| 研究生: |
劉洪生 Liu, Hung-Sheng |
|---|---|
| 論文名稱: |
量子神經網路中Ansatz架構對模型表現之效應 The Effects of Ansatz Architecture on the Performance of Quantum Neural Networks |
| 指導教授: |
陳宏斌
Chen, Hong-Bin |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 工程科學系 Department of Engineering Science |
| 論文出版年: | 2026 |
| 畢業學年度: | 114 |
| 語文別: | 英文 |
| 論文頁數: | 83 |
| 中文關鍵詞: | 量子神經網路 、參數化量子電路 、Ansatz 架構 、量子資訊 、量子操縱性 |
| 外文關鍵詞: | Quantum neural networks, Parameterized quantum circuits, Ansatz architecture, Quantum information, Quantum steering |
| 相關次數: | 點閱:2 下載:0 |
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隨著量子計算與量子機器學習的發展,如何設計合適的參數化量子電路已成為量子神經網路中的重要問題。量子神經網路的學習能力不只取決於參數數量,也會受到ansatz 架構、電路深度、耦合方式與量子態空間中有效參數方向的影響。因此,如何理解不同ansatz 架構對模型表現的影響,是近程量子機器學習中值得研究的問題。
本論文以雙量子位元態的量子操縱性問題作為迴歸任務,研究ansatz架構對量子神經網路表現的影響。模型的輸入為與量子操縱性相關的特徵表示,預測目標為透過半正定規劃程序產生的最大可操縱權重。在固定的學習框架下,本研究比較由不同局域旋轉、耦合區塊、連接方式與電路層數所形成的ansatz架構。
本研究以迴歸表現評估訓練後的模型,並進一步透過expressibility、entangling power、量子費雪資訊矩陣(QFIM)秩與梯度變異數來描述不同電路架構的性質。這些觀察量用來連結模型的預測行為與ansatz的量子態生成能力、有效參數方向及可訓練性。
結果顯示,增加電路深度可以提升量子神經網路的表現,但提升幅度會受到ansatz 架構明顯影響。即使參數成長方式相近,不同電路仍可能呈現不同的有效參數方向、可訓練性與預測表現。特別是當QFIM秩達到飽和後,額外增加的層數不一定提供新的獨立方向,但超參數化仍可能影響最佳化過程,使模型表現緩慢提升。整體而言,本研究顯示有效的ansatz需要在表達能力、糾纏生成能力、有效參數方向與可訓練性之間取得合適的平衡。
With the development of quantum computing and quantum machine learning, the design of suitable parameterized quantum circuits has become an important issue in quantum neural networks (QNNs). The learning performance of a QNN is not determined only by the number of rainable parameters, but can also depend on the ansatz architecture, circuit depth, coupling structure, and effective parameter directions in the quantum state space. Understanding how different ansatz architectures affect model performance is therefore an important roblem for near-term quantum machine learning.
This dissertation uses a quantum steering problem of qubit-pair states as a regression task to study the effect of ansatz architecture on QNN performance. The input data are steering-related feature representations, and the learning target is the ground-truth maximum steerable weight generated by a semidefinite programming-based procedure. Under a fixed learning framework, different ansatz architectures are compared by changing the local rotation blocks, coupling blocks, connectivity patterns, and circuit depths.
The trained models are evaluated by their regression performance, and the circuit architectures are further characterized using expressibility, entangling power, quantum Fisher information matrix (QFIM) rank, and gradient variance. These quantities are used to connect the observed prediction behavior with the state generation ability, effective parameter directions, and trainability of each ansatz.
The results show that increasing circuit depth can improve QNN performance, but the improvement is strongly dependent on the ansatz architecture. Circuits with similar parameter growth can exhibit different ffective parameter directions, trainability, and prediction performance. In particular, QFIM-rank saturation in dicates that additional layers do not always introduce new independent directions, while overparameterization may still influence optimization and allow gradual performance improvement. Overall, the results suggest that an effective ansatz should balance expressibility, entangling power, effective parameter directions, and trainability.
[1] Qiskit Machine Learning, “Quantum neural networks”, https://qiskit-community.github.io/qiskit-machine-learning/tutorials/01_neural_networks.html (2026), qiskit Machine Learning 0.9.0, accessed 2026-05-25.
[2] J. Preskill, “Quantum computing in the NISQ era and beyond”, Quantum 2, 79 (2018).
[3] J. R. McClean, J. Romero, R. Babbush, and A. Aspuru-Guzik, “The theory of variational hybrid quantum-classical algorithms”, New Journal of Physics 18, 023023 (2016).
[4] M. Cerezo, A. Arrasmith, R. Babbush, S. C. Benjamin, S. Endo, K. Fujii, J. R.McClean, K. Mitarai, X. Yuan, L. Cincio, and P. J. Coles, “Variational quantum algorithms”, Nature Reviews Physics 3, 625 (2021).
[5] M. Schuld and N. Killoran, “Quantum machine learning in feature Hilbert spaces”,Physical Review Letters 122, 040504 (2019).
[6] V. Havlicek, A. D. Corcoles, K. Temme, A. W. Harrow, A. Kandala, J. M. Chow, and J. M. Gambetta, “Supervised learning with quantum-enhanced feature spaces”, Nature 567, 209 (2019).
[7] K. Mitarai, M. Negoro, M. Kitagawa, and K. Fujii, “Quantum circuit learning”, Physical Review A 98, 032309 (2018).
[8] M. Schuld, A. Bocharov, K. M. Svore, and N. Wiebe, “Circuit-centric quantum classifiers”, Physical Review A 101, 032308 (2020).
