An integral for which I don't trust WolframAlpha The Next CEO of Stack OverflowIntegral $int_0^4 int_sqrty^2 y^2 e^x^7 operatorname d!x operatorname d!y,$Holomorphic Functions and Cauchy TheoremShould it be obvious that this integral is zero?How to integrate the following? $int_0^+inftyfrac1-cos xx^alpha+1,dx$Complex integral with Residues TheoremEvaluation of integral related to Gamma functionGive a recursive formula for calculating the value of $ int_0^pi sin^n x , mathrm dx$Convergence of This integral?Function defined by Cauchy IntegralNeed verification for this integral

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An integral for which I don't trust WolframAlpha



The Next CEO of Stack OverflowIntegral $int_0^4 int_sqrty^2 y^2 e^x^7 operatorname d!x operatorname d!y,$Holomorphic Functions and Cauchy TheoremShould it be obvious that this integral is zero?How to integrate the following? $int_0^+inftyfrac1-cos xx^alpha+1,dx$Complex integral with Residues TheoremEvaluation of integral related to Gamma functionGive a recursive formula for calculating the value of $ int_0^pi sin^n x , mathrm dx$Convergence of This integral?Function defined by Cauchy IntegralNeed verification for this integral










31












$begingroup$


WolframAlpha tells me that $$int_-infty^infty e^-(t-i)^4 , mathrmdt = 0.$$ I am suspicious of this, because of the idea that for nice enough $f$, since $$int_-infty^infty f(t-a) , mathrmdt$$ is holomorphic in $a$ and takes the same value for all $a in mathbbR$, it should be independent of $a$ by the identity principle; and then $$int_-infty^infty e^-(t-i)^4 , mathrmdt = int_-infty^infty e^-t^4 , mathrmdt = 2 cdot Gamma(5/4).$$ But WolframAlpha even tells me numerically that $int_-infty^infty e^-(t-i)^4 , mathrmdt$ is close to $0$. Am I doing something wrong?










share|cite|improve this question









$endgroup$







  • 3




    $begingroup$
    The integrals are equal provided that $i$ is a real number, but it isn't.
    $endgroup$
    – WW1
    Jun 26 '17 at 3:23






  • 2




    $begingroup$
    @WW1 That shouldn't matter by the identity principle, or as User8128 suggests (essentially) the contour of integration can be shifted in the $y$ direction without changing the integral, since it only matters that it connects $mathrmRe[z] = -infty$ and $mathrmRe[z] = infty.$ I am pretty confident in either argument but I thought I would ask here just to double check. (I usually trust wolframalpha blindly so it is irritating when something strange like this turns up)
    $endgroup$
    – user457218
    Jun 26 '17 at 4:06







  • 3




    $begingroup$
    @WW1: The argument for $a=i$ isn't about making a change of variable: it's about analytic continuation.
    $endgroup$
    – Hurkyl
    Jun 26 '17 at 10:04







  • 1




    $begingroup$
    For the fun type $int_-infty^infty e^-(t-colorred1.0i)^4 ,dt $ and you will get the value !!!
    $endgroup$
    – Claude Leibovici
    Jun 26 '17 at 10:07







  • 1




    $begingroup$
    They seem to have already corrected this.
    $endgroup$
    – sophros
    Jun 26 '17 at 17:11















31












$begingroup$


WolframAlpha tells me that $$int_-infty^infty e^-(t-i)^4 , mathrmdt = 0.$$ I am suspicious of this, because of the idea that for nice enough $f$, since $$int_-infty^infty f(t-a) , mathrmdt$$ is holomorphic in $a$ and takes the same value for all $a in mathbbR$, it should be independent of $a$ by the identity principle; and then $$int_-infty^infty e^-(t-i)^4 , mathrmdt = int_-infty^infty e^-t^4 , mathrmdt = 2 cdot Gamma(5/4).$$ But WolframAlpha even tells me numerically that $int_-infty^infty e^-(t-i)^4 , mathrmdt$ is close to $0$. Am I doing something wrong?










share|cite|improve this question









$endgroup$







  • 3




    $begingroup$
    The integrals are equal provided that $i$ is a real number, but it isn't.
    $endgroup$
    – WW1
    Jun 26 '17 at 3:23






  • 2




    $begingroup$
    @WW1 That shouldn't matter by the identity principle, or as User8128 suggests (essentially) the contour of integration can be shifted in the $y$ direction without changing the integral, since it only matters that it connects $mathrmRe[z] = -infty$ and $mathrmRe[z] = infty.$ I am pretty confident in either argument but I thought I would ask here just to double check. (I usually trust wolframalpha blindly so it is irritating when something strange like this turns up)
    $endgroup$
    – user457218
    Jun 26 '17 at 4:06







  • 3




    $begingroup$
    @WW1: The argument for $a=i$ isn't about making a change of variable: it's about analytic continuation.
    $endgroup$
    – Hurkyl
    Jun 26 '17 at 10:04







  • 1




    $begingroup$
    For the fun type $int_-infty^infty e^-(t-colorred1.0i)^4 ,dt $ and you will get the value !!!
    $endgroup$
    – Claude Leibovici
    Jun 26 '17 at 10:07







  • 1




    $begingroup$
    They seem to have already corrected this.
    $endgroup$
    – sophros
    Jun 26 '17 at 17:11













