| 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 |
| 相關次數: | 點閱:61 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 |
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.
[1] C. Shu, X. Guo, P. Chen, M. M. T. Loy, and S. Du, “Narrowband biphotons with polarization-frequency-coupled entanglement,” Phys. Rev. A, vol. 91, p. 043820, 2015.
[2] C. Chen, C. Xu, A. Riazi, E. Y. Zhu, A. V. Gladyshev, P. G. Kazansky, and L. Qian, “Broadband fiber-based entangled photon-pair source at telecom o-band,” Opt. Lett., vol. 46, pp. 1261–1264, 2021.
[3] J. Bae, J. Park, Y. J. Yu, H.-R. Noh, and H. S. Moon, “Polarization-entangled pho ton pairs from warm atomic ensemble with magnetic background noise,” Adv. Quantum Technol., vol. 6, p. 2200118, 2023.
[4] Y.-W. Cho, K.-K. Park, J.-C. Lee, and Y.-H. Kim, “Engineering frequency-time quantum correlation of narrow-band biphotons from cold atoms,” Phys. Rev. Lett., vol. 113, p. 063602, 2014.
[5] H. Jeong, S. Du, and N. Y. Kim, “Proposed narrowband biphoton generation from an ensemble of solid-state quantum emitters,” J. Opt. Soc. Am. B, vol. 36, pp. 646–651, 2019.
[6] H. Liu and A. S. Helmy, “Joint measurement of time–frequency entanglement via sum frequency generation,” npj Quantum Inf., vol. 6, p. 66, 2020.
[7] A. Mair, A. Vaziri, G. Weihs, and A. Zeilinger, “Entanglement of the orbital angular momentum states of photons,” Nature, vol. 412, p. 313–316, 2001.
[8] Z.-Y. Zhou, Y. Li, D.-S. Ding, W. Zhang, S. Shi, B.-S. Shi, and G.-C. Guo, “Orbital angular momentum photonic quantum interface,” Light Sci. Appl., vol. 5, p. e16019, 2016.
[9] X. Qiu, H. Guo, Y. Ren, and L. Chen, “High-dimensional photonic orbital-angular momentum frequency interface,” Phys. Rev. Appl., vol. 19, p. 044072, 2023.
[10] C.-W. Lin, Y.-T. Ma, J.-S. Shiu, and Y.-F. Chen, “Polarization entanglement in atomic biphotons via orbital-angular-momentum-to-spin mapping,” Phys. Rev. A, vol. 113, p. L041702, 2026.
[11] T. Honjo, S. W. Nam, H. Takesue, Q. Zhang, H. Kamada, Y. Nishida, O. Tadanaga, M.Asobe, B. Baek, R. Hadfield, S. Miki, M. Fujiwara, M. Sasaki, Z. Wang, K. Inoue, and Y. Yamamoto, “Long-distance entanglement-based quantum key distribution over optical fiber,” Opt. Express, vol. 16, pp. 19118–19126, 2008.
[12] D. P. Nadlinger, P. Drmotaa, B. C. Nichol, G. Araneda, D. Main, R. Srinivas, D. M. Lucas, C. J. Ballance, K. Ivanov, E. Y.-Z. Tan, P. Sekatski, R. L. Urbanke, R. Renner, N. Sangouard, and J.-D. Bancal, “Experimental quantum key distribution certified by bell’s theorem,” Nature, vol. 607, p. 682–686, 2022.
[13] X.-H. Zhan, S. Wang, Z.-Q. Zhong, Z.-Q. Yin, W. Chen, D.-Y. He, G.-C. Guo, and Z.-F. Han, “Quantum key distribution with a continuous-wave-pumped spontaneous-parametric-down-conversion heralded single-photon source,” Phys. Rev. Appl., vol. 19, p. 034027, 2023.
[14] Y. Liu, W.-J. Zhang, C. Jiang, J.-P. Chen, C. Zhang, W.-X. Pan, D. Ma, H. Dong, J. M. Xiong, C.-J. Zhang, H. Li, R.-C. Wang, J. Wu, T.-Y. Chen, L. You, X.-B. Wang, Q. Zhang, and J.-W. Pan, “Experimental twin-field quantum key distribution over 1000 km fiber distance,” Phys. Rev. Lett., vol. 130, p. 210801, 2023.
