Prospective Optical Lattice Clocks in Neutral Atoms with Hyperfine Structure

Atoms Pub Date : 2024-03-05 DOI:10.3390/atoms12030014
Tobias Bothwell
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Abstract

Optical lattice clocks combine the accuracy and stability required for next-generation frequency standards. At the heart of these clocks are carefully engineered optical lattices tuned to a wavelength where the differential AC Stark shift between ground and excited states vanishes—the so called ‘magic’ wavelength. To date, only alkaline-earth-like atoms utilizing clock transitions with total electronic angular momentum J=0 have successfully realized these magic wavelength optical lattices at the level necessary for state-of-the-art clock operation. In this article, we discuss two additional types of clock transitions utilizing states with J≠0, leveraging hyperfine structure to satisfy the necessary requirements for controlling lattice-induced light shifts. We propose realizing (i) clock transitions between same-parity clock states with total angular momentum F=0 and (ii) M1/E2 clock transitions between a state with F=0 and a second state with J=1/2, mF=0. We present atomic species which fulfill these requirements before giving a detailed discussion of both manganese and copper, demonstrating how these transitions provide the necessary suppression of fine structure-induced vector and tensor lattice light shifts for clock operations. Such realization of alternative optical lattice clocks promises to provide a rich variety of new atomic species for neutral atom clock operation, with applications from many-body physics to searches for new physics.
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具有超精细结构的中性原子中的前瞻性光晶格时钟
光晶格时钟兼具下一代频率标准所需的精度和稳定性。这些时钟的核心是经过精心设计的光晶格,其波长经过调整后,基态和激发态之间的交流斯塔克偏移差消失,即所谓的 "神奇 "波长。迄今为止,只有利用总电子角动量 J=0 的时钟跃迁的碱土类原子成功实现了这些魔幻波长光晶格,达到了最先进时钟运行所需的水平。在本文中,我们将讨论利用 J≠0 状态的另外两类时钟跃迁,利用超精细结构来满足控制晶格诱导的光偏移的必要条件。我们建议实现(i)总角动量 F=0 的同位时钟态之间的时钟转换,以及(ii)F=0 的态与 J=1/2, mF=0 的第二态之间的 M1/E2 时钟转换。 在详细讨论锰和铜之前,我们介绍了满足这些要求的原子种类,展示了这些转换如何为时钟操作提供必要的精细结构诱导的矢量和张量晶格光偏移抑制。这种替代光晶格时钟的实现有望为中性原子钟的运行提供丰富多样的新原子种类,其应用范围从多体物理到新物理搜索。
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