Particle bound by quadratic potential

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Homework Help Overview

The discussion revolves around a particle in a one-dimensional quadratic potential, specifically described by the potential V(x) = (1/2)kx^2. The original poster seeks to determine a constant 'a' such that the wave function \psi(x) = Aexp(-x^2/2a^2) represents an energy state, and also to find the energy of the particle.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss setting up the Schrödinger equation and equating the left-hand and right-hand sides to find 'a'. There are questions about the implications of the wave function being an energy state and how to proceed when the energy E is unknown.

Discussion Status

Some participants have provided guidance on how to manipulate the equations derived from the wave function and the Schrödinger equation. There is an ongoing exploration of the conditions under which the derived equation holds for all x, and the discussion includes clarifications about the notation used in integrals.

Contextual Notes

Participants are navigating the challenge of determining constants in the context of quantum mechanics without having explicit values for energy. The discussion also touches on the nuances of mathematical notation in the context of integrals.

kasse
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Homework Statement



A particle that can move in one dimension and that is in a stationary state, is bound by a potential V(x) = (1/2)kx^2. The wave function is \Psi(x,t) = \psi(x)exp(-iEt/\hbar)

We look at a state in which \psi(x) = Aexp(-x^2/2a^2a^2), where a is a constant and A is the normalisation constant. Determine a so that \psi(x) is an energy state. What is the energ of the particle?

The Attempt at a Solution



I don't really know what to do here, but setting up the wave equation tends to be a good start:

H\psi(x) = E\psi(x), where H = -(\hbar^2/2m)(d^2/dx^2) + kx^2/2

How can I determine a so that \psi(x) is an energy state?
 
Last edited:
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Just calculate the left-hand and right-hand sides, and set them equal.
 
That the wave function is an energy state simply means that it's described by the Schrödinger equation?
 
Yes, it's a solution to the *time-independent* SE, to be precise.
 
OK, but I still don't see how to find a when E is unknown. My expression after differentiating twice is:

(\hbar^2/2ma^2) (A - x^2/a^2) + kx^2/2 = E
 
First, you didn't calculate it right.

Second, the correct equation you'll get will have to be true for every x.
 
Now I ended up with

(\hbar^2/2ma^2)(1 - x^2/a^2) + kx^2/2 = E

What I should do here is to eliminate x so that the equation holds for all x-es? In that case, a must be (\hbar^2/km)^0.25
 
Your equation is now of the form (if you move E to the left-hand side)

C+Dx^2=0,

where C and D are constants (independent of x).
If this is to be true for all x, then both C and D must be zero.
 
I got it right now, didn't I?

My next problem is to calculate the expectation value. That's not hard, I just wonder why the integral is written

\intdx \psi*(x)x\psi(x)

and not

\int \psi*(x)x\psi(x) dx
 
Last edited:
  • #10
In this case it doesn't matter where you put the "dx", it is the same thing.

(note that there are cases where it DOES matter; e.g. if dx is a vector)
 

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