The patterns of bifurcation governing the escape of periodically force
d oscillations from a potential well over a smooth potential barrier a
re studied by numerical simulation. Both the generic asymmetric single
-well cubic potential and the symmetric twin-well potential Duffing os
cillator are surveyed by varying three parameters: forcing frequency,
forcing amplitude, and damping coefficient. The close relationship bet
ween optimal escape and nonlinear resonance within the well is confirm
ed over a wide range of damping, Subtle but significant differences ar
e observed at: higher damping ratios. The possibility of indeterminate
outcomes of jumps to and from resonance near optimal escape is comple
tely suppressed above a critical level of the damping ratio (about 0.1
2 for the asymmetric single-well oscillator). Coincidentally, at almos
t the same level of damping, the optimal escape condition becomes dist
inct from the apex in the to, Fl plane of the bistable regime; this co
rresponds to the appearance of chaotic attractors which subsume both r
esonant and non-resonant motions within one well. At higher damping le
vels, further changes occur involving conversions from chaotic-saddle
to regular-saddle bifurcations, These changes in optimal escape phenom
ena correspond to codimension three bifurcations at exceptional points
in the space of three parameters. These bifurcations are described in
terms of homoclinic and heteroclinic structures of invariant manifold
s, and changes in accessible boundary orbits, The same sequence of cod
imension three bifurcations is observed in both the twin-well Duffing
oscillator and the asymmetric single-well escape equation. Within the
codimension three bifurcation patterns governing escape, one particula
r codimension two global bifurcation involves a chaotic attractor expl
osion, or interior crisis, compounded with a blue sky catastrophe or b
oundary crisis of the exploded attractor, This codimension two bifurca
tion has structure containing a form of predictive power: knowledge of
attractor bifurcations in part of the codimension two pattern permits
inference of the attractor and basin bifurcations in the remainder. T
his predictive power is applicable beyond the context of escape from p
otential wells, Quantitative correlation of bifurcation patterns betwe
en the two equations according to simple scaling laws is tested. The u
nstable periodic orbits which figure most prominently in the major att
ractor-basin bifurcations are of periods one and three. Their linking
is conveniently interpreted by a three-layer spiral horseshoe structur
e for the folding action in phase space within a well, The structure o
f this 3-shoe implies a partial ordering among order three subharmonic
saddle-node bifurcations, This helps explain the sequence of codimens
ion three bifurcations near optimal escape. Some bifurcational precede
nce relations are known to follow from the Inking of periodic orbits i
n a braid on a 3-shoe. Additional bifurcational precedence relations f
ollow from a quantitative property of generic potential wells: the dyn
amic hilltop saddle has a very large expanding multiplier over one cyc
le of forcing near fundamental resonance. This quantitative property e
xplains the close coincidence of codimension three bifurcations near t
he suppression of indeterminate outcomes. An experimentalist's approac
h to identifying the three-layer template structure from time series d
ata is discussed, including a consistency check involving Poincare ind
ices. The bifurcation patterns emerging at higher damping values creat
e favorable conditions for realizing experimental strategies to recogn
ize optimal escape and locate it in parameter space. Strategies based
solely on observations of quasi-steady behavior while remaining always
within one well are discussed.