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Towards a strontium optical lattice clockBridge, Elizabeth Michelle January 2012 (has links)
Due to the recent success, in terms of accuracy and precision, of a number of strontium optical lattice optical frequency standards, and the classification of the 5s<sup>2</sup> <sup>1</sup>S<sub>0</sub> to 5s5p <sup>3</sup>P<sub>0</sub> transition in neutral strontium as a secondary definition of the SI unit of the second, many new strontium lattice clocks are under development. The strontium optical lattice clock (Sr OLC) at the National Physical Laboratory (NPL) is one such project. This thesis describes the design and build of the NPL Sr OLC, discussing the considerations behind the design. Details of the first cooling stage are given, which includes the characterisation of a novel permanent-magnet Zeeman slower by measurements of the longitudinal velocity distributions and loading of the MOT at 461 nm. Development of a narrow linewidth laser system at 689 nm is described, which is used for initial spectroscopy of the second-stage cooling transition. In particular, this work describes progress towards two independent ultra-narrow linewidth clock lasers. The new generation of strontium lattice clock experiments have focused on characterising the systematic frequency shifts and reducing their associated fractional frequency uncertainties, as well as reducing the fractional frequency instability of the measurement. One focus of the Sr OLC at NPL is to help characterise the frequency shift of the clock transition due to black-body radiation (BBR), which is currently the largest contributor to the uncertainty budget of the measured clock frequency. Our approach, discussed here, is to make a direct, differential measurement of the shift with the atoms housed alternately in environments of differing temperatures. Better characterisation and control of the BBR frequency shift of the strontium clock transition is crucial for the future of the Sr OLC as a leading frequency standard.
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Desenvolvimento de um laser de Nd:YLF bombeado por diodo laser e duplicado em freqüência para 657 nm / Development of a diode pumped Nd:YLF laser, frency doubled to 657 nmNuñez Portela, Mayerlin 14 August 2018 (has links)
Orientador: Flavio Caldas da Cruz / Dissertação (mestrado) - Universidade Estadual de Campinas, Instituto de Fisica Gleb Wataghin / Made available in DSpace on 2018-08-14T07:51:57Z (GMT). No. of bitstreams: 1
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Previous issue date: 2009 / Resumo: Os relógios atômicos são usados na atualidade em um grande número de aplicações científicas e tecnológicas que vão desde experimentos de relatividade e determinação de constantes fundamentais, até sistema de navegação (GPS) e telecomunicações. A proxima geração de relógios atômicos de alta precisão estará baseada em transições ópticas de átomos frios. Neste trabalho foi desenvolvido um laser de estado sólido de Nd:YLF bombeado por um laser de diodo e duplicado em frequência em 657 nm. Este sistema é proposto como oscilador local em um relógio atômico óptico baseado em átomos de cálcio. Comparado com os lasers de diodo, este apresenta uma potência maior no vermelho, um ruído de frequência e amplitude menores e a possibilidade de transferência remota usando obras ópticas no comprimento de onda fundamental de 1314 nm. Duplicação em frequência intra-cavidade é feita usando um cristal de BiBO, com superfícies anti-refletoras, e com um casamento de fase crítico tipo I à temperatura ambiente. Uma potência de 270 mW na saída do vermelho foi obtida para uma potência de bombeamento de 11.6 W. / Abstract: Atomic clocks are used today in a number of scientific and technological applications, ranging from tests of relativity, or variations of fundamental constants, to the use in navigation and telecommunication. The next generation of such high precision devices will be based on optical transitions of suitable laser cooled and trapped atoms. In this work we describe a frequency-doubled, diode-pumped solid-state Nd:YLF ring laser emitting at 657 nm, proposed as a local oscillator in an optical atomic clock based on laser cooled and trapped calcium atoms. Compared to diode lasers, its main advantages include higher power, less intrinsic frequency noise, and the possibility of remote transfer in optical fibers using the fundamental light at 1314 nm. Frequency doubling is performed inside the cavity using a 10 mm long AR-coated BiBO crystal, under type I, critical phase-matching at room temperature. Red output power of 270 mW was achieved for 11.6 W of pumping power. / Mestrado / Física Atômica e Molecular / Mestre em Física
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Frequency Comb Experiments and Radio Frequency Instrumentation Analysis for Optical Atomic ClocksRyan J Schneider (14187461) 29 November 2022 (has links)
<p>Space-based global navigation and precision timing systems are critical for modern infrastructure. Atomic clock technology has increased the precision of these systems so that they are viable for military operations, navigation, telecommunications, and finance. Advances in optical atomic clocks, based on optical frequencies, provide an opportunity for even more precise timing. Therefore, developments in chip-scale optical atomic clock technologies could lead to increased and more wide-spread application of this precision timing. One component of the optical atomic clock is the optical frequency comb which serves as an interface between optical and microwave frequencies. This thesis will cover experiments related to these optical frequency combs. A 2$\mu$m fiber laser was developed in order to test second harmonic devices required to stabilize an optical frequency comb. The laser was then employed to measure the operating wavelengths and efficiencies of non-linear devices. In addition, an analysis of the radio frequency instruments used to evaluate microwave outputs was conducted to determine whether a digital signal analyzer (oscilloscope) or an analog electronic spectrum analyzer provides more accurate results for optical frequency comb based experiments.</p>
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Microcombs for Timekeeping and RF PhotonicsNathan Patrick O'Malley (17053956) 27 September 2023 (has links)
<p dir="ltr">Optical frequency combs have revolutionized metrology and advanced other fields such as RF photonics and astronomy. While powerful, they can be bulky, expensive, and difficult to manufacture. This tends to limit uses in real-world scenarios. Within the last decade or so, coherent frequency combs have begun to be generated in millimeter-scale, CMOS fabrication-compatible nonlinear crystals. These so-called “microcombs” have led to hopes of overcoming deployability constraints of more traditional bulk combs.</p><p dir="ltr">One of the first applications for \textit{bulk} frequency combs after their explosion in 2000 was the optical atomic clock. It promised extreme long-term time stability better than that of the Cesium clock that currently defines the SI second. More recently, interest in a fully portable optical atomic clock has grown. Such a device could reliably keep time even without the aid of GPS references, and potentially with greater accuracy than current GPS synchronization can provide.</p><p dir="ltr">Frequency combs have also been used to sample electrical signals more rapidly than traditional electronics can accomplish. This has been used to achieve dramatically increased effective frequency bandwidths for signal detection architectures. One can imagine how this capability would be beneficial in a portable (microcomb-driven) form: a lightweight, comb-enhanced receiver able to capture a broadband snapshot of its surrounding electromagnetic environment could be a powerful tool.</p><p dir="ltr">Timekeeping and RF photonics are the primary applications of microcombs focused upon here. I will attempt to roughly summarize important concepts and highlight relevant work in both subjects in the Introduction. Then I will move a step closer to the hands-on lab work that has largely kept me preoccupied over the last several years and describe important or commonly-employed Methods for experiments. A collection of three journal manuscripts (two published, and the third recently submitted) will follow in the Publications chapter, highlighting some experimental results. Finally, I will conclude with a brief Outlook.</p>
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