| 研究生: |
劉彥柏 Liu, Yan-Bo |
|---|---|
| 論文名稱: |
利用長延遲相互耦合半導體雷射產生物理隨機亂數 Physical random number generation using two mutually coupled semiconductor lasers with long delay time |
| 指導教授: |
黃勝廣
Hwang, Sheng-Kwang |
| 學位類別: |
碩士 Master |
| 系所名稱: |
理學院 - 光電科學與工程學系 Department of Photonics |
| 論文出版年: | 2026 |
| 畢業學年度: | 114 |
| 語文別: | 中文 |
| 論文頁數: | 88 |
| 中文關鍵詞: | 半導體雷射 、互注入系統 、雷射混沌 、亂數產生 、NIST SP 800-90B |
| 外文關鍵詞: | semiconductor laser, mutual injection system, laser chaos, random number generation, NIST SP 800-90B |
| 相關次數: | 點閱:5 下載:0 |
| 分享至: |
| 查詢本校圖書館目錄 查詢臺灣博碩士論文知識加值系統 勘誤回報 |
亂數在現今被廣泛應用於資訊安全、人工智慧和不同領域的蒙地卡羅模擬中。其中,亂數可依照不同產生方式,分為偽隨機亂數和物理隨機亂數;不同於偽隨機亂數利用公式計算,物理隨機數利用物理源本身的不可預測特性,如量子力學或非線性機制進行亂數產生。此亂數產生的優點可使亂數本身不具潛在週期性,大幅減少應用上可能的缺點。
本研究選用雷射互注入系統作為亂數產生的熵源。亂數產生速率和系統的頻寬有關,選用此系統的優勢為可產生較寬頻的混沌訊號。並且,由於同時使用兩雷射,因此在亂數產生中,具有雙通道輸出特性,進一步增加亂數產生的速率。但是在具有回饋機制的系統中,混沌動態受到時間延遲特徵(time-delay signature) TDS影響,導致混沌動態具有較高週期顯現性存在。
為了探討TDS對於亂數產生速率的影響。本研究首先討論系統操作在強度對稱注入下,探討不同區域對亂數產生的影響。透過固定失諧頻率在-20、-40、-60、-80和-100 GHz,將耦合強度逐漸增加,觀察對亂數產生的變化。得出當失諧頻率固定於-20、-40和-60 GHz時,系統的熵會因為混沌訊號週期成分增加而下降;而操作在-80和-100 GHz時,系統的熵不隨耦合強度增加而有明顯的下降趨勢,僅有數值上浮動的變化。
同時,本研究也探討互注入系統,在不同延遲時間下對於混沌動態的變化。利用平坦度地圖得知,選取同一操作點下,延遲時間的增加可使該操作點的平坦度略為上升,但不改變亂數產生速率。接著,本研究也針對幾個操作點進行強度非對稱注入,其結果為強度非對稱注入對於亂數產生速率的提升有限。
最後,透過不同條件及參數的模擬下,得出雷射在長延遲互注入系統下,亂數產生速率最高可達1.288 Tbit/s,適合作為超高速亂數產生的應用。
Random numbers are widely used in applications such as information security, artificial intelligence, and Monte Carlo simulations. One approach to generate random numbers is to take advantage of chaos excited in two mutually injected semiconductor lasers. The time series generated by the laser system, however, exhibits a periodic signature, known as time-delay signature (TDS), that results from the inherent nature of a delayed feedback system. It is the purpose of this study to understand how such a periodic signature affects the randomness of numbers generated by the laser system. Because the TDS increases with the coupling strength, this study investigates how entropy changes as the coupling strength increases. The results show that, when the detuning frequency is fixed at −20, −40, and −60 GHz, the entropy decreases with increasing coupling strength because the chaotic time series exhibits more regular patterns. In contrast, when the detuning frequency is fixed at −80 and −100 GHz, the entropy remains nearly unchanged as the coupling strength increases. Finally, the entropy rate and random bit generation rate of this system can reach up to 1.503 Tb/s and 1.288 Tb/s, respectively.
