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研究生: 陳鈴淳
Chen, Ling-Chun
論文名稱: 冷原子系綜的高效率通訊波段量子轉頻介面
High-Efficiency Telecom Quantum Frequency Interface in Cold Atomic Ensembles
指導教授: 陳泳帆
Chen, Yong-Fan
學位類別: 博士
Doctor
系所名稱: 理學院 - 物理學系
Department of Physics
論文出版年: 2026
畢業學年度: 114
語文別: 英文
論文頁數: 214
中文關鍵詞: 鑽石型四波混頻冷原子系綜量子轉頻原子雙光子通訊波段轉換電磁誘發透明
外文關鍵詞: diamond-type four-wave mixing, cold atomic ensemble, quantum frequency conversion, atomic biphotons, telecom-band conversion, electromagnetically induced transparency
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  • 本論文研究冷銣原子系綜的高效率通訊波段量子轉頻介面,目標是將適合原子量子記憶與量子節點操作的 795 nm 近紅外光子轉換至適合低損耗光纖傳輸的 1367 nm 通訊波段,同時保留其量子態與非古典關聯特性。本研究以鑽石型四波混頻為核心機制,結合理論模型、實驗最佳化與關聯雙光子轉換實驗,建立原子系綜量子轉頻介面的完整研究架構。在理論方面,本論文建立半古典與全量子模型,分析轉換效率、殘餘穿透率與光學深度、控制場強度及失諧量之間的關係,並以海森堡–朗之萬(Heisenberg–Langevin)方程與約化密度算符方法描述轉頻過程中的量子噪聲、轉換效率與量子態保真度。理論結果顯示,在高轉換效率條件下,鑽石型原子系綜可有效保存光子數、路徑與偏振自由度中所攜帶的量子資訊。實驗上,本研究先以弱同調光輸入實現 795 nm 至 1367 nm 的高效率通訊波段轉頻,並透過分析 Λ 型、階梯型與 V 型電磁誘發透明響應,以及最佳化光學深度、耦合場、驅動場與失諧條件,在光學深度為 75 與 110 時分別達到 66% 與 80% 的轉換效率。進一步地,本研究將此轉頻平台與雙 Λ 型自發四波混頻雙光子源結合,實現觸發式原子雙光子波包的通訊波段轉換;當 2.5 MHz 的窄頻觸發式光子頻譜與轉頻器的高效率響應區域良好匹配時,轉換效率可達 79.4(2.6)% ,並保留強烈的時間關聯、單光子特性與明確的時間波包形狀。對於 17.4 MHz 的較寬輸入頻寬,轉換效率降至約 55%,但主要時間波包仍大致維持,顯示有限轉換頻寬主要造成頻譜邊緣損失,而非嚴重的時間模態變形。綜合而言,本論文建立並實現了冷原子系綜的高效率通訊波段量子轉頻介面,為連接原子相容窄頻量子光源、量子記憶與長距離光纖量子通訊提供重要基礎。

    This dissertation investigates a high-efficiency telecom quantum frequency interface in cold rubidium atomic ensembles for converting 795 nm near-infrared photons, which are compatible with atomic quantum memories and quantum nodes, into 1367 nm telecom-band photons suitable for low-loss fiber transmission while preserving their quantum states and nonclassical correlations. The work is based on diamond-type four-wave mixing and combines theoretical modeling, experimental optimization, and telecom conversion of correlated atomic biphotons. Theoretically, this dissertation develops semiclassical and fully quantum models to describe the conversion efficiency, residual transmission, quantum noise, and quantum-state fidelity of the frequency-conversion process. Using the Heisenberg-Langevin approach and the reduced-density-operator method, the theory shows that, under high-efficiency conditions, the diamond-type atomic ensemble can preserve quantum information encoded in photon-number, path, and polarization degrees of freedom. Experimentally, high-efficiency 795 nm to 1367 nm telecom conversion is first realized using weak coherent inputs. By characterizing the Λ-, cascade-, and V-type electromagnetically induced transparency responses and optimizing optical depth, coupling and driving fields, and optical detunings, signal conversion efficiencies of 66% and 80% are achieved at optical depths of 75 and 110, respectively. This converter is further integrated with a double-Λ spontaneous four-wave-mixing biphoton source to realize telecom conversion of heralded atomic biphoton wavepackets. When a 2.5 MHz heralded-photon spectrum is well matched to the high efficiency region of the converter response, a conversion efficiency of 79.4(2.6)% is obtained while preserving strong time-resolved correlations, single-photon characteristics, and well-defined temporal wavepackets. For a broader 17.4 MHz input bandwidth, the efficiency decreases to about 55%, whereas the dominant temporal waveform remains largely preserved, indicating that finite spectral acceptance mainly causes spectral-edge loss rather than severe temporal-mode distortion. These results establish a high-efficiency atom-based telecom quantum frequency interface and provide a foundation for connecting narrowband atomic quantum light sources, quantum memories, and long-distance fiber based quantum networks.