[15] C. H. Bennett, G. Brassard, C. Crépeau, R. Jozsa, A. Peres, and W. K. Wootters, “Teleporting an unknown quantum state via dual classical and einstein-podolsky-rosen channels,” Phys. Rev. Lett., vol. 70, pp. 1895–1899, 1993.
[16] D. Bouwmeester, J.-W. Pan, K. Mattle, M. Eibl, H. Weinfurter, and A. Zeilinger, “Experimental quantum teleportation,” Nature, vol. 390, p. 575–579, 1997.
[17] X.-S. Ma, T. Herbst, T. Scheidl, D. Wang, S. Kropatschek, W. Naylor, B. Wittmann, A. Mech, J. Kofler, E. Anisimova, V. Makarov, T. Jennewein, R. Ursin, and A. Zeilinger, “Quantum teleportation over 143 kilometres using active feed-forward,” Nature, vol. 489, p. 269–273, 2012.
[18] R. Valivarthi, S. I. Davis, C. Peña, S. Xie, N. Lauk, L. Narváez, J. P. Allmaras, A. D. Beyer, Y. Gim, M. Hussein, G. Iskander, H. L. Kim, B. Korzh, A. Mueller, M. Romin sky, M. Shaw, D. Tang, E. E. Wollman, C. Simon, P. Spentzouris, D. Oblak, N. Sinclair, and M. Spiropulu, “Teleportation systems toward a quantum internet,” PRX Quantum, vol. 1, p. 020317, 2020.
[19] T. Strobel, M. Vyvlecka, I. Neureuther, T. Bauer, M. Schäfer, S. Kazmaier, N. L. Sharma, R. Joos, J. H. Weber, C. Nawrath, W. Nie, G. Bhayani, C. Hopfmann, C. Becher, P. Michler, and S. L. Portalupi, “Telecom-wavelength quantum teleportation using frequency-converted photons from remote quantum dots,” Nat. Commun., vol. 16, p. 10027, 2025.
[20] C. K. Hong, Z. Y. Ou, and L. Mandel, “Measurement of subpicosecond time intervals between two photons by interference,” Phys. Rev. Lett., vol. 59, pp. 2044–2046, 1987.
[21] H. Kim, D. Kim, J. Park, and H. S. Moon, “Hong–ou–mandel interference of two independent continuous-wave coherent photons,” Photon. Res., vol. 8, pp. 1491–1495, 2020.
[22] H. Ollivier, S. E. Thomas, S. C. Wein, I. M. de Buy Wenniger, N. Coste, J. C. Loredo, N. Somaschi, A. Harouri, A. Lemaitre, I. Sagnes, L. Lanco, C. Simon, C. Anton, O. Krebs, and P. Senellart, “Hong-ou-mandel interference with imperfect single pho ton sources,” Phys. Rev. Lett., vol. 126, p. 063602, 2021.
[23] Y.-S. Kim, T. Pramanik, Y.-W. Cho, M. Yang, S.-W. Han, S.-Y. Lee, M.-S. Kang, and S. Moon, “Informationally symmetrical bell state preparation and measurement,” Opt. Express, vol. 26, pp. 29539–29549, 2018.
[24] E. Arenskötter, S. Kucera, O. Elshehy, M. Bergerhoff, M. Kreis, L. Brunel, and J. Es chner, “Full bell-basis measurement of an atom-photon 2-qubit state and its application for quantum networks,” Phys. Rev. Res., vol. 6, p. 023061, 2024.
[25] N. Hauser, M. J. Bayerbach, S. E. D'Aurelio, R. Weber, M. Santandrea, S. P. Ku mar, I. Dhand, and S. Barz, “Boosted bell-state measurements for photonic quantum computation,” npj Quantum Inf., vol. 11, p. 41, 2025.
