For a particle on a sphere, is zero energy possible?

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blaisem
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In my introduction to quantum mechanics, I learned about the particle in a box, followed by the quantum harmonic oscillator. In both instances, zero energy was not possible; the ground states had non-zero energy.

However, in deriving the solutions to the Schrödinger equation for a particle on a field-free sphere, the energy was found proportional to:

E ∝ (l2 + l )

Furthermore, the ground-state spherical harmonic corresponds to l = 0, which does indeed yield zero energy as the eigenvalue of the hamiltonian. Since the particle is confined to the surface of the sphere, dρ = 0, and the radial component also contributes zero energy.

Questions:
  1. Doesn't zero energy violate the uncertainty principle?
  2. For a particle in a box, n = 0 was not allowed because it violated the uncertainty principle—why then is l = 0 permitted for a particle on a sphere?
Thank you!
 
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I haven't checked your solution to confirm that it does yield zero energy, but...
blaisem said:
Doesn't zero energy violate the uncertainty principle?
No, just as any other eigenstate of the Hamiltonian doesn't violate the uncertainty principle. Prepare the system in such a state and it won't (in general) be in an eigenstate of any operator that doesn't commute with the Hamiltonian - and that's all that the uncertainty principle requires.
For a particle in a box, n = 0 was not allowed because it violated the uncertainty principle—why then is l = 0 permitted for a particle on a sphere?
The problem with ##n=0## for a particle in a box isn't that it violates the uncertainty principle, it is that that wave function is zero everywhere when ##n=0##.
 
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blaisem said:
In my introduction to quantum mechanics, I learned about the particle in a box, followed by the quantum harmonic oscillator. In both instances, zero energy was not possible; the ground states had non-zero energy.

However, in deriving the solutions to the Schrödinger equation for a particle on a field-free sphere, the energy was found proportional to:

E ∝ (l2 + l )

Furthermore, the ground-state spherical harmonic corresponds to l = 0, which does indeed yield zero energy as the eigenvalue of the hamiltonian. Since the particle is confined to the surface of the sphere, dρ = 0, and the radial component also contributes zero energy.

Questions:
  1. Doesn't zero energy violate the uncertainty principle?
  2. For a particle in a box, n = 0 was not allowed because it violated the uncertainty principle—why then is l = 0 permitted for a particle on a sphere?
Thank you!

The value of energy depends on the arbitrary energy of your potential. You can always add a constant. There's no physical significance to zero energy.

For example, taking electric potential energy to be zero at infinity, the ground state of hydrogen has an energy of ##-13.6eV##. If you take the potential to be ##13.6eV## at infinity, then the ground state would have zero energy.
 
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Well being on a sphere then physical chemistry comes into it and you have stuff like van der Waals forces etc. I would not even guess at a solution without more detail.

Thanks
Bill
 
Even a particle constrained on a circular path on 2d plane, with Hamiltonian

##H=-\frac{\hbar^2}{2mR^2}\frac{\partial^2}{\partial \theta^2}##

has an energy eigenfunction ##\psi(\theta)## which is a ##\theta##-independent constant and is therefore most conveniently described as having zero energy.

The difference to a particle in a box is that here the boundary condition doesn't require the wave function to be zero at any points, it only requires ##\psi(\theta)## to be continuous.

The free-particle eigenstates have been studied for many different topologies, like particle on a torus or even on a Möbius strip.
 
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Indeed, and it's always important to remember that for a particle on a sphere the translations are the rotations, i.e., you have angular momentum. Also note that position observables are at least problematic on the sphere. So there's no analogue of the position-momentum uncertainty relation for a particle on a sphere, and thus zero energy for a free particle is no contradiction to any well-defined uncertainty relation (e.g., between the components of angular momentum).
 
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