- Open Access
Generalized Schawlow-Townes limit
Phys. Rev. A 113, 043717 – Published 8 April, 2026
DOI: https://doi.org/10.1103/6t5c-swxn
Abstract
We study a class of feedback oscillators realized by a phase-insensitive amplifier in positive feedback, where either the amplifier or the feedback element may determine the oscillator's linewidth. The spectral purity of the output of such a device originates from basic demands of quantum mechanics and causality. The resulting expression generalizes the Schawlow-Townes limit, which is itself one component of a standard quantum limit for feedback oscillators. Recently realized bad-cavity oscillators, such as superradiant lasers and solid-state masers, can saturate this generalized Schawlow-Townes limit. This limit can be surpassed through appropriate quantum engineering, for example, by atomic spin squeezing in a superradiant laser.
Physics Subject Headings (PhySH)
Article Text
References (58)
- A. L. Schawlow and C. H. Townes, Infrared and optical masers, Phys. Rev. 112, 1940 (1958).
- R. Hempstead and M. Lax, Classical noise. VI. Noise in self-sustained oscillators near threshold, Phys. Rev. 161, 350 (1967).
- M. O. Scully and W. E. Lamb, Quantum theory of an optical maser. I. General theory, Phys. Rev. 159, 208 (1967).
- H. Haken, Laser Theory (Springer, New York, 1984).
- M. Sargent, M. O. Scully, and W. E. Lamb, Laser Physics (Westview, Boulder, CO, 1974).
- A. Yariv and W. Caton, Frequency, intensity, and field fluctuations in laser oscillators, IEEE J. Quantum Electron. 10, 509 (1974).
- C. Henry, Theory of the phase noise and power spectrum of a single mode injection laser, IEEE J. Quantum Electron. 19, 1391 (1983).
- P. Goldberg, P. W. Milonni, and B. Sundaram, Theory of the fundamental laser linewidth, Phys. Rev. A 44, 1969 (1991).
- H. A. Loughlin and V. Sudhir, Quantum noise and its evasion in feedback oscillators, Nat. Commun. 14, 7083 (2023).
- H. M. Goldenberg, D. Kleppner, and N. F. Ramsey, Atomic hydrogen maser, Phys. Rev. Lett. 5, 361 (1960).
- S. J. M. Kuppens, M. P. van Exter, and J. P. Woerdman, Quantum-limited linewidth of a bad-cavity laser, Phys. Rev. Lett. 72, 3815 (1994).
- K. Benmessai, D. L. Creedon, M. E. Tobar, P.-Y. Bourgeois, Y. Kersalé, and V. Giordano, Measurement of the fundamental thermal noise limit in a cryogenic sapphire frequency standard using bimodal maser oscillations, Phys. Rev. Lett. 100, 233901 (2008).
- J. G. Bohnet, Z. Chen, J. M. Weiner, D. Meiser, M. J. Holland, and J. K. Thompson, A steady-state superradiant laser with less than one intracavity photon, Nature (London) 484, 78 (2012).
- M. Oxborrow, J. D. Breeze, and N. M. Alford, Room-temperature solid-state maser, Nature (London) 488, 353 (2012).
- M. A. Norcia and J. K. Thompson, Cold-strontium laser in the superradiant crossover regime, Phys. Rev. X 6, 011025 (2016).
- M. A. Norcia, M. N. Winchester, J. R. K. Cline, and J. K. Thompson, Superradiance on the millihertz linewidth strontium clock transition, Sci. Adv. 2, e1601231 (2016).
- J. Yablon, Z. Zhou, N. Condon, D. Hileman, S. Tseng, and S. Shahriar, Demonstration of a highly subluminal laser with suppression of cavity length sensitivity by nearly three orders of magnitude, Opt. Express 25, 30327 (2017).
- J. D. Breeze, E. Salvadori, J. Sathian, N. M. Alford, and C. W. M. Kay, Continuous-wave room-temperature diamond maser, Nature (London) 555, 493 (2018).
