JP2006214833A - Resonator exciting method and measuring method of electromagnetic physical property values - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a resonator exciting method capable of easily adjusting the insertion loss, and a measuring method of an electromagnetic physical property values, capable of precisely measuring the electromagnetic physical property values of metallization or ceramics, in the millimeter wave band of 30 GHz or higher. <P>SOLUTION: A resonant conductor 1 is formed on one side of a dielectric substrate 2 and a ground conductor 3, having the same electromagnetic physical property values as the resonant conductor 1, is formed on the other side of the dielectric substrate 2 to constitute a resonator A. In the resonator exciting method for resonating the resonator A by a loop antenna 11 with a diameter of 0.6 m or smaller, the resonance frequency (f) and no-load Q value Qu of the resonator A are measured by exciting and detecting the resonator A by the loop antenna 11 and the electromagnetic physical property value of the dielectric substrate 2 and/or the resonant conductor 1 are calculated, on the basis of the measured values of the resonance frequency (f) and the no-load Q value Qu. <P>COPYRIGHT: (C)2006,JPO&NCIPI

Description

  The present invention relates to a resonator excitation method and an electromagnetic property measurement method, and in particular, the metallized conductivity and the dielectric substrate dielectric in a metallized co-fired dielectric substrate used as an electronic component in a millimeter wave region of 30 GHz or more. It relates to a method for measuring constants and the like.

  In recent years, with the development and popularization of mobile communication technology, there is a strong demand for a dielectric constant measurement method for dielectric substrates for microwave circuit configuration. Various methods for measuring dielectric constants of microwaves on dielectric substrates have been proposed. Among them, the cavity resonator method (JIS R 1641, established in 2002) is recognized as a high-precision measurement method. In the cavity resonator method, the dielectric constant in the surface direction of the substrate is measured.

  On the other hand, when ceramics are used as an electronic component, the metallization and the ceramic are often fired at the same time by the simultaneous firing technique to constitute an electronic component. In this case, the dielectric constant of ceramics may change due to differences in firing conditions compared to firing with ceramics alone or due to interdiffusion with metallization. There is.

However, a sample that can be measured by the cavity resonator method is a substrate made of a single dielectric, and a ceramic substrate that is fired simultaneously with metallization cannot be measured. As a method for measuring dielectric characteristics of a ceramic substrate fired simultaneously with metallization, a measurement method using a ring resonator excited and detected by gap coupling from an input / output microstrip line has been proposed (for example, non-patent literature). 1).
Aly E. Fathy, et al., “An innovative semianalytical technique for ceramic evaluation at microwave frequencies,” IEEE Trans. MTT., Vol. 50, pp. 2247-2252, Oct. 2002.

  However, in Non-Patent Document 1, the resonator performs excitation detection by gap coupling from the input / output microstrip line. In such a method, the excitation detection efficiency is fixed. There is a problem that it is difficult to adjust the value to a suitable value (for example, -20 to -50 dB).

  Furthermore, in recent years, the measurement of electromagnetic property values at higher frequencies has been required, but in the non-patent document 1, the measurement (resonance) is performed at 2 GHz or lower, particularly 30 GHz or higher. In the millimeter wave band, the conventional excitation method cannot adjust the insertion loss to a suitable value, so that measurement is difficult. As a result, it is difficult to measure the dielectric characteristics in the millimeter wave band of 30 GHz or higher with the measurement method as described in Non-Patent Document 1.

  The present invention provides an excitation method for a resonator that can easily adjust insertion loss, and an electromagnetic property that can accurately measure the electromagnetic properties of metallized ceramics and ceramics simultaneously fired with metallized in the millimeter wave band of 30 GHz or higher. It aims at providing the measuring method of a physical-property value.

  According to the resonator excitation method of the present invention, a resonator having a resonant conductor formed on one surface of a dielectric substrate and a ground conductor formed on the other surface of the dielectric substrate is connected to a loop having a diameter of 0.6 mm or less. It is characterized by being excited by an antenna. As the resonator, there is a microstrip line ring resonator or a microstrip line resonator.

  The resonator excitation method of the present invention is characterized in that a resonator having a resonance conductor and a ground conductor formed on one surface of a dielectric substrate is excited by a loop antenna having a diameter of 0.6 mm or less. As the resonator, there are a coplanar line ring resonator and a coplanar line resonator.

