The article proposes three lumped-distributed resonators, each of which introduces two transmission zeros (TZ) at real frequencies into the transfer function of inline bandpass filter (BPF). The use of such resonators in mixed-coupled BPFs without cross-coupling increases the number of TZs from ( <tex-math notation="LaTeX">$N + 1$</tex-math> ) to (3 <tex-math notation="LaTeX">$N + 1$</tex-math> ). It improves the filter performance. Lumped-distributed resonators represent a stepped-impedance or uniform transmission line segment to which one capacitance or inductance is connected in cascade. These resonators have two antiresonant frequencies <tex-math notation="LaTeX">ω ₚ₁</tex-math> , <tex-math notation="LaTeX">ω ₚ₂</tex-math> , which are placed next to the main resonant frequency <tex-math notation="LaTeX">ω ₀</tex-math> , which leads to two TZs. Antiresonant frequencies <tex-math notation="LaTeX">ω ₚ₁</tex-math> , <tex-math notation="LaTeX">ω ₚ₂</tex-math> are the poles of the input admittance <tex-math notation="LaTeX">Y(jω )</tex-math> , their position is controlled by the parameters of the resonators. Lumped-distributed resonators can form equidistant TZ pairs, including those of higher degree, allowing the implementation of BPFs with quasielliptic frequency responses and improved selectivity. It has been established that reducing Q-factors of inductor <tex-math notation="LaTeX">QL</tex-math> and capacitor <tex-math notation="LaTeX">QC</tex-math> do not increase the insertion loss in the passband of BPF. A design method for BPF with mixed couplings between adjacent resonators is established. It is also suitable for filters that use the proposed resonators. As result, the TZ number of such BPFs is increased from ( <tex-math notation="LaTeX">N</tex-math> <tex-math notation="LaTeX">$+$</tex-math> 1) to (3 <tex-math notation="LaTeX">$N + 1$</tex-math> ).
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Zakharov et al. (2024) studied this question.
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