Read the Shape of the Estimate First
Integral estimates often become simpler once the expression to be bounded is classified by its structure. A product of functions suggests Hölder’s inequality; a sum inside an \(L^p\) norm suggests Minkowski’s inequality; and a convex function applied to an average suggests Jensen’s inequality. The choice is not merely a matter of taste: each inequality has specific hypotheses, and applying the right one at the right stage avoids unnecessary estimates or invalid steps.
Throughout, \((X,\mathcal{M},\mu)\) is a measure space, with no assumption that \(\mu\) is finite unless stated. Functions in \(L^p(\mu)\) are measurable, real- or complex-valued functions with finite \(L^p\) norm, understood up to equality \(\mu\)-a.e. For \(1\le p<\infty\), \(\|f\|_p=(\int_X|f|^p\,d\mu)^{1/p}\); \(\|f\|_\infty\) is the essential supremum of \(|f|\). The inequalities below apply to measurable representatives, and their integral conclusions are unchanged by modifying those representatives on null sets.
In the forms used here, Hölder says that if \(1\le p,q\le\infty\) are conjugate exponents, meaning \(1/p+1/q=1\) with \(1/\infty=0\), then \(f\in L^p(\mu)\) and \(g\in L^q(\mu)\) imply \(\int_X|fg|\,d\mu\le\|f\|_p\|g\|_q\). Minkowski says that for \(1\le p\le\infty\) and \(f,g\in L^p(\mu)\), \(\|f+g\|_p\le\|f\|_p+\|g\|_p\). These inequalities, including their endpoint cases, were established in the earlier material on Hölder and Minkowski. Jensen’s integral inequality says that if \(\mathbb{P}\) is a probability measure, \(f\) is an integrable real-valued function, \(\phi\) is convex on an interval containing the values of \(f\), and \(\phi(f)\) is integrable, then \(\phi(\int f\,d\mathbb{P})\le\int\phi(f)\,d\mathbb{P}\). We use these standard results with their hypotheses checked below.
Worked Estimates by Structure
Worked Example: A Product Calls for Hölder
On \([0,1]\) with Lebesgue measure \(m\), define \(f(x)=x^{-1/4}\) for \(0<x\le1\), set \(f(0)=0\), and let \(g(x)=1+x\). Estimate \(\int_0^1|fg|\,dm\) using Hölder with exponents \(2,2\), then check the estimate directly.
Both functions are measurable and real-valued. The assigned value at \(0\) does not affect any integral. First compute the squared norms:
Thus \(f,g\in L^2(m)\), and the exponents are conjugate since \(1/2+1/2=1\). Hölder gives
To check, \(fg=x^{-1/4}+x^{3/4}\) for \(x>0\), so direct integration gives
The bound holds: both sides are nonnegative, and \((40/21)^2=1600/441\le2058/441=14/3\). The direct value is smaller than the Hölder bound, as expected; Hölder need not give equality.
Worked Example: A Sum Inside a Norm Calls for Minkowski
On \([0,1]\) with Lebesgue measure, let \(f(x)=x\) and \(g(x)=1\). Estimate \(\|f+g\|_2\). Both functions are measurable and belong to \(L^2(m)\), since \(\int_0^1x^2\,dm=1/3\) and \(\int_0^1 1\,dm=1\). Minkowski therefore applies and yields
Compute the left side independently:
For an exact check, both sides are nonnegative and \(\frac73\le(1+\frac1{\sqrt3})^2=\frac43+\frac2{\sqrt3}\). This last inequality is equivalent to \(1\le2/\sqrt3\), which holds because \(1\le4/3\) after squaring positive quantities. Thus the computed norm satisfies the Minkowski bound.
Worked Example: A Convex Function of an Average Calls for Jensen
Give a lower bound for \(\int_0^1x^2\,dm\) by applying Jensen to \(\phi(t)=t^2\). The measure space is \(([0,1],\mathcal{L},m)\), and \(m([0,1])=1\), so \(m\) is already a probability measure on this interval. The function \(f(x)=x\) is integrable and takes values in the convexity interval \([0,1]\); \(\phi(t)=t^2\) is convex there, and \(\phi(f(x))=x^2\) is integrable. All hypotheses hold. Jensen gives
The average is \(\int_0^1x\,dm=1/2\), so Jensen gives the lower bound \(1/4\). Direct integration gives \(\int_0^1x^2\,dm=1/3\), and \(1/4\le1/3\). This verifies the bound and its direction: for a convex function, the function of the average is at most the average of the function.
