Wide Stopband Attenuation Design of 5G Cavity Lowpass Filters

Power amplifiers (PAs) in 5G transmit paths inevitably generate 2nd, 3rd, and higher-order harmonic and wideband spurious components alongside the desired output signal. Without suppression, these violate the spurious emission limits of 3GPP TS 38.104 for base stations and interfere with adjacent frequency bands. Cavity Lowpass Filters (Cavity LPFs) — offering low insertion loss, high power handling, and excellent shielding — are the key hardware solution for harmonic suppression and wideband noise management. This paper focuses on Wide Stopband Attenuation as the core metric, systematically clarifying the physical distinction and design trade-offs between stopband attenuation and insertion loss (IL); comparing the effects of Chebyshev and Elliptic filter responses on cutoff roll-off and transmission zeros; reviewing multi-section cascade, spurious mode management, and Stepped Impedance Resonator (SIR) techniques for achieving wide stopbands; and using the Temwell Standard Cavity Lowpass Filter (STLP series) as a practical case study to analyze the ≥ 60 dB stopband attenuation specification and measurement verification workflow for 5G Sub-6 GHz transmit paths. A regulatory-driven, step-by-step framework for stopband attenuation specification is proposed as an industry design reference.
1. Introduction: Lowpass Filters in Harmonic Suppression and Noise Management
In the 5G transmit path, the power amplifier (PA) is the primary source of nonlinear distortion. In addition to the desired output signal, the PA generates 2nd, 3rd, and higher-order harmonics; if these are not effectively suppressed, they interfere with adjacent frequency bands and violate 3GPP regulatory requirements.
Cavity Lowpass Filters (Cavity LPFs) are the core components addressing this problem, serving two main functions:
- Harmonic Suppression: Suppress the 2nd and 3rd harmonics at the PA output to below regulatory limits.
- Wideband Noise Management: Suppress broadband spurious emissions in the transmit path to maintain spectral purity.
3GPP TS 38.104 explicitly specifies spurious emission limits for 5G NR base stations: −57 dBm (100 kHz measurement bandwidth) in the 30 MHz–1 GHz range; −47 dBm (1 MHz measurement bandwidth) in the 1 GHz–12.75 GHz range, with some bands requiring test extension to the 5th harmonic or 12.75 GHz. Positioned at the 5G transmit front-end, the Cavity LPF is the most direct hardware solution for meeting these regulatory targets. The design priority for a lowpass filter is not to set the cutoff frequency as low as possible, but rather to achieve the optimal balance among passband loss, transition band slope, stopband attenuation, power handling, size, and cost.
2. Attenuation Definitions: Fundamental Distinction Between Stopband Attenuation and Insertion Loss
In RF filter specifications, the term "attenuation" is often used ambiguously. However, Insertion Loss (IL) and Stopband Attenuation (As) differ fundamentally in physical meaning and design objectives, and must be clearly distinguished. Figure 1 marks both on a single S21 curve.
2.1 Insertion Loss (IL)
Insertion Loss describes the energy loss within the passband — the attenuation of the useful signal after passing through the filter: IL = −20·log₁₀|S₂₁| (dB, in-band). Lower values are better; ideally approaching 0 dB. A typical excellent standard is ≤ 0.5 dB; values exceeding 3 dB indicate poor design. Sources include conductor loss, dielectric loss, and mismatch loss.
2.2 Stopband Attenuation (As)
Stopband Attenuation describes the suppression capability against unwanted signals in the stopband: As = −20·log₁₀|S₂₁| (dB, in stopband). Higher values are better, indicating stronger harmonic suppression capability. Typical design targets range from ≥ 40 dB (basic requirement) to ≥ 60 dB (high-performance base station). Specification sheets often label this as "Stop Band Rejection" or "Attenuation."
