Kawamura J, Blundell R, Tong C-YE, Gol'tsman G, Gershenzon E, Voronov B, et al. Phonon-cooled NbN HEB mixers for submillimeter wavelengths. In: Proc. 8th Int. Symp. Space Terahertz Technol.; 1997. p. 23–8.
Abstract: The noise performance of receivers incorporating NbN phonon-cooled superconducting hot electron bolometric mixers is measured from 200 GHz to 900 GHz. The mixer elements are thin-film (thickness — 4 nm) NbN with —5 to 40 pm area fabricated on crystalline quartz sub- strates. The receiver noise temperature from 200 GHz to 900 GHz demonstrates no unexpected degradation with increasing frequency, being roughly TRx ,; 1-2 K The best receiver noise temperatures are 410 K (DSB) at 430 GHz, 483 K at 636 GHz, and 1150 K at 800 GHz.
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Ekstörm H, Kollberg E, Yagoubov P, Gol'tsman G, Gershenzon E, Yngvesson S. Gain and noise bandwidth of NbN hot-electron bolometric mixers. Appl Phys Lett. 1997;70(24):3296–8.
Abstract: We have measured the noise performance and gain bandwidth of 35 Å thin NbN hot-electron mixers integrated with spiral antennas on silicon substrate lenses at 620 GHz. The best double-sideband receiver noise temperature is less than 1300 K with a 3 dB bandwidth of ≈5 GHz. The gain bandwidth is 3.2 GHz. The mixer output noise dominated by thermal fluctuations is 50 K, and the intrinsic conversion gain is about −12 dB. Without mismatch losses and excluding the loss from the beamsplitter, we expect to achieve a receiver noise temperature of less than 700 K.
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Kerr AR, Feldman MJ, Pan S-K. Receiver noise temperature, the quantum noise limit, and zero–point fluctuations. In: Proc. 8th Int. Symp. Space Terahertz Technol.; 1997. p. 101–11.
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de Lange G, Hu Q, Huang H, Lichtenberger AW. Development of a 170-210 GHz 3×3 micromachined SIS imaging array. In: Proc. 8th Int. Symp. Space Terahertz Technol.; 1997. 518.
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Boreman GD. Infrared microantennas. SPIE. 1997;3110:882–5.
Abstract: We present results of mesurments of the polarization response of asymetric spiral antennas coupled Ni-NiO-Ni diodes, over the wavelength range 10.2 to 10.7 μm. The feed structure of the antenna imposes an elliptical polarization singature that is different from the circular polarization expected from a symmetric spiral. We develop a lossy-transmission-line model yielding the measured polarization response. A combination of a balanced and an unbalanced mode is required. Reflected current waves from the arm ends are significant.
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