Particles with Spin in a Box - Energy Levels

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Homework Help Overview

The discussion revolves around a problem involving five particles in a box with various spins (0, ½, 1, 3/2) and the determination of their ground and excited state energies. The context is set within quantum mechanics, specifically dealing with the energy levels of particles in an infinite potential well.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants explore the calculation of ground state energies for different spins, questioning the treatment of particles as bosons or fermions. There is discussion about the occupancy of energy levels based on the spin values and the implications for calculating total energy.
  • Some participants express uncertainty about moving particles to excited states and whether multiple particles need to be moved or just one, leading to further clarification on the exclusion principle and energy level occupancy.

Discussion Status

The conversation is ongoing, with participants providing feedback on each other's calculations and reasoning. Some guidance has been offered regarding the correct approach to calculating energies and the configuration of particles in excited states, but there is still a lack of consensus on certain aspects, particularly regarding the treatment of fermions and bosons in this context.

Contextual Notes

There are mentions of confusion regarding the number of allowed states for particles based on their spin and the implications for energy calculations. Participants are also navigating the rules of occupancy for different spins, which affects how they approach the problem.

erok81
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Homework Statement



This is a two part problem. I think I am pretty close, but I'm quite understanding it. Which sucks because this is probably an extremely easy question.:frown:

I have five particles in a box with S spin. I am to find the ground state of the five particles if they have spin 0,½,1,3/2.

Homework Equations



My energy in box (infinite potential well) is given by:

E=\frac{n^2 \pi^2 \hbar^2}{2mL^2}

The Attempt at a Solution



For S=0,1 all particles are Bosons and therefore can all fit in the same level. Therefore my ground state energy is given by:

E= \frac{5 \cdot 1^2 \pi^2 \hbar^2}{2mL^2}~=~ \frac{5 \pi^2 \hbar^2}{2mL^2}

For my S=½ I can fit 2n2 where the factor of two arises because the allowed states are doubles since I can fit ± 1/2 spins per level. Since I have five particles, I will occupy up to n=2. Therefore my ground state energy is given by:

E= \frac{2(n_{1}^{2}+n_{2}^{2}) \pi^2 \hbar^2}{2mL^2}~=~ \frac{5 n^2 \pi^2 \hbar^2}{mL^2}

And finally for my S=3/2 I can fit a factor of 4 per level (±3/2,±1/2). Using the same justification as in S=½ I arrive at the ground energy of:

E= \frac{10 n^2 \pi^2 \hbar^2}{2mL^2}

Since the first level will contain four particles and n=2 will have one.

First. Is this correct so far?

The next part is where I am having the most trouble.

I have to find the excited state for all spins in the first half.

I know in order to do this I only need to move one particle to the next energy level. So for S=1,0 I think I have it. They are all in the ground state and only one needs to move up - four stay in the ground state and one moves up. Therefore I have.

E=\frac{4 \cdot 1^2 \pi^2 \hbar^2}{2mL^2}+\frac{2^2 \pi^2 \hbar^2}{2mL^2}~=~ \frac{4 n^2 \pi^2 \hbar^2}{mL^2}

Is this looking okay so far?

That's about as far as I am comfortable with. The next spin I tried was S=½.

Here I have two particles in n=1 and three particles in n=2. Similar to the above case I only need to move one particle up. So I would have two in n=1, two in n=2, and one in n=3 to raise it to the first excited state. I know that much, but when I try to write it out, I am stuck. I think it's that factor of two that throws me off. I don't know if I should include it in each level.

So how does the work look so far? Am I even close?
 
Last edited:
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erok81 said:

Homework Statement



This is a two part problem. I think I am pretty close, but I'm quite understanding it. Which sucks because this is probably an extremely easy question.:frown:

I have five particles in a box with S spin. I am to find the ground state of the five particles if they have spin 0,½,1,3/2.

Homework Equations



My energy in box (infinite potential well) is given by:

E=\frac{n^2 \pi^2 \hbar^2}{2mL^2}

The Attempt at a Solution



For S=0,1 all particles are Bosons and therefore can all fit in the same level. Therefore my ground state energy is given by:

E= \frac{5 \cdot 1^2 \pi^2 \hbar^2}{2mL^2}~=~ \frac{5 \pi^2 \hbar^2}{2mL^2}

For my S=½ I can fit 2n2 where the factor of two arises because the allowed states are doubles since I can fit ± 1/2 spins per level. Since I have five particles, I will occupy up to n=2. Therefore my ground state energy is given by:

E= \frac{2(n_{1}^{2}+n_{2}^{2}) \pi^2 \hbar^2}{2mL^2}~=~ \frac{5 n^2 \pi^2 \hbar^2}{mL^2}

And finally for my S=3/2 I can fit a factor of 4 per level (±3/2,±1/2). Using the same justification as in S=½ I arrive at the ground energy of:

E= \frac{10 n^2 \pi^2 \hbar^2}{2mL^2}

Since the first level will contain four particles and n=2 will have one.

