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易化过程中递质释放统计数据的变化。

Changes in the statistics of transmitter release during facilitation.

作者信息

Zucker R S

出版信息

J Physiol. 1973 Mar;229(3):787-810. doi: 10.1113/jphysiol.1973.sp010167.

Abstract
  1. The statistical nature of transmitter release during facilitation was studied at single synaptic sites by recording extracellular excitatory junctional potentials from the claw opener muscle in crayfish.2. At low temperatures, single quanta could be counted in the responses to nerve impulses. The distribution of the number of quanta observed (x) was most accurately described by assuming that x is a binomial random variable.3. A quantitative estimate was made of the effects of errors in counting quanta due to the simultaneous release of quanta and the release of quanta which were not individually detectable above the noise of the recording system. Such errors of observation cannot account for the deviation of quantal release from a Poisson distribution.4. Facilitated release occurred in the responses to the second of two closely following nerve impulses and in the responses to successive impulses in a tetanus. In both cases, the increase in the average number of quanta released (m) could be attributed entirely to an increase in the probability (p) that available quanta were released.5. The results can be interpreted most easily in terms of a model in which the maximum number of releasable quanta is limited by a finite number of discrete release sites within recording distance of the microelectrode. In this model, the binomial parameter n is an estimate of the number of these sites, and the statistical parameter p is a compound probability depending on the rate of re-occupying sites after a nerve discharge and the probability that an impulse activates an occupied site.
摘要
  1. 通过记录小龙虾爪 opener 肌肉的细胞外兴奋性突触后电位,在单个突触位点研究了易化过程中递质释放的统计学性质。

  2. 在低温下,对神经冲动的反应中可以计数单个量子。假设 x 是二项式随机变量,观察到的量子数(x)的分布得到了最准确的描述。

  3. 对由于量子的同时释放和在记录系统噪声之上无法单独检测到的量子释放而导致的量子计数误差的影响进行了定量估计。这种观察误差不能解释量子释放偏离泊松分布的情况。

  4. 易化释放发生在对两个紧随其后的神经冲动中的第二个冲动的反应以及对强直刺激中连续冲动的反应中。在这两种情况下,释放的量子平均数量(m)的增加完全可以归因于可用量子被释放的概率(p)的增加。

  5. 就一个模型而言,结果最容易解释,在该模型中,可释放量子的最大数量受到微电极记录距离内有限数量的离散释放位点的限制。在这个模型中,二项式参数 n 是这些位点数量的估计值,统计参数 p 是一个复合概率,取决于神经放电后位点重新占据的速率以及冲动激活被占据位点的概率。

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J Physiol. 1960 Jan;150(1):134-44. doi: 10.1113/jphysiol.1960.sp006378.
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