II. STRUCTURE, ANALYSIS, AND DESIGN

Figure 1 shows the proposed ring-cavity eight-way power combiner/divider. A coaxial taper feeding port has been applied to provide axially symmetric electromagnetic-field excitation for the ring-cavity power divider and to implement good amplitude and phase balance for the power-combining ports, which can also obtain good impedance matching from the coaxial port to the oversized ring cavity. The coaxial taper can be designed according to [Reference Song and Xue1]. The proposed ring-cavity power combiner/divider is terminated by the Sub-Miniature-A (SMA) connector (coaxial port). The power combiner/divider can be divided into three parts: the transition from input SMA connector to the oversized coaxial waveguide, the transition from the oversized waveguide to the ring cavity, and the transition from the ring cavity to the output SMA connector.

Fig. 1.

Proposed ring-cavity eight-way power divider: (a) sketch of the ring cavities with output ports and (b) structure of the power divider.

In general, the length of the coaxial probes is chosen to be normally about λg/4 to implement impedance matching, where λg is the wavelength at central frequency. However, for the capacitance-loaded coaxial probe, its length is far less than λg/4. As shown in Fig. 1, the length of L ₀ should be maintained as about λg/4 to make the outer side of the ring cavity be the short wall. So the width (R − R ₀) and height of the ring cavity are kept constant. That is to say, when the number of probes increases greatly, only the perimeter of the ring cavity increases, the section of the ring cavity keeps constant, and the higher-order modes cannot propagate in the ring cavity after an appropriate design. So, this type of power-combining structure is very suitable for large numbers of power-combining ports. The proposed ring power combiner/divider can be constructed and optimized in the three-dimensional electromagnetic simulation tools (such as Ansoft-HFSS), and the optimized structural dimensions of the proposed ring-cavity power combiner/divider can also be obtained.

When compared the proposed structure in Fig. 1(b) and the structure in [Reference Song and Xue1], stepped-impedance technology is used between the coaxial taper feeding port and the ring cavity to improve the impedance matching which will broaden the bandwidth. The approximate equivalent circuit of the proposed eight-way ring-cavity power divider is shown in Fig. 2. The stepped discontinuity from the output port of the coaxial taper to the ring cavity is modeled as a capacitive reactance −jX _S, which is marked by the dashed line. In the structure of [Reference Song and Xue1], the capacitive reactance X _S cannot be modulated when the size of the ring cavity is determined, while in the proposed structure of this paper, X _S, could be modulated easily (by modulating the size of L ₂ and R _s), that means the impedance matching between the coaxial taper feeding port and the ring cavity would be improved.

Fig. 2.

The approximate equivalent circuit of the proposed power divider.

In the equivalent circuit above, Z _rc is the input impedance of the ring cavity with inner probes, Γ_s is the reflection coefficient of the stepped impedance and ring cavity including the planar probe array, and Z _oc is the impedance of the extended coaxial. Based on the transmission-line theory, the reflection coefficient Γ_s can be given by

(1)$${\Gamma _s}=\displaystyle{{\left({\left({ - j{X_S}{Z_{rc}}} \right)/\left({ - j{X_S}+{Z_{rc}}} \right)} \right)- {Z_{oc}}} \over {\left({\left({ - j{X_S}{Z_{rc}}} \right)/\left({ - j{X_S}+{Z_{rc}}} \right)} \right)+{Z_{oc}}}}.$$

It can be seen that the reflection coefficient Γ_s is determined by X _S, Z _rc, and Z _oc. So the adjustability of X _S will improve the impedance matching greatly. Figure 3 shows the simulated S ₁₁ at different structural parameters. It can be seen that the stepped-impedance part could improve the impedance match effectively.

Fig. 3.

The simulated S ₁₁ at different structural parameters: (a) L _s and (b) R _s.

The characteristics of the proposed structure can be analyzed by the microwave network theory. As it is known, for the n-port lossless reciprocal network, there is

(2)$$\sum\limits_{k=1}^N {{S_{ki}}S_{ki}^\ast }={\delta _{ij}}.$$

If i = j, then δ_ij = 1; if i ≠ j, then δ_ij = 0. That is

(3)$$\left\{{\matrix{ {\sum\limits_{k\,=\,1}^N {{S_{ki}}S_{ki}^\ast =1\comma \; } } \cr {\sum\limits_{k\,=\,1}^N {{S_{ki}}S_{kj}^\ast =0\comma \; \quad i \ne j.} } \cr } } \right.$$

For the proposed ring-cavity eight-way power combiner/divider in this paper, its structure is axially symmetric. Port 1 is set as the input port, and the last n ports are set as the output ports in turn (shown in Fig. 1(a)). Assuming that the input port is impedance matched, the S-parameter matrix of this kind of axially symmetric power combiner/divider could be given as

(4)$$S=\left({\matrix{ 0 & {{S_{1n}}} & {{S_{1n}}} & \cdots & {{S_{1n}}} \cr {{S_{1n}}} & {{S_{22}}} & {{S_{23}}} & \cdots & {{S_{2n}}} \cr {{S_{1n}}} & {{S_{32}}} & {{S_{33}}} & \cdots & {{S_{3n}}} \cr \cdots & \cdots & \cdots & \cdots & \cdots \cr {{S_{1n}}} & {{S_{n2}}} & {{S_{n3}}} & \cdots & {{S_{nn}}} \cr } } \right).$$

