Ns. Peters et al., CHARACTERISTICS OF THE TEMPORAL AND SPATIAL EXCITABLE GAP IN ANISOTROPIC REENTRANT CIRCUITS CAUSING SUSTAINED VENTRICULAR-TACHYCARDIA, Circulation research, 82(2), 1998, pp. 279-293
The excitable gap of a reentrant circuit has both temporal (time durin
g the cycle length that the circuit is excitable) and spatial (length
oi the circuit that is excitable at a given time) properties. We deter
mined the temporal and spatial properties of the excitable gap in reen
trant circuits caused by nonuniform anisotropy, Myocardial infarction
was produced in canine hearts by ligation of the left anterior descend
ing coronary artery, Four days later, reentrant circuits were mapped i
n the epicardial border-zone of the infarcts with a multielectrode arr
ay during sustained ventricular tachycardia induced by programmed stim
ulation. During tachycardia, premature impulses were initiated by stim
ulation at sites around and in the reentrant circuits, and their condu
ction characteristics in the circuit were mapped. All circuits had a t
emporal excitable gap in at least part oithe circuit, which allowed pr
emature impulses to enter the circuit. Completely and partially excita
ble segments of the temporal gap were identified by measuring conducti
on velocity of the premature impulses; conduction was equal to the nat
ive reentrant wave front in completely excitable regions and slower th
an the reentrant wave front in partially excitable regions. In some ci
rcuits, a temporal gap existed throughout the circuit, permitting the
entire circuit to be reset over a range of premature premature couplin
g intervals, although the size of the gap varied at different sites. I
n other circuits, the gap became so small at local sites that even tho
ugh premature impulses could enter the circuit, the circuit could not
be reset. Premature impulses could terminate reentry in circuits that
could be reset or not. We also found a significant spatial gap, which
was identified by determining the distance between the head oithe circ
ulating wave front, which could be located on the activation map, and
its tail, which was the site most distal from the head as located by t
he site of entry of the premature wave front into the circuit. The spa
tial gap could also vary in different parts of the circuit. Therefore,
nonuniform anisotropic reentrant circuits have both a temporal and sp
atial excitable gap with fully and partially excitable components that
change in different parts of the circuit.