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通过在突触处的细胞附着记录揭示了两种融合孔开放模式
Liming He1, Xin-Sheng Wu, Raja Mohan
1National Institute of Neurological Disorders and Stroke, 35 Convent Drive, Building 35, Room 2B-1012, Bethesda, Maryland 20892, USA.
Nature
|October 27, 2006
概括
一个有争议的机制 - - 亲吻逃跑融合 - - 发生在突触处,可以产生快速的突触后电流. 不同的融合孔尺寸控制着突触电流的动力学和振幅.
科学领域:
- 神经科学是一个神经科学.
- 细胞生物学 细胞生物学
- 生物物理学的生物物理.
背景情况:
- 囊泡与细胞膜的融合释放神经递质.
- 聚合孔的大小会影响发射器释放率.
- 讨论了"亲吻逃跑"融合及其在突触传输中的作用.
研究的目的:
- 在突触处的单囊泡融合过程中研究融合孔动力学.
- 确定"亲吻和逃跑"融合是否发生在杯状突触.
- 评估不同尺寸的融合孔对突触电流的贡献.
主要方法:
- 在单囊泡融合过程中记录聚变孔动力学.
- 分析电容闪时间和聚变孔导电性 (G(p)).
- 完全崩和"亲吻和逃跑"的融合事件之间的区别.
主要成果:
- 在杯状突触中观察到完全崩和"亲吻和逃跑"融合.
- 完全崩显示出高的初始G (p) (>375 pS) 随着快速增加.
- "亲吻和逃跑"的核聚变显示了短暂的电容闪 (<2秒),G(p) 从15-288 psi到>288 psi不等.
结论:
- 吻和逃跑融合被证实在突触中发生.
- 融合孔径大小的变化,包括"亲吻和跑步",可以产生快速的突触后电流.
- 不同的融合孔尺寸调节突触电流动力学和振幅.
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