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Surface acoustic wave (SAW) and bulk acoustic wave (BAW) filters are the building blocks of RF front-ends in smartphones, base stations, and wireless infrastructure. Their compact size, excellent selectivity, and low insertion loss make them indispensable. However, their piezoelectric nature introduces a unique challenge: unlike conventional passive components, SAW/BAW devices can exhibit even-order nonlinearity because of the crystallographic asymmetry required for piezoelectricity. This means that second harmonics (H2) and second-order intermodulation (IMD2) products can fall directly into receive bands, desensitizing the receiver.
As wireless standards evolve toward carrier aggregation and higher-order modulation, the requirements for linearity become stricter. A filter that generates -80 dBm of IMD2 in a band where the receiver noise floor is -95 dBm can significantly degrade sensitivity. IEC 62761 addresses this by providing standardized measurement methods that enable fair comparison between devices from different manufacturers.
The standard specifies a basic measurement setup using a signal generator, power amplifier, and spectrum analyzer. The device under test (DUT) is driven with a single-tone signal at frequency f0, and the output is measured at harmonics 2f0, 3f0, etc. The standard emphasizes the critical importance of proper impedance matching: because SAW/BAW filters achieve their frequency selectivity through impedance matching with peripheral circuitry, the termination impedance must be precisely controlled for reproducible results.
For IMD characterization, the standard describes two-tone and three-tone test methods. In the two-tone test, signals at frequencies fa and fb are applied, and the IMD products at frequencies (m·fa ± n·fb) are measured. The standard specifically addresses IMD2 measurement for antenna duplexers, where the transmit signal at ftx can mix with a blocker or with itself to produce distortion in the receive band frx. A three-tone method is also described for more complete characterization.
The standard specifies equipment requirements including signal generator phase noise, power amplifier linearity, and spectrum analyzer dynamic range. Accessories such as circulators, isolators, and diplexers are discussed for their role in preventing measurement setup nonlinearity from masking the DUT’s true nonlinearity.
| Measurement Type | Input Signals | Measured Products | Typical Dynamic Range |
|---|---|---|---|
| Harmonics (H2) | f0 | 2f0 | -80 to -120 dBc |
| Harmonics (H3) | f0 | 3f0 | -90 to -130 dBc |
| IMD2 (two-tone) | fa, fb | fa ± fb | -85 to -125 dBm |
| IMD3 (two-tone) | fa, fb | 2fa±fb, 2fb±fa | -90 to -130 dBm |
| IMD2 (duplexer) | ftx, blocker | ftx ± blocker | -80 to -120 dBm |
The standard devotes significant attention to how circuit impedance affects nonlinearity measurement. SAW/BAW devices are impedance-sensitive — their nonlinear behavior changes with source and load impedance. The standard recommends using 50 Ω measurement systems with specified return loss, and provides guidance for situations where the DUT’s passband impedance deviates from 50 Ω.
For a 2:1 duplexer with transmit band 1710-1785 MHz and receive band 1805-1880 MHz, proper test frequency selection ensures that IMD products fall in the band of interest. The standard provides a specific table relating fa, fb, and the target frequency ft to guarantee that measurements correspond to real-world operating conditions.
Accurate nonlinearity measurement requires de-embedding the effects of test fixtures, cables, and peripheral components. The standard discusses calibration techniques including short-open-load-through (SOLT) and thru-reflect-line (TRL) methods adapted for nonlinear measurements. Without proper de-embedding, errors of 3-6 dB in absolute nonlinearity levels are common.
The standard recommends testing at the device’s maximum rated input power or at power levels representative of the application. For smartphone duplexers, this is typically +24 to +27 dBm for transmit path testing and -10 to 0 dBm for receive path testing.
Temperature significantly impacts nonlinearity because the piezoelectric coefficients and acoustic velocities are temperature-dependent. The standard recommends testing at -20 °C, +25 °C, and +85 °C as a minimum characterization set.
Generally, higher insertion loss correlates with lower nonlinearity because less acoustic energy is confined in the resonator. However, this relationship is not monotonic and depends on the specific design, substrate material (e.g., LiTaO3 vs. LiNbO3), and electrode configuration.
Yes. The measurement principles are frequency-independent within the RF range. The standard has been applied to bands up to 6 GHz, and the methodology is extendable to mmWave frequencies with appropriate equipment upgrades.