TY - JOUR
T1 - Norton Equivalent Circuit for Pulsed Photoconductive Antennas - Part II
T2 - Experimental Validation
AU - Garufo, Alessandro
AU - Carluccio, Giorgio
AU - Freeman, Joshua R.
AU - Bacon, David R.
AU - Llombart, Nuria
AU - Linfield, Edmund H.
AU - Davies, Alexander G.
AU - Neto, Andrea
PY - 2018
Y1 - 2018
N2 - This second part of two papers' sequence presents the experimental validation of the Norton equivalent circuit model for pulsed photoconductive antennas (PCAs) provided in the first paper of the sequence. To this goal, different prototypes of photoconductive antenna sources have been manufactured and assembled. The average powers radiated and their pertinent energy spectral densities have been measured. In order to obtain a validation of the original equivalent circuit proposed, an auxiliary electromagnetic analysis of the complete setup, including the quasi-optical (QO) link for the signals from the antenna feeds to the detectors had to be developed. By using the combined theoretical model (circuit and quasi-optics), an excellent agreement is achieved between the measured power and the power estimated. This agreement fully validates the circuit model, which can now be used to design new PCAs, including optical and electrical features of the semiconductor materials, as well as the details of the antenna gaps and the purely QO components.
AB - This second part of two papers' sequence presents the experimental validation of the Norton equivalent circuit model for pulsed photoconductive antennas (PCAs) provided in the first paper of the sequence. To this goal, different prototypes of photoconductive antenna sources have been manufactured and assembled. The average powers radiated and their pertinent energy spectral densities have been measured. In order to obtain a validation of the original equivalent circuit proposed, an auxiliary electromagnetic analysis of the complete setup, including the quasi-optical (QO) link for the signals from the antenna feeds to the detectors had to be developed. By using the combined theoretical model (circuit and quasi-optics), an excellent agreement is achieved between the measured power and the power estimated. This agreement fully validates the circuit model, which can now be used to design new PCAs, including optical and electrical features of the semiconductor materials, as well as the details of the antenna gaps and the purely QO components.
KW - Equivalent circuit
KW - photoconductivity
KW - terahertz (THz) measurement
KW - THz photoconductive antenna
KW - THz radiated power
KW - THz source
KW - THz technology
UR - http://www.scopus.com/inward/record.url?scp=85041418520&partnerID=8YFLogxK
UR - http://resolver.tudelft.nl/uuid:c342ab3d-593a-4bd1-a6b2-20c954931be3
U2 - 10.1109/TAP.2018.2800704
DO - 10.1109/TAP.2018.2800704
M3 - Article
AN - SCOPUS:85041418520
VL - 66
SP - 1646
EP - 1659
JO - IEEE Transactions on Antennas and Propagation
JF - IEEE Transactions on Antennas and Propagation
SN - 0018-926X
IS - 4
ER -