Development of an XUV Frequency Comb for Precision Spectroscopy of Highly Charged Ions

J. Oelmann, J. Nauta, A. Ackermann, P. Knauer, R. Pappenberger, S. Kühn, J. Stark, José R. Crespo López-Urrutia, T. Pfeifer
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Abstract

Highly charged ions (HCI) have a few tightly bound electrons and many interesting properties for probing fundamental physics and developing new frequency standards [1,2]. Many optical transitions of HCI are located in the extreme ultraviolet (XUV) and conventional light sources do not allow to study these transistions with highest precision. For this reason, we are developing an XUV frequency comb by transfering the coherence and stability of a near infrared frequency comb to the XUV by means of high-harmonic generation (HHG) [3–4]. Reaching intensity levels necessary for HHG 1013W/cm2), while operating at high repetition rates (100 MHz) for large comb line spacing, is challenging. Therefore, the laser pulses are first amplified in a rod-type fiber to 70 W and compressed to sub-200 fs in a grating and prism compressor. Afterwards, pulses are resonantly overlapped in an astigmatism-compensated femtosecond enhancement cavity, which is locked to the frequency comb. To achieve high stability and low-noise performance, the cavity is built on a rigid titanium structure with vibrational decoupling from the vacuum pumps. High-harmonics will then be generated in a target gas in the tight focus of the cavity and coupled out of the cavity by minus-first order diffraction from a small-period grating etched into a high-reflective cavity mirror [5]. Mirror degradation due to contamination and hydrocarbon aggregation is prevented by operating the whole cavity under ultra-high vacuum conditions. A differential pumping scheme will enable high target gas pressures in the laser focus without impairing the pressure elsewhere in the chamber [6].
用于高电荷离子精密光谱分析的XUV频率梳的研制
高电荷离子(HCI)具有一些紧密结合的电子和许多有趣的特性,可用于探索基础物理和开发新的频率标准[1,2]。HCI的许多光学跃迁位于极紫外(XUV),传统光源不允许以最高的精度研究这些跃迁。因此,我们正在开发一种XUV频率梳,通过高谐波产生(HHG)将近红外频率梳的相干性和稳定性转移到XUV[3-4]。达到HHG所需的强度水平(1013W/cm2),同时在高重复频率(100 MHz)下运行,以实现大梳线间距,这是一项挑战。因此,激光脉冲首先在棒型光纤中被放大到70w,然后在光栅和棱镜压缩机中被压缩到200fs以下。然后,脉冲在一个像散补偿飞秒增强腔中共振重叠,该腔锁定在频率梳上。为了实现高稳定性和低噪声性能,腔体建立在刚性钛结构上,与真空泵的振动解耦。高次谐波将在腔体紧密聚焦的目标气体中产生,并通过蚀刻在高反射腔镜上的小周期光栅的负一阶衍射耦合出腔体[5]。通过在超高真空条件下操作整个腔体,可以防止因污染和碳氢化合物聚集而导致的镜像降解。差动泵浦方案将使激光聚焦中的目标气体压力高,而不损害腔室其他地方的压力[6]。
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