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Applied Optics

Fabrication of an Rb–Xe gas cell with optical components attached by optical contact bonding for an atom spin gyroscope

Sang Hyuk Hong, Sin Hyuk Yim, Taek Jeong, Jeong Bin Nam, Sangkyung Lee

Published Apr 18, 2025• 3 citations
Publisher

Abstract

We describe the fabrication of a cubic Rb–Xe gas cell integrated with optical components. Two prism mirrors and a reflection mirror are attached to the Rb–Xe gas cell by optical contact bonding. This concept was studied by using free induction decay measurements of Xe gas with two diode lasers at 795 nm in a magnetic shield. The transverse spin relaxation times of 129 Xe and 131 Xe are 7.0 s and 7.2 s, respectively, with sufficient signal amplitude. Optical contact bonding is shown to be promising to provide the monolithic atomic gas cell with optical components and the compact design of an atom spin gyroscope.

DOI
10.1364/ao.554573

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We describe the fabrication of a cubic Rb–Xe gas cell integrated with optical components. Two prism mirrors and a reflection mirror are attached to the Rb–Xe gas cell by optical contact bonding. This concept was studied by using free induction decay measurements of Xe gas with two diode lasers at 795 nm in a magnetic shield. The transverse spin relaxation times of 129 Xe and 131 Xe are 7.0 s and 7.2 s, respectively, with sufficient signal amplitude. Optical contact bonding is shown to be promising to provide the monolithic atomic gas cell with optical components and the compact design of an atom spin gyroscope.
An experimental setup to fabricate atomic vapor cells for atom spin gyroscope application, containing 87Rb, 129Xe, 131Xe, N2, and H2, is described. The setup comprises a high-vacuum chamber, an 87Rb ampule, a glass cell, gas lines, and a turbopump. First, the glass cell is baked for a week at 450 °C to reduce outgassing from the inner walls of the glass cell. Next, rubidium atoms are evaporated into the cubic glass cell. Then, the cubic glass cell is cooled to 2 °C to increase the amount of 87Rb in the cubic glass cell while the vacuum chamber is heated to 100 °C. 6 Torr of 129Xe, 48 Torr of 131Xe, 140 Torr of N2, and 24 Torr of H2 are injected into the cubic glass cell. The sealing method employs pinch-off glass welding. The transverse spin relaxation times of 129Xe and 131Xe at a magnetic field of 6.2 µT applied to the quantization axis are measured to be 8.1 and 16.5 s, respectively, at a cell temperature of 96 °C using nuclear magnetic resonance spectroscopy. The pressure ratio between 129Xe and 131Xe is determined by comparing the output signals from our atom spin gyroscope. The signal-to-noise ratios are 2500 for 129Xe and 3333 for 131Xe, respectively, and the expected angular random walk of the atom spin gyroscope is 0.062°/h1/2 with a 1-Hz repetition rate.
The combination of MEMS technology with atomic spin devices could fabricate chip scale atomic sensors. In most of the atomic devices based on alkali metals, the key component is an alkali vapor cell. Here we describe an alkali vapor cell fabrication technic for atomic spin gyroscope study. In the alkali vapor cell, alkali metal is filled in an oxygen and water free glovebox and noble gas isotopes such as129Xe and131Xe are also filled. Compared to an atomic magnetometer, in an atomic spin gyroscope, the isotope enriched noble gases are typically very expensive. We need to do recycling of these expensive gases after filling in the anode bonding chamber or else the gases will be wasted. Due to the large volume of the anode bonding chamber utilized in the fabrication process, a recycling platform is built based on liquid nitrogen. The relaxation time is a very important parameter of an alkali vapor cell. We developed a platform with magnetic field shielding system, non-magnetic field heating and single beam atomic spin detection subsystem. The spin relaxation time of the noble gases is tested in this study.
We report on the fabrication and characterization of MEMS atomic vapor cells suitable for applications in miniaturized quantum sensors such as atomic gyroscopes. Our MEMS cells are filled with natural abundance Rb alkali atoms and enriched noble Xe atoms and are operated in the regime of spin exchange optical pumping. The transverse relaxation time T2* of the nuclear spin in 129Xe atoms directly defines the angular random walk parameter of an atomic gyroscope. Using a field switch technique, we measure the dephasing time T2* of the 129Xe isotope as a function of temperature. Our results showing a decrease of T2* from about 1 to 0.4 seconds with an increasing temperature in the range from 80 to 150 °C are in good agreement with a simple theoretical model taking into account the most important decoherence mechanisms. We show that the observed decoherence behavior can be mostly explained trough collisions of the Xe atoms with the walls. Further characterization steps in order to gain more insight in the decoherence physics involved in our MEMS cells are discussed.
We describe a 3 He- 129 Xe comagnetometer using 87 Rb atoms for noble-gas spin polarization and detection.We use a train of 87 Rb π pulses and σ þ =σ -optical pumping to realize a finite-field Rb magnetometer with suppression of spin-exchange relaxation.We suppress frequency shifts from polarized Rb by measuring the 3 He and 129 Xe spin precession frequencies in the dark, while applying π pulses along two directions to depolarize Rb atoms.The plane of the π pulses is rotated to suppress the Bloch-Siegert shifts for the nuclear spins.We measure the ratio of 3 He to 129 Xe spin precession frequencies with sufficient absolute accuracy to resolve Earth's rotation without changing the orientation of the comagnetometer.A frequency resolution of 7 nHz is achieved after integration for 8 h without evidence of significant drift.
The spin polarization of 87Rb and 129Xe atomic ensemble has great impact on the signal intensity of a nuclear magnetic resonance gyroscope. The coupled spin polarization modelling process for 87Rb and 129Xe atoms ensemble is presented in detail. Three dimensional spatial distribution of the spin polarization field is obtained by numerical solution and is in good agreement with the experiment results. Influencing factors including temperature, power and detuned frequency of the pumping laser, average collision times of anti-relaxation coatings and partial pressure of gas composition are investigated. The work presents an indirect method to estimate the average collision times given the Xe polarization with different temperatures. It is found the average collision times of the 129Xe atoms with the inner surface of a bare glass cell of 3×3×3mm3 can reach up to about 2.7×105 times. It is also found that the pumping frequency corresponding to the maximum polarization of the Xe atoms polarized by spin exchange of Rb atoms is not consistent with the D1 line of the 87Rb atom when the temperature of the cell is above a certain temperature, but is detuned at a certain frequency. Quantitative analysis of the effect of anti-relaxation coatings on the spin polarization suggests that the appropriate average number of collisions of the Rb atoms with the inner surface of the cell is about 1500 times.