2016
DOI: 10.1126/sciadv.1600190
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Noninvasive, near-field terahertz imaging of hidden objects using a single-pixel detector

Abstract: Terahertz imaging for noninvasive measurements.

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Cited by 399 publications
(248 citation statements)
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“…24 These systems, in fact, exhibit complex transmission properties that cannot be easily interpreted using a time-independent, intensity-based analysis, which constitutes the standard methodology available today. 25 Despite the large body of research in this field, however, one of the practical challenges in implementing field-sensitive THz GI lies in the realization of controllable structured light. 26,27 Spatial-light-modulator (SLM) devices, which are readily accessible at optical frequencies, cannot be easily extended to the THz domain.…”
mentioning
confidence: 99%
“…24 These systems, in fact, exhibit complex transmission properties that cannot be easily interpreted using a time-independent, intensity-based analysis, which constitutes the standard methodology available today. 25 Despite the large body of research in this field, however, one of the practical challenges in implementing field-sensitive THz GI lies in the realization of controllable structured light. 26,27 Spatial-light-modulator (SLM) devices, which are readily accessible at optical frequencies, cannot be easily extended to the THz domain.…”
mentioning
confidence: 99%
“…Near-field THz microscopy has seen tremendous progress over recent years towards very high spatial resolutions [21][22][23][24], and has previously been employed in many successful implementations to explore near-field dynamics in both resonant structures [18,25,26] and apertures [27][28][29][30][31]. In the work of Bitzer et al [25], lattice modes were investigated for the case of split ring resonators (SRR), where the array was shown to hybridize lattice modes with magnetic dipole resonances.…”
Section: Resultsmentioning
confidence: 99%
“…36 However, single apertures and scatterers produce tiny signals due to their small size with respect to the THz wavelength. 37 To achieve optimum signal-to-noise, we therefore pattern our photoexcitation beam into binary intensity masks derived from Hadamard matrices, 37,38 as explicitly described in ref (37) and in the Supporting Information. Knowledge of the masking patterns and the corresponding far-field detector readout is combined to obtain an image of the THz photoconductivity of the object, our CVD graphene sample.…”
mentioning
confidence: 99%