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Mann, C. M., Matheson, D. N., Ellison, B. N., Oldfield, M. L., Moyna, B. P., Spencer, J. J., et al. (1998). On the design and measurement of a 2.5 THz waveguide mixer. In Proc. 9th Int. Symp. Space Terahertz Technol. (161).
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Chouvaev, D., Kuzmin, L., Tarasov, M., Sundquist, P., Willander, M., & Claeson, T. (1998). Normal metal hot-electron microbolometer with Andreev mirrors for THz space applications. In Proc. 9th Int. Symp. Space Terahertz Technol. (pp. 331–335).
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Tetsu Suzuki, Chris Mann, Takanari Yasui, Hirotomo Fujishima, & Koji Mizuno. (1998). Quasi–integrated planar Schottky barrier diodes for 2.5 THz receivers. In Proc. 9th Int. Symp. Space Terahertz Technol. (187).
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Maddison, B. J., Martin, R. J., Oldfield, M. L., Mann, C. M., Matheson, D. N., Ellison, B. N., et al. (1998). A compact 500 GHz planar schottky siode receiver with a wide instantaneous bandwidth. In Proc. 9th Int. Symp. Space Terahertz Technol. (367).
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Brown, R. L. (1998). Technical specification of the Millimeter Array. In T. G. Phillips (Ed.), Proc. SPIE, Advanced Technology MMW, Radio, and Terahertz Telescopes, vol. 3357 (pp. 231–237).
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Dahl, H., Metz, H. J., & Wriedt, T. (1998). Light scattering of silver halide crystals. In Proc. 3rd Workshop on Electromagnetic and Light Scattering (pp. 51–58). Universität Bremen.
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Floet, D. W., Baselmans, J. J. A., Klapwijk, T. M., & Gao, J. R. (1998). Resistive transition of niobium superconducting hot-electron bolometer mixers. Appl. Phys. Lett., 73(19), 2826.
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Burke, P. J., Schoelkopf, R. J., Prober, D. E., Skalare, A., Karasik, B. S., Gaidis, M. C., et al. (1998). Spectrum of thermal fluctuation noise in diffusion and phonon cooled hot-electron mixers. Appl. Phys. Lett., 72(12), 1516–1518.
Abstract: A systematic study of the intermediate frequency noise bandwidth of Nb thin-film superconducting hot-electron bolometers is presented. We have measured the spectrum of the output noise as well as the conversion efficiency over a very broad intermediate frequency range (from 0.1 to 7.5 GHz) for devices varying in length from 0.08 μm to 3 μm. Local oscillator and rf signals from 8 to 40 GHz were used. For a device of a given length, the spectrum of the output noise and the conversion efficiency behave similarly for intermediate frequencies less than the gain bandwidth, in accordance with a simple thermal model for both the mixing and thermal fluctuation noise. For higher intermediate frequencies the conversion efficiency decreases; in contrast, the noise decreases but has a second contribution which dominates at higher frequency. The noise bandwidth is larger than the gain bandwidth, and the mixer noise is low, between 120 and 530 K (double side band).
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Kawamura, J., Blundell, R., Tong, C. - Y. E., Papa, D. C., Hunter, T. R., Gol'tsman, G., et al. (1998). First light with an 800 GHz phonon-cooled HEB mixer receiver. In Proc. 9th Int. Symp. Space Terahertz Technol. (pp. 35–43). Pasadena, California, USA.
Abstract: Phonon-cooled superconductive hot-electron bolometric (HEB) mixers are incorporated in a waveguide receiver designed to operate near 800 Gliz. The mixer elements are thin-film nio- bium nitride microbridges with dimensions of 4 nm thickness, 0.2 to 0.3 p.m in length and 2 jun in width. At 780 GHz the best receiver noise temperature is 840 K (DSB). The mixer IF bandwidth is 2.0 GHz, the absorbed LO power is —0.1 1.1W. A fixed-tuned version of the re- ceiver was installed at the Submillimeter Telescope Observatory on Mt. Graham, Arizona, to conduct astronomical observations. These observations represent the first time that a receiver incorporating any superconducting HEB mixer has been used to detect a spectral line of celes- tial origin.
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Il’in, K. S., Ptitsina, N. G., Sergeev, A. V., Gol’tsman, G. N., Gershenzon, E. M., Karasik, B. S., et al. (1998). Interrelation of resistivity and inelastic electron-phonon scattering rate in impure NbC films. Phys. Rev. B, 57(24), 15623–15628.
Abstract: A complex study of the electron-phonon interaction in thin NbC films with electron mean free path l=2–13nm gives strong evidence that electron scattering is significantly modified due to the interference between electron-phonon and elastic electron scattering from impurities. The interference T2 term, which is proportional to the residual resistivity, dominates over the Bloch-Grüneisen contribution to resistivity at low temperatures up to 60 K. The electron energy relaxation rate is directly measured via the relaxation of hot electrons heated by modulated electromagnetic radiation. In the temperature range 1.5–10 K the relaxation rate shows a weak dependence on the electron mean free path and strong temperature dependence ∼Tn, with the exponent n=2.5–3. This behavior is explained well by the theory of the electron-phonon-impurity interference taking into account the electron coupling with transverse phonons determined from the resistivity data.
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