2.3 Core Design Trade-off
Insertion Loss and Stopband Attenuation are not independent parameters — a fundamental design trade-off exists between them, as summarized in Table 1.
| Comparison Dimension | Insertion Loss (IL) | Stopband Attenuation (As) |
|---|---|---|
| Operating Band | Passband | Stopband |
| Ideal Direction | Lower is better (→ 0 dB) | Higher is better (→ ∞ dB) |
| Impact if Poor | Signal power loss, degraded noise figure | Harmonic / interference leakage into adjacent bands |
| Key Design Lever | Q factor, resonator quality | Filter order N, number of transmission zeros |
| Trade-off Relationship | Improving As → IL often increases | Reducing IL → As typically decreases |
3. Design Techniques: Effect of Chebyshev and Elliptic Responses on Attenuation Characteristics
The transfer function design of a lowpass filter directly determines its attenuation characteristics. In practice, the Chebyshev and Elliptic (Cauer) responses are most commonly used. A comparison of their cutoff roll-off and stopband behavior is shown in Figure 2.
3.1 Chebyshev Response
The Chebyshev filter uses an equal-ripple design: the passband allows a finite-amplitude ripple (typically 0.1–1 dB); stopband attenuation increases monotonically with no transmission zeros; the cutoff slope is steeper than a same-order Butterworth but not as steep as Elliptic. Its attenuation function is |S₂₁(jω)|² = 1 / [1 + ε²·T_N²(ω/ω_c)], where T_N is the Nth-order Chebyshev polynomial and ε controls the passband ripple. For Cavity LPFs, the Chebyshev response provides the most practical balance between passband ripple and stopband roll-off, making it the most common implementation choice.
3.2 Elliptic (Cauer) Response
The Elliptic filter introduces finite Transmission Zeros into the transfer function, achieving theoretically infinite attenuation at specific frequencies: both passband and stopband have ripple (equiripple stopband); the transition band slope is the steepest of all response types — providing the fastest cutoff for the same order; phase linearity is the worst, making it unsuitable for systems with strict group delay requirements.
3.3 Practical Selection Guidelines
| Characteristic | Butterworth | Chebyshev | Elliptic (Cauer) |
|---|---|---|---|
| Passband Ripple | None (maximally flat) | Controlled ripple | Yes |
| Stopband Attenuation | Monotonically increasing | Monotonically increasing | Multiple transmission zeros |
| Transition Band Slope | Slowest | Moderate | Steepest |
| Order for Same Steepness | Highest | Moderate | Lowest |
| Phase Linearity | Best | Moderate | Worst |
| 5G Harmonic Suppression Suitability | Fair | ✔ Primary choice | ✔ When steeper transition required |
Conclusion: 5G Cavity LPF design typically favors the Chebyshev response, which provides sufficient stopband attenuation (≥ 60 dB) while maintaining low insertion loss. When the system requires an extremely steep transition band near the cutoff frequency (e.g., Sub-6 GHz closely adjacent interference bands), the Elliptic response is the more efficient choice.
4. Wide Stopband Implementation: Multi-Section Cascade and Spurious Frequency Management
The stopband width of a single cavity resonator is naturally limited because the cavity itself has higher-order modes that form spurious passbands within the stopband, interrupting stopband attenuation. Achieving a "wide and continuous" stopband is one of the greatest engineering challenges in Cavity LPF design, as illustrated in Figure 3.
4.1 Method 1: Multi-Section Cascade
The most straightforward wide-stopband approach is to cascade two or more sub-filters, distributing their transmission zeros across different frequencies to cover a wider stopband range. Each additional order N adds approximately 20 dB/decade to the roll-off rate; cascading two complementary sub-filters distributes transmission zeros quasi-periodically across the entire stopband. The trade-off is increased volume, higher insertion loss, and greater sensitivity to manufacturing tolerances. Research from Cambridge indicates that arranging cavity elements in quasi-periodic arrays combined with TEM and TM coupled resonances can achieve an ultra-wide, continuously spurious-free stopband while maintaining low insertion loss.
4.2 Method 2: Spurious Mode Management
Higher-order spurious modes of cavity resonators (e.g., TE₁₀₂, TE₂₀₂) are the fundamental cause of stopband narrowing. Common suppression techniques include:
- Mode Staggering: Adjust individual cavity dimensions to offset the higher-order mode resonant frequencies of adjacent cavities, preventing spurious passbands from forming at the same frequency.
