Why is the ground state always symmetric?

In summary, the ground state of a system with a potential is always symmetric, but the first excited state can be either symmetric or anti-symmetric.
  • #1
jasony
11
0

Homework Statement


Why is the ground state always symmetric and first excited state anti-symmetric?
OR Why does the ground state always have no node and first excited state has one node?

Homework Equations


The Attempt at a Solution

 
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  • #2
This is not true in general. The ground state is symmetric only for symmetric potentials.

As to why exactly this is the case, I've seen some sketchy proofs, but I cannot offer anything deep. Perhaps the next poster will have a better response.
 
  • #3
jasony said:

Homework Statement


Why is the ground state always symmetric and first excited state anti-symmetric?
OR Why does the ground state always have no node and first excited state has one node?

Homework Equations





The Attempt at a Solution


I think you should consider a more specific example .. because the situation would be different (i.e) for different boundaries ..

say you have a particle in a box, and the length is from x = 0 to x = a .. when you solve the Schrodinger equation you will end up with a solution that is neither even nor odd ..

but if the length is from x = -a/2 to x = a/2 .. then for n=1,3,5.. it is even (symmetric) and for n=2,4,6... is it odd (antisymmetric)
 
  • #4
But generally speaking, is it true that ground state must have no node? Why?
 
  • #5
The greater the curvature of a wave function, the more kinetic energy that it has. Wave functions with nodes have more curvature than nodeless wave functions. Since we are trying to minimize the energy, it makes sense to me that wave functions with no nodes would be good candidates to be the ground state so long as the potential energy doesn't make them have greater total energy than wave functions with nodes. This certainly isn't a proof, but hopefully it helps.
 
  • #6
Anyone knows any simple proof?
 
  • #7
im not sure if that would help..

a symmetric function is such a function which has the property f(x)=f(-x) .. and the antisymmertric f(x) = - f(-x) ..
 
  • #8
I think that second way that jasony phrased his question is really more of what he is aiming for: why does the ground state have no nodes? Correct me if I'm wrong jasony.
 
  • #9
yes why does the ground state has no node? Can anyone provide a simple maths proof?
 
  • #10
Hi, I know this is an old thread, but I have a simple Hamiltonian whose ground state is anti-symmetric.

[tex]H=\left[\begin{array}{cc}0 & \Delta\\\Delta & 0\end{array}\right]\,.[/tex]

Eigenstates and eigenenergies are:

[tex]\psi_{\eta}=\left[\begin{array}{c}1\\ \eta\end{array}\right]\,,\quad\varepsilon_{\eta}=\eta\Delta\,,[/tex]

where [itex]\eta=\pm 1[/itex]. The ground state corresponds to [itex]\eta=-1[/itex], which is anti-symmetric.
 
  • #11
Badphysicist is on the right track.

The Schrodinger Equation in one dimension can be written as

[tex]\frac{d^2 \psi}{dx^2}+k^2 \psi=0[/tex]

where

[tex]k^2=\frac{2m(E-V)}{\hbar^2}[/tex]

For the ground state, lowest energy means lowest possible value of k.
Lowest possible value of k means longest possible value of the sinusoidal wavelength inside the well.
A wavefunction with a node has shorter wavelength than a wavelength with no nodes.
That's why.
 
Last edited:
  • #12
Well, that demonstrates that the ground-state for the 1D Schroedinger equation in a piece-wise constant potential contains no nodes. If that's the OP's question then you can simply solve the SE and verify that the ground state indeed contains no nodes.

If you want to prove that it's true in the case of, say [itex]H=\sum_i\left\{-\nabla^2_i+V(\vec{r_i})\right\} + \sum_{i\neq j}U(\vec{r_i}, \vec{r_j})[/itex] (or any Hamiltonian you can write down) then it's not so easy to show that the ground state really contains no nodes as far as I'm aware - although it is true.

You can look at appendix A of this thesis http://thesis.library.caltech.edu/1007/ for some hints of how this might be proven in the case of a single particle.

Also try looking for the derivations of the equations used in DFT. I'm not sure if that's so useful, but they relate the ground state energy of a system its particle density, so you might find from these equations that for some reason the ground state never contains a nodal point.
 
  • #13
jpr0 said:
Hi, I know this is an old thread, but I have a simple Hamiltonian whose ground state is anti-symmetric.

[tex]H=\left[\begin{array}{cc}0 & \Delta\\\Delta & 0\end{array}\right]\,.[/tex]

Eigenstates and eigenenergies are:

[tex]\psi_{\eta}=\left[\begin{array}{c}1\\ \eta\end{array}\right]\,,\quad\varepsilon_{\eta}=\eta\Delta\,,[/tex]

where [itex]\eta=\pm 1[/itex]. The ground state corresponds to [itex]\eta=-1[/itex], which is anti-symmetric.

its the how of the question. not the why?
 
  • #14
i think answer is simple. ground state is n=0 that is even. first excited stat is n=1 odd.


by the way you can use ladder operators.
 

1. Why is the ground state always symmetric?

The ground state, also known as the lowest energy state, is always symmetric because of the fundamental principles of quantum mechanics. In quantum mechanics, particles are described by wave functions, and the ground state is the state in which the wave function has the lowest energy. Symmetry is a fundamental aspect of wave functions, and in order for the ground state to have the lowest energy, it must also be symmetric.

2. How does symmetry affect the ground state?

Symmetry plays a crucial role in determining the energy level of the ground state. In quantum mechanics, symmetrical states have lower energy levels compared to asymmetrical ones. This means that the ground state, being the state with the lowest energy, must also be symmetrical.

3. Can the ground state be asymmetrical?

No, the ground state cannot be asymmetrical. As mentioned before, the ground state is always the state with the lowest energy, and in quantum mechanics, symmetrical states have lower energy levels. Any asymmetrical state would have a higher energy level, making it not the ground state.

4. What happens if the ground state is not symmetric?

If the ground state is not symmetric, it would not be the lowest energy state. This means that the system would not be in its most stable state, and it would be susceptible to changes and fluctuations. In order for a system to be in its most stable state, the ground state must be symmetric.

5. Is there any exception to the rule that the ground state is always symmetric?

No, there are no exceptions to this rule. The ground state is always symmetric because of the fundamental principles of quantum mechanics. Symmetry is a fundamental aspect of wave functions, and in order for the ground state to have the lowest energy, it must also be symmetric.

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