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使用8毫米消融导管进行肺静脉射频消融时微泡形成的发生率、时间进程及特征

Incidence, time course, and characteristics of microbubble formation during radiofrequency ablation of pulmonary veins with an 8-mm ablation catheter.

作者信息

Alaeddini Jamshid, Wood Mark A, Lee Benjamin P, Ellenbogen Kenneth A

机构信息

Division of Cardiology, Virginia Commonwealth University, Medical Center, Richmond, Virginia 23298-0053, USA.

出版信息

Pacing Clin Electrophysiol. 2006 Sep;29(9):979-84. doi: 10.1111/j.1540-8159.2006.00473.x.

Abstract

BACKGROUND

Microbubble formation during pulmonary vein (PV) radiofrequency (RF) ablation of atrial fibrillation (AF) occurs relatively frequently. Prior studies have shown that microbubble formation may be associated with an increased risk of complications. However, the incidence, time course, and temperature characteristics of microbubble formation during AF ablation with an 8-mm catheter have not been prospectively described in humans.

METHODS

We studied 46 (30 men, age 56+/-10 years) patients with AF who underwent RF ablation of PVs between January 2005 and December 2005 using an 8F, 8-mm Biosensetrade mark ablation catheter (Biosense-Webster, Diamond Bar, CA, USA). All patients underwent continuous intracardiac echocardiography (ICE). Microbubble patterns were classified as either type 1 (intermittent, scattered microbubble formation) or type 2 (explosive shower of dense microbubbles). Formation of any microbubbles was detected by ICE and the time, PV location, and electrode temperature were recorded.

RESULT

A total of 1,479 (32+/-13, range 12-73) RF lesions were delivered to 167 veins. Twenty (2%) lesions were classified as type 2. Since the number of lesions resulting in type 2 bubbles was very small, only type 1 lesions were included in the final analysis. Thirty-nine (85%) patients had at least one lesion associated with bubble formation during ablation (mean: 7+/-7 lesions, range 1-28 lesions). Twenty-three percent (327) of the RF lesions resulted in bubble formation. RF generator power setting during lesions resulting in bubble formation was lower than lesions which did not result in bubble formation (47.9+/-7.4 W vs 49.7+/-7.1 W, P<0.001). Logistic regression analysis revealed a significant negative correlation (P<0.001) between RF generator power settings and a positive correlation between the generator temperature settings and formation of bubbles (both P<0.02). However, the maximum temperature attained was not different between lesions resulting in bubble formation (n=327) and those which did not result in bubble formation (n=1,139). Fifty-three (16%) of the lesions associated with bubble formation occurred within 2-10 seconds after RF was begun. Bubble formation was significantly more frequent in left superior PVs compared to the other PVs (left superior PV 27.3% left inferior PV 18.6%, right superior PV 20.5%, and right inferior PV 18.8%, P=0.005, left superior PV vs other PVs, P<0.001) even after adjustment for the other factors including generator power settings and the temperature setting.

CONCLUSION

Bubble formation is common during RF ablation of PV with 8-mm tip catheter and can occur as early as 2 seconds after starting RF. RF generator power is negatively correlated with bubble formation while generator temperature settings are positively correlated with formation of bubbles. Microbubble formation is also more frequent with ablation of the left superior PV probably due to better catheter contact in that area.

摘要

背景

在心房颤动(AF)肺静脉(PV)射频(RF)消融过程中,微泡形成相对频繁。先前的研究表明,微泡形成可能与并发症风险增加有关。然而,使用8毫米导管进行AF消融时微泡形成的发生率、时间进程和温度特征尚未在人体中进行前瞻性描述。

方法

我们研究了2005年1月至2005年12月期间使用8F、8毫米Biosensetrade标记消融导管(美国加利福尼亚州钻石吧市Biosense-Webster公司)接受PVs射频消融的46例(30例男性,年龄56±10岁)AF患者。所有患者均接受连续心内超声心动图(ICE)检查。微泡模式分为1型(间歇性、散在微泡形成)或2型(密集微泡爆发性涌出)。通过ICE检测任何微泡的形成,并记录时间、PV位置和电极温度。

结果

共对167条静脉进行了1479次(32±13次,范围12 - 73次)RF消融。20次(2%)消融被归类为2型。由于导致2型气泡的消融次数非常少,最终分析仅纳入1型消融。39例(85%)患者在消融过程中至少有一次与气泡形成相关的消融(平均:7±7次,范围1 - 28次)。23%(327次)的RF消融导致气泡形成。导致气泡形成的消融过程中RF发生器功率设置低于未导致气泡形成的消融(47.9±7.4瓦对49.7±7.1瓦,P<0.001)。逻辑回归分析显示,RF发生器功率设置与气泡形成之间存在显著负相关(P<0.001),发生器温度设置与气泡形成之间存在正相关(两者P<0.02)。然而,导致气泡形成的消融(n = 327)与未导致气泡形成的消融(n = 1139)所达到的最高温度并无差异。与气泡形成相关的消融中有53次(16%)发生在RF开始后2 - 10秒内。与其他PVs相比,左上PVs中气泡形成明显更频繁(左上PV 27.3%,左下PV 18.6%,右上PV 20.5%,右下PV 18.8%,P = 0.005,左上PV与其他PVs相比,P<0.001),即使在调整包括发生器功率设置和温度设置等其他因素后也是如此。

结论

使用8毫米尖端导管进行PVs射频消融时气泡形成很常见,且可在开始RF后最早2秒出现。RF发生器功率与气泡形成呈负相关,而发生器温度设置与气泡形成呈正相关。左上PVs消融时微泡形成也更频繁,可能是由于该区域导管接触更好。

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