- Mixed EM Coupling: Select specific weak coupling points between electric coupling windows and magnetic coupling slots to selectively suppress particular higher-order modes.
- Orthogonal Feeding: Use orthogonal input/output port layouts at different layers to naturally block excitation of higher-order modes.
4.3 Method 3: Stepped Impedance Resonator (SIR)
By alternating high-impedance (High-Z) and low-impedance (Low-Z) transmission line sections, the spurious resonance positions can be artificially controlled, pushing parasitic passbands to higher frequencies and thus extending the effective stopband width. In 5G Sub-6 GHz applications, this is a practical approach for balancing size and stopband performance.
5. Temwell Case Study: Cavity Lowpass Filter Attenuation Specifications in 5G Transmit Paths
The Temwell Standard Cavity Lowpass Filter (STLP series) is designed for high-frequency applications above 1 GHz, covering a broad range from DC to 60 GHz. Figure 4 shows a representative S21 response for 5G Sub-6 GHz, and Table 3 provides the actual specification comparison.
5.1 STLP Series 5G-Related Specification Comparison
| Part Number | Cutoff Frequency | Insertion Loss | VSWR | Stopband Attenuation | Power |
|---|---|---|---|---|---|
| STLP-DC-3.5GA57 | 3.5 GHz | ≤ 1.0 dB | ≤ 1.3:1 | ≥ 60 dB @ 4.05–11.5 GHz | 15 W |
| STLP-DC-3.75GA58 | 3.75 GHz | ≤ 1.0 dB | ≤ 1.3:1 | ≥ 60 dB @ 4.25–11.8 GHz | 15 W |
| STLP-DC-4GA33 | 4.0 GHz | ≤ 1.0 dB | ≤ 1.3:1 | ≥ 60 dB @ 4.5–12.3 GHz | 15 W |
| STLP-DC-4.5GA60 | 4.5 GHz | ≤ 1.0 dB | ≤ 1.3:1 | ≥ 60 dB @ 5.1–13.7 GHz | 15 W |
| STLP-DC-5GA61 | 5.0 GHz | ≤ 1.0 dB | ≤ 1.3:1 | ≥ 60 dB @ 5.58–15 GHz | 15 W |
5.2 Specification Interpretation
Taking the STLP-DC-3.5GA57 (3.5 GHz cutoff, corresponding to 5G NR Band n78) as an example: Insertion Loss ≤ 1.0 dB indicates minimal useful signal loss within the passband (DC–3.5 GHz); Stopband Attenuation ≥ 60 dB @ 4.05–11.5 GHz means that from approximately 1.16× the cutoff frequency onward, all frequencies receive at least 60 dB attenuation, suppressing the 2nd harmonic (7.0 GHz) and 3rd harmonic (10.5 GHz) by more than 60 dB. Stopband coverage extends to approximately 3.3× the passband frequency range, fully satisfying the 3GPP requirement to test up to 12.75 GHz.
Another high-frequency example, STLP-DC-12.5GA73 (12.5 GHz cutoff), provides IL ≤ 1.0 dB and stopband attenuation ≥ 50 dB @ 13.7–20 GHz, suitable for millimeter-wave harmonic suppression at the front end.
For comparison, the Temwell DC-200 MHz LC LPF offers IL ≤ 0.5 dB, stopband attenuation ≥ 40 dB @ 600–1000 MHz, and power handling up to 50 W. The LC type is more compact but provides lower stopband attenuation depth (40 dB) and narrower stopband coverage than the cavity type (60 dB), highlighting the superiority of cavity structures for high stopband attenuation requirements.
6. Measurement Verification: Reading S21 Stopband Data with a Vector Network Analyzer
The attenuation performance of Cavity LPFs is primarily characterized via S-parameter measurements using a Vector Network Analyzer (VNA). The VNA is a two-port instrument that transmits swept-frequency signals of known power and simultaneously measures reflection (S11) and transmission (S21), fully describing the linear characteristics of the filter in complex form (magnitude + phase). The reading procedure and key markers are shown in Figure 5.
6.1 Stopband S21 Reading Procedure
- Calibration: Perform SOLT (Short-Open-Load-Through) or TRL calibration before measurement to eliminate parasitic effects from test cables and connectors.
