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Characterizing Far-infrared Laser Emissions and the Measurement of Their Frequencies
Published on: December 18, 2015
Ramsey-Bordé Matter-Wave Interferometry for Laser Frequency Stabilization at 10^{-16} Frequency Instability and Below
Judith Olson1,2, Richard W Fox1, Tara M Fortier1
1Time and Frequency Division, National Institute of Standards and Technology, Boulder, Colorado 80305, USA.
Ramsey-Bordé atom interferometry achieves high-performance laser stabilization with fractional frequency instability below 2×10⁻¹⁶. This method surpasses other atomic systems, offering a new standard for laser stability.
Area of Science:
- Atomic Physics
- Laser Spectroscopy
- Quantum Metrology
Background:
- Laser stabilization is crucial for precision measurements.
- Atomic spectroscopy offers high-resolution frequency references.
- Ramsey-Bordé (RB) interferometry provides a sensitive probe for atomic transitions.
Purpose of the Study:
- To demonstrate high-performance laser stabilization using RB atom interferometry.
- To achieve fractional frequency instability below 2×10⁻¹⁶.
- To evaluate the performance of RB spectroscopy on the ⁴⁰Ca ⁶⁵⁷ nm transition.
Main Methods:
- Utilizing RB atom interferometry with two counterpropagating ⁴⁰Ca atomic beams.
- Interrogating the ¹S₀-³P₁ transition at 657 nm.
- Employing fluorescence detection on the ³P₁-³P₀ transition at 431 nm.
Main Results:
- Achieved fractional frequency instability <2×10⁻¹⁶ for timescales of 10–1000 s.
- Observed 1.6 kHz linewidth interference fringes.
- Demonstrated superior stability compared to other atomic/molecular systems.
Conclusions:
- RB atom interferometry is a highly effective technique for laser stabilization.
- The demonstrated stability surpasses existing methods by 1–2 orders of magnitude.
- Further improvements in laser stability are anticipated with this technique.
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Consider the electromagnetic wave passing through a dielectric medium. In such a case, Maxwell's equations get modified. In Ampere's law, ε0 , the dielectric permittivity of free space is replaced with ε, the permittivity of dielectric. Also, the vacuum permeability μ0 is replaced by the permeability of the medium, μ.
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