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As we know, unfaithful model of SINR loss curve is tantamount to the clutter residue, target cancellation, and increasing minimum detectable velocity (MDV), which finally leads to poor detection ability of a GMTI system.
Minimum detectable velocity.
Therefore, the minimum detectable velocity of the bistatic system is dependent on the cone angle.
Doppler division multiple access (DDMA) waveforms are approximately orthogonal providing good minimum detectable velocity (MDV) performance.
The minimum detectable velocity (MDV) as an important system design parameter is limited by the radar parameters,,, target RCSs, and signal processing and detection techniques.
Moreover, as shown in Fig. 14, D3SR-STAP and DA-SDS-SRSTAP can provide a higher SINR level in the pass-band area and a narrower clutter notch than D3-STAP, which means a better performance of minimum detectable velocity (MDV).
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Consequently, the minimum detectable axial velocity (V axial,min) is given by The range from the minimum to the maximum detectable velocities, as defined above, determines the axial Velocity Dynamic Range (VDR) of each PR-DOCT system.
Let us discuss the minimum detectable azimuth velocity component Vmin,a.
As a result, the minimum detectable azimuth velocity is approximately V min, a ≈ ∊ ρ a 2 V p 2 ( 1 − ∊ ) λ R 0, (52).
In theory, the minimum detectable axial velocity is determined by the phase stability of the light source, and was measured to be 1.8 mrad.
The noise on the phase-difference, the phase-noise σΔ ϕ, defines the smallest observable phase-difference and therefore the minimum detectable flow velocity is given by: v min = (σΔ ϕ∙λ0)/(4 πnτ∙cos [ 9, 23].
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