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Functional -> operator
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README.md

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@@ -42,7 +42,7 @@ function test_basis(B)
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# This is the continuous axis
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x = axes(B,1)
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# This corresponds to a functional L whose action on a function
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# This corresponds to a operator L whose action on a function
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# f(x) is defined as Lf(x) = sin(2πx)*f(x). In physics this is a
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# potential.
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@info "Sine operator"

docs/src/bsplines/theory.md

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@@ -270,7 +270,7 @@ $$\begin{equation}
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\operator{L}f = g,
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\end{equation}$$
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where $\operator{L}$ is a linear functional, we can solve the equation
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where $\operator{L}$ is a linear operator, we can solve the equation
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approximately by expanding $f$ and $g$ in terms of B-splines:
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$$\begin{equation}
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The right-hand side is trivially in the space $\space{P}_{t,k}$,
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whereas is not necessary true for the left-hand side, i.e. the
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functional $\operator{L}$ may take $f$ out of the space. We can
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operator $\operator{L}$ may take $f$ out of the space. We can
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project the equation into the space $\space{P}_{t,k}$ by
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left-multiplying by the projector $BB^H$:
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