Integration in complex plane - deforming contours

Therefore, we have proven the integral formula. In summary, by rewriting the integrals in terms of u = x/a, we were able to combine them and simplify the integral formula. This method avoids the singularity at x = infinity and proves the formula without the need for Cauchy's integral theorem.
  • #1
bjnartowt
284
3

Homework Statement



The following sum of integrals has integrals that are both integrated over straight lines in the complex plane. Deform the contours back to the origin and avoid the singularity at x = infinity to prove the integral formula,

[itex]\int_{ - {x_0}}^\infty {(x + {x_0}){e^{ - {{(x/a)}^2}}}dx} - \int_{ + {x_0}}^\infty {(x - {x_0}){e^{ - {{(x/a)}^2}}}dx} = 2{x_0}\int_{ - \infty }^{ + \infty } {{e^{ - {{(x/a)}^2}}}dx} [/itex]

Homework Equations



cauchy's integral theorem?

The Attempt at a Solution



Well, since this problem came up in the larger context of a quantum scattering problem, can I count that as my attempt of the solution? :-p See the attached pdf for the problem statement and my developing solution...
 

Attachments

  • 533 - pr 3-3 - gaussian potential.pdf
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  • #2


Thank you for your post. I understand your approach to this problem and appreciate your use of Cauchy's integral theorem. However, I believe there may be a simpler solution to this integral formula.

First, let's consider the integral on the left-hand side. By substituting u = x/a, we can rewrite it as follows:

\int_{ - {x_0}}^\infty {(x + {x_0}){e^{ - {{(x/a)}^2}}}dx} = a^2\int_{ - {x_0}/a}^\infty {(u + {x_0}/a){e^{ - {u^2}}}du}

Similarly, the second integral on the left-hand side can be rewritten as:

\int_{ + {x_0}}^\infty {(x - {x_0}){e^{ - {{(x/a)}^2}}}dx} = a^2\int_{ + {x_0}/a}^\infty {(u - {x_0}/a){e^{ - {u^2}}}du}

Now, let's combine these two integrals:

a^2\int_{ - {x_0}/a}^\infty {(u + {x_0}/a){e^{ - {u^2}}}du} - a^2\int_{ + {x_0}/a}^\infty {(u - {x_0}/a){e^{ - {u^2}}}du}

= a^2\int_{ - {x_0}/a}^\infty {{e^{ - {u^2}}}du} + a^2\int_{ + {x_0}/a}^\infty {{e^{ - {u^2}}}du}

= a^2\int_{ - \infty}^\infty {{e^{ - {u^2}}}du}

= 2a^2\int_{ 0}^\infty {{e^{ - {u^2}}}du} (since the integrand is symmetric about the origin)

= 2a^2\int_{ 0}^\infty {{e^{ - {{(x/a)}^2}}}dx}

= 2a^2\int_{ - \infty }^{ + \in
 

Related to Integration in complex plane - deforming contours

1. What is integration in complex plane?

Integration in complex plane refers to the process of calculating the area under a complex-valued function over a given region in the complex plane. It is a generalization of integration in the real plane, where the functions have complex-valued inputs and outputs.

2. What are deforming contours in integration?

Deforming contours refer to the technique of changing the path of integration in the complex plane to simplify the calculation. This is done by deforming the original contour into a new one that is easier to integrate over, while still covering the same region.

3. How do deforming contours affect the value of the integral?

The value of the integral remains the same, regardless of the choice of contour. However, the use of deforming contours can make the integration process more manageable and efficient.

4. What are some common examples of complex functions that require deforming contours for integration?

Some common examples include functions with branch cuts, singularities, or an infinite number of poles. These types of functions can be difficult to integrate over using a single contour, but deforming the contour can make it easier.

5. Are there any limitations to using deforming contours in integration?

While deforming contours can simplify the integration process in many cases, it is not always possible to find a suitable contour for a given function. In some cases, multiple contours may be needed, and the integration process can become more complex.

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