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Palermo, C., Varani, L., Vaissière, J. - C., Millithaler, J. - F., Starikov, E., Shiktorov, P., et al. (2005). Monte Carlo calculation of diffusion coefficient, noise spectral density and noise temperature in HgCdTe. In Proc. AIP Conf. (Vol. 780, pp. 151–154).
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Colombelli, R. (2002). FIR quantum cascade lasers at λ>20 μm and THz emitters at λ=80 μm. Phys. E: Low-dimensional Systems and Nanostructures, 13(2-4), 848–853.
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Matsushima, F., Odashima, H., Iwasaki, T., Tsunekawa, S., & Takagi, K. (1994). Frequency measurement of pure rotational transitions of H2O from 0.5 to 5 THz. In Conference on precision electromagnetic measurements digest (pp. 23–24).
Abstract: Frequencies of H2O pure rotational transitions from 0.5 to 5 THz have been measured with an accuracy of one part in 109 using a tunable far-infrared spectrometer. Measured frequencies of more than a hundred spectral lines provide an excellent wavelength and frequency calibration standard for the far infrared.
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Benford, D. J., Moseley, S. H., & Chervenak, J. A. (2002). Mission requirements for ultralow-background, large format bolometer arrays. In Proc. Far-Infrared Submillimeter, & Millimeter Detector Workshop. Monterey, California.
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Vystavkin, A. N. (1999). Estimation of noise equivalent power and design analysis of an andreev reflection hot-electron microbolometer for submillimeter radioastronomy. Rus. J. Radio Electron., (10).
Abstract: Results of theoretical estimations and measurements of characteristics of an Andreev reflection hot-electron microbolometer for submillimeter radioastronomy made by different researchers are reviewed and analysed. Peculiarities and characteristics of the microbolometers using two types of microthermometer for measurement of the electron temperature increment under influence of the radiation: the SIN-junction and the transition-edge sensor (TES) with electrothermal feedback – are compared. Advantages of the microbolometer with the second type of the microthermometer when the TES is used simultaneously as the absorber of radiation are shown. Methods of achievement of the best noise equivalent power of the microbolometer in such version as well as methods of the matching the microbolometer with the incident radiation flow using planar antennas and with the channel of output signal measurement using a SQUID-picoammeter are considered.
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