2014
DOI: 10.1063/1.4863671
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Imaging of free carriers in semiconductors via optical feedback in terahertz quantum cascade lasers

Abstract: To monitor the density of photo-generated charge carriers on a semiconductor surface, we demonstrate a detectorless imaging system based on the analysis of the optical feedback in terahertz quantum cascade lasers. Photo-excited free electron carriers are created in high resistivity n-type silicon wafers via low power (≅40 mW/cm2) continuous wave pump laser in the near infrared spectral range. A spatial light modulator allows to directly reconfigure and control the photo-patterned intensity and the associated f… Show more

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Cited by 39 publications
(22 citation statements)
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“…The inherent stability of QCLs against optical feedback [16] has been recently exploited in a number of self-mixing interferometry (SMI) configurations, providing an interesting method to control the emission of THz QCLs by reconfigurable photo-generated anisotropic metamaterials [17], to trace the free carrier distribution in a semiconductor target [18], and to map the real and imaginary refractive index of polymeric materials [12], for example.…”
Section: The General Concept Of Sd-s-snommentioning
confidence: 99%
“…The inherent stability of QCLs against optical feedback [16] has been recently exploited in a number of self-mixing interferometry (SMI) configurations, providing an interesting method to control the emission of THz QCLs by reconfigurable photo-generated anisotropic metamaterials [17], to trace the free carrier distribution in a semiconductor target [18], and to map the real and imaginary refractive index of polymeric materials [12], for example.…”
Section: The General Concept Of Sd-s-snommentioning
confidence: 99%
“…Self-mixing interferometry in QCLs has recently shown a strong potential in different configurations, ranging from near field imaging with sub-wavelength spatial resolution (1 -7 m), 38 to the control of the emission of THz QCLs 39 and the detection of free carrier distribution in semiconductors. 40 In our optical setup (Fig 3a) the 2.7 THz radiation emitted by a QCL is collected by a parabolic mirror (p1), directed to a couple of flat mirrors (m1 (moveable with a motorized stage) and m2 (fixed)) and finally focused at the apex of a Pt AFM tip by a second parabolic mirror (p2). The tip is positioned in close proximity to the surface of the sample and is dithered at Ω = 20 KHz (i.e.…”
Section: Detector-less Thz S-snom Microscopymentioning
confidence: 99%
“…The principle of the spatial filter is similar as in the research by Minoni et al 18 Due to the stationary pinhole, the filtering is more effective at longer wavelengths, since its diameter was selected according to the diffraction limited spot size of the 933-nm beam of the IR diode laser, which has initially a distorted, elliptical beam profile caused by the spatial free carrier density distribution and the rectangular-shaped junction. 19,20 In the ultraviolet region, the filtering is not as good as in IR but sufficient since the beam profiles are good naturally. Also the beams are not attenuated much, which provides better signal-to-noise ratios.…”
Section: Design Of the High-resolution Measurement Setupmentioning
confidence: 99%