Identical Particles in Harmonic Potential: Hamiltonian & Ground State

In summary, the ground state energy of a simple harmonic oscillator is \frac{1}{2}\hbar\omega. All 2N fermions in the system have an energy equal to this ground state energy.
  • #1
Urvabara
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0

Homework Statement



There are identical particles in a harmonic potential [tex]V(x)=\frac{1}{2}m\omega^{2}x^{2}[/tex]. The number of particles is 2N, where N is a positive integer.

Homework Equations



a) What is the system's Hamilton's operator for bosons in the second quantization? How about the fermions?

b) What is the energy of the ground level, if the particles are i) S = 0 bosons, ii) S = 1/2 fermions?

c) Write the state vector of the ground level for S = 0 bosons and S = 1/2 fermions using creation and annihilation operators to vacuum.

The Attempt at a Solution



a) I have no idea... :cry:

b) Maybe I have to solve the Schrödinger's Equation, and using boudary conditions (?) solve the equation for energy E. There are 2N bosons all in the ground state, because Pauli's Exclusion Principle does not hold for bosons. So, I just put n = 1 to the E-equation and multiply it by 2N. Right? :uhh:

How about fermions? The Pauli Exclusion Principle holds for them, at least... :confused:

c) I have no idea... :cry:
 
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  • #2
You look very confused, have you comprehended your notes completely, before trying the qeustions?

to answer this question, you need to know what are energy levels of harmonic oscillator, the fact that no two fermions can occupy one energy level, and all bosons can occupy one energy level.

then you need to know how to use Fock space, the difference with Hilbert space (tensor products of hilbert spaces). A ket in Fock space contains numbers that tell you how many particles occupy what energy level.

Then you need to know the creation and annihilations operators, Fermionic and Bosonic, a creation operator labeled by an energy level creates a particle at at energy level. What commutation, anti-commutation relations these operators satisfy.

e.g. one particle at energy level 1, another at energy level 2
the Hamiltonian should be E1 a1^dagger a1 + E2 a2^dagger a2
 
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  • #3
(b) What is the ground state energy of a single simple harmonic oscillator? [You might want to memorize this expression. Memorize the expression for all the higher energy levels too.] Now, the bosonic case, if there are 2N particles all of which are in the single-particle ground state then they all have an energy equal to the ground state energy of a single simple harmonic oscillator. Hence what is the total energy of the system?
 
  • #4
(a) your teacher should have given you a general form of the hamiltonian "in second quantization" for a given potential V. Something along the lines of
[tex]
H=\int d^3x\psi^{\dagger}(\vec x)\left(
\frac{-\nabla^2\hbar^2}{2m}+V(\vec x)
\right)\psi(\vec x)
[/tex]
where psi and psi-dagger are particle annihilation and creation fields, respectively.
 
  • #5
(c) the creation and annihilation operators mentioned about can be expanded in terms of operators which create particles not at a given position, but rather in a given mode of the single-particle Hamiltonian. These mode-creation and annihilation operators are what you use to do this problem.
 
  • #6
The ground state energy of a simple harmonic oscillator is [tex]\frac{1}{2}\hbar\omega[/tex].

The energy levels of a simple harmonic oscillator are given by
[tex](n+\frac{1}{2})\hbar\omega,\qquad n=0,1,2,...[/tex]

a) for bosons: [tex]H=2NE_{1}a_{1}^{\dagger}a_{1}[/tex]?
b) for S = 0 bosons: [tex]E=2N\cdot\frac{1}{2}\hbar\omega = N\hbar\omega[/tex]?
 
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  • #7
(b) correct.
(a) incorrect.
 
  • #8
b) For S=1/2 fermions: There are two fermions in the ground state. Right?
So, the energy is [tex]E=2\cdot\frac{1}{2}\hbar\omega = \hbar\omega[/tex]?
 
  • #9
Urvabara said:
b) For S=1/2 fermions: There are two fermions in the ground state. Right?
So, the energy is [tex]E=2\cdot\frac{1}{2}\hbar\omega = \hbar\omega[/tex]?

...that's the energy of those 2. There are 2N-2 more that you have to take into account. The next 2 may not be in the lowest state, but you can put them in the next lowest state with energy [tex]3/2\hbar\omega[/tex].

Those next 2 together contribute an energy [tex]3\hbar\omega[/tex].

So, for the first 4 the energy is [tex]\hbar\omega + 3\hbar\omega[/tex], but there are still 2N-4 more to take into account.

Now just keep on filling up the states until you have put all 2N fermions into the lowest N energy levels.
 
  • #10
Yes. Yes, of course! Thanks! :)
 

1. What is the Hamiltonian of identical particles in a harmonic potential?

The Hamiltonian is a mathematical operator that represents the total energy of a system. In the case of identical particles in a harmonic potential, the Hamiltonian can be written as H = ∑i=1N (pi2/2m + ½ kxi2), where N is the number of particles, pi is the momentum of particle i, m is the mass of the particles, k is the force constant of the harmonic potential, and xi is the displacement of particle i from its equilibrium position.

2. What is the ground state of identical particles in a harmonic potential?

The ground state is the lowest energy state that a system can have. In the case of identical particles in a harmonic potential, the ground state is when all the particles are in their lowest energy states, with each particle having a harmonic oscillator wavefunction centered at the equilibrium position of the potential. This state is also known as the quantum mechanical ground state or the zero-point energy state.

3. What is the significance of the ground state in this system?

The ground state is significant because it represents the most stable and lowest energy state of the system. It is also important in understanding the behavior of the system as it provides a baseline or starting point for analyzing the excited states of the particles.

4. How does the Hamiltonian affect the ground state of identical particles in a harmonic potential?

The Hamiltonian determines the energy of the particles in the system, including the ground state. As the Hamiltonian is an operator, it affects the ground state by determining the probability of finding the particles in certain energy states, which is represented by the wavefunction. The lower the energy of the Hamiltonian, the more likely it is for the particles to be in the ground state.

5. Can the ground state of identical particles in a harmonic potential be degenerate?

Yes, the ground state can be degenerate, which means that there are multiple states with the same lowest energy. In the case of identical particles in a harmonic potential, this can occur when the particles are in a state of superposition, meaning that they can be found in multiple energy levels simultaneously. However, the degeneracy of the ground state is dependent on the specific conditions and parameters of the system.

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