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CS-TC08 Scheda tecnica(PDF) 1 Page - Wavelength Electronics, Inc.

Il numero della parte CS-TC08
Spiegazioni elettronici  VCSEL Absorption Spectroscopy of Chip-scale Rubidium Atomic Vapor
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Produttore elettronici  WAVELENGTH [Wavelength Electronics, Inc.]
Homepage  https://www.teamwavelength.com/
Logo WAVELENGTH - Wavelength Electronics, Inc.

CS-TC08 Scheda tecnica(HTML) 1 Page - Wavelength Electronics, Inc.

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© 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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