Table C.2.

Lorentzian model parameters of the simultaneous fit of observation 2636010101 of Cyg X-1 (Fig. 16). Each non-zero-centered Lorentzian adds 6 free parameters: Frequency, width, and two normalizations for the low- and high-energy PSD plus the lag and modulus of the cross vector. The norm of the real/imaginary part is the modulus of the cross vector times the cosine/sine of the phase lag, respectively. The frequency of the zeroth Lorentzian (L₀) is fixed to 0 Hz and phase zero is anchored to the strongest component (L₁). L_n denotes the narrow component at the frequency of the timing feature. Uncertainties denote 90% confidence limits.

Parameter	Value
νL0 [Hz]	0 (frozen)
νL1 [Hz]	0.186 ± 0.010
νL2 [Hz]	1.76 ± 0.12
νLn [Hz]	1.57 ± 0.04
ΔL0 [Hz]	(8±6) × 10−3
ΔL1 [Hz]	0.703 ± 0.018
ΔL2 [Hz]	4.79 ± 0.10
ΔLn [Hz]	$0.{62}_{-0.12}^{+0.14}$
ΔϕL0 [rad]	$-0.{13}_{-0.13}^{+0.09}$
ΔϕL1 [rad]	0 (frozen)
ΔϕL2 [rad]	$0.{197}_{-0.022}^{+0.021}$
ΔϕLn [rad]	$1.{01}_{-0.14}^{+0.16}$
N(L0, CPD)	$(6.1_{-2.3}^{+4.0(\mathrm{p})})\times {10}^{-4}$
N(L0,0.5–1 keV)	$(6.6_{-2.0}^{+3.5(\mathrm{p})})\times {10}^{-4}$
N(L0,2–4 keV)	(6±4) × 10−4 (p)
N(L1, CPD)	0.0448 ± 0.0009
N(L1,0.5–1 keV)	0.0307 ± 0.0006
N(L1,2–4 keV)	$0.{0665}_{-0.0017}^{+0.0016}$
N(L2, CPD)	0.0129 ± 0.0007
N(L2,0.5–1 keV)	(3.7±0.4) × 10−3
N(L2,2–4 keV)	0.0428 ± 0.0016
N(Ln, CPD)	$(1.{59}_{-0.28}^{+0.34})\times {10}^{-3}$
N(Ln,0.5–1 keV)	$(9.6_{-2.0}^{+2.3})\times {10}^{-4}$
N(Ln,2–4 keV)	$\left({10}_{-7}^{+8}\right)\times {10}^{-4}$