Wavefunction matching two different H, not just V

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Discussion Overview

The discussion revolves around the application of wavefunction matching techniques in quantum mechanics, specifically in scenarios involving Hamiltonians with varying Fermi velocities. Participants explore whether these techniques, typically used for potential barriers, can be adapted for Hamiltonians that exhibit step-like changes in velocity rather than potential.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions whether the wavefunction matching techniques applicable to a potential barrier can be extended to a Hamiltonian with a step-like change in Fermi velocity.
  • Another participant raises a concern regarding the hermiticity of the Hamiltonian if the commutator between the velocity function and the derivative operator does not equal zero.
  • A participant describes a simpler generalization of the problem, emphasizing the need to understand the implications of having different Hamiltonians on either side of a discontinuity.
  • Further elaboration is made on the hermiticity of the Hamiltonian when combining different operators, suggesting that careful treatment of the derivatives is necessary to maintain hermiticity.

Areas of Agreement / Disagreement

Participants express uncertainty about the extension of wavefunction matching techniques to the proposed Hamiltonian scenario. There is no consensus on whether the methods can be applied directly or what modifications might be necessary.

Contextual Notes

Participants note the potential complications arising from the non-commutativity of operators involved and the need for careful mathematical treatment to ensure hermiticity, but do not resolve these issues.

SturgySturges
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Can the basic techniques of wavefunction matching that one would use to calculate the transmission through a step barrier potential and the Dirac hamiltonian of graphene be used for a situation where instead the fermi velocity changes in a step like fashion. i.e. instead of a Hamiltonian like

\begin{pmatrix}V(x) & k_x - i k_y \\ k_x + i k_y & V(x)\end{pmatrix}

where V(x)=V_0 \Theta(x) and \Theta(x) is the unit step function, you have a Hamiltonain like

v(x) \begin{pmatrix}0 & k_x - i k_y \\ k_x + i k_y & 0\end{pmatrix}

where v(x)=v_0 \Theta(x).

If not, what would be a way to approach this problem? Many thanks.
 
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I assume the ##k_x+ik_y## terms originate form a ##\gamma^\mu \partial_\mu## applied to the wave function. This being the case I would be concerned that the commutator, ##[v(x),\gamma^\mu \partial_\mu]\ne 0##. This would make your Hamiltonian not hermitian? Just a thought.
 
Hmm I'm not sure, I've described a much simpler generalisation of the problem that I'm working on just to get down to the key concept I'm uncertain about. Basically it's this business of having two different Hamiltonians either side of x=0 (normally the difference is just the `V' in H=H_0+V) and using wave function matching techniques at the discontinuity. It works for just a V but I want to know if/why/how these ideas can be extended to a situation like the above.
 
SturgySturges said:
It works for just a ##V## but I want to know if/why/how these ideas can be extended to a situation like the above.
I used to work with an old guy back in the 80's whose favorite question was; "what is it?"

if you write out the ##V(x)## case ##H=H_o + V(x)##. Clearly, ##[V(x),H_o]\ne 0## because of the derivatives that appear in ##H_o##. This is all fine and good because you are adding two hermitian operators which yields an hermitian ##H##. If you write out the generalization, what does it look like in terms of derivatives (which is where the k's come from) and the new ##v(x)##? Unless you are careful the result will not be hermitian. I assume that one could symmetrize any product and get a hermitian operators but the details might be different than what you've written, Don't know because it's unclear what you intend from what you have written out.
 

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