Analytical, Numerical, and Experimental Investigation of an Eccentric Double-Ring Microwave Resonator for Electromagnetic Shielding Applications

Abstract

This study presents an in-depth investigation of an eccentric double-ring microwave resonator comprising two asymmetrically coupled conductive loops connected at a single point. The configuration was systematically analyzed using analytical modeling, full-wave electromagnetic simulations (Ansys HFSS), and experimental characterization. Analytical formulations based on the resonant condition of thin conductive rings provided theoretical estimates of the fundamental and higher-order eigenmodes, while simulations yielded accurate resonance frequencies, transmission responses, and electric field distributions. The transmission coefficient (S₂₁) exhibited two distinct resonance dips at 436 MHz and 708 MHz, confirming strong inter-ring coupling and hybrid mode formation. Electric field mapping revealed pronounced confinement within the resonator region (E > 170 V/m) and substantial attenuation of the transmitted field (E < 13 V/m), demonstrating efficient electromagnetic energy suppression. Experimental results showed excellent consistency with theoretical predictions. This paper aims to establish a compact, low-cost, and tunable resonant structure capable of frequency-selective attenuation and field confinement without using lossy materials. Unlike conventional symmetric resonators, the eccentric configuration enables enhanced coupling control and modal diversity, making it highly relevant for the design of next-generation electromagnetic shielding, filtering, and sensing systems.

1. Introduction

Ring-shaped microwave resonators are fundamental components in the design of resonant networks intended for electromagnetic (EM) wave suppression within specified frequency bands. Accurate identification of their resonant frequencies is essential for predicting and optimizing the overall network performance. This study investigates a resonator topology comprising conductive rings arranged eccentrically so that they make contact at a single point.

Research on microwave ring resonators has expanded rapidly over the past decade, particularly regarding multi-ring, concentric, and eccentric configurations applied in filtering, sensing, and electromagnetic shielding.

Many years ago, resonators based on split rings were studied, and research demonstrated their positive characteristics and various useful applications. For example, in [1] (2004), Kastrakis et al. described the electric excitation of magnetic resonance (EEMR) effect, which is distinct from the SRR’s response to a magnetic field that is excited when the incident magnetic field is perpendicular to the gap. In closely spaced SRR arrays, the electric and magnetic couplings between the resonators can also be strong and influence each other, leading to complex behavior such as modified resonance frequencies and transmission dips. In 2005, Baena et al. presented a new approach to developing planar metamaterial structures based on split-ring resonators, which find application in devices operating in the microwave region [2]. Landy and his associates also worked with metamaterial-based absorbers in 2008 [3]. Shadrivov et al. experimentally studied split-ring resonators and showed that the eigenfrequencies of the resonators can be tuned over a wide frequency range [4]. In addition, in 2008, Aydin and his colleagues studied split ring resonators (SRR) to improve electromagnetic wave transmission through subwavelength apertures [5]. In his paper published in 2010, Cheng presented a polarization-insensitive metamaterial absorber comprising a dielectric substrate with a split-ring-cross resonator and a continuous metal film. The experiment demonstrated excellent field absorption at high frequencies [6]. Kapoor et al. [7] demonstrated that coupled ring resonators enable precise dielectric material characterization due to strong EM interaction, while Islam et al. [8] presented a mutually coupled concentric crossed-line split-ring resonator, demonstrating strong mode coupling and tunable responses in the C, X, and Ku bands. Furthermore, ring resonators are widely recognized for their compact structure, high Q-factor, and ease of integration into planar microwave systems [8,9]. Alahnomi et al. [9] provided a detailed review of planar resonator-based sensors, highlighting advances in high sensitivity and multi-band applications. Hossain et al. [10] reported multilayer metamaterial absorbers using E-shaped and ring-based resonators that achieved high absorption over targeted frequency ranges. Recent studies have explored the effect of eccentric coupling between rings, which modifies field confinement and broadens the resonance bandwidth [11,12]. Walsten et al. [12] experimentally compared single and concentric split-ring resonators and confirmed significant improvements in field localization. In addition to sensing and filtering, ring resonators have been investigated for electromagnetic shielding and absorption [10,13,14]. Liu et al. [13] showed that embedding split-ring resonators into composite fabrics substantially enhances electromagnetic shielding effectiveness. Such innovations underline the versatility of ring-resonator topologies for compact and tunable EM structures [15,16,17]. Other recent developments include metamaterial absorbers with flexible substrates [18], biodegradable resonator sensors [19], and quad-band resonator arrays for advanced wireless systems [20]. Rabani et al. designed a metamaterial absorber for S, X, and Ku-band frequencies, achieving peak absorption in each band at 3.26 GHz, 11.6 GHz, and 17.13 GHz, respectively. The design uses a modified circular ring resonator structure with a dumbbell-shaped element and is intended for use in microwave sensing applications. Metamaterials like this are engineered materials that manipulate waves through their structure rather than their composition and can be used in applications like sensing, wireless communication, and radars [21]. In [22], Jahan et al. researched a metamaterial absorber (PMA) for multiple sensing applications. The PMA consists of two split ring resonators with six split gaps, configured to exhibit rotational symmetry.

