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Palermo C, Varani L, Vaissière J-C, Millithaler J-F, Starikov E, Shiktorov P, et al. Monte Carlo calculation of diffusion coefficient, noise spectral density and noise temperature in HgCdTe. In: Proc. AIP Conf. Vol 780.; 2005. p. 151–4.
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Kinch MA, Wan C-F Beck J. D. 1/f noise in HgCdTe photodiodes. J. Electron. Mater.. 2005;34(6):928–32.
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Shelkovnikov A, Grain C, Nguyen CT, Butcher RJ, Amy-Klein A, Chardonnet C. 500-Hz two-photon Ramsey fringes with a SF6 beam: towards a new frequency standard in the 30-THz spectral region. Appl Phys B: Lasers and Optics. 2001;73:93–8.
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Semenov A, Il'yin K, Siegel M, Smirnov A, Pavlov S, Richter H, et al. Intermediate frequency bandwidth of a hot-electron mixer: Comparision with bolometric models. In: Proc. 17th Int. Symp. Space Terahertz Technol. Paris, France; 2006. p. 73–6.
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Shitov SV, Inatani J, Shan W-L, Takeda M, Wang Z, Uvarov AV, et al. Measurement of emissivity of the ALMA antenna panel at 840 GHz using NbN-based heterodyne SIS receiver. In: Proc. 19th Int. Symp. Space Terahertz Technol.; 2008. p. 263–6.
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Tol J van, Brunel L-C, Wylde RJ. A quasioptical transient electron spin resonance spectrometer operating at 120 and 240 GHz. Rev Sci Instrum. 2005;76(7):074101 (1 to 8).
Abstract: A new multifrequency quasioptical electron paramagnetic resonance (EPR) spectrometer is described. The superheterodyne design with Schottky diode mixer/detectors enables fast detection with subnanosecond time resolution. Optical access makes it suitable for transient EPR (TR-EPR) at 120 and 240 GHz. These high frequencies allow for an accurate determination of small g-tensor anisotropies as are encountered in excited triplet states of organic molecules like porphyrins and fullerenes. The measured concentration sensitivity for continuous-wave (cw) EPR at 240 GHz and at room temperature without cavity is 1013 spins/cm3 (15 nM) for a 1 mT linewidth and a 1 Hz bandwidth. With a Fabry-Perot cavity and a sample volume of 30 nl, the sensitivity at 240 GHz corresponds to [approximate]3×109 spins for a 1 mT linewidth. The spectrometer's performance is illustrated with applications of transient EPR of excited triplet states of organic molecules, as well as cw EPR of nitroxide reference systems and a thin film of a colossal magnetoresistance material.
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Stucki D, Barreiro C, Fasel S, Gautier J-D, Gay O, Gisin N, et al. Continuous high speed coherent one-way quantum key distribution. Opt Express. 2009;17(16):13326–34.
Abstract: Quantum key distribution (QKD) is the first commercial quantum technology operating at the level of single quanta and is a leading light for quantum-enabled photonic technologies. However, controlling these quantum optical systems in real world environments presents significant challenges. For the first time, we have brought together three key concepts for future QKD systems: a simple high-speed protocol; high performance detection; and integration both, at the component level and for standard fibre network connectivity. The QKD system is capable of continuous and autonomous operation, generating secret keys in real time. Laboratory and field tests were performed and comparisons made with robust InGaAs avalanche photodiodes and superconducting detectors. We report the first real world implementation of a fully functional QKD system over a 43dB-loss (150km) transmission line in the Swisscom fibre optic network where we obtained average real-time distribution rates over 3 hours of 2.5bps.
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An Z, Chen J-C, Ueda T, Komiyama S, Hirakawa K. Infrared phototransistor using capacitively coupled two-dimensional electron gas layers. Appl Phys Lett. 2005;86:172106-3.
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Uzawa Y, Kojima T, Kroug M, Takeda M, Candotti M, Fujii Y, et al. Development of the 787-950 GHz ALMA band 10 cartridge. In: Proc. 20th Int. Symp. Space Terahertz Technol.; 2009. p. 12.
Abstract: We are developing the Atacama Large Millimeter/Submillimeter Array (ALMA) Band 10 (787-950 GHz) receiver cartridge. The incoming beam from the 12-m antenna is reflected by a pair of two ellipsoidal mirrors placed in the cartridge, and then split into two orthogonal polarizations by a free-standing wire-grid. Each beam enters a corrugated feed horn attached to a double-side-band (DSB) mixer block. The mixer uses a full-height waveguide and an NbTiN- or NbN-based superconductor-insulator-superconductor (SIS) mixer chip. We are testing the following three types of mixer chips: 1) Nb SIS junctions + NbTiN/SiO2/Al tuning circuits on a quartz substrate, 2) Nb SIS junctions + NbN/SiO2/Al tuning circuits on an MgO substrate, and 3) NbN SIS junctions + NbN or NbTiN tuning circuits on an MgO substrate. The IF system uses a 4-12-GHz cooled low-noise InP-based MMIC amplifier developed by Caltech. So far, the type 1) has shown the best performance. At LO frequencies from 800 to 940 GHz, the mixer noise temperatures measured by using the standard Y-factor method were below 240 K at an operating physical temperature of 4 K. The lowest noise temperature, 169 K, was obtained at the center frequency of the band 10, as designed. These well-developed technologies will be implemented in the band 10 cartridge to achieve the ALMA specifications.
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Li C-T, Chen T-J, Ni T-L, Lu W-C, Chiu C-P, Chen C-W, et al. Development of SIS mixers for SMA 400-520 GHz band. In: Proc. 20th Int. Symp. Space Terahertz Technol.; 2009. p. 24–30.
Abstract: SIS junction mixers were developed for SMA 400-520 GHz band. The results show receiver noise temperature around 100 K across the band, with noise contribution from RF loss and IF estimated to be around 50 K and 20K, respectively. Two schemes were used to tune out junction's parasitic capacitance. When a parallel inductor is employed, the input impedance is close to Rn, which facilitates impedance matching between the junction and the waveguide probe. Waveguide probes were designed to achieve a low feed-point impedance to match to the junction resistance. Optimum embedding impedances for lower receiver noise temperature were investigated. Performances of two schemes and composition of receiver noise were also discussed.
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