[1] N. Heninger, Z. Durumeric, E. Wustrow, and J. A. Halderman, "Mining your Ps and Qs: Detection of widespread weak keys in network devices," in 21st USENIX Security Symposium (USENIX Security 12), 2012, pp. 205–220.
[2] K. Li and Q. Cai, "Practical Security of RSA Against NTC-Architecture Quantum Computing Attacks," International Journal of Theoretical Physics, vol. 60, no. 8, pp. 2733–2744, Aug 2021, doi: 10.1007/s10773-021-04789-x.
[3] K. Lee, S. Lee, C. Seo, and K. Yim, "TRNG (True Random Number Genarator) Method Using Visible Spectrum for Secure Communication on 5G Network," Ieee Access, vol. 6, pp. 12838–12847, 2018 2018, doi: 10.1109/access.2018.2799682.
[4] K. Yoshimura et al., "Secure Key Distribution Using Correlated Randomness in Lasers Driven by Common Random Light," Physical Review Letters, vol. 108, no. 6, Feb 14 2012, Art no. 070602, doi: 10.1103/PhysRevLett.108.070602.
[5] M. Naruse, T. Matsubara, N. Chauvet, K. Kanno, T. Yang, and A. Uchida, "Generative adversarial network based on chaotic time series," Scientific Reports, vol. 9, Sep 10 2019, Art no. 12963, doi: 10.1038/s41598-019-49397-2.
[6] C.-H. Tseng, A. Uchida, and S.-K. Hwang, "Generation of High-Entropy, Bandwidth-Enhanced Chaos in Semiconductor Lasers for Tbit/S Random Bit Generation," in 2026 International Conference on Artificial Intelligence in Information and Communication (ICAIIC), 2026: IEEE, pp. 1115–1118.
[7] C. Franzke, T. O'Kane, J. Berner, P. Williams, and V. Lucarini, "Stochastic climate theory and modeling," Wiley Interdisciplinary Reviews-Climate Change, vol. 6, no. 1, pp. 63–78, Jan–Feb 2015, doi: 10.1002/wcc.318.
[8] M. Leutbecher et al., "Stochastic representations of model uncertainties at ECMWF: state of the art and future vision," Quarterly Journal of the Royal Meteorological Society, vol. 143, no. 707, pp. 2315–2339, Jul 2017, doi: 10.1002/qj.3094.
[9] J. Hart, Y. Terashima, A. Uchida, G. Baumgartner, T. Murphy, and R. Roy, "Recommendations and illustrations for the evaluation of photonic random number generators," Apl Photonics, vol. 2, no. 9, Sep 2017, Art no. 090901, doi: 10.1063/1.5000056.
[10] M. Herrero-Collantes and J. C. Garcia-Escartin, "Quantum random number generators," Reviews of Modern Physics, vol. 89, no. 1, p. 015004, 2017.
[11] T. Mikami et al., "Estimation of entropy rate in a fast physical random-bit generator using a chaotic semiconductor laser with intrinsic noise," Physical Review E, vol. 85, no. 1, Jan 23 2012, Art no. 016211, doi: 10.1103/PhysRevE.85.016211.
[12] P. Gaspard and X.-J. Wang, "Noise, chaos, and (e,‘r)-entropy per unit time."
[13] J. Dynes, Z. Yuan, A. Sharpe, and A. Shields, "A high speed, postprocessing free, quantum random number generator," Applied Physics Letters, vol. 93, no. 3, Jul 21 2008, Art no. 031109, doi: 10.1063/1.2961000.
[14] B. Wang et al., "Efficient quantum random number generation via simultaneously detecting photons in temporal and spatial dimensions," Scientific Reports, vol. 15, no. 1, May 30 2025, Art no. 18996, doi: 10.1038/s41598-025-03680-7.