As shown above, most available literature and scientific research focus on metamaterial structures comprising up to a hundred elementary units—rings arranged in a network —which operate at extremely high frequencies (up to 40 GHz). The aim of this research was to analyze how an eccentric ring composed of only two basic elements (rings) can attenuate electric field strength in the lower high-frequency range (below 1 GHz). These frequencies are widely used (e.g., military VHF/UHF, biomedical telemetry, FM, GSM, DVB-T2, IoT, 5G NR), and it is necessary to determine how field suppression can be achieved specifically in this frequency range. By using only one physical element (with an eccentric connection of the rings), the field on the ring can be clearly localized, while the field behind the ring can be significantly attenuated. As this research involves a metal wire and a copper ring, emphasis is also placed on the simplicity of construction and the low fabrication cost of the structure, making it particularly suitable for EM shielding below 1 GHz.

In this paper, we propose and experimentally verify a microwave resonator consisting of two eccentrically coupled conductive rings connected at a single point. Analytical modeling, full-wave simulation (Ansys HFSS), and experimental validation were used to determine resonant frequencies, field distributions, and transmission characteristics. The proposed structure is analyzed as a potential unit element for resonant networks designed to suppress electromagnetic wave propagation in selected frequency ranges.

2. Design Requirements and Modeling

The aim of this research was to develop a resonator structure capable of reducing the electromagnetic field level within a targeted frequency range, suitable for use as an absorber network to protect human environments or to ensure the proper operation of nearby devices.

Two key questions arise:

(1)

What is the target frequency range?

(2)

What should the resonator configuration be?

The frequency range of interest can be determined based on the known state of the electromagnetic spectrum and previous measurements of ambient EM levels. Figure 1 shows the most significant field contributions in the target frequency range, particularly below 1 GHz, where stationary field sources such as FM radio, DVB-T2, 5G NR, and GSM are ubiquitous.

Among the available configurations, the circular ring resonator is compact, mechanically robust, and suitable for microwave applications. To broaden its operating frequency range, a modified dual-ring version was designed (Figure 2). Microwave ring resonators are widely used in telecommunications, optics, and integrated photonics as filters, oscillators, sensors, and multiplexers. Their inherent frequency selectivity enables their use as absorber components across broad frequency bands.

3. Analytical and Numerical Modeling

3.1. Analytical Modeling

Analytical calculations were performed to estimate the resonant frequencies of the proposed structure, while full-wave electromagnetic simulations using Ansys HFSS verified these predictions. Resonance occurs when the ring circumference equals an integer multiple of the guided wavelength:

$$2\pi R=m{\lambda }_m$$

(1)

and the corresponding resonant frequency is:

$$f_m={\displaystyle \frac{mc}{2\pi R\sqrt{{\epsilon }_{eff}}}},$$

(2)

where R is the ring radius, c the speed of light in air, and ε_eff the effective dielectric constant (ε_eff ≈ 1 for free space). This relation is valid for a thin conducting ring of radius R.

In accordance with the above, Figure 3 shows the actual behavior of the structure. It is struck by an electromagnetic wave of various frequencies (and wavelengths). The condition for resonance in this structure is that its physical length is a multiple of one of the wavelengths. It is important to determine this value in our case, because at this frequency the energy does not propagate further but is absorbed. In theory, multiple frequencies are involved, possibly even a range of frequencies. Based on the condition stated in (1), the resonance of each ring is calculated. After this, the resonant frequency can be determined according to (2).

