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Complex Measures and Duality · Tutorial 504 of 798

Bounded Functionals from L1 Pairings

Learn to construct the bounded L1 functional associated with an essentially bounded function, compute its exact norm, and understand why sigma-finiteness matters.

Advanced 11 min read

What You'll Learn

  • Define the complex-valued L1 pairing induced by an essentially bounded function.
  • Verify that the pairing is well-defined on almost-everywhere equivalence classes.
  • Prove the upper and lower bounds that give the exact operator norm.
  • Construct unit L1 functions that approach the norm using level sets and complex phases.
  • Distinguish the operator norm from attainment of that norm.
  • See why sigma-finiteness is needed for the stated norm formula.

The Pairing and Its Operator Norm

Let \((X,\mathcal{M},\mu)\) be a sigma-finite measure space; completeness is not required. Sigma-finiteness means that \(X\) is a countable union of measurable sets of finite measure. We work with complex-valued measurable functions, identifying functions that agree \(\mu\)-almost everywhere. The space \(L^1(\mu)\) consists of these equivalence classes \(f\) for which \(\int |f|\,d\mu<\infty\), with norm \(\|f\|_1=\int |f|\,d\mu\).

Definition: For a measurable complex-valued function \(g\), its essential supremum norm is \(\|g\|_\infty=\inf\{C\ge0: |g|\le C\ \mu\text{-a.e.}\}\). The function \(g\) is essentially bounded if this number is finite. For such a \(g\), define \(T_g:L^1(\mu)\to\mathbb{C}\) by \(T_g(f)=\int fg\,d\mu\). This pairing is bilinear: it does not put a complex conjugate on \(f\).

The integral defining \(T_g(f)\) exists because \(|fg|\le\|g\|_\infty|f|\) almost everywhere. If \(f\) is changed on a null set, \(fg\) is changed only on a null set, so the value of the integral is unchanged. Thus \(T_g\) is defined on equivalence classes, not just on particular representatives. Its operator norm is \(\|T_g\|=\sup\{|T_g(f)|:\|f\|_1\le1\}\).

Essential Bounds and the Exact Norm

Lemma: If \(g\) is essentially bounded and \(M=\|g\|_\infty\), then \(|g|\le M\) almost everywhere. Moreover, for every \(a\) with \(0\le a<M\), the set \(\{|g|>a\}\) has positive measure.

Proof. By the definition of the infimum, for each positive integer \(n\) there is a bound \(C_n<M+1/n\) such that \(|g|\le C_n\) almost everywhere. Therefore \(|g|\le M+1/n\) outside a null set \(N_n\). The union \(N=\bigcup_nN_n\) is null, and outside \(N\) all these bounds hold. Letting \(n\) tend to infinity gives \(|g|\le M\) there. Now suppose \(0\le a<M\) and \(\{|g|>a\}\) were null. Then \(|g|\le a\) almost everywhere, which would imply \(M\le a\) by the definition of \(M\), a contradiction. Hence \(\{|g|>a\}\) has positive measure. \(\square\)

Theorem: For a sigma-finite measure space \((X,\mathcal{M},\mu)\) and an essentially bounded measurable complex-valued function \(g\), the map \(T_g(f)=\int fg\,d\mu\) is a bounded linear functional on \(L^1(\mu)\), and \(\|T_g\|=\|g\|_\infty\).

Proof. Linearity follows from the linearity of the complex Lebesgue integral. Write \(M=\|g\|_\infty\). The lemma gives \(|g|\le M\) almost everywhere, so for every \(f\in L^1(\mu)\), \[ |T_g(f)|=\left|\int fg\,d\mu\right|\le\int|f||g|\,d\mu\le M\int|f|\,d\mu=M\|f\|_1. \] Thus \(T_g\) is bounded and \(\|T_g\|\le M\). This also covers \(M=0\): then \(g=0\) almost everywhere and \(T_g\) is the zero functional.

