Non-integrable functions
-
∫11+x2=arctan(x)x→∞→π/2<∞
-
Any bounded function (or continuous on a compact set, by EVT)
-
∫101√x<∞
-
∫101x1−ε<∞
-
∫∞11x1+ε<∞
- ∫101x=∞.
- ∫∞11x=∞.
- ∫∞11√x=∞
- ∫∞11x1−ε=∞
- ∫101x1+ε=∞
Sequences fka.e.→f but fk:
-
For 1\leq p < \infty: The skateboard to infinity, f_k = \chi_{[k, k+1]}.
Then f_k \overset{a.e.}\to 0 but {\left\lVert {f_k} \right\rVert}_p = 1 for all k.
Converges pointwise and a.e., but not uniformly and not in norm.
-
For p = \infty: The sliding boxes f_k = k \cdot \chi_{[0, \frac 1 k]}.
Then similarly f_k \overset{a.e.}\to 0, but {\left\lVert {f_k} \right\rVert}_p = 1 and {\left\lVert {f_k} \right\rVert}_\infty = k \to \infty
Converges a.e., but not uniformly, not pointwise, and not in norm.
Notions of convergence:
- Uniform
- Pointwise
- Almost everywhere
- In norm
Uniform \implies pointwise \implies almost everywhere, but in general non of these can be reversed.
- Uniform: f_n \rightrightarrows f: \forall \varepsilon ~\exists N {~\mathrel{\Big\vert}~}~n\geq N \implies {\left\lvert {f_N(x) - f(x)} \right\rvert} < \varepsilon \quad \forall x.
- Pointwise: f_n(x) \to f(x) for all x. (This is just a sequence of numbers)
- Almost Everywhere: f_n(x) \to f(x) for almost all x.
- Norm: {\left\lVert {f_n - f} \right\rVert}_1 = \int {\left\lvert {f_n(x) - f(x)} \right\rvert} \to 0.
We have 1 \implies 2 \implies 3, and in general no implication can be reversed, but (warning) none of 1,2,3 imply 4 or vice versa.
-
f_n = (1/n) \chi_{(0, n)}. This converges uniformly to 0, but the integral is identically 1. So this satisfies 1,2,3 and not 4.
-
f_n = \chi_{(n, n+1)} (skateboard to infinity). This satisfies 2,3 but not 1, 4.
-
f_n = n\chi_{(0, \frac 1 n)}. This satisfies 3 but not 1,2,4.
-
f_n: one can construct a sequence where f_n \to 0 in L^1 but is not 1,2, or 3. The construction:
- Break I into 2 intervals, let f_1 be the indicator on the first half, f_2 the indicator on the second.
- Break I into 2^2=4 intervals, like f_3 be the indicator on the first quarter, f_4 on the second, etc.
- Break I into 2^k intervals and cyclic through k indicator functions.
- Then \int f_n = 1/2^n \to 0, but f_n\not\to 0 pointwise since for every x, there are infinitely many n for which f_n(x) = 0 and infinitely many for which f_n(x) = 1.
Almost everywhere convergence does not imply L^p convergence for any 1\leq p \leq \infty. In the following examples, f_k \overset{a.e.}\to f but f_k \overset{L^p}{\not\to} f:
-
For 1\leq p < \infty: The skateboard to infinity, f_k = \chi_{[k, k+1]}.
- Then f_k \overset{a.e.}\to 0 but {\left\lVert {f_k} \right\rVert}_p = 1 for all k.
- Converges pointwise and a.e., but not uniformly and not in norm.
-
For p = \infty: The sliding boxes f_k = k \cdot \chi_{[0, \frac 1 k]}.
-
Then similarly f_k \overset{a.e.}\to 0, but {\left\lVert {f_k} \right\rVert}_p = 1 and {\left\lVert {f_k} \right\rVert}_\infty = k \to \infty
-
Converges a.e., but not uniformly, not pointwise, and not in norm.
-
For any measure space (X, {\mathcal{M}}, \mu),
- L^1(X) is Banach space.
- L^2(X) is a (possibly non-separable) Hilbert space.