Mott transition in hardcore Bose Hubbard model for honeycomb lattice
The purpose of this study is to learn how to use direct loop update Stochastic Series Expansion Quantum Monte Carlo simulation to observe Mott transition for a hard core bosonic system in a honeycomb lattice using a Bose-Hubbard model. Lattice occupancy is set at 1/2, and the simulation is run on 3...
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sg-ntu-dr.10356-636152023-02-28T23:17:03Z Mott transition in hardcore Bose Hubbard model for honeycomb lattice Yonathan, Priambada Pinaki Sengupta School of Physical and Mathematical Sciences DRNTU::Science::Physics::Atomic physics::Solid state physics The purpose of this study is to learn how to use direct loop update Stochastic Series Expansion Quantum Monte Carlo simulation to observe Mott transition for a hard core bosonic system in a honeycomb lattice using a Bose-Hubbard model. Lattice occupancy is set at 1/2, and the simulation is run on 3 different lattice size, namely for L=4,6, and 8. During the simulation, the transition of the stiffness of the system is measured against the iterating parameter t/V, where t is the amplitude of the hopping component and V is the amplitude of the nearest neighbour potential. The critical point of the transition is then approximated from the intersection of the 3 transition curves. Bachelor of Science in Applied Physics 2015-05-18T01:31:38Z 2015-05-18T01:31:38Z 2015 2015 Final Year Project (FYP) http://hdl.handle.net/10356/63615 en 19 p. application/pdf |
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DRNTU::Science::Physics::Atomic physics::Solid state physics Yonathan, Priambada Mott transition in hardcore Bose Hubbard model for honeycomb lattice |
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The purpose of this study is to learn how to use direct loop update Stochastic Series Expansion Quantum Monte Carlo simulation to observe Mott transition for a hard core bosonic system in a honeycomb lattice using a Bose-Hubbard model. Lattice occupancy is set at 1/2, and the simulation is run on 3 different lattice size, namely for L=4,6, and 8. During the simulation, the transition of the stiffness of the system is measured against the iterating parameter t/V, where t is the amplitude of the hopping component and V is the amplitude of the nearest neighbour potential. The critical point of the transition is then approximated from the intersection of the 3 transition curves. |
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Pinaki Sengupta |
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Pinaki Sengupta Yonathan, Priambada |
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Final Year Project |
author |
Yonathan, Priambada |
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Yonathan, Priambada |
title |
Mott transition in hardcore Bose Hubbard model for honeycomb lattice |
title_short |
Mott transition in hardcore Bose Hubbard model for honeycomb lattice |
title_full |
Mott transition in hardcore Bose Hubbard model for honeycomb lattice |
title_fullStr |
Mott transition in hardcore Bose Hubbard model for honeycomb lattice |
title_full_unstemmed |
Mott transition in hardcore Bose Hubbard model for honeycomb lattice |
title_sort |
mott transition in hardcore bose hubbard model for honeycomb lattice |
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2015 |
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http://hdl.handle.net/10356/63615 |
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1759856903944404992 |