Momentum Operator w/ Dirac Delta Potential: Justification

In summary, the conversation discusses a particle in one dimension with a Dirac delta potential. The wave functions on the left and right sides are given by Aexp(kx) and Aexp(-kx) respectively. The momentum operator acting on these wave functions results in two complex numbers, which may seem contradictory since the momentum operator is Hermitian. The justification for this lies in considering a finite square well potential, where the kinetic energy and momentum can be both positive and negative in different regions. This is consistent with p being Hermitian, as the focus is on the expectation value of p rather than p itself.
  • #1
hokhani
483
8
Consider a particle in one dimention. there is a dirac delta potential such as V=-a delat(x). The wave functions in two sides(left and right) are Aexp(kx) and Aexp(-kx) respectively. So if the momentum operator acts on the wave functions, would give two complex numbers while the momentum operator is Hermitian. what is the justification here?
 
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  • #2
To see it more clearly, step away from the delta function for a moment and consider instead a finite square well potential, V(x) = -V0 for |x| < a and zero otherwise. Assuming the well is deep enough to have a bound state, the ground state wavefunction will be sinusoidal within the well and exponential without. Inside the well the kinetic energy p2/2m is positive and p is real. But outside the well is a classically forbidden region where the kinetic energy is negative and p is imaginary.

This is perfectly consistent with p being Hermitian, because the thing that must be real is not p itself, it's the matrix element or expectation value ∫ψ*pψ dx
 

What is the momentum operator in quantum mechanics?

The momentum operator in quantum mechanics is a mathematical operator that describes the momentum of a quantum particle. It is represented by the symbol p and is defined as the derivative of the particle's position with respect to time.

What is the Dirac delta potential in quantum mechanics?

The Dirac delta potential is a type of potential energy function used in quantum mechanics to model interactions between particles. It is represented by the symbol δ and is defined as a function that is infinite at one point and zero everywhere else.

What is the justification for using the momentum operator with a Dirac delta potential?

The justification for using the momentum operator with a Dirac delta potential is based on the principle of superposition in quantum mechanics. This principle states that the overall momentum of a particle can be determined by adding together the momenta of all the individual interactions acting on the particle, including the delta potential.

How does the momentum operator act on a particle in the presence of a Dirac delta potential?

When the momentum operator acts on a particle in the presence of a Dirac delta potential, it takes into account the effect of the potential on the particle's momentum. This is done by incorporating the delta potential function into the derivative operation, resulting in a modified momentum operator.

What are some applications of the momentum operator with a Dirac delta potential?

The momentum operator with a Dirac delta potential is commonly used in quantum mechanics to study the behavior of particles in a variety of physical systems, such as quantum wells and quantum dots. It is also used in the study of scattering processes and tunneling phenomena.

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