2021
DOI: 10.1021/acsphotonics.1c00717
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THz Ultrastrong Coupling in an Engineered Fabry–Perot Cavity

Abstract: We report a monolithic THz planar Fabry−Perot cavity fabricated with wafer bonding and provided with metallic mirrors with subwavelength apertures. We demonstrate its coupling to the cyclotron resonance of a high-mobility, twodimensional electron gas. Q factors up to 89 are observed for the first mode at ≃300 GHz, with cooperativity C = 56.4 and a normalized coupling ratio ω Ω in the first mode of up to 17.5% and the third mode of up to 6.4%.

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Cited by 20 publications
(9 citation statements)
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“…The mirrors establish symmetry, enabling the waves to travel within the cavity; in addition, because the mirrors have a modulus close to zero, the waves behave like standing ones. The Fabry–Perot cavity displays a high quality factor Q and a small modal volume V / V 0 , and for this reason, they play a decisive role in quantum electrodynamics investigation and light/matter interaction. The high factor derives from a line width that is narrower than the vibrational frequency of the molecular species and imposes the crucial hierarchy in a resolved sideband regime where the mechanical frequency exceeds the optical line width as a fundamental condition . An important family of Fabry–Perot systems is constituted by the metal/dielectric/metal stack layer cavity, which is frequently used in cutting-edge plasmonics research.…”
Section: Introductionmentioning
confidence: 99%
“…The mirrors establish symmetry, enabling the waves to travel within the cavity; in addition, because the mirrors have a modulus close to zero, the waves behave like standing ones. The Fabry–Perot cavity displays a high quality factor Q and a small modal volume V / V 0 , and for this reason, they play a decisive role in quantum electrodynamics investigation and light/matter interaction. The high factor derives from a line width that is narrower than the vibrational frequency of the molecular species and imposes the crucial hierarchy in a resolved sideband regime where the mechanical frequency exceeds the optical line width as a fundamental condition . An important family of Fabry–Perot systems is constituted by the metal/dielectric/metal stack layer cavity, which is frequently used in cutting-edge plasmonics research.…”
Section: Introductionmentioning
confidence: 99%
“…As an alternative route to control over material properties, light-matter coupling (LMC) in cavities has been suggested [53][54][55][56][57]. In these setups, instead of achieving strong modifications of material properties by strong driving, one focuses on realizing strong coupling (SC) between light and matter, supported by recent experimental advances [58][59][60][61][62][63][64][65][66]. This might enable the engineering of material properties already with few photons [67,68] or even inside a dark cavity, utilizing only the vacuum fluctuations of the light field [69].…”
Section: Introductionmentioning
confidence: 99%
“…The effective volume can be markedly improved by introducing microcavity structures, such as Fabry–Perot (FP) interferometers. In semiconductors, it has been adopted as an ideal cavity system to address the exciton polaritons in the visible and near-IR range. ,,, Besides, in the mid-IR range, an intersubband polariton has been introduced; for instance, mid-IR laser emission was observed through polariton-LO phonon scattering. , In particular, strong coupling of the vibrational modes with THz fields in FP microcavities has been demonstrated for α-lactose monohydrate, polar liquids, and carbonyl (PMMA) . To incorporate perovskite phonons into the microcavity, the thin perovskite film must be located at the center of the cavity, which can have strong field enhancement effects. , Conversely, the presence of supporting substrates disturbs the field distribution in the cavity and, hence, the light–matter coupling efficiency.…”
mentioning
confidence: 99%