For the reverse inequality, suppose \(M>0\) and fix \(a\) with \(0\le a<M\). By the lemma, \(E=\{|g|>a\}\) has positive measure. Sigma-finiteness gives a countable cover \(X=\bigcup_jX_j\) with each \(X_j\) measurable and of finite measure. Since \(E=\bigcup_j(E\cap X_j)\) has positive measure, at least one set \(A=E\cap X_j\) has positive measure. It has finite measure because \(\mu(A)\le\mu(X_j)<\infty\).

Define \(u(x)=\overline{g(x)}/|g(x)|\) where \(g(x)\ne0\), and \(u(x)=0\) where \(g(x)=0\). This is measurable, and \(|u|=1\) on \(A\), since \(|g|>a\ge0\) there. Set \(f=u\chi_A/\mu(A)\). Then \(\|f\|_1=1\), and \[ T_g(f)=\frac{1}{\mu(A)}\int_A |g|\,d\mu>a. \] The strict inequality holds because \(|g|-a\) is positive at every point of \(A\); a positive measurable function on a set of positive measure has positive integral. Consequently \(\|T_g\|\ge a\) for every \(a<M\), and hence \(\|T_g\|\ge M\). Combined with the upper bound this gives equality. \(\square\)

The phase \(u\) in the proof is essential: it makes \(u g=|g|\), so cancellation cannot reduce the integral. Sigma-finiteness is used to find a subset \(A\) of finite, positive measure, making the normalized indicator an admissible \(L^1\) function.

Worked Pairings

Worked Example: A Complex Pairing on a Finite Space

Let \(X=\{1,2,3\}\), let \(\mathcal{M}\) be its power set, and let \(\mu\) be counting measure. Set \(g(1)=3\), \(g(2)=4i\), and \(g(3)=0\). Compute the norm of \(T_g\) and exhibit a unit vector attaining it.

For \(f=(f(1),f(2),f(3))\), the \(L^1\) norm is \(|f(1)|+|f(2)|+|f(3)|\), while \[ T_g(f)=3f(1)+4i f(2). \] Therefore \[ |T_g(f)|\le3|f(1)|+4|f(2)|\le4\bigl(|f(1)|+|f(2)|+|f(3)|\bigr)=4\|f\|_1. \] The essential supremum of \(|g|\) is \(\max\{3,4,0\}=4\). Take \(f(1)=0,\ f(2)=-i,\ f(3)=0\). Its norm is \(|-i|=1\), and \(T_g(f)=(-i)(4i)=4\). Thus the bound is attained and \(\|T_g\|=4=\|g\|_\infty\). Check: the general upper bound gives \(\|T_g\|\le4\), and this unit vector gives \(\|T_g\|\ge4\).

Worked Example: Approaching the Norm on an Interval

On \(X=(0,1)\) with Lebesgue measure \(m\), let \(g(x)=x\). Its essential supremum is \(1\): \(x\le1\) everywhere on the domain, and for every \(a<1\) with \(a\ge0\), the set \(\{x\in(0,1):x>a\}=(a,1)\) has positive measure.

For each integer \(n\ge2\), let \(A_n=(1-1/n,1)\) and \(f_n=n\chi_{A_n}\). The interval has measure \(m(A_n)=1/n\), so \(\|f_n\|_1=n(1/n)=1\). Direct integration gives \[ T_g(f_n)=n\int_{1-1/n}^{1}x\,dx =\frac{n}{2}\left(1-\left(1-\frac1n\right)^2\right) =1-\frac{1}{2n}. \] For \(n=2\) this is \(3/4\); for \(n=4\) it is \(7/8\). In general these values approach \(1\), so the operator norm is at least \(1\), and the theorem's upper bound makes it exactly \(1\). Check: \(1-1/(2n)<1=\|g\|_\infty\) for each finite \(n\), while the limit of these values is \(1\).

