How does the following hold?












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For a vector valued function $f(t)in{L_{2}}~[0,infty)$ with Laplace transform of $f(t)$ being $F(s)$, how to show that the following holds:



$dfrac{1}{2pi}int_{-infty}^{infty}|F(jomega)|^2~domega=int_{0}^{infty}|f(t)|^2~dt$.



I know this directly follows from Perseval's identity but is there any other way to prove the claim using the definition of Laplace transformation $$F(s)=int_{0}^{infty}f(t)e^{-st}dt.$$



Any hint is greatly appreciated.










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$endgroup$

















    0












    $begingroup$


    For a vector valued function $f(t)in{L_{2}}~[0,infty)$ with Laplace transform of $f(t)$ being $F(s)$, how to show that the following holds:



    $dfrac{1}{2pi}int_{-infty}^{infty}|F(jomega)|^2~domega=int_{0}^{infty}|f(t)|^2~dt$.



    I know this directly follows from Perseval's identity but is there any other way to prove the claim using the definition of Laplace transformation $$F(s)=int_{0}^{infty}f(t)e^{-st}dt.$$



    Any hint is greatly appreciated.










    share|cite|improve this question









    $endgroup$















      0












      0








      0





      $begingroup$


      For a vector valued function $f(t)in{L_{2}}~[0,infty)$ with Laplace transform of $f(t)$ being $F(s)$, how to show that the following holds:



      $dfrac{1}{2pi}int_{-infty}^{infty}|F(jomega)|^2~domega=int_{0}^{infty}|f(t)|^2~dt$.



      I know this directly follows from Perseval's identity but is there any other way to prove the claim using the definition of Laplace transformation $$F(s)=int_{0}^{infty}f(t)e^{-st}dt.$$



      Any hint is greatly appreciated.










      share|cite|improve this question









      $endgroup$




      For a vector valued function $f(t)in{L_{2}}~[0,infty)$ with Laplace transform of $f(t)$ being $F(s)$, how to show that the following holds:



      $dfrac{1}{2pi}int_{-infty}^{infty}|F(jomega)|^2~domega=int_{0}^{infty}|f(t)|^2~dt$.



      I know this directly follows from Perseval's identity but is there any other way to prove the claim using the definition of Laplace transformation $$F(s)=int_{0}^{infty}f(t)e^{-st}dt.$$



      Any hint is greatly appreciated.







      norm laplace-transform fourier-transform






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      share|cite|improve this question










      asked Dec 10 '18 at 23:54









      jbgujgujbgujgu

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