L y = b$ on $I$. Then $y - y_p$ is $n$ times differentiable, and $L(y - y_p) = L y - L y_p = b - b = 0$ by step 2.\n5. So $y - y_p \\in S$. By step 3, $y - y_p = c_1 y_1 + \\dots + c_n y_n$ for some real numbers $c_1, \\dots, c_n$. This gives the stated form of $y$.\n6. Conversely, let $y = y_p + c_1 y_1 + \\dots + c_n y_n$ with $c_1, \\dots, c_n \\in \\R$. Then $y$ is $n$ times differentiable, as a combination of such functions.\n7. By step 2, $L y = L y_p + c_1 L y_1 + \\dots + c_n L y_n = b + 0 + \\dots + 0 = b$ on $I$. So $y$ solves $L y = b$ on $I$.\n\n## Idea\n\nThe operator $L$ is linear. So two solutions of $L y = b$ differ by a solution of $L y = 0$. The fundamental system describes all solutions of $L y = 0$, and adding $y_p$ describes all solutions of $L y = b$.\n",
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