[15] K. Tanizawa, K. Kato, and F. Futami, "Real-Time 50-Gbi/s Spatially Multiplexed Quantum Random Number Generator Based on Vacuum Fluctuation," Journal of Lightwave Technology, vol. 42, no. 4, pp. 1209–1214, Feb 15 2024, doi: 10.1109/jlt.2024.3353268.
[16] X. Wang et al., "Highly integrated broadband entropy source for quantum random number generators based on vacuum fluctuations," Science China-Information Sciences, vol. 69, no. 6, Feb 9 2026, Art no. 162501, doi: 10.1007/s11432-025-4660-1.
[17] B. Qi, Y. Chi, H. Lo, and L. Qian, "High-speed quantum random number generation by measuring phase noise of a single-mode laser," Optics Letters, vol. 35, no. 3, pp. 312–314, Feb 1 2010, doi: 10.1364/ol.35.000312.
[18] J. Li et al., "Quantum random number generation based on phase reconstruction," Optics Express, vol. 32, no. 4, pp. 5056–5071, Feb 12 2024, doi: 10.1364/oe.515390.
[19] C. Bruynsteen, T. Gehring, C. Lupo, J. Bauwelinck, and X. Yin, "100-Gbit/s Integrated Quantum Random Number Generator Based on Vacuum Fluctuations," Prx Quantum, vol. 4, no. 1, Mar 2023, Art no. 010330, doi: 10.1103/PRXQuantum.4.010330.
[20] G. Cao, L. Zhang, X. Huang, W. Hu, and X. Yang, "16.8 Tb/s True Random Number Generator Based on Amplified Spontaneous Emission," Ieee Photonics Technology Letters, vol. 33, no. 14, pp. 699–702, Jul 15 2021, doi: 10.1109/lpt.2021.3088156.
[21] Y. Guo et al., "40 Gb/s quantum random number generation based on optically sampled amplified spontaneous emission," Apl Photonics, vol. 6, no. 6, Jun 1 2021, Art no. 066105, doi: 10.1063/5.0040250.
[22] Y. Akizawa et al., "Fast Random Number Generation With Bandwidth-Enhanced Chaotic Semiconductor Lasers at 8 x 50 Gb/s," Ieee Photonics Technology Letters, vol. 24, no. 12, pp. 1042–1044, Jun 15 2012, doi: 10.1109/lpt.2012.2193388.
[23] K. Yoshiya, Y. Terashima, K. Kanno, and A. Uchida, "Entropy evaluation of white chaos generated by optical heterodyne for certifying physical random number generators," Optics Express, vol. 28, no. 3, pp. 3686–3698, Feb 3 2020, doi: 10.1364/oe.382234.
[24] I. Reidler, Y. Aviad, M. Rosenbluh, and I. Kanter, "Ultrahigh-Speed Random Number Generation Based on a Chaotic Semiconductor Laser," Physical Review Letters, vol. 103, no. 2, Jul 10 2009, Art no. 024102, doi: 10.1103/PhysRevLett.103.024102.
[25] Y. Kawaguchi, T. Okuma, K. Kanno, and A. Uchida, "Entropy rate of chaos in an optically injected semiconductor laser for physical random number generation," Optics Express, vol. 29, no. 2, pp. 2442–2457, Jan 18 2021, doi: 10.1364/oe.411694.
[26] V. KOVANIS, A. GAVRIELIDES, T. SIMPSON, and J. LIU, "INSTABILITIES AND CHAOS IN OPTICALLY INJECTED SEMICONDUCTOR-LASERS," Applied Physics Letters, vol. 67, no. 19, pp. 2780–2782, Nov 6 1995, doi: 10.1063/1.114591.
[27] T. Simpson, J. Liu, K. Huang, and K. Tai, "Nonlinear dynamics induced by external optical injection in semiconductor lasers," Quantum and Semiclassical Optics, vol. 9, no. 5, pp. 765–784, Oct 1997, doi: 10.1088/1355-5111/9/5/009.
[28] S. Hwang, J. Liu, and J. White, "Characteristics of period-one oscillations in semiconductor lasers subject to optical injection," Ieee Journal of Selected Topics in Quantum Electronics, vol. 10, no. 5, pp. 974–981, Sep–Oct 2004, doi: 10.1109/jstqe.2004.836017.