If the ring has length, width, and height (see Figure 4), the effective radius is calculated according to Equation (3), where r is the radius, t the depth of the ring, and w ring width.

$$R_{eff}=R-{\displaystyle \frac{w}{2}}$$

(3)

The effective radius accounts for the width w and is therefore suitable for our intended purpose.

This paper analyzes a resonator constructed as a thin conductive ring (comprising two eccentric rings) as a basic resonator structure, and a conductive cylindrical ring as a resonator with high strength that can be used for applications such as forming an absorber network within a building material (e.g., concrete).

Table 1. Analytical determination of resonant frequencies (MHz) for the first five modes of ring resonators with outer radius R and effective radius R_eff using Equation (3)—large (outer) resonator ring.

A Thin Conducting Ring of Radius R
R, mm	Mod m = 1	Mod m = 2	Mod m = 3	Mod m = 4	Mod m = 5
85	561.3	1122.7	1684.0	2245.3	2806.7
95	502.3	1004.5	1506.7	2009.0	2511.2
105	454.4	908.8	1363.2	1817.7	2272.1
A Cylindrical Conductive Ring of Radius Ref (w = 4 mm, t = 10 mm) (Reff = R − w/2)
83	574.9	1149.7	1724.6	2299.4	2874.3
93	513.0	1026.1	1539.1	2052.2	2565.2
103	463.2	926.5	1389.7	1852.9	2316.2

and

Table 2. Analytical determination of resonant frequencies (MHz) for the first five modes of ring resonators with outer radius R and effective radius R_eff using Equation (3)—small (inner) resonator ring.

A Thin Conducting Ring of Radius R
R, mm	Mod m = 1	Mod m = 2	Mod m = 3	Mod m = 4	Mod m = 5
56.5	844.9	1689.8	2534.7	3379.6	4224.5
66.5	717.5	1435.8	2153.7	2871.6	3589.5
76.5	623.8	1247.7	1871.5	2495.4	3119.2
A Cylindrical Conductive Ring of Radius Ref (w = 4 mm, t = 10 mm) (Reff = R − w/2)
54.5	875.4	1750.7	2626.1	3501.5	4376.8
64.5	739.7	1479.5	2219.2	2958.9	3698.7
74.5	639.4	1278.9	1918.3	2557.7	3197.2

present analytically determined resonant frequencies of thin and cylindrical conductive (a ring that can be applied in reality) rings. The selected radii (R₁ = 95.0 mm, R₂ = 66.5 mm) ensure that the first mode is below 1 GHz, with several higher modes below 2 GHz.

Table 1 and Table 2 detail the resonant frequency calculations for the individual rings, providing the values needed to create a real-world situation in HFSS.

The radii of the rings (outer and inner rings of the resonator) are selected so that the resonant frequency (first mode) is below 1 GHz. By setting the first mode resonant frequency below 1 GHz, the three modes of the outer (large—Figure 5b) ring and the two modes of the inner (small—Figure 5a) ring of the resonator fall within the target frequency range below 2 GHz. By connecting these two rings to form an eccentric resonator (Figure 5c), the attenuation regions (transmission reduction) are further extended around these resonances.

Figure 5a–c relates to Table 2, Table 1, and

Table 3. Analytical determination of resonant frequencies for the first five modes of eccentric ring resonators with different coupling factors k. Resonator dimensions: R₁ = 95.0 mm; R₂ = 66.5 mm (Coeff = 0.7); $\omega$ = 4 mm; t = 10 mm.

A Thin, Eccentric Ring Resonator (Oo) with Radii R1 + R2
k	m = 1 f−/f+ (MHz)	m = 2 f−/f+ (MHz)	m = 3 f−/f+ (MHz)	m = 4 f−/f+ (MHz)	m = 5 f−/f+ (MHz)
0.00	502.30/717.50	1004.60/1435.00	1506.90/2152.50	2009.20/2870.00	2511.50/3587.50
0.25	489.20/760.88	978.39/1521.76	1467.59/2282.64	1956.78/3043.52	2445.98/3804.40
0.75	435.76/1250.41	871.52/2500.81	1307.27/3751.22	1743.03/5001.62	2178.79/6252.03
Cylindrical Oo Eccentric Ring Resonators with Radii: Reff1 + Reff2 (ω = 4 mm, t = 10 mm) (Reff = R − ω/2)
0.00	513.05/739.74	1026.10/1479.49	1539.14/2219.23	2052.19/2958.97	2565.24/3698.72
0.25	500.07/783.84	1000.13/1567.68	1500.20/2351.51	2000.26/3135.35	2500.33/3919.19
0.75	446.25/1285.81	892.49/2571.61	1338.74/3857.42	1784.99/5143.22	2231.23/6429.03

, respectively.

