ZTE Communications ›› 2026, Vol. 24 ›› Issue (1): 88-96.DOI: 10.12142/ZTECOM.202601012
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Xiong Zhi’ang1, Fan Jiyuan1, Zhao Ping1(
), Zhou Jinzhu1, Shen Nan2, Wu Qingqiang2
Received:2024-03-20
Online:2026-03-25
Published:2026-03-17
About author:Xiong Zhi'ang received his BS degree from Jiangxi University of Science and Technology, China in 2021, and the master's degree from Xidian University, Xi'an, China in 2024. His current research interests include mixed electric and magnetic coupling filters and modeling and optimization of microwave passive filters.Supported by:Xiong Zhi’ang, Fan Jiyuan, Zhao Ping, Zhou Jinzhu, Shen Nan, Wu Qingqiang. Synthesis and Design of Generalized Strongly Coupled Resonator Quartet Combline Filters with Redundant Resonance[J]. ZTE Communications, 2026, 24(1): 88-96.
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URL: https://zte.magtechjournal.com/EN/10.12142/ZTECOM.202601012
Figure 2 Iterations of Remez-like algorithm in solving the equi-ripple function for the 7th-order filter with an out-of-band RZ: (a) the first iteration; (b) the second iteration; (c) the third iteration; (d) the fourth iteration
| si, i = | F(s) (F22(s)) | P(s) | E(s) |
|---|---|---|---|
| 0 | 0.373 8j | 1.700 0 | 0.868 3 + 3.731 5j |
| 1 | 0.422 9 | 0.110 0j | 2.769 1 +12.801 1j |
| 2 | 5.464 5j | 1.000 0 | 4.956 1 + 24.638 4j |
| 3 | 2.012 0 | 6.466 5 + 30.408 0j | |
| 4 | 13.070 5j | 5.796 9 + 28.889 2j | |
| 5 | 2.613 9 | 4.560 8 + 16.045 3j | |
| 6 | 8.137 5j | 1.973 3 + 8.137 5j | |
| 7 | 1.000 0 | 1.000 0 | |
| εR = 1.000 0 | ε = 0.445 8 | ||
Table 1 Coefficients of F(s), P(s), and E(s) of seven-poles with one upper TZ and one lower TZ
| si, i = | F(s) (F22(s)) | P(s) | E(s) |
|---|---|---|---|
| 0 | 0.373 8j | 1.700 0 | 0.868 3 + 3.731 5j |
| 1 | 0.422 9 | 0.110 0j | 2.769 1 +12.801 1j |
| 2 | 5.464 5j | 1.000 0 | 4.956 1 + 24.638 4j |
| 3 | 2.012 0 | 6.466 5 + 30.408 0j | |
| 4 | 13.070 5j | 5.796 9 + 28.889 2j | |
| 5 | 2.613 9 | 4.560 8 + 16.045 3j | |
| 6 | 8.137 5j | 1.973 3 + 8.137 5j | |
| 7 | 1.000 0 | 1.000 0 | |
| εR = 1.000 0 | ε = 0.445 8 | ||
| Rotation sequence | Elements to be annihilated | Pivot [i, j] | Rotation sequence | Elements to be annihilated | Pivot [i, j] |
|---|---|---|---|---|---|
| 1 | MS7 | [7, 6] | 16 | M37 | [7, 6] |
| 2 | MS6 | [6, 5] | 17 | M36 | [6, 5] |
| 3 | MS5 | [5, 4] | 18 | M35 | [5, 4] |
| 4 | MS4 | [4, 3] | 19 | M47 | [7, 6] |
| 5 | MS3 | [3, 2] | 20 | M46 | [6, 5] |
| 6 | MS2 | [2, 1] | 21 | M57 | [7, 6] |
| 7 | M17 | [7, 6] | 22 | M5L | [ |
| 8 | M16 | [6, 5] | 23 | M6L | [ |
| 9 | M15 | [5, 4] | 24 | M46 | [ |
| 10 | M14 | [4, 3] | 25 | M47 | [ |
| 11 | M13 | [3, 2] | 26 | M57 | [ |
