"for a stable operation point, the structure needs overall negative DC loop gain"
Not true; positive feedback is okay, as long as it is less than unity.
To illustrate this, consider a system where a
positive feedback loop wraps around a stable first-order transfer function, a(jw)=a0/(s/w0+1):
\[a(j\omeg)=\frac{a_0}{s/\omeg_0+1}\]
Let the input be X, and the output be Y. Then,
\[Y=a(j\omeg)(X+Y)=\frac{a_0}{s/\omeg_0+1}(X+Y)\]
\[\frac{Y}{X}=\frac{a}{1-a}\frac{1}{\frac{s}{\omeg_0(1-a_0)}+1}\]
As you can see, the result is a single-pole system with a corner frequency of w0(1-a0). As long as a0<1, this pole remains in the LHP. It will travel to the RHP if a0>1. Also notable, when a0=0.5 this system's gain is 1, and as a0 approaches 1 the gain approaches infinity.
One must be careful to ensure there is no peaking in a(jw)'s transfer function, because if it peaks greater than 1, the loop will go unstable. Some ECG's have this problem--they use shielded wires for noise rejection, but this presents lots of capacitance to a high-impedance source (skin), causing severe attenuation. So they actively drive the shield to the same potential as the signal, reducing the effective capacitance and increasing the circuit's frequency range, but this introduces the possibility of instability. To solve this, the shield buffer's gain is reduced to slightly sub-unity (thus, not fully canceling the capacitance but still canceling most of it). Care must be taken to prevent any frequency peaking in the active shield's driver.