Worked Example: A Complex Phase Near the Essential Maximum

Again use \((0,1)\) with Lebesgue measure, now with \(g(x)=i(1+x)\). Since \(|g(x)|=1+x<2\) on \((0,1)\), and for each \(a<2\) sufficiently close to \(2\) the set \(\{x:1+x>a\}=(a-1,1)\) has positive measure, \(\|g\|_\infty=2\).

For \(n\ge2\), put \(A_n=(1-1/n,1)\) and \(f_n(x)=-in\chi_{A_n}(x)\). Then \(\|f_n\|_1=n\,m(A_n)=1\). On \(A_n\), \(f_ng=(-in)i(1+x)=n(1+x)\), so \[ T_g(f_n)=n\int_{1-1/n}^{1}(1+x)\,dx =n\cdot\frac1n\left(1+\frac{(1-1/n)+1}{2}\right) =2-\frac{1}{2n}. \] For \(n=2\), the value is \(7/4\); for \(n=4\), it is \(15/8\). These approach \(2\), in agreement with the theorem. Check: the average of \(1+x\) over \(A_n\) is \(2-1/(2n)\), and the chosen phase makes the product real and nonnegative.

Norm Attainment and a Common Pitfall

The operator norm is a supremum over the unit ball; it need not be the value at any one function. In the example \(g(x)=x\) on \((0,1)\), no \(f\in L^1(m)\) with \(\|f\|_1\le1\) satisfies \(|T_g(f)|=1\). Indeed, \[ |T_g(f)|\le\int_0^1|f(x)|x\,dm =\|f\|_1-\int_0^1|f(x)|(1-x)\,dm. \] If \(f\ne0\) as an \(L^1\) equivalence class, then \(|f|(1-x)>0\) on a set of positive measure: \(|f|>0\) on a set of positive measure, and \(1-x>0\) everywhere on \((0,1)\). Its integral is therefore strictly positive. Hence \(|T_g(f)|<\|f\|_1\le1\). For \(f=0\), the pairing is \(0<1\) as well. Thus the norm \(1\) is approached by the displayed sequence but is not attained.

A common mistake is to try to attain the norm by normalizing the indicator of the set where \(|g|=\|g\|_\infty\). For \(g(x)=x\) on \((0,1)\), that set is empty, so this construction cannot work. The correct argument uses the positive-measure level sets \(\{|g|>a\}\) for \(a<\|g\|_\infty\), and then lets \(a\) increase to the essential supremum.

Sigma-finiteness is also a real hypothesis for this version of the result. For example, take \(X\) uncountable, \(\mathcal{M}=\{\varnothing,X\}\), and \(\mu(\varnothing)=0,\ \mu(X)=\infty\). This measure space is not sigma-finite. Every measurable complex-valued function on it is constant: a nonconstant function would have two distinct values separated by an open set, whose preimage would have to be neither \(\varnothing\) nor \(X\). For \(g=1\), the essential supremum is \(1\), but every nonzero constant function has infinite \(L^1\) norm, so \(L^1(\mu)=\{0\}\) and \(T_g\) has norm \(0\). This shows why one cannot omit sigma-finiteness without further assumptions on the measure space.

Check Your Understanding

Use the definition of the pairing and the proof of the norm formula to answer the following.

  1. For counting measure on \(\{1,2\}\), let \(g(1)=2i\) and \(g(2)=1\). Find \(\|T_g\|\) and a unit \(f\) for which \(|T_g(f)|=\|T_g\|\).
  2. Explain why \(\int fg\,d\mu\) is unchanged if \(f\) is replaced by an almost-everywhere equal representative.
  3. For \(g(x)=x\) on \((0,1)\), compute \(\|n\chi_{(1-1/n,1)}\|_1\) and its pairing with \(g\).
  4. In the lower-bound proof, why must the selected set \(A\) have finite as well as positive measure?
  5. Give the reason that the essential supremum may fail to be attained by any individual unit \(L^1\) function.