Potential operator in positional space

In summary, for a spinless particle, the most general Hamiltonian satisfying Galilean invariance is diagonal in the positional/space basis and not diagonal in the complementary momentum space. This holds true for both one dimensional and three-dimensional cases.
  • #1
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Is the potential operator (in positional/space basis) of the Hamiltonian always diagonal in that basis? And is the kinetic energy operator always diagonal in complementary momentum space?
 
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  • #2
For a spinless particle in one dimension, the most general Hamiltonian which satisfies Galilean invariance is

Ht = P2/2m + Vt(Q) .

So, in this case, the answer to your question is "yes".
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However, for the case of a spinless particle in three dimensions, the most general Hamiltonian which satisfies Galilean invariance is

Ht = |P - At(Q)|2/2m + Vt(Q) .

The first term on the right hand side is the "kinetic" term ... clearly, it is not diagonal in the momentum representation.
 
  • #3


The potential operator in positional space refers to the mathematical representation of the potential energy in terms of the position of a particle. It is an operator that acts on the wavefunction of a system to determine the potential energy at a given position.

The answer to whether the potential operator of the Hamiltonian is always diagonal in positional space is dependent on the specific system being studied. In some cases, the potential energy may only depend on the position of the particle, making the potential operator diagonal. However, in other cases, the potential energy may depend on other variables such as time or other parameters, making the potential operator non-diagonal.

Similarly, the kinetic energy operator in complementary momentum space may or may not be diagonal. In some systems, the kinetic energy may only depend on the momentum of the particle, making the kinetic energy operator diagonal. However, in other systems, the kinetic energy may depend on other variables such as position or spin, making the kinetic energy operator non-diagonal.

In summary, the diagonal nature of the potential and kinetic energy operators in positional and momentum space is dependent on the specific system being studied. In general, these operators can be either diagonal or non-diagonal, and it is important to consider the specific properties of the system when determining their nature.
 

FAQ: Potential operator in positional space

What is a potential operator in positional space?

A potential operator in positional space is a mathematical operator that represents the potential energy of a particle in a given position. It is typically denoted as V(x), where x is the position of the particle.

How is the potential operator related to the Hamiltonian operator?

The potential operator, along with the kinetic energy operator, is a component of the Hamiltonian operator, which represents the total energy of a system. The potential operator is responsible for accounting for the potential energy of a particle in a given position.

How is the potential operator used in quantum mechanics?

In quantum mechanics, the potential operator is used to calculate the energy states of a particle in a given position. It is an essential component in solving the Schrödinger equation and predicting the behavior of quantum systems.

Can the potential operator be applied to systems with multiple particles?

Yes, the potential operator can be applied to systems with multiple particles. In this case, the operator becomes a function of the positions of all the particles and is denoted as V(x1, x2, ..., xn).

How is the potential operator different from the potential function?

The potential operator is a mathematical operator that acts on a wave function to determine the potential energy of a particle in a given position. The potential function, on the other hand, is a mathematical function that describes the potential energy of a system as a function of position. While the potential operator is used in quantum mechanics, the potential function is more commonly used in classical mechanics.

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