Abstract:A clever way to simulate numerical matched loads is presented and applied in the mathematical framework of the moment method. This approach presents a lot of advantages with regard to other numerical matched load simulations, and could be used whateier the shape of the planar circuit without the help of the characteristic impedance concept. Results show that very good efficiency is obtained for the reflection coefficient of such matched loads. Typical results are exhibited for S‐parameter determination of mult… Show more
“…The determinaton of Qp is performed by considering the loaded quality factor of a perfect shielded resonator (CCE), with no substrate and radiation losses, connected to the measurements ports throught coupling gaps. Both ports have been in this numerical experience matched with the help of numerical matched loads, as described in [8].…”
mentioning
confidence: 99%
“…This equivalent surface impedance of the strip may be accurately derived from the numerical determination of the electromagnetic field within the strip with a point matching technique [61, and may be written throught the use of geometrical weighting factors kr and ki [7]:' Zseq = kr Rs + jki Xs (2) where Rs and Xs are respectively the real and imaginary parts of the classical surface impedance [8]:…”
This paper presents a large investigation on the microwave properties of a high;Tc YBaiCuO superconducting thin film and, for the first time, meets in a global and comparative approach determination of the complex Conductivity cr-from a transmission measurement, experimental study on linear mmicrostrip resonators and Spectral Domain Approach (SDA) baWEd computations of quality factors and resonance frequencies.Sample characteristics The high Tc superconducting thin film (3.000A) considered in this study was deposited by pulsed laser ablation technique [1] on MgO substrate (250pm). X-ray diffraction analysis performed on the sample revealed a predominantly c-axis orientation of the film and the DC transition temperature (Tc,R=OtTcJC was 87K.Measurement of the complex conductivity The sample has been characterized with a transmission measurement's technique [2][3]. The sample is clamped between two rectangular waveguides working in the 18-26 GHz frequency range and the microwave power transmitted through the film and the substrate is determined. The measurements of the amplitude Tr and the phase + of the S21 transmitted coefficient were carried out betwetn 3OQK and 30K With-a HPS51OB network analyser coupled to,a liquid helium cryostat. From t and + (figure 1), it is possible to extract, without the help of any ph&omenological model, the complex conductivity a*=a1Ijcr2 (figure 2). The calculation takes into account the multiple reflections in the substrate.
“…The determinaton of Qp is performed by considering the loaded quality factor of a perfect shielded resonator (CCE), with no substrate and radiation losses, connected to the measurements ports throught coupling gaps. Both ports have been in this numerical experience matched with the help of numerical matched loads, as described in [8].…”
mentioning
confidence: 99%
“…This equivalent surface impedance of the strip may be accurately derived from the numerical determination of the electromagnetic field within the strip with a point matching technique [61, and may be written throught the use of geometrical weighting factors kr and ki [7]:' Zseq = kr Rs + jki Xs (2) where Rs and Xs are respectively the real and imaginary parts of the classical surface impedance [8]:…”
This paper presents a large investigation on the microwave properties of a high;Tc YBaiCuO superconducting thin film and, for the first time, meets in a global and comparative approach determination of the complex Conductivity cr-from a transmission measurement, experimental study on linear mmicrostrip resonators and Spectral Domain Approach (SDA) baWEd computations of quality factors and resonance frequencies.Sample characteristics The high Tc superconducting thin film (3.000A) considered in this study was deposited by pulsed laser ablation technique [1] on MgO substrate (250pm). X-ray diffraction analysis performed on the sample revealed a predominantly c-axis orientation of the film and the DC transition temperature (Tc,R=OtTcJC was 87K.Measurement of the complex conductivity The sample has been characterized with a transmission measurement's technique [2][3]. The sample is clamped between two rectangular waveguides working in the 18-26 GHz frequency range and the microwave power transmitted through the film and the substrate is determined. The measurements of the amplitude Tr and the phase + of the S21 transmitted coefficient were carried out betwetn 3OQK and 30K With-a HPS51OB network analyser coupled to,a liquid helium cryostat. From t and + (figure 1), it is possible to extract, without the help of any ph&omenological model, the complex conductivity a*=a1Ijcr2 (figure 2). The calculation takes into account the multiple reflections in the substrate.
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