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研究生: 林渼葶
Lin, Mei-Ting
論文名稱: The use of weak-value metrology in the gravitational-wave detector
The use of weak-value metrology in the gravitational-wave detector
指導教授: 林豐利
Lin, Feng-Li
學位類別: 碩士
Master
系所名稱: 物理學系
Department of Physics
論文出版年: 2019
畢業學年度: 107
語文別: 英文
論文頁數: 56
中文關鍵詞: Gravitational Wave DetectorQuantum NoiseStandard Quantum LimitWeak Values
英文關鍵詞: Gravitational Wave Detector, Quantum Noise, Standard Quantum Limit, Weak Values
DOI URL: http://doi.org/10.6345/NTNU201901074
論文種類: 學術論文
相關次數: 點閱:112下載:21
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  • Weak-value metrology refers to quantum measurement with a weak measurement process and post-selection. The outcome, called weak values, can be amplified beyond the eigenvalues of the observable; however, there is some debate on the usefulness of weak-value metrology in increasing the sensitivity of a gravitational wave detector. In this thesis, we investigated the sensitivity limit with regard to quantum shot noise and radiation pressure noise. For this purpose, we formulated an input-output
    relation with a model via weak-value metrology, which allowed us to understand the optical processes under a condition wherein the weak value is applied intuitively. However, we found that the sensitivity of the modified model was not improved as the modified model destroyed the symmetry of the interferometer, which contributed to additional noise. Despite signal amplification, increasing sensitivity to detect more gravitational wave events is more vital.

    Contents Abstract . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ii Acknowledgements . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . iii List of Figures . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .vii 1Introduction 1 1.1 Introduction to Gravitational Waves . . . . . . . . . . . . . . . . . .3 1.2 Introduction to Gravitational-Wave Detection . . . . . . . . . . . . .5 1.2.1 The basic idea of interferometer . . . . . . . . . . . . . . . . .5 1.2.2 Fabry–Perot arm cavities . . . . . . . . . . . . . . . . . . . .8 1.2.3 Sideband . . . . . . . . . . . . . . . . . . . . . . . . . . . . .9 1.3 Introduction to Weak Measurements and Weak Values . . . . . . . .9 1.3.1 Difference between strong and weak measurements . . . . . .11 1.3.2 Weak-value amplification . . . . . . . . . . . . . . . . . . . .15 1.4 Gravitational Wave Detector via Weak Measurement . . . . . . . . .16 2 Mathematical Description of Conventional Gravitational Wave Interferometers 18 2.1 Quantization of the Dynamics . . . . . . . . . . . . . . . . . . . . . . 18 2.2 Quantum States of the Optical Field . . . . . . . . . . . . . . . . . . 21 2.2.1 Fock or number state . . . . . . . . . . . . . . . . . . . . . . 21 2.2.2 Coherent state . . . . . . . . . . . . . . . . . . . . . . . . . . 22 2.2.3 Squeezed state . . . . . . . . . . . . . . . . . . . . . . . . . . 24 2.3 Basic Dynamic Processes of the Optical Field . . . . . . . . . . . . .26 2.3.1 Light propagation in the interferometer . . . . . . . . . . . . .26 2.3.2 Dynamics of the test mass . . . . . . . . . . . . . . . . . . . 29 2.4 Input–Output Relation of Basic Optomechanical System Model . . .30 2.4.1 A single end mirror . . . . . . . . . . . . . . . . . . . . . . . .30 2.4.2 Input–output relation . . . . . . . . . . . . . . . . . . . . . . 32 2.5 Standard Quantum Limit . . . . . . . . . . . . . . . . . . . . . . . .39 3 Gravitational-Wave Detector Using Weak Values 41 3.1 Setup . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .41 3.2 Weak-Value Metrology in Gravitational-wave Detector . . . . . . . .42 3.3 Input–Output Relation Using Weak Values . . . . . . . . . . . . . . .46 3.4 Sensitivity . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .49 3.5 Amplification . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .51 Conclusion 53 Bibliography 55

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