| 12 | M27 | [7, 6] | 27 | M35 | [ |
| 13 | M26 | [6, 5] | 28 | M36 | [ |
| 14 | M25 | [5, 4] | 29 | M46 | [ |
| 15 | M24 | [4, 3] | 30 | M34 | [ |
Table 2 Rotation sequence to the filter in Fig. 4a
| Rotation sequence | Elements to be annihilated | Pivot [i, j] | Rotation sequence | Elements to be annihilated | Pivot [i, j] |
|---|---|---|---|---|---|
| 1 | MS7 | [7, 6] | 16 | M37 | [7, 6] |
| 2 | MS6 | [6, 5] | 17 | M36 | [6, 5] |
| 3 | MS5 | [5, 4] | 18 | M35 | [5, 4] |
| 4 | MS4 | [4, 3] | 19 | M47 | [7, 6] |
| 5 | MS3 | [3, 2] | 20 | M46 | [6, 5] |
| 6 | MS2 | [2, 1] | 21 | M57 | [7, 6] |
| 7 | M17 | [7, 6] | 22 | M5L | [ |
| 8 | M16 | [6, 5] | 23 | M6L | [ |
| 9 | M15 | [5, 4] | 24 | M46 | [ |
| 10 | M14 | [4, 3] | 25 | M47 | [ |
| 11 | M13 | [3, 2] | 26 | M57 | [ |
| 12 | M27 | [7, 6] | 27 | M35 | [ |
| 13 | M26 | [6, 5] | 28 | M36 | [ |
| 14 | M25 | [5, 4] | 29 | M46 | [ |
| 15 | M24 | [4, 3] | 30 | M34 | [ |
Figure 5 Frequency responses of three filter designs: the 7th-order filter with an out-of-band reflection zero (solid), 6th-order traditional filter (dashed), and 7th-order traditional filter (dotted)
| k | poles | zeros |
|---|---|---|
| 1 | -0.692 7 + 0.104 7i | 0.001 0 + 0.072 2i |
| 2 | -0.556 11-0.675 5i | -0.000 1-0.530 2i |
| 3 | -0.481 2 + 0.805 7i | -0.000 5 + 0.657 6i |
| 4 | -0.180 53-1.073 5i | -0.000 7-0.889 7i |
| 5 | -0.156 41 + 1.149 1i | 0.000 3 + 1.000 2i |
| 6 | -0.009 1-11.503 2i | 0.000 0-11.503 1i |
| 7 | 1.132 2 + 14.087 9i | 1.664 5 + 13.927 9i |
| 8 | -26.468 1 + 3.616 4i | 26.542 8 + 3.463 7i |
Table 3 Zeros and poles of VF results for S11
| k | poles | zeros |
|---|---|---|
| 1 | -0.692 7 + 0.104 7i | 0.001 0 + 0.072 2i |
| 2 | -0.556 11-0.675 5i | -0.000 1-0.530 2i |
| 3 | -0.481 2 + 0.805 7i | -0.000 5 + 0.657 6i |
| 4 | -0.180 53-1.073 5i | -0.000 7-0.889 7i |
| 5 | -0.156 41 + 1.149 1i | 0.000 3 + 1.000 2i |
| 6 | -0.009 1-11.503 2i | 0.000 0-11.503 1i |
| 7 | 1.132 2 + 14.087 9i | 1.664 5 + 13.927 9i |
| 8 | -26.468 1 + 3.616 4i | 26.542 8 + 3.463 7i |
| Resonator ID | T1 | T2 | T3 | T4 | T5 | T6 | T12 | T25 | T56 |
|---|---|---|---|---|---|---|---|---|---|
| Final/mm | 4.70 | 3.55 | 9.10 | 4.7 | 3.55 | 4.70 | 1.70 | 2.00 | 2.00 |
| Dimension | d12 | d25_1 | d25_2 | d34_1 | d34_2 | Hport | |||
| Final/mm | 1.77 | 7.55 | 7.55 | 6.40 | 11.43 | 6.32 |
Table 4 Dimensions of the filter in Fig. 8
| Resonator ID | T1 | T2 | T3 | T4 | T5 | T6 | T12 | T25 | T56 |
|---|---|---|---|---|---|---|---|---|---|
| Final/mm | 4.70 | 3.55 | 9.10 | 4.7 | 3.55 | 4.70 | 1.70 | 2.00 | 2.00 |
| Dimension | d12 | d25_1 | d25_2 | d34_1 | d34_2 | Hport | |||
| Final/mm | 1.77 | 7.55 | 7.55 | 6.40 | 11.43 | 6.32 |
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