Ciaccio E J, Biviano A B, Wan E Y, Peters N S, Garan H
Department of Medicine, Division of Cardiology, Columbia University College of Physicians and Surgeons, New York, NY, USA.
Department of Medicine, Division of Cardiology, Columbia University College of Physicians and Surgeons, New York, NY, USA.
Comput Biol Med. 2017 Apr 1;83:166-181. doi: 10.1016/j.compbiomed.2017.02.008. Epub 2017 Mar 2.
Atrial fibrillation (AF) is difficult to treat effectively, owing to uncertainty in where to best ablate to eliminate arrhythmogenic substrate. A model providing insight into the electrical activation events would be useful to guide catheter ablation strategy. Method A two-dimensional, 576×576 node automaton was developed to simulate atrial electrical activity. The substrate field was altered by the presence of differing refractory period at varying locations. Fibrosis was added in the form of short, randomly positioned lines of conduction block. Larger areas of block were used to simulate ablation lesions. Anisotropy was imposed in a 2:1 ratio. A premature electrical impulse from one of four grid corners was utilized to initiate activation.
Rotational activity was uninducible when refractory patch dimensions were less than 20×20mm. For larger refractory regions, a single premature stimulus was capable of inducing an average of 1.19±1.10 rotors, which often formed near the patch edges. A maximum of 5 rotors formed when refractory patch dimensions approached the size of the entire left atrial virtual field. Rotors formed along a refractory patch edge, after wavefront arrival was delayed at turning points or due to the presence of a fiber cluster of sufficient size. However, rotational activity could also occur around a large fiber cluster without the need of spatially variable refractoriness. When obstacles to conduction were lacking in size, nascent rotors drifted and either extinguished, or stabilized upon anchoring at a sufficiently large fiber cluster elsewhere in the field. Transient rotors terminated when traversing a region with differing refractory periods, if no obstacle to conduction was present to sufficiently delay wavefront arrival beyond the longest refractory period. Other rotors were annihilated when a nearby rotor with faster spin rate gradually interrupted the activation pathway. Elimination of anchors by removal, or by simulated ablation over a sufficient region, prevented rotor onset at a particular location where it would otherwise form.
The presence of obstacles to conduction and spatial differences in refractory period are important parameters for initiating and maintaining rotational activity in this simulation of an atrial substrate.
心房颤动(AF)难以有效治疗,原因在于难以确定最佳的消融位置以消除致心律失常基质。一个能够深入了解电激活事件的模型将有助于指导导管消融策略。方法:开发了一个二维、576×576节点的自动机来模拟心房电活动。通过在不同位置设置不同的不应期来改变基质场。以短的、随机定位的传导阻滞线的形式添加纤维化。使用更大面积的阻滞来模拟消融损伤。以2:1的比例施加各向异性。利用来自四个网格角之一的过早电冲动来启动激活。
当不应期斑块尺寸小于20×20mm时,无法诱导出旋转活动。对于更大的不应期区域,单个过早刺激能够平均诱导出1.19±1.10个转子,这些转子通常在斑块边缘附近形成。当不应期斑块尺寸接近整个左心房虚拟场大小时,最多可形成5个转子。转子沿着不应期斑块边缘形成,这是由于波前在转折点处延迟到达或由于存在足够大的纤维簇。然而,旋转活动也可能在没有空间可变不应期的情况下围绕大的纤维簇发生。当传导障碍尺寸不足时,新生转子会漂移,要么消失,要么在锚定到场中其他地方足够大的纤维簇上时稳定下来。如果没有传导障碍来充分延迟波前到达超过最长不应期,瞬态转子在穿过具有不同不应期的区域时会终止。当附近自旋速率更快的转子逐渐中断激活路径时,其他转子会被湮灭。通过移除或在足够区域进行模拟消融来消除锚点,可防止转子在原本会形成的特定位置出现。
在这个心房基质模拟中,传导障碍的存在和不应期的空间差异是启动和维持旋转活动的重要参数。