function is not Lebesgue integrable











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How to prove that $f(x)=2xsin(frac{1}{x^2})-frac{2}{x}cos(frac{1}{x^2})$ on if $xneq0$ and $f(x)=0$ if $x=0$ is not Lebesgue-integrable on $[-1,1]$? I think the reason is, that $frac{2}{x}$ is part of the function Showing that $1/x$ is NOT Lebesgue Integrable on $(0,1]$.



I tried to construct step functions using the step function for $1/x$ on $(0,1]$: Let $lfloor wrfloor$ be the greatest integer less than or equal to $w$. Then the function
$$xmapsto begin{cases} lfloor 2/xrfloor & text{if } lfloor 1/xrfloorle n \[8pt]
n & text{otherwise} end{cases}$$
is simple. It is $le 2/x$ and its integral over $(0,1]$ approaches $infty$ as $ntoinfty$.



Now with the upper gaussian brackets and using that $-1le sin(frac{1}{x^2}),cos(frac{1}{x^2})le 1$. But I don't get it










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  • It's worth commenting that this thing integrates to $x^2 sin x^{-2}$, and is Riemann integrable ...
    – Richard Martin
    Nov 21 at 15:43












  • The problem with the Lebesgue integral is the wild oscillation of $f'$ near zero.
    – Richard Martin
    Nov 21 at 15:45















up vote
1
down vote

favorite












How to prove that $f(x)=2xsin(frac{1}{x^2})-frac{2}{x}cos(frac{1}{x^2})$ on if $xneq0$ and $f(x)=0$ if $x=0$ is not Lebesgue-integrable on $[-1,1]$? I think the reason is, that $frac{2}{x}$ is part of the function Showing that $1/x$ is NOT Lebesgue Integrable on $(0,1]$.



I tried to construct step functions using the step function for $1/x$ on $(0,1]$: Let $lfloor wrfloor$ be the greatest integer less than or equal to $w$. Then the function
$$xmapsto begin{cases} lfloor 2/xrfloor & text{if } lfloor 1/xrfloorle n \[8pt]
n & text{otherwise} end{cases}$$
is simple. It is $le 2/x$ and its integral over $(0,1]$ approaches $infty$ as $ntoinfty$.



Now with the upper gaussian brackets and using that $-1le sin(frac{1}{x^2}),cos(frac{1}{x^2})le 1$. But I don't get it










share|cite|improve this question
























  • It's worth commenting that this thing integrates to $x^2 sin x^{-2}$, and is Riemann integrable ...
    – Richard Martin
    Nov 21 at 15:43












  • The problem with the Lebesgue integral is the wild oscillation of $f'$ near zero.
    – Richard Martin
    Nov 21 at 15:45













up vote
1
down vote

favorite









up vote
1
down vote

favorite











How to prove that $f(x)=2xsin(frac{1}{x^2})-frac{2}{x}cos(frac{1}{x^2})$ on if $xneq0$ and $f(x)=0$ if $x=0$ is not Lebesgue-integrable on $[-1,1]$? I think the reason is, that $frac{2}{x}$ is part of the function Showing that $1/x$ is NOT Lebesgue Integrable on $(0,1]$.



I tried to construct step functions using the step function for $1/x$ on $(0,1]$: Let $lfloor wrfloor$ be the greatest integer less than or equal to $w$. Then the function
$$xmapsto begin{cases} lfloor 2/xrfloor & text{if } lfloor 1/xrfloorle n \[8pt]
n & text{otherwise} end{cases}$$
is simple. It is $le 2/x$ and its integral over $(0,1]$ approaches $infty$ as $ntoinfty$.



Now with the upper gaussian brackets and using that $-1le sin(frac{1}{x^2}),cos(frac{1}{x^2})le 1$. But I don't get it










share|cite|improve this question















How to prove that $f(x)=2xsin(frac{1}{x^2})-frac{2}{x}cos(frac{1}{x^2})$ on if $xneq0$ and $f(x)=0$ if $x=0$ is not Lebesgue-integrable on $[-1,1]$? I think the reason is, that $frac{2}{x}$ is part of the function Showing that $1/x$ is NOT Lebesgue Integrable on $(0,1]$.