    摘要i Abstract ii 誌謝iii Table of Contents v List of Tables viii List of Figures ix Chapter 1. Introduction 1 Chapter 2. Semiclassical Description of Electromagnetically Induced Transparency 5 2.1 Introduction 5 2.2 Λ-Type EIT 6 2.2.1. Steady-State Analysis 9 2.2.2. Transient Analysis 11 2.3 Cascade-Type EIT 14 2.3.1. Steady-State Analysis 16 2.3.2. Transient Analysis 17 2.4 V-Type EIT 21 2.4.1. Steady-State Analysis 23 2.4.2. Transient Analysis 25 2.5 Comparison of Different EIT Configurations 27 Chapter 3. Semiclassical Model of Diamond-Type Four-Wave Mixing 29 3.1 Semiclassical Theory of Diamond-Type Four-Wave Mixing 29 3.2 Parameters for Optimal Conversion Efficiency 33 Chapter 4. Experimental Platform and Methods 37 4.1 Cold-Atom Preparation 37 4.1.1. Principles of Laser Cooling 38 4.1.2. Magneto-Optical Trap (MOT) 39 4.1.3. Rubidium-87 Atom 42 4.1.4. Vacuum System and Rubidium Source Operation 44 4.1.5. Laser Systems and Frequency Stabilization Mechanisms 44 4.2 1324 ECDL Frequency Stabilization System 51 4.3 Experimental Setup and Optical Geometry 53 4.3.1. Experimental Configuration for Λ-Type EIT 53 4.3.2. Experimental Configuration for Diamond-Type FWM 55 4.3.3. Experimental Setup for Cascade-Type and V-Type EIT 58 4.4 Rabi Frequencies, Clebsch-Gordan Coefficients, and Parameter Calibration 60 4.4.1. Definition of Rabi Frequency 60 4.4.2. Clebsch-Gordan Coefficients 61 4.4.3. Sub-Zeeman Population Distribution and Relaxation Matrix Elements In Λ-Type EIT 62 4.4.4. Sub-Zeeman Population Distribution and Relaxation Matrix Elements In Diamond-Type FWM 64 4.5 Timing Sequence and Experimental Control 67 4.5.1. Timing Sequence for Λ-Type EIT 67 4.5.2. Timing Sequence for Diamond-Type FWM and V-Type EIT 68 4.5.3. Timing Sequence for Cascade-Type EIT 69 Chapter 5. Semiclassical Experimental Results and Discussion 71 5.1 Λ-Type EIT Spectra and Optical Depth Calibration 71 5.2 Cascade-Type EIT Spectra and Pulse Evolution 74 5.3 V-Type EIT Spectra and Pulse Evolution 77 5.4 Spectral and Temporal Characteristics of Diamond-Type FWM 79 Chapter 6. Quantum Description of Diamond-Type Four-Wave Mixing 82 6.1 Quantum Theory of Diamond-Type Four-Wave Mixing 83 6.2 Quantum Noise, Einstein Relation, and Conversion Efficiency 93 6.2.1. Brownian Motion and the Classical Langevin Equation 93 6.2.2. The Langevin Equation in Quantum Optics 95 6.2.3. Einstein Relation 96 6.2.4. Conversion Efficiency and Theoretical Model Comparison 100 6.3 Quadrature Variance 101 6.3.1. Evolution of the Fock State 104 6.3.2. Evolution of the Coherent State 105 6.3.3. Evolution of the Squeezed State 105 6.4 Quantum Fidelity between the Converted Signal and Input Probe Fields 109 6.4.1. Formulation of the Converted Signal Field Density Matrix 109 6.4.2. Configuration of a Fock State Input Field 113 6.4.3. Configuration of a Coherent State Input Field 116 6.5 Qubit Retention 120 6.5.1. Photon-Number Encoding: Single-Rail-Encoded Qubit 120 6.5.2. Path-Encoded Qubit 123 6.5.3. Polarization-Encoded Qubit 126 Chapter 7. Biphoton Source Generation 128 7.1 Energy Level Structure and Biphoton Generation Mechanism 128 7.2 Generation Rate and Second-Order Correlated Functions 133 7.3 Biphoton Source Based on Atomic Ensembles 139 7.4 Experimental Configuration of the Quantum Frequency Conversion System 142 Chapter 8. Quantum Experimental Results and Discussion 145 8.1 Single-Photon-Level Cascade- and V-Type EIT 145 8.2 Coherent-State and Single-Photon Diamond-Type FWM 148 8.3 Preservation of Quantum Correlations through Frequency Conversion 149 8.3.1. Non-Classical Correlation Functions of the Biphoton Source 149 8.3.2. Preservation of Temporal Wavepackets via QFC 151 8.3.3. High-Efficiency QFC under Narrowband Single-Photon Condition 152 8.4 Analysis and Discussion 155 Chapter 9. Conclusion 159 References 161 Appendix A. Two Level System 170 A.1 Rotating Wave Approximation (RWA) 174 A.2 Unitary Transformation to the Rotating Frame 176 Appendix B. Coupling Solution in V-Type EIT 187 Appendix C. Derivation of the Corrected Correlation Functions with Experimental Imperfections 190

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