  Furthermore, the resonator excitation method of the present invention includes a resonator in which a resonant conductor is formed inside a dielectric substrate and ground conductors are formed on both surfaces of the dielectric substrate with a loop antenna having a diameter of 0.6 mm or less. It is characterized by excitation. As the resonator, there are a stripline ring resonator and a stripline resonator.

  Furthermore, the resonator excitation method of the present invention is characterized in that the resonance frequency f of the resonator is 30 GHz or more. When the resonance frequency f of the resonator is 30 GHz or more, excitation is difficult because the excitation efficiency cannot be adjusted by the conventional excitation by gap coupling. However, in the excitation method of the resonator according to the present invention, excitation is inherently not possible. Even in high-order modes with high resonance frequency such as difficult ring resonators and stripline resonators, excitation detection is possible even at 30 GHz or higher by using a loop antenna with a small diameter, especially 0.6 mm or less. It becomes.

  That is, for the excitation detection of a conventional planar circuit resonator such as a ring resonator, coupling by a gap provided between the input / output line and the resonant conductor has been used. With gap coupling, it is difficult to adjust the insertion loss at the resonance point (preferably -20 to -50 dB). In the present invention, the position of the loop antenna is finely adjusted by using the loop antenna provided at the end of the coaxial cable. Therefore, the excitation detection of the resonator can be easily performed. In particular, the excitation detection can be performed even at 30 GHz or more by using a loop antenna having a diameter of 0.6 mm or less.

  In addition, the inventors have excited a higher order mode such as a ring resonator with a line width of 0.5 mm or more with a loop antenna having a small loop diameter, and measured the resonance frequency and no-load Q, thereby simultaneously with metallization. The present inventors have found that electromagnetic property values such as the relative dielectric constant, dielectric loss tangent, and metallization conductivity of a ceramic substrate that has been fired can be accurately measured in the millimeter wave band of 30 GHz or higher.

  That is, according to the method for measuring an electromagnetic property value of the present invention, a resonant conductor is formed on one surface of a dielectric substrate, and a ground surface having the same electromagnetic property value as that of the resonant conductor is formed on the other surface of the dielectric substrate. The resonator on which the conductor is formed is excited and detected with a loop antenna having a diameter of 0.6 mm or less, and the resonance frequency f and the unloaded Q value Qu of the resonator are measured. An electromagnetic property value of the dielectric substrate and / or the resonant conductor is calculated based on a measured value. As resonators used in such a measuring method, there are a stripline ring resonator and a stripline resonator, and it is desirable that the line width of these resonators is 0.5 mm or more.

  In addition, according to the method for measuring an electromagnetic property value of the present invention, a resonator in which a resonant conductor and a ground conductor having the same electromagnetic property value as the resonant conductor are formed on one surface of a dielectric substrate has a diameter of 0. Excitation detection is performed with a loop antenna of 6 mm or less, and the resonance frequency f and the unloaded Q value Qu of the resonator are measured. Based on the measured values of the resonance frequency f and the unloaded Q value Qu, the dielectric substrate and / or An electromagnetic property value of the resonant conductor is calculated. As a resonator used in such a measurement method, there are a coplanar line ring resonator and a coplanar line resonator, and the line width of the coplanar line ring resonator and the coplanar line resonator is 0.5 mm or more. It is characterized by that.

  Further, according to the method for measuring an electromagnetic property value of the present invention, a resonant conductor is formed inside a dielectric substrate, and ground conductors having the same electromagnetic property value as the resonant conductor are formed on both surfaces of the dielectric substrate. The resonator is excited and detected with a loop antenna having a diameter of 0.6 mm or less, and the resonance frequency f and the unloaded Q value Qu of the resonator are measured. Based on the measured values of the resonance frequency f and the unloaded Q value Qu. The electromagnetic property value of the dielectric substrate and / or the resonant conductor is calculated. As a resonator used in such a measurement method, there are a microstrip line ring resonator and a microstrip line resonator, and the line width of the microstrip line ring resonator and the microstrip line resonator is 0.5 mm or more. It is desirable.

  The method for measuring an electromagnetic property value of the present invention is based on the resonance frequency f and the no-load Q value Qu, and at least one of the electromagnetic property of the conductivity of the resonance conductor, the relative dielectric constant of the dielectric substrate, and the dielectric loss tangent. A value is calculated.

