The Bootstrap Principle and the Uniqueness of the World

B. Nicolescu
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Abstract

The bootstrap hypothesis emerged first as a possible explanation of certain experimental data in particle physics. This hypothesis was formulated for the first time in 1959 by Geoffrey Chew (1959; Chew & Jacob, 1964), a professor at the University of California, Berkeley, and was immediately used, for detailed physics calculations, by Chew and Mandelstam (1961). The word bootstrap itself is untranslatable. Indeed, bootstrap, in the proper sense laces, also means to levitate while dragging your boots. The most appropriate term in translation would be that of self-consistency. The bootstrap theory has emerged as a natural reaction against classical realism, which received a death blow, and against the idea, to which it was associated, of a need for equations of motion in space-time, during the formulation of quantum mechanics, around 1930. According to Newton, we learned about the existence of equations of motion, in order to describe physical reality: Newton’s equation regarding macroscopic bodies, Maxwell’s equations for electric and magnetic fields, and Schrödinger and Dirac’s equations for the movements of atomic systems. The movement described by these equations is that of certain entities considered as fundamental building blocks of physical reality, defined at each point of the space-time continuum. By definition, these equations possess an intrinsic deterministic character (the fact that, in some cases, large ensembles of objects can lead to a chaotic behavior does not alter the deterministic character of the basic equations of motion). Quantum entities are not subject to classical determinism. The bootstrap theory is just drawing the logical conclusions of this situation by proposing the abdication of any equation of motion. This attitude is consistent with the schedule of the matrix S (S is the initial for the English word scattering) initiated by Heisenberg in 1943: A realist theory must be expressed in terms of quantities directly related to experimental observation (Cushing, 1990). The abdication of any equation of motion has an immediate consequence: the absence of any fundamental brick of physical reality. In bootstrap, the part appears simultaneously as the whole. Nature is conceived as a global entity, inseparable at a fundamental level. The particle plays the role of a system in the irreducible interaction with other systems, which is a first rapprochement between the bootstrap theory and the current systemic thinking.
引导原理与世界的唯一性
自举假说最初是作为对粒子物理学中某些实验数据的可能解释而出现的。这一假说在1959年由Geoffrey Chew (1959;加州大学伯克利分校的教授Chew & Jacob, 1964),并立即被Chew和Mandelstam(1961)用于详细的物理计算。bootstrap这个词本身是不可翻译的。事实上,bootstrap,在正确的意义上,也意味着在拖着你的靴子漂浮。翻译中最恰当的术语应该是“自洽”。自举理论的出现,是对经典实在论的一种自然反应。经典实在论在1930年左右形成量子力学时,受到了致命的打击,也反对与自举理论相关联的需要时空运动方程的想法。根据牛顿的理论,我们了解了运动方程的存在,以便描述物理现实:牛顿关于宏观物体的方程,麦克斯韦关于电场和磁场的方程,Schrödinger和狄拉克关于原子系统运动的方程。这些方程所描述的运动是某些实体的运动,这些实体被认为是物理现实的基本组成部分,在时空连续体的每一点上都有定义。根据定义,这些方程具有内在的确定性特征(事实上,在某些情况下,大量物体的集合可能导致混沌行为,但不会改变基本运动方程的确定性特征)。量子实体不受经典决定论的约束。自举理论只是通过提出放弃任何运动方程来得出这种情况的逻辑结论。这种态度与海森堡于1943年提出的矩阵S (S是英语单词scattering的首字母)的时间表是一致的:现实主义理论必须用与实验观测直接相关的量来表达(Cushing, 1990)。放弃任何运动方程都有一个直接的后果:物理实在的任何基本组成部分的缺失。在bootstrap中,部分作为整体同时出现。自然被认为是一个全球性的实体,在基本层面上是不可分割的。粒子在与其他系统不可约的相互作用中扮演一个系统的角色,这是自举理论与当前系统思想的第一次和解。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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