ML inequality on $|int_{gamma} e^{iaz^{2}}dz|$ such that $z=Re^{itheta},theta in [0,frac{pi}{4}]$












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On a contour defined by sector of radius $R$ making an angle of $frac{pi}{4}$, I applied the ML inequality on the curvy(angular) part ofcontour and this is what i found $|int_{gamma} e^{iaz^{2}}dz|leqfrac{pi R}{4}$ since $|f(z)|leq 1$ and $L=frac{pi R}{4}$



But this doesn't seem right as $lim_{Rtoinfty}frac{pi R}{4}=infty$,even though I know that it should go to zero.



I am evaluating the fresnel integrals using this.










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    0












    $begingroup$


    On a contour defined by sector of radius $R$ making an angle of $frac{pi}{4}$, I applied the ML inequality on the curvy(angular) part ofcontour and this is what i found $|int_{gamma} e^{iaz^{2}}dz|leqfrac{pi R}{4}$ since $|f(z)|leq 1$ and $L=frac{pi R}{4}$



    But this doesn't seem right as $lim_{Rtoinfty}frac{pi R}{4}=infty$,even though I know that it should go to zero.



    I am evaluating the fresnel integrals using this.










    share|cite|improve this question











    $endgroup$















      0












      0








      0





      $begingroup$


      On a contour defined by sector of radius $R$ making an angle of $frac{pi}{4}$, I applied the ML inequality on the curvy(angular) part ofcontour and this is what i found $|int_{gamma} e^{iaz^{2}}dz|leqfrac{pi R}{4}$ since $|f(z)|leq 1$ and $L=frac{pi R}{4}$



      But this doesn't seem right as $lim_{Rtoinfty}frac{pi R}{4}=infty$,even though I know that it should go to zero.



      I am evaluating the fresnel integrals using this.










      share|cite|improve this question











      $endgroup$




      On a contour defined by sector of radius $R$ making an angle of $frac{pi}{4}$, I applied the ML inequality on the curvy(angular) part ofcontour and this is what i found $|int_{gamma} e^{iaz^{2}}dz|leqfrac{pi R}{4}$ since $|f(z)|leq 1$ and $L=frac{pi R}{4}$



      But this doesn't seem right as $lim_{Rtoinfty}frac{pi R}{4}=infty$,even though I know that it should go to zero.



      I am evaluating the fresnel integrals using this.







      complex-analysis contour-integration






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      share|cite|improve this question













      share|cite|improve this question




      share|cite|improve this question








      edited Jan 28 at 13:25









      Dylan

      14.2k31127




      14.2k31127










      asked Jan 28 at 9:29









      ben tenysonben tenyson

      414




      414






















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          $begingroup$

          Note that



          $$ leftvert int_{gamma} e^{iaz^2} dz rightvert le int_{gamma} leftvert e^{iaz^2} rightvert leftvert dz rightvert = int_0^{pi/4} e^{-aR^2sin 2theta} R dtheta $$



          You can show geometrically that on $theta in [0,pi/4]$, the function $g(theta) = sin 2theta$ lies completely above its secant line, i.e.



          $$ sin 2theta ge frac{4}{pi}theta implies e^{-aR^2sin2theta} le e^{-4aR^2 theta /pi} $$



          Hence, the integral is bounded above by



          $$ int_0^{pi/4} e^{-4aR^2 theta /pi} R dtheta = frac{pi}{4aR}left(1 - e^{-aR^2}right) $$



          which tends to $0$ as $R to infty$






          share|cite|improve this answer









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            $begingroup$

            Note that



            $$ leftvert int_{gamma} e^{iaz^2} dz rightvert le int_{gamma} leftvert e^{iaz^2} rightvert leftvert dz rightvert = int_0^{pi/4} e^{-aR^2sin 2theta} R dtheta $$



            You can show geometrically that on $theta in [0,pi/4]$, the function $g(theta) = sin 2theta$ lies completely above its secant line, i.e.



            $$ sin 2theta ge frac{4}{pi}theta implies e^{-aR^2sin2theta} le e^{-4aR^2 theta /pi} $$



            Hence, the integral is bounded above by



            $$ int_0^{pi/4} e^{-4aR^2 theta /pi} R dtheta = frac{pi}{4aR}left(1 - e^{-aR^2}right) $$



            which tends to $0$ as $R to infty$






            share|cite|improve this answer









            $endgroup$


















              0












              $begingroup$

              Note that



              $$ leftvert int_{gamma} e^{iaz^2} dz rightvert le int_{gamma} leftvert e^{iaz^2} rightvert leftvert dz rightvert = int_0^{pi/4} e^{-aR^2sin 2theta} R dtheta $$



              You can show geometrically that on $theta in [0,pi/4]$, the function $g(theta) = sin 2theta$ lies completely above its secant line, i.e.



              $$ sin 2theta ge frac{4}{pi}theta implies e^{-aR^2sin2theta} le e^{-4aR^2 theta /pi} $$



              Hence, the integral is bounded above by



              $$ int_0^{pi/4} e^{-4aR^2 theta /pi} R dtheta = frac{pi}{4aR}left(1 - e^{-aR^2}right) $$



              which tends to $0$ as $R to infty$






              share|cite|improve this answer









              $endgroup$
















                0












                0








                0





                $begingroup$

                Note that



                $$ leftvert int_{gamma} e^{iaz^2} dz rightvert le int_{gamma} leftvert e^{iaz^2} rightvert leftvert dz rightvert = int_0^{pi/4} e^{-aR^2sin 2theta} R dtheta $$



                You can show geometrically that on $theta in [0,pi/4]$, the function $g(theta) = sin 2theta$ lies completely above its secant line, i.e.



                $$ sin 2theta ge frac{4}{pi}theta implies e^{-aR^2sin2theta} le e^{-4aR^2 theta /pi} $$



                Hence, the integral is bounded above by



                $$ int_0^{pi/4} e^{-4aR^2 theta /pi} R dtheta = frac{pi}{4aR}left(1 - e^{-aR^2}right) $$



                which tends to $0$ as $R to infty$






                share|cite|improve this answer









                $endgroup$



                Note that



                $$ leftvert int_{gamma} e^{iaz^2} dz rightvert le int_{gamma} leftvert e^{iaz^2} rightvert leftvert dz rightvert = int_0^{pi/4} e^{-aR^2sin 2theta} R dtheta $$



                You can show geometrically that on $theta in [0,pi/4]$, the function $g(theta) = sin 2theta$ lies completely above its secant line, i.e.



                $$ sin 2theta ge frac{4}{pi}theta implies e^{-aR^2sin2theta} le e^{-4aR^2 theta /pi} $$



                Hence, the integral is bounded above by



                $$ int_0^{pi/4} e^{-4aR^2 theta /pi} R dtheta = frac{pi}{4aR}left(1 - e^{-aR^2}right) $$



                which tends to $0$ as $R to infty$







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Jan 28 at 13:33









                DylanDylan

                14.2k31127




                14.2k31127






























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