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Philosophers
Mortimer Adler Rogers Albritton Alexander of Aphrodisias Samuel Alexander William Alston Anaximander G.E.M.Anscombe Anselm Louise Antony Thomas Aquinas Aristotle David Armstrong Harald Atmanspacher Robert Audi Augustine J.L.Austin A.J.Ayer Alexander Bain Mark Balaguer Jeffrey Barrett William Barrett William Belsham Henri Bergson George Berkeley Isaiah Berlin Richard J. Bernstein Bernard Berofsky Robert Bishop Max Black Susanne Bobzien Emil du Bois-Reymond Hilary Bok Laurence BonJour George Boole Émile Boutroux Daniel Boyd F.H.Bradley C.D.Broad Michael Burke Lawrence Cahoone C.A.Campbell Joseph Keim Campbell Rudolf Carnap Carneades Nancy Cartwright Gregg Caruso Ernst Cassirer David Chalmers Roderick Chisholm Chrysippus Cicero Tom Clark Randolph Clarke Samuel Clarke Anthony Collins Antonella Corradini Diodorus Cronus Jonathan Dancy Donald Davidson Mario De Caro Democritus Daniel Dennett Jacques Derrida René Descartes Richard Double Fred Dretske John Dupré John Earman Laura Waddell Ekstrom Epictetus Epicurus Austin Farrer Herbert Feigl Arthur Fine John Martin Fischer Frederic Fitch Owen Flanagan Luciano Floridi Philippa Foot Alfred Fouilleé Harry Frankfurt Richard L. 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Statistical Interpretation of the Wave Function
It is often said that Max Born gave us the “statistical interpretation” of quantum mechanics that lies at the heart of Niels Bohr’s and Werner Heisenberg’s principle of complementarity and so was included in their “Copenhagen Interpretation” of quantum mechanics. But Born himself said many times he had only applied an idea of Albert Einstein that had circulated privately for many years. To be sure, Born and Einstein quarreled for years over determinism and causality, but as we have seen, it was Einstein who in 1916 discovered “chance” in the statistical or "chance" interaction of matter and radiation, even if he considered chance a “weakness in the theory.” Probability and statistics were very important in the two centuries before Born’s work, but most physicists and philosophers saw the implied randomness to be “epistemic,” the consequence of human ignorance. Random distributions of all kinds were thought to be completely deterministic at the particle level, with collisions between atoms following Newton’s time-reversible dynamical laws. Ludwig Boltzmann’s transport equation and H-Theorem showed that the increase of entropy is statistically irreversible at the macroscopic level, even if the motions of individual particles were time reversible. Boltzmann did speculate that there might be some kind of molecular “chaos” or “disorder” that could cause particles traveling between collisions to lose the “correlations” or information about their past paths that would be needed for the paths to be time reversible and deterministic, but nothing came of this idea. In his early career, Erwin Schrödinger was a great exponent of fundamental chance in the universe. He followed his mentor Franz S. Exner, who as a colleague of Boltzmann at the University of Vienna was a great promoter of statistical thinking. In his inaugural lecture at Zurich in 1922, Schrödinger argued that available evidence can not justify our assumptions that physical laws are deterministic and strictly causal. His inaugural lecture was modeled on that of Exner in 1908. Exner’s assertion amounts to this: It is quite possible that Nature’s laws are of thoroughly statistical character. The demand for an absolute law in the background of the statistical law — a demand which at the present day almost everybody considers imperative — goes beyond the reach of experience.
Several years later, Schrödinger presented a paper on
“Indeterminism in Physics” to the June, 1931 If nature is more complicated than a game of chess, a belief to which one tends to incline, then a physical system cannot be determined by a finite number of observations. But in practice a finite number of observations is all that we can make. All that is left to determinism is to believe that an infinite accumulation of observations would in principle enable it completely to determine the system. Such was the standpoint and view of classical physics, which latter certainly had a right to see what it could make of it. But the opposite standpoint has an equal justification: we are not compelled to assume that an infinite number of observations, which cannot in any case be carried out in practice, would suffice to give us a complete determination.In the history of science it is hard to find ears more likely to be sympathetic to a new idea than Schrödinger should have been to Max Born’s suggestion that the absolute modulus of the amplitude of Schrödinger’s wave function |ψ|
should be interpreted statistically
as the likelihood of finding a particle. And Schrödinger should
have known Einstein thought quantum mechanics is statistical.
