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  "body": "\n## Definition\n\nLet $g \\colon \\R \\to \\R$ be a [[non-decreasing|0WFF6AZPBP]], right-continuous function.\nLet $\\mu_g$ be its [[Lebesgue–Stieltjes measure|QV75XJBFCS]], the Borel measure with $\\mu_g((a, b]) = g(b) - g(a)$ for all $a \u003c b$.\nLet $f \\colon \\R \\to \\R$ be a Borel measurable function that is [[integrable|X7GTF3D98F]] with respect to $\\mu_g$.\nThe *Lebesgue–Stieltjes integral* of $f$ with respect to $g$ is the [[Lebesgue integral|DWJF7ABPR1]]\n$$\\int_\\R f \\, dg = \\int_\\R f \\, d\\mu_g.$$\n\n## Remarks\n\nExample: let $g = \\mathbf{1}_{[0, \\infty)}$, the Heaviside step function with $g(0) = 1$, which is non-decreasing and right-continuous.\nThen $\\mu_g$ is the Dirac measure at $0$, so $\\int f \\, dg = f(0)$ for every Borel function $f$.\nFor $g(x) = x$ the measure $\\mu_g$ is Lebesgue measure, and the integral is the usual Lebesgue integral.\n\nNon-example: $g(x) = -x$ is not non-decreasing, so the definition does not apply directly.\nThe formula $\\mu_g((a, b]) = g(b) - g(a)$ would give negative mass.\n\nFor $g$ of bounded variation and right-continuous, one writes $g = g_1 - g_2$ with $g_1, g_2$ non-decreasing and right-continuous, and sets $\\int f \\, dg = \\int f \\, dg_1 - \\int f \\, dg_2$.\nOn $[a, b]$ one writes $\\int_{(a, b]} f \\, dg$, and the endpoints matter when $g$ jumps there.\nIf $f$ is continuous on $[a, b]$, the integral over $(a, b]$ equals the Riemann–Stieltjes integral $\\int_a^b f \\, dg$.\nIf $g$ is absolutely continuous on bounded intervals, then $\\int f \\, dg = \\int f(x) g'(x) \\, dx$.\n",
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