First. Is this correct so far?
No, you didn't get the fermions right. There's only one spatial state for each n for the particle in the box, not n2 states. You're thinking of the hydrogen atom.
The next part is where I am having the most trouble.

I have to find the excited state for all spins in the first half.

I know in order to do this I only need to move one particle to the next energy level. So for S=1,0 I think I have it. They are all in the ground state and only one needs to move up - four stay in the ground state and one moves up. Therefore I have.

E=\frac{4 \cdot 1^2 \pi^2 \hbar^2}{2mL^2}+\frac{2^2 \pi^2 \hbar^2}{2mL^2}~=~ \frac{4 n^2 \pi^2 \hbar^2}{mL^2}

Is this looking okay so far?

That's about as far as I am comfortable with. The next spin I tried was S=½.

Here I have two particles in n=1 and three particles in n=2. Similar to the above case I only need to move one particle up. So I would have two in n=1, two in n=2, and one in n=3 to raise it to the first excited state. I know that much, but when I try to write it out, I am stuck. I think it's that factor of two that throws me off. I don't know if I should include it in each level.

So how does the work look so far? Am I even close?
 
Ok...that's what I originally thought, but got off track looking around on Wikipedia.

So disregard my fermions above. New energies given by:

spin-1/2 I can have two per energy level. Therefore I need three energy levels to get all five.

<br /> E=\frac{(1^2+2^2+3^2) \pi^2 \hbar^2}{2mL^2}~=~ \frac{15 \pi^2 \hbar^2}{2mL^2}<br />

Then for my spin-3/2 I can have four per level. Therefore I only need two levels for all five particles.

<br /> E=\frac{(1^2+2^2) \pi^2 \hbar^2}{2mL^2}~=~\frac{5 \pi^2 \hbar^2}{2mL^2}<br />

Does that look better?
 
Yes, that's right.
 
For the next part, to get to the next energy (spin-1/2) I will need to move two particles, right? Since I can't only move the one currently in n=3, since that will leave n=3 empty.

At the ground state I have two in n=1, two in n=2, and one in n=3.

The first excited state I would need two in n=1, one in n=2, one in n=3, and one in n=4?
 
No, you should only have to move one. The only restriction is you can't end up with 3 particles in the same state.
 
Ooooh so it doesn't necessarily have to start a new energy level (like I did with n=4) just that one particle needs to move up an energy level. Of course keeping to the exclusion rule.

So in that case I'd only need to move one from n=2 to n=3.

Then I'd have two in n=1, one in n=2, and two in n=3?
 
Yes. You didn't explicitly state it, but I assume you were looking for the configuration with the next lowest energy level after the ground state. If you're just looking for any excited state, you could bump any of the particles up as long as you don't end up with 3 with the same n.
 
Yeah, sorry. I am looking for the first excited state. In this case spin-1/2

I tried to write it out, but I'm not sure how to show this with my energy equation.

My ground state energy for spin-1/2 is

<br /> <br /> E=\frac{(1^2+2^2+3^2) \pi^2 \hbar^2}{2mL^2}~=~ \frac{15 \pi^2 \hbar^2}{2mL^2}<br /> <br />

I am still only occupying the same energy levels as the ground state (n=1,2,3). Except now I have one less particle in n=2 and one more in n=3.

So unless my ground state is wrong, I don't see how it will change.
 
  • #10
Sorry, I was mistaken in post 4. The energies you listed in post 3 aren't correct. You want to sum the energies of each particle, so if you have two particles in the n=1 state, the total energy would be 2E1, for instance.
 
  • #11
Ah, okay. That makes sense now. I can also see how to bump up the energies. I'll write these out and post again.

So for the spin-1/2 would I have:

E=\frac{(2(1^2)+1(2^2)+2(3^2)) \pi^2 \hbar^2}{2mL^2}~=~ \frac{12 \pi^2 \hbar^2}{mL^2}
 
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