I tried to construct step functions using the step function for $1/x$ on $(0,1]$: Let $lfloor wrfloor$ be the greatest integer less than or equal to $w$. Then the function
$$xmapsto begin{cases} lfloor 2/xrfloor & text{if } lfloor 1/xrfloorle n \[8pt]
n & text{otherwise} end{cases}$$
is simple. It is $le 2/x$ and its integral over $(0,1]$ approaches $infty$ as $ntoinfty$.



Now with the upper gaussian brackets and using that $-1le sin(frac{1}{x^2}),cos(frac{1}{x^2})le 1$. But I don't get it







analysis measure-theory lebesgue-integral






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edited Nov 21 at 15:32









Tianlalu

2,9901936




2,9901936










asked Nov 21 at 15:31









Gero

23319




23319












  • It's worth commenting that this thing integrates to $x^2 sin x^{-2}$, and is Riemann integrable ...
    – Richard Martin
    Nov 21 at 15:43












  • The problem with the Lebesgue integral is the wild oscillation of $f'$ near zero.
    – Richard Martin
    Nov 21 at 15:45


















  • It's worth commenting that this thing integrates to $x^2 sin x^{-2}$, and is Riemann integrable ...
    – Richard Martin
    Nov 21 at 15:43












  • The problem with the Lebesgue integral is the wild oscillation of $f'$ near zero.
    – Richard Martin
    Nov 21 at 15:45
















It's worth commenting that this thing integrates to $x^2 sin x^{-2}$, and is Riemann integrable ...
– Richard Martin
Nov 21 at 15:43






It's worth commenting that this thing integrates to $x^2 sin x^{-2}$, and is Riemann integrable ...
– Richard Martin
Nov 21 at 15:43














The problem with the Lebesgue integral is the wild oscillation of $f'$ near zero.
– Richard Martin
Nov 21 at 15:45




The problem with the Lebesgue integral is the wild oscillation of $f'$ near zero.
– Richard Martin
Nov 21 at 15:45










2 Answers
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The precise meaning that a function $f$ is Lebesgue integrable on some measurable set $E$ is that both positive and negative parts, $f^+(x) = max(f(x),0)$ and $f^-(x) = max(-f(x),0)$, must have finite-valued integrals



$$int_E f^+ < +infty, ,, int_E f^- < +infty$$



Since $f^+$ and $f^-$ are nonnegative and $|f| = f^+ +f^-$, Lebesgue integrability requires that $int_E|f| < +infty$.



In this case there is no problem with $x mapsto 2xsinfrac{1}{x^2}$ as this can be continuously extended at $0$ and so is both Riemann and Lebesgue integrable on $[0,1]$ and $[-1,0]$. Recall that a bounded function that is Riemann integrable on a bounded interval is always Lebesgue integrable.



On the other hand, $x mapsto frac{2}{x} cos frac{1}{x^2}$ is not Lebesgue integrable on $[0,1]$. If it were we could apply the change-of-variables $x to frac{1}{sqrt{t}}$ and have



$$int_1^infty frac{|cos t|}{t} , dt = int_0^1 frac{2}{x} left|cos frac{1}{x^2}right| , dx < +infty$$



However,



$$int_1^infty frac{|cos t|}{t} , dt > sum_{k=1}^inftyint_{kpi}^{kpi + pi} frac{|cos t|}{t} , dt > sum_{k=1}^infty frac{1}{kpi +pi}int_{kpi}^{kpi + pi} |cos t| , dt = frac{2}{pi}sum_{k=1}^{infty} frac{1}{k+1} \ = +infty $$



since the harmonic series on the RHS is divergent.



Note that the improper (Riemann) integral, without the absolute value present,



$$int_0^1 frac{2}{x} cos frac{1}{x^2} , dx $$



is convergent, but this does not enforce Lebesgue integrability.






share|cite|improve this answer






























    up vote
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    The derivative of $F(x)= x^2 sin (1/x^2)$ if $f$, except at $x=0$, where the former is zero and the latter is not defined.