[26] P. Kumar, “Quantum frequency conversion,” Opt. Lett., vol. 15, pp. 1476–1478, 1990.
[27] S. Zaske, A. Lenhard, C. A. Keßler, J. Kettler, C. Hepp, C. Arend, R. Albrecht, W. M. Schulz, M. Jetter, P. Michler, and C. Becher, “Visible-to-telecom quantum frequency conversion of light from a single quantum emitter,” Phys. Rev. Lett., vol. 109, p. 147404, 2012.
[28] N. Maring, D. Lago-Rivera, A. Lenhard, G. Heinze, and H. de Riedmatten, “Quantum frequency conversion of memory-compatible single photons from 606 nm to the telecom c-band,” Optica, vol. 5, pp. 507–513, 2018.
[29] C. L. Morrison, M. Rambach, Z. X. Koong, F. Graffitti, F. Thorburn, A. K. Kar, Y. Ma, S.-I. Park, J. D. Song, N. G. Stoltz, D. Bouwmeester, A. Fedrizzi, and B. D. Gerardot, “A bright source of telecom single photons based on quantum frequency conversion,” Appl. Phys. Lett., vol. 118, p. 174003, 2021.
[30] S. Wengerowsky, S. Duranti, L. Heller, and H. de Riedmatten, “Quantum frequency conversion of photons with microsecond duration from the visible to the telecommunication c band,” Phys. Rev. Appl., vol. 23, p. 024049, 2025.
[31] A. G. Radnaev, Y. O. Dudin, R. Zhao, H. H. Jen, S. D. Jenkins, A. Kuzmich, and T. A. B. Kennedy, “A quantum memory with telecom-wavelength conversion,” Nature Phys., vol. 6, pp. 894–899, 2010.
[32] Y. O. Dudin, A. G. Radnaev, R. Zhao, J. Z. Blumoff, T. A. B. Kennedy, and A. Kuzmich, “Entanglement of light-shift compensated atomic spin waves with telecom light,” Phys. Rev. Lett., vol. 105, p. 260502, 2010.
[33] W.-H. Zhang, Y.-H. Ye, L. Zeng, M.-X. Dong, E.-Z. Li, J.-Y. Peng, Y. Li, D.-S. Ding, and B.-S. Shi, “Telecom-wavelength conversion in a high optical depth cold atomic system,” Opt. Express, vol. 31, pp. 8042–8048, 2023.
[34] L.-C. Chen, M.-Y. Lin, J.-S. Shiu, X.-Q. Zhong, P.-H. Tseng, and Y.-F. Chen, “High efficiency telecom frequency conversion via a diamond-type atomic ensemble,” Phys. Rev. A, vol. 112, p. 013709, 2025.
[35] R. T. Willis, F. E. Becerra, L. A. Orozco, and S. L. Rolston, “Four-wave mixing in the diamond configuration in an atomic vapor,” Phys. Rev. A, vol. 79, p. 033814, 2009.
[36] F. E. Becerra, R. T. Willis, S. L. Rolston, H. J. Carmichael, and L. A. Orozco, “Non degenerate four-wave mixing in rubidium vapor: Transient regime,” Phys. Rev. A, vol. 82, p. 043833, 2010.
[37] H. Jeong, H. Kim, J. Bae, J. Park, and H. S. Moon, “Doppler-broadened four-wave mixing under double-resonance optical pumping in the 5s1/2–5p3/2–4d5/2 transition of warm 87rb atoms,” Opt. Express, vol. 29, pp. 42384–42393, 2021.
[38] A. Hamer, S. M. R. Tabar, P. Yashwantrao, A. Aghababaei, F. Vewinger, and S. Stellmer, “Frequency conversion to the telecom o-band using pressurized hydrogen,” Opt. Lett., vol. 49, pp. 506–509, 2024.
[39] A. Hamer, F. Vewinger, T. Peters, M. H. Frosz, and S. Stellmer, “Frequency conversion in a hydrogen-filled hollow-core fiber using continuous-wave fields,” Opt. Lett., vol. 49, pp. 6952–6955, 2024.