31












31








31


6



$begingroup$


WolframAlpha tells me that $$int_-infty^infty e^-(t-i)^4 , mathrmdt = 0.$$ I am suspicious of this, because of the idea that for nice enough $f$, since $$int_-infty^infty f(t-a) , mathrmdt$$ is holomorphic in $a$ and takes the same value for all $a in mathbbR$, it should be independent of $a$ by the identity principle; and then $$int_-infty^infty e^-(t-i)^4 , mathrmdt = int_-infty^infty e^-t^4 , mathrmdt = 2 cdot Gamma(5/4).$$ But WolframAlpha even tells me numerically that $int_-infty^infty e^-(t-i)^4 , mathrmdt$ is close to $0$. Am I doing something wrong?










share|cite|improve this question









$endgroup$




WolframAlpha tells me that $$int_-infty^infty e^-(t-i)^4 , mathrmdt = 0.$$ I am suspicious of this, because of the idea that for nice enough $f$, since $$int_-infty^infty f(t-a) , mathrmdt$$ is holomorphic in $a$ and takes the same value for all $a in mathbbR$, it should be independent of $a$ by the identity principle; and then $$int_-infty^infty e^-(t-i)^4 , mathrmdt = int_-infty^infty e^-t^4 , mathrmdt = 2 cdot Gamma(5/4).$$ But WolframAlpha even tells me numerically that $int_-infty^infty e^-(t-i)^4 , mathrmdt$ is close to $0$. Am I doing something wrong?







integration complex-analysis proof-verification






share|cite|improve this question













share|cite|improve this question











share|cite|improve this question




share|cite|improve this question










asked Jun 26 '17 at 3:01









user457218user457218

17525




17525







  • 3




    $begingroup$
    The integrals are equal provided that $i$ is a real number, but it isn't.
    $endgroup$
    – WW1
    Jun 26 '17 at 3:23






  • 2




    $begingroup$
    @WW1 That shouldn't matter by the identity principle, or as User8128 suggests (essentially) the contour of integration can be shifted in the $y$ direction without changing the integral, since it only matters that it connects $mathrmRe[z] = -infty$ and $mathrmRe[z] = infty.$ I am pretty confident in either argument but I thought I would ask here just to double check. (I usually trust wolframalpha blindly so it is irritating when something strange like this turns up)
    $endgroup$
    – user457218
    Jun 26 '17 at 4:06







  • 3




    $begingroup$
    @WW1: The argument for $a=i$ isn't about making a change of variable: it's about analytic continuation.
    $endgroup$
    – Hurkyl
    Jun 26 '17 at 10:04







  • 1




    $begingroup$
    For the fun type $int_-infty^infty e^-(t-colorred1.0i)^4 ,dt $ and you will get the value !!!
    $endgroup$
    – Claude Leibovici
    Jun 26 '17 at 10:07







  • 1




    $begingroup$
    They seem to have already corrected this.
    $endgroup$
    – sophros
    Jun 26 '17 at 17:11












  • 3




    $begingroup$
    The integrals are equal provided that $i$ is a real number, but it isn't.
    $endgroup$
    – WW1
    Jun 26 '17 at 3:23






  • 2




    $begingroup$
    @WW1 That shouldn't matter by the identity principle, or as User8128 suggests (essentially) the contour of integration can be shifted in the $y$ direction without changing the integral, since it only matters that it connects $mathrmRe[z] = -infty$ and $mathrmRe[z] = infty.$ I am pretty confident in either argument but I thought I would ask here just to double check. (I usually trust wolframalpha blindly so it is irritating when something strange like this turns up)
    $endgroup$
    – user457218
    Jun 26 '17 at 4:06







  • 3




    $begingroup$
    @WW1: The argument for $a=i$ isn't about making a change of variable: it's about analytic continuation.
    $endgroup$
    – Hurkyl
    Jun 26 '17 at 10:04







  • 1




    $begingroup$
    For the fun type $int_-infty^infty e^-(t-colorred1.0i)^4 ,dt $ and you will get the value !!!
    $endgroup$
    – Claude Leibovici
    Jun 26 '17 at 10:07







  • 1




    $begingroup$
    They seem to have already corrected this.
    $endgroup$
    – sophros
    Jun 26 '17 at 17:11







3




3




$begingroup$
The integrals are equal provided that $i$ is a real number, but it isn't.
$endgroup$
– WW1
Jun 26 '17 at 3:23




$begingroup$
The integrals are equal provided that $i$ is a real number, but it isn't.
$endgroup$
– WW1
Jun 26 '17 at 3:23




2




2




$begingroup$
@WW1 That shouldn't matter by the identity principle, or as User8128 suggests (essentially) the contour of integration can be shifted in the $y$ direction without changing the integral, since it only matters that it connects $mathrmRe[z] = -infty$ and $mathrmRe[z] = infty.$ I am pretty confident in either argument but I thought I would ask here just to double check. (I usually trust wolframalpha blindly so it is irritating when something strange like this turns up)
$endgroup$
– user457218
Jun 26 '17 at 4:06





$begingroup$
@WW1 That shouldn't matter by the identity principle, or as User8128 suggests (essentially) the contour of integration can be shifted in the $y$ direction without changing the integral, since it only matters that it connects $mathrmRe[z] = -infty$ and $mathrmRe[z] = infty.$ I am pretty confident in either argument but I thought I would ask here just to double check. (I usually trust wolframalpha blindly so it is irritating when something strange like this turns up)
$endgroup$
– user457218
Jun 26 '17 at 4:06





3




3




$begingroup$
@WW1: The argument for $a=i$ isn't about making a change of variable: it's about analytic continuation.
$endgroup$
– Hurkyl
Jun 26 '17 at 10:04