[29] F. Lin and J. Liu, "Chaotic radar using nonlinear laser dynamics," Ieee Journal of Quantum Electronics, vol. 40, no. 6, pp. 815–820, Jun 2004, doi: 10.1109/jqe.2004.828237.
[30] F. Lin, Y. Chao, and T. Wu, "Effective Bandwidths of Broadband Chaotic Signals," Ieee Journal of Quantum Electronics, vol. 48, no. 8, pp. 1010–1014, Aug 2012, doi: 10.1109/jqe.2012.2198195.
[31] Y. Wu, Y. Wang, P. Li, A. Wang, and M. Zhang, "Can Fixed Time Delay Signature be Concealed in Chaotic Semiconductor Laser With Optical Feedback?," Ieee Journal of Quantum Electronics, vol. 48, no. 11, pp. 1371–1379, Nov 2012, doi: 10.1109/jqe.2012.2212001.
[32] L. Wang, Q. He, A. Wang, and Y. Wang, "Wideband and flat-spectrum chaos generation from a semiconductor laser with strong dispersive light feedback," Ieice Nonlinear Theory and Its Applications, vol. 13, no. 1, pp. 36–43, 2022 2022, doi: 10.1587/nolta.13.36.
[33] L. Qiao et al., "Generation of flat wideband chaos based on mutual injection of semiconductor lasers," Optics Letters, vol. 44, no. 22, pp. 5394–5397, Nov 15 2019, doi: 10.1364/ol.44.005394.
[34] Q. Yang et al., "Flat Broadband Chaos Generation Using a Semiconductor Laser Subject to Asymmetric Dual-Path Optical Feedback," Journal of Lightwave Technology, vol. 39, no. 19, pp. 6246–6252, Oct 2021, doi: 10.1109/jlt.2021.3095972.
[35] R. Sakuraba, K. Iwakawa, K. Kanno, and A. Uchida, "Tb/s physical random bit generation with bandwidth-enhanced chaos in three-cascaded semiconductor lasers," Optics Express, vol. 23, no. 2, pp. 1470–1490, Jan 26 2015, doi: 10.1364/oe.23.001470.
[36] S. Xiang, B. Wang, Y. Wang, Y. Han, A. Wen, and Y. Hao, "2.24-Tb/s Physical Random Bit Generation With Minimal Post-Processing Based on Chaotic Semiconductor Lasers Network," Journal of Lightwave Technology, vol. 37, no. 16, pp. 3987–3993, Aug 15 2019, doi: 10.1109/jlt.2019.2920476.
[37] X. Tang et al., "Tbits/s physical random bit generation based on mutually coupled semiconductor laser chaotic entropy source," Optics Express, vol. 23, no. 26, pp. 33130–33141, Dec 28 2015, doi: 10.1364/oe.23.033130.
[38] M. Zhang et al., "A Hybrid Integrated Short-External-Cavity Chaotic Semiconductor Laser," Ieee Photonics Technology Letters, vol. 29, no. 21, pp. 1911–1914, Nov 1 2017, doi: 10.1109/lpt.2017.2756906.
[39] M. Chai et al., "Simulation of Monolithically Integrated Semiconductor Laser Subject to Random Feedback and Mutual Injection," Ieee Journal of Quantum Electronics, vol. 56, no. 5, pp. 1–8, Oct 2020, doi: 10.1109/jqe.2020.3010812.
[40] Y. Peng et al., "Broadband chaos of an interband cascade laser with a 6-GHz bandwidth," Optics Letters, vol. 49, no. 11, pp. 3142–3145, Jun 1 2024, doi: 10.1364/ol.525636.
[41] X. Wei, L. Qiao, B. Wang, M. Chai, and M. Zhang, "Generation of Wideband Chaos With Time-Delay Signature Suppression in Semiconductor Lasers by Asymmetrical Mutual Injection," Journal of Lightwave Technology, vol. 42, no. 5, pp. 1556–1565, Mar 1 2024, doi: 10.1109/jlt.2023.3322629.
