Do these integrals evaluate to terms involving Kronecker Deltas?

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There is a famous integral representation of the Kronecker delta:
$$
delta_N,M = int_0^1 dx e^-2 pi i (N-M)x
$$



Noting this, I have encountered two integrals where $N,M,m in mathbbZ$. First:
$$
mathcalI_1 = int_m-tfrac12^m+tfrac12 dx x e^-2 pi i (N-M)x
$$
I have a reference which seems to be implying that $mathcalI_1 = m delta_M,N$.



The second integral is worse (for any $y > 0$):
$$
mathcalI_2 = int_m-tfrac12^m+tfrac12 dx sqrt x^2 + y^2 e^-2 pi i (N-M)x
$$
I have no clue how to evaluate either of these. Do they both involve a $delta_N,M$?







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    There is a famous integral representation of the Kronecker delta:
    $$
    delta_N,M = int_0^1 dx e^-2 pi i (N-M)x
    $$



    Noting this, I have encountered two integrals where $N,M,m in mathbbZ$. First:
    $$
    mathcalI_1 = int_m-tfrac12^m+tfrac12 dx x e^-2 pi i (N-M)x
    $$
    I have a reference which seems to be implying that $mathcalI_1 = m delta_M,N$.



    The second integral is worse (for any $y > 0$):
    $$
    mathcalI_2 = int_m-tfrac12^m+tfrac12 dx sqrt x^2 + y^2 e^-2 pi i (N-M)x
    $$
    I have no clue how to evaluate either of these. Do they both involve a $delta_N,M$?







    share|cite|improve this question





















      up vote
      2
      down vote

      favorite









      up vote
      2
      down vote

      favorite











      There is a famous integral representation of the Kronecker delta:
      $$
      delta_N,M = int_0^1 dx e^-2 pi i (N-M)x
      $$



      Noting this, I have encountered two integrals where $N,M,m in mathbbZ$. First:
      $$
      mathcalI_1 = int_m-tfrac12^m+tfrac12 dx x e^-2 pi i (N-M)x
      $$
      I have a reference which seems to be implying that $mathcalI_1 = m delta_M,N$.



      The second integral is worse (for any $y > 0$):
      $$
      mathcalI_2 = int_m-tfrac12^m+tfrac12 dx sqrt x^2 + y^2 e^-2 pi i (N-M)x
      $$
      I have no clue how to evaluate either of these. Do they both involve a $delta_N,M$?







      share|cite|improve this question











      There is a famous integral representation of the Kronecker delta:
      $$
      delta_N,M = int_0^1 dx e^-2 pi i (N-M)x
      $$



      Noting this, I have encountered two integrals where $N,M,m in mathbbZ$. First:
      $$
      mathcalI_1 = int_m-tfrac12^m+tfrac12 dx x e^-2 pi i (N-M)x
      $$
      I have a reference which seems to be implying that $mathcalI_1 = m delta_M,N$.



      The second integral is worse (for any $y > 0$):
      $$
      mathcalI_2 = int_m-tfrac12^m+tfrac12 dx sqrt x^2 + y^2 e^-2 pi i (N-M)x
      $$
      I have no clue how to evaluate either of these. Do they both involve a $delta_N,M$?









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      asked Aug 5 at 23:13









      Greg.Paul

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          First note that your representation of the Kronecker delta is still correct if we shift the limits of integration:
          $$ delta_N,M = int limits_m-frac12^m+frac12 mathrmd x , mathrme^- 2 pi mathrmi (N-M) x , .$$



          For the first integral we get
          $$ mathcalI_1 = int limits_m-frac12^m+frac12 mathrmd x , x = m $$
          if $N=M$ . If $N neq M$, we can integrate by parts to obtain
          beginalign
          mathcalI_1 &= left[- fracx mathrme^- 2 pi mathrmi (N-M) x2 pi mathrmi (N-M)right]_x=m-frac12^x=m+frac12 + frac12 pi mathrmi (N-M)int limits_m-frac12^m+frac12 mathrmd x , mathrme^- 2 pi mathrmi (N-M) x \
          &= fracmathrmi (-1)^N-M2 pi (N-M) , ,
          endalign
          since the second integral vanishes by our initial observation. Therefore it does not lead to a Kronecker delta. We see that $operatornameRe (mathcalI_1) = m delta_N,M$ holds, however.