$begingroup$
@WW1: The argument for $a=i$ isn't about making a change of variable: it's about analytic continuation.
$endgroup$
– Hurkyl
Jun 26 '17 at 10:04





1




1




$begingroup$
For the fun type $int_-infty^infty e^-(t-colorred1.0i)^4 ,dt $ and you will get the value !!!
$endgroup$
– Claude Leibovici
Jun 26 '17 at 10:07





$begingroup$
For the fun type $int_-infty^infty e^-(t-colorred1.0i)^4 ,dt $ and you will get the value !!!
$endgroup$
– Claude Leibovici
Jun 26 '17 at 10:07





1




1




$begingroup$
They seem to have already corrected this.
$endgroup$
– sophros
Jun 26 '17 at 17:11




$begingroup$
They seem to have already corrected this.
$endgroup$
– sophros
Jun 26 '17 at 17:11










2 Answers
2






active

oldest

votes


















27












$begingroup$

Just as User8128 commented, I believe that you are perfectly correct.



Without changing variable and using another CAS
$$int mathrme^-(t-i)^4 , mathrmdt=colorred-frac(t-i), Gamma left(frac14,(t-i)^4right)4 sqrt[4](t-i)^4=-frac14 (t-i) E_frac34left((t-i)^4right)$$
$$int_-infty^infty mathrme^-(t-i)^4 , mathrmdt=i left(E_frac34(-4)-Releft(E_frac34(-4)right)right)$$ $$int_-infty^infty mathrme^-(t-i)^4 , mathrmdt=frac(-1)^1/4, Gamma left(frac14,-4right)sqrt2-i
Releft(-frac(-1)^3/4, Gamma left(frac14,-4right)sqrt2right)=2, Gamma left(frac54right) $$
Notice that, for the indefinite integral, Wolfram Alpha correctly reports the expression written in red.



What is interesting is that, if you ask Wolfram Alpha
$$int_0^infty mathrme^-(t-i)^4 , mathrmdt=-frac i4E_frac34(-1)$$
$$int^0_-infty mathrme^-(t-i)^4 , mathrmdt=+frac i4E_frac34(-1)$$ leading to the $0$ you obtained.



There is obviously a bug that I suggest you to report.






share|cite|improve this answer











$endgroup$








  • 3




    $begingroup$
    The bug is kind of interesting. Just below i it still works, e.g. for 0.99 i see here at 1 i it fails.
    $endgroup$
    – Jannick
    Jun 26 '17 at 9:36







  • 10




    $begingroup$
    @Jannick. Type $1.0i$ and it works !!!
    $endgroup$
    – Claude Leibovici
    Jun 26 '17 at 10:09










  • $begingroup$
    Yes true, that is really funny. For integer one it already fails but for float one it still works. For 1.01 it fails however.
    $endgroup$
    – Jannick
    Jun 26 '17 at 10:13






  • 3




    $begingroup$
    @Jannick.**Funny** may not be the most appropriate term here ! Cheers and thanks for your previous comment which made me trying $1.0i$.
    $endgroup$
    – Claude Leibovici
    Jun 26 '17 at 10:15







  • 1




    $begingroup$
    @MeniRosenfeld: The original bug does, at the least in Mathematica 9. Integrate[Exp[-(t - I)^4], t, -Infinity, Infinity] yields 0. NIntegrate with the same argument returns 1.8128 + very little i, just like what you see.
    $endgroup$
    – user22961
    Jun 26 '17 at 18:27



















14












$begingroup$

$newcommandbbx[1],bbox[15px,border:1px groove navy]displaystyle#1,
newcommandbraces[1]leftlbrace,#1,rightrbrace
newcommandbracks[1]leftlbrack,#1,rightrbrack
newcommandddmathrmd
newcommandds[1]displaystyle#1
newcommandexpo[1],mathrme^#1,
newcommandicmathrmi
newcommandmc[1]mathcal#1
newcommandmrm[1]mathrm#1
newcommandpars[1]left(,#1,right)
newcommandpartiald[3][]fracpartial^#1 #2partial #3^#1
newcommandroot[2][],sqrt[#1],#2,,
newcommandtotald[3][]fracmathrmd^#1 #2mathrmd #3^#1
newcommandverts[1]leftvert,#1,rightvert$
beginalign
int_-infty^inftyexpo-parst - ic^4dd t & =
int_0^inftybracksexpo-parst - ic^4 +
expo-pars-t - ic^4dd t =
2,Reint_0^inftyexpo-parst + ic^4dd t =
2,Reint_ic^infty + icexpo-t^4dd t
\[5mm] & =
-2,lim_R to inftyReint_1^0expo-parsR + ic y^4ic,dd y -
2,Reint_infty^0expo-t^4dd t -
2,Reint_0^1expo-parsic y^4ic,dd y
\[5mm] & =
-2,lim_R to inftyImint_0^1expo-parsR + ic y^4,dd y +
1 over 2int_0^inftyt^-3/4expo-t,dd t
\[5mm] & =
-2,lim_R to inftyImint_0^1exppars-R^4 - 4R^3yic + 6R^2y^2 + 4Ry^3ic - y^4,dd y +
1 over 2,Gammapars1 over 4
\[1cm] & =
1 over 2,Gammapars1 over 4
\[2mm] & -
2lim_R to inftybraces%
expo-R^4int_0^1expparsy^2bracks6R^2 - y^2
sinpars4Rybracksy^2 - R^2,dd y
endalign




  • $dsy^2pars6R^2 - y^2$ has a maximum at $dsy_m = root3R$.
    $dsy_m > 1$ when $dsR > root3 over 3$.