- T. Day, M. Isarov, W. J. Pappas, B. C. Johnson, H. Abe, T. Ohshima, D. R. McCamey, A. Laucht, and J. J. Pla, Room-temperature solid-state maser amplifier, Phys. Rev. X 14, 041066 (2024).
- J. Zhang, T. Shi, J. Miao, D. Yu, and J. Chen, An extremely bad-cavity laser, npj Quantum Inf. 10, 87 (2024).
- M. O. Scully, G. Süssmann, and C. Benkert, Quantum noise reduction via maser memory effects: Theory and applications, Phys. Rev. Lett. 60, 1014 (1988).
- J. Chen, Active optical clock, Sci. Bull. 54, 348 (2009).
- D. Meiser, J. Ye, D. R. Carlson, and M. J. Holland, Prospects for a millihertz-linewidth laser, Phys. Rev. Lett. 102, 163601 (2009).
- M. A. Norcia, J. R. Cline, J. A. Muniz, J. M. Robinson, R. B. Hutson, A. Goban, G. E. Marti, J. Ye, and J. K. Thompson, Frequency measurements of superradiance from the strontium clock transition, Phys. Rev. X 8, 021036 (2018).
- M. Lax, in Physics of Quantum Electronics, edited by P. L. Kelley, B. Lax, and P. E. Tannenwald (McGraw-Hill, New York, 1966), p. 735.
- L. Davidovich, Sub-Poissonian processes in quantum optics, Rev. Mod. Phys. 68, 127 (1996).
- D. Kleppner, H. M. Goldenberg, and N. F. Ramsey, Theory of the hydrogen maser, Phys. Rev. 126, 603 (1962).
- H. A. Haus and J. A. Mullen, Quantum noise in linear amplifiers, Phys. Rev. 128, 2407 (1962).
- C. M. Caves, Quantum limits on noise in linear amplifiers, Phys. Rev. D 26, 1817 (1982).
- H. Bode, Network Analysis and Feedback Amplifier Design (Van Nostrand, New York, 1945).
- J. S. Toll, Causality and the dispersion relation: Logical foundations, Phys. Rev. 104, 1760 (1956).
- M. Prevedelli, A. Perinelli, and L. Ricci, Bode gain-phase relation beyond the minimum phase condition, Europhys. Lett. 149, 22002 (2025).
- H. Haken, Theory of coherence of laser light, Phys. Rev. Lett. 13, 329 (1964).
- H. Haken, Theory of intensity and phase fluctuations of a homogeneously broadened laser, Z. Phys. 190, 327 (1966).
- J. Ding, H. A. Loughlin, and V. Sudhir, Quantum linear time-translation-invariant systems: Conjugate symplectic structure, uncertainty bounds, and tomography, arXiv:2410.09976.
- K. Debnath, Y. Zhang, and K. Mølmer, Lasing in the superradiant crossover regime, Phys. Rev. A 98, 063837 (2018).
- J. G. Bohnet, Z. Chen, J. M. Weiner, K. C. Cox, and J. K. Thompson, Linear-response theory for superradiant lasers, Phys. Rev. A 89, 013806 (2014).
- T. Holstein and H. Primakoff, Field dependence of the intrinsic domain magnetization of a ferromagnet, Phys. Rev. 58, 1098 (1940).
- F. Persico and G. Vetri, Coherence properties of the -atom-radiation interaction and the Holstein-Primakoff transformation, Phys. Rev. A 12, 2083 (1975).
- M. J. Collett and C. W. Gardiner, Squeezing of intracavity and traveling-wave light fields produced in parametric amplification, Phys. Rev. A 30, 1386 (1984).
- V. Meyer, M. A. Rowe, D. Kielpinski, C. A. Sackett, W. M. Itano, C. Monroe, and D. J. Wineland, Experimental demonstration of entanglement-enhanced rotation angle estimation using trapped ions, Phys. Rev. Lett. 86, 5870 (2001).
