Sato Hirokazu, Yagi Tetsuo, Namekawa Akio, Ishida Akihiko, Yamashina Yoshihiro, Nakagawa Takashi, Sakuramoto Manjirou, Sato Eiji, Yambe Tomoyuki
Division of Cardiology, Sendai City Hospital, Wakabayashi-ku, Shimizukouji3-1, Sendai, Japan.
J Interv Card Electrophysiol. 2010 Jun;28(1):39-44. doi: 10.1007/s10840-010-9468-6. Epub 2010 Feb 23.
Pathological studies have demonstrated that the cavotricuspid isthmus (CTI) is often composed of discrete muscle bundles, which are thought to be represented electrically as high-amplitude electrograms. Based on this observation, we visualized the bundles using an electro-anatomical mapping system (EAMS) and investigate the efficacy of bundle ablation which is an ablation method for selectively targeting high-voltage sites obtained by high-density electro-anatomical mapping along the CTI.
Sixty patients with atrial flutter were randomly assigned to cavotricuspid isthmus ablation using a conventional anatomical approach (Group 1) or bundle ablation approach (Group 2). In Group 2, CTI was mapped in detail with EAMS, and we visualized the bundles that were 1.5 mV or more on a bipolar voltage map. Radiofrequency (RF) ablation was delivered sequentially from the maximum voltage site at the shortest distance of the bundle until bidirectional block was achieved.
Bidirectional block was achieved in all patients. Mean ablation times (Group 1, 1,392 + or - 960 s; Group 2, 638 + or - 342 s, p < 0.01), the mean number of RF applications (Group 1, 31.7 + or - 23.6; Group 2, 13.0 + or - 7.0, p < 0.01), and fluoroscopy times (Group 1, 50.4 + or - 28.3 min; Group 2, 42.3 + or - 21.3 min, p < 0.01) were significantly shorter in Group 2 than those in Group 1.
Bundle ablation at CTI is highly effective for achieving a bidirectional block requiring shorter ablation times, shorter fluoroscopy times, and fewer RF applications.
病理研究表明,腔静脉三尖瓣峡部(CTI)通常由离散的肌束组成,这些肌束在电活动上被认为表现为高振幅电信号。基于这一观察结果,我们使用电解剖标测系统(EAMS)对这些肌束进行可视化,并研究肌束消融的疗效,这是一种通过沿CTI进行高密度电解剖标测来选择性靶向高压部位的消融方法。
60例心房扑动患者被随机分为两组,分别采用传统解剖方法进行腔静脉三尖瓣峡部消融(第1组)或肌束消融方法(第2组)。在第2组中,使用EAMS对CTI进行详细标测,并在双极电压图上可视化电压为1.5 mV或更高的肌束。从肌束最短距离处的最大电压部位依次进行射频(RF)消融,直至达到双向阻滞。
所有患者均实现了双向阻滞。第2组的平均消融时间(第1组,1392±960秒;第2组,638±342秒,p<0.01)、平均RF应用次数(第1组,31.7±23.6;第2组,13.0±7.0,p<0.01)和透视时间(第1组,50.4±28.3分钟;第2组,42.3±21.3分钟,p<0.01)均显著短于第1组。
CTI处的肌束消融对于实现双向阻滞非常有效,所需的消融时间更短、透视时间更短且RF应用次数更少。