  • It vanishes at $dsy = 0$ and at $dsy = root6R$.

  • It $dsto -infty$ when $dsy to infty$.

  • It's clear that $ds0 < y^2pars6R^2 - y^2 < 6R^2 - 1$ when $dsy in pars0,1$ with $dsR > root3 over 3$.



Then,
beginalign
0 & < vertsexpo-R^4int_0^1expparsy^2bracks6R^2 - y^2
sinpars4Rybracksy^2 - R^2,dd y_ R > !root3/3
\[5mm] & <
expo-R^4int_0^1exppars1^2bracks6R^2 - 1^2,dd y =
exppars-R^4 + 6R^2 - 1
,,,stackrelmrmas R to inftyto,,,
color#f00large 0
endalign



beginalign
mboxsuch thatquad
bbxint_-infty^inftyexpo-parst - ic^4dd t =
1 over 2,Gammapars1 over 4 approx 1.8128
endalign




share|cite|improve this answer











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    2 Answers
    2






    active

    oldest

    votes








    2 Answers
    2






    active

    oldest

    votes









    active

    oldest

    votes






    active

    oldest

    votes









    27












    $begingroup$

    Just as User8128 commented, I believe that you are perfectly correct.



    Without changing variable and using another CAS
    $$int mathrme^-(t-i)^4 , mathrmdt=colorred-frac(t-i), Gamma left(frac14,(t-i)^4right)4 sqrt[4](t-i)^4=-frac14 (t-i) E_frac34left((t-i)^4right)$$
    $$int_-infty^infty mathrme^-(t-i)^4 , mathrmdt=i left(E_frac34(-4)-Releft(E_frac34(-4)right)right)$$ $$int_-infty^infty mathrme^-(t-i)^4 , mathrmdt=frac(-1)^1/4, Gamma left(frac14,-4right)sqrt2-i
    Releft(-frac(-1)^3/4, Gamma left(frac14,-4right)sqrt2right)=2, Gamma left(frac54right) $$
    Notice that, for the indefinite integral, Wolfram Alpha correctly reports the expression written in red.



    What is interesting is that, if you ask Wolfram Alpha
    $$int_0^infty mathrme^-(t-i)^4 , mathrmdt=-frac i4E_frac34(-1)$$
    $$int^0_-infty mathrme^-(t-i)^4 , mathrmdt=+frac i4E_frac34(-1)$$ leading to the $0$ you obtained.



    There is obviously a bug that I suggest you to report.






    share|cite|improve this answer











    $endgroup$








    • 3




      $begingroup$
      The bug is kind of interesting. Just below i it still works, e.g. for 0.99 i see here at 1 i it fails.
      $endgroup$
      – Jannick
      Jun 26 '17 at 9:36







    • 10




      $begingroup$
      @Jannick. Type $1.0i$ and it works !!!
      $endgroup$
      – Claude Leibovici
      Jun 26 '17 at 10:09










    • $begingroup$
      Yes true, that is really funny. For integer one it already fails but for float one it still works. For 1.01 it fails however.
      $endgroup$
      – Jannick
      Jun 26 '17 at 10:13






    • 3




      $begingroup$
      @Jannick.**Funny** may not be the most appropriate term here ! Cheers and thanks for your previous comment which made me trying $1.0i$.
      $endgroup$
      – Claude Leibovici
      Jun 26 '17 at 10:15







    • 1




      $begingroup$
      @MeniRosenfeld: The original bug does, at the least in Mathematica 9. Integrate[Exp[-(t - I)^4], t, -Infinity, Infinity] yields 0. NIntegrate with the same argument returns 1.8128 + very little i, just like what you see.
      $endgroup$
      – user22961
      Jun 26 '17 at 18:27
















    27












    $begingroup$

    Just as User8128 commented, I believe that you are perfectly correct.



    Without changing variable and using another CAS
    $$int mathrme^-(t-i)^4 , mathrmdt=colorred-frac(t-i), Gamma left(frac14,(t-i)^4right)4 sqrt[4](t-i)^4=-frac14 (t-i) E_frac34left((t-i)^4right)$$
    $$int_-infty^infty mathrme^-(t-i)^4 , mathrmdt=i left(E_frac34(-4)-Releft(E_frac34(-4)right)right)$$ $$int_-infty^infty mathrme^-(t-i)^4 , mathrmdt=frac(-1)^1/4, Gamma left(frac14,-4right)sqrt2-i
    Releft(-frac(-1)^3/4, Gamma left(frac14,-4right)sqrt2right)=2, Gamma left(frac54right) $$
    Notice that, for the indefinite integral, Wolfram Alpha correctly reports the expression written in red.



    What is interesting is that, if you ask Wolfram Alpha
    $$int_0^infty mathrme^-(t-i)^4 , mathrmdt=-frac i4E_frac34(-1)$$
    $$int^0_-infty mathrme^-(t-i)^4 , mathrmdt=+frac i4E_frac34(-1)$$ leading to the $0$ you obtained.



