Definite integral: exponential with squared exponent

Click For Summary
SUMMARY

The discussion centers on solving the definite integral f(x) = ∫-∞ ceyx - y2/2 dy, where c is a constant. The integral is identified as a Gaussian integral, which is crucial in theoretical physics. The solution involves completing the square to transform the expression into a more manageable form, ultimately leading to the use of the standard result I = ∫-∞ e-x2/2 dx = √(2π). This method simplifies the evaluation of the integral significantly.

PREREQUISITES
  • Understanding of Gaussian integrals
  • Knowledge of completing the square in algebra
  • Familiarity with polar coordinates
  • Basic calculus concepts, including integration techniques
NEXT STEPS
  • Study Gaussian integrals and their applications in physics
  • Learn about completing the square in quadratic expressions
  • Explore the derivation of the integral I = ∫-∞ e-x2/2 dx = √(2π)
  • Investigate variable substitution techniques in integrals
USEFUL FOR

The discussion is beneficial for students and professionals in mathematics and physics, particularly those interested in integral calculus and its applications in theoretical physics.

jumble0469
Messages
1
Reaction score
0
Hi,

I'm trying to solve the following:
[tex]f(x) = \int^\infty_{-\infty}ce^{yx-y^2/2} dy[/tex]
where c is a constant
My only idea thus far was that since it is an even function, the expression can be simplified to:
[tex]= 2c\int^\infty_0 e^{y(x-{1/2}y)} dy[/tex]

but I'm stuck here.

Anyone know how to do this?
 
Physics news on Phys.org
This is a Gaussian integral (which is ubiquitous in theoretical physics, so if you have any aspirations in that direction pay extra attention :smile:)

The trick is to complete the square: write*
[tex]y^2 - 2 y x = (y - a)^2 - b[/tex]
where a and b are independent of y, so you get
[tex]f(x) = c e^{-b/2} \int_{-\infty}^{\infty} e^{- (y - a)^2 / 2} \, dy.[/tex]
Then you can do a variable shift and use the standard result
[tex]I = \int_{-\infty}^\infty e^{-x^2 / 2} = \sqrt{2 \pi}[/tex]
which you can easily prove (if you've never done it, try it: consider [itex]I^2[/itex] and switch to polar coordinates).

* From this line onwards, I take no responsibility for sign errors and wrong factors of 1/2 - please check yourself :)
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 11 ·
Replies
11
Views
3K
  • · Replies 27 ·
Replies
27
Views
3K
  • · Replies 14 ·
Replies
14
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 11 ·
Replies
11
Views
3K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 21 ·
Replies
21
Views
4K