- Frequency Range Setup: For 5G Sub-6 GHz Cavity LPFs, sweep from DC (100 kHz) to at least 15 GHz to cover the 4th harmonic and beyond.
- Dynamic Range Verification: When measuring ≥ 60 dB stopband attenuation, VNA dynamic range must be at least 80 dB (20 dB margin) to ensure results are not limited by noise floor.
- Reading Stopband Data: S21 in the passband region should be near 0 dB (e.g., −0.8 dB indicates IL of 0.8 dB); in the stopband region it drops sharply (e.g., −62 dB indicates stopband attenuation of 62 dB).
- Mark Key Points: Use Markers to identify the cutoff frequency (−3 dB point), the stopband start frequency, and the actual attenuation at each harmonic frequency.
6.2 Common Measurement Pitfalls
- Connector Leakage: When SMA connectors are not fully tightened, fixture leakage paths appear near the 60 dB attenuation level, preventing the stopband floor from meeting spec. Verify mechanical connection quality.
- Impedance Mismatch: If passband VSWR exceeds specification (e.g., > 1.5:1), IL will increase. Confirm test environment matches the 50 Ω system impedance.
7. Conclusions: Attenuation Specification Recommendations
Defining the stopband attenuation specification for 5G Cavity Lowpass Filters requires simultaneous consideration of three dimensions: regulatory requirements, system link budget, and achievability. The following step-by-step specification framework is proposed.
7.1 Specification Framework
| 5G Band | Fundamental Frequency | Coverage Required Up To | Recommended Cutoff Frequency |
|---|---|---|---|
| n78 (5G Sub-6 GHz) | 3.3–3.8 GHz | 4th harmonic (~15.2 GHz) | 3.5 GHz (STLP-DC-3.5GA57) |
| n77 (C-Band) | 3.7–4.2 GHz | 3rd harmonic (~12.6 GHz) | 4.0 GHz (STLP-DC-4GA33) |
| ISM 5.8 GHz | 5.725–5.875 GHz | 2nd harmonic (~11.75 GHz) | 6.0 GHz (STLP-DC-6GA42) |
7.2 Core Principles for Wide Stopband Design
- Prefer Chebyshev response: In Cavity LPF implementations, Chebyshev provides the best monotonic stopband attenuation and design predictability.
- Enhance transition band with transmission zeros: When an extremely steep transition band is required, use Elliptic or Generalized Chebyshev response to introduce finite transmission zeros near the cutoff frequency.
- Use multi-section cascades for wide stopband requirements: The effective stopband of a single section is typically 2–3× the passband frequency. When coverage to the 5th harmonic is required, a two-section cascade should be considered.
- Spurious modes are the primary design variable: Higher-order TE/TM modes form spurious passbands within the stopband; manage them through mode staggering, orthogonal feeding, or dimensional optimization.
- Measurement is more critical than simulation: Cavity machining tolerances (±0.1–0.3 mm), contact resistance, and surface treatment all affect actual stopband depth. All specifications must be verified by VNA measurement.
Summary: Stopband attenuation is not a single-frequency specification, but a systematic metric encompassing stopband start frequency, bandwidth coverage, and attenuation depth. With more than 25 years of RF filter production experience, Temwell possesses immediately deployable R&D capabilities in high-Q cavity design, spurious mode suppression, transmission zero placement, and VNA measurement verification — delivering customized Cavity Lowpass Filter solutions for 5G transmit paths that combine low insertion loss with wide stopband attenuation.
Appendix - Complete source FAQ
FAQ: Wide Stopband Attenuation Design of 5G Cavity Lowpass Filters (A-03)
This FAQ is compiled from the theory, the specifications in Tables 1–4, and the Temwell STLP series product data presented in this paper (Article No. A-03). Unless otherwise noted, all figures are taken from Temwell product specification pages and 3GPP TS 38.104 regulatory values. Items marked [Supplement] are extended notes added after cross-checking against the main text.
Category 1: Technical Specifications and Design
- Which band and bandwidth does this filter design primarily support?
