Diagonalization of a hamiltonian for a quantum wire

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SUMMARY

The discussion focuses on diagonalizing the Hamiltonian for a one-dimensional quantum wire with proximity-induced superconductivity. The Hamiltonian is given by H=η(k)τz+Bσ_x+αkσ_yτ_z+Δτ_x, where σ and τ represent Pauli matrices for spin and particle-hole space, respectively. The correct energy spectrum is derived as E^2(k)=Δ^2+η^2(k)+B^2+(αk)^2 ± √(B^2Δ^2+η^2(k)B^2+η^2(k)(αk)^2). The main issue raised is the incorrect interpretation of the Pauli matrices τ, leading to erroneous eigenvalue calculations. The user suggests that tensor notation may be necessary for proper matrix representation.

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  • Understanding of quantum mechanics, specifically Hamiltonians and eigenvalues.
  • Familiarity with Pauli matrices and their applications in quantum systems.
  • Knowledge of tensor products in matrix algebra.
  • Experience with computational tools like Mathematica for eigenvalue calculations.
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  • Study the application of tensor products in quantum mechanics, particularly in Hamiltonian formulations.
  • Learn how to properly represent Hamiltonians using Pauli matrices in quantum systems.
  • Explore the derivation of energy spectra from Hamiltonians in proximity-induced superconductivity contexts.
  • Review the relevant literature, specifically arXiv:1302.5433, to clarify the symbols and calculations presented in the paper.
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Lars Milz
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I try diagonalize the Hamiltonian for a 1D wire with proximity-induced superconductivity. In the case without a superconductor is all fine. However, with a superconductor I don't get the correct result for the energy spectrum of the Hamiltonian (arxiv:1302.5433)

H=\eta(k)τz+Bσ_x+αkσ_yτ_z+Δτ_x

Here σ and τ are the Pauli matrices for the spin and particle-hole space.

Now the correct result is: E^2(k)=Δ^2+η^2(k)+B^2+(αk)^2 ± \sqrt{B^2Δ^2+η^2(k)B2+η^2(k)(αk)^2}
My problem is now that I don't know how I bring the Hamiltonian in the correct matrix form for the calculation of the eigenvalues. If i try it with the upper Hamiltonian I have completely wrong results for the energy spectrum. I believe my mistake is the interpretation of the Pauli matrices τ but I don't know how I can write the Hamiltonian in the form to get the correct eigenvalues.
 
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I believe what you have here is tensor notation but with the tensor sign left out to reduce clutter. By the tensor A \otimes B of two matrices A,B, we mean at every entry of A, insert a copy of B multiplied by that entry in A. For example, i'll work out the first term in that Hamiltonian. I'll take the convention that the \sigma matrices come first followed by the \tau matrices and 1 as a matrix is the 2 \times 2 identity matrix:

\displaystyle \tau_z = 1 \otimes \tau_z = \begin{pmatrix} 1 & 0 \\ 0 & 1 \end{pmatrix} \otimes \begin{pmatrix} 1 & 0 \\ 0 & -1 \end{pmatrix} = \begin{pmatrix} 1 & 0 & 0 & 0 \\ 0 & -1 & 0 & 0 \\ 0 & 0 & 1 & 0 \\ 0 & 0 & 0 & -1 \end{pmatrix}.

Similarly, the second term is really \sigma_x = \sigma_x \otimes 1, the third is \sigma_y \otimes \tau_z and so on.

Using the standard Pauli matrices \sigma_x = \begin{pmatrix} 0 &amp; 1 \\ 1 &amp; 0 \end{pmatrix},<br /> \sigma_y = \begin{pmatrix} 0 &amp; -i \\ i &amp; 0 \end{pmatrix}, \sigma_z = \begin{pmatrix} 1 &amp; 0 \\ 0 &amp; -1 \end{pmatrix}, i don't actually agree with the expression for energy you wrote down. When I plug the 4 \times 4 matrix H into Mathematica and ask for the eigenvalues I get the same expression you wrote down except with a factor of 2 in front of the \pm \sqrt{\phantom{a}} term in E^2.

I know you're getting this from a paper. After a quick scan, the most similar expression for H I can find is equation 3 on page 4. The expression for E^2 in equation 4 on page 5 has the factor of 2 in front of the square root. However, admittedly, I haven't followed that calculation closely and I'm not entirely sure what all the symbols in equation 4 mean.
 

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