“…To obtain ∆ω, Maggiore [12] embraced the BH as a damped harmonic oscillator having a characteristic frequency in the form of ω = ω 2 R + ω 2 I [17,18] was the first physicist who considered the quasinormal modes (QNMs) or the so-called ringing modes for computing ∆ω and hence obtaining I adb . Then, many studies have used the MM to test the Bekenstein's conjecture for various BH solutions (see for instance [19,20,21,22,23,24,25,26,27,28]). Today, there are several methods to compute the QNMs, such as the WKB method, the phase integral method, continued fractions and direct integrations of the wave equation in the frequency domain [29].…”