Numerical study of the spatial coherence of light in collective spontaneous emission

We present a numerical study of the spatial coherence of light that is radiated from a dilute ensemble of atoms. The spatial coherence is established as a result of the collective (cooperative) coupling of the atoms to the light and is qualitatively different from the coherence of a laser. Specifically, the coherence in collective spontaneous emission does not rely on population inversion and stimulated emission, is governed by antiphasing of the dipoles (subradiance), and the key figure of merit for the observed coherence is $\ensuremath{\approx}N/(L/\ensuremath{\lambda})$. Here, $N$ is the number of atoms in the ensemble, $L$ is the size of the sample, and $\ensuremath{\lambda}$ is the wavelength of the emitted light.

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Publication Details

Journal
Physical review. A/Physical review, A
Published
2024-10-08
DOI
https://doi.org/10.1103/physreva.110.043705
Citations
2
Primary Topic
Quantum optics and atomic interactions
Type
article
Field-Weighted Citation Impact
0.68

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article

Numerical study of the spatial coherence of light in collective spontaneous emission

D. C. Gold, M. Saffman, Thad Walker, D. D. Yavuz et al.
2 citations
Physical review. A/Physical review, A
Quantum optics and atomic interactions
0.68
article

Numerical study of the spatial coherence of light in collective spontaneous emission

D. C. Gold, M. Saffman, Thad Walker, D. D. Yavuz, Anirudh Yadav
article en
2 citations

Abstract

We present a numerical study of the spatial coherence of light that is radiated from a dilute ensemble of atoms. The spatial coherence is established as a result of the collective (cooperative) coupling of the atoms to the light and is qualitatively different from the coherence of a laser. Specifically, the coherence in collective spontaneous emission does not rely on population inversion and stimulated emission, is governed by antiphasing of the dipoles (subradiance), and the key figure of merit for the observed coherence is $\ensuremath{\approx}N/(L/\ensuremath{\lambda})$. Here, $N$ is the number of atoms in the ensemble, $L$ is the size of the sample, and $\ensuremath{\lambda}$ is the wavelength of the emitted light.

Physical review. A/Physical review, AVol. 110(4)
University of Wisconsin–Madison (US)
National Science Foundation, Purdue University, University of Wisconsin-Madison
Reduced inequalities
Openalex Percentile: Top 31%
Quantum optics and atomic interactions
0.68
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Numerical study of the spatial coherence of light in collective spontaneous emission — D. C. Gold, M. Saffman, et al. · Physical review. A/Physical review, A (2024) | TGRS Research Map | TGRS