It can be concluded that an increase in the number of rings in such a resonator also increases the range of the resonant region within which the EM wave passing through it is attenuated.

A thicker ring has a shorter effective length, as the calculation uses the effective radius of the ring, which is smaller than the actual radius. Therefore, the resonant frequencies are slightly higher than for a thin ring. In practice, these values will be further shifted due to finite conductivity, distribution effects, and possible parasitic capacitances to the environment.

The resonator was shaped with two eccentrically connected rings to increase attenuation in the region below 2 GHz, which is critical in terms of transmission coefficients (very high transmission coefficients of the EM wave compared to the rest of the microwave spectrum (f > 2 GHz)), and includes many fixed sources of EM radiation (FM radio, DVBT2, 5G mobile telephony below 1 GHz, LTE 1600, etc.). To achieve this, the following ring radius values were chosen: R₁ = 95 mm, R₂ = 66.5 mm, $\omega$ = 4 mm, t = 10 mm.

If the resonator is represented by an equivalent circuit of two coupled inductances (with magnetic coupling factor k) without capacitive coupling (assumption), then a pair of separated resonance frequencies for such a structure can be determined. This pair of separated frequencies is based on the resonant angular frequencies of the individual rings (inductances) ${\omega }_1=2\pi f_1$ and ${\omega }_2=2\pi f_2$, where $f_1$ and $f_2$ are the resonant frequencies of the individual rings (inductances), and is calculated according to the following relation:

$${{\omega }_{\mp }}^2={\displaystyle \frac{{{\omega }_{1m}}^2+{{\omega }_{2m}}^2\mp \sqrt{{{({\omega }_{1m}}^2-{{\omega }_{2m}}^2)}^2-4(1-k^2){{\omega }_{1m}}^2{{\omega }_{2m}}^2}}{2(1-k^2)}}$$

(4)

where m—mode number, ${\omega }_{1m}$ = m ${\omega }_1$—resonant angular frequency of the mth mode of the first inductance (first resonant ring), ${\omega }_{2m}$= m ${\omega }_2$—resonant angular frequency of the mth mode of the second inductance (second resonant ring), ${\omega }_1$—resonant angular frequency of the first mode of the first isolated inductance (independent resonant ring, m = 1), and ${\omega }_2$—resonant angular frequency of the first mode of the second isolated inductance (independent resonant ring, m = 1). See Table 1 and Table 2 (second column).

For the first mode, Relation (5) reads:

$${{\omega }_{\mp }}^2={\displaystyle \frac{{{\omega }_1}^2+{{\omega }_2}^2\mp \sqrt{{{({\omega }_1}^2-{{\omega }_2}^2)}^2-4(1-k^2){{\omega }_1}^2{{\omega }_2}^2}}{2(1-k^2)}}$$

(5)

where m = 1, ${\omega }_{11}={\omega }_1=2\pi f_1$—resonant angular frequency of the first mode of the first inductance (resonant ring), and ${\omega }_{21}={\omega }_1=2\pi f_1$—resonant angular frequency of the second mode of the second inductance (resonant ring).

In accordance with the target frequency range, the radii of the resonant rings of the resonator were selected as follows: R₁ = 95.0 mm and R₂ = 66.5 mm. Using Relation (3), the resonant frequencies of the first mode of each ring are calculated, given the radius of each ring: $f_1={\displaystyle \frac{c}{2\pi R_1}}$ = 502.30 MHz and $f_2={\displaystyle \frac{c}{2\pi R_2}}$ = 717.50 MHz (see Table 1 and Table 2, column two), and then the split frequencies $f$₊ and $f$₋. Table 3 presents the results of the split frequencies for the first five modes with different values of the coupling parameter k in the range from 0.0 to 0.75. The table shows the results separately for thin rings and for rings with cross-sectional dimensions $\omega$ = 3 mm and t = 10 mm, using the effective radii of these rings.