    Now if $f$ were integrable, then $F$ would be absolutely continuous.



    We show that this is not the case.



    For $j=1,2,dots$ let $a_j= frac{1}{sqrt{pi j}}$ and $b_j = frac{1}{sqrt{pi( j + 1/2)}}$.



    Then $F(a_j)=0$ and $F(b_j)=pi (j+1/2)$.



    To conclude, for any $j_1$:





    • $sum_{j>j_1}| a_j - b_j| < a_{j_1}to 0$ as $j_1toinfty$, while


    • $sum_{j>j_1} |F(a_j)-F(b_j)| = sum_{j>j_1} pi (j+1/2)= infty$.






    share|cite|improve this answer





















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      The precise meaning that a function $f$ is Lebesgue integrable on some measurable set $E$ is that both positive and negative parts, $f^+(x) = max(f(x),0)$ and $f^-(x) = max(-f(x),0)$, must have finite-valued integrals



      $$int_E f^+ < +infty, ,, int_E f^- < +infty$$



      Since $f^+$ and $f^-$ are nonnegative and $|f| = f^+ +f^-$, Lebesgue integrability requires that $int_E|f| < +infty$.



      In this case there is no problem with $x mapsto 2xsinfrac{1}{x^2}$ as this can be continuously extended at $0$ and so is both Riemann and Lebesgue integrable on $[0,1]$ and $[-1,0]$. Recall that a bounded function that is Riemann integrable on a bounded interval is always Lebesgue integrable.



      On the other hand, $x mapsto frac{2}{x} cos frac{1}{x^2}$ is not Lebesgue integrable on $[0,1]$. If it were we could apply the change-of-variables $x to frac{1}{sqrt{t}}$ and have



      $$int_1^infty frac{|cos t|}{t} , dt = int_0^1 frac{2}{x} left|cos frac{1}{x^2}right| , dx < +infty$$



      However,



      $$int_1^infty frac{|cos t|}{t} , dt > sum_{k=1}^inftyint_{kpi}^{kpi + pi} frac{|cos t|}{t} , dt > sum_{k=1}^infty frac{1}{kpi +pi}int_{kpi}^{kpi + pi} |cos t| , dt = frac{2}{pi}sum_{k=1}^{infty} frac{1}{k+1} \ = +infty $$



      since the harmonic series on the RHS is divergent.



      Note that the improper (Riemann) integral, without the absolute value present,



      $$int_0^1 frac{2}{x} cos frac{1}{x^2} , dx $$



      is convergent, but this does not enforce Lebesgue integrability.






      share|cite|improve this answer



























        up vote
        3
        down vote



        accepted










        The precise meaning that a function $f$ is Lebesgue integrable on some measurable set $E$ is that both positive and negative parts, $f^+(x) = max(f(x),0)$ and $f^-(x) = max(-f(x),0)$, must have finite-valued integrals



        $$int_E f^+ < +infty, ,, int_E f^- < +infty$$



        Since $f^+$ and $f^-$ are nonnegative and $|f| = f^+ +f^-$, Lebesgue integrability requires that $int_E|f| < +infty$.



        In this case there is no problem with $x mapsto 2xsinfrac{1}{x^2}$ as this can be continuously extended at $0$ and so is both Riemann and Lebesgue integrable on $[0,1]$ and $[-1,0]$. Recall that a bounded function that is Riemann integrable on a bounded interval is always Lebesgue integrable.



        On the other hand, $x mapsto frac{2}{x} cos frac{1}{x^2}$ is not Lebesgue integrable on $[0,1]$. If it were we could apply the change-of-variables $x to frac{1}{sqrt{t}}$ and have



        $$int_1^infty frac{|cos t|}{t} , dt = int_0^1 frac{2}{x} left|cos frac{1}{x^2}right| , dx < +infty$$



        However,



        $$int_1^infty frac{|cos t|}{t} , dt > sum_{k=1}^inftyint_{kpi}^{kpi + pi} frac{|cos t|}{t} , dt > sum_{k=1}^infty frac{1}{kpi +pi}int_{kpi}^{kpi + pi} |cos t| , dt = frac{2}{pi}sum_{k=1}^{infty} frac{1}{k+1} \ = +infty $$



        since the harmonic series on the RHS is divergent.



