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Betz AL, Boreiko RT, Sivananthan S, Ashokan R. HgCdTe photoconductive mixers for 2-8 THz. In: Jet Propulsion Laboratory CIit.u.t.e of T, editor. Proc. 12th Int. Symp. Space Terahertz Technol. San Diego, CA, USA; 2001. p. 92–101.
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Siemsen KJ, Bernard JE, Madej AA, Marmet L. Absolute frequency measurement of a CO2/OsO4 stabilized laser at 28.8 THz. Appl Phys B: Lasers and Optics. 2001;72:567–73.
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Eliasson BJ. Metal-insulator-metal diodes for solar energy conversion [Ph.D. thesis].; 2001.
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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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Murk A, Kämpfer N, Wylde R, Inatani J, Manabe T, Seta M. Characterization of various quasi-optical components for the submillimeter limb-sounder SMILES. In: Proc. 12th Int. Symp. Space Terahertz Technol.; 2001. p. 426–35.
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Kasparek W, Fernandez A, Hollmann F, Wacker R. Measurements of ohmic losses of metallic reflectors at 140 GHz using a 3-mirror resonator technique. Int. J. Infrared and Millimeter Waves. 2001;22(11):1695–707.
Abstract: The reflectivity of metallic mirrors in the millimeter wave region does not only depend on the material, but also on the structure and roughness of the surface. We have performed measurements of the reflectivity of various plane and grooved metallic and graphite samples at 140 GHz. The technique is based on the comparison of the quality factor of a 2-mirror reference resonator with the quality factor of a 3-mirror resonator which has identical dimensions and includes the mirror to be tested. After a brief presentation of the theory, the set-up is described and the reflection loss for various aluminium and copper mirrors as well as vacuum compatible materials for applications in thermonuclear fusion experiments are presented and discussed.
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Boreman GD. A Users guide to IR detectors. In: Proc. SPIE. Vol 4420.; 2001. p. 79–90.
Abstract: This paper will guide the first-time user toward proper selection and use of IR detectors for applications in industrial inspection, process control, and laser measurements.
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Codreanu I, Boreman GD. Infrared microstrip dipole antennas. Microw Opt Technol Lett. 2001;29(6):381–3.
Abstract: Abstract 10.1002/mop.1184.abs We report on the successful use of niobium microbolometers coupled to microstrip dipole antennas for the detection of midinfrared radiation. Measurements of the detector response versus antenna length performed at the 10.6 μm wavelength allowed us to identify the first three current-wave resonances along the antenna arms. The detector response was also measured as a function of the radiation wavelength in the 911 μm spectral domain. Excellent agreement between the experimental results and finite-difference time-domain (FDTD) predictions was obtained.
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Puscasu I, Boreman GD. Theoretical and experimental analysis of transmission and enchanced absorption of frequency selective surfaces in the infrared. In: Proc. SPIE. Vol 4293.; 2001. p. 185–90.
Abstract: A comparative study between theory and experiment is presented for transmission through lossy frequency selective surfaces (FSSs) on silicon in the 2 – 15 micrometer range. Important parameters controlling the resonance shape and location are identified: dipole length, spacing, impedance, and dielectric surroundings. Their separate influence is exhibited. The primary resonance mechanism of FSSs is the resonance of the individual metallic patches. There is no discernable resonance arising from a feed-coupled configuration. The real part of the element's impedance controls the minimum value of transmission, while scarcely affecting its location. Varying the imaginary part shifts the location of resonance, while only slightly changing the minimum value of transmission. With such fine-tuning, it is possible to make a good fit between theory and experiment near the dipole resonance on any sample. A fixed choice of impedance can provide a reasonable fit to all samples fabricated under the same conditions. The dielectric surroundings change the resonance wavelength of the FSS compared to its value in air. The presence of FSS on the substrate increases the absorptivity/emissivity of the surface in a resonant way. Such enhancement is shown for dipole and cross arrays at several wavelengths.
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ГОСТ 2.102-68. ЕСКД. Виды и комплектность конструкторских документов.; 2001.
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