The Temwell Standard Cavity Lowpass Filter (STLP series) covers DC to 60 GHz. 5G-related models such as the STLP-DC-3.5GA57 (cutoff frequency 3.5 GHz, passband DC-3.5 GHz) correspond to the 5G NR n78 band.
[Supplement] A lowpass filter has no "center frequency / bandwidth"; its passband is defined by the single cutoff-frequency parameter. Per Table 3, the 5G-related STLP models span five cutoff frequencies — 3.5 / 3.75 / 4.0 / 4.5 / 5.0 GHz — all rated at ≥ 60 dB stopband attenuation, with the stopband range shifting upward together with the cutoff frequency (e.g. 4.05–11.5 GHz for the 3.5 GHz model). - What are the power rating and impedance conditions of this filter?
Standard models handle approximately 15 W with VSWR ≤ 1.3:1 in a 50 Ω system, and are used mainly to suppress the 2nd and 3rd harmonics of the PA output together with wideband spurious emissions.
[Supplement] Where higher power is required, the Temwell DC-200 MHz LC LPF (50 W, IL ≤ 0.5 dB) is an alternative, but its stopband attenuation is only ≥ 40 dB @ 600–1000 MHz — inferior to the cavity type in both stopband depth and width. Power handling and stopband performance must therefore be traded off against the actual system requirement. - Under what measurement conditions were the insertion loss and return loss shown in the paper obtained?
S21 is measured with a Vector Network Analyzer (VNA) after SOLT or TRL calibration, with the frequency range set from DC up to at least the 4th harmonic. Measuring ≥ 60 dB stopband attenuation requires a VNA dynamic range of at least 80 dB so that the noise floor does not affect the result.
[Supplement] Per Section 6.1, a 5G Sub-6 GHz cavity LPF should be swept from DC (100 kHz) to at least 15 GHz; the 80 dB dynamic range provides 20 dB of margin over the 60 dB specification. When reading results, the S21 passband region approaches 0 dB (−0.8 dB means IL = 0.8 dB), while the stopband region expresses attenuation as the absolute value of the negative reading (−62 dB means 62 dB of attenuation). - What are the main advantages of this structure over conventional designs such as PCB filters or SAW/BAW?
Compared with an LC LPF (stopband attenuation around 40 dB), a cavity LPF achieves ≥ 60 dB of stopband attenuation depth over a much wider stopband range, comfortably meeting the strict spurious-emission requirements of 3GPP TS 38.104.
[Supplement] Taking the STLP-DC-3.5GA57 as an example, the stopband covers 4.05–11.5 GHz — roughly 3.3 times the passband frequency range — suppressing both the 2nd harmonic (7.0 GHz) and the 3rd harmonic (10.5 GHz) by more than 60 dB. The trade-off is a larger volume than the LC type. - Under what circumstances does performance degrade noticeably, and what should be watched for?
A single cavity resonator is affected by higher-order spurious modes (such as TE₁₀₂ and TE₂₀₂), which create spurious passbands within the stopband and interrupt the attenuation. This is the single greatest engineering challenge in realizing a wide, continuous stopband.
[Supplement] A second common source of degradation is manufacturing and assembly: cavity machining tolerances (±0.1–0.3 mm), contact resistance, and surface treatment all affect the achieved stopband depth. Every stopband specification must therefore be confirmed by VNA measurement rather than by simulation alone.
Category 2: Application Scenarios and Selection
- Which equipment or application scenarios is this filter best suited to?
It is used mainly for harmonic suppression and wideband noise management in the 5G transmit path, ensuring that base stations meet the 3GPP TS 38.104 spurious emission limits (−57 dBm / 100 kHz over 30 MHz–1 GHz, and −47 dBm / 1 MHz over 1 GHz–12.75 GHz).
- If I need a narrower or wider bandwidth, how can this design be adjusted?
The Chebyshev response is the mainstream choice, balancing passband ripple against stopband roll-off. Where an extremely steep transition band is required, the Elliptic response delivers the fastest roll-off by introducing finite transmission zeros.