        Note that the improper (Riemann) integral, without the absolute value present,



        $$int_0^1 frac{2}{x} cos frac{1}{x^2} , dx $$



        is convergent, but this does not enforce Lebesgue integrability.






        share|cite|improve this answer

























          up vote
          3
          down vote



          accepted







          up vote
          3
          down vote



          accepted






          The precise meaning that a function $f$ is Lebesgue integrable on some measurable set $E$ is that both positive and negative parts, $f^+(x) = max(f(x),0)$ and $f^-(x) = max(-f(x),0)$, must have finite-valued integrals



          $$int_E f^+ < +infty, ,, int_E f^- < +infty$$



          Since $f^+$ and $f^-$ are nonnegative and $|f| = f^+ +f^-$, Lebesgue integrability requires that $int_E|f| < +infty$.



          In this case there is no problem with $x mapsto 2xsinfrac{1}{x^2}$ as this can be continuously extended at $0$ and so is both Riemann and Lebesgue integrable on $[0,1]$ and $[-1,0]$. Recall that a bounded function that is Riemann integrable on a bounded interval is always Lebesgue integrable.



          On the other hand, $x mapsto frac{2}{x} cos frac{1}{x^2}$ is not Lebesgue integrable on $[0,1]$. If it were we could apply the change-of-variables $x to frac{1}{sqrt{t}}$ and have



          $$int_1^infty frac{|cos t|}{t} , dt = int_0^1 frac{2}{x} left|cos frac{1}{x^2}right| , dx < +infty$$



          However,



          $$int_1^infty frac{|cos t|}{t} , dt > sum_{k=1}^inftyint_{kpi}^{kpi + pi} frac{|cos t|}{t} , dt > sum_{k=1}^infty frac{1}{kpi +pi}int_{kpi}^{kpi + pi} |cos t| , dt = frac{2}{pi}sum_{k=1}^{infty} frac{1}{k+1} \ = +infty $$



          since the harmonic series on the RHS is divergent.



          Note that the improper (Riemann) integral, without the absolute value present,



          $$int_0^1 frac{2}{x} cos frac{1}{x^2} , dx $$



          is convergent, but this does not enforce Lebesgue integrability.






          share|cite|improve this answer














          The precise meaning that a function $f$ is Lebesgue integrable on some measurable set $E$ is that both positive and negative parts, $f^+(x) = max(f(x),0)$ and $f^-(x) = max(-f(x),0)$, must have finite-valued integrals



          $$int_E f^+ < +infty, ,, int_E f^- < +infty$$



          Since $f^+$ and $f^-$ are nonnegative and $|f| = f^+ +f^-$, Lebesgue integrability requires that $int_E|f| < +infty$.



          In this case there is no problem with $x mapsto 2xsinfrac{1}{x^2}$ as this can be continuously extended at $0$ and so is both Riemann and Lebesgue integrable on $[0,1]$ and $[-1,0]$. Recall that a bounded function that is Riemann integrable on a bounded interval is always Lebesgue integrable.



          On the other hand, $x mapsto frac{2}{x} cos frac{1}{x^2}$ is not Lebesgue integrable on $[0,1]$. If it were we could apply the change-of-variables $x to frac{1}{sqrt{t}}$ and have



          $$int_1^infty frac{|cos t|}{t} , dt = int_0^1 frac{2}{x} left|cos frac{1}{x^2}right| , dx < +infty$$



          However,



          $$int_1^infty frac{|cos t|}{t} , dt > sum_{k=1}^inftyint_{kpi}^{kpi + pi} frac{|cos t|}{t} , dt > sum_{k=1}^infty frac{1}{kpi +pi}int_{kpi}^{kpi + pi} |cos t| , dt = frac{2}{pi}sum_{k=1}^{infty} frac{1}{k+1} \ = +infty $$



          since the harmonic series on the RHS is divergent.



