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  1. NTU Theses and Dissertations Repository
  2. 理學院
  3. 物理學系
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/41590
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor趙挺偉
dc.contributor.authorYu-Ying Leeen
dc.contributor.author李昱穎zh_TW
dc.date.accessioned2021-06-15T00:24:04Z-
dc.date.available2009-02-10
dc.date.copyright2009-02-10
dc.date.issued2009
dc.date.submitted2009-01-23
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49
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dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/41590-
dc.description.abstract在這篇論文中,我們應用最佳手則對稱之新費米場作用量(optimal domain-wall fermion),研究Schwinger模型上的拓樸率。藉由拓樸率的定義,我們可以利用整體拓樸荷(global topological charge)來決定拓樸率。同時,透過鞍點近似法(saddle point expansion),我們也可以在一個固定的拓樸區(fixed topological sector)內,藉由拓樸密度(topological charge density)的兩點相關係數以得到拓樸率。最後我們將證明在晶格上,這兩種方法會得出相同的拓樸率。zh_TW
dc.description.abstractIn this thesis, we study the topological susceptibility in the Schwinger model with optimal domain-wall fermions. We obtain the topological susceptibility from counting the global topological charge. Also, using the saddle point
expansion, topological susceptibility can be extracted from the 2-point correlation functions of topological charge density in a fixed topological sector.We can demonstrate that the values obtained from this two methods are in
good agreement.
en
dc.description.provenanceMade available in DSpace on 2021-06-15T00:24:04Z (GMT). No. of bitstreams: 1
ntu-98-R95222050-1.pdf: 315528 bytes, checksum: 21dc5a1f6712d2d9a3efb434d4774094 (MD5)
Previous issue date: 2009
en
dc.description.tableofcontents1 Introduction 3
1.1 Schwinger Model . . . . . . . . . . . . . . . . . . . . . . . . . 5
1.2 Lattice Formulation of U(1) Gauge Field . . . . . . . . . . . . 6
1.3 Naive Lattice Formulation of Fermion Field . . . . . . . . . . 7
2 Dirac Operator Schemes 10
2.1 Wilson Dirac Operator . . . . . . . . . . . . . . . . . . . . . . 10
2.2 Ginsparg-Wilson relation . . . . . . . . . . . . . . . . . . . . . 11
2.3 Overlap Dirac Operator . . . . . . . . . . . . . . . . . . . . . 13
2.4 Conventional Domain Wall Fermion . . . . . . . . . . . . . . . 16
2.5 Optimal Domain Wall Fermion . . . . . . . . . . . . . . . . . 18
3 Monte Carlo Method 22
3.1 Fermion Field . . . . . . . . . . . . . . . . . . . . . . . . . . . 23
3.2 Pseudo-Fermion Field . . . . . . . . . . . . . . . . . . . . . . . 24
1
3.3 Hybrid Monte Carlo Method . . . . . . . . . . . . . . . . . . . 25
4 Topological Susceptibility 29
4.1 Topological Charge On the Lattice . . . . . . . . . . . . . . . 29
4.2 Topological Susceptibility On the Lattice . . . . . . . . . . . . 31
4.3 Fixed Topological Sector . . . . . . . . . . . . . . . . . . . . 31
5 Data Analysis 35
5.1 Autocorrelations in Monte Carlo simulation time . . . . . . . . 35
5.2 Data Blocking . . . . . . . . . . . . . . . . . . . . . . . . . . . 36
5.3 Jackknife Method . . . . . . . . . . . . . . . . . . . . . . . . . 37
6 Results 38
6.1 Topological Susceptibility from Global Topological Charge . . 38
6.2 Topological Susceptibility from Fixed Topological Sector . . . 42
7 Conclusion 46
Bibliography 48
A Force in Hybrid Monte Carlo 51
A.1 Gauge Force . . . . . . . . . . . . . . . . . . . . . . . . . . . . 51
A.2 Fermion Force . . . . . . . . . . . . . . . . . . . . . . . . . . . 52
dc.language.isoen
dc.subject拓樸荷zh_TW
dc.subject拓樸zh_TW
dc.subject晶格zh_TW
dc.subject二維場論zh_TW
dc.subject場論zh_TW
dc.subject拓樸率zh_TW
dc.subjecttopologyen
dc.subjecttopological chargeen
dc.subjecttopoligical susceptibilityen
dc.titleSchwinger模型上的拓樸率zh_TW
dc.titleTopological Susceptibility in the Schwinger Modelen
dc.typeThesis
dc.date.schoolyear97-1
dc.description.degree碩士
dc.contributor.oralexamcommittee高涌泉,謝東翰
dc.subject.keyword拓樸,晶格,二維場論,場論,拓樸率,拓樸荷,zh_TW
dc.subject.keywordtopology,topoligical susceptibility,topological charge,en
dc.relation.page53
dc.rights.note有償授權
dc.date.accepted2009-01-23
dc.contributor.author-college理學院zh_TW
dc.contributor.author-dept物理研究所zh_TW
顯示於系所單位:物理學系

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