[9] S. Sim, P. D. Johnson, and A. Aspuru-Guzik, “Expressibility and entangling capability of parameterized quantum circuits for hybrid quantum-classical algorithms”, Advanced Quantum Technologies 2, 1900070 (2019).
[10] T. Hubregtsen, J. Pichlmeier, P. Stecher, and K. Bertels, “Evaluation of parameterized quantum circuits: On the relation between classification accuracy, expressibility, and entangling capability”, Quantum Machine Intelligence 3, 9 (2021).
[11] M. Larocca, N. Ju, D. Garcia-Martin, P. J. Coles, and M. Cerezo, “Theory of overparametrization in quantum neural networks”, Nature Computational Science 3, 542 (2023).
[12] J. R. McClean, S. Boixo, V. N. Smelyanskiy, R. Babbush, and H. Neven, “Barren plateaus in quantum neural network training landscapes”, Nature Communications 9, 4812 (2018).
[13] Z. Holmes, K. Sharma, M. Cerezo, and P. J. Coles, “Connecting ansatz expressibility to gradient magnitudes and barren plateaus”, PRX Quantum 3, 010313 (2022).
[14] C. O. Marrero, M. Kieferova, and N. Wiebe, “Entanglement-induced barren plateaus”, PRX Quantum 2, 040316 (2021).
[15] H. Hashimoto, A. Nakabayashi, L. Nagano, Y. Iiyama, R. Sawada, J. Tanaka, and K. Terashi, “Comprehensive numerical studies of barren plateau and overparametrization in variational quantum algorithm” (2026), arXiv:2602.03291 [quant-ph].
[16] H. M. Wiseman, S. J. Jones, and A. C. Doherty, “Steering, entanglement, nonlocality, and the einstein-podolsky-rosen paradox”, Phys. Rev. Lett. 98, 140402 (2007).
[17] R. Uola, A. C. S. Costa, H. C. Nguyen, and O. Gühne, “Quantum steering”, Rev. Mod. Phys. 92, 015001 (2020).
[18] N. Brunner, D. Cavalcanti, S. Pironio, V. Scarani, and S. Wehner, “Bell nonlocality”, Rev. Mod. Phys. 86, 419 (2014).
[19] A. Einstein, B. Podolsky, and N. Rosen, “Can quantum-mechanical description of physical reality be considered complete?”, Phys. Rev. 47, 777 (1935).
[20] J. S. Bell, “On the einstein podolsky rosen paradox”, Physics 1, 195 (1964).
[21] D. Cavalcanti and P. Skrzypczyk, “Quantum steering: A review with focus on semidefinite programming”, Reports on Progress in Physics 80, 024001 (2017).
[22] C. Branciard, E. G. Cavalcanti, S. P. Walborn, V. Scarani, and H. M. Wiseman,“One-sided device-independent quantum key distribution: Security, feasibility, and the connection with steering”, Physical Review A 85, 010301 (2012).
[23] H.-M. Wang, H.-Y. Ku, J.-Y. Lin, and H.-B. Chen, “Deep learning the hierarchy of steering measurement settings of qubit-pair states”, Communications Physics 7, 72 (2024).
[24] Z.-L. Tsai, H.-M. Wang, and H.-B. Chen, “Learning the hierarchy of steering measurement settings of qubit-pair states with kernel-based quantum models”, New Journal of Physics 27, 094502 (2025).
[25] V. Dunjko and H. J. Briegel, “Machine learning & artificial intelligence in the quantum domain: A review of recent progress”, Reports on Progress in Physics 81, 074001 (2018).
[26] M. Benedetti, E. Lloyd, S. Sack, and M. Fiorentini, “Parameterized quantum circuits as machine learning models”, Quantum Science and Technology 4, 043001 (2019).
[27] A. Abbas, D. Sutter, C. Zoufal, A. Lucchi, A. Figalli, and S. Woerner, “The power of quantum neural networks”, Nature Computational Science 1, 403 (2021).
[28] R. Horodecki, P. Horodecki, M. Horodecki, and K. Horodecki, “Quantum entanglement”, Rev. Mod. Phys. 81, 865 (2009).
[29] D. A. Meyer and N. R. Wallach, “Global entanglement in multiparticle systems”, Journal of Mathematical Physics 43, 4273 (2002).
[30] G. K. Brennen, “An observable measure of entanglement for pure states of multiqubit systems”, Quantum Information and Computation 3, 619 (2003).
[31] K. Życzkowski and H.-J. Sommers, “Average fidelity between random quantum states”, Physical Review A 71, 032313 (2005).
[32] K. Nakaji and N. Yamamoto, “Expressibility of the alternating layered ansatz for quantum computation”, Quantum 5, 434 (2021).
[33] S. L. Braunstein and C. M. Caves, “Statistical distance and the geometry of quantum states”, Physical Review Letters 72, 3439 (1994).
[34] J. J. Meyer, “Fisher information in noisy intermediate-scale quantum applications”, Quantum 5, 539 (2021).
[35] T. Haug, K. Bharti, and M. S. Kim, “Capacity and quantum geometry of parametrized quantum circuits”, PRX Quantum 2, 040309 (2021).
[36] M. Schuld, V. Bergholm, C. Gogolin, J. Izaac, and N. Killoran, “Evaluating analytic gradients on quantum hardware”, Physical Review A 99, 032331 (2019).
[37] M. Cerezo, A. Sone, T. Volkoff, L. Cincio, and P. J. Coles, “Cost function dependent barren plateaus in shallow parametrized quantum circuits”, Nature Communications 12, 1791 (2021).
[38] P. Skrzypczyk, M. Navascués, and D. Cavalcanti, “Quantifying einstein-podolskyrosen steering”, Phys. Rev. Lett. 112, 180404 (2014).