Memory effects represent a deviation from static nonlinearity, causing the amplifier's AM-AM distortion and AM-PM distortion characteristics to become frequency-dependent and history-dependent. These effects manifest as asymmetry in intermodulation distortion sidebands and hysteresis in the amplifier's dynamic transfer function, fundamentally limiting the correction bandwidth of memoryless digital predistortion.
Glossary
Memory Effects

What is Memory Effects?
Memory effects in power amplifiers are dynamic nonlinear distortions where the current output depends not only on the instantaneous input envelope but also on past signal values due to finite thermal, electrical, and trapping time constants within the transistor and bias network.
Short-term memory effects arise from bias network impedance at envelope frequencies and harmonic terminations, while long-term memory effects originate from self-heating and trap effects in GaN HEMT devices. Accurate behavioral modeling using Volterra series or memory polynomial models is essential to capture these dispersive phenomena for effective Doherty amplifier linearization.
Memory Effects vs. Memoryless Nonlinearity
Comparison of instantaneous nonlinear distortion with dynamic memory-dependent distortion mechanisms in power amplifiers
| Feature | Memoryless Nonlinearity | Short-Term Memory Effects | Long-Term Memory Effects |
|---|---|---|---|
Definition | Output depends only on instantaneous input envelope | Output depends on signal envelope history within a few symbol periods | Output depends on signal envelope history over hundreds of symbols |
Primary Cause | AM-AM and AM-PM conversion in active device transconductance | Bias circuit impedance at modulation frequency, harmonic terminations | Self-heating, trap effects, thermal time constants in semiconductor substrate |
Time Constant | Instantaneous (sub-nanosecond) | Nanoseconds to microseconds | Microseconds to milliseconds |
Frequency Domain Signature | Spectral regrowth symmetric around carrier | Asymmetric intermodulation products, frequency-dependent AM-PM | Low-frequency dispersion, memory kernel extending below 1 MHz |
Modeling Approach | Static polynomial or look-up table | Memory polynomial, Volterra series with short taps | Generalized memory polynomial with sparse delays, thermal sub-circuit models |
DPD Compensation Complexity | Low: single-dimensional LUT or polynomial | Moderate: requires temporal taps in predistorter | High: requires long delay taps or auxiliary thermal models |
Impact on ACLR | 3-5 dB degradation at rated power | Additional 2-4 dB asymmetry between upper and lower sidebands | 1-3 dB low-frequency regrowth, worsens with sustained high-power operation |
GaN HEMT Susceptibility |
Frequently Asked Questions
Addressing the most common questions about dynamic nonlinear distortions in Doherty power amplifiers, where output depends on both instantaneous and past signal values due to thermal, electrical, and trapping time constants.
Memory effects are dynamic nonlinear distortions in a power amplifier where the current output depends not only on the instantaneous input envelope but also on past signal values. Unlike static nonlinearities (AM-AM and AM-PM distortion), memory effects introduce a time-dependent component to the amplifier's transfer function. This means the same instantaneous input power can produce different output responses depending on the signal's recent history. Memory effects manifest as asymmetry in intermodulation distortion sidebands and frequency-dependent behavior in the amplifier's nonlinear characteristics. They are classified by their physical origin into electrical memory effects (caused by bias network impedances and envelope frequency-dependent matching), thermal memory effects (from dynamic self-heating of the transistor channel), and trapping effects (from slow charge capture and release in semiconductor materials like GaN HEMTs). Understanding and compensating for memory effects is essential for achieving the linearity required by modern wideband communication signals with high peak-to-average power ratios.
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Related Terms
Understanding memory effects requires familiarity with the underlying physical mechanisms, modeling approaches, and compensation techniques that define dynamic nonlinear behavior in power amplifiers.
Thermal Memory Effects
Dynamic variations in amplifier gain and phase caused by transient temperature changes in the transistor channel. As instantaneous dissipated power fluctuates with the signal envelope, the junction temperature rises and falls with time constants ranging from microseconds to milliseconds.
- Self-heating: Power dissipation heats the channel, reducing carrier mobility and gain
- Bias circuit interaction: Temperature-dependent quiescent current shifts alter the operating point
- Long time constants: Thermal capacitance of the die and package creates low-frequency memory
GaN HEMT devices exhibit particularly complex thermal memory due to high power density and multi-finger thermal coupling.