          The second integral is a lot more complicated, but numerical calculations suggest that neither real nor imaginary part vanish in general, so it seems unlikely that it has any connection to the Kronecker delta.






          share|cite|improve this answer





















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            active

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            up vote
            2
            down vote



            accepted










            First note that your representation of the Kronecker delta is still correct if we shift the limits of integration:
            $$ delta_N,M = int limits_m-frac12^m+frac12 mathrmd x , mathrme^- 2 pi mathrmi (N-M) x , .$$



            For the first integral we get
            $$ mathcalI_1 = int limits_m-frac12^m+frac12 mathrmd x , x = m $$
            if $N=M$ . If $N neq M$, we can integrate by parts to obtain
            beginalign
            mathcalI_1 &= left[- fracx mathrme^- 2 pi mathrmi (N-M) x2 pi mathrmi (N-M)right]_x=m-frac12^x=m+frac12 + frac12 pi mathrmi (N-M)int limits_m-frac12^m+frac12 mathrmd x , mathrme^- 2 pi mathrmi (N-M) x \
            &= fracmathrmi (-1)^N-M2 pi (N-M) , ,
            endalign
            since the second integral vanishes by our initial observation. Therefore it does not lead to a Kronecker delta. We see that $operatornameRe (mathcalI_1) = m delta_N,M$ holds, however.



            The second integral is a lot more complicated, but numerical calculations suggest that neither real nor imaginary part vanish in general, so it seems unlikely that it has any connection to the Kronecker delta.






            share|cite|improve this answer

























              up vote
              2
              down vote



              accepted










              First note that your representation of the Kronecker delta is still correct if we shift the limits of integration:
              $$ delta_N,M = int limits_m-frac12^m+frac12 mathrmd x , mathrme^- 2 pi mathrmi (N-M) x , .$$



              For the first integral we get
              $$ mathcalI_1 = int limits_m-frac12^m+frac12 mathrmd x , x = m $$
              if $N=M$ . If $N neq M$, we can integrate by parts to obtain
              beginalign
              mathcalI_1 &= left[- fracx mathrme^- 2 pi mathrmi (N-M) x2 pi mathrmi (N-M)right]_x=m-frac12^x=m+frac12 + frac12 pi mathrmi (N-M)int limits_m-frac12^m+frac12 mathrmd x , mathrme^- 2 pi mathrmi (N-M) x \
              &= fracmathrmi (-1)^N-M2 pi (N-M) , ,
              endalign
              since the second integral vanishes by our initial observation. Therefore it does not lead to a Kronecker delta. We see that $operatornameRe (mathcalI_1) = m delta_N,M$ holds, however.



              The second integral is a lot more complicated, but numerical calculations suggest that neither real nor imaginary part vanish in general, so it seems unlikely that it has any connection to the Kronecker delta.






              share|cite|improve this answer























                up vote
                2
                down vote



                accepted







                up vote
                2
                down vote



                accepted






                First note that your representation of the Kronecker delta is still correct if we shift the limits of integration:
                $$ delta_N,M = int limits_m-frac12^m+frac12 mathrmd x , mathrme^- 2 pi mathrmi (N-M) x , .$$



                For the first integral we get
                $$ mathcalI_1 = int limits_m-frac12^m+frac12 mathrmd x , x = m $$
                if $N=M$ . If $N neq M$, we can integrate by parts to obtain
                beginalign
                mathcalI_1 &= left[- fracx mathrme^- 2 pi mathrmi (N-M) x2 pi mathrmi (N-M)right]_x=m-frac12^x=m+frac12 + frac12 pi mathrmi (N-M)int limits_m-frac12^m+frac12 mathrmd x , mathrme^- 2 pi mathrmi (N-M) x \
                &= fracmathrmi (-1)^N-M2 pi (N-M) , ,
                endalign
                since the second integral vanishes by our initial observation. Therefore it does not lead to a Kronecker delta. We see that $operatornameRe (mathcalI_1) = m delta_N,M$ holds, however.



                The second integral is a lot more complicated, but numerical calculations suggest that neither real nor imaginary part vanish in general, so it seems unlikely that it has any connection to the Kronecker delta.






                share|cite|improve this answer













                First note that your representation of the Kronecker delta is still correct if we shift the limits of integration:
                $$ delta_N,M = int limits_m-frac12^m+frac12 mathrmd x , mathrme^- 2 pi mathrmi (N-M) x , .$$



                For the first integral we get
                $$ mathcalI_1 = int limits_m-frac12^m+frac12 mathrmd x , x = m $$
                if $N=M$ . If $N neq M$, we can integrate by parts to obtain
                beginalign
                mathcalI_1 &= left[- fracx mathrme^- 2 pi mathrmi (N-M) x2 pi mathrmi (N-M)right]_x=m-frac12^x=m+frac12 + frac12 pi mathrmi (N-M)int limits_m-frac12^m+frac12 mathrmd x , mathrme^- 2 pi mathrmi (N-M) x \
                &= fracmathrmi (-1)^N-M2 pi (N-M) , ,
                endalign
                since the second integral vanishes by our initial observation. Therefore it does not lead to a Kronecker delta. We see that $operatornameRe (mathcalI_1) = m delta_N,M$ holds, however.



                The second integral is a lot more complicated, but numerical calculations suggest that neither real nor imaginary part vanish in general, so it seems unlikely that it has any connection to the Kronecker delta.







                share|cite|improve this answer













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                answered Aug 6 at 15:40









                ComplexYetTrivial

                2,817624




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