4.7 Article

Higgs-Mediated Optical Amplification in a Nonequilibrium Superconductor

期刊

PHYSICAL REVIEW X
卷 11, 期 1, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevX.11.011055

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资金

  1. European Research Council under the European Union's Seventh Framework Programme (FP7/2007-2013)/ERC Grant [319286]
  2. Deutsche Forschungsgemeinschaft via the excellence cluster The Hamburg Centre for Ultrafast Imaging Structure, Dynamics and Control of Matter at the Atomic Scale
  3. National Science Foundation (NSF)
  4. Israel Science Foundation [1803/18]
  5. Harvard-MIT Center for Ultracold Atoms
  6. DARPA DRINQS program [D18AC00014]
  7. Vannevar Bush Faculty Fellowship
  8. Postdoctoral Fellowship of the Harvard-MPQ Center for Quantum Optics
  9. AFOSR-MURI Photonic Quantum Matter [FA95501610323]
  10. National Energy Research Scientific Computing Center (NERSC), a U.S. Department of Energy Office of Science User Facility [DEAC02-05CH11231]
  11. NSF [PHY-1607611]
  12. Deutsche Forschungsgemeinschaft [SFB925]

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The study introduces a novel nonequilibrium phenomenon where a prompt quench from a metal to a transient superconducting state induces large oscillations of the order parameter amplitude. The oscillating mode is suggested to act as a source of parametric amplification of the incident radiation, with experimental results on optically driven K3C60 supporting these predictions. The effect diminishes when the excitation onset surpasses the Higgs-mode period, presenting new possibilities for inducing nonlinear optical effects using collective modes in many-body systems.
We propose a novel nonequilibrium phenomenon, through which a prompt quench from a metal to a transient superconducting state can induce large oscillations of the order parameter amplitude. We argue that this oscillating mode acts as a source of parametric amplification of the incident radiation. We report experimental results on optically driven K3C60 that are consistent with these predictions. The effect is found to disappear when the onset of the excitation becomes slower than the Higgs-mode period, consistent with the theory proposed here. These results open new possibilities for the use of collective modes in many-body systems to induce nonlinear optical effects.

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