[40] J. A. Rowland, C. Perrella, R. F. Offer, A. N. Luiten, B. M. Sparkes, and T. J. Weinhold, “Characterization of near-infrared to telecom frequency conversion in a rubidium-filled hollow-core photonic-crystal fiber,” Opt. Express, vol. 33, pp. 18076 18088, 2025.
[41] T. van Leent, M. Bock, R. Garthoff, K. Redeker, W. Zhang, T. Bauer, W. Rosenfeld, C. Becher, and H. Weinfurter, “Long-distance distribution of atom-photon entanglement at telecom wavelength,” Phys. Rev. Lett., vol. 124, p. 010510, 2020.
[42] R. Ikuta, Y. Kusaka, T. Kitano, H. Kato, T. Yamamoto, M. Koashi, and N. Imoto, “Wide-band quantum interface for visible-to-telecommunication wavelength conversion,” Nat. Commun., vol. 2, p. 537, 2011.
[43] X. Fernandez-Gonzalvo, G. Corrielli, B. Albrecht, M. Grimau, M. Cristiani, and H. de Riedmatten, “Quantum frequency conversion of quantum memory compatible photons to telecommunication wavelengths,” Opt. Express, vol. 21, pp. 19473–19487, 2013.
[44] L.-M. Duan, M. D. Lukin, J. I. Cirac, and P. Zoller, “Long-distance quantum communication with atomic ensembles and linear optics,” Nature, vol. 414, p. 413–418, 2001.
[45] L.-C. Chen, C.-W. Lin, J.-S. Shiu, W.-L. Chen, Y.-C. Wang, and Y.-F. Chen, “High efficiency telecom conversion of heralded atomic biphoton wavepackets,” Opt. Lett., vol. 51, pp. 3862–3865, 2026.
[46] T. Chanelière, D. N. Matsukevich, S. D. Jenkins, T. A. B. Kennedy, M. S. Chapman, and A. Kuzmich, “Quantum telecommunication based on atomic cascade transitions,” Phys. Rev. Lett., vol. 96, p. 093604, 2006.
[47] R. T. Willis, F. E. Becerra, L. A. Orozco, and S. L. Rolston, “Correlated photon pairs generated from a warm atomic ensemble,” Phys. Rev. A, vol. 82, p. 053842, 2010.
[48] R. T. Willis, F. E. Becerra, L. A. Orozco, and S. L. Rolston, “Photon statistics and polarization correlations at telecommunications wavelengths from a warm atomic ensemble,” Opt. Express, vol. 19, pp. 14632–14641, 2011.
[49] H. H. Jen, “Cascaded cold atomic ensembles in a diamond configuration as a spectrally entangled multiphoton source,” Phys. Rev. A, vol. 95, p. 043840, 2017.
[50] K. Niizeki, K. Ikeda, M. Zheng, X. Xie, K. Okamura, N. Takei, N. Namekata, S. Inoue, H. Kosaka, and T. Horikiri, “Ultrabright narrow-band telecom two-photon source for long-distance quantum communication,” Appl. Phys. Express, vol. 11, p. 042801, 2018.
[51] M.-Y. Gao, Y.-H. Li, Y. Li, Z. Zhou, G.-C. Guo, Z.-Y. Zhou, and B.-S. Shi, “Narrow band telecom-band polarization-entangled photon source by superposed monolithic cavities,” Phys. Rev. A, vol. 109, p. 033720, 2024.
[52] E. Pomarico, B. Sanguinetti, N. Gisin, R. Thew, H. Zbinden, G. Schreiber, A. Thomas, and W. Sohler, “Waveguide-based opo source of entangled photon pairs,” New J. Phys., vol. 11, p. 113042, 2009.
[53] Z.-Y. Zhou, D.-S. Ding, Y. Li, F.-Y. Wang, and B.-S. Shi, “Cavity-enhanced bright photon pairs at telecom wavelengths with a triple-resonance configuration,” J. Opt. Soc. Am. B, vol. 31, pp. 128–134, 2014.
