Monte Carlo Simulation of Interacting Electron Models by a New Determinant Approach

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Monte Carlo Simulation of Interacting Electron Models by a New Determinant Approach Mucheng Zhang (Under the direction of Robert W. Robinson and Heinz-Bernd Schüttler)

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Monte Carlo Simulation of Interacting Electron Models by a New Determinant Approach. Mucheng Zhang (Under the direction of Robert W. Robinson and Heinz-Bernd Schüttler ). INTRODUCTION. Hubbard model . Hubbard model - PowerPoint PPT Presentation

Transcript of Monte Carlo Simulation of Interacting Electron Models by a New Determinant Approach

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Monte Carlo Simulationof Interacting Electron Models

by a New Determinant Approach

Mucheng Zhang(Under the direction of Robert W.

Robinson and Heinz-Bernd Schüttler)

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INTRODUCTION

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Hubbard model

• Hubbard model – describe magnetism and super conductivity in

strongly correlated electron systems.

– originally developed to explain metal-insulator transition in strongly correlated electronic materials.

– has been applied to the study of magnetism.

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• 2D Hubbard model

– used as “minimal” model to describe high- temperature superconductors

– has been applied extensively.

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Some Methods

• Some reliable numerical solution methods ([2])– quantum Monte Carlo – exact diagonalization – density matrix renormalization these methods are limited to only small 2D clusters.

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• Cluster mean–field embedding approaches – allow small cluster calculations to be effectively

extrapolated to larger and even infinite lattice sizes ([4],[5],[7] and [1]).

• A determinant formalism ([10])– derived by functional integral techniques– used for Monte Carlo simulations of small 2D

Hubbard model clusters.

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Our New Method

• A new determinant approach is derived from a Feynman diagram expansion for the single particle Green’s function of the Hubbard model.

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• Green’s functions – mathematical objects of particular interest in the

quantum theory of many-electron systems– model predictions can be directly compared to the

data obtained in real materials .• The single-particle Green’s function – used to predict the result of photo-emission

spectroscopy experiments.

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• Determinant formalism for the extended Hubbard model.

• Monte Carlo summation algorithm to evaluate the relevant determinant diagram sums.

• We have tested it on small 2 × 2 Hubbard clusters.

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CALCULATION OF DETERMINANTS

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Four Algorithms

• Gaussian Elimination With Partial Pivoting (GEP)

• Givens Rotation (GR)• Householder Reflection (HR)• Fast Givens Transformation (FGT)

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Conclusion

• GEP– the most efficient.– in most cases, the most accurate.

• In terms of efficiency and accuracy, GEP is a good algorithm for evaluating determinants.

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FEYNMAN DIAGRAM EXPANSIONS

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Notation

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Integral Padding Function

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EXTENDED HUBBARD MODEL (EHM)

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The Lattice

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Interaction Potential Function

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The Simplest EHM For CV

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The -Spacek

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Reciprocal lattice

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Energy Band

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Fourier Sum Over Matsubara Frequencies

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The Function g

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Notation

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The m–electron Green’s Function

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MONTE CARLO EVALUATION OF EHM

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Notation

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Score and Weight

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Probability Function For EHM

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Monte Carlo Evaluation

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Evaluation of Determinants

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Metropolis MCMC method

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Generating The Chain

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MC Move Types

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Type 1: Move a Pair of V-Lines

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Type 2: Flip a Spin at a Vertex

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Type 3: Move at a Vertexr

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Type 5: Update τ–Padding Variable ψ

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Type 6: Raise/Lower Diagram Order

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Type 6+: Raise Diagram Order

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Type 6-: Lower Diagram Order

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Acceptance Probability of Type 6

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Type 7: Exchange a pair of Spins

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RESULTS

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The Experiments

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Continuous Time Scheme

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Parameter Sets

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Accept Ratio

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Running Time

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Order Frequency

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Convergence of Parameter Set 3b

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Scores VS. 1/T

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The Green’s Function

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Conclusion

• Our new method works well.

• Our program can be used– for any rectangle lattice– for m–electron system with m > 1 after slight

modification.