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This research demonstrates an optical-frequency superradiant laser that surpasses the standard quantum limit for coherence scaling, achieving performance closer to the Heisenberg limit through collective pumping mechanisms. By extending previous microwave-frequency circuit QED results to the optical regime, this work advances fundamental limits in quantum optics and precision measurement technologies.
Collectively pumped superradiant laser with coherence scaling beyond the standard quantum limit
arXiv:2611.05976v1 Announce Type: new Abstract: For more than half a century, the standard quantum limit (SQL) was thought to limit the laser coherence $\mathfrak{C}$ -- the number of photons emitted from the laser into the beam in one coherence time -- to a scaling $\Theta(\mu^2)$, where $\mu$ is the mean number of optical-frequency excitations stored inside the laser. However, recently it has been shown [Baker et al., Nat. Phys. 17, 179 (2021)] that the Heisenberg limit -- an achievable ultimate limit set by quantum mechanics for the task of producing a beam with the standard properties of a laser beam -- is $\mathfrak{C}=\Theta(\mu^4)$, a quadratic enhancement. So far, proposals to demonstrate beyond-SQL scaling of $\mathfrak{C}$ have been limited to circuit QED, at microwave frequencies (i.e., a maser). Here, we introduce a class of generalized far-above-threshold (FAT) laser models, obtained by replacing the ordinary bosonic lowering operator $\hat{a}$ by a general lowering operator $\hat{L}$ in the superoperators appearing in the master equation that governs the FAT laser dynamics. We then show that an optical-frequency superradiant laser in the bad-cavity limit, with feedback-controlled collective pumping, realizes one such model, in which $\hat{L}$ is identified with the collective superradiant lowering operator $\hat{J}$. This model can surpass the SQL scaling, with the coherence exhibiting a scaling as large as $\mathfrak{C}= \Theta(\mu^{8/3})$ in the optimal parameter regime. Here, in the bad-cavity limit, $\mu\approx N/2$, where $N$ is the number of superradiant atoms.
Abstract:For more than half a century, the standard quantum limit (SQL) was thought to limit the laser coherence $\mathfrak{C}$ -- the number of photons emitted from the laser into the beam in one coherence time -- to a scaling $\Theta(\mu^2)$, where $\mu$ is the mean number of optical-frequency excitations stored inside the laser. However, recently it has been shown [Baker et al., Nat. Phys. 17, 179 (2021)] that the Heisenberg limit -- an achievable ultimate limit set by quantum mechanics for the task of producing a beam with the standard properties of a laser beam -- is $\mathfrak{C}=\Theta(\mu^4)$, a quadratic enhancement. So far, proposals to demonstrate beyond-SQL scaling of $\mathfrak{C}$ have been limited to circuit QED, at microwave frequencies (i.e., a maser). Here, we introduce a class of generalized far-above-threshold (FAT) laser models, obtained by replacing the ordinary bosonic lowering operator $\hat{a}$ by a general lowering operator $\hat{L}$ in the superoperators appearing in the master equation that governs the FAT laser dynamics. We then show that an optical-frequency superradiant laser in the bad-cavity limit, with feedback-controlled collective pumping, realizes one such model, in which $\hat{L}$ is identified with the collective superradiant lowering operator $\hat{J}$. This model can surpass the SQL scaling, with the coherence exhibiting a scaling as large as $\mathfrak{C}= \Theta(\mu^{8/3})$ in the optimal parameter regime. Here, in the bad-cavity limit, $\mu\approx N/2$, where $N$ is the number of superradiant atoms.
36 pages, 16 figures. Submitted to Physical Review X
Quantum Physics (quant-ph); Atomic Physics (physics.atom-ph); Optics (physics.optics)
arXiv:2611.05976 [quant-ph]
(or arXiv:2611.05976v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2611.05976 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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Full text under the publisher's open licence · 340 words
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