[54] Y.-S. Wang, K.-B. Li, C.-F. Chang, T.-W. Lin, J.-Q. Li, S.-S. Hsiao, J.-M. Chen, Y.-H. Lai, Y.-C. Chen, Y.-F. Chen, C.-S. Chuu, and I. A. Yu, “Temporally ultralong biphotons with a linewidth of 50 khz,” APL Photonics, vol. 7, p. 126102, 2022.
[55] S. E. Harris, J. E. Field, and A. Imamoğlu, “Nonlinear optical processes using electro magnetically induced transparency,” Phys. Rev. Lett., vol. 64, pp. 1107–1110, 1990.
[56] K.-J. Boller, A. Imamoğlu, and S. E. Harris, “Observation of electromagnetically induced transparency,” Phys. Rev. Lett., vol. 66, pp. 2593–2596, 1991.
[57] M. Fleischhauer and M. D. Lukin, “Dark-state polaritons in electromagnetically induced transparency,” Phys. Rev. Lett., vol. 84, pp. 5094–5097, 2000.
[58] D. A. Braje, V. Balić, S. Goda, G. Y. Yin, and S. E. Harris, “Frequency mixing using electromagnetically induced transparency in cold atoms,” Phys. Rev. Lett., vol. 93, p. 183601, 2004.
[59] M. Kiffner and T. N. Dey, “Dynamical control of pulse propagation in electromagnetically induced transparency,” Phys. Rev. A, vol. 79, p. 023829, 2009.
[60] N. Lauk, C. O’Brien, and M. Fleischhauer, “Fidelity of photon propagation in electromagnetically induced transparency in the presence of four-wave mixing,” Phys. Rev. A, vol. 88, p. 013823, 2013.
[61] H. Hsu, C.-Y. Cheng, J.-S. Shiu, L.-C. Chen, and Y.-F. Chen, “Quantum fidelity of electromagnetically induced transparency: the full quantum theory,” Opt. Express, vol. 30, pp. 2097–2111, 2022.
[62] E. Robertson, L. Esguerra, L. Meßner, G. Gallego, and J. Wolters, “Machine-learning optimal control pulses in an optical quantum memory experiment,” Phys. Rev. Appl., vol. 22, p. 024026, 2024.
[63] A. Kasapi, M. Jain, G. Y. Yin, and S. E. Harris, “Electromagnetically induced transparency: Propagation dynamics,” Phys. Rev. Lett., vol. 74, pp. 2447–2450, 1995.
[64] M. Fleischhauer, A. Imamoğlu, and J. P. Marangos, “Electromagnetically induced transparency: Optics in coherent media,” Rev. Mod. Phys., vol. 77, pp. 633–673, 2005.
[65] D. F. Phillips, A. Fleischhauer, A. Mair, R. L. Walsworth, and M. D. Lukin, “Storage of light in atomic vapor,” Phys. Rev. Lett., vol. 86, pp. 783–786, 2001.
[66] D. F. Phillips, A. Fleischhauer, A. Mair, R. L. Walsworth, and M. D. Lukin, “Observation of coherent optical information storage in an atomic medium using halted light pulses,” Nature, vol. 409, pp. 490–493, 2001.
[67] M. Fleischhauer and M. D. Lukin, “Quantum memory for photons: Dark-state polaritons,” Phys. Rev. A, vol. 65, p. 022314, 2002.
[68] L. Ma, O. Slattery, and X. Tang, “Optical quantum memory based on electromagnetically induced transparency,” J. Opt., vol. 19, p. 043001, 2017.
[69] C.-Y. Cheng, Z.-Y. Liu, P.-S. Hu, T.-N. Wang, C.-Y. Chien, J.-K. Lin, J.-Y. Juo, J.-S. Shiu, I. A. Yu, Y.-C. Chen, and Y.-F. Chen, “Efficient frequency conversion based on resonant four-wave mixing,” Opt. Lett., vol. 46, pp. 681–684, 2021.
[70] C.-Y. Cheng, J.-J. Lee, Z.-Y. Liu, J.-S. Shiu, and Y.-F. Chen, “Quantum frequency conversion based on resonant four-wave mixing,” Phys. Rev. A, vol. 103, p. 023711, 2021.
