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vol 2: Synopsis part III: Modern physics page 19: John von Neumann
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John von Neumann(1903-1957) When George Cantor first announced the transfinite numbers, some theologians objected on the ground that the only actual infinity in existence is God. David Hilbert showed that these new infinities fitted easily into mathematics and described new class of infinite spaces known as function spaces. John von Neumann used Hilbert space to resolve the apparent conflict between the particle and wave (discrete and continuous) descriptions of the world, opening the way for the consistent development of quantum theory. Hilbert space is a function space. This means that each point in the space represents a function. A function is a mapping between a set of elements called the domain of the function (say x ) to a set called the range of the function (say y ). We write this y = f(x). Some functions can be represented very simply as an arithmetic expression, eg y = x 2. Then if x = 1, y = 1; x = 2, y = 4; x = 3, y = 9; and so on. This is a function whose range and domain are the natural numbers. When no law exists that enables the succinct expression of a function, we must represent it by a table of values. We note here that there are n! ways of mapping n things onto themselves. Since there are aleph(0) natural numbers, there are aleph(0)! functions whose range and domain are the natural numbers. In Hilbert space, functions are expressed as ordered lists of values called vectors. For a given application, the dimension of the appropriate Hilbert space must be equal to complexity of the state represented, ranging from 2 for the spin states of an electron to a countable infinity for the energy states of a hydrogen atom. In this respect, Hilbert space is a natural extension of ordinary three dimensional space. Quantum mechanics represents physical motion, that is changes of state, by operators which transform state vectors into one another. Since a change of state in the quantum world is generally accompanied by the emission or absorption of observable particles, quantum mechanics uses operators to represent observables. Different operators acting on state vectors yield the energy, momentum and angular momentum on the particles involved. When we come to consider two or more particles, the Hilbert space we need is the tensor product of the Hilbert spaces for the original particles. The size of the resulting Hilbert space grows exponentially with the number of particles represented, in the same way as the size of the number represented by an 'Arabic' numeral grows exponentially with the length of the numeral. It is this growth that leads us to suspect that the 'state vectors of the universe' are so large that they require the formal Cantor universe for their adequate representation. Books
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