sp0110">Here we discuss perturbations of this scenario which are both non-reversible and non-conservative. We treat this problem analytically in the spirit of the work <span id="bbr0030">[3]span>. The continuation of homoclinic orbits happens with respect to both the original continuation parameter 渭 and the perturbation parameter 位. The continuation curves are parametrised by the dwelling time L of the homoclinic orbit near P . It turns out that <span id="mmlsi1" class="mathmlsrc"><span class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022039615004593&_mathId=si1.gif&_user=111111111&_pii=S0022039615004593&_rdoc=1&_issn=00220396&md5=5c35dfde518bbfa0907c44610d33c250" title="Click to view the MathML source">位(L)span><span class="mathContainer hidden"><span class="mathCode">span>span>span> tends to zero while the 渭 vs. L diagram displays isolas or criss-cross snaking curves in a neighbourhood of the original snakes-and-ladder structure.
sp0120">In the course of our studies we adapt both Fenichel coordinates near P and the analysis of Shilnikov problems near P to the present situation.