  The method for measuring electromagnetic property values according to the present invention can be used for ring resonators, stripline resonators, etc., as long as the line width is 0.5 mm or more. It is possible to measure the electromagnetic property value without receiving the effect of. That is, the inventors found that the ring resonator and stripline resonator formed by the screen printing method have severe irregularities on the end face of the resonant conductor. It was discovered that dielectric constant and dielectric loss tangent are greatly measured. FIG. 9 shows the measurement of the resonance frequency f of the higher-order mode of a ring resonator having a diameter of 10 mm, a line width of 0.1 to 2.0 mm, and a dielectric thickness of 0.3 mm prepared by simultaneous firing of glass ceramics and copper metallization. This is the result of calculating the relative permittivity, and shows the dependence of the relative permittivity on the line width. When the line width is reduced, the current distribution is concentrated at the end of the line. Therefore, the current path becomes longer by concentrating the current on the uneven portion of the line end surface by the screen printing method, and as a result, the relative dielectric constant is measured to be large. I guess that.

  In the method for measuring electromagnetic property values according to the present invention, the dielectric substrate is made of ceramics or glass ceramics, and the resonant conductor and the ground conductor are printed by a screen printing method or the like, and are simultaneously fired and integrated. Features. Thereby, the electromagnetic property value can be measured in a more realistic state in the ceramic that is fired simultaneously with the metallization. In addition, because the support substrate and resonator are fired and integrated, the dielectric layer is thin, and even if a single layer cannot form a resonator, the resonator is integrally formed on the support substrate by simultaneous firing. By doing so, the sample used for the measurement can be easily produced in a state that is realistic (thickness that is actually used).

  Furthermore, according to the electromagnetic property value measuring method of the present invention, the temperature dependency of the resonance frequency f and the no-load Q value Qu can be measured to obtain the temperature dependency of the electromagnetic property value. In addition, the method for measuring an electromagnetic property value of the present invention is effective in the millimeter wave band, and is particularly suitable when the resonance frequency is 30 GHz or more.

  Next, a calculation method of the electromagnetic property value measuring method of the present invention will be described. In the electromagnetic property value measuring method of the present invention, the resonance frequency f and the no-load Q value Qu of a ring resonator or the like are measured, and by using these data, numerical analysis such as FEM is performed to determine the conductivity and dielectric of the ring conductor. It is possible to calculate at least one electromagnetic property value of the relative dielectric constant and the dielectric loss tangent of the body substrate.

  In order to calculate the relative permittivity of the dielectric substrate, the relationship between the relative permittivity and the resonance frequency is obtained by numerical analysis such as FEM within an assumed range, and this relationship is approximated by an appropriate function. The relative dielectric constant can be calculated from the measured value of the function and the resonance frequency f. For calculating the conductivity of the ring conductor and the dielectric loss tangent of the dielectric substrate, the resonator form factor G and the electric field energy concentration rate Pe of the dielectric substrate are calculated by FEM. From the measured values, the conductivity of the ring conductor and the dielectric loss tangent of the dielectric substrate can be calculated.

  According to the resonator excitation method of the present invention, the resonator can be easily excited at a frequency of 30 GHz or more. Moreover, according to the method for measuring electromagnetic property values of the present invention, it is possible to realize dielectric property measurement at 30 GHz or more of a co-fired body with metallization, which has been difficult in the past.

  The method for measuring electromagnetic property values of the present invention will be described with reference to FIG. First, a microstrip line ring resonator A shown in FIG. 1 used for measurement is prepared as a measurement sample.

  The ring resonator A includes a ring conductor 1 that is a resonance conductor, a dielectric substrate 2, and a ground conductor 3, and these microstrip line ring resonators A are formed on a support substrate 4. Has been. The ring conductor 1 and the ground conductor 3 are made of the same material and have the same electromagnetic property values.

  That is, the ring conductor 1 is formed on the upper surface of the dielectric substrate 2, and the ground conductor 3 is formed between the dielectric substrate 2 and the support substrate 4. The diameter D of the ring conductor 1 indicates the distance between the centers of the widths of the ring conductors.

  When the radiation loss of the microstrip line ring resonator A cannot be ignored, it is desirable to install a shielding conductor 5 surrounding the microstrip line ring resonator A as shown in FIG. The shield conductor 5 is configured to surround the entire microstrip line ring resonator A, and a structure in which a conductor plate is added to the end surface of the hollow cylindrical conductor is suitable.

