- #1
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
[tex]\begin{pmatrix}V(x) & k_x - i k_y \\ k_x + i k_y & V(x)\end{pmatrix}[/tex]
where [itex]V(x)=V_0 \Theta(x)[/itex] and [itex]\Theta(x)[/itex] is the unit step function, you have a Hamiltonain like
[tex]v(x) \begin{pmatrix}0 & k_x - i k_y \\ k_x + i k_y & 0\end{pmatrix}[/tex]
where [itex]v(x)=v_0 \Theta(x)[/itex].
If not, what would be a way to approach this problem? Many thanks.
[tex]\begin{pmatrix}V(x) & k_x - i k_y \\ k_x + i k_y & V(x)\end{pmatrix}[/tex]
where [itex]V(x)=V_0 \Theta(x)[/itex] and [itex]\Theta(x)[/itex] is the unit step function, you have a Hamiltonain like
[tex]v(x) \begin{pmatrix}0 & k_x - i k_y \\ k_x + i k_y & 0\end{pmatrix}[/tex]
where [itex]v(x)=v_0 \Theta(x)[/itex].
If not, what would be a way to approach this problem? Many thanks.