By Watatani Y.
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The TT2-111-series measurements presented herein were done on a batch with a stated DC resistivity of 435 Ωm, which we designate “TT2-111V” (the manufacturer’s designation for all varieties is TT2-111R). 50 Ωm). 9 mm) for each material, with liquid metal filling the gaps. In almost all cases, different samples of the same material were machined from the same piece. We tried to choose the sample length d to minimise the error in our µ and values. We followed the usual strategy for choosing d, a rationalisation for which can be found elsewhere [30].
13a more directly, but none of them are available with AMOS yet. 13. An HOM load with the ferrite layer protruding inward, (a) with a straight beam pipe and (b) with a tapered beam pipe. In (b), the inner diameter of the ferrite is the same as that of the end pipes. 5). As Re Zm goes through its maximum, Im Zm goes through zero. 5 GHz, but there is some discrepancy between the AMOS and analytic predictions for Z1 . 5 GHz. As we will now see, this feature can be understood via a simplified coupling impedance model, which we will derive in this section.
Similar agreement between repeated measurements on a longer sample was also seen. This suggests that the reproducibility problems stem mostly from variation in the properties or the machining from one sample to another. Kramers-Kronig Relations The electric field and the electric polarisation must both be real-valued functions in the time domain. With the additional requirement that the relationship between these two quantities be causal, one can obtain constraints on the complex permittivity, the so-called Kramers-Kronig relations (see [38], for example).