Search for bose glass phase in the Shastry-Sutherland model

Physicists are interested on the physical properties during the phase transition of lattices under various Hamiltonian model. In this project, we are dealing with the hard core boson in the Shastry-Sutherland model under the Bose-Hubbard Hamiltonian model, where the diagonal bonds and square (vertic...

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Main Author: Leong, Wui Seng
Other Authors: School of Physical and Mathematical Sciences
Format: Final Year Project
Language:English
Published: 2014
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Online Access:http://hdl.handle.net/10356/60937
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Institution: Nanyang Technological University
Language: English
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spelling sg-ntu-dr.10356-609372023-02-28T23:11:13Z Search for bose glass phase in the Shastry-Sutherland model Leong, Wui Seng School of Physical and Mathematical Sciences Pinaki Sengupta DRNTU::Science::Physics::Atomic physics::Solid state physics DRNTU::Science::Physics::Atomic physics::Statistical physics Physicists are interested on the physical properties during the phase transition of lattices under various Hamiltonian model. In this project, we are dealing with the hard core boson in the Shastry-Sutherland model under the Bose-Hubbard Hamiltonian model, where the diagonal bonds and square (vertical and horizontal) bonds are of different strength. We only focus on the low temperature since we want to search its Bose glass phase. In this project, 4 physical properties are determined: boson density, structure factor, stiffness and energy, by using the one of the quantum Monte Carlo methods called the \emph{stochastic series expansion}. Stochastic series expansion was studied thoroughly and instead of using the quantum states $\alpha$, it uses $\left\{ \alpha,S_{M}\right\} $ as the sample configuration where $S_{M}$ is the set of permutation of $M$ bond operators. The Monte Carlo simulation, which consists of 3 types of updates (namely diagonal update, off-diagonal/loop update and site update), was written by \CC and it was verified with the analytical solution of $2\times2$ lattice. It was realised that the system consists of 3 different states: dimer, checkerboard and superfluid, where superfluid lies as the ``intermediate state'' between dimer and checkerboard. Bachelor of Science in Physics 2014-06-03T06:14:21Z 2014-06-03T06:14:21Z 2014 2014 Final Year Project (FYP) http://hdl.handle.net/10356/60937 en 66 p. application/pdf
institution Nanyang Technological University
building NTU Library
continent Asia
country Singapore
Singapore
content_provider NTU Library
collection DR-NTU
language English
topic DRNTU::Science::Physics::Atomic physics::Solid state physics
DRNTU::Science::Physics::Atomic physics::Statistical physics
spellingShingle DRNTU::Science::Physics::Atomic physics::Solid state physics
DRNTU::Science::Physics::Atomic physics::Statistical physics
Leong, Wui Seng
Search for bose glass phase in the Shastry-Sutherland model
description Physicists are interested on the physical properties during the phase transition of lattices under various Hamiltonian model. In this project, we are dealing with the hard core boson in the Shastry-Sutherland model under the Bose-Hubbard Hamiltonian model, where the diagonal bonds and square (vertical and horizontal) bonds are of different strength. We only focus on the low temperature since we want to search its Bose glass phase. In this project, 4 physical properties are determined: boson density, structure factor, stiffness and energy, by using the one of the quantum Monte Carlo methods called the \emph{stochastic series expansion}. Stochastic series expansion was studied thoroughly and instead of using the quantum states $\alpha$, it uses $\left\{ \alpha,S_{M}\right\} $ as the sample configuration where $S_{M}$ is the set of permutation of $M$ bond operators. The Monte Carlo simulation, which consists of 3 types of updates (namely diagonal update, off-diagonal/loop update and site update), was written by \CC and it was verified with the analytical solution of $2\times2$ lattice. It was realised that the system consists of 3 different states: dimer, checkerboard and superfluid, where superfluid lies as the ``intermediate state'' between dimer and checkerboard.
author2 School of Physical and Mathematical Sciences
author_facet School of Physical and Mathematical Sciences
Leong, Wui Seng
format Final Year Project
author Leong, Wui Seng
author_sort Leong, Wui Seng
title Search for bose glass phase in the Shastry-Sutherland model
title_short Search for bose glass phase in the Shastry-Sutherland model
title_full Search for bose glass phase in the Shastry-Sutherland model
title_fullStr Search for bose glass phase in the Shastry-Sutherland model
title_full_unstemmed Search for bose glass phase in the Shastry-Sutherland model
title_sort search for bose glass phase in the shastry-sutherland model
publishDate 2014
url http://hdl.handle.net/10356/60937
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