  When the dielectric substrate of the measurement sample is made of ceramics or glass ceramics, the microstrip line ring resonator A is formed by simultaneous firing or formed by baking the ring conductor 1 and the ground conductor 3 on the dielectric substrate 2. The That is, a conductor pattern is formed on a substrate molded body and fired simultaneously, or a conductor pattern is formed on a fired dielectric substrate and baked at a high temperature to form a microstrip line ring resonator. In the case of simultaneous firing, the support substrate 4 can also be fired simultaneously with the microstrip line ring resonator A, and the production of the microstrip line ring resonator becomes particularly easy.

  When the dielectric substrate of the measurement sample is made of an organic resin, the microstripline ring resonator A is formed by bonding or press-bonding the dielectric substrate 2, the ring conductor 1, and the ground conductor 3. In any case, the thickness of the ring conductor 1 and the ground conductor 3 is preferably at least 5 μm, particularly preferably 10 μm or more, so that the resonant electromagnetic field is not radiated.

  In FIG. 1, the ground 3 is formed on the entire lower surface of the dielectric substrate 2, but may be formed on a part of the lower surface of the dielectric substrate 2 as long as it is formed below the ring conductor 1. More specifically, the ground 3 may be a ring-shaped ground conductor having a ring width three or more times the ring width of the ring conductor 1.

  Below, the measurement process of electrical conductivity and a dielectric constant is demonstrated. First, the ring resonator is excited by a loop antenna 11 having a diameter of 0.6 mm or less formed at the end of the coaxial cable 10, and detected by a loop antenna 11 having a diameter of 0.6 mm or less provided at an opposing position. Then, the resonance frequency f and the no-load Q value Qu of the microstrip line ring resonator are obtained. As shown in FIG. 3B, the diameter of the loop antenna 11 is defined by the maximum length of the loop antenna.

  As shown in FIG. 3, the loop antenna 11 is formed at the tip of the coaxial cable 10. One end of the loop antenna 11 is connected to the center conductor of the coaxial cable 10, and the other end is connected to the coaxial cable. 10 external conductors are connected by solder 12 or the like. (A) is a side view, (b) is a view of (a) seen from above, and (c) is a view of (a) seen from an oblique direction.

  Waveform diagrams obtained by exciting the ring resonator by changing the diameter of the loop antenna 11 are shown in FIGS. FIG. 4 shows a microstrip line having a diameter D = 10 mm, a line width W = 0.5 mm, and a dielectric thickness d = 0.3 mm, produced by simultaneous firing of glass ceramics and copper metallization using a loop antenna having a diameter of 1 mm. It is a wave form diagram obtained by exciting a ring resonator. It can be seen that the noise level rises above 30 GHz. Such an increase in noise level causes a decrease in measurement accuracy of the unloaded Q value Qu. On the other hand, FIG. 5 is a waveform diagram obtained by exciting the same microstrip line ring resonator as in FIG. 1 with a loop antenna having a diameter of 0.6 mm. It can be seen that no increase in noise level was observed even at 30 GHz or higher, and that a good resonance waveform was obtained.

  In FIG. 4, since the wavelength of the electromagnetic field decreases with increasing frequency, it is considered that the noise level is increased because unnecessary signals other than the resonant electromagnetic field are detected unless the antenna is also reduced accordingly. In FIG. 5, by using a loop antenna having a diameter of 0.6 mm, an unnecessary signal other than the resonance electromagnetic field is not detected, and a good noise level is realized. 4 and 5, it can be seen that a loop antenna having a diameter of 0.6 mm or less can realize a good noise level without detecting unnecessary signals other than the resonance electromagnetic field at 30 GHz or more.

  Next, the analysis process will be described. First, the relative dielectric constant ε ′ of the dielectric substrate 2 is obtained from the measured value of the resonance frequency f by numerical analysis such as a finite element method (FEM) or a mode matching method. Here, the case where the finite element method is used will be described. The resonance frequency f of the ring resonator shown in FIG. 1 is a function of the dielectric constant ε ′, thickness d, ring diameter D, ring width w, and ring conductor thickness t of the dielectric substrate 2. d, D, w, and t are fixed to measured values or design values, the dielectric constant ε ′ of the dielectric substrate 2 is set at several points within an expected range, and the corresponding resonance frequency f is calculated by the finite element method. To do. From these calculation results, the relationship between the resonance frequency f and the relative dielectric constant ε ′ is approximated by an appropriate function, and the relative dielectric constant ε ′ of the dielectric substrate is calculated from the approximate expression and the measured value of the resonance frequency f.

