2008
DOI: 10.1063/1.2988896
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Terahertz heterodyne receiver with quantum cascade laser and hot electron bolometer mixer in a pulse tube cooler

Abstract: A liquid cryogen-free terahertz heterodyne receiver in a pulse tube cooler has been realized. The receiver operates at 2.5 THz. It is based on a quantum cascade laser (QCL) as local oscillator and a hot electron bolometric mixer. A detailed study of the QCL beam quality yielded a beam propagation factor of 1.1-1.2. The double sideband noise temperature of the system is 2000 K and when corrected for optical losses in the signal path it is similar to 800 K. (C) 2008 American Institute of Physics

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Cited by 71 publications
(30 citation statements)
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“…Emission is then highly polarized, as both the selection rules of the intersubband transitions and the surface-plasmon waveguide design strongly select only TM polarization for lasing. Even if they require cooling to low temperatures, this can easily be achieved by low vibration, cryogen-free devices, like pulse tube and Sterling coolers [16,17]. This is a crucial aspect as it allows the deployment of a self-contained compact source weighing less than 15 kg overall, with a total power consumption of no more than 240 W, requiring no further connections beyond the electrical one, and producing a reasonably Gaussian collimated beam with no external optics [17].…”
Section: Beamshapementioning
confidence: 99%
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“…Emission is then highly polarized, as both the selection rules of the intersubband transitions and the surface-plasmon waveguide design strongly select only TM polarization for lasing. Even if they require cooling to low temperatures, this can easily be achieved by low vibration, cryogen-free devices, like pulse tube and Sterling coolers [16,17]. This is a crucial aspect as it allows the deployment of a self-contained compact source weighing less than 15 kg overall, with a total power consumption of no more than 240 W, requiring no further connections beyond the electrical one, and producing a reasonably Gaussian collimated beam with no external optics [17].…”
Section: Beamshapementioning
confidence: 99%
“…In ref. [16] the M2 of a 2.5 THz laser was determined by measuring the beam profile scanning a Golay cell detector with a 0.4-mm diameter aperture in a plane orthogonal to the emission direction of the QCL at different positions in front and behind the position of the beam On the other side, as mentioned previously, double-metal waveguides allow the highest operating temperatures and also represent by far the best choice for frequencies below 2 THz. From an application point of view, though, such strong sub-wavelength waveguides radiate into the entire semi-sphere above the device, more similar to an antenna than to a conventional semiconductor ridge waveguide, and often present very irregular profiles.…”
Section: Beamshapementioning
confidence: 99%
“…In the free running mode, the observed low frequency fluctuations and drift in the lock-in signal are a result of the frequency noise of the laser due to external contributions mainly from the temperature variations of the cryocooler. The contribution of the cryocooler also induces amplitude instability, 15 reflected by the fluctuations of the HEB mixer current and of the IF output power. In the second operating mode when the frequency stabilization loop is enabled, the lock-in signal becomes well stabilized and is maintained at the set point of zero, which implies that the QCL frequency is fully stabilized.…”
Section: -mentioning
confidence: 99%
“…Owing to the reduced overlap of the waveguide mode with doped semiconductor and metallic layers, the SP waveguide exhibits lower waveguide losses compared to MM waveguides. More significantly, though, is the far superior beam quality and lower beam divergence demonstrated [38]. The majority of THz QCLbased systems developed to date have consequently employed the SP waveguide .…”
Section: Introductionmentioning
confidence: 99%