Noise, Sensitivity, and Receiver Design Advanced Noise Topics Informational

What is the effect of feedback on the noise figure of a common source FET amplifier?

Feedback in a common-source FET amplifier affects the noise figure through two mechanisms: the feedback element itself contributes noise (thermal noise from resistive feedback), and the feedback changes the transistor's effective noise parameters (Gamma_opt, NF_min, R_n) by modifying the device's input and output impedances and gain. Resistive shunt feedback (a resistor R_f from drain to gate) degrades the noise figure because: the feedback resistor contributes thermal noise (4kTR_f) that appears at the output and, referred to the input, adds approximately 10 log(1 + Z_0/R_f) dB to the noise figure; additionally, the feedback reduces the transistor gain, increasing the noise contribution of subsequent stages via Friis formula. A typical 300 ohm shunt feedback resistor contributes approximately 0.7 dB additional noise. Resistive series feedback (a resistor in the source terminal) also degrades noise figure by adding thermal noise directly in the signal path. Inductive series feedback (an inductor L_s in the source terminal) is the preferred feedback type for LNAs because the inductor is theoretically lossless (no thermal noise contribution) and it simultaneously creates a real part in the input impedance (R_in approximately omega_T x L_s) and shifts Gamma_opt closer to S11*, enabling simultaneous noise and impedance match with minimal noise figure penalty. The noise figure penalty from inductive degeneration is only 0.05-0.2 dB, compared to 0.5-2 dB for resistive feedback.
Category: Noise, Sensitivity, and Receiver Design
Updated: April 2026
Product Tie-In: LNAs, Noise Sources

Feedback Effects on FET LNA Noise Figure

Understanding how different feedback types affect noise is critical for LNA design: the wrong feedback choice can easily double the amplifier's noise figure, while the right choice (inductive degeneration) can improve the system noise figure by enabling SNIM (simultaneous noise and impedance match).

ParameterSuperheterodyneDirect ConversionDigital IF
Image Rejection60-90 dB (filter)30-50 dB (mismatch)N/A (digital)
DC OffsetNo issueMajor issueNo issue
LO LeakageLowHighLow
IntegrationDifficultEasy (single chip)Moderate
Dynamic Range80-120 dB60-90 dB70-100 dB
  • Performance verification: confirm specifications against the application requirements before finalizing the design
  • Environmental factors: temperature range, humidity, and vibration affect long-term reliability and parameter drift
  • Cost vs. performance: evaluate whether the application demands premium components or standard commercial grades
Common Questions

Frequently Asked Questions

Why does inductive degeneration not significantly degrade noise figure?

An ideal inductor is a lossless, noiseless element (no thermal noise). Adding L_s in the source does not introduce any new noise sources. The small NF penalty (0.05-0.2 dB) comes from: the slight shift of Gamma_opt away from the true NF_min source impedance, the reduction in gain (which slightly increases the Friis noise contribution of stage 2), and practical inductor losses (finite Q). The net effect is much smaller than the benefit of enabling impedance match at the input.

Can I use inductive degeneration at millimeter-wave frequencies?

Yes, but the required inductance values are very small (0.01-0.1 nH at 30-100 GHz). At these values, the inductance is often realized by the bond wire or via inductance connecting the FET source to ground, or by a short transmission line stub. MMIC designs use thin-film spiral inductors or shorted transmission line sections. Precise control of sub-0.1 nH inductance is challenging and requires careful EM simulation.

What is the optimal amount of feedback for noise figure?

For resistive shunt feedback: the minimum noise figure occurs with the smallest feedback resistor that still provides the required bandwidth and stability (larger R_f means less noise but less feedback effect). For inductive degeneration: the optimal L_s provides R_in = R_s (50 ohms), which simultaneously optimizes input match and noise. Too much inductance (R_in > R_s) degrades both noise and match. The optimal value is uniquely determined by the transistor's omega_T and C_gs.

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