Superradiance of ultracold cesium Rydberg |65D 5/2 〉 → |66P 3/2

We investigate Rydberg |65D 5/2 〉 → |66P 3/2 〉 superradiance in dense ultracold cesium atoms, where the ground atoms are excited to |65D 5/2 〉 Rydberg states via two-photon excitation in a standard magneto-optical trap. The superradiant spectrum of |65D 5/2 〉 → |66P 3/2 〉 is obtained using the state...

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Veröffentlicht in:Chinese physics B 2024-04, Vol.33 (5), p.54204
Hauptverfasser: Hao 郝, Liping 丽萍, Han 韩, Xiaoxuan 小萱, Bai 白, Suying 素英, You 游, Xiufen 秀芬, Jiao 焦, Yuechun 月春, Zhao 赵, Jianming 建明
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container_issue 5
container_start_page 54204
container_title Chinese physics B
container_volume 33
creator Hao 郝, Liping 丽萍
Han 韩, Xiaoxuan 小萱
Bai 白, Suying 素英
You 游, Xiufen 秀芬
Jiao 焦, Yuechun 月春
Zhao 赵, Jianming 建明
description We investigate Rydberg |65D 5/2 〉 → |66P 3/2 〉 superradiance in dense ultracold cesium atoms, where the ground atoms are excited to |65D 5/2 〉 Rydberg states via two-photon excitation in a standard magneto-optical trap. The superradiant spectrum of |65D 5/2 〉 → |66P 3/2 〉 is obtained using the state-selective field ionization technique. We observe its dynamic evolution process by varying the delay time of ionization field t d . The results show that the evolution process of |65D 5/2 〉 → |66P 3/2 〉 is much shorter than its radiation lifetime at room temperature, which verifies the superradiance effect. The dependence of the superradiance process on Rydberg atoms number N e and principal quantum number n is investigated. The results show that the superradiance becomes faster with increasing N e , while it is suppressed for stronger van der Waals (vdW) interactions. Superradiance has potential applications in quantum technologies, and the Rydberg atom is an ideal medium for superradiance. Our system is effective for studying the strong two-body interaction between Rydberg atoms.
doi_str_mv 10.1088/1674-1056/ad20da
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The superradiant spectrum of |65D 5/2 〉 → |66P 3/2 〉 is obtained using the state-selective field ionization technique. We observe its dynamic evolution process by varying the delay time of ionization field t d . The results show that the evolution process of |65D 5/2 〉 → |66P 3/2 〉 is much shorter than its radiation lifetime at room temperature, which verifies the superradiance effect. The dependence of the superradiance process on Rydberg atoms number N e and principal quantum number n is investigated. The results show that the superradiance becomes faster with increasing N e , while it is suppressed for stronger van der Waals (vdW) interactions. Superradiance has potential applications in quantum technologies, and the Rydberg atom is an ideal medium for superradiance. 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The superradiant spectrum of |65D 5/2 〉 → |66P 3/2 〉 is obtained using the state-selective field ionization technique. We observe its dynamic evolution process by varying the delay time of ionization field t d . The results show that the evolution process of |65D 5/2 〉 → |66P 3/2 〉 is much shorter than its radiation lifetime at room temperature, which verifies the superradiance effect. The dependence of the superradiance process on Rydberg atoms number N e and principal quantum number n is investigated. The results show that the superradiance becomes faster with increasing N e , while it is suppressed for stronger van der Waals (vdW) interactions. Superradiance has potential applications in quantum technologies, and the Rydberg atom is an ideal medium for superradiance. 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The superradiant spectrum of |65D 5/2 〉 → |66P 3/2 〉 is obtained using the state-selective field ionization technique. We observe its dynamic evolution process by varying the delay time of ionization field t d . The results show that the evolution process of |65D 5/2 〉 → |66P 3/2 〉 is much shorter than its radiation lifetime at room temperature, which verifies the superradiance effect. The dependence of the superradiance process on Rydberg atoms number N e and principal quantum number n is investigated. The results show that the superradiance becomes faster with increasing N e , while it is suppressed for stronger van der Waals (vdW) interactions. Superradiance has potential applications in quantum technologies, and the Rydberg atom is an ideal medium for superradiance. Our system is effective for studying the strong two-body interaction between Rydberg atoms.</abstract><doi>10.1088/1674-1056/ad20da</doi></addata></record>
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