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Advancements in Silicon-Wafer Atomic Cells

New silicon wafer atomic cells show improved performance for quantum sensors.

― 6 min read


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Atom spin sensors are essential in the field of quantum technology. They provide accurate measurements while being compact, making them suitable for various applications. This article discusses a new design of small silicon-wafer cells, which have two chambers and built-in heaters. These cells were tested to see how they perform under different conditions, such as changes in temperature and magnetic fields.

Importance of Miniaturization

In recent years, advances in technology have allowed Atomic Magnetometers (special types of sensors) to move from laboratories to real-world applications. A critical factor for many of these uses, like detecting small magnetic fields or aiding navigation, is the size and weight of the sensors. Reducing size, weight, power, and cost-commonly referred to as SWaP-C-can help lower operational expenses and facilitate mass production.

The Cell Design

The first small atomic vapor cells based on silicon wafers were created for specific timekeeping devices. These cells are constructed using layers of glass sealed to a silicon wafer. Over time, various designs have emerged, leading to performance improvements. For instance, gold spots were added to reduce the condensation of alkali metal atoms on the windows, and coatings with materials like aluminum oxide extended the life of the cells by reducing how quickly atoms moved through the walls.

Engineers have also experimented with using thicker wafers and mirrored surfaces to boost the optical path length, allowing more atoms to be addressed. An essential task in developing these cells is to understand how the atoms behave and how they interact under different conditions.

New Miniature Cells

In this article, we introduce a cost-efficient, compact silicon wafer cell featuring double chambers and integrated heating components. This design allows the storage of Alkali Metals separately from where they interact with laser beams. The temperature differences created in these cells help avoid issues like condensation on the windows, which can affect performance.

Using a special chemical precursor, we streamline the production of these cells without sacrificing performance. Our cells have been thoroughly tested in various conditions using a technique called indirect pumping. While this method is known to work in larger, traditional cells, it had not been demonstrated in these smaller wafer-based designs until now.

Measurement Setup

The structure of the measurement setup is crucial for understanding the performance of these cells. The sensors are placed inside a protective shield to reduce interference from outside magnetic fields. We create a static magnetic field using coils, ensuring it is uniform within the cell.

Various temperatures and atomic densities are maintained during tests as the cell is heated using a simple current-driven system. A circularly polarized laser beam is used for pumping, while a linearly polarized probe beam assesses the state of the atoms. The responses are recorded using a specialized amplifier.

Thermal Properties

To ensure optimal performance, we model the thermal properties of the cells, which helps us create designs that minimize unwanted side effects, like stray magnetic fields. The heating elements are carefully positioned to maintain consistent temperatures across the interaction chamber, ensuring that there is no block in the laser's path.

Dynamics of Polarization

The behavior of the atom spins and their Coherence, which refers to their phase relationship, is affected by different rates of interaction. These include collisions with the walls of the cell, diffusion, optical pumping, and spin-exchange collisions.

When atoms are pumped optically, they can become polarized, but if the rate of pumping is too high, it might disrupt the coherence. Spin-exchange collisions can either keep the atoms synchronized or lead to a decay in their coherence, depending on the situation.

Indirect Pumping Explained

Indirect pumping involves both optical excitation and spin-exchange interactions. In this process, some atoms are directly acted upon by laser light while others receive energy through interactions with their neighbors. This technique has been successfully applied in larger cells but needed to be validated in miniature designs.

As we study the behavior of our new cells, we observe how the light affects the atomic spins. The aim is to maintain a balance between excitation and the resulting decoherence to optimize sensor performance.

Temperature Dependence

As we vary the temperature of the atomic vapor, the interaction between atoms changes. At lower temperatures, wall collisions dominate, while higher temperatures enable the effects of spin-exchange collisions. The temperature significantly influences how well the atoms interact with the light, the linewidth (or clarity) of the resonance obtained, and overall coherence.

As we increase the temperature, we find the linewidth begins to change less dramatically, suggesting a more stable polarization among the atoms. Notably, at a temperature of 110 degrees Celsius, only some atoms interact effectively with the laser, leading to less overall impact on the measurements.

Observing Magnetic Field Effects

The strength of the magnetic field has a significant influence on the sensor's performance. As we adjust the bias field strength, we can observe changes in the linewidth of the signals obtained. The results show a clear relationship between the magnetic field and the coherence transfer process between different atomic states.

As the magnetic field strength decreases, the linewidth reduces, indicating better coherence among the atomic spins. At low pump power, the interaction between the atomic states becomes more evident, which can enhance the overall performance of our sensors.

Conclusion

We have successfully designed and characterized innovative silicon wafer-based cells that push the boundaries of atomic magnetometry. The introduction of features like dual chambers and heating circuits opens new avenues for compact and robust sensors.

Through detailed testing, we have shown how these cells perform under various conditions, shedding light on the dynamics of atomic vapor polarization influenced by indirect pumping and spin-exchange interactions. The findings indicate that while our miniature cells differ substantially from traditional paraffin-coated cells, they exhibit similar behaviors under certain conditions.

Our work lays a strong foundation for future enhancements in both portable sensors and fundamental research in atomic vapor dynamics, which could positively impact quantum imaging and information technologies as they continue to evolve. Furthermore, as manufacturing processes improve, our new designs hold significant promise for creating integrated, compact atomic devices that can find applications across many areas of quantum technology.

Original Source

Title: Indirect pumping of alkali-metal gases in a miniature silicon-wafer cell

Abstract: Atom spin sensors occupy a prominent position in the scenario of quantum technology, as they can combine precise measurements with appealing miniature packages which are crucial for many applications. In this work, we report on the design and realization of miniature silicon-wafer cells, with a double-chamber configuration and integrated heaters. The cells are tested by systematically studying the spin dynamics dependence on the main pump parameters, temperature, and bias magnetic field. The results are benchmarked against cm-sized paraffin-coated cells, which allows for optimisation of operating conditions of a radio-frequency driven atomic magnetometer. In particular, we observe that, when indirect optical pumping is performed on the two cells, an analogous line narrowing mechanism appears in otherwise very different cells' conditions. Competitive results are obtained, with magnetic resonance linewidths of roughly 100 Hz at the maximum signal-to-noise ratio, in a non-zero magnetic field setting, and in an atomic shot-noise limited regime.

Authors: J. D. Zipfel, P. Bevington, L. Wright, W. Chalupczak, G. Quick, B. Steele, J. Nicholson, V. Guarrera

Last Update: 2024-02-26 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2402.16695

Source PDF: https://arxiv.org/pdf/2402.16695

Licence: https://creativecommons.org/licenses/by/4.0/

Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.

Thank you to arxiv for use of its open access interoperability.

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