Impedance Matching of THz Plasmonic Antennas

Autor(en): Bettenhausen, Maximilian
Gruessing, Soenke
Hardt, Elena
Flesch, Julia
Roemer, Friedhard
Chavarin, Carlos Alvarado
Klesse, Wolfgang M.
You, Changjiang 
Piehler, Jacob 
Capellini, Giovanni
Witzigmann, Bernd
Stichwörter: Engineering; Engineering, Electrical & Electronic; Germanium on silicon; Graphene; Impedance matching; MOBILITY; Optics; Physics; Physics, Applied; Plasmonics; Semiconductor antennas; TERAHERTZ
Erscheinungsdatum: 2019
Herausgeber: SPRINGER
Journal: JOURNAL OF INFRARED MILLIMETER AND TERAHERTZ WAVES
Volumen: 40
Ausgabe: 9
Startseite: 929
Seitenende: 942
Zusammenfassung: 
Plasmonic antennas with subwavelength gaps work as sensing devices for molecules for the optical and terahertz (THz) frequency range. In such a configuration, the sensing gap creates a high impedance, in contrast to the antenna itself, which is designed for low ohmic losses. Besides metals, highly doped semiconductors can be used as plasmonic materials for the THz range, which increase the impedance of the antenna while keeping the strong electromagnetic intensity enhancement in the sensing gap. Still, a substantial impedance mismatch remains. In this paper, an approach for matching the gap to the antenna impedance is proposed. First, a germanium semiconductor slab antenna is designed for THz operation, with a dipole resonance at 4 THz. Based on an impedance analysis, an impedance matching element consisting of a graphene sheet is inserted in parallel to the gap. Employing impedance matching, a strong intensity enhancement occurs and the normal dipole mode of the plasmonic antenna is split into a symmetric one at 0.67 THz and an antisymmetric one at 4 THz. The symmetric mode provides a very high-quality factor and a substantial enhancement; furthermore, its resonance can be tuned by the Fermi level adjustment in the graphene. First designs of this structure are computed analytically with a circuit model and are verified by 3D full-wave simulations.
ISSN: 18666892
DOI: 10.1007/s10762-019-00613-0

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