          Note that the improper (Riemann) integral, without the absolute value present,



          $$int_0^1 frac{2}{x} cos frac{1}{x^2} , dx $$



          is convergent, but this does not enforce Lebesgue integrability.







          share|cite|improve this answer














          share|cite|improve this answer



          share|cite|improve this answer








          edited Nov 22 at 1:45

























          answered Nov 22 at 1:40









          RRL

          48.1k42573




          48.1k42573






















              up vote
              2
              down vote













              The derivative of $F(x)= x^2 sin (1/x^2)$ if $f$, except at $x=0$, where the former is zero and the latter is not defined.



              Now if $f$ were integrable, then $F$ would be absolutely continuous.



              We show that this is not the case.



              For $j=1,2,dots$ let $a_j= frac{1}{sqrt{pi j}}$ and $b_j = frac{1}{sqrt{pi( j + 1/2)}}$.



              Then $F(a_j)=0$ and $F(b_j)=pi (j+1/2)$.



              To conclude, for any $j_1$:





              • $sum_{j>j_1}| a_j - b_j| < a_{j_1}to 0$ as $j_1toinfty$, while


              • $sum_{j>j_1} |F(a_j)-F(b_j)| = sum_{j>j_1} pi (j+1/2)= infty$.






              share|cite|improve this answer

























                up vote
                2
                down vote













                The derivative of $F(x)= x^2 sin (1/x^2)$ if $f$, except at $x=0$, where the former is zero and the latter is not defined.



                Now if $f$ were integrable, then $F$ would be absolutely continuous.



                We show that this is not the case.



                For $j=1,2,dots$ let $a_j= frac{1}{sqrt{pi j}}$ and $b_j = frac{1}{sqrt{pi( j + 1/2)}}$.



                Then $F(a_j)=0$ and $F(b_j)=pi (j+1/2)$.



                To conclude, for any $j_1$:





                • $sum_{j>j_1}| a_j - b_j| < a_{j_1}to 0$ as $j_1toinfty$, while


                • $sum_{j>j_1} |F(a_j)-F(b_j)| = sum_{j>j_1} pi (j+1/2)= infty$.






                share|cite|improve this answer























                  up vote
                  2
                  down vote










                  up vote
                  2
                  down vote









                  The derivative of $F(x)= x^2 sin (1/x^2)$ if $f$, except at $x=0$, where the former is zero and the latter is not defined.



                  Now if $f$ were integrable, then $F$ would be absolutely continuous.



                  We show that this is not the case.



                  For $j=1,2,dots$ let $a_j= frac{1}{sqrt{pi j}}$ and $b_j = frac{1}{sqrt{pi( j + 1/2)}}$.



                  Then $F(a_j)=0$ and $F(b_j)=pi (j+1/2)$.



                  To conclude, for any $j_1$:





                  • $sum_{j>j_1}| a_j - b_j| < a_{j_1}to 0$ as $j_1toinfty$, while


                  • $sum_{j>j_1} |F(a_j)-F(b_j)| = sum_{j>j_1} pi (j+1/2)= infty$.






                  share|cite|improve this answer












                  The derivative of $F(x)= x^2 sin (1/x^2)$ if $f$, except at $x=0$, where the former is zero and the latter is not defined.



                  Now if $f$ were integrable, then $F$ would be absolutely continuous.



                  We show that this is not the case.



                  For $j=1,2,dots$ let $a_j= frac{1}{sqrt{pi j}}$ and $b_j = frac{1}{sqrt{pi( j + 1/2)}}$.



                  Then $F(a_j)=0$ and $F(b_j)=pi (j+1/2)$.



                  To conclude, for any $j_1$:





                  • $sum_{j>j_1}| a_j - b_j| < a_{j_1}to 0$ as $j_1toinfty$, while


                  • $sum_{j>j_1} |F(a_j)-F(b_j)| = sum_{j>j_1} pi (j+1/2)= infty$.







                  share|cite|improve this answer












                  share|cite|improve this answer



                  share|cite|improve this answer










                  answered Nov 22 at 2:11









                  Fnacool

                  4,966511




                  4,966511






























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