Quantum correlations, mixed states, and bistability at the onset of lasing
Quantum correlations, mixed states, and bistability at the onset of lasing
We derive a model for a single-mode laser that includes all two-particle quantum correlations between photons and electrons. In contrast to the predictions of semiclassical models, we find that lasing takes place in the presence of quantum bistability between a nonlasing and a nonclassical coherent state. The coherent state is characterized by a central frequency and a finite linewidth and emerges with finite amplitude from a saddle-node bifurcation together with an unstable coherent state. Hence coherent emission in nanolasers originates through a mixing of lasing and nonlasing states. In the limit of a macrolaser with a large number of emitters and nonresonant modes, the laser threshold approaches the prediction of the semiclassical theory, but with the important difference that lasing can be achieved only in the presence of finite-size perturbations.
Optical coherence, Laser, quantum optics, nanolaser
Papoff, Francesco
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Carroll, Mark Anthony
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Lippi, Gian Luca
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Oppo, Gian-Luca
698002dc-8087-466d-90db-7cc18b3dc34d
D'Alessandro, Giampaolo
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7 January 2025
Papoff, Francesco
c845380e-f3e9-4c20-9d6c-0b7a66918174
Carroll, Mark Anthony
65b99dd5-caf3-4e77-a30d-f97c2678963c
Lippi, Gian Luca
ec4e6c7e-f969-4774-8e20-cb02b1504f21
Oppo, Gian-Luca
698002dc-8087-466d-90db-7cc18b3dc34d
D'Alessandro, Giampaolo
bad097e1-9506-4b6e-aa56-3e67a526e83b
Papoff, Francesco, Carroll, Mark Anthony, Lippi, Gian Luca, Oppo, Gian-Luca and D'Alessandro, Giampaolo
(2025)
Quantum correlations, mixed states, and bistability at the onset of lasing.
Physical Review A, 111 (1), [L011501].
(doi:10.1103/PhysRevA.111.L011501).
Abstract
We derive a model for a single-mode laser that includes all two-particle quantum correlations between photons and electrons. In contrast to the predictions of semiclassical models, we find that lasing takes place in the presence of quantum bistability between a nonlasing and a nonclassical coherent state. The coherent state is characterized by a central frequency and a finite linewidth and emerges with finite amplitude from a saddle-node bifurcation together with an unstable coherent state. Hence coherent emission in nanolasers originates through a mixing of lasing and nonlasing states. In the limit of a macrolaser with a large number of emitters and nonresonant modes, the laser threshold approaches the prediction of the semiclassical theory, but with the important difference that lasing can be achieved only in the presence of finite-size perturbations.
Text
PhysRevA.111.L011501
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Accepted/In Press date: 17 December 2024
Published date: 7 January 2025
Additional Information:
Publisher Copyright:
© 2025 authors. Published by the American Physical Society.
Keywords:
Optical coherence, Laser, quantum optics, nanolaser
Identifiers
Local EPrints ID: 497500
URI: http://eprints.soton.ac.uk/id/eprint/497500
ISSN: 1050-2947
PURE UUID: ffb9419c-1378-4962-9d2f-7da48608de5e
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Date deposited: 23 Jan 2025 17:56
Last modified: 22 Aug 2025 01:39
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Contributors
Author:
Francesco Papoff
Author:
Mark Anthony Carroll
Author:
Gian Luca Lippi
Author:
Gian-Luca Oppo
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