In the early years of the 1920s, as a sequential protégé of both Bohr and Born, the young physicist-mathematician Werner Karl Heisenberg (1901-1976) was debating whether Bohr’s quantum mechanics with its idea of quantum jumps or Schrödinger’s with its idea of standing matter waves is more realistically plausible and acceptable for the then growing modern post-Newtonian physics community. Both theories agree with the experimental discoveries of the science of spectroscopy by their independent theoretical calculations of the measured Rydberg constant. The first seems to indicate the particle nature of while the second the wave nature of the transport of useful energy and also providing a fundamental structure of matter. Nonetheless, the inseparability of this duality of particle and wave natures of matter and energy culminated in his discovery of the uncertainty principle in 1926.
With the help of Born and Jordan, Heisenberg had already fully developed matrix mechanics by 1925. Matrix mechanics uses the data accumulated from spectroscopic analyses. Organizing them led Heisenberg to the discovery of non-commutativity of products of conjugate variables for both the linear momentum and the wavelength of both particles and waves. In order to fit his matrix mechanics with Bohr’s and Schrödinger’s versions of quantum mechanics, he had to invent a new physical principle of uncertainty. This principle simply states that the product of the uncertainty of position and the uncertainty of linear momentum is never less than Planck’s constant of action, which has the same physical dimensions as angular momentum. Consequently, Einstein had indicated that the product of the uncertainty of energy and the uncertainty of temporal duration is also never less than Planck’s constant of action. This latter idea implies that great amount of energy can be borrowed from the quantum vacuum fluctuations for a very short time interval. However, the greater is the amount borrowed the lesser is the time this borrowed energy must be paid back to the quantum vacuum fluctuations such that their product can never be less than Planck’s constant of action. Borrowing almost infinite amount of energy would then require practically zero time interval for paying back, which is practically the same as not borrowing at all.


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