Peaks in the frequency response can only exist in systems with conjugate complex poles.
For an underdamped (\$\zeta<1\$ or \$Q > 0.5\$) second-order system, the peak appears specifically for \$\zeta<1/\sqrt{2}=0.707\$.
$$H(s)=\frac{\omega_n^2}{s^2+2\zeta\omega_ns+\omega_n^2}$$
where \$\omega_n\$ is the natural frequency (also called corner frequency when considering assymptotes), the peak
$$M_p=\frac{1}{2\zeta\sqrt{1-\zeta^2}}$$
occurs at resonant frequency
$$\omega_p=\omega_n\sqrt{1-2\zeta^2}$$
Note on figure below: When varying the damping ratio \$\zeta\$, the peak follows a specific curve. In filter theory, that special value for \$\zeta=0.707\$ corresponds to a Butterworth response. The magnitude curve is sais to be maximally flat (no peak). The meaning of \$w_n\$ for the Butterworth response is the same as for the first-order case, that is, \$w_n\$ represents the -3 dB frequency, also called cuttoff frequency. Only in this case. Also, \$w_n=w_p\$, causes an infinite response (undamped system - oscillator).