Electrical Memory Effects
Nonlinear distortion arising from frequency-dependent impedance interactions between the transistor and its surrounding bias and matching networks. The envelope-frequency impedance seen by the device's intrinsic current source modulates the output waveform.
- Bias network resonance: Inductive bias lines and capacitive bypass networks create envelope-frequency resonances
- Baseband impedance: The impedance presented to the low-frequency difference-frequency components generated by the nonlinearity directly controls memory depth
- Harmonic terminations: Improper harmonic impedances reflect energy back to the device, mixing with the fundamental
Minimizing electrical memory requires careful baseband impedance engineering across the entire modulation bandwidth.
Trap Effects (Charge Trapping)
Slow charge capture and release at deep-level traps in the semiconductor material, particularly in GaN HEMTs and GaAs devices. Trapped charge modulates the channel's electric field, causing gate lag and drain lag phenomena.
- Gate lag: Trapping under the gate edge reduces drain current after a high-voltage pulse
- Drain lag: Trapping in the buffer or surface states alters the channel's conductivity
- Time constants: Ranging from nanoseconds (surface traps) to seconds (buffer traps)
- Bias dependence: Trap occupancy is a function of the instantaneous and recent drain voltage history
Trap effects introduce complex, history-dependent nonlinearities that are difficult to distinguish from thermal memory without specialized characterization.
Memory Polynomial Model
A simplified Volterra series derivative that captures memory effects using a diagonal kernel structure. The model expresses the current output as a sum of nonlinear functions of delayed input samples, dramatically reducing the coefficient count compared to the full Volterra series.
- Structure: y(n) = Σ_k Σ_m a_{km} · x(n-m) · |x(n-m)|^{k-1}
- Diagonal-only: Only terms where all delays are equal are retained, eliminating cross-memory products
- Generalized Memory Polynomial (GMP): Extends the model by adding cross-terms between the current sample and lagging envelope values
- Implementation: Highly efficient for FPGA and ASIC DPD implementations due to its regular, parallelizable structure
The memory polynomial is the most widely adopted model for commercial digital predistortion systems.
Long-Term vs Short-Term Memory
A classification of memory effects based on their time constant relative to the modulation envelope period. This distinction determines the required memory depth in the predistorter model.
Short-Term Memory:
- Time constants comparable to the inverse modulation bandwidth
- Caused by matching network dispersion and harmonic terminations
- Captured by memory taps spanning 1–5 symbol periods
Long-Term Memory:
- Time constants much longer than the symbol period
- Caused by thermal dynamics, trap effects, and bias circuit charge/discharge
- Requires extended memory depth or specialized long-memory kernels
- Often exhibits a frequency response below 1 MHz
Accurate DPD must span both regimes, often requiring hybrid model structures that separately address short-term and long-term dynamics.
Envelope Frequency Analysis
A two-dimensional characterization technique that separates the nonlinear behavior of a power amplifier into the carrier-frequency domain and the envelope-frequency domain. This reveals how memory effects manifest as asymmetry in the intermodulation distortion spectrum.
- Envelope domain: Represents the dynamic variation of the complex gain as a function of the modulation frequency
- Asymmetric IMD: Memory effects cause upper and lower intermodulation sidebands to have unequal amplitudes and phases
- Measurement: Extracted using two-tone or multi-tone tests with swept tone spacing to map the envelope-frequency response
- Visualization: Envelope-frequency gain surfaces directly show the memory depth required for linearization
This analysis is essential for diagnosing whether memory effects originate from electrical, thermal, or trapping mechanisms.

About the author
Prasad Kumkar
CEO & MD, Inference Systems
Prasad Kumkar is the CEO & MD of Inference Systems and writes about AI systems architecture, LLM infrastructure, model serving, evaluation, and production deployment. Over 5+ years, he has worked across computer vision models, L5 autonomous vehicle systems, and LLM research, with a focus on taking complex AI ideas into real-world engineering systems.
His work and writing cover AI systems, large language models, AI agents, multimodal systems, autonomous systems, inference optimization, RAG, evaluation, and production AI engineering.
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