What is the Constant λ in the Wave Equation for Normalising the Wavefunction?

Click For Summary

Homework Help Overview

The discussion revolves around determining the constant λ in the wave equation for a wavefunction, specifically in the context of normalizing the wavefunction. The equation provided involves parameters related to quantum mechanics, including mass and angular frequency.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the normalization of the wavefunction and the implications of complex constants. There are attempts to derive the normalization condition and questions about the correctness of mathematical steps taken. Some participants suggest starting from the definition of the wavefunction's modulus squared.

Discussion Status

The discussion is ongoing, with various interpretations and approaches being explored. Some participants have offered guidance on how to approach the normalization process, while others are questioning the assumptions made regarding the constants involved.

Contextual Notes

There is mention of using standard integrals and the need for assumptions about the parameters involved. The complexity of the wavefunction and its normalization is a central theme, with participants noting the potential for complex values of constants.

ParoxysmX
Messages
21
Reaction score
0

Homework Statement


Determine the constant λ in the wave equation

\Psi(x) = C(2a^2 x^2 + \lambda)e^{-(a^2 x^2/2)}

where a=\sqrt{mω/\hbar}

Homework Equations



Some standard integrals I guess

The Attempt at a Solution



So I believe the wave equation just needs to be normalised. Using the usual conditions for normalisation,

(C2a^2 + C\lambda)^2 \int^{∞}_{-∞} | x^2 e^{-(a^2 x^2/2)} + e^{-(a^2 x^2/2)} |^2 dx =1

From there,

(C2a^2 + C\lambda)^2 \int^{∞}_{-∞} |2x^2 e^{-(a^2 x^2/2)}|^2 dx =1

Then squaring the function inside the integral and moving the '4' outside the integral as it is a constant,

4(C2a^2 + C\lambda)^2 \int^{∞}_{-∞} x^4 e^{-(a^2 x^2)} dx =1

Now that should be a standard integral but I don't know any involving an x term to the fourth power. Or perhaps I've done something else wrong?
 
Physics news on Phys.org
ParoxysmX said:
(C2a^2 + C\lambda)^2 \int^{∞}_{-∞} | x^2 e^{-(a^2 x^2/2)} + e^{-(a^2 x^2/2)} |^2 dx =1
Since when is
$$
[(ab+c) d]^2 = (a+c)^2(bd+d)^2
$$

The next step is also completely wrong. Start again from ##|\psi|^2 = \psi^* \psi##. You should also allow ##C## and ##\lambda## to be complex.
 
If the function doesn't contain any complex exponentials, then \psi^{*} is the same as \psi, isn't it?
 
As all physical observables depend ultimately on ##| \psi |^2##, the wave function of a physical system is only defined up to a complex phase. In other words, ##\psi## and ##\psi e^{i \delta}##, with ##\delta## real, decribe the same thing. Therefore, you can choose the normalization constant ##C## in
$$
\psi(x) = C f(x)
$$
to be real, because if it is complex, you can always do a rotation in the complex plane such that ##C' = C e^{i \delta}## is real.

But you also have the ##\lambda## in there and, unless told otherwise, you can't assume that it is real. You should appraoch the problem without restricting ##C## or ##\lambda## to be real, and see what you get.
 
use Maple to do the follow step:

assume(a>0)

int(C*(2*a^2*x^2+B)*exp(-(a^2*x^2)/2),x=-infinity..infinity)

where B is your λ. then we can get the result is
(B+2)*C*(2*Pi)^0.5/a

I hope this can help you
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 1 ·
Replies
1
Views
4K
  • · Replies 8 ·
Replies
8
Views
1K
  • · Replies 7 ·
Replies
7
Views
3K
Replies
3
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K