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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/123456789/9314
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor高英哲(Ying-Jer Kao)
dc.contributor.authorYu-Cheng Suen
dc.contributor.author蘇育正zh_TW
dc.date.accessioned2021-05-20T20:17:11Z-
dc.date.available2009-07-14
dc.date.available2021-05-20T20:17:11Z-
dc.date.copyright2009-07-14
dc.date.issued2009
dc.date.submitted2009-07-02
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dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/9314-
dc.description.abstract在一維量子自旋系統中,矩陣積態可作為變量數值模擬的試驗波函數。在此研究中,我們展示了兩種建構矩陣積態的方法,這些方法源自於密度矩陣重整群與量子資訊理論。我們發展了兩種在一維量子系統中矩陣積態的演算法,分別為隨機最佳化的量子蒙地卡羅變量模擬 (Variational quantum Monte Carlo simulations with stochastic optimization) 與時間演化間隔消除法 (Time-evolving block decimation)。我們推廣了隨機最佳化的方法至開放邊界 (open boundary condition) 並且探討了伊辛模型加入橫向磁場與海森堡模型。另外,我們處理了無限長的伊辛模型加入橫向磁場,我們的結果顯示量子糾纏 (quantum entanglement)與量子相變息息相關。zh_TW
dc.description.abstractIn one-dimensional quantum spin systems, the matrix product states (MPS) can be used as a trail wave function for variational numerical simulations. In this thesis, we investigate the construction of MPS which is related to the density matrix renormalization group (DMRG) and the Quantum information theory (QIT). We develop two algorithms, variational quantum Monte Carlo (QMC) simulations with stochastic optimization [1] and time-evolving block decimation (TEBD) [2, 3], in one dimensional systems. We generalize QMC with stochastic optimization to the open boundary condition and study the transverse Ising model and Heisenerg model. We also applied the infinite TEBD algorithm [4] to the infinite transverse Ising model and demonstrate that entanglement is a key ingredient in the quantum phase transition.en
dc.description.provenanceMade available in DSpace on 2021-05-20T20:17:11Z (GMT). No. of bitstreams: 1
ntu-98-R96222011-1.pdf: 916947 bytes, checksum: 535dd33f697f13df3f55a1928bac7c9f (MD5)
Previous issue date: 2009
en
dc.description.tableofcontentsAbstract i
1 Introduction 1
1.1 Overview. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
1.2 Latticemodels . . . . . . . . . . . . . . . . . . . . . . . . . . . 2
1.2.1 Transverse Ising model . . . . . . . . . . . . . . . . . . 2
1.2.2 Heisenberg model . . . . . . . . . . . . . . . . . . . . . 2
2 Matrix Product States 4
2.1 MPS fromthe DMRG point of view . . . . . . . . . . . . . . . 4
2.2 MPS fromthe QIT point of view . . . . . . . . . . . . . . . . 6
2.2.1 Tools in Linear Algebra . . . . . . . . . . . . . . . . . 6
2.2.2 Entanglement . . . . . . . . . . . . . . . . . . . . . . . 8
2.2.3 A variant formofMPS . . . . . . . . . . . . . . . . . . 8
3 Variational quantum Monte Carlo simulation with stochastic
optimization 12
3.1 Introduction toMonte Carlo simulation . . . . . . . . . . . . . 12
3.1.1 TheMetropolis algorithm . . . . . . . . . . . . . . . . 13
3.1.2 Measuring observable quantities . . . . . . . . . . . . . 15
3.2 Stochastic optimization . . . . . . . . . . . . . . . . . . . . . . 16
3.3 Approximation forms for the open boundary condition . . . . 19
3.4 Methods ofmeasurements . . . . . . . . . . . . . . . . . . . . 22
3.4.1 Measurements byMonte Carlo sampling . . . . . . . . 22
3.4.2 Measurements by summing over all states . . . . . . . 22
3.5 Studies of the transverse Ising model . . . . . . . . . . . . . . 24
3.5.1 The D dependence . . . . . . . . . . . . . . . . . . . . 24
3.5.2 Ground state energy, magnetization and correlation
functions . . . . . . . . . . . . . . . . . . . . . . . . . . 24
3.6 Applications to the Heisenberg model . . . . . . . . . . . . . . 28
3.6.1 The D dependence . . . . . . . . . . . . . . . . . . . . 29
3.6.2 Exploiting symmetry . . . . . . . . . . . . . . . . . . . 29
4 Imaginary time evolution with TEBD 33
4.1 Imaginary time evolution . . . . . . . . . . . . . . . . . . . . . 33
4.2 Normalization conditions forMPS . . . . . . . . . . . . . . . . 34
4.3 Updating thematrices . . . . . . . . . . . . . . . . . . . . . . 35
4.4 The formof the wave function . . . . . . . . . . . . . . . . . . 38
4.4.1 Infinite system . . . . . . . . . . . . . . . . . . . . . . 38
4.4.2 Finite system . . . . . . . . . . . . . . . . . . . . . . . 39
4.5 Imaginary time evolution algorithm . . . . . . . . . . . . . . . 40
4.6 Infinite transeverse Ising model . . . . . . . . . . . . . . . . . 41
5 Conclusions 46
Bibliography 47
dc.language.isoen
dc.title矩陣積態在一維量子自旋系統的應用zh_TW
dc.titleMatrix Product States in One Dimensional Quantum Spin Systemsen
dc.typeThesis
dc.date.schoolyear97-2
dc.description.degree碩士
dc.contributor.oralexamcommittee管希聖(Hsi-Sheng Goan),陳柏中(Po-Chung Chen)
dc.subject.keyword矩陣積態,量子蒙地卡&#63759,隨機最佳化,時間演化間隔消除法,量子糾纏,zh_TW
dc.subject.keywordmatrix product state,quantum Monte Carlo,stochastic optimization,TEBD,iTEBD,entanglement,en
dc.relation.page48
dc.rights.note同意授權(全球公開)
dc.date.accepted2009-07-03
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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