E. Castro-Camus, M. Alfaro, "Photoconductive devices for terahertz pulsed spectroscopy: a review [Invited]," Photonics Res. 4, 0A36 (2016)

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- Photonics Research
- Vol. 4, Issue 3, 0A36 (2016)

Fig. 1. Typical THz-TDS setup. The photoconductive emitter and detector are shown.

Fig. 2. Typical THz transient produced and detected by photoconductive switches (left) and its spectrum (right).
![Resistance and lifetime measurements for a bow-tie antenna with a 5 μm photoconductive gap. Regions (I) and (II) are marked according to the two-stage increase in the resistivity at intermediate anneal temperatures and correspond to expected optimum requirements for THz receivers and emitters, respectively. Reproduced with permission from [28], copyright 2003, American Institute of Physics.](/Images/icon/loading.gif)
Fig. 3. Resistance and lifetime measurements for a bow-tie antenna with a 5 μm photoconductive gap. Regions (I) and (II) are marked according to the two-stage increase in the resistivity at intermediate anneal temperatures and correspond to expected optimum requirements for THz receivers and emitters, respectively. Reproduced with permission from [28], copyright 2003, American Institute of Physics.
![Schematic of a single nanowire photoconductive detector geometry and optical arrangement used in its characterization. The upper inset shows a THz transient measured with this device. The lower inset shows a SEM image of the device. Reproduced with permission from [56], copyright 2014, American Chemical Society.](/Images/icon/loading.gif)
Fig. 4. Schematic of a single nanowire photoconductive detector geometry and optical arrangement used in its characterization. The upper inset shows a THz transient measured with this device. The lower inset shows a SEM image of the device. Reproduced with permission from [56], copyright 2014, American Chemical Society.
![(a) Normalized luminescence distribution without bias field minus normalized luminescence distributions with bias field from a photoconductive emitter. Dark tones mark a strong field-induced reduction of the luminescence, white: enhancement of the normalized luminescence. Reproduced with permission from [62], copyright 2000, American Institute of Physics. (b) Charge distribution from a Monte Carlo simulation similar to the one presented in [65].](/Images/icon/loading.gif)
Fig. 5. (a) Normalized luminescence distribution without bias field minus normalized luminescence distributions with bias field from a photoconductive emitter. Dark tones mark a strong field-induced reduction of the luminescence, white: enhancement of the normalized luminescence. Reproduced with permission from [62], copyright 2000, American Institute of Physics. (b) Charge distribution from a Monte Carlo simulation similar to the one presented in [65].

Fig. 6. (a) Dipole, (b) bow-tie, and (c) strip-line photoconductive antenna geometries are shown.

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