BPS VORTEKS IN THE GENERALIZED MAXWELL-CHERN-SIMONS-HIGGS MODEL IN 1+ 2 DIMENSIONS

Vortex is a two-dimensional soliton with finite core size. In this final project, we analyze the vortex solution of the generalized Maxwell-Chern-Simons-Higgs (MCSH) model using the BPS Lagrangian method. In the first part, we consider the generalized MCSH model that was introduced in Ref. [1]. U...

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Main Author: Yudha Prasetya Tama, Laurenzius
Format: Final Project
Language:Indonesia
Online Access:https://digilib.itb.ac.id/gdl/view/54972
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Institution: Institut Teknologi Bandung
Language: Indonesia
id id-itb.:54972
spelling id-itb.:549722021-06-11T10:42:25ZBPS VORTEKS IN THE GENERALIZED MAXWELL-CHERN-SIMONS-HIGGS MODEL IN 1+ 2 DIMENSIONS Yudha Prasetya Tama, Laurenzius Indonesia Final Project BPS Lagrangian, BPS equation, Maxwell-Chern-Simons-Higgs, Soliton, and Vortex INSTITUT TEKNOLOGI BANDUNG https://digilib.itb.ac.id/gdl/view/54972 Vortex is a two-dimensional soliton with finite core size. In this final project, we analyze the vortex solution of the generalized Maxwell-Chern-Simons-Higgs (MCSH) model using the BPS Lagrangian method. In the first part, we consider the generalized MCSH model that was introduced in Ref. [1]. Using the radially symmetric ansatz, we define the BPS Lagrangian with non-boundary terms containing zeroth order of the first-derivative of effective fields and quadratic terms of the first-order derivative for N and A0 field. From this, we can obtain the BPS equations for a(r) and g(r) rigorously. The governing equation for N and A0 is obtained as an additional constraint equation derived as the Euler-Lagrange equation of the BPS Lagrangian. There is another possible identification for the effective field N and A0 that is A0 = N from the remaining constrain equation. For this possibility, we analyze the numerical solution. From the obtained numerical result, we can say that this identification corresponds to the negative electric charge of the vortex. We also show that the plus and minus sign in the BPS equation is related to the magnetic charge of a vortex. For the second part, we consider the generalized MCSH model without a neutral scalar field, N. In this model, we define BPS Lagrangian with the non-boundary term only consist of the zeroth-order of the first derivative of a field. We obtain the BPS equation for each effective field with the BPS equation for the scalar gauge field is A0 = k0 with k0 being a real positive definite constant such that the obtained result can the regarded as an electrically neutral vortex solution. The stability of this solution is analyzed via finite energy condition which gives EBPS = 2pk0n from which can be concluded that this solution is, in fact, stable. text
institution Institut Teknologi Bandung
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continent Asia
country Indonesia
Indonesia
content_provider Institut Teknologi Bandung
collection Digital ITB
language Indonesia
description Vortex is a two-dimensional soliton with finite core size. In this final project, we analyze the vortex solution of the generalized Maxwell-Chern-Simons-Higgs (MCSH) model using the BPS Lagrangian method. In the first part, we consider the generalized MCSH model that was introduced in Ref. [1]. Using the radially symmetric ansatz, we define the BPS Lagrangian with non-boundary terms containing zeroth order of the first-derivative of effective fields and quadratic terms of the first-order derivative for N and A0 field. From this, we can obtain the BPS equations for a(r) and g(r) rigorously. The governing equation for N and A0 is obtained as an additional constraint equation derived as the Euler-Lagrange equation of the BPS Lagrangian. There is another possible identification for the effective field N and A0 that is A0 = N from the remaining constrain equation. For this possibility, we analyze the numerical solution. From the obtained numerical result, we can say that this identification corresponds to the negative electric charge of the vortex. We also show that the plus and minus sign in the BPS equation is related to the magnetic charge of a vortex. For the second part, we consider the generalized MCSH model without a neutral scalar field, N. In this model, we define BPS Lagrangian with the non-boundary term only consist of the zeroth-order of the first derivative of a field. We obtain the BPS equation for each effective field with the BPS equation for the scalar gauge field is A0 = k0 with k0 being a real positive definite constant such that the obtained result can the regarded as an electrically neutral vortex solution. The stability of this solution is analyzed via finite energy condition which gives EBPS = 2pk0n from which can be concluded that this solution is, in fact, stable.
format Final Project
author Yudha Prasetya Tama, Laurenzius
spellingShingle Yudha Prasetya Tama, Laurenzius
BPS VORTEKS IN THE GENERALIZED MAXWELL-CHERN-SIMONS-HIGGS MODEL IN 1+ 2 DIMENSIONS
author_facet Yudha Prasetya Tama, Laurenzius
author_sort Yudha Prasetya Tama, Laurenzius
title BPS VORTEKS IN THE GENERALIZED MAXWELL-CHERN-SIMONS-HIGGS MODEL IN 1+ 2 DIMENSIONS
title_short BPS VORTEKS IN THE GENERALIZED MAXWELL-CHERN-SIMONS-HIGGS MODEL IN 1+ 2 DIMENSIONS
title_full BPS VORTEKS IN THE GENERALIZED MAXWELL-CHERN-SIMONS-HIGGS MODEL IN 1+ 2 DIMENSIONS
title_fullStr BPS VORTEKS IN THE GENERALIZED MAXWELL-CHERN-SIMONS-HIGGS MODEL IN 1+ 2 DIMENSIONS
title_full_unstemmed BPS VORTEKS IN THE GENERALIZED MAXWELL-CHERN-SIMONS-HIGGS MODEL IN 1+ 2 DIMENSIONS
title_sort bps vorteks in the generalized maxwell-chern-simons-higgs model in 1+ 2 dimensions
url https://digilib.itb.ac.id/gdl/view/54972
_version_ 1822001923764518912