    There is obviously a bug that I suggest you to report.






    share|cite|improve this answer











    $endgroup$








    • 3




      $begingroup$
      The bug is kind of interesting. Just below i it still works, e.g. for 0.99 i see here at 1 i it fails.
      $endgroup$
      – Jannick
      Jun 26 '17 at 9:36







    • 10




      $begingroup$
      @Jannick. Type $1.0i$ and it works !!!
      $endgroup$
      – Claude Leibovici
      Jun 26 '17 at 10:09










    • $begingroup$
      Yes true, that is really funny. For integer one it already fails but for float one it still works. For 1.01 it fails however.
      $endgroup$
      – Jannick
      Jun 26 '17 at 10:13






    • 3




      $begingroup$
      @Jannick.**Funny** may not be the most appropriate term here ! Cheers and thanks for your previous comment which made me trying $1.0i$.
      $endgroup$
      – Claude Leibovici
      Jun 26 '17 at 10:15







    • 1




      $begingroup$
      @MeniRosenfeld: The original bug does, at the least in Mathematica 9. Integrate[Exp[-(t - I)^4], t, -Infinity, Infinity] yields 0. NIntegrate with the same argument returns 1.8128 + very little i, just like what you see.
      $endgroup$
      – user22961
      Jun 26 '17 at 18:27














    27












    27








    27





    $begingroup$

    Just as User8128 commented, I believe that you are perfectly correct.



    Without changing variable and using another CAS
    $$int mathrme^-(t-i)^4 , mathrmdt=colorred-frac(t-i), Gamma left(frac14,(t-i)^4right)4 sqrt[4](t-i)^4=-frac14 (t-i) E_frac34left((t-i)^4right)$$
    $$int_-infty^infty mathrme^-(t-i)^4 , mathrmdt=i left(E_frac34(-4)-Releft(E_frac34(-4)right)right)$$ $$int_-infty^infty mathrme^-(t-i)^4 , mathrmdt=frac(-1)^1/4, Gamma left(frac14,-4right)sqrt2-i
    Releft(-frac(-1)^3/4, Gamma left(frac14,-4right)sqrt2right)=2, Gamma left(frac54right) $$
    Notice that, for the indefinite integral, Wolfram Alpha correctly reports the expression written in red.



    What is interesting is that, if you ask Wolfram Alpha
    $$int_0^infty mathrme^-(t-i)^4 , mathrmdt=-frac i4E_frac34(-1)$$
    $$int^0_-infty mathrme^-(t-i)^4 , mathrmdt=+frac i4E_frac34(-1)$$ leading to the $0$ you obtained.



    There is obviously a bug that I suggest you to report.






    share|cite|improve this answer











    $endgroup$



    Just as User8128 commented, I believe that you are perfectly correct.



    Without changing variable and using another CAS
    $$int mathrme^-(t-i)^4 , mathrmdt=colorred-frac(t-i), Gamma left(frac14,(t-i)^4right)4 sqrt[4](t-i)^4=-frac14 (t-i) E_frac34left((t-i)^4right)$$
    $$int_-infty^infty mathrme^-(t-i)^4 , mathrmdt=i left(E_frac34(-4)-Releft(E_frac34(-4)right)right)$$ $$int_-infty^infty mathrme^-(t-i)^4 , mathrmdt=frac(-1)^1/4, Gamma left(frac14,-4right)sqrt2-i
    Releft(-frac(-1)^3/4, Gamma left(frac14,-4right)sqrt2right)=2, Gamma left(frac54right) $$
    Notice that, for the indefinite integral, Wolfram Alpha correctly reports the expression written in red.



    What is interesting is that, if you ask Wolfram Alpha
    $$int_0^infty mathrme^-(t-i)^4 , mathrmdt=-frac i4E_frac34(-1)$$
    $$int^0_-infty mathrme^-(t-i)^4 , mathrmdt=+frac i4E_frac34(-1)$$ leading to the $0$ you obtained.



    There is obviously a bug that I suggest you to report.







    share|cite|improve this answer














    share|cite|improve this answer



    share|cite|improve this answer








    edited Mar 18 at 10:57









    YuiTo Cheng

    2,1512937




    2,1512937










    answered Jun 26 '17 at 3:37









    Claude LeiboviciClaude Leibovici

    125k1158135




    125k1158135







    • 3




      $begingroup$
      The bug is kind of interesting. Just below i it still works, e.g. for 0.99 i see here at 1 i it fails.
      $endgroup$
      – Jannick
      Jun 26 '17 at 9:36







    • 10




      $begingroup$
      @Jannick. Type $1.0i$ and it works !!!
      $endgroup$
      – Claude Leibovici
      Jun 26 '17 at 10:09










    • $begingroup$
      Yes true, that is really funny. For integer one it already fails but for float one it still works. For 1.01 it fails however.
      $endgroup$
      – Jannick
      Jun 26 '17 at 10:13






    • 3




      $begingroup$
      @Jannick.**Funny** may not be the most appropriate term here ! Cheers and thanks for your previous comment which made me trying $1.0i$.
      $endgroup$
      – Claude Leibovici
      Jun 26 '17 at 10:15







    • 1




      $begingroup$
      @MeniRosenfeld: The original bug does, at the least in Mathematica 9. Integrate[Exp[-(t - I)^4], t, -Infinity, Infinity] yields 0. NIntegrate with the same argument returns 1.8128 + very little i, just like what you see.
      $endgroup$
      – user22961
      Jun 26 '17 at 18:27













    • 3




      $begingroup$
      The bug is kind of interesting. Just below i it still works, e.g. for 0.99 i see here at 1 i it fails.
      $endgroup$
      – Jannick
      Jun 26 '17 at 9:36







    • 10




      $begingroup$
      @Jannick. Type $1.0i$ and it works !!!
      $endgroup$
      – Claude Leibovici
      Jun 26 '17 at 10:09