The following text refers to the parameter Coeff, which represents the ratio of the radii of the small and large rings (R₂/R₁), and is used in the simulation of the transmission parameter S₂₁.

Since the effective radii are smaller than the actual radii in thin-wire rings, the resonant frequencies of these resonators are higher than those of thin-wire resonators. These changes are evident in the simulation results examining the influence of the resonator ring width w and ring thickness t on the transmission parameter, which are presented in the next chapter.

If, in addition to inductive coupling, capacitive coupling is also included in the analytical calculation, the resonator can be modeled as two series RLC circuits with mutual inductive (coefficient k) and capacitive coupling (C₁₂). The analytical calculation then changes significantly, and the resonant frequencies are (according to [23]) calculated using the equation:

$${{\omega }_{\mp }}^2={\displaystyle \frac{T\mp \sqrt{T^2-4D}}{2D}},$$

(6)

where

$$T=L_1\left(C_1+C_{12}\right)+L_2\left(C_2+C_{12}\right)-2M{C}_{12},$$

$$D=\left({L_{1}L}_2-M^2\right)\left({C_{1}C}_2+C_{12}(C_1+C_2\right)).$$

If the inductance values used in the previous model of the resonator with two inductances (L₁ = 0.390 μH and L₂ = 0.241 μH) are applied, along with the previously determined resonance frequencies of the ring resonator (Table 3—values k = 0, m = 1; $f$ ₋/ $f$ ₊ = 513.05/739.74 MHz) from the resonance conditions ($f_i={\displaystyle \frac{1}{2\pi \sqrt{L_i{C}_i}}},\mathrm{w}\mathrm{h}\mathrm{e}\mathrm{r}\mathrm{e}i=1,2$), the equivalent capacitances of each ring can be determined (C₁ = 0.247 pF and C₂ = 0.192 pF). Using Relation (6), and varying the values of the magnetic and capacitive coupling parameters, the results shown in

Table 4. Analytical determination of resonant frequencies for the first five modes of eccentric ring resonators with a constant factor k = 0.435 and variable capacitive coupling (C₁₂). Resonator dimensions: R₁ = 95.0 mm; R₂ = 66.5 mm (Coeff = 0.7); $\omega$ = 4 mm; t = 10 mm.

C12, pF	Mod m = 1	Mod m = 2	Mod m = 3	Mod m = 4	Mod m = 5
0.088	459.56/680.75	919.11/1361.50	1378.67/2042.25	1838.22/2723.00	2297.78/3403.75
0.089	459.25/679.47	918.51/1358.93	1377.76/2038.40	1837.01/2717.87	2296.27/3397.33
0.090	458.95/678.20	917.90/1356.39	1376.85/2034.59	1835.80/2712.78	2294.75/3390.98

,

Table 5. Analytical determination of resonant frequencies for the first five modes of eccentric ring resonators with a constant factor k = 0.445 and variable capacitive coupling (C₁₂). Resonator dimensions: R₁ = 95.0 mm; R₂ = 66.5 mm (Coeff = 0.7); $\omega$ = 4 mm; t = 10 mm.

C12, pF	Mod m = 1	Mod m = 2	Mod m = 3	Mod m = 4	Mod m = 5
0.088	459.37/684.75	918.74/1369.51	1378.11/2054.26	1837.48/2739.01	2296.85/3423.76
0.089	459.08/683.44	918.16/1366.88	1377.24/2050.32	1836.32/2733.76	2295.40/3417.20
0.090	458.79/682.14	917.58/1364.29	1376.37/2046.43	1835.16/2728.57	2293.96/3410.71

and

Table 6. Analytical determination of resonant frequencies for the first five modes of eccentric ring resonators with constant factor k = 0.455 and variable capacitive coupling (C₁₂). Resonator dimensions: R₁ = 95.0 mm; R₂ = 66.5 mm (Coeff = 0.7); $\omega$ = 4 mm; t = 10 mm.