[71] P. Kolchin, “Electromagnetically-induced-transparency-based paired photon generation,” Phys. Rev. A, vol. 75, p. 033814, 2007.
[72] J.-M. Chen, C.-Y. Hsu, W.-K. Huang, S.-S. Hsiao, F.-C. Huang, Y.-H. Chen, C.-S. Chuu, Y.-C. Chen, Y.-F. Chen, and I. A. Yu, “Room-temperature biphoton source with a spectral brightness near the ultimate limit,” Phys. Rev. Res., vol. 4, p. 023132, 2022.
[73] D.-S. Ding, Z.-Y. Zhou, B.-S. Shi, X.-B. Zou, and G.-C. Guo, “Generation of nonclassical correlated photon pairs via a ladder-type atomic configuration: theory and experiment,” Opt. Express, vol. 20, pp. 11433–11444, 2012.
[74] J. Park, T. Jeong, and H. S. Moon, “Temporal intensity correlation of bunched light from a warm atomic vapor with a ladder-type two-photon transition,” Sci. Rep., vol. 8, p. 10981, 2018.
[75] C. Foot, Atomic physics. Oxford University Press, USA, 2005.
[76] P.-H. Tseng, L.-C. Chen, J.-S. Shiu, and Y.-F. Chen, “Quantum interface for telecom frequency conversion based on diamond-type atomic ensembles,” Phys. Rev. A, vol. 109, p. 043716, 2024.
[77] J. E. Sansonetti, “Wavelengths, transition probabilities, and energy levels for the spectra of rubidium (rb i through rb xxxvii),” Journal of Physical and Chemical Reference Data, vol. 35, pp. 301–421, 2006.
[78] D. Steck, “Rubidium 87 d line data,” 2003.
[79] O. S. Heavens, “Radiative transition probabilities of the lower excited states of the alkali metals,” J. Opt. Soc. Am., vol. 51, pp. 1058–1061, 1961.
[80] W. Ketterle, K. B. Davis, M. A. Joffe, A. Martin, and D. E. Pritchard, “High densities of cold atoms in a dark spontaneous-force optical trap,” Phys. Rev. Lett., vol. 70, pp. 2253–2256, 1993.
[81] R. Boucher, M. Breton, N. Cyr, and M. Tetu, “Dither-free absolute frequency locking of a 1.3 µm dfb laser on 87rb,” IEEE Photonics Technology Letters, vol. 4, pp.327–329, 1992.
[82] H. Sasada, “Wavenumber measurements of sub-doppler spectral lines of rb at 1.3 µm and 1.5 µm,” IEEE Photonics Technology Letters, vol. 4, pp. 1307–1309, 1992.
[83] M. Breton, N. Cyr, P. Tremblay, M. Tetu, and R. Boucher, “Frequency locking of a 1324 nm dfb laser to an optically pumped rubidium vapor,” IEEE Transactions on Instrumentation and Measurement, vol. 42, pp. 162–166, 1993.
[84] H. S. Moon, W. K. Lee, L. Lee, and J. B. Kim, “Double resonance optical pumping spectrum and its application for frequency stabilization of a laser diode,” Appl. Phys. Lett., vol. 85, pp. 3965–3967, 2004.
[85] H. S. Moon, L. Lee, and J. B. Kim, “Double-resonance optical pumping of rb atoms,” J. Opt. Soc. Am. B, vol. 24, pp. 2157–2164, 2007.
[86] H. S. Moon, “Frequency stabilization of a 1.3 μm laser diode using double resonance optical pumping in the 5p3/2–6s1/2 transition of rb atoms,” Appl. Opt., vol. 47, pp. 1097–1102, 2008.
[87] B. Yang, J. Gao, T. Zhang, and J. Wang, “Electromagnetically induced transparency without a doppler background in a multilevel ladder-type cesium atomic system,” Phys. Rev. A, vol. 83, p. 013818, 2011.
