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CS-TC08 Scheda tecnica(PDF) 1 Page - Wavelength Electronics, Inc. |
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CS-TC08 Scheda tecnica(HTML) 1 Page - Wavelength Electronics, Inc. |
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1 / 5 page ![]() © 2003 • Sales & Technical Support: (406) 587-4910 • email: sales@teamWavelength.com • web: www.teamWavelength.com Case Study CS-TC08 Rev. A VCSEL Absorption Spectroscopy of Chip-scale Rubidium Atomic Vapor August, 2023 Page 1 ABSTRACT Researchers from the Indian Space Research Organization in Bengaluru, India have developed and demonstrated the absorption spectroscopic capabilities of a chip-scale Rubidium (Rb) atomic vapor cell using a thermoelectric cooler integrated VCSEL light source in a magneto-optic package. The custom three-dimensionally printed design provides real time analysis of spectral data by laser interrogation of the D1 hyperfine transition states of the Rb vapor in the chip-scale cell. With over 600 hours of data, absorption resonance lines were recorded and analyzed for transitions 85Rb and 87Rb with absorption amplitude and FWHM data agreeing with known literature values. This magneto-optic Rb atomic cell package proves potential for atomic sensors, particularly in space borne applications or payloads. HOT ATOMIC VAPORS Recent developments of quantum sensors rely on sensing hot atomic vapors in a specific type of vapor cell.1 By optically interrogating the atoms and their states, an absorption spectra can be obtained that can lead to changes or monitoring of the sensor's object of interest. The miniaturization of these quantum sensors also requires increasingly smaller-sized hot vapor cells. Fabrication on a single wafer with hundreds of vapor cells or chip-scale vapor cells enable quantum sensors to be utilized in a wide range of applications. Quantum sensing applications include: atomic clocks, gyroscopes, magnetometers, frequency-stabilized lasers, frequency standards, gas sensors, as well as GHz and THz imaging and detectors.1 There are multiple parameters that are changed and manipulated for different experiments. First, the vapor cell is filled with the appropriate metallic alkali vapor. Common vapors are Rubidium (Rb) or Cesium (Cs). Secondly, some applications require the addition of inert buffer gases and spin polarizable atomic species such as Xenon (Xe).1 Lastly, and most importantly, the configuration of the chip- scale cells determine how the atomic vapors are spectrally observed. Vapor cells can be constructed with planar, spherical, and cubical shapes using MEMS fabrication technology. Typically, the alkali vapor cell is the first priority of the system, as a miniature chip-scale cell and absorption spectroscopy based on that vapor cell can be a tedious task to setup and calibrate. The other component that is crucial for this type of sensor is the light source for optical interrogation of the atoms inside the vapor cell. A laser diode, Light Emitting Diode (LED), or a Vertical Cavity Surface Emitting Laser (VCSEL) are common choices for absorption spectroscopy in a small package. PROBLEMS AND GOALS The packaging containing the light source, vapor cell, heating element, and optics requires precise alignment to allow absorption spectra measurements to become repeatable and accurate. Compactness and error-free alignment can expand the range of applications for quantum sensors, especially in space applications. Vibrations in handling and testing also can affect the alignment of components inside the packaging containing the vapor cell and optics. Careful consideration of the packaging materials and design must be taken to ensure longevity and repeatability. Because the cell needs to be heated, ex. 70ºC, thermal isolation and control is required for the light source. The element used in the vapor cell needs to have a boiling point that is reasonable to achieve and maintain for a constant vapor phase to observe atomic absorption resonances. Higher temperatures can also create stronger absorption resonances for observation. The cell heating design and method can effect temperature stability, power consumption, and number density of vapor required for absorption spectroscopy experiments. In this study, two approaches are developed for integrated thin film heaters. When the packaging, optics, and alignment have shown to be reliable for absorption studies, obtaining spectra is one of the final steps for developing an atomic sensor using chip-scale vapor cells. Achieving stable and repeatable absorption spectra is critical for demonstrating a viable atomic sensor that can be implemented into a wide range of applications in space borne sensors and payloads.1 |
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