This is an (n + 1)-order square matrix [Reference Kagan16]. If this structure is lossless, the above matrix would be the unitary matrix. So according to equation (3), there will be

(5)$${\left\vert {{S_{1n}}} \right\vert ^2}=\displaystyle{1 \over n}\comma \;$$

(6)$${\left\vert {{S_{1n}}} \right\vert ^2}+{\left\vert {{S_{22}}} \right\vert ^2}+{\left\vert {{S_{32}}} \right\vert ^2}+\cdots+{\left\vert {{S_{n2}}} \right\vert ^2}=1\comma \;$$

(7)$${S_{1n}}\left({S_{_{22} }^\ast +S_{_{32} }^\ast +\cdots+S_{_{n2} }^\ast } \right)=0.$$

Here, as the structure is axially symmetric, there is

(8)$$\left\vert {{S_{i\comma j}}} \right\vert =\left\vert {{S_{i\comma n+4 - j}}} \right\vert \comma \; \quad \left\vert {{S_{i\comma j}}} \right\vert =\left\vert {{S_{i+1\comma j+1}}} \right\vert .$$

According to equations (6) and (8), it could be concluded that the return loss of the output port is in correspondence with the isolation of the output port. In general, the isolation of the output port is not equal, but they are all around the average value. So the derivation of this average value can provide a certain reference. It can be given by

(9)$${\left\vert {{S_{ij}}} \right\vert ^2}=\displaystyle{{n - 1} \over {{n^2}}}\comma \; \quad i \ne 1\comma \; \; i \ne j.$$

As to the proposed ring-cavity eight-way power combiner/divider, n is equal to 8, so the average value of isolation and return loss of the output ports is

(10)$$10\lg \left({{{\left\vert {{S_{ij}}} \right\vert }^2}} \right)=- 9.6\, {\rm dB}\quad \left({n=8\comma \; \; i \ne 1\comma \; \; i \ne j} \right).$$

Table 1 shows some average values of several different n (n is the number of the output ports). From Table 1, it can be seen that the power divider/combiner designed by this structure (axially symmetric) is not suitable for the power divider/combiner with fewer output ports, as the isolation or the return loss of the output port could not reach the requirement of some systems. But, to the multi-way power divider's design, this issue will not exist.

Table 1.

Average value with different n.

III. RESULTS AND DISCUSSION

According to the above analysis, the proposed ring-cavity eight-way power combiner/divider is designed, simulated, and optimized using the electromagnetic simulation tool Ansoft-HFSS. The optimized dimensions of the proposed power combiner/divider are listed in Table 2 (as shown in Fig. 1). The ring-cavity eight-way power dividing structure has been fabricated by machining of a ring cavity and a coaxial taper. In addition, the coaxial probes are machined and inserted inside the ring cavity at the designed locations. The assembly and overview of the fabricated power divider is shown in Fig. 4.

Fig. 4.

Photograph of the fabricated power divider.

Table 2.

Optimized dimensions of the ring-cavity power divider (unit: millimetre).

The fabricated power divider has been measured by using an Agilent network analyzer. The simulated and measured reflection coefficients of the fabricated power divider are shown in Fig. 5, which also include the simulated transmission coefficient between the input port and one of the output ports (the measured transmission coefficients are shown in Fig. 7(a)). Only insertion loss S ₂₁ is plotted in Fig. 5 and the insertion losses between port 1 and the other ports are the same as S ₂₁ because of the n-fold symmetry with respect to the input port axis. It can be seen that the measured results agree with the simulated ones closely. The simulated and measured −10 dB return loss bandwidths are 13.6 GHz (from 5.3 to 18.9 GHz) and 13.4 GHz (from 5.2 to 18.6 GHz), respectively. The difference between the simulated and measured S ₁₁ is most likely attributed to the fabrication and assembly. We have found that there is a mistake for the length L ₂ when the power divider was fabricated. In fact, L ₂ should be equal to 1.8 mm for an optimized power divider. However, L ₂ of the fabricated power divider was equal to 1.2 mm, which greatly affects S ₁₁. As shown in Fig. 6, the measured S ₁₁ of the fabricated power divider is close to the simulated S ₁₁ for L ₂ = 1.2 mm.

Fig. 5.

Simulated and measured results of the proposed power divider.

Fig. 6.

Simulated and measured results of S ₁₁ with different values of L ₂.

Fig. 7.

Measured transmission coefficients of the fabricated coaxial power divider (n = 2, 3, …, 8): (a) amplitude and (b) phase.

Figure 7 shows the measured transmission characteristics of the fabricated power divider. The average insertion loss is around 9.4 dB (including the 9-dB power-dividing insertion loss). A maximum amplitude imbalance of ±0.7 dB and a phase imbalance of ±6° are observed over the entire band. The amplitude and phase imbalance is due to the fabrication errors. Moreover, the comparison of the presented power combiner/divider with other designs is summarized in Table 3. It can be seen that the novel power combiner/divider presented in this paper has a wider bandwidth and low insertion loss, good amplitude, and phase balance.

Table 3.

Comparison with some prior power dividers.

RBW: relative bandwidth; AIL: average insertion loss; A/PI: amplitude/phase imbalance.