RF Toolbox

Schottky Diode Detector

A small-signal Schottky diode rectifies RF power in its square-law region, producing a video (baseband) voltage proportional to the input power. Its usefulness as a detector is set by the current and voltage responsivity, the video (junction) resistance that sets the Johnson noise, and the resulting noise-equivalent power (NEP) and tangential signal sensitivity (TSS). This tool computes all of these from the diode's ideality factor, saturation current, series resistance and bias.

Equations & Parameters ▸
\(V_T=\dfrac{kT}{q},\qquad R_v=\dfrac{nV_T}{I_s+I_b}\) (video resistance)
current resp. \(\beta_i=\dfrac{1}{2nV_T}\cdot\dfrac{R_v}{R_v+R_s}\) (A/W), voltage resp. \(\beta_v=\beta_i R_v\) (V/W)
\(NEP=\dfrac{\sqrt{4kTR_v}}{\beta_v},\quad MDS=NEP\sqrt{B},\quad TSS\approx 2.5\,MDS\)
nDiode ideality factor (~1.05–1.2).
IsSaturation current (µA); sets zero-bias video resistance.
RsDiode series resistance (Ω).
IbDC bias current (µA); 0 for a zero-bias detector.
B, TVideo bandwidth (MHz) and temperature (K).
Reference: D. M. Pozar, Microwave Engineering, 4th ed., §10.3. TSS uses the conventional ≈2.5× (4 dB) tangential factor.
Inputs
~1.1
µA
Sat. current
Ω
Series R
µA
0 = zero-bias
MHz
Video
K
Physical
Results

Responsivity

Video resistance Rv
Current resp. βi
Voltage resp. βv

Sensitivity

Noise voltage
NEP
MDS in B
TSS