You didn't exactly "start with a real signal". What
you started with, was differential equations for inductors,
capacitors, and resistors in an equivalent to your real circuit.
Those simultaneous differential equations become linear equations
when you use complex conductances/impedances like "j⍵C" and "j⍵L"
and you need both the real parts and imaginary parts to track
the phase of your output results for all those frequency components.
This is happening because you are using a set of simple linear
equations instead of coupled differential equations.
The resulting signals can be interpreted with both AC amplitudes,
and phases, and all that takes is a conversion from
Cartesian (real and imaginary axes) to polar (phase and amplitude)
representation. And, summation over any and all frequencies under
consideration, because your results are one-frequency-at-a-time
depictions.