2017
DOI: 10.1364/optica.4.001358
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Solid-state-biased coherent detection of ultra-broadband terahertz pulses

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Cited by 32 publications
(26 citation statements)
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“…This way, we are able to provide a fair comparison between the results achieved in the two configurations. In order to demonstrate the validity of Equations (4) and (5), we placed the SSBCD device at the detection position of an ultra-broadband THz Time-Domain Spectroscopy setup [ 29 ], featuring a two-color plasma source fed by a 150 fs, 800 nm, 1 kHz, 1.3 mJ pulsed laser. Such a source emitted ~10-THz-wide single-cycle pulses with a peak amplitude of = 170 kV/cm, measured via electro-optic sampling in a 200-µm-thick GaP crystal [ 33 ], in a nitrogen-purged atmosphere.…”
Section: Resultsmentioning
confidence: 99%
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“…This way, we are able to provide a fair comparison between the results achieved in the two configurations. In order to demonstrate the validity of Equations (4) and (5), we placed the SSBCD device at the detection position of an ultra-broadband THz Time-Domain Spectroscopy setup [ 29 ], featuring a two-color plasma source fed by a 150 fs, 800 nm, 1 kHz, 1.3 mJ pulsed laser. Such a source emitted ~10-THz-wide single-cycle pulses with a peak amplitude of = 170 kV/cm, measured via electro-optic sampling in a 200-µm-thick GaP crystal [ 33 ], in a nitrogen-purged atmosphere.…”
Section: Resultsmentioning
confidence: 99%
“…The SSBCD technique has been extensively discussed in Refs [ 29 , 30 ]. For the sake of completeness, here we recall that the SSBCD method exploits the TFISH mechanism to sense THz radiation [ 31 ].…”
Section: Ssbcd Device Working Principlementioning
confidence: 99%
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“…parabolic mirror (see Figure S6 in the Supporting Information). [ 64 ] As for the previous case, Figure a depicts the experimental temporal waveforms recorded at the TTWWG input ( E in ) and output ( E out ), whereas Figure 5b shows their corresponding spectra. We note that the TTWWG spectrum is once again strongly enhanced in the low‐frequency range, as stated by the ≈1 THz redshift experienced by the peak frequency, compared to the air case.…”
Section: Experimental and Simulation Resultsmentioning
confidence: 99%
“…For the ⊥ geometry, the non-resonant contribution was only distinguishable for Δυ= 3.8 THz. When the non-resonant contribution was significant, we fit the data with a function that was the sum of two contributions: a Gaussian, which accounts for the instantaneous processes at sans-serifΔt = 0 ps, corresponding to the signal commonly considered in THz field-induced SHG (TFISH) [23,24,25,26,27], and a single-exponential decay, whose decay time τ represents the relaxation time of the non-resonant term. The resulting fit functions of this ‘non-resonant’ part of the THYR signal are reported as red solid curve in Figure 6a,c.…”
Section: Discussionmentioning
confidence: 99%