[42] J. Shen et al., "Conversion between anticipating and lag chaos synchronization induced by different bias current levels in mutually delay-coupled semiconductor lasers," Applied Physics B-Lasers and Optics, vol. 103, no. 4, pp. 941–945, Jun 2011, doi: 10.1007/s00340-010-4347-5.
[43] J. Hu and J. Ma, "Synchronization and communication of two mutual coupling lasers subject to incoherent injection," Journal of Modern Optics, vol. 56, no. 8, pp. 1029–1035, 2009 2009, doi: 10.1080/09500340902898432.
[44] L. Jia-Ming and T. B. Simpson, "Four-wave mixing and optical modulation in a semiconductor laser," IEEE Journal of Quantum Electronics, vol. 30, no. 4, pp. 957–965, 1994, doi: 10.1109/3.291366.
[45] B. Liao, C. Tseng, Y. Chu, and S. Hwang, "Effects of Asymmetric Coupling Strength on Nonlinear Dynamics of Two Mutually Long-Delay-Coupled Semiconductor Lasers," Photonics, vol. 9, no. 1, Jan 2022, Art no. 28, doi: 10.3390/photonics9010028.
[46] C. Sun et al., "Modulation Characteristics Enhancement of Monolithically Integrated Laser Diodes Under Mutual Injection Locking," Ieee Journal of Selected Topics in Quantum Electronics, vol. 21, no. 6, Nov–Dec 2015, Art no. 1802008, doi: 10.1109/jstqe.2015.2478817.
[47] J. Tang et al., "Experimental Research on Dynamic Characteristics of Mutual Optical Injection Semiconductor Lasers With Long Delay," Journal of Lightwave Technology, vol. 43, no. 7, pp. 3366–3375, Apr 1 2025, doi: 10.1109/jlt.2024.3516208.
[48] G. Gottwald and I. Melbourne, "Testing for chaos in deterministic systems with noise," Physica D-Nonlinear Phenomena, vol. 212, no. 1-2, pp. 100–110, Dec 1 2005, doi: 10.1016/j.physd.2005.09.011.
[49] G. Gottwald and I. Melbourne, "On the Implementation of the 0-1 Test for Chaos," Siam Journal on Applied Dynamical Systems, vol. 8, no. 1, pp. 129–145, 2009 2009, doi: 10.1137/080718851.
[50] Y. Qu, S. Xiang, Y. Wang, L. Lin, A. Wen, and Y. Hao, "Concealment of Time Delay Signature of Chaotic Semiconductor Nanolasers With Double Chaotic Optical Injections," Ieee Journal of Quantum Electronics, vol. 55, no. 2, Apr 2019, Art no. 2000407, doi: 10.1109/jqe.2019.2898673.
[51] F. Lin and J. Liu, "Nonlinear dynamical characteristics of an optically injected semiconductor laser subject to optoelectronic feedback," Optics Communications, vol. 221, no. 1-3, pp. 173–180, Jun 1 2003, doi: 10.1016/s0030-4018(03)01466-4.
[52] M. S. Turan, E. Barker, J. Kelsey, K. McKay, M. Baish, and M. Boyle, "Recommendation for the Entropy Sources Used for Random Bit Generation," ed: Special Publication (NIST SP), National Institute of Standards and Technology, Gaithersburg, MD, 2018.
[53] M. Aslan, A. Doğanaksoy, Z. Saygı, M. Sönmez Turan, and F. Sulak, "Observations on NIST SP 800-90B entropy estimators," Cryptography and Communications, vol. 18, no. 1, pp. 63–81, 2026.
[54] F. Lin and J. Liu, "Diverse waveform generation using semiconductor lasers for radar and microwave applications," Ieee Journal of Quantum Electronics, vol. 40, no. 6, pp. 682–689, Jun 2004, doi: 10.1109/jqe.2004.828254.