Table 3: Growth of resonant modes. Models which present a global maximum growth rate (according to the linear analysis) for all resonant modes (i.e., at any wavelength) above the growth rates of the perturbed modes are listed. $w_{i,\rm max}$ : maximum growth rate for all resonant modes from linear analysis; $w_{i,p,v_{\perp}}\!$ : fitted growth rates of pressure and perpendicular velocity perturbations for the fast growth linear regime in the simulation, only for those simulations where it occurs; $w_{i,\parallel }$ : same as $w_{i,p,v_{\perp }}$ for axial velocity. All values are in c/R_j units.
Model $w_{i,\rm max}$ $w_{i,p,v_{\perp }}$ $w_{i,v_\parallel}$

B05 0.052 - -

D05 0.11 - -

A10 0.013 0.017 0.009

B10 0.035 - -

D10 0.057 - -

B20 0.026 0.036 0.036

D20 0.035 0.070 0.047

**Table 3:** Growth of resonant modes. Models which present a global maximum growth rate (according to the linear analysis) for all resonant modes (i.e., at any wavelength) above the growth rates of the perturbed modes are listed. $w_{i,\rm max}$ : maximum growth rate for all resonant modes from linear analysis; $w_{i,p,v_{\perp}}\!$ : fitted growth rates of pressure and perpendicular velocity perturbations for the fast growth linear regime in the simulation, only for those simulations where it occurs; $w_{i,\parallel }$ : same as $w_{i,p,v_{\perp }}$ for axial velocity. All values are in c/R_j units.
Model	$w_{i,\rm max}$	$w_{i,p,v_{\perp }}$	$w_{i,v_\parallel}$
B05	0.052	-	-
D05	0.11	-	-
A10	0.013	0.017	0.009
B10	0.035	-	-
D10	0.057	-	-
B20	0.026	0.036	0.036
D20	0.035	0.070	0.047

Source LaTeX | All tables | In the text

	1 Introduction
	2 Setup for numerical simulations
	3 Results
	4 Discussion
	5 Conclusions
	References
	Online Material
	Appendix A: Single antisymmetric mode simulations
	Appendix B: Cylindrical jet simulations