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处于P态和S态的超冷锶在390纳米处的光电离截面以及由此产生的蓝失谐魔术波长光晶格钟约束。

Photoionization cross sections of ultracold Sr in P and S states at 390 nm and the resulting blue-detuned magic wavelength optical lattice clock constraints.

作者信息

Witkowski Marcin, Bilicki Sławomir, Bober Marcin, Kovačić Domagoj, Singh Vijay, Tonoyan Ara, Zawada Michał

出版信息

Opt Express. 2022 Jun 6;30(12):21423-21438. doi: 10.1364/OE.460554.

DOI:10.1364/OE.460554
PMID:36224862
Abstract

We present the measurements of the photoionization cross sections of the excited P and S states of ultracold Sr atoms at 389.889 nm wavelength, which is the magic wavelength of the S-P clock transition. The photoionization cross section of the P state is determined from the measured ionization rates of Sr in the magneto-optical trap in the P state to be 2.20(50)×10 m, while the photoionization cross section of Sr in the S state is inferred from the photoionization-induced reduction in the number of atoms transferred through the S state in an operating optical lattice clock to be 1.38(66) ×10 m. Furthermore, the resulting limitations of employing a blue-detuned magic wavelength optical lattice in strontium optical lattice clocks are evaluated. We estimated photoionization induced loss rates of atoms at 389.889 nm wavelength under typical experimental conditions and made several suggestions on how to mitigate these losses. In particular, the large photoionization induced losses for the S state would make the use of the S state in the optical cycle in a blue-detuned optical lattice unfeasible and would instead require the less commonly used D states during the detection part of the optical clock cycle.

摘要

我们给出了在389.889 nm波长下超冷锶原子激发态P和S的光电离截面测量结果,该波长是S-P钟跃迁的魔术波长。P态的光电离截面由测量处于P态的磁光阱中锶的电离率确定为2.20(50)×10⁻¹⁸ m²,而S态锶的光电离截面是根据在运行的光晶格钟中通过S态传输的原子数因光电离而减少推断得出,为1.38(66)×10⁻¹⁸ m²。此外,评估了在锶光晶格钟中使用蓝失谐魔术波长光晶格所产生的限制。我们估计了在典型实验条件下389.889 nm波长处原子的光电离诱导损失率,并就如何减轻这些损失提出了一些建议。特别是,S态较大的光电离诱导损失将使得在蓝失谐光晶格的光学循环中使用S态不可行,而是在光钟循环的检测部分需要使用较少使用的D态。

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