Table 6.

Maximal absolute non-linear frequency shifts as a fraction of the linear inertial-frame angular frequency $\mid \delta {\mathrm{\Omega }}_{\phi ,\mathrm{m}}^s{\mathrm{\Omega }}_{\phi ,i}\mid$ (in parts-per-thousand), zero-point-corrected non-linear combination phases ${\stackrel{\sim }{\mathrm{\Phi }}}_{s,0}^s$, and expected stationary surface luminosity fluctuation ratios $\mid {\mathfrak{L}}_2^s\mid /\mid {\mathfrak{L}}_1^s\mid$ and $\mid {\mathfrak{L}}_3^s\mid /\mid {\mathfrak{L}}_1^s\mid$ for the mode triads listed in Table 4.

Model	(n1,  n2,  n3)	$\left|\delta {\mathrm{\Omega }}_{\phi ,\mathrm{m}}^s{\displaystyle /{\mathrm{\Omega }}_{\phi ,i}}\right|$ (ppt)	${\stackrel{\sim }{\mathrm{\Phi }}}_{s,0}^s$ (rad)	$\mid {\mathfrak{L}}_2^s\mid /\mid {\mathfrak{L}}_1^s\mid$	$\mid {\mathfrak{L}}_3^s\mid /\mid {\mathfrak{L}}_1^s\mid$
Fiducial	(−51, −38, −90)	0.764733	0.21819	0.55605	0.06168
ΔXc,  1	(−20, −13, −58)	0.708263	−0.79901	0.42858	0.03261
	(−21, −14, −54)	1.839526	−0.30412	0.65585	0.06390
	(−22, −15, −53)	1.283029	0.39313	0.91831	0.08677
	(−39, −40, −40)	0.593527	0.11515	0.48298	0.48298
ΔXc,  2(a)	(−10, −7, −22)	2.639689	−0.06776	0.32000	0.05700
	(−14, −10, −26)	6.021050	0.10383	2.53183	0.14379
ΔXc,  2(b)	(−10, −6, −36)	1.589962	−0.44842	0.32190	0.00750
	(−12, −8, −23)	0.766883	−0.18324	0.84057	0.08189
	(−17, −12, −30)	0.701324	−0.61847	3.08804	0.06054
	(−18, −13, −31)	3.238349	0.17297	2.02044	0.04897
ΔMini,  1	(−50, −48, −56)	0.443377	−0.54958	0.79629	0.41179
	(−40, −30, −70)	5.086921	0.16921	2.05217	0.20288
ΔXc|Mini	(−16, −14, −22)	0.330309	0.09168	0.07627	0.05190
	(−17, −13, −29)	2.600074	0.10985	0.29260	0.08237
	(−23, −17, −41)	5.594778	0.29998	0.72069	0.08163
ΔMini,  2	(−31, −23, −56)	1.760714	0.61936	0.34623	0.07864
	(−32, −24, −58)	3.997386	0.33231	0.48095	0.07250
	(−35, −26, −62)	1.832881	−0.81546	0.61223	0.07525
	(−36, −27, −63)	3.610779	0.46404	0.30289	0.04729
	(−38, −28, −67)	3.885665	−0.44231	0.12459	0.01283