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Conference on Lasers and Electro-Optics

Demonstration of sub-micron hot vapor cells for quantum technology applications

Eliran Talker, Roy Zektzer, Yefim Barash, Noa Mazurski, Uriel Levy

Published Jan 1, 2020• 0 citations
Publisher

Abstract

We report on the fabrication of a glass vapor cell with a scalable thickness varying from 50 nm to 30 pm. It is used to demonstrate atomic based laser stabilization at 780 nm wavelength.
DOI
10.1364/cleo_si.2020.sth3g.5

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We report on the atomic spectroscopy and laser frequency stabilization using a new type of a miniaturized glass vapor cell with a scalable thickness varying from 500 nm up to 8 μm. The cell is fabricated by lithography and etching techniques in a Pyrex glass substrate, followed by anodic bonding. It is filled with rubidium vapor using a distillation procedure. This simple and cost-effective fabrication method provides an attractive and compact solution for atomic cells, with applications in quantum metrology, sensing, communication, and light-vapor manipulations at the subwavelength scale. Using the fabricated cell, we have performed fluorescence and transmission spectroscopy of the Rubidium D2 line and observed sub-Doppler broadened lines. As an example, for a potential application, we have used the fabricated cell to demonstrate the stabilization of a 780 nm diode laser to the level about 10−10 in fractional frequency.

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•Sep 30, 2024•0 citations
We report on the atomic spectroscopy and laser frequency stabilization using a new type of a miniaturized glass vapor cell with a scalable thickness varying from 500 nm up to 8 μm. The cell is fabricated by lithography and etching techniques in a Pyrex glass substrate, followed by anodic bonding. It is filled with rubidium vapor using a distillation procedure. This simple and cost-effective fabrication method provides an attractive and compact solution for atomic cells, with applications in quantum metrology, sensing, communication, and light-vapor manipulations at the subwavelength scale. Using the fabricated cell, we have performed fluorescence and transmission spectroscopy of the Rubidium D2 line and observed sub-Doppler broadened lines. As an example, for a potential application, we have used the fabricated cell to demonstrate the stabilization of a 780 nm diode laser to the level about 10−10 in fractional frequency.
Precision spectroscopy is an important tool across a wide array of applications, from communications, timing and navigation, to many emerging quantum technologies. I will talk about our groups work to enable robust operation and integration of spectroscopic techniques for laser stabilization using nanophotonics for light delivery and microfabricated vapor cells for containing atomic references. Our approach is able to span a large wavelength range, from the telecommunications band using on chip second harmonic generation to wavelengths in the blue using vapor cells containing alkaline earth atoms.
Abstract Laser-induced fluorescence (LIF) in the spectral range of 400–1000 nm has been investigated in rubidium vapor excited by narrowband diode laser radiation at 780 nm and 795 nm, resonant with the 5 S 1 / 2 → 5 P 1 / 2 , 3 / 2 transitions. Experiments were performed using three specially fabricated all-sapphire cells with thicknesses of L = 1 cm, 10 μ m, and 500 nm. Multiple fluorescence channels were observed, and it is shown that many LIF signals are suppressed with decreasing cell thickness due to enhanced atom–wall collisions leading to quenching of excited states. Nevertheless, for a nanocell of thickness L = 500 nm at temperatures of ∼ 300 ∘ C, blue fluorescence at 420 nm remains observable, and its intensity is compared with results available in the literature. It is further demonstrated that LIF spectroscopy enables detection and estimation of residual cesium vapor in rubidium cells via energy-transfer processes. In addition, the Rb vapor cell can operate as an efficient optical filter and frequency up-converter, converting radiation at 780 nm or 795 nm into shorter wavelengths, notably 420 nm. These results highlight the potential of broadband LIF spectroscopy in alkali vapors for applications in precision measurements, optical frequency standards, and quantum technologies.
Microfabricated (MEMS) alkali vapor cells are at the core of high-precision integrated atomic quantum sensors and devices [1], such as microwave and optical clocks, or magnetometers. The first chip-scale atomic device was a microwave atomic clock based on coherent population trapping [2]. It has offered in its industrial and commercialized version an ultra-low size-power -instability budget, impacting a plethora of industrial and scientific applications. Nevertheless, the short-term stability of these clocks is usually limited at about 10−10 at 1 s. Hot vapor MEMS-based optical frequency standards constitute a new generation of miniaturized clocks, with enhanced stability. These references keep the benefit of using wafer-scalable and mass-producible vapor cells while preventing ultra-high vacuum technologies and laser cooling. Among the transitions explored, the 6S1/2 → 7P1/2 near-UV transition of Cs atom was used to demonstrate an optical reference with a stability of 2.1 × 10−13 at 1 s and averaging down to a few 10−14 [3]. However, this reference was based on a 5 cm-long glass-blown cell, not compliant with the advent of a fully-miniaturized and low-power optical clock. In this work [4], we present the characterization of sub-Doppler resonances detected in a microfabricated cell by probing, in a simple saturated absorption configuration, the Cs atom 6S1/2 → 7P1/2 transition at 459 nm. The impact of the laser intensity and cell temperature on the sub-Doppler resonance is experimentally investigated. Optimal values are identified for the development of a near-UV microcell-stabilized frequency reference. Detection noise measurements are also reported, predicting a short-term stability in the 10−13 range at 1 s. Tests of cells with embedded getters are under progress for improved purity of the cell inner atmosphere and narrowing of the resonance.