integration with respect to non-canonical simple functionsIntegration of non-negative functionsIntegral of...

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integration with respect to non-canonical simple functions


Integration of non-negative functionsIntegral of simple functions in standard and non-standard representationRepresentations of Simple FunctionsSubclasses of simple functions dense in $L^2$If $mu$ is $sigma$-finite, then there exist increasing simple functions $s_n rightarrow f$ with $mu({x:s_n neq 0})< infty$Real Analysis, Folland Proposition 2.13 Integration of Nonnegative Functionsprove Lesbesgue Integration definition for simple function is well definedFinite sigma-algebra; integrating a non-simple function.Simple question on simple functions: interpreting the sum signA simple function and its canonical form.













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$begingroup$


I am currently reading Rudin. Rudin defines integration of simple functions as follows:



Let $phi : X rightarrow mathbb{R}$ be a nonnegative simple function with the canonical representation:



$$phi = Sigma_{j = 0}^n c_j chi_{E_j}$$



Recall given a simple function $phi : X rightarrow mathbb{R}$. We have the following canonical representation:



$$phi = Sigma_{j = 0}^n c_j chi_{E_j}$$



$$c_j: text{ are distinct}$$
$$c_0 = 0, text{ and }, E_j = phi^{-1}({c_j})$$



Define integral of $phi$ as follows:



$$int{ phi } = int{ phi d mu} := Sigma_{j = 0}^n c_j mu(E_j)$$



What I am trying to prove is integration with respect to non-canonical representation:



For a nonnegative simple function $phi = Sigma_{j = 1}^m a_k chi_{A_k}$, then



$$int{ phi mu} = Sigma_{k = 1}^m a_k dmu(A_k)$$



My work:



I will first do it for the case when $A_m$ are disjoint. Set $A_0 = (A_1 cup ldots cup A_k)^{c}$ together with $a_0 := 0 $.



$int phi dmu = Sigma c_j chi_{E_j} = Sigma c_j mu(E_j) = Sigma c_j Sigma mu(E_j cap A_k) = Sigma c_j mu(A_k)$. The last step is by interchanging the sum as we are dealing with finite summation.



If we write $phi = Sigma a_k chi_{A_k}$. If we apply the same trick as above we arrive at the following formula:



$$Sigma a_i u(A_k) = Sigma a_i u(E_k).$$



By uniqueness of the $c_j$ we must have that $c_j = a_i$. Completing the proof.



Now we prove it for general $A^{prime}_m$. We can form disjoint set $A_m$ such that:



$$bigcup A_m = bigcup A^{prime}_m$$



By the result we proved $int(phi dmu) = Sigma a_k mu(A_k) = Sigma a_k mu(A_k)$ by invoking the following properties of measure $mu(A_1 cup A_2) = mu(A_1) +mu(A_2)$.










share|cite|improve this question









$endgroup$

















    0












    $begingroup$


    I am currently reading Rudin. Rudin defines integration of simple functions as follows:



    Let $phi : X rightarrow mathbb{R}$ be a nonnegative simple function with the canonical representation:



    $$phi = Sigma_{j = 0}^n c_j chi_{E_j}$$



    Recall given a simple function $phi : X rightarrow mathbb{R}$. We have the following canonical representation:



    $$phi = Sigma_{j = 0}^n c_j chi_{E_j}$$



    $$c_j: text{ are distinct}$$
    $$c_0 = 0, text{ and }, E_j = phi^{-1}({c_j})$$



    Define integral of $phi$ as follows:



    $$int{ phi } = int{ phi d mu} := Sigma_{j = 0}^n c_j mu(E_j)$$



    What I am trying to prove is integration with respect to non-canonical representation:



    For a nonnegative simple function $phi = Sigma_{j = 1}^m a_k chi_{A_k}$, then



    $$int{ phi mu} = Sigma_{k = 1}^m a_k dmu(A_k)$$



    My work:



    I will first do it for the case when $A_m$ are disjoint. Set $A_0 = (A_1 cup ldots cup A_k)^{c}$ together with $a_0 := 0 $.



    $int phi dmu = Sigma c_j chi_{E_j} = Sigma c_j mu(E_j) = Sigma c_j Sigma mu(E_j cap A_k) = Sigma c_j mu(A_k)$. The last step is by interchanging the sum as we are dealing with finite summation.



    If we write $phi = Sigma a_k chi_{A_k}$. If we apply the same trick as above we arrive at the following formula:



    $$Sigma a_i u(A_k) = Sigma a_i u(E_k).$$



    By uniqueness of the $c_j$ we must have that $c_j = a_i$. Completing the proof.



