2015
DOI: 10.15446/ing.investig.v35n1.45310
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Simulation of photoconductive antennas for terahertz radiation

Abstract: Simulation of terahertz (THz) emission based on PC antennas imposes a challenge to couple the semiconductor carrier phenomena, optical transport and the THz energy transport. In this paper a Multi-physics simulation for coupling these phenomena using COMSOL Multi-physics 4.3b is introduced. The main parameters of THz photoconductive (PC) antenna as THz emitter have been reviewed and discussed. The results indicate the role of each parameter in the resulting photocurrent waveform and THz frequency: The radiated… Show more

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Cited by 9 publications
(3 citation statements)
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“…Different PCA designs and development have been done to serve different industries and applications However, many of these designs have been numerically studied without taking the manufacturing cost in their account [3,7,10]. Furthermore, most of these simulated designs have not considered the manufacturing viability.…”
Section: Introductionmentioning
confidence: 99%
“…Different PCA designs and development have been done to serve different industries and applications However, many of these designs have been numerically studied without taking the manufacturing cost in their account [3,7,10]. Furthermore, most of these simulated designs have not considered the manufacturing viability.…”
Section: Introductionmentioning
confidence: 99%
“…And the ECM can also be hardly used to simulate the generation of THz in the near field. Criollo et al simulated the THz emission of PCA with multiphysics processes by using COMSOL Multi‐physics 4.3b . Jitao Zhang et al numerically studied the physical mechanism of THz emission in the PCA by using three‐dimensional finite‐difference time‐domain (3D‐FDTD) method.…”
Section: Introductionmentioning
confidence: 99%
“…Numerous structures of photoconductive antennas have been proposed, which were based on the incorporation of optical nano antennas [17], fractal geometries [18], gammadion-type structure [19], tapered helix monopole [20], hexagonal nano-antenna [21], interdigitated metallic dipole nanoantenna [22]- [24], 3D plasmon contact electrodes [25], nano-structured electrodes [26], thin-film plasma electrode [27], rectangular metal dipole nanoantenna [28], bow-tie metallic dipole nanoantenna [28], plasmon contact electrodes [29], [30], SRR-loaded antennas [31], and arrays of bowtie and four-leaf-clover-shaped antennas [32]. Further, several numerical models have been proposed for understanding the dynamics of these photoconductive antennas, such as full-wave numerical technique based on Maxwell and hydrodynamic transport equations [33], semiconductor carrier transport and migration models [22], [34], time-domain numerical modeling [35], numerical solution of induced current based on Monte Carlo simulation [36], finite element method [27], [37], and three-dimensional full-wave model [38].…”
Section: Introductionmentioning
confidence: 99%