Design of Third-Order Dual-Band BPF With a Tunable Lower Band Using Third-Harmonic Dual-Null-Points Loading Scheme on λ/4 UIR

This letter presents a reconfigurable third-order dual-band bandpass filter (BPF) that features independent frequency tuning of a lower passband with constant absolute bandwidth (CABW) and a fixed upper passband. A combline structure using a third-harmonic (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${f} _{3}$ </tex-math></inline-formula>) dual-null-point semi-lumped loading scheme on quarter-wavelength (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\lambda $ </tex-math></inline-formula>/4) uniform impedance resonator (UIR) is proposed. This configuration enables frequency tuning of the lower band at fundamental frequency (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${f} _{1}$ </tex-math></inline-formula>) and the fixing of the upper band at <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${f} _{3}$ </tex-math></inline-formula> by series-loading varactors at the current null point (CNP) at <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${f} _{3}$ </tex-math></inline-formula>. Meanwhile, the coupling coefficient of the lower band can be controlled to meet the requirements of CABW by parallel-loading lumped inductors between each two resonators and located at their voltage null points (VNPs) at <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${f} _{3}$ </tex-math></inline-formula>. The mutual independence of parallel- and series-loading at the VNP and CNP is advantageous, as both lumped loadings do not affect the upper band entirely, including frequency and ABW. Based on these, the fabricated BPF exhibits a frequency-tuning range (TR) of 52.1% with a CABW of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$150~\pm ~6$ </tex-math></inline-formula> MHz in the lower band, while the upper band maintains a fixed frequency and an ABW of 150 MHz, which shows good agreements between simulated and measured results.

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Publication Details

Journal
IEEE Microwave and Wireless Technology Letters
Published
2025-03-05
DOI
https://doi.org/10.1109/lmwt.2025.3545809
Citations
4
Primary Topic
Optical Systems and Laser Technology
Type
article
Field-Weighted Citation Impact
2.92

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article

Design of Third-Order Dual-Band BPF With a Tunable Lower Band Using Third-Harmonic Dual-Null-Points Loading Scheme on λ/4 UIR

Wei Qin, Qing‐Yuan Lu, Jing Cai, Jian‐Xin Chen
4 citations
IEEE Microwave and Wireless Technology Letters
Optical Systems and Laser Technology
2.92
article

Design of Third-Order Dual-Band BPF With a Tunable Lower Band Using Third-Harmonic Dual-Null-Points Loading Scheme on λ/4 UIR

Wei Qin, Qing‐Yuan Lu, Jing Cai, Jian‐Xin Chen
article en
4 citations

Abstract

This letter presents a reconfigurable third-order dual-band bandpass filter (BPF) that features independent frequency tuning of a lower passband with constant absolute bandwidth (CABW) and a fixed upper passband. A combline structure using a third-harmonic (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${f} _{3}$ </tex-math></inline-formula>) dual-null-point semi-lumped loading scheme on quarter-wavelength (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\lambda $ </tex-math></inline-formula>/4) uniform impedance resonator (UIR) is proposed. This configuration enables frequency tuning of the lower band at fundamental frequency (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${f} _{1}$ </tex-math></inline-formula>) and the fixing of the upper band at <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${f} _{3}$ </tex-math></inline-formula> by series-loading varactors at the current null point (CNP) at <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${f} _{3}$ </tex-math></inline-formula>. Meanwhile, the coupling coefficient of the lower band can be controlled to meet the requirements of CABW by parallel-loading lumped inductors between each two resonators and located at their voltage null points (VNPs) at <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${f} _{3}$ </tex-math></inline-formula>. The mutual independence of parallel- and series-loading at the VNP and CNP is advantageous, as both lumped loadings do not affect the upper band entirely, including frequency and ABW. Based on these, the fabricated BPF exhibits a frequency-tuning range (TR) of 52.1% with a CABW of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$150~\pm ~6$ </tex-math></inline-formula> MHz in the lower band, while the upper band maintains a fixed frequency and an ABW of 150 MHz, which shows good agreements between simulated and measured results.

IEEE Microwave and Wireless Technology LettersVol. 35(5)
Nantong University (CN)
National Natural Science Foundation of China
Openalex Percentile: Top 10%
Optical Systems and Laser Technology
2.92
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