Infinite square potential well

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SUMMARY

The discussion centers on solving the Schrödinger equation for a quasielectron in an infinite square potential well, specifically within a quantum dot device where the potential V(x) = 0 for 0 ≤ x < L and infinite otherwise. Participants emphasize the importance of boundary conditions, particularly noting that ψ(L) = 0 due to the infinite potential at L. The challenge lies in determining the second boundary condition at x = 0, where the potential is zero, leading to confusion about the wavefunction's behavior at that point. Ultimately, it is concluded that sketching the ground-state probability density does not require solving for ψ, but understanding the ground state of the infinite square well is essential.

PREREQUISITES
  • Understanding of the Schrödinger equation and its application in quantum mechanics.
  • Familiarity with concepts of quantum dots and potential wells.
  • Knowledge of boundary conditions in quantum systems.
  • Basic principles of probability density in quantum mechanics.
NEXT STEPS
  • Study the ground state wavefunction of the infinite square well.
  • Learn how to apply boundary conditions in quantum mechanics.
  • Explore the concept of probability density and its calculation in quantum systems.
  • Investigate the properties and applications of quantum dots in modern physics.
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Students and educators in quantum mechanics, physicists working with quantum dots, and anyone interested in the foundational principles of quantum systems and their mathematical descriptions.

whatisreality
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Homework Statement


I think this is a square well potential problem. The question asks me to sketch the ground-state probability density, for the following situation:

A quasielectron moves in a 'quantum dot' device. The potential V(x) = 0 for 0 ≤ x < L, and is infinite otherwise.

Homework Equations

The Attempt at a Solution


I'm going to need to solve the Schrödinger equation within the device. I have no idea what a quantum dot is, but presumably it doesn't actually matter! I think you can just treat it like an infinite square potential. The Schrödinger equation is

##-\frac{\hbar^2}{2m} \frac{\partial \psi}{\partial x^2} = E \psi##
Within the device. And I also need boundary conditions. One of these boundary conditions is ##\psi(L)=0##, since the potential is infinite at L. Annoyingly, the potential is 0 at x=0, so I can't use the same reasoning there. So my first question is, how do I get my second boundary condition? I don't see how the potential being zero at x=0 in any way restricts what ##\psi## could be...
 
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A. I wouldn't solve anything. It says "sketch".

B. If I were going to solve something, I'd make the problem more symmetric.
 
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Vanadium 50 said:
A. I wouldn't solve anything. It says "sketch".

B. If I were going to solve something, I'd make the problem more symmetric.
Don't I need to calculate the probability density in order to sketch it?
 
whatisreality said:
And I also need boundary conditions. One of these boundary conditions is ##\psi(L)=0##, since the potential is infinite at L. Annoyingly, the potential is 0 at x=0, so I can't use the same reasoning there. So my first question is, how do I get my second boundary condition? I don't see how the potential being zero at x=0 in any way restricts what ##\psi## could be...

Specifying ##V(x) = 0 \ (0 \le x < 1)## is equivalent to ##V(x) = 0 \ (0 < x < 1)##.
 
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PeroK said:
Specifying ##V(x) = 0 \ (0 \le x < 1)## is equivalent to ##V(x) = 0 \ (0 < x < 1)##.
Why? In the first inequality V(x) is zero at x = 0, but in the second inequality the potential is infinite at x = 0. So I can't say that at x = 0, the wavefunction is zero, and I don't know where else to get a second boundary condition from.
 
whatisreality said:
Why? In the first inequality V(x) is zero at x = 0, but in the second inequality the potential is infinite at x = 0. So I can't say that at x = 0, the wavefunction is zero, and I don't know where else to get a second boundary condition from.

Whether the boundary points are in or out doesn't affect the functions or the integrals. If the wavefunction is not ##0## at ##x=0## then it is discontinuous when viewed as a function for all ##x##.
 
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PeroK said:
Whether the boundary points are in or out doesn't affect the functions or the integrals. If the wavefunction is not ##0## at ##x=0## then it is discontinuous when viewed as a function for all ##x##.
So if I said the wavefunction is zero at x = 0, then I'm excluding the electron from being at x = 0, even though at x = 0 the potential is zero... that's ok? I thought it would have something to do with continuity! I was trying to find a way to use the derivative of ##\psi##.

Vanadium's post makes it sound like I don't actually need to solve for ##\psi## though to sketch the probability distribution. I know it's zero at the edges, but don't I need to integrate the magnitude between infinity and negative infinity to work out the probability density? How could I sketch it without an equation?
 
whatisreality said:
So if I said the wavefunction is zero at x = 0, then I'm excluding the electron from being at x = 0, even though at x = 0 the potential is zero... that's ok? I thought it would have something to do with continuity! I was trying to find a way to use the derivative of ##\psi##.

Vanadium's post makes it sound like I don't actually need to solve for ##\psi## though to sketch the probability distribution. I know it's zero at the edges, but don't I need to integrate the magnitude between infinity and negative infinity to work out the probability density? How could I sketch it without an equation?

Yes. I suspect whover set the question didn't give it a second thought!
 
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PeroK said:
Yes. I suspect whover set the question didn't give it a second thought!
I know I'd only actually have to integrate between L and 0, and it should equal 1. And it's zero at both edges. Where does the whole 'ground state' thing come into it, anyway?

If this is actually a really easy question, I must be missing some fairly basic information.
 
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whatisreality said:
I know I'd only actually have to integrate between L and 0, and it should equal 1. And it's zero at both edges. Where does the whole 'ground state' thing come into it, anyway?

Are you supposed to know the ground state of the infinite square well? If not, then to sketch it, you'd have to solve the Schrödinger equation, I imagine.
 
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  • #11
PeroK said:
Are you supposed to know the ground state of the infinite square well? If not, then to sketch it, you'd have to solve the Schrödinger equation, I imagine.
OK. We haven't done anything specifically about ground states of infinite square wells. I'd better solve the Schrödinger equation then!
 
  • #12
whatisreality said:
OK. We haven't done anything specifically about ground states of infinite square wells. I'd better solve the Schrödinger equation then!

It can't do any harm!
 
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