C12, pF	Mod m = 1	Mod m = 2	Mod m = 3	Mod m = 4	Mod m = 5
0.088	459.14/688.97	918.28/1377.94	1377.42/2066.91	1836.56/2755.88	2295.70/3444.85
0.089	458.87/687.63	917.73/1375.26	1376.60/2062.89	1835.46/2750.52	2294.33/3438.16
0.090	458.59/686.31	917.18/1372.61	1375.77/2058.92	1834.36/2745.22	2292.94/3431.53

are obtained. The selection of parameters for both types of coupling is based on the assumption of fairly strong inductive coupling (k > 0.3 represents strong coupling) and moderate to strong capacitive coupling (about 20% of the sum of both equivalent capacitances).

For rough estimates of the resonant frequencies of the analyzed resonators, the first model used provides a very good approximation, while the analytical model accounting for both types of coupling, as expected, describes the operation of the ring eccentric resonators analyzed in this paper much more precisely.

3.2. Numerical Calculations—Simulations

Numerical simulations were conducted using the Ansys HFSS 2022/R1 software package. The simulations involved determining the eigenfrequencies of the resonator and the transmission coefficient as the electromagnetic wave passed through the resonator. The simulation models are shown in Figure 6.

In this paper, two simulation models were used:

(a)

simulation of eigenfrequency calculation (Figure 6a), and

(b)

simulation of coupling coefficient and E field distribution calculation (Figure 6b).

The first simulation model featured a resonator with variable outer and inner ring radii, as well as other geometric parameters, depending on the resonator configuration being calculated (a single or double ring resonator, and thin or cylindrical rings). This resonator was placed in a radiation space (air) with dimensions of 300 × 300 × 300 mm.

The second simulation model included two biconical antennas, each with a total length of l = 280 mm, a cone diameter of 100 mm, and a cone thickness of 2 mm, separated by 1690 mm. The analyzed resonator was positioned midway between them. Using this model, simulation calculations of the transmission coefficients and E field distribution were performed for all versions of the resonator with one and two rings (MODEL I and MODEL II). This assembly was placed in a radiation space (air) with dimensions of 800 × 800 × 3500 mm.

4. Simulation Results and Field Distribution

HFSS simulations determined the eigenfrequencies, S-parameters, and E-field distributions. Figure 7 and Figure 8 show how resonant frequencies vary with geometry. A second resonance at approximately 708 MHz appears due to inner-ring coupling, confirming bandwidth expansion.

4.1. Coupling (Transmission) Parameters

Since the resonator under consideration represents the elementary unit of a resonant network, understanding its transmission characteristics is critically important for designing larger periodic structures.

Figure 7 and Figure 8 show that the resonant frequency of the ring resonator changes significantly with variations in the radius of the large ring, as expected. The resonant frequency increases as the radius of the large ring decreases (with other geometric parameters held constant: Coeff = 0.7, $\omega$ = 4 mm, t = 10 mm), rising from 435.70 MHz with R₁ = 95.0 mm to 558.95 MHz with R₁ = 75.0 mm, and reaching 1.01 GHz with R₁ = 45.0 mm. Similarly, changing the proportionality ratio between the radii of the large and small rings also alters the resonant frequency. Adjusting this coefficient changes only the radius of the small ring, while the outer radius of the large ring remains constant at R₁ = 95.0 mm.

Changing the thickness t and width w of the ring has a very small effect on the resonant frequency. It is important to note, as shown in Figure 7, that with the coefficient proportional to the large and small resonator rings, as well as with the resonator with R₁ = 95 mm, a second resonance (a minimum of the S₂₁-f curve) appears at 707.60 MHz. This is precisely the effect of expanding the frequency range of attenuation of the amplitude of the EM wave passing through the ring resonator constructed with an additional (inner) ring placed eccentrically.

This effect of widening the frequency range of amplitude attenuation of the EM wave passing through the ring resonator is particularly noticeable in Figure 8, which shows the transmission parameters of the eccentric ring resonator (marked as Oo resonator) with dimensions (R₁ = 95.0 mm); Coeff = 0.7 (R₂ = 66.5 mm; $\omega$ = 4 mm; t = 10 mm) and its rings as separate resonators (marked as O_R1 and O_R2). Resonators made with only one ring (O_R1 and O_R2) have only one resonance in this frequency range, namely f₁ = 566.16 MHz (O_R1) and f₂ = 727.89 MHz (O_R2), while in the case of resonators with both rings placed eccentrically (Figure 5), two resonances appear at 435.70 MHz and 707.60 MHz.