    • $begingroup$
      Yes true, that is really funny. For integer one it already fails but for float one it still works. For 1.01 it fails however.
      $endgroup$
      – Jannick
      Jun 26 '17 at 10:13






    • 3




      $begingroup$
      @Jannick.**Funny** may not be the most appropriate term here ! Cheers and thanks for your previous comment which made me trying $1.0i$.
      $endgroup$
      – Claude Leibovici
      Jun 26 '17 at 10:15







    • 1




      $begingroup$
      @MeniRosenfeld: The original bug does, at the least in Mathematica 9. Integrate[Exp[-(t - I)^4], t, -Infinity, Infinity] yields 0. NIntegrate with the same argument returns 1.8128 + very little i, just like what you see.
      $endgroup$
      – user22961
      Jun 26 '17 at 18:27








    3




    3




    $begingroup$
    The bug is kind of interesting. Just below i it still works, e.g. for 0.99 i see here at 1 i it fails.
    $endgroup$
    – Jannick
    Jun 26 '17 at 9:36





    $begingroup$
    The bug is kind of interesting. Just below i it still works, e.g. for 0.99 i see here at 1 i it fails.
    $endgroup$
    – Jannick
    Jun 26 '17 at 9:36





    10




    10




    $begingroup$
    @Jannick. Type $1.0i$ and it works !!!
    $endgroup$
    – Claude Leibovici
    Jun 26 '17 at 10:09




    $begingroup$
    @Jannick. Type $1.0i$ and it works !!!
    $endgroup$
    – Claude Leibovici
    Jun 26 '17 at 10:09












    $begingroup$
    Yes true, that is really funny. For integer one it already fails but for float one it still works. For 1.01 it fails however.
    $endgroup$
    – Jannick
    Jun 26 '17 at 10:13




    $begingroup$
    Yes true, that is really funny. For integer one it already fails but for float one it still works. For 1.01 it fails however.
    $endgroup$
    – Jannick
    Jun 26 '17 at 10:13




    3




    3




    $begingroup$
    @Jannick.**Funny** may not be the most appropriate term here ! Cheers and thanks for your previous comment which made me trying $1.0i$.
    $endgroup$
    – Claude Leibovici
    Jun 26 '17 at 10:15





    $begingroup$
    @Jannick.**Funny** may not be the most appropriate term here ! Cheers and thanks for your previous comment which made me trying $1.0i$.
    $endgroup$
    – Claude Leibovici
    Jun 26 '17 at 10:15





    1




    1




    $begingroup$
    @MeniRosenfeld: The original bug does, at the least in Mathematica 9. Integrate[Exp[-(t - I)^4], t, -Infinity, Infinity] yields 0. NIntegrate with the same argument returns 1.8128 + very little i, just like what you see.
    $endgroup$
    – user22961
    Jun 26 '17 at 18:27





    $begingroup$
    @MeniRosenfeld: The original bug does, at the least in Mathematica 9. Integrate[Exp[-(t - I)^4], t, -Infinity, Infinity] yields 0. NIntegrate with the same argument returns 1.8128 + very little i, just like what you see.
    $endgroup$
    – user22961
    Jun 26 '17 at 18:27












    14












    $begingroup$

    $newcommandbbx[1],bbox[15px,border:1px groove navy]displaystyle#1,
    newcommandbraces[1]leftlbrace,#1,rightrbrace
    newcommandbracks[1]leftlbrack,#1,rightrbrack
    newcommandddmathrmd
    newcommandds[1]displaystyle#1
    newcommandexpo[1],mathrme^#1,
    newcommandicmathrmi
    newcommandmc[1]mathcal#1
    newcommandmrm[1]mathrm#1
    newcommandpars[1]left(,#1,right)
    newcommandpartiald[3][]fracpartial^#1 #2partial #3^#1
    newcommandroot[2][],sqrt[#1],#2,,
    newcommandtotald[3][]fracmathrmd^#1 #2mathrmd #3^#1
    newcommandverts[1]leftvert,#1,rightvert$
    beginalign
    int_-infty^inftyexpo-parst - ic^4dd t & =
    int_0^inftybracksexpo-parst - ic^4 +
    expo-pars-t - ic^4dd t =
    2,Reint_0^inftyexpo-parst + ic^4dd t =
    2,Reint_ic^infty + icexpo-t^4dd t
    \[5mm] & =
    -2,lim_R to inftyReint_1^0expo-parsR + ic y^4ic,dd y -
    2,Reint_infty^0expo-t^4dd t -
    2,Reint_0^1expo-parsic y^4ic,dd y
    \[5mm] & =
    -2,lim_R to inftyImint_0^1expo-parsR + ic y^4,dd y +
    1 over 2int_0^inftyt^-3/4expo-t,dd t
    \[5mm] & =
    -2,lim_R to inftyImint_0^1exppars-R^4 - 4R^3yic + 6R^2y^2 + 4Ry^3ic - y^4,dd y +
    1 over 2,Gammapars1 over 4
    \[1cm] & =
    1 over 2,Gammapars1 over 4
    \[2mm] & -
    2lim_R to inftybraces%
    expo-R^4int_0^1expparsy^2bracks6R^2 - y^2
    sinpars4Rybracksy^2 - R^2,dd y
    endalign




    • $dsy^2pars6R^2 - y^2$ has a maximum at $dsy_m = root3R$.
      $dsy_m > 1$ when $dsR > root3 over 3$.

    • It vanishes at $dsy = 0$ and at $dsy = root6R$.

