How would I know if my integrand is odd?

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Discussion Overview

The discussion revolves around understanding the properties of odd and even functions in the context of integrals, particularly in quantum mechanics normalization. Participants explore how to identify odd integrands, the implications of symmetry in integration limits, and specific examples involving Gaussian integrals.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants suggest that to determine if an integrand is odd, one can replace x with -x and check if the integrand transforms as f(x) → f(-x) = -f(x).
  • Others inquire about the reasoning behind the integral of an odd function being zero, prompting discussions about specific examples like the integral of sin(x).
  • One participant points out that the property of odd functions leading to zero integrals only holds if the integration interval is symmetric.
  • Another participant emphasizes that when integrating functions with infinite limits, one must ensure the limit exists and cannot assume the integral of an odd function over an infinite interval is zero without further justification.
  • Participants discuss a specific normalization example in quantum mechanics involving the integral of |ψ(x)|² and the appearance of a factor of 2 in the integral, leading to questions about the assumptions made in the derivation.
  • Some participants mention the relationship between the evenness or oddness of functions and their derivatives, noting that the derivative of an odd function is even and vice versa.
  • There is a reference to Gaussian integrals and the importance of understanding related special functions in quantum mechanics.

Areas of Agreement / Disagreement

Participants express varying levels of understanding regarding the properties of odd and even functions, with some agreeing on the definitions and implications while others raise questions and seek clarification. The discussion remains unresolved on certain points, particularly regarding specific examples and the application of these properties in quantum mechanics.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the symmetry of integration limits and the conditions under which certain integrals evaluate to zero. The specific mathematical steps and justifications for the factor of 2 in the normalization example are also not fully resolved.

jhosamelly
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So, I'm studying normalization (Quantum Mechanics). I came across examples of integrands which they say are odd. So, they say the integral of an odd function is zero. How would I know my integrand is odd? Thanks :)
 
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Replace x\rightarrow -x. If the integrand transforms f(x)\rightarrow f(-x)=-f(x) then it is odd.
 
Why is the integral of an odd function ZERO?
 
Take the definite integral of sin(x) w.r.t. x between 0 and 2*pi. (Or between -pi and pi). What is its value?
Plot sin(x) between 0 and 2*pi (or between -pi and pi). What do you notice about the plot?
 
How would you take the derivative of this?


\int^{∞}_{0} e ^{\frac{-2amx^2}{\hbar}}


What's the trick in doing integrals having infinity as one of its limit? Or what if the limit is from ∞ to -∞?
 
Last edited:
The derivative of an even function is odd and the derivative of an odd function is even (a simple proof, just use the definition). So, if you have an odd integrand f(-x)=-f(x), then for F(x) such that F'(x)=f(x) F(-x)=F(x) and so

\int_{-a}^{a} f(x) \mathrm{d}x = F(a) - F(-a) = F(a) - F(a) = 0

which is what is usually used when an integral over a symmetric interval is said to be zero because the integrand is odd.
 
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The key in Deldeals post that has been ignored until now: it works only if the integration interval is symmetric. In QM it usually is, by convenient choice of x = 0, but in general it is something you should check.
 
CompuChip said:
The key in Deldeals post that has been ignored until now: it works only if the integration interval is symmetric. In QM it usually is, by convenient choice of x = 0, but in general it is something you should check.

Adding to this, it's exactly why in jhosamelly's latest post the symmetry properties won't be of much use ** – basically the value of \int_0^\infty e^{-x^2}\mathrm{d}x needs to be known from elsewhere – but were it integrated from -∞ to ∞, the integral would evaluate to twice the value of \int_0^\infty e^{-x^2}\mathrm{d}x, as the integrand is even.

** And there are no specific "tricks" related to symmetry properties when it comes to having infinity as a limit for integrals like these, although the limit obviously must exist – you can't just say that \int_{-\infty}^{\infty} x \mathrm{d}x =0 even though f(x)=x is odd. That would be the so-called Cauchy principal value of the integral, although one that I don't think is very useful.
 
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Thanks for the responses guys. I'm learning.

But, let me show you the example I'm having difficulty understanding.

So, in normalization.

\int_{-∞}^{∞} |ψ(x)|^{2} \mathrm{d}x = 1

(I get this)

Say our

ψ(x) = A e^{-amx^2 / \hbar}

So we have

\int_{-∞}^{∞} |A e^{-amx^2 / \hbar}|^{2} \mathrm{d}x = 1
A^2\int_{-∞}^{∞} e^{-2amx^2 / \hbar} \mathrm{d}x = 1

The example I'm looking at suddenly have 2 in front.
2A^2\int_{-∞}^{∞} e^{-2amx^2 / \hbar} \mathrm{d}x = 1

Then,

2 A^2 \left(\frac{1}{2}\sqrt{\frac{\pi}{\frac{2am}{\hbar}}} \right)= 1

I assume the ones on the parenthesis is the integral. Any help understanding this more?
 
  • #10
jhosamelly said:
How would you take the derivative of this?


\int^{∞}_{0} e ^{\frac{-2amx^2}{\hbar}}


What's the trick in doing integrals having infinity as one of its limit? Or what if the limit is from ∞ to -∞?

It's not clear what the variable of integration is in this expression.

And, take the derivative w.r.t. which variable?
 
  • #11
jhosamelly said:
The example I'm looking at suddenly have 2 in front.
2A^2\int_{-∞}^{∞} e^{-2amx^2 / \hbar} \mathrm{d}x = 1

The lower limit was probably changed to zero, which is what I mentioned in #8: The integrand is even, so

\int_{-a}^a f(x) \mathrm{d}x = F(a)-F(-a) = F(a) -(-F(a)) = 2F(a)

holds. The book/material probably lists or assumes (maybe even proves!) the result \int_0^\infty e^{-rx^2} \mathrm{d}x=\frac{\sqrt{\pi}}{2\sqrt{r}} or something similar. Using that,

A^2 (\int_{-\infty}^{\infty} e^{-rx^2} \mathrm{d}x) = A^2(2\int_0^\infty e^{-rx^2} \mathrm{d}x)

(because of the symmetric interval & evenness)

= A^2 (2 \frac{\sqrt{\pi}}{2\sqrt{r}})= 2A^2 (\frac{1}{2} \frac{\sqrt{\pi}}{\sqrt{r}})

Did that help at all?
 
  • #12
DeIdeal said:
The lower limit was probably changed to zero, which is what I mentioned in #8: The integrand is even, so

\int_{-a}^a f(x) \mathrm{d}x = F(a)-F(-a) = F(a) -(-F(a)) = 2F(a)

holds.


YES!

Did that help at all?


Certainly! Thanks!
 
  • #13
jhosamelly said:
How would you take the derivative of this? \int^{∞}_{0} e ^{\frac{-2amx^2}{\hbar}}What's the trick in doing integrals having infinity as one of its limit? Or what if the limit is from ∞ to -∞?

These are known as Gaussian Integrals, which are integration over Gaussian function. I can perceive that you did Griffiths Quantum Mechanics. Make sure you even learn about Gamma functions and few other special functions which you come across.
 

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