Determination of the change in resonant frequencies depending on the geometric parameters in this chapter was conducted with the aim of designing a ring eccentric microwave resonator. The effect of this resonator on the reduction in the transmission parameter at and outside the resonant frequencies was confirmed by calculating the distribution of the electric field strength in the next chapter.

4.2. Field Distribution Analysis

Following the transmission analysis, spatial field distributions were evaluated to understand energy localization within the resonator. At 436 MHz (resonance), the E-field shows strong confinement around the ring edges with E > 170 V/m, while behind the resonator (ANT2 plane) it drops to <13 V/m, confirming high attenuation. At 1.0 GHz (non-resonant), the field is uniform and weak (E < 60 V/m).

At the resonant frequency, strong confinement of the electric field (E-field) is observed in the immediate vicinity of the resonator (Figure 9a). Figure 9 shows the distribution of the electric field strength in the plane where the resonator is located and in the plane that horizontally intersects the antenna. The field vectors form closed, intensified loops around the edges of both rings, indicating constructive interference and the formation of a standing-wave pattern.

Maximum field magnitudes exceed 170 V/m, concentrated at the eccentric contact point between the inner and outer rings, where capacitive coupling dominates. This confirms the existence of a strong local resonance that enhances energy storage within the structure.

In contrast, at the non-resonant frequency of 1.0 GHz, the E-field is uniformly distributed, and its amplitude decreases sharply, remaining mostly below 60 V/m (see Figure 10). This reduction indicates that the structure acts as a low-loss scatterer outside the resonant region, allowing most of the incident energy to propagate through with minimal distortion.

The longitudinal field distribution between the antennas (Figure 9b) further demonstrates the attenuation effect at resonance. Along the propagation axis (ANT 1 → Resonator → ANT 2), the simulated E-field magnitude at the receiving antenna drops from 26.7 to 80 V/m (non-resonant) to 0–13.3 V/m (resonant), indicating a substantial decrease in transmitted field intensity (see Figure 11a,b). The corresponding S₂₁ parameter minimum at 436 MHz matches this attenuation, confirming that the resonator efficiently absorbs or redirects a large portion of the incident electromagnetic energy. The same field behavior at the receiving antenna ANT2 applies at the frequency of 1 GHz (see Figure 11c,d).

Such a field pattern is typical of resonant metallic inclusions exhibiting both inductive and capacitive coupling. The enhanced field at the ring interface represents localized surface current accumulation and energy confinement, while the shadowed region behind the resonator indicates destructive interference between transmitted and reflected waves.

Overall, the simulation results clearly show that the eccentrically coupled double-ring resonator produces two distinct field-enhanced zones—one near each ring—and a pronounced shadowing region along the propagation path. This confirms its suitability for use as a unit absorber element or EM-shielding cell in larger resonant networks. The strong spatial localization of the E-field also suggests possible applications in near-field sensing and energy-harvesting structures where field confinement is desirable.

This pattern, typical of metallic inclusions with inductive and capacitive coupling, demonstrates energy confinement at the ring interface and destructive interference in the transmission zone. The double-ring configuration thus serves as an effective EM-shielding or absorption element.

5. Experimental Validation

Measurement results were obtained to validate the analytical and simulation models. The comparison shows strong agreement across all methods, confirming the reliability of the proposed approach. Laboratory measurements were conducted to validate analytical and simulated results using two prototypes (see Figure 12):

(a)

copper rings R₁ = 95 mm, R₂ = 66.5 mm (Model I);

(b)

steel rings R₁ = 45 mm, R₂ = 30 mm (Model II).

The ring resonator shown in Figure 12a was used to measure the resonant frequency, while the one shown in Figure 12b was used to measure the transmission coefficients. The measurement, the results of which are shown in Figure 13, was conducted to determine the resonant frequencies of all resonators used in this study: resonators with a single ring, R₁ and R₂ (Figure 13b), and a ring resonator with eccentric rings (Oo ring eccentric microwave resonator, Figure 13a).

Figure 14 shows that the measured results and the simulation calculations match very well. Variations in the measured results are due to the fact that the measurements were not carried out in a room without electromagnetic resonance, but in a laboratory with many reflections.

