2-7 June 2019
Simon Fraser University
America/Vancouver timezone
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27 - Exact Diagonalization on Pyrochlore System

4 Jun 2019, 16:49
SWH 9082 + AQ South-East Corner / coin sud-est (Simon Fraser University)

SWH 9082 + AQ South-East Corner / coin sud-est

Simon Fraser University

Poster not-in-competition (Graduate Student) / Affiche non-compétitive (Étudiant(e) du 2e ou 3e cycle) Condensed Matter and Materials Physics / Physique de la matière condensée et matériaux (DCMMP-DPMCM) DCMMP Poster Session & Student Poster Competition Finals (10) | Session d'affiches DPMCM et finales du concours d'affiches étudiantes (10)


Mr chen wei (Memorial University)


In quantum physics, if we can find the eigenstates $| \phi_i\rangle$ of a Hamiltonian $H$, and the respective eigenergies $E_i$, we can calculate many aspects such as time evolution, or its thermal properties. Exact diagonalization is a method which can solve the Hamiltonian numerically. For a small Hamiltonian system, we can find the eigenvalues by solve the characteristic polynomial equation of the matrix. However, as the system goes larger, the calculation will go exponentially. Instead of calculating the eigenstates directly, We will use the unitary transformation matrix to block diagonalise the Hamiltonian first. As a consequence, instead of solving the Hamiltonian directly, we will solve each block. In order to find the unitary transformation matrix U, we will use the symmetry of the Hamiltonian, and with the help of group theory, we can construct U matrix and do the block diagonalization.
The space group for Pyrochlore is No.227, it contains the point group $O_h$ with space translations. Here we consider the conventional cell contains 16 sites, and use three translations T1:$(0,1/2,1/2)$, T2:$(1/2,0,1/2)$ and T3:$(1/2,1/2,0)$. Additionally, we also use the subgroup $D_2$ and the time reversal symmetry. As a result, we will block diagonalise the Hamiltonian into 32 blocks, which can be analyze easily.

Primary author

Mr chen wei (Memorial University)

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