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Real Analysis




                    Notes          Notation: We shall denote the set of all (real-valued) bounded measurable functions defined on
                                   E which vanishes outside a set of finite measure by B (E).
                                                                             0
                                   So from now on for f Î B (E), we have
                                                       0
                                                A ò  f =  inf { A ò   : f   Î So (E) } = sup { ò  : f   Î So (E) }
                                                                             A
                                   for any A  E.
                                   Note also that B (E) is a vector lattice, by which we mean it is a vector space partially ordered by
                                               0
                                    (such that f  g if and only if f(x)  g(x) for all x Î E) and every two elements of it (say f, g Î B (E))
                                                                                                           0
                                   have a least upper bound in it (namely f V g Î B (E)). (Why is it a least upper bound?)
                                                                          0
                                   We have the following nice proposition concerning the relationship between the Riemann and
                                   the Lebsegue integrals.
                                   Proposition: If f : [a, b]  is Riemann integrable on the closed and bounded interval [a, b], then
                                   f Î B ([a, b]) and
                                       0
                                              b
                                   (3)    ()  f =   [a, b] f,
                                                 ( )ò
                                              a ò
                                   where the () and () represents Riemann integral and Lebesgue integral respectively.
                                   Proof: Since step functions defined on closed and bounded interval [a, b] are simple and have the
                                   same Lebesgue and Riemann integral over [a, b] (why?), we see from the definitions
                                                b       b
                                          () = ò  f =  sup { a ò   : f   step on [a, b] }
                                                 a
                                           () = ò  f =  sup ò   : f    simple on [a, b] }
                                                         { [a, b]
                                                 [a, b]
                                           () = ò  f =  inf ò    : f    simple on [a, b] }
                                                 [a, b]  { [a, b]
                                                 b      b
                                          () = ò  f =  inf { a ò   : f    step on [a, b] }
                                                 a
                                   that

                                                b                     b
                                   (4)    () = ò  f ( )ò  f ( )ò  [a, b] f ( )ò  a  f
                                                 a       [a, b]
                                   whenever the four quantities exist. Now if f is Riemann integrable over [a, b], then f is bounded
                                   on [a,b].  Since [a,b] is of finite measure, we see that all four quantities in (4) exist. In that case
                                    
                                           ( )ò
                                   ( )ò  b  f =   b  f  as well so all four quantities in (4) are equal, which implies that f is measurable
                                        a       a
                                   (so f Î B ([a, b])) and (3) holds.
                                         0
                                   Proposition: Properties of the Lebesgue integral
                                   Suppose f, g Î B (E). Then f + g, af, |f|Î B (E), and for any A  E, we have
                                                0                     0
                                   (a)  A ò  (f g) =  A ò  f  A ò +  g
                                           +
                                   (b)  A ò a = a  A ò  f for all a Î .
                                           f
                                             f
                                   (c)  A ò  f =  E ò  A
                                   (d)  If B  A then  f +  ò A\B f .
                                                   B ò
                                   (e)  If B  A and  f   A ò  f
                                                  B ò



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