The measurement results are presented alongside the simulation and analytical calculation results in

Table 7. Values of calculated (analytical and numerical) and measured resonant frequencies for various resonators.

Ring Resonator		Analytical: fres, MHz (Equation (3))	Numerical: fres, MHz (HFSS)	* Experimental: fres, MHz
R1 (95.0 mm) R2 (66.5 mm) R1 + R2 (95.0 + 66.5) first mode R1 + R2 (95.0 + 66.5) second mode		513.00	566.16 ** (606.49) *** (569.39)	549.33
		739.74	727.89 ** (707.66) *** (706.48)	745.96
		489.20 **** 459.14	435.70 ** (408.67) *** (438.96)	482.24
		760.88 **** 688.97	707.60 ** 646.68 *** (642.54)	665.38

* Measured on a thin-wire resonator (r = 0.892 mm; MODEL I); ** Eigenmode simulation ($\omega$ = 4 mm; t = 10 mm; MODEL II); *** Eigenmode simulation (r = 0.892 mm; MODEL I). Note: Resonant frequency values without asterisks in the Analytical and Numerical columns are given for MODEL II; **** Calculation using the RLC model and both types of coupling (inductive and capacitive) with k = 0.445 and C₁₂ = 0.088 pF.

(column *Experimental). The results from all three methods (analytical, simulation, and measurement) correspond very well. Significant deviations occur only in the second mode of the resonator when comparing the analytical calculation with the numerical calculation and measurements. This is likely due to the use of a simplified analytical model that, among other limitations, does not account for capacitive coupling. It should be noted that the analytical calculation was performed prior to the construction of the resonator, serving as a guideline for its implementation. The simulation results obtained using the HFSS application model the resonator much more precisely and accurately, and the final simulation results are closer to the measured values.

In addition to determining the resonance frequencies of the individual rings and the annular eccentric resonator both analytically and through simulation, and verifying these results by measurement, measurements and simulation calculations of the transmission coefficient S₂₁ were performed for the derived resonator model with dimensions R₁ = 45.0 mm and R₂ = 30.0 mm to verify the simulation results.

The measured transmission parameters (S₂₁) closely matched the simulated values (Figure 14), with minor deviations attributed to environmental reflections. Table 7 compares the analytical, numerical, and measured resonant frequencies, showing strong consistency across all methods.

6. Conclusions

This paper presents an analytical, numerical, and experimental study of a microwave ring resonator composed of two eccentrically coupled conductive rings. Analytical predictions and HFSS simulations identified two resonances at approximately 436 MHz and 708 MHz, which were validated experimentally under laboratory conditions.

The electric field distribution analysis revealed pronounced localization of the E-field within the resonator structure at resonance, with simulated intensities exceeding 170 V/m, while the transmitted field behind the resonator was significantly reduced to below 13 V/m. This strong attenuation confirms the structure’s potential as an effective electromagnetic energy absorber or filter within the sub-1 GHz range. Experimental measurements validated the numerical results, with minor deviations attributed to environmental reflections and model simplifications.

The strong agreement among methods indicates that the proposed configuration can serve as a compact and tunable building block for resonant networks. By adjusting the geometric parameters of the resonator, it is possible to tune this structure for different frequency ranges.

This paper introduces a dual-ring eccentric configuration that expands the attenuation bandwidth below 1 GHz, combining analytical modeling, HFSS simulation, and experimental validation.

Compared to previously reported concentric or symmetrically coupled ring resonators, the proposed eccentric double-ring configuration introduces asymmetric coupling that enables tunable mode interaction, extended attenuation bandwidth, and improved field localization. This distinctive topology provides enhanced control over resonance characteristics without requiring complex multilayer geometries or additional loading materials offering a simpler, more compact, and highly efficient alternative to conventional designs.

The strong correlation between analytical, numerical, and experimental results validates the robustness of the developed model and demonstrates the predictive reliability of eccentric coupling theory. The results establish a new design paradigm for low-frequency resonant structures optimized for electromagnetic shielding, selective absorption, and energy localization applications.

Future research will focus on the implementation of multi-element eccentric resonator arrays, integration into metamaterial composites, and adaptive tuning mechanisms for broadband field control and reconfigurable shielding systems.