DEVICE FOR MEASURING PROPERTIES OF HIGH-TEMPERATURE SUPERCONDUCTORS IN ELECTROMAGNETIC FIELDS

摘要

the invention u043eu0442u043du043eu0441u0438u0442u0441u00a0 to measuring technology. the purpose of u0438u0437u043eu0431u0440u0435u0442u0435u043du0438u00a0 - improve the accuracy and sensitivity of measurements. in the disc u0434u0438u044du043bu0435u043au0442u0440u0438u0447u0435u0441u043au043eu043c u0440u0435u0437u043eu043du0430u0442u043eu0440u0435 1 u0432u043eu0437u0431u0443u0436u0434u0430u0435u0442u0441u00a0 u0432u043eu043bu043du043eu0432u043eu0434u043eu043c 4 u0441u0442u043eu00a0u0447u0430u00a0 wave type u0448u0435u043fu0447u0443u0449u0435u0439 gallery, u043eu0431u0440u0430u0437u043eu0432u0430u043du043du0430u00a0 overlaid waves falling on the metal with u0435u0440u043au0430u043bu043e 2 and a sample 3 and a reflected from them.due to the localization of u043fu043eu043bu00a0 waves of this type with the cylindrical boundary section u0434u0438u044du043bu0435u043au0442u0440u0438u043au0430 and external environment u043fu00a0u0442u043du043e u043fu043eu043bu00a0 model 3 has the dimensions of length in u043fu043eu0440u00a0u0434u043au0430 u043bu043du044b in u0434u0438u044du043bu0435u043au0442u0440u0438u043au0435. this u043fu043eu0437u0432u043eu043bu00a0u0435u0442 to structural u0438u0437u043cu0435u0440u0435u043du0438u00a0 samples 3 of high temperature superconductors locally on their surface by u0441u043au0430u043du0438u0440u043eu0432u0430u043du0438u00a0 u043fu00a0u0442u043du0430 u043fu043eu043bu00a0 in per u0435u043cu0435u0449u0435u043du0438u0438 model 3.u0434u043bu00a0 u0432u043eu0437u0431u0443u0436u0434u0435u043du0438u00a0 fluctuations in u0440u0435u0437u043eu043du0430u0442u043eu0440u0435 1, in the case of u0430u043du0438u0437u043eu0442u0440u043eu043fu043du043eu0433u043e u0432u044bu043fu043eu043bu043du0435u043du0438u00a0 crystal u043bu0435u0439u043au043eu0441u0430u043fu0444u0438u0440u0430 sector to cut the central angle 180 & deg; christ all must be designed so that it u043eu043fu0442u0438u0447u0435u0441u043au0430u00a0 axis was parallel to u043eu0441u043du043eu0432u0430u043du0438u00a0u043c resonator 1 and the surface of the u0441u0435u043au0442u043eu0440u043du043eu0433u043e u0441u0435u0447u0435u043du0438u00a0, 1 z. s - lu, 2). (l, c