Yet Schrödinger objected strenuously, not so much to the
probability and statistics as to the conviction of Born and his
brilliant student Heisenberg that quantum phenomena, like
quantum jumps between atomic energy levels, were only predictable
^{2}statistically, and that there is a fundamental indeterminacy in the
classical idea that particles have simultaneously knowable exact
positions and velocities (momenta). Born, Heisenberg, and Bohr
had declared classical determinism and causality untrue of the
physical world.
It is likely that Schrödinger was ecstatic that his wave equation implied a deterministic physical theory. His wave function ψ evolves in time to give exact values for itself for all times and places. Perhaps Schrödinger thought that the waves themselves could provide a field theory of physics, much as fields in Newton's gravitational theory and in Maxwell's electromagnetic theory provide complete descriptions of nature. Schrödinger began to wonder whether nature might be only waves, no particles.
In July of 1926, Born used Louis de Broglie’s matter waves
for electrons, as described by Schrödinger’s wave equation, but he
interpreted the wave as the Born's interpretation of the quantum mechanical wave function of a material particle as the probability (amplitude) of finding the material particle was a direct extension of Einstein's interpretation of light waves giving probability of finding photons. To be sure, Einstein's interpretation may be considered only qualitative, where Born's was quantitative, since the new quantum mechanics now allowed exact calculations and measurements to test its predictions. Born initially gave Einstein full credit for the statistical interpretation as Einstein had described his "ghost field" idea. Although the original idea is pure Einstein, it is widely referred to today as “Born’s statistical interpretation” or "Born's Rule," another example of others getting credit for a concept first seen by Einstein. Born described his insights in 1926, Collision processes not only yield the most convincing experimental proof of the basic assumptions of quantum theory, but also seem suitable for explaining the physical meaning of the formal laws of the so-called “quantum mechanics.”... The matrix form of quantum mechanics that was founded by Heisenberg and developed by him and the author of this article starts from the thought that an exact representation of processes in space and time is quite impossible and that one must then content oneself with presenting the relations between the observed quantities, which can only be interpreted as properties of the motions in the limiting classical cases. On the other hand, Schrödinger (3) seems to have ascribed a reality of the same kind that light waves possessed to the waves that he regards as the carriers of atomic processes by using the de Broglie procedure; he attempts “to construct wave packets that have relatively small dimensions in all directions,” and which can obviously represent the moving corpuscle directly. Neither of these viewpoints seems satisfactory to me. Here, I would like to try to give a third interpretation and probe its utility in collision processes. I shall recall a remark that Einstein made about the behavior of the wave field and light quanta. He said that perhaps the waves only have to be wherever one needs to know the path of the corpuscular light quanta, and in that sense, he spoke of a “ghost field.” It determines the probability that a light quantum - viz., the carrier of energy and impulse – follows a certain path; however, the field itself is ascribed no energy and no impulse. This last sentence is a remarkably concise description of the dualism in quantum mechanics, a strange mixture of indeterminism and determinism, of chance and necessity. In his 1948 Waynflete lectures, Born elaborated on his understanding of chance, There is no doubt that the formalism of quantum mechanics and its statistical interpretation are extremely successful in ordering and predicting physical experiences. But can our desire of understanding, our wish to explain things, be satisfied by a theory which is frankly and shamelessly statistical and indeterministic? Can we be content with accepting chance, not cause, as the supreme law of the physical world?Ever since 1930, when Born's young graduate student Heisenberg had been selected for the Nobel Prize in physics although much of the theory was his own work, Born felt he had been treated unfairly. He finally received recognition, with the Nobel Prize for physics in 1954, for his "statistical interpretation." But Born's voluminous correspondence with Einstein reveals that he had perhaps come to think that Einstein's supposed determinism meant Einstein did not believe in the statistical nature of quantum physics, so this idea may now rightfully belong to Born. He called it "his own" in the 1950's. Normal | Teacher | Scholar |