    Now we prove it for general $A^{prime}_m$. We can form disjoint set $A_m$ such that:



    $$bigcup A_m = bigcup A^{prime}_m$$



    By the result we proved $int(phi dmu) = Sigma a_k mu(A_k) = Sigma a_k mu(A_k)$ by invoking the following properties of measure $mu(A_1 cup A_2) = mu(A_1) +mu(A_2)$.










    share|cite|improve this question









    $endgroup$















      0












      0








      0





      $begingroup$


      I am currently reading Rudin. Rudin defines integration of simple functions as follows:



      Let $phi : X rightarrow mathbb{R}$ be a nonnegative simple function with the canonical representation:



      $$phi = Sigma_{j = 0}^n c_j chi_{E_j}$$



      Recall given a simple function $phi : X rightarrow mathbb{R}$. We have the following canonical representation:



      $$phi = Sigma_{j = 0}^n c_j chi_{E_j}$$



      $$c_j: text{ are distinct}$$
      $$c_0 = 0, text{ and }, E_j = phi^{-1}({c_j})$$



      Define integral of $phi$ as follows:



      $$int{ phi } = int{ phi d mu} := Sigma_{j = 0}^n c_j mu(E_j)$$



      What I am trying to prove is integration with respect to non-canonical representation:



      For a nonnegative simple function $phi = Sigma_{j = 1}^m a_k chi_{A_k}$, then



      $$int{ phi mu} = Sigma_{k = 1}^m a_k dmu(A_k)$$



      My work:



      I will first do it for the case when $A_m$ are disjoint. Set $A_0 = (A_1 cup ldots cup A_k)^{c}$ together with $a_0 := 0 $.



      $int phi dmu = Sigma c_j chi_{E_j} = Sigma c_j mu(E_j) = Sigma c_j Sigma mu(E_j cap A_k) = Sigma c_j mu(A_k)$. The last step is by interchanging the sum as we are dealing with finite summation.



      If we write $phi = Sigma a_k chi_{A_k}$. If we apply the same trick as above we arrive at the following formula:



      $$Sigma a_i u(A_k) = Sigma a_i u(E_k).$$



      By uniqueness of the $c_j$ we must have that $c_j = a_i$. Completing the proof.



      Now we prove it for general $A^{prime}_m$. We can form disjoint set $A_m$ such that:



      $$bigcup A_m = bigcup A^{prime}_m$$



      By the result we proved $int(phi dmu) = Sigma a_k mu(A_k) = Sigma a_k mu(A_k)$ by invoking the following properties of measure $mu(A_1 cup A_2) = mu(A_1) +mu(A_2)$.










      share|cite|improve this question









      $endgroup$




      I am currently reading Rudin. Rudin defines integration of simple functions as follows:



      Let $phi : X rightarrow mathbb{R}$ be a nonnegative simple function with the canonical representation:



      $$phi = Sigma_{j = 0}^n c_j chi_{E_j}$$



      Recall given a simple function $phi : X rightarrow mathbb{R}$. We have the following canonical representation:



      $$phi = Sigma_{j = 0}^n c_j chi_{E_j}$$



      $$c_j: text{ are distinct}$$
      $$c_0 = 0, text{ and }, E_j = phi^{-1}({c_j})$$



      Define integral of $phi$ as follows:



      $$int{ phi } = int{ phi d mu} := Sigma_{j = 0}^n c_j mu(E_j)$$



      What I am trying to prove is integration with respect to non-canonical representation:



      For a nonnegative simple function $phi = Sigma_{j = 1}^m a_k chi_{A_k}$, then



      $$int{ phi mu} = Sigma_{k = 1}^m a_k dmu(A_k)$$



      My work:



      I will first do it for the case when $A_m$ are disjoint. Set $A_0 = (A_1 cup ldots cup A_k)^{c}$ together with $a_0 := 0 $.



      $int phi dmu = Sigma c_j chi_{E_j} = Sigma c_j mu(E_j) = Sigma c_j Sigma mu(E_j cap A_k) = Sigma c_j mu(A_k)$. The last step is by interchanging the sum as we are dealing with finite summation.



      If we write $phi = Sigma a_k chi_{A_k}$. If we apply the same trick as above we arrive at the following formula:



      $$Sigma a_i u(A_k) = Sigma a_i u(E_k).$$



      By uniqueness of the $c_j$ we must have that $c_j = a_i$. Completing the proof.



      Now we prove it for general $A^{prime}_m$. We can form disjoint set $A_m$ such that:



      $$bigcup A_m = bigcup A^{prime}_m$$



      By the result we proved $int(phi dmu) = Sigma a_k mu(A_k) = Sigma a_k mu(A_k)$ by invoking the following properties of measure $mu(A_1 cup A_2) = mu(A_1) +mu(A_2)$.







      measure-theory






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