From Superfluorescence to Ultrastrong Light-Matter Coupling: Dicke Physics in Solid-State Quantum Matter
ORAL · Invited
Abstract
Ultrafast and ultrastrong light–matter interaction in solids can reveal collective optical phenomena that are traditionally studied in quantum optics [1]. Solid-state systems provide new platforms with giant dipole moments, highlighting the pivotal role of many-body enhancement of light-matter coupling. We explore Dicke phenomena in solids, including cooperative emission and collective decay. We demonstrated superfluorescence in electron–hole ensembles [2], a burst of emission where peak intensity scales as $N^2$ [3]. We also observe cooperative radiative damping of cyclotron resonance in high-mobility electron systems, where the decoherence rate scales linearly with carrier density [4]. Motivated by the Dicke superradiant phase transition (SRPT), we first explored the ultrastrong coupling regime in a 2D electron gas in a THz cavity [5,6], showing the breakdown of the rotating-wave approximation via the vacuum Bloch–Siegert shift. We also demonstrated Dicke cooperativity [7] and the magnonic SRPT [8] in the $Er^{3+}-Fe^{3+}$ exchange interaction within the antiferromagnet $ErFeO_3$. This matter-matter coupling avoids the no-go theorem, enabling the experimental observation of the magnonic SRPT, characterized by the simultaneous kink and softening of the hybrid spin-magnon modes [8]. These studies demonstrate cooperative light–matter interactions in solids are not perturbative; they emerge naturally and profoundly shape the dynamics of correlated electrons. I will discuss implications for realizing novel nonequilibrium quantum phases and engineering functional quantum devices through cavity control.
1. K. Cong et al., J. Opt. Soc. Am. B 33, C80 (2016); 2. G. T. Noe II et al., Nat. Phys. 8, 219 (2012); 3. R. H. Dicke, Phys. Rev. 93, 99 (1954); 4. Q. Zhang et al., Phys. Rev. Lett. 113, 047601 (2014); 5. Q. Zhang et al., Nat. Phys. 12, 1005 (2016); 6. X. Li et al., Nat. Photon. 12, 324 (2018); 7. X. Li et al., Science 361, 794 (2018); 8. D. Kim et al., Sci. Adv. 11, eadt1691 (2025).
1. K. Cong et al., J. Opt. Soc. Am. B 33, C80 (2016); 2. G. T. Noe II et al., Nat. Phys. 8, 219 (2012); 3. R. H. Dicke, Phys. Rev. 93, 99 (1954); 4. Q. Zhang et al., Phys. Rev. Lett. 113, 047601 (2014); 5. Q. Zhang et al., Nat. Phys. 12, 1005 (2016); 6. X. Li et al., Nat. Photon. 12, 324 (2018); 7. X. Li et al., Science 361, 794 (2018); 8. D. Kim et al., Sci. Adv. 11, eadt1691 (2025).
*We acknowledge support from the U.S. Army Research Office (through Award No. W911NF2110157), the Gordon and Betty Moore Foundation (through Grant No. 11520), the W. M. Keck Foundation (through Award No. 995764), and the Robert A. Welch Foundation (through Grant No. C-1509).
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Presenters
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Junichiro Kono
- Rice University
- Department of Electrical and Computer Engineering, Rice University, Houston, TX 77005, USA