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QUANTUM METAPHYSICS - E-thesis

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and phases. As every waveform corresponds to a unique Fourier spectrum, sine waves can be<br />

thought of as a universal alphabet which can be used to express any wave. Subsequently, it has<br />

been shown that there is nothing particularly special about Fourier sine waves, since any other<br />

waveform family such as impulse waves or spherical harmonics will do just as well, so a specific<br />

wave can be decomposed in many different ways. This means that there is no “natural” way to<br />

take a wave apart, and that unlike a clock, a wave has no specific intrinsic parts. 465 When<br />

considering their adaptation to quantum systems, this means that the same shape of wave can be<br />

represented in many different ways. The way of expression that is chosen will depend on the<br />

measurement being attempted.<br />

To some degree, Schrödinger's equation resembles the classical equations of motion of Hamilton<br />

and Maxwell. In fact, the relationship between Schrödinger's wave mechanics and classical<br />

mechanics has been compared to the relationship between wave optics and geometrical optics:<br />

classical mechanics represents a special case within the more general wave mechanics. 468 For<br />

example, while it is possible in certain situations to solve for the position of a particle with the<br />

probability "one" using the classical equation, i.e. with absolute certainty, the square value of the<br />

amplitude of the wave function at a given point is interpreted as the probability n/N, statistical<br />

likelihood with which a particle can be observed at that point if many measurements are made.<br />

The wave function was generally thought to be some kind of probability function and Max Born<br />

stated his probability interpretation in 1926. This idea, which replaced causally-problematic<br />

words concerning quantum jumps, was adopted into the developing Copenhagen<br />

interpretation. 469<br />

Schrödinger hoped his theory would show that the world fundamentally consisted of waves.<br />

However, he soon encountered problems when he tried to explain the world realistically by only<br />

using the wave explanation. In his equation, waves could not be interpreted as the waves of<br />

three-dimensional physical space, because in order to describe several particles one needs to<br />

operate with multi-dimensional spaces. Moreover, the waves are complex, and their form is<br />

465 Herbert 1985, 84-88.<br />

466 Herbert 1985, 72.<br />

467 Herbert 1985, 84-88.<br />

468 Petersen 1968, 90.<br />

469 Pais 1991, 286. March 1957, 105. While the Psi-function is in general complex in the technical mathematical<br />

sense, the square of its absolute value is real. The Psi-function is related to matters of observation by a circuitous<br />

route. Probabilities associated with Psi enter in the calculation of various other probabilities and some of these latter<br />

probabilities are finally coordinated by rules of correspondence with certain experimental concepts. Nagel 1961,<br />

307-308.<br />

182

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