Next, from the measured value of Qu, the conductivity σ of the conductor of the ring resonator or the dielectric loss tangent tan δ of the dielectric substrate is obtained by the following formula 1. However, tan δ needs to be known when obtaining the conductivity σ, and σ needs to be known when obtaining tan δ.

In Equation 1, μ is the magnetic permeability of the conductor. Concentration rate of P _e is the electric field energy, G is the form factor, non-patent document 2 "J. Krupka, K. Derzakowski, A. Abramowicz, ME Tobar and RG Geyer," Use of whispering-gallery modes for complex permittivity determinations of ultra-low-loss dielectric materials, “IEEE Trans. Microwave Theory Tech., vol. 47, pp. 752-759, June 1999”.

More specifically, _Pe is the concentration ratio of the electric field energy in the dielectric substrate 2 of the microstrip line ring resonator. The concentration ratio of the electric field energy is defined as a fraction of the electric field energy stored in each part with respect to the electric field energy stored in the resonator. _Pe is given by the following equation 2.

G in Equation 1 indicates the form factor of the ring resonator, and is given by Equation 3 below.

  Expressions 2 and 3 are obtained by a numerical analysis method such as a finite element method (FEM) or a mode matching method.

The obtained P _e, by substituting _G in Formula 1, the conductivity sigma, obtains the relational expression of the dielectric loss tangent tan [delta. After this, when obtaining σ, other methods such as “Yoshikawa, Nakayama,“ Study on the method of measuring the complex permittivity of a flat plate loaded at the end of a cavity resonator in the V and W bands ”, Substituting the value of tan δ measured or inferred by Dai, C-2-63, Sept. 2004. into Equation 1 to obtain σ.

To obtain tan δ, other methods such as “A. Nakayama, Y. Terashi, H. Uchimura and, A. Fukuura,“ Conductivity measurement at the interface between the sintered conductor and dielectric substrate at microwave frequencies, ”IEEE Trans. Microwave Theory Tech., Vol. MTT-50, No.7, pp. 1665-1674, July 2002.
Substituting the value of σ measured or estimated in (1) into Equation 1 to obtain tan δ.

  In the above embodiment, the case where a ring resonator is used as the resonator has been described. However, as shown in FIG. 6, a line 21 is formed instead of the ring conductor to form a microstrip line resonator. It can also be measured using a measuring instrument. Here, reference numeral 22 denotes a dielectric substrate, 23 denotes a ground conductor, and 24 denotes a support substrate.

  Further, as shown in FIG. 7, a coplanar line resonator in which a resonant conductor 31 and a ground conductor 33 having the same electromagnetic properties as the resonant conductor 31 are formed on one surface of a dielectric substrate 32, It can also be measured using this resonator. Here, the code | symbol 34 shows a support substrate.

  Further, as shown in FIG. 8, a strip line in which a resonant conductor 41 is formed inside a dielectric substrate 42, and a ground conductor 43 having the same electromagnetic properties as the resonant conductor 41 is formed on both surfaces of the dielectric substrate 42. It is also possible to form a resonator and measure using this resonator. Here, reference numeral 44 denotes a support substrate.

Table 1 shows the results obtained by using the method shown in FIG. 1 for the relative dielectric constant ε ′ and dielectric loss tangent tanδ of glass ceramics co-fired with copper metallization at 30 GHz or higher using the electromagnetic property measurement method of the present invention. It is shown in 1. Here, the diameter of the loop antenna was 0.6 mm. The thickness d of the dielectric of the microstrip line ring resonator as the measurement sample was 0.3 mm and 0.1 mm, and the width w of the ring conductor was 1.0 mm and 0.5 mm. Measurement of ε ′ and tan δ at frequencies near 30, 50, and 80 GHz is realized by measuring the higher-order resonance mode. The value of the conductivity σ was set to 3.0 × 10 ⁷ (S / m) at 30 to 40 GHz and 2.2 × 10 ⁷ (S / m) at 50 GHz or more from the above literature.

It can be seen from Table 1 that the dielectric constant of the glass ceramic is ε ′ = 4.96 to 5.00 and tan δ = 10 to 20 × 10 ⁻⁴ in the region of 30 to 80 GHz. On the other hand, when the present inventors excited the resonator shown in FIG. 1 using a loop antenna having a diameter of 1 mm, the noise level increased at a resonance frequency of 30 GHz or higher, and tan δ at 30 GHz or higher could not be measured.

