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QT离散度的细胞基础。

Cellular basis for QT dispersion.

作者信息

Antzelevitch C, Shimizu W, Yan G X, Sicouri S

机构信息

Masonic Medical Research Laboratory, Utica, New York 13504, USA.

出版信息

J Electrocardiol. 1998;30 Suppl:168-75. doi: 10.1016/s0022-0736(98)80070-8.

Abstract

The cellular basis for the dispersion of the QT interval recorded at the body surface is incompletely understood. Contributing to QT dispersion are heterogeneities of repolarization time in the three-dimensional structure of the ventricular myocardium, which are secondary to regional differences in action potential duration (APD) and activation time. While differences in APD occur along the apicobasal and anteroposterior axes in both epicardium and endocardium of many species, transitions are usually gradual. Recent studies have also demonstrated important APD gradients along the transmural axis. Because transmural heterogeneities in repolarization time are more abrupt than those recorded along the surfaces of the heart, they may represent a more onerous substrate for the development of arrhythmias, and their quantitation may provide a valuable tool for evaluation of arrhythmia risk. Our data, derived from the arterially perfused canine left ventricular wedge preparation, suggest that transmural gradients of voltage during repolarization contribute importantly to the inscription of the T wave. The start of the T wave is caused by a more rapid decline of the plateau, or phase 2 of the epicardial action potential, creating a voltage gradient across the wall. The gradient increases as the epicardial action potential continues to repolarize, reaching a maximum with full repolarization of epicardium; this juncture marks the peak of the T wave. The next region to repolarize is endocardium, giving rise to the initial descending limb of the upright T wave. The last region to repolarize is the M region, contributing to the final segment of the T wave. Full repolarization of the M region marks the end of the T wave. The time interval between the peak and the end of the T wave therefore represents the transmural dispersion of repolarization. Conditions known to augment QTc dispersion, including acquired long QT syndrome (class IA or III antiarrhythmics) lead to augmentation of transmural dispersion of repolarization in the wedge, due to a preferential effect of the drugs to prolong the M cell action potential. Antiarrhythmic agents known to diminish QTc dispersion, such as amiodarone, also diminish transmural dispersion of repolarization in the wedge by causing a preferential prolongation of APD in epicardium and endocardium. While exaggerated transmural heterogeneity clearly can provide the substrate for reentry, a precipitating event in the form of a premature beat that penetrates the vulnerable window is usually required to initiate the reentrant arrhythmia. In long QT syndrome, the trigger is thought to be an early afterdepolarization (EAD)-induced triggered beat. The likelihood of developing EADs and triggered activity is increased when repolarizing forces are diminished, making for a slower and more gradual repolarization of phases 2 and 3 of the action potential, which translates into broad, low amplitude and sometimes bifurcated T waves in the electrocardiogram. Our findings suggest that regional differences in the duration of the M cell action potential may be the basis for QT dispersion measured at the body surface under normal and long QT conditions. The data indicate that the interval delimited by the peak and the end of the T wave represents an accurate measure of regional dispersion of repolarization across the ventricular wall and as such may be a valuable index for assessment of arrhythmic risk. The presence of low amplitude, broad and/or bifurcated T waves, particularly under conditions of long QT syndrome, is indicative of diminished repolarizing forces and may represent an independent variable of arrhythmic risk, forecasting the development of EAD-induced triggered beats that can precipitate torsade de pointes. Although the QT interval, QT dispersion, the T wave peak-to-end interval, and the width and amplitude of the T wave often change in parallel, they contain different information and should not be expected to be e

摘要

体表记录的QT间期离散度的细胞基础尚未完全明确。心室肌三维结构中复极时间的异质性导致了QT离散度,这是动作电位持续时间(APD)和激动时间区域差异的继发结果。虽然许多物种的心外膜和心内膜在基底部-心尖部和前后轴上APD存在差异,但通常是逐渐过渡的。最近的研究也表明跨壁轴上存在重要的APD梯度。由于复极时间的跨壁异质性比沿心脏表面记录的更为突然,它们可能是心律失常发生的更严重基础,对其进行量化可能为评估心律失常风险提供有价值的工具。我们从动脉灌注的犬左心室楔形标本获得的数据表明,复极期间的跨壁电压梯度对T波的形成有重要作用。T波的起始是由于平台期或心外膜动作电位2期更快地下降,在心室壁上产生电压梯度。随着心外膜动作电位继续复极,该梯度增大,在心外膜完全复极时达到最大值;此时标志着T波的峰值。下一个复极的区域是心内膜,产生直立T波的初始下降支。最后复极的区域是M区,对T波的最后部分有贡献。M区的完全复极标志着T波的结束。因此,T波峰值与结束之间的时间间隔代表复极的跨壁离散度。已知会增加QTc离散度的情况,包括获得性长QT综合征(IA类或III类抗心律失常药物),会导致楔形标本中复极的跨壁离散度增加,这是因为药物优先延长M细胞动作电位。已知会减小QTc离散度的抗心律失常药物,如胺碘酮,也会通过优先延长心外膜和心内膜的APD来减小楔形标本中复极的跨壁离散度。虽然过度的跨壁异质性显然可为折返提供基础,但通常需要以早搏形式出现的促发事件穿透易损窗才能引发折返性心律失常。在长QT综合征中,触发因素被认为是早期后除极(EAD)诱发的触发搏动。当复极力量减弱时,发生EAD和触发活动的可能性增加,导致动作电位2期和3期复极更缓慢、更渐进,这在心电图上表现为T波宽大、低振幅,有时呈双峰。我们的研究结果表明,M细胞动作电位持续时间的区域差异可能是正常和长QT条件下体表测量的QT离散度的基础。数据表明,由T波峰值和结束界定的间期代表了整个心室壁复极区域离散度的准确测量,因此可能是评估心律失常风险的有价值指标。低振幅、宽大和/或双峰T波的存在,特别是在长QT综合征情况下,表明复极力量减弱,可能代表心律失常风险的一个独立变量,预示着可引发尖端扭转型室速的EAD诱发触发搏动的发生。虽然QT间期、QT离散度、T波峰末间期以及T波的宽度和振幅通常平行变化,但它们包含不同信息,不应期望它们……

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