- D. Leibfried, M. D. Barrett, T. Schaetz, J. Britton, J. Chiaverini, W. M. Itano, J. D. Jost, C. Langer, and D. J. Wineland, Toward Heisenberg-limited spectroscopy with multiparticle entangled states, Science 304, 1476 (2004).
- J. Appel, P. J. Windpassinger, D. Oblak, U. B. Hoff, N. Kjærgaard, and E. S. Polzik, Mesoscopic atomic entanglement for precision measurements beyond the standard quantum limit, Proc. Natl. Acad. Sci. 106, 10960 (2009).
- I. D. Leroux, M. H. Schleier-Smith, and V. Vuletic, Implementation of cavity squeezing of a collective atomic spin, Phys. Rev. Lett. 104, 073602 (2010).
- C. Gross, T. Zibold, E. Nicklas, J. Estève, and M. K. Oberthaler, Nonlinear atom interferometer surpasses classical precision limit, Nature (London) 464, 1165 (2010).
- R. J. Sewell, M. Koschorreck, M. Napolitano, B. Dubost, N. Behbood, and M. W. Mitchell, Magnetic sensitivity beyond the projection noise limit by spin squeezing, Phys. Rev. Lett. 109, 253605 (2012).
- O. Hosten, N. J. Engelsen, R. Krishnakumar, and M. A. Kasevich, Measurement noise 100 times lower than the quantum-projection limit using entangled atoms, Nature (London) 529, 505 (2016).
- C. Miller, A. N. Carroll, J. Lin, H. Hirzler, H. Gao, H. Zhou, M. D. Lukin, and J. Ye, Two-axis twisting using Floquet-engineered xyz spin models with polar molecules, Nature (London) 633, 332 (2024).
- D. J. Wineland, J. J. Bollinger, W. M. Itano, F. L. Moore, and D. J. Heinzen, Spin squeezing and reduced quantum noise in spectroscopy, Phys. Rev. A 46, R6797 (1992).
- M. Kitagawa and M. Ueda, Squeezed spin states, Phys. Rev. A 47, 5138 (1993).
- Y. C. Liu, Z. F. Xu, G. R. Jin, and L. You, Spin squeezing: Transforming one-axis twisting into two-axis twisting, Phys. Rev. Lett. 107, 013601 (2011).
- C. Luo, H. Zhang, A. Chu, C. Maruko, A. M. Rey, and J. K. Thompson, Hamiltonian engineering of collective XYZ spin models in an optical cavity, Nat. Phys. 21, 916 (2025).
- Note that is the ratio of the rate of spin squeezing generation to the rate at which atomic excitation leaves the cavity as optical photons. It plays the role of the squeezing factor in this problem.
- H. Loughlin, Plots for a generalized Schawlow-Townes limit (2026), https://dx.doi.org/10.6084/m9.figshare.31768990.
- A. A. Clerk, M. H. Devoret, S. M. Girvin, F. Marquardt, and R. J. Schoelkopf, Introduction to quantum noise, measurement, and amplification, Rev. Mod. Phys. 82, 1155 (2010).
- In the spin-squeezed case, this assumption is necessary since the drive that determines the squeezing angle implies a preferred quadrature. Note that classical noise in this drive needs to be considered in any practical implementation of this scheme.
- G. Di Domenico, S. Schilt, and P. Thomann, Simple approach to the relation between laser frequency noise and laser line shape, Appl. Opt. 49, 4801 (2010).
- T. Kashiwazaki, T. Yamashima, N. Takanashi, A. Inoue, T. Umeki, and A. Furusawa, Fabrication of low-loss quasi-single-mode PPLN waveguide and its application to a modularized broadband high-level squeezer, Appl. Phys. Lett. 119, 251104 (2021).