Combining the Choices
Some targets contain more than one structure. A sum of products, for example, may require first separating the sum inside a norm and then estimating each product. The order matters: Minkowski handles the sum, while Hölder handles each product. The following result records this common two-stage estimate.
Proof. For each \(j\), the definition of essential supremum gives \(|b_j|\le\|b_j\|_\infty\) \(\mu\)-a.e. Therefore \(|a_jb_j|^p\le\|b_j\|_\infty^p|a_j|^p\) a.e.; integrating shows that \(a_jb_j\in L^p(\mu)\) and \(\|a_jb_j\|_p\le\|a_j\|_p\|b_j\|_\infty\). For \(N=1\), this is the claimed inequality. For \(N>1\), repeated application of Minkowski to the finite sum gives \(\|\sum_{j=1}^Na_jb_j\|_p\le\sum_{j=1}^N\|a_jb_j\|_p\). Substituting the bound for each product proves the result. No finiteness or sigma-finiteness assumption on \(\mu\) is needed. \(\square\)
This proposition illustrates a useful order of operations. A norm of a sum is not itself a product, so first use the inequality designed for sums. Afterward, estimate each product. The same reasoning works with Hölder in place of the \(L^\infty\) product bound when the factors have suitable conjugate exponents, provided each resulting product belongs to the \(L^p\) space required by Minkowski.
Proof. Define a probability measure \(\mathbb{P}\) on \(E\) by \(\mathbb{P}(A)=\mu(A)/\mu(E)\) for measurable \(A\subseteq E\). It is a probability measure because \(\mathbb{P}(E)=1\). The integral with respect to it satisfies \(\int_E h\,d\mathbb{P}=(1/\mu(E))\int_Eh\,d\mu\) for integrable \(h\). Apply integral Jensen for \(\mathbb{P}\) to \(f\) and \(\phi\), using the stated integrability and convexity hypotheses, to obtain the displayed inequality. \(\square\)
A Common Normalization Error
Jensen’s probability-measure form cannot be applied to an unnormalized finite measure as if its total mass were one. For a concrete countercheck, take \(E=[0,2]\), Lebesgue measure, \(f(x)=x\), and \(\phi(t)=t^2\). A mistaken use of probability Jensen would assert \(\int_0^2x^2\,dm\ge(\int_0^2x\,dm)^2\). But the left side is \(8/3\), while the right side is \(2^2=4\), so this asserted inequality is false.
The correction is to divide by the mass \(m(E)=2\). The average of \(f\) is \((1/2)\int_0^2x\,dm=1\), and the average of \(f^2\) is \((1/2)\int_0^2x^2\,dm=4/3\). Jensen correctly gives \(1^2\le4/3\). Equivalently, in unnormalized form the inequality is \(\int_E f^2\,dm\ge(\int_E f\,dm)^2/m(E)\), not \(\int_E f^2\,dm\ge(\int_E f\,dm)^2\).
A different mistake is to use Minkowski on a product simply because the expression contains two functions, or to use Jensen without an average. Instead, inspect the precise target: \(\int|fg|\) has product form; \(\|f+g\|_p\) has a sum inside a norm; and \(\phi(\int f\,d\mathbb{P})\) has a convex function of an average. In a longer calculation, identify the innermost structure first, check its hypotheses, and then move outward.
Check Your Understanding
For each problem, identify the relevant inequality and state the hypothesis that allows its use.
- On a probability space, \(f\) is real-valued and integrable, and \(f^2\) is integrable. What lower bound does Jensen with \(\phi(t)=t^2\) give for \(\int f^2\,d\mathbb{P}\)?
- If \(f,g\in L^3(\mu)\), which inequality directly estimates \(\|f+g\|_3\), and what is the resulting bound?
- If \(f\in L^2(\mu)\) and \(g\in L^2(\mu)\), which inequality estimates \(\int|fg|\,d\mu\), and what are the conjugate exponents?
- For a measurable set \(E\) with \(0<\mu(E)<\infty\), write the normalized Jensen inequality for a convex \(\phi\) and identify the probability measure used.
- In an estimate of \(\|a_1b_1+a_2b_2\|_p\), which inequality should be applied to the sum first, and which type of bound can then be used for each product?