    • It $dsto -infty$ when $dsy to infty$.

    • It's clear that $ds0 < y^2pars6R^2 - y^2 < 6R^2 - 1$ when $dsy in pars0,1$ with $dsR > root3 over 3$.



    Then,
    beginalign
    0 & < vertsexpo-R^4int_0^1expparsy^2bracks6R^2 - y^2
    sinpars4Rybracksy^2 - R^2,dd y_ R > !root3/3
    \[5mm] & <
    expo-R^4int_0^1exppars1^2bracks6R^2 - 1^2,dd y =
    exppars-R^4 + 6R^2 - 1
    ,,,stackrelmrmas R to inftyto,,,
    color#f00large 0
    endalign



    beginalign
    mboxsuch thatquad
    bbxint_-infty^inftyexpo-parst - ic^4dd t =
    1 over 2,Gammapars1 over 4 approx 1.8128
    endalign




    share|cite|improve this answer











    $endgroup$

















      14












      $begingroup$

      $newcommandbbx[1],bbox[15px,border:1px groove navy]displaystyle#1,
      newcommandbraces[1]leftlbrace,#1,rightrbrace
      newcommandbracks[1]leftlbrack,#1,rightrbrack
      newcommandddmathrmd
      newcommandds[1]displaystyle#1
      newcommandexpo[1],mathrme^#1,
      newcommandicmathrmi
      newcommandmc[1]mathcal#1
      newcommandmrm[1]mathrm#1
      newcommandpars[1]left(,#1,right)
      newcommandpartiald[3][]fracpartial^#1 #2partial #3^#1
      newcommandroot[2][],sqrt[#1],#2,,
      newcommandtotald[3][]fracmathrmd^#1 #2mathrmd #3^#1
      newcommandverts[1]leftvert,#1,rightvert$
      beginalign
      int_-infty^inftyexpo-parst - ic^4dd t & =
      int_0^inftybracksexpo-parst - ic^4 +
      expo-pars-t - ic^4dd t =
      2,Reint_0^inftyexpo-parst + ic^4dd t =
      2,Reint_ic^infty + icexpo-t^4dd t
      \[5mm] & =
      -2,lim_R to inftyReint_1^0expo-parsR + ic y^4ic,dd y -
      2,Reint_infty^0expo-t^4dd t -
      2,Reint_0^1expo-parsic y^4ic,dd y
      \[5mm] & =
      -2,lim_R to inftyImint_0^1expo-parsR + ic y^4,dd y +
      1 over 2int_0^inftyt^-3/4expo-t,dd t
      \[5mm] & =
      -2,lim_R to inftyImint_0^1exppars-R^4 - 4R^3yic + 6R^2y^2 + 4Ry^3ic - y^4,dd y +
      1 over 2,Gammapars1 over 4
      \[1cm] & =
      1 over 2,Gammapars1 over 4
      \[2mm] & -
      2lim_R to inftybraces%
      expo-R^4int_0^1expparsy^2bracks6R^2 - y^2
      sinpars4Rybracksy^2 - R^2,dd y
      endalign




      • $dsy^2pars6R^2 - y^2$ has a maximum at $dsy_m = root3R$.
        $dsy_m > 1$ when $dsR > root3 over 3$.

      • It vanishes at $dsy = 0$ and at $dsy = root6R$.

      • It $dsto -infty$ when $dsy to infty$.

      • It's clear that $ds0 < y^2pars6R^2 - y^2 < 6R^2 - 1$ when $dsy in pars0,1$ with $dsR > root3 over 3$.



      Then,
      beginalign
      0 & < vertsexpo-R^4int_0^1expparsy^2bracks6R^2 - y^2
      sinpars4Rybracksy^2 - R^2,dd y_ R > !root3/3
      \[5mm] & <
      expo-R^4int_0^1exppars1^2bracks6R^2 - 1^2,dd y =
      exppars-R^4 + 6R^2 - 1
      ,,,stackrelmrmas R to inftyto,,,
      color#f00large 0
      endalign



      beginalign
      mboxsuch thatquad
      bbxint_-infty^inftyexpo-parst - ic^4dd t =
      1 over 2,Gammapars1 over 4 approx 1.8128
      endalign




      share|cite|improve this answer











      $endgroup$















        14












        14








        14





        $begingroup$

        $newcommandbbx[1],bbox[15px,border:1px groove navy]displaystyle#1,
        newcommandbraces[1]leftlbrace,#1,rightrbrace
        newcommandbracks[1]leftlbrack,#1,rightrbrack
        newcommandddmathrmd
        newcommandds[1]displaystyle#1
        newcommandexpo[1],mathrme^#1,
        newcommandicmathrmi
        newcommandmc[1]mathcal#1
        newcommandmrm[1]mathrm#1
        newcommandpars[1]left(,#1,right)
        newcommandpartiald[3][]fracpartial^#1 #2partial #3^#1
        newcommandroot[2][],sqrt[#1],#2,,
        newcommandtotald[3][]fracmathrmd^#1 #2mathrmd #3^#1
        newcommandverts[1]leftvert,#1,rightvert$
        beginalign
        int_-infty^inftyexpo-parst - ic^4dd t & =
        int_0^inftybracksexpo-parst - ic^4 +
        expo-pars-t - ic^4dd t =
        2,Reint_0^inftyexpo-parst + ic^4dd t =
        2,Reint_ic^infty + icexpo-t^4dd t
        \[5mm] & =
        -2,lim_R to inftyReint_1^0expo-parsR + ic y^4ic,dd y -
        2,Reint_infty^0expo-t^4dd t -
        2,Reint_0^1expo-parsic y^4ic,dd y
        \[5mm] & =
        -2,lim_R to inftyImint_0^1expo-parsR + ic y^4,dd y +
        1 over 2int_0^inftyt^-3/4expo-t,dd t
        \[5mm] & =
        -2,lim_R to inftyImint_0^1exppars-R^4 - 4R^3yic + 6R^2y^2 + 4Ry^3ic - y^4,dd y +
        1 over 2,Gammapars1 over 4
        \[1cm] & =
        1 over 2,Gammapars1 over 4
        \[2mm] & -
        2lim_R to inftybraces%
        expo-R^4int_0^1expparsy^2bracks6R^2 - y^2
        sinpars4Rybracksy^2 - R^2,dd y
        endalign




