What would be their resonance frequency ω_0?
You are slightly missing the point here. For the CL high-pass and LC low-pass L-pads, true impedance matching is not at the natural resonant frequency of the circuit. True impedance matching can be significantly lower than the natural resonant frequency (low-pass) or, significantly higher for the high-pass.
However, if you are using an L-pad to match (say) 50 Ω to (say) a load of 300 Ω the difference is quite small but, there is still a difference: -
Image from my basic website. The derivation of the formulas are included as well so, when you say this question: -
Is there a way to simplify and / or solve equations using a program
tool, online?
The answer is yes for the common examples provided on this page. It's still a work-in-progress by the way. As a double-check I had this set-up in microcap: -
I've plotted input impedance (magnitude and phase) against frequency. As you can see, at 10 MHz, the input impedance (bar the insignificant rounding errors) is resistive at 50 Ω. At the natural resonant frequency, the angle of the input impedance is lagging by nearly 11°. Now this isn't much but, it's important enough to note.
You will also find that the amplification at the true matching frequency equals the Q of the circuit. This is interesting because, at the natural resonant frequency, amplification is also equal to the Q-factor for a 2nd order filter. However, you don't get good impedance matching of resistive impedances at the natural resonant frequency.
I've seen that while evaluating ZL is being taken as real in some
online materials, should I also follow that for simplicity?
That's the sensible approach because, complex impedances can easily be made resistive by using another series or parallel reactive component at the impedance matching frequency.