The microstrip line ring resonator used for the electromagnetic measuring method of this invention is shown, (a) is a top view, (b) is a schematic sectional drawing. It is a figure for demonstrating the structure which added the shielding conductor to the ring resonator used for the measuring method of this invention. It is a figure which shows a loop antenna. A waveform diagram obtained by exciting a ring resonator having a diameter of 10 mm, a line width of 0.5 mm, and a dielectric thickness of 0.3 mm, which was created by simultaneous firing of glass ceramics and copper metallized by a loop antenna having a diameter of 1 mm. is there. Waveform obtained by exciting a ring resonator with a diameter of 10 mm, a line width of 0.5 mm, and a dielectric thickness of 0.3 mm made by simultaneous firing of glass ceramics and copper metallization using a loop antenna with a diameter of 0.6 mm FIG. 1 shows a microstrip line resonator, where (a) is a plan view and (b) is a schematic cross-sectional view. 1 shows a coplanar resonator, where (a) is a plan view and (b) is a schematic cross-sectional view. 1 shows a stripline resonator, (a) shows a resonant conductor, and (b) is a schematic sectional view. The resonance frequency f of the higher-order mode of a ring resonator having a diameter of 10 mm, a line width of 0.1 to 2.0 mm, and a dielectric thickness of 0.3 mm, created by simultaneous firing of glass ceramics and copper metallization, is measured. It is a result of calculating the dielectric constant, and is a diagram showing the line width dependence of the relative dielectric constant.

Explanation of symbols

DESCRIPTION OF SYMBOLS 1 ... Ring conductor 2, 22, 32, 42 ... Dielectric substrate 3, 23, 33, 43 ... Ground conductor 4, 24, 34, 44 ... Support substrate 5 ... Shielding conductor A ... Ring resonators

Claims (8)

A resonator having a resonant conductor formed on one surface of a dielectric substrate and a ground conductor formed on the other surface of the dielectric substrate is excited by a loop antenna having a diameter of 0.6 mm or less. Method of excitation. A resonator excitation method, wherein a resonator having a resonance conductor and a ground conductor formed on one surface of a dielectric substrate is excited by a loop antenna having a diameter of 0.6 mm or less. A resonator excitation method characterized by exciting a resonator having a resonant conductor formed inside a dielectric substrate and ground conductors on both sides of the dielectric substrate with a loop antenna having a diameter of 0.6 mm or less. . 4. The resonator excitation method according to claim 1, wherein the resonance frequency f of the resonator is 30 GHz or more. A resonator in which a resonant conductor is formed on one surface of a dielectric substrate, and a ground conductor having the same electromagnetic properties as the resonant conductor is formed on the other surface of the dielectric substrate, has a diameter of 0.6 mm or less. And detecting the resonance frequency f and the unloaded Q value Qu of the resonator, and based on the measured values of the resonance frequency f and the unloaded Q value Qu, the dielectric substrate and / or the resonance A method for measuring an electromagnetic property value, comprising calculating an electromagnetic property value of a conductor. A resonator in which a resonant conductor and a ground conductor having the same electromagnetic property value as that of the resonant conductor are formed on one surface of the dielectric substrate is excited and detected by a loop antenna having a diameter of 0.6 mm or less. A resonance frequency f and an unloaded Q value Qu are measured, and an electromagnetic property value of the dielectric substrate and / or the resonant conductor is calculated based on the measured values of the resonance frequency f and the unloaded Q value Qu. A method for measuring electromagnetic properties. A resonator in which a resonant conductor is formed inside a dielectric substrate and a ground conductor having the same electromagnetic properties as the resonant conductor is formed on both sides of the dielectric substrate with a loop antenna having a diameter of 0.6 mm or less. Excitation detection is performed to measure the resonance frequency f and the unloaded Q value Qu of the resonator, and based on the measured values of the resonance frequency f and the unloaded Q value Qu, the electromagnetic of the dielectric substrate and / or the resonant conductor is measured. A method for measuring an electromagnetic property value, wherein the property value is calculated. 8. The electromagnetic property value of at least one of the electrical conductivity of the resonant conductor, the relative dielectric constant of the dielectric substrate, and the dielectric loss tangent is calculated based on the resonant frequency f and the no-load Q value Qu. A method for measuring an electromagnetic property value according to any one of the above.

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