        • $dsy^2pars6R^2 - y^2$ has a maximum at $dsy_m = root3R$.
          $dsy_m > 1$ when $dsR > root3 over 3$.

        • It vanishes at $dsy = 0$ and at $dsy = root6R$.

        • It $dsto -infty$ when $dsy to infty$.

        • It's clear that $ds0 < y^2pars6R^2 - y^2 < 6R^2 - 1$ when $dsy in pars0,1$ with $dsR > root3 over 3$.



        Then,
        beginalign
        0 & < vertsexpo-R^4int_0^1expparsy^2bracks6R^2 - y^2
        sinpars4Rybracksy^2 - R^2,dd y_ R > !root3/3
        \[5mm] & <
        expo-R^4int_0^1exppars1^2bracks6R^2 - 1^2,dd y =
        exppars-R^4 + 6R^2 - 1
        ,,,stackrelmrmas R to inftyto,,,
        color#f00large 0
        endalign



        beginalign
        mboxsuch thatquad
        bbxint_-infty^inftyexpo-parst - ic^4dd t =
        1 over 2,Gammapars1 over 4 approx 1.8128
        endalign




        share|cite|improve this answer











        $endgroup$



        $newcommandbbx[1],bbox[15px,border:1px groove navy]displaystyle#1,
        newcommandbraces[1]leftlbrace,#1,rightrbrace
        newcommandbracks[1]leftlbrack,#1,rightrbrack
        newcommandddmathrmd
        newcommandds[1]displaystyle#1
        newcommandexpo[1],mathrme^#1,
        newcommandicmathrmi
        newcommandmc[1]mathcal#1
        newcommandmrm[1]mathrm#1
        newcommandpars[1]left(,#1,right)
        newcommandpartiald[3][]fracpartial^#1 #2partial #3^#1
        newcommandroot[2][],sqrt[#1],#2,,
        newcommandtotald[3][]fracmathrmd^#1 #2mathrmd #3^#1
        newcommandverts[1]leftvert,#1,rightvert$
        beginalign
        int_-infty^inftyexpo-parst - ic^4dd t & =
        int_0^inftybracksexpo-parst - ic^4 +
        expo-pars-t - ic^4dd t =
        2,Reint_0^inftyexpo-parst + ic^4dd t =
        2,Reint_ic^infty + icexpo-t^4dd t
        \[5mm] & =
        -2,lim_R to inftyReint_1^0expo-parsR + ic y^4ic,dd y -
        2,Reint_infty^0expo-t^4dd t -
        2,Reint_0^1expo-parsic y^4ic,dd y
        \[5mm] & =
        -2,lim_R to inftyImint_0^1expo-parsR + ic y^4,dd y +
        1 over 2int_0^inftyt^-3/4expo-t,dd t
        \[5mm] & =
        -2,lim_R to inftyImint_0^1exppars-R^4 - 4R^3yic + 6R^2y^2 + 4Ry^3ic - y^4,dd y +
        1 over 2,Gammapars1 over 4
        \[1cm] & =
        1 over 2,Gammapars1 over 4
        \[2mm] & -
        2lim_R to inftybraces%
        expo-R^4int_0^1expparsy^2bracks6R^2 - y^2
        sinpars4Rybracksy^2 - R^2,dd y
        endalign




        • $dsy^2pars6R^2 - y^2$ has a maximum at $dsy_m = root3R$.
          $dsy_m > 1$ when $dsR > root3 over 3$.

        • It vanishes at $dsy = 0$ and at $dsy = root6R$.

        • It $dsto -infty$ when $dsy to infty$.

        • It's clear that $ds0 < y^2pars6R^2 - y^2 < 6R^2 - 1$ when $dsy in pars0,1$ with $dsR > root3 over 3$.



        Then,
        beginalign
        0 & < vertsexpo-R^4int_0^1expparsy^2bracks6R^2 - y^2
        sinpars4Rybracksy^2 - R^2,dd y_ R > !root3/3
        \[5mm] & <
        expo-R^4int_0^1exppars1^2bracks6R^2 - 1^2,dd y =
        exppars-R^4 + 6R^2 - 1
        ,,,stackrelmrmas R to inftyto,,,
        color#f00large 0
        endalign



        beginalign
        mboxsuch thatquad
        bbxint_-infty^inftyexpo-parst - ic^4dd t =
        1 over 2,Gammapars1 over 4 approx 1.8128
        endalign





        share|cite|improve this answer














        share|cite|improve this answer



        share|cite|improve this answer








        edited Jun 26 '17 at 6:33

























        answered Jun 26 '17 at 6:27









        Felix MarinFelix Marin

        68.8k7109146




        68.8k7109146



























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