Tol J van, Brunel L-C, Wylde RJ. A quasioptical transient electron spin resonance spectrometer operating at 120 and 240 GHz. Rev Sci Instrum. 2005;76(7):074101 (1 to 8).
Abstract: A new multifrequency quasioptical electron paramagnetic resonance (EPR) spectrometer is described. The superheterodyne design with Schottky diode mixer/detectors enables fast detection with subnanosecond time resolution. Optical access makes it suitable for transient EPR (TR-EPR) at 120 and 240 GHz. These high frequencies allow for an accurate determination of small g-tensor anisotropies as are encountered in excited triplet states of organic molecules like porphyrins and fullerenes. The measured concentration sensitivity for continuous-wave (cw) EPR at 240 GHz and at room temperature without cavity is 1013 spins/cm3 (15 nM) for a 1 mT linewidth and a 1 Hz bandwidth. With a Fabry-Perot cavity and a sample volume of 30 nl, the sensitivity at 240 GHz corresponds to [approximate]3×109 spins for a 1 mT linewidth. The spectrometer's performance is illustrated with applications of transient EPR of excited triplet states of organic molecules, as well as cw EPR of nitroxide reference systems and a thin film of a colossal magnetoresistance material.
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de Graauw T, Caux E, Guesten R, Helmich F, Pearson J, Phillips TG, et al. The Herschel-heterodyne instrument for the far-infrared (HIFI). In: Bulletin of the American Astronomical Society.; 2005. 1219. (Bulletin of the American Astronomical Society; vol 37).
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Cherednichenko S, Kollberg E, Angelov I, Drakinskiy V, Berg T, Merkel H. Effect of the direct detection effect on the HEB receiver sensitivity calibration. In: Proc. 16th Int. Symp. Space Terahertz Technol. Göteborg, Sweden; 2005. p. 235–9.
Abstract: We analyze the scale of the HEB receiver sensitivity calibration error caused by the so called “direct detection effect”. The effect comes from changing of the HEB parameters when whey face the calibration loads of different temperatures. We found that for HIFI Band 6 mixers (Herschel Space Observatory) the noise temperature error is of the order of 8% for 300K/77K loads (lab receiver) and 2.5% for 100K/10K loads (in HIFI). Using different approach we also predict that with an isolator between the mixer and the low noise amplifiers the error can be much smaller.
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Karpov A, Miller D, Stern JA, Bumble B, LeDuc HG, Zmuidzinas J. Low noise NbTiN 1.25 THz SIS mixer for Herschel Space Observatory. In: Proc. 16th Int. Symp. Space Terahertz Technol. Göteborg, Sweden; 2005. 450.
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Marrone DP, Raymond Blundell, Edward Tong, Paine SN, Denis Loudkov, Jonathan Kawamura, et al. Observations in the 1.3 and 1.5 THz atmospheric windows with the Receiver Lab Telescope. In: Proc. 16th Int. Symp. Space Terahertz Technol. Göteborg, Sweden; 2005. p. 64–7.
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