[Supplement] For a lowpass filter, "adjusting the bandwidth" is in practice "selecting the cutoff frequency." Per Table 4: n78 (3.3–3.8 GHz) suggests 3.5 GHz (STLP-DC-3.5GA57); n77 C-Band (3.7–4.2 GHz) suggests 4.0 GHz (STLP-DC-4GA33); ISM 5.8 GHz suggests 6.0 GHz (STLP-DC-6GA42). The stopband start frequency is generally set at f_stop ~ 1.1 x f_cutoff; the actual ratio in the Temwell STLP series is approximately 1.14–1.16. - Are there additional requirements or limitations in high-power or high-temperature environments?
The STLP series is rated at 15 W as standard. Higher power requires verifying the thermal design against conductor loss and cavity Q, so that temperature variation does not compromise stopband attenuation stability.
[Supplement] Changes in temperature and power conditions affect both cavity dimensions and contact impedance, which in turn shift the stopband start frequency and attenuation depth. For high-power projects, the operating temperature range and the continuous/peak power conditions should be stated explicitly at the specification stage and confirmed by measurement. - For space-constrained designs, roughly how much volume or mounting space should be reserved?
A Stepped Impedance Resonator (SIR) can push spurious passbands to higher frequencies and thereby extend the effective stopband width, making it a practical way to balance volume against stopband performance. The actual volume varies by model and frequency band.
[Supplement] Volume and stopband performance are a direct trade-off: a multi-section cascade yields a wider and more continuous stopband but increases volume and insertion loss and is more sensitive to manufacturing tolerances. Where space is severely constrained, relaxing the stopband depth from 60 dB to 40–50 dB in exchange for size, or switching to an LC structure, can be evaluated.
Category 3: Customization and Cooperation Process
- To customize a similar filter, what specification data should be prepared first?
Please provide the cutoff frequency, passband range, insertion loss limit, stopband attenuation target and its corresponding frequency range, VSWR requirement, and power handling capability.
[Supplement] It also helps to provide the PA output power (used to back-calculate the required attenuation), the highest harmonic order that must be covered, the operating temperature range, the connector type, and any mechanical mounting constraints. This substantially shortens the specification round-trip. - How long does it take from specification confirmation to the first sample batch?
Lead time depends on the model and the degree of customization. Providing a complete specification requirement allows an accurate schedule assessment.
- What reliability or qualification testing is performed before mass production?
Before shipment, S21 stopband data are verified on a VNA, connectors are confirmed to be properly torqued so that leakage paths do not prevent the stopband floor from meeting specification, and passband VSWR is confirmed to match the system impedance requirement.
[Supplement] Section 6.2 identifies two common measurement pitfalls. First, an insufficiently tightened SMA connector creates a fixture leakage path near the 60 dB attenuation level, preventing the stopband floor from meeting specification. Second, an out-of-specification passband VSWR (e.g. > 1.5:1) directly raises insertion loss, so the test environment must be confirmed to match the 50 Ω system. - If an existing design does not fully meet the requirement, what adjustments or evaluation support can you provide?
We can evaluate a multi-section cascade to cover a wider stopband, or apply spurious-mode management techniques such as mode staggering and mixed electromagnetic coupling in a customized design.
[Supplement] The three principal spurious-mode management techniques are: Mode Staggering (adjusting individual cavity dimensions so that higher-order mode resonances are offset from one another); Mixed EM Coupling (selecting a weak-coupling point between electric and magnetic coupling to selectively suppress specific modes); and Orthogonal Feeding (using an orthogonal input/output port layout to inherently block higher-order mode excitation).
Category 4: Supplementary Questions
- [Supplement] How much stopband attenuation is enough, and is there a way to back-calculate it?
It can be derived from the regulation. 3GPP TS 38.104 sets the base-station spurious limit over 1–12.75 GHz at −47 dBm (1 MHz BW). Assuming a PA output of +43 dBm (20 W), the minimum system attenuation required is 43 — (-47) = 90 dB. However, PA harmonics are already 20–30 dBc below the fundamental, so the LPF itself only needs to supply roughly 60–70 dB — which is precisely why the STLP series is specified at ≥ 60 dB.
- [Supplement] What is the quantitative trade-off between insertion loss and stopband attenuation?
