Continuous superradiant laser based on a simple hot atomic beam
ORAL
Abstract
We will report on our recent work that aims to experimentally demonstrate continuous superradiance on the 1S0-3P1 transition of 88Sr. Our approach employs a simple architecture based on a hot atomic beam of excited atoms passing through a cavity that was recently proposed [1,2]. Superradiant lasing in the bad-cavity regime decreases cavity pulling reducing sensitivity to environmental perturbations. Due to the promise of cavity noise suppression, superradiant lasers have been proposed as a next generation optical frequency reference for atomic clocks [3].
To achieve sufficient atomic flux through the cavity mode we use an oven with an elongated aperture aligned to the cavity axis and employ transverse cooling to reduce the transverse velocity of the atoms to below 1 m/s. Atoms with a velocity along the cavity axis below 0.5 m/s are selectively stored in the metastable 3P0 state. This allows remaining ground-state atoms to be Doppler shifted away from the bare atomic resonance preventing interaction with the collective cavity mode. Immediately before the velocity-selected atoms enter the cavity, they are optically pumped to the 3P1 state. This architecture shows potential as a compact, robust and simple, optical frequency reference with microwatt power levels and linewidths of about 10 Hz, ideal for a wide range of industrial and scientific applications.
[1] Jingbiao Chen, arXiv:physics/0512096 (2005).
[2] Liu et al, Phys. Rev. Lett. 125, 253602 (2020).
[3] Meiser et al., Phys. Rev. Lett. 102, 163601 (2009).
To achieve sufficient atomic flux through the cavity mode we use an oven with an elongated aperture aligned to the cavity axis and employ transverse cooling to reduce the transverse velocity of the atoms to below 1 m/s. Atoms with a velocity along the cavity axis below 0.5 m/s are selectively stored in the metastable 3P0 state. This allows remaining ground-state atoms to be Doppler shifted away from the bare atomic resonance preventing interaction with the collective cavity mode. Immediately before the velocity-selected atoms enter the cavity, they are optically pumped to the 3P1 state. This architecture shows potential as a compact, robust and simple, optical frequency reference with microwatt power levels and linewidths of about 10 Hz, ideal for a wide range of industrial and scientific applications.
[1] Jingbiao Chen, arXiv:physics/0512096 (2005).
[2] Liu et al, Phys. Rev. Lett. 125, 253602 (2020).
[3] Meiser et al., Phys. Rev. Lett. 102, 163601 (2009).
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Presenters
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Sheng Zhou
University of Amsterdam
Authors
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Sheng Zhou
University of Amsterdam
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Francesca Fama
University of Amsterdam
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Camila Beli Silva
University of Amsterdam
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Mikkel Tang
University of Copenhagen, University of Amsterdam
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Zeyuan Zhang
University of Amsterdam
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Stefan Alaric Schäffer
University of Amsterdam
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ChunChia Chen
University of Amsterdam, National Institute of Standards and Technology, University of Colorado, NIST, University of Colorado, Boulder
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Benjamin Pasquiou
University of Amsterdam
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Shayne Bennetts
University of Amsterdam
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Florian Schreck
University of Amsterdam