Dec 3, 2024
8:00pm - 10:00pm
Hynes, Level 1, Hall A
Prasanna Das1,Sourav Rudra1,Dheemahi Rao1,Souvik Banerjee1,Ashalatha Indiradevi Kamalasanan Pillai2,Magnus Garbrecht2,Alexandra Boltasseva3,Igor Bondarev4,Vladimir Shalaev3,Bivas Saha1
Jawaharlal Nehru Centre for Advanced Scientific Research1,The University of Sydney2,Purdue University3,North Carolina Central University4
Prasanna Das1,Sourav Rudra1,Dheemahi Rao1,Souvik Banerjee1,Ashalatha Indiradevi Kamalasanan Pillai2,Magnus Garbrecht2,Alexandra Boltasseva3,Igor Bondarev4,Vladimir Shalaev3,Bivas Saha1
Jawaharlal Nehru Centre for Advanced Scientific Research1,The University of Sydney2,Purdue University3,North Carolina Central University4
Plasmon resonance in metals represents the collective oscillation of the free electron gas density and enables enhanced light-matter interactions in nanoscale dimensions. Traditionally, the classical Drude model describes the plasmonic excitation, wherein the plasma frequency exhibits no spatial dispersion. Here, we show conclusive experimental evidence of the breakdown of the plasmon resonance and a consequent photonic metal-insulator transition in an ultrathin archetypal refractory plasmonic material, hafnium nitride (HfN). Epitaxial HfN thick films exhibit a low-loss and high-quality Drude-like plasmon resonance in the visible spectral range. However, as the film thickness is reduced to nanoscale dimensions, the Coulomb interaction among electrons increases due to the electron confinement, leading to the spatial dispersion of the plasma frequency. Importantly, with the further decrease in thickness, electrons lose their ability to shield the incident electric field, turning the medium into a dielectric. The breakdown of the plasmon resonance in epitaxial ultrathin metals could be useful for fundamental physics studies in transdimensional regimes and novel photonic device applications.