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Explicit wave-package solution of the Klein Gordon equation


Trouble deriving DE for fourier transform from DE of functionIntegration by parts with few regularityIn the numerical solution of the Wave Equation, using finite differences, where do I obtain the spatial values from?Solving a wave equation using Fourier transformWhy can I change the integration unit in Fourier transform>Solving linear dispersive wave equation with Fourier transformSolving a simple Schrodinger equation with Fast Fourier TransformsSpherical Harmonic integration1D scalar wave equation PML finite difference implementationVelocity Auto-correlation on Spinning Disk













0












$begingroup$


I need to generate initial for a 3D Klein Gordon (KG) solver. Therefore I'm interested in physical meaningful wave-package solutions. By considering the free KG equation
beginequation
Box psi(t,x) = psi(t,x), quad (x,t) in Omega times mathbbR^+,
endequation

an obvious wave-package solution is given by
beginequation
psi(x,t) = int e^-k^2 +i x cdot k - iomega(k)t dk,
endequation

with $omega(k)=sqrtk^2+1$. From this formula we immediatly see that
beginequation
psi(x,0) = e^-fracx^24 +i x cdot k,
endequation

and the time derivative at $t=0$ becomes
beginequation
partial_t psi(x,0) = -i int omega(k) e^-k^2 +i x cdot k dk.
endequation

And one can recognize this as the Fourier transform of
beginequation
mathcalFleft( omega(k) e^-k^2 right).
endequation

So far so good, the idea was just to calculate the FFT of the function $omega(k) e^-k^2$ on my array but that isn't so accurate as it can be by an explicit expression of the initial time derivative. So my question if anyone has an idea how to write the soultion explicitly. (this can also include the erf function as well)










share|cite|improve this question











$endgroup$
















    0












    $begingroup$


    I need to generate initial for a 3D Klein Gordon (KG) solver. Therefore I'm interested in physical meaningful wave-package solutions. By considering the free KG equation
    beginequation
    Box psi(t,x) = psi(t,x), quad (x,t) in Omega times mathbbR^+,
    endequation

    an obvious wave-package solution is given by
    beginequation
    psi(x,t) = int e^-k^2 +i x cdot k - iomega(k)t dk,
    endequation

    with $omega(k)=sqrtk^2+1$. From this formula we immediatly see that
    beginequation
    psi(x,0) = e^-fracx^24 +i x cdot k,
    endequation

    and the time derivative at $t=0$ becomes
    beginequation
    partial_t psi(x,0) = -i int omega(k) e^-k^2 +i x cdot k dk.
    endequation

    And one can recognize this as the Fourier transform of
    beginequation
    mathcalFleft( omega(k) e^-k^2 right).
    endequation

    So far so good, the idea was just to calculate the FFT of the function $omega(k) e^-k^2$ on my array but that isn't so accurate as it can be by an explicit expression of the initial time derivative. So my question if anyone has an idea how to write the soultion explicitly. (this can also include the erf function as well)










    share|cite|improve this question











    $endgroup$














      0












      0








      0





      $begingroup$


      I need to generate initial for a 3D Klein Gordon (KG) solver. Therefore I'm interested in physical meaningful wave-package solutions. By considering the free KG equation
      beginequation
      Box psi(t,x) = psi(t,x), quad (x,t) in Omega times mathbbR^+,
      endequation

      an obvious wave-package solution is given by
      beginequation
      psi(x,t) = int e^-k^2 +i x cdot k - iomega(k)t dk,
      endequation

      with $omega(k)=sqrtk^2+1$. From this formula we immediatly see that
      beginequation
      psi(x,0) = e^-fracx^24 +i x cdot k,
      endequation

      and the time derivative at $t=0$ becomes
      beginequation
      partial_t psi(x,0) = -i int omega(k) e^-k^2 +i x cdot k dk.
      endequation

      And one can recognize this as the Fourier transform of
      beginequation
      mathcalFleft( omega(k) e^-k^2 right).
      endequation

      So far so good, the idea was just to calculate the FFT of the function $omega(k) e^-k^2$ on my array but that isn't so accurate as it can be by an explicit expression of the initial time derivative. So my question if anyone has an idea how to write the soultion explicitly. (this can also include the erf function as well)










      share|cite|improve this question











      $endgroup$




      I need to generate initial for a 3D Klein Gordon (KG) solver. Therefore I'm interested in physical meaningful wave-package solutions. By considering the free KG equation
      beginequation
      Box psi(t,x) = psi(t,x), quad (x,t) in Omega times mathbbR^+,
      endequation

      an obvious wave-package solution is given by
      beginequation
      psi(x,t) = int e^-k^2 +i x cdot k - iomega(k)t dk,
      endequation

      with $omega(k)=sqrtk^2+1$. From this formula we immediatly see that
      beginequation
      psi(x,0) = e^-fracx^24 +i x cdot k,
      endequation

      and the time derivative at $t=0$ becomes
      beginequation
      partial_t psi(x,0) = -i int omega(k) e^-k^2 +i x cdot k dk.
      endequation

      And one can recognize this as the Fourier transform of
      beginequation
      mathcalFleft( omega(k) e^-k^2 right).
      endequation

      So far so good, the idea was just to calculate the FFT of the function $omega(k) e^-k^2$ on my array but that isn't so accurate as it can be by an explicit expression of the initial time derivative. So my question if anyone has an idea how to write the soultion explicitly. (this can also include the erf function as well)







      integration numerical-methods fourier-analysis






      share|cite|improve this question















      share|cite|improve this question













      share|cite|improve this question




      share|cite|improve this question








      edited Mar 22 at 0:03









      J. W. Tanner

      4,4891320




      4,4891320










      asked Mar 21 at 23:50









      HamilcarHamilcar

      404211




      404211




















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