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Phenomena will involve an interaction with theĪgency of observation not to be neglected. Bohr later regretted his 'irrationality' comment. The "point" at which the observation involves the quantum is called the Heisenberg "cut". The space-time co-ordination of different observersīohr denied an "independent reality" to quantum phenomena observation involves subjective elements dependent on both human senses and theoretical concepts. Will not be affected by any differences which On the coincidence of two independent events at As emphasised by Einstein,Įvery observation or measurement ultimately rests
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Has been so fruitful for the elucidation of theĬlassical theories. This appears, forĮxample, clearly in the theory of relativity, which Phenomena concerned may be observed withoutĭisturbing them appreciably. Phenomena is based entirely on the idea that the Indeed, our usual description of physical The causal space-time co-ordination of atomic processes. This postulate implies a renunciation as regards Theories and symbolised by Planck's quantum of Process an essential discontinuity, or rather individuality, Quantum postulate, which attributes to any atomic That its essence may be expressed in the so-called Of the quantum theory, it seems, as we shall see, The Schrdinger wavefunction for the electron in a hydrogen atom may be written: n l (r) Yl m(, ), where (r,, ) are spherical polar coordinates. The only information that was important was the size of the orbit. Which hence are involved in the formulation Compared to Bohrs model, It was a one-dimensional model that used one quantum number to describe the distribution of electrons in the atom. The "quantum postulate" is Bohr's assumption of "stationary states" and the discontinuous "quantum jump" of an electron between states, with the emission of radiation of frequency ν, following Planck's 1900 postulate of discrete oscillators with energy E = hν, with h Planck's famous constant for the "quantum of action". The French version was published as Bohr's contribution to the Solvay conference of 1927, although his talk in Brussels was quite different from this paper. This was Bohr's Como Lecture in September, 1927, famous as the first publication of his concept of " complementarity." It was also published in Dutch, French, and German versions. Originally published in a Supplement to Nature, April 14, 1928, p.580.
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