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Unit 22: Introduction to Riemann-Stieltjes Integration, using Riemann Sums




          Then, if n and n¢ are so large that (b – a)/n <  and (b – a)/n¢ < , we have         Notes
                               mesh( ) <  and mesh( ) <   | –  | < /2.
                                     n             n¢       n   n¢
          This means (since  was arbitrary) that { } is a Cauchy sequence in our space. Thus we define
                                           n
                                    RSI :=  lim 
                                         n®¥  n
          and it remains to show that if |[a, b] then
                                mesh() <   |RS() – RSI| <.
          This is  essentially done. We choose the first n such  that mesh( ) < ,  and we suppose that
                                                               n
          mesh() < . Then
                            |RS() – RI|  |RS() –  | + |   – RSI| < /2 + /2 = ,
                                                 n     n
          since RS()—  = RS() – RS(f, ,  ,  ). The proof is complete.
                      n               n  n



             Notes Nothing is said at first about the functions f and  , beside the demand that the
             integrability definition hold.
          If f and  have a discontinuity at the same point, then the Riemann-Stieltjes integral does not
          exist.
          They also show that if the Riemann-Stieltjes integral exists, then this integration-by-parts formula
          holds:
                                 b       b
                                                  
                                                           
                                a ò  f d  = ò a   df +  f(b) (b) -  f(a) (a)
                                       -
          (in the applications have far, far back in my mind, the integral on the right would have to be
           b
              
           a ò  df , in order to keep the order of “multiplication” the same). The proof amounts to rearranging
          the  Riemann-Stieltjes sums, adding and subtracting terms in such a way that the    become
                                                                               i
          partition points and the x  become selection-vector components when 1 < i < n . There are some
                               i                                         
                                                              b
          leftovers, and these turn out to be the “boundary” term f(x)(x)| .
                                                              a
          Wheeden and  Zygmund state several properties, routine to prove, about Riemann-Stieltjes
          integrals:
                                  b
                                 a ò  f d is linear in both f and 
                                                  b                               c
          as long as all the integrals involved exist, and if  ò  f d  exists and a < c <b, then both of  ò  f d
                                                  a                               a
               b              c      b       b
          and   c ò  f d  exist, and  ò a  f d  +  ò c  f d  =  ò a  f d .
          What has been covered applies to all Riemann-Stieltjes integrals. That continuity plays a role
          has already been mentioned.
          22.5 Functions of Bounded Variation: Definition and Properties

          In what we do from now on, at least one of f and  will be a function of bounded variation, unless
          otherwise stated. We will begin by discussing real-valued functions of bounded variation. This
          material can also be found in Measure and Integral, by Wheeden and Zygmund.
          Definition: A function f: [a, b] ®  is a function of bounded variation on [a, b] if

                                           n 
                            V(f, [a, b]) := sup å|f(x ) – f(x i – 1 )| < ¥ and we say that f Î BV[a, b].
                                                i
                                        |[a,b] 1


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