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This study establishes a fundamental no-go theorem proving that vacuum fluctuations in passive cavities inherently suppress superconductivity rather than enhancing it, challenging recent experimental claims of cavity-modified transition temperatures. The authors identify two specific pathways to overcome this limit by coupling the system to additional collective degrees of freedom or competing orders, effectively turning theoretical constraints into practical design principles for future quantum materials.
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No-Go Theorem and Routes towards Cavity-Enhanced Superconductivity

arXiv2 min de cititArticolul și perspectiva sunt în engleză.

arXiv:2608.14784v1 Announce Type: cross Abstract: Recent experiments reporting cavity-vacuum-modified superconductivity raise a fundamental question: under what conditions can vacuum electromagnetic fluctuations increase a superconducting transition temperature? Starting from a Ginzburg--Landau theory minimally coupled to a quantized cavity mode, we derive the cavity-induced renormalization of the superconducting free energy. This correction comprises a positive diamagnetic contribution and a negative paramagnetic exchange contribution. We prove that, in a passive cavity, the latter cannot exceed the former, establishing a no-go theorem: within minimal cavity electrodynamics, vacuum fluctuations suppress, rather than enhance, superconductivity. We then identify two routes beyond this constraint, both involving additional collective degrees of freedom. In the collective-mode route, a cavity-active excitation amplifies the attractive paramagnetic contribution. In the competing-order route, the cavity weakens an order that competes with superconductivity, thereby indirectly enhancing superconductivity. Together, these results turn the no-go theorem into a practical design principle: cavity superconductivity enhancement requires an additional cavity-coupled material mode that either strengthens paramagnetic exchange or suppresses a competing order.

Abstract:Recent experiments reporting cavity-vacuum-modified superconductivity raise a fundamental question: under what conditions can vacuum electromagnetic fluctuations increase a superconducting transition temperature? Starting from a Ginzburg--Landau theory minimally coupled to a quantized cavity mode, we derive the cavity-induced renormalization of the superconducting free energy. This correction comprises a positive diamagnetic contribution and a negative paramagnetic exchange contribution. We prove that, in a passive cavity, the latter cannot exceed the former, establishing a no-go theorem: within minimal cavity electrodynamics, vacuum fluctuations suppress, rather than enhance, superconductivity. We then identify two routes beyond this constraint, both involving additional collective degrees of freedom. In the collective-mode route, a cavity-active excitation amplifies the attractive paramagnetic contribution. In the competing-order route, the cavity weakens an order that competes with superconductivity, thereby indirectly enhancing superconductivity. Together, these results turn the no-go theorem into a practical design principle: cavity superconductivity enhancement requires an additional cavity-coupled material mode that either strengthens paramagnetic exchange or suppresses a competing order.

Superconductivity (cond-mat.supr-con); Quantum Physics (quant-ph)

arXiv:2608.14784 [cond-mat.supr-con]

(or arXiv:2608.14784v1 [cond-mat.supr-con] for this version)

https://doi.org/10.48550/arXiv.2608.14784 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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