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Colombelli R. FIR quantum cascade lasers at λ>20 μm and THz emitters at λ=80 μm. Phys. E: Low-dimensional Systems and Nanostructures. 2002;13(2-4):848–53.
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Smolyaninov II, Zayats AV, Stanishevsky A, Davis CC. Optical control of photon tunneling through an array of nanometer-scale cylindrical channels. Phys Rev B. 2002;66(20):205414_1–5.
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Semenov AD, Gol'tsman GN, Sobolewski R. Hot-electron effect in superconductors and its applications for radiation sensors. Supercond Sci Technol. 2002;15(4):R1–R16.
Abstract: The paper reviews the main aspects of nonequilibrium hot-electron phenomena in superconductors and various theoretical models developed to describe the hot-electron effect. We discuss implementation of the hot-electron avalanche mechanism in superconducting radiation sensors and present the most successful practical devices, such as terahertz mixers and direct intensity detectors, for far-infrared radiation. Our presentation also includes the novel approach to hot-electron quantum detection implemented in superconducting x-ray to optical photon counters.
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Uzawa Y, Miki S, Wang Z, Kawakami A, Kroug M, Yagoubov P, et al. Performance of a quasi-optical NbN hot-electron bolometric mixer at terahertz frequencies. Supercond Sci Technol. 2002;15(1):141–5.
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Lipatov A, Okunev O, Smirnov K, Chulkova G, Korneev A, Kouminov P, et al. An ultrafast NbN hot-electron single-photon detector for electronic applications. Supercond Sci Technol. 2002;15(12):1689–92.
Abstract: We present the latest generation of our superconducting single-photon detector (SPD), which can work from ultraviolet to mid-infrared optical radiation wavelengths. The detector combines a high speed of operation and low jitter with high quantum efficiency (QE) and very low dark count level. The technology enhancement allows us to produce ultrathin (3.5 nm thick) structures that demonstrate QE hundreds of times better, at 1.55 μm, than previous 10 nm thick SPDs. The best, 10 × 10 μm2, SPDs demonstrate QE up to 5% at 1.55 μm and up to 11% at 0.86 μm. The intrinsic detector QE, normalized to the film absorption coefficient, reaches 100% at bias currents above 0.9 Ic for photons with wavelengths shorter than 1.3 μm.
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