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BS EN IEC 61788-7:2020

$189.07

Superconductivity – Electronic characteristic measurements. Surface resistance of high-temperature superconductors at microwave frequencies

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BSI 2020 50
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IEC 61788-7:2020 is available as IEC 61788-7:2020 RLV which contains the International Standard and its Redline version, showing all changes of the technical content compared to the previous edition.IEC 61788-7:2020 describes measurement of the surface resistance (Rs) of superconductors at microwave frequencies by the standard two-resonator method. The object of measurement is the temperature dependence of Rs at the resonant frequency. The applicable measurement range of Rs for this method is as follows: – Frequency: 8 GHz < f < 30 GHz – Measurement resolution: 0,01 m ? at 10 GHz The Rs data at the measured frequency, and that scaled to 10 GHz, assuming the f 2 rule for comparison, is reported. This third edition cancels and replaces the second edition, published in 2006. This edition constitutes a technical revision. This edition includes the following significant technical changes with respect to the previous edition: a) informative Annex B, relative combined standard uncertainty for surface resistance measurement has been added; b) precision and accuracy statements have been converted to uncertainty; c) reproducibility in surface resistant measurement has been added.

PDF Catalog

PDF Pages PDF Title
2 undefined
5 Annex ZA(normative)Normative references to international publicationswith their corresponding European publications
7 English
CONTENTS
10 FOREWORD
12 INTRODUCTION
13 1 Scope
2 Normative references
3 Terms and definitions
4 Requirements
14 5 Apparatus
5.1 Measurement system
Figure 1 – Schematic diagram of measurement system for temperature dependence of Rs using a cryocooler
15 5.2 Measurement apparatus for Rs
Figures
16 Figure 2 – Typical measurement apparatus for Rs
17 5.3 Dielectric rods
6 Measurement procedure
6.1 Specimen preparation
Table 1 – Typical dimensions of pairs of single-crystal sapphire rods for 12 GHz, 18 GHz and 22 GHz
18 6.2 Set-up
6.3 Measurement of reference level
Tables
Table 2 – Dimensions of superconductor film for 12 GHz, 18 GHz, and 22 GHz
19 6.4 Measurement of the frequency response of resonators
Figure 3 – Insertion attenuation, IA, resonant frequency, f0, and half power bandwidth, Δf, measured at T kelvin
21 6.5 Determination of surface resistance of the superconductor and ε′ and tan δ of the standard sapphire rods
Figure 4 – Reflection scattering parameters (S11 and S22)
22 7 Uncertainty of the test method
7.1 Surface resistance
Table 3 – Specifications for vector network analyzer
Table 4 – Specifications for sapphire rods
23 7.2 Temperature
7.3 Specimen and holder support structure
Figure 5 – Term definitions in Table 4
24 7.4 Specimen protection
7.5 Uncertainty of surface resistance measured by standard two-resonator method
8 Test report
8.1 Identification of test specimen
8.2 Report of Rs values
8.3 Report of test conditions
25 Annex A (informative) Additional information relating to Clauses 1 to 8
A.1 Scope
A.1.1 General
A.1.2 Cylindrical cavity method [10] [17]
A.1.3 Parallel-plates resonator method [18] [19]
A.1.4 Microstrip-line resonance method [20] [21]
A.1.5 Dielectric resonator method [22] [23] [24] [25]
26 A.1.6 Image-type dielectric resonator method [26] [27]
Figure A.1 – Schematic configuration of several measurement methods for the surface resistance
27 A.1.7 Two-resonator method [28] [29]
A.2 Requirements
A.3 Theory and calculation equations
28 Figure A.2 – Configuration of a cylindrical dielectric rod resonator short-circuited at both ends by two parallel superconductor films deposited on dielectric substrates
29 Figure A.3 – Computed results of the u-v and W-v relations for TE01p mode
30 A.4 Apparatus
Figure A.4 – Configuration of standard dielectric rods for measurement of Rs and tan δ
31 A.5 Dimensions of the standard sapphire rods
Figure A.5 – Three types of dielectric resonators
32 Figure A.6 – Mode chart to design TE011 resonator short-circuited at both ends by parallel superconductor films [28]
33 A.6 Dimension of the closed type resonator
Figure A.7 – Mode chart to design TE013 resonator short-circuited at both ends by parallel superconductor films [28]
34 Figure A.8 – Mode chart for TE011 closed-type resonator [28]
35 A.7 Sapphire rod reproducibility
A.8 Test results
Figure A.9 – Mode chart for TE013 closed-type resonator [28]
36 A.9 Reproducibility of measurement method
Figure A.10 – Temperature-dependent Rs of YBCO film with a thickness of 500 nm and size of 25 mm square
37 A.10 tan δ deviation effect of sapphire rods on surface resistance
Figure A.11 – Temperature dependent Rs of YBCO film when Rs was measured three times
Table A.1 – Standard deviation of the surface resistance calculated from the results of Figure A.11
38 Table A.2 – Relationship between x, defined by Equation (A.12), and y, defined by Equation (A.13)
39 Annex B (informative) Evaluation of relative combined standard uncertainty for surface resistance measurement
B.1 Practical surface resistance measurement
Figure B.1 – Schematic diagram of TE011 and TE013 mode resonance
40 B.2 Determination of surface resistance of the superconductor
Figure B.2 – Typical frequency characteristics of TE011 mode resonance
41 B.3 Combined standard uncertainty
B.3.1 General
B.3.2 Calculation of c2 to c5 (12 GHz resonance at 20 K)
42 B.3.3 Determination of u1 to u5
44 B.3.4 Combined relative standard uncertainty
Figure B.3 – Frequency characteristics of a resonator approximated by a Lorentz distribution
46 Bibliography
BS EN IEC 61788-7:2020
$189.07