Difference between revisions of "Hilbert space"
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== See also == | == See also == | ||
*[[w:Linear algebra|Linear algebra]] | *[[w:Linear algebra|Linear algebra]] | ||
| + | *[[w:C*-algebra|C*-algebra]] | ||
*[[w:Wave function|Wave function]] | *[[w:Wave function|Wave function]] | ||
*[[w:Probability amplitude|Probability amplitude]] | *[[w:Probability amplitude|Probability amplitude]] | ||
Revision as of 02:55, 9 December 2008
Originally, classical mechanics was described by Newton's three laws, and these were geometrically expressed in the three-dimensional Cartesian coordinate system.
Hamilton formulated a new description of classical mechanics which was eventually housed in an infinite-dimensional phase space. In this space, a point represents the entire physical system.
First Dirac, and then Von Neumann set quantum theory in an infinite-dimensional complex ray space called Hilbert space. In this space, a ray, or single direction, represents a quantum state, as does the wave function in Schrödinger's formulation.
Each dimension in Hilbert space represents a possible state for a quantum system, so an unmeasured electron exists as a very complicated pattern.
A particular state is selected by projecting the total quantum ray on to one of the basic rays. The set of basic rays forms a frame of reference to observe some property. Each basic ray represents a possible choice or result of a measurement. The resulting coordinates are quantum probability amplitudes that are points in a complex plane, one plane for each basic ray. Points in the complex plane are two real dimensional vectors with a magnitude and also a direction known as the relative phase. The relative phase is observable when we change the experiment and measure a property that is incompatible with the original experiment.
The wave function description in Hilbert space cannot by itself tell us which state will be selected for reality. The projection, of the total ray onto a basic ray, multiplied by its complex conjugate projection is the real number probability for the transformation of a quantum potentiality into a classical actuality. The different quantum potentialities, which coherently co-exist in quantum reality, are mutually exclusive in the classical reality of our consciousness. A particle cannot be in two places at the same time in classical reality, but it is so in quantum reality. This point is basic to the so-called measurement problem and to our understanding of what underlies our three-dimensional world.