[88] M. S. Ali, A. Ray, and A. Chakrabarti, “Tunable offset locking in a Ξ system: an experimental study on the rubidium atom,” Phys. Scr., vol. 88, p. 065301, 2013.
[89] K. Hecht, Quantum mechanics. Springer, 2000.
[90] J.-T. Xiao, High-efficiency backward resonant four-wave mixing by quantum interference, vol. Thesis. National Cheng Kung University, 2017.
[91] S. Blanes, F. Casas, J. Oteo, and J. Ros, “The magnus expansion and some of its applications,” Physics Reports, vol. 470, pp. 151–238, 2009.
[92] K. Huang, Introduction to Statistical Physics, 2nd. Chapman and Hall/CRC, 9 2009.
[93] J. Garrison and R. Chiao, Quantum optics. Oxford University Press, 2016.
[94] M. O. Scully and M. S. Zubairy, Quantum optics. Cambridge: Cambridge University Press, 1997.
[95] C. C. Gerry and P. Knight, Introductory quantum optics. New York: Cambridge University Press, 2005.
[96] M. Körber, O. Morin, S. Langenfeld, A. Neuzner, S. Ritter, and G. Rempe, “Decoherence-protected memory for a single-photon qubit,” Nat. Photonics, vol. 12, pp. 18–21, 2018.
[97] Y. Wang, J. Li, S. Zhang, K. Su, Y. Zhou, K. Liao, S. Du, H. Yan, and S.-L. Zhu, “Efficient quantum memory for single-photon polarization qubits,” Nat. Photonics, vol. 13, p. 346–351, 2019.
[98] Y.-C. Tseng, Y.-C. Wei, and Y.-C. Chen, “Efficient quantum memory for photonic polarization qubits generated by cavity-enhanced spontaneous parametric down conversion,” Opt. Express, vol. 30, pp. 19944–19960, 2022.
[99] S. Ramelow, A. Fedrizzi, A. Poppe, N. K. Langford, and A. Zeilinger, “Polarization entanglement-conserving frequency conversion of photons,” Phys. Rev. A, vol. 85, p. 013845, 2012.
[100] M. Bock, P. Eich, S. Kucera, M. Kreis, A. Lenhard, C. Becher, and J. Eschner, “High fidelity entanglement between a trapped ion and a telecom photon via quantum frequency conversion,” Nat. Commun., vol. 9, p. 1998, 2018.
[101] J. Hannegan, J. D. Siverns, and Q. Quraishi, “Entanglement between a trapped-ion qubit and a 780-nm photon via quantum frequency conversion,” Phys. Rev. A, vol. 106, p. 042441, 2022.
[102] A. G. White, A. Gilchrist, G. J. Pryde, J. L. O’Brien, M. J. Bremner, and N. K. Lang ford, “Measuring two-qubit gates,” J. Opt. Soc. Am. B, vol. 24, pp. 172–183, 2007.
[103] R. Bialczak, M. Ansmann, M. Hofheinz, E. Lucero, M. Neeley, D. Sank, W. Haohua, J. Wenner, M. Steffen, A. Cleland, and J. Martinis, “Quantum process tomography of a universal entangling gate implemented with josephson phase qubits,” Nature Phys., vol. 6, pp. 409–413, 2010.
[104] X. L. Zhang, A. T. Gill, L. Isenhower, T. G. Walker, and M. Saffman, “Fidelity of a rydberg-blockade quantum gate from simulated quantum process tomography,” Phys. Rev. A, vol. 85, p. 042310, 2012.
[105] M. Mičuda, M. Sedlák, I. Straka, M. Miková, M. Dušek, M. Ježek, and J. Fiurášek, “Efficient experimental estimation of fidelity of linear optical quantum toffoli gate,” Phys. Rev. Lett., vol. 111, p. 160407, 2013.
[106] E. Vashukevich, T. Golubeva, and Y. Golubev, “High-fidelity quantum gates for oam qudits on quantum memory,” Laser Phys. Lett., vol. 19, p. 025202, 2022.