Per Step 4 of Section 7.1: a passband IL ≤ 1.0 dB is the practical upper limit acceptable to 5G systems. If IL ≤ 0.5 dB is required, stopband attenuation can typically only reach ≥ 40–50 dB; if ≥ 70 dB of stopband attenuation is insisted upon, IL usually rises to 1.5–2.0 dB. When setting specifications, first confirm the IL that the system link budget allows, then work back to a realistically achievable stopband target.
- [Supplement] How wide is the effective stopband of a single section, and when is a two-section cascade required?
The effective stopband of a single-section cavity LPF is typically 2–3 times the passband in frequency. When the system requires stopband coverage up to the 5th harmonic, a cascade of two complementary sub-filters should be considered so that transmission zeros are distributed quasi-periodically across the entire stopband. Each additional order N adds roughly 20 dB/decade to the cutoff roll-off rate.
- [Supplement] In practice, how should one choose between the Chebyshev and Elliptic responses?
5G cavity LPFs generally favor the Chebyshev response: its stopband attenuation increases monotonically and its design predictability is the best, stably delivering ≥ 60 dB of stopband attenuation while keeping insertion loss low. Only when the system demands an extremely steep transition band near the cutoff frequency (for example, Sub-6 GHz immediately adjacent to an interfering band) should an Elliptic or Generalized Chebyshev response be adopted, trading stopband equal-ripple and higher implementation sensitivity for the steepest possible roll-off.
References
- Tektronix, "Spurious Emission Measurement on 5G NR Base Station Transmitters and Receivers," Application Note.
- 3GPP TS 38.104, "NR; Base Station (BS) Radio Transmission and Reception," Release 17/18.
- Temwell Corporation, "What Is Insertion Loss of RF Filters and Why It Matters," Technical Article, temwell.com.
- Temwell Corporation, "Customized Standard Cavity Lowpass Filter (STLP) Solutions," Product Page & Datasheets, temwell.com.
- J. Stiles, "Microwave Filter Design," University of Kansas (ITTC) course handout.
- Microwaves101, "Filter Response Types," Encyclopedia entry.
- P. Butzopulos, "Low-Pass Chebyshev Filter Based on Integrated Passive Device Technology," Theseus, 2023.
- "Chebyshev filter," Wikipedia.
- CSUN, "ECE 440 Filters," course notes.
- Mini-Circuits, "A Quick Guide to RF & Microwave Filter Topologies," Blog.
- "Synthesis and Design of a Generalized Chebyshev Filter," UiTM Institutional Repository.
- "Multilayer Circular Substrate-Integrated Waveguide Cavity Band-Pass Filters with Ultrawide Stopband Characteristics," Int. J. Microwave and Wireless Technologies, Cambridge.
- "New Coaxial Low-Pass Filters with Ultra-Wide and Spurious-Free Stopband," Int. J. Microwave and Wireless Technologies, Vol. 14, Issue 3.
- Cambridge Core, Cascaded independently-matched sub-filter low-pass design (Figs. 6b, 8a).
- "Multi-Stage RC Low-Pass Filters," ECE311 Lab 11 handout.
- "Spurious Suppression Techniques for 3-D Printed Coaxial Resonator Bandpass Filters," University College Cork (CORA).
- Multilayer circular SIW cavity BPF (ultrawide stopband), arXiv preprint mirror.
- "Realization of a Wide Stopband Filter Using the Weakest Electric Field Method and EM Hybrid Coupling," Wiley, 2024 (Article 9298815).
- Temwell Corporation, "STLP-DC-12.5GA73 Low Pass Filter Specifications," Datasheet PDF.
- Temwell Corporation, "DC-200 MHz LC Low Pass Filter Preliminary Specifications," Datasheet PDF.
- Fujicrystal, "How to Measure SAW Filters: VNA S-Parameters & Group Delay."
- Microwaves101, "Network Analyzer Measurements," Encyclopedia entry.
- CERN Accelerator School, "RF Measurement Techniques," 2022 lecture (Indico).
- E. Musonda, "Design of Generalised Chebyshev Lowpass Filters Using Coupled Line-Stub Sections," White Rose, 2015.