2013
DOI: 10.1007/s10762-013-9977-3
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Saturation and Polarization Characteristics of 1.56 μm Optical Probe Pulses in a LTG-GaAs Photoconductive Antenna Terahertz Detector

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Cited by 9 publications
(7 citation statements)
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“…Figure 5(c) demonstrates that the amplitude increases linearly as the probe power is raised from 5 mW to 20 mW. But after that, the amplitude turns to saturation when the probe beam power continues to rise414243.…”
Section: Resultsmentioning
confidence: 95%
“…Figure 5(c) demonstrates that the amplitude increases linearly as the probe power is raised from 5 mW to 20 mW. But after that, the amplitude turns to saturation when the probe beam power continues to rise414243.…”
Section: Resultsmentioning
confidence: 95%
“…For the optimization of the device, it is important to clarify the mechanism of the nonlinearity. For example, the order of the nonlinearity reported so far scatters in a range between 1 and 2 [1][2][3][4][5]. The ill-defined nonlinearity was explained qualitatively by a two-step absorption via the mid-gap states combined with the intraband transition [3].…”
Section: Introductionmentioning
confidence: 90%
“…THz time‐domain‐spectroscopy (TDS) system based on emitters and detectors made from moderately annealed LTG GaAs and activated with femtosecond Yb:KGW laser pulses ( λ = 1030 nm) was demonstrated by us in Ref. ; while the other groups examined LTG GaAs photoconductive antennas operation as THz detectors and emitters activated with 1.5 µm laser pulses.…”
Section: Introductionmentioning
confidence: 99%