[107] M. Cramer, M. B. Plenio, S. T. Flammia, R. Somma, D. Gross, S. D. Bartlett, O. Landon-Cardinal, D. Poulin, and Y.-K. Liu, “Efficient quantum state tomography,” Nat. Commun., vol. 1, p. 149, 2010.
[108] E. Toninelli, B. Ndagano, A. Vallés, B. Sephton, I. Nape, A. Ambrosio, F. Capasso, M. J. Padgett, and A. Forbes, “Concepts in quantum state tomography and classical implementation with intense light: a tutorial,” Adv. Opt. Photon., vol. 11, pp. 67–134, 2019.
[109] M. A. Nielsen and I. L. Chuang, Quantum Computation and Quantum Information. Cambridge University Press, 2010.
[110] M. Rambach, A. Nikolova, T. J. Weinhold, and A. G. White, “Sub-megahertz linewidth single photon source,” APL Photonics, vol. 1, p. 096101, 2016.
[111] J. Liu, J. Liu, P. Yu, and G. Zhang, “Sub-megahertz narrow-band photon pairs at 606 nm for solid-state quantum memories,” APL Photonics, vol. 5, p. 066105, 2020.
[112] R. Pollmann, F. Roeder, V. Quiring, R. Ricken, C. Eigner, B. Brecht, and C. Silberhorn, “Integrated, bright broadband, two-colour parametric down-conversion source,” Opt. Express, vol. 32, no. 14, pp. 23945–23955, 2024.
[113] V. Balić, D. A. Braje, P. Kolchin, G. Y. Yin, and S. E. Harris, “Generation of paired photons with controllable waveforms,” Phys. Rev. Lett., vol. 94, p. 183601, 2005.
[114] S. Du, P. Kolchin, C. Belthangady, G. Y. Yin, and S. E. Harris, “Subnatural linewidth biphotons with controllable temporal length,” Phys. Rev. Lett., vol. 100, p. 183603, 2008.
[115] Z. Han, P. Qian, L. Zhou, J. F. Chen, and W. Zhang, “Coherence time limit of the biphotons generated in a dense cold atomcloud,” Sci. Rep., vol. 5, p. 9126, 2015.
[116] J.-S. Shiu, C.-W. Lin, Y.-C. Huang, M.-J. Lin, I.-C. Huang, T.-H. Wu, P.-C. Kuan, and Y.-F. Chen, “Frequency-tunable biphoton generation via spontaneous four-wave mixing,” Phys. Rev. A, vol. 110, p. 063723, 2024.
[117] J.-K. Lin, T.-H. Chien, C.-T. Wu, R. Chinnarasu, S. Du, I. A. Yu, and C.-S. Chuu, “Observation of subnatural-linewidth biphotons in a two-level atomic ensemble,” Phys. Rev. Lett., vol. 134, p. 043602, 2025.
[118] J.-M. Chen, T. Peters, P.-H. Hsieh, and I. A. Yu, “Review of biphoton sources based on the double-λ spontaneous four-wave mixing process,” Adv. Quantum Technol., vol. 7, p. 2400138, 2024.
[119] J.-S. Shiu, Z.-Y. Liu, C.-Y. Cheng, Y.-C. Huang, I. A. Yu, Y.-C. Chen, C.-S. Chuu, C.-M. Li, S.-Y. Wang, and Y.-F. Chen, “Observation of highly correlated ultrabright biphotons through increased atomic ensemble density in spontaneous four-wave mixing,” Phys. Rev. Res., vol. 6, p. L032001, 2024.
[120] J.-S. Shiu, C.-W. Lin, and Y.-F. Chen, “Asymmetric biphoton generation under ground-state decoherence and phase mismatch in a cold atomic ensemble,” Adv. Quantum Technol., vol. 8, p. e2500052, 2025.
[121] J.-S. Shiu, Tailored Photon Pair Generation in Atomic Ensembles: A Versatile Plat form for Quantum Information Applications, vol. Dissertation. National Cheng Kung University, 2025.
[122] R. Corless, G. Gonnet, D. Hare, D. Jeffrey, and D. Knuth, “On the lambert w function,” Adv. Comput. Math., vol. 5, pp. 329–359, 1996.