By Daniel Greenberger, Klaus Hentschel, Friedel Weinert
With contributions via prime quantum physicists, philosophers and historians, this complete A-to-Z of quantum physics offers a lucid knowing of key techniques of quantum conception and scan. It covers technical and interpretational features alike, and contains either conventional and new techniques, making it an necessary source for concise, updated information regarding the numerous points of quantum physics.
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Extra resources for Compendium of Quantum Physics: Concepts, Experiments, History and Philosophy
Thesis at the University of Copenhagen, he obtained a fellowship for postgraduate study abroad. J. Thomson, who was director of the Cavendish laboratory since 1884. The two personalities did not match, however, and Bohr soon decided to move on to Manchester where Ernest Rutherford introduced him to the intricacies of scattering experiments with α-rays and discussed his brand new nuclear core model of the atom. J. Thomson, Rutherford and Nagaoka ( Atomic models). g. , and . J. J. Thomson for his part rejected Bohr’s advances as “meretricious superficialities obtained without, or at the price of, an understanding of the mechanism of atoms” [7, p.
J. J. Thomson for his part rejected Bohr’s advances as “meretricious superficialities obtained without, or at the price of, an understanding of the mechanism of atoms” [7, p. 23]. J. Thomson’s hope to arrive at an intuitive, quasi-mechanical understanding of the atom was in vain – but at the time no one could be sure. Primary Literature 1. Alfred M. Mayer: Floating magnets. American Journal of Science 116, 248–9 (1878), also in Nature 17, 487–488 2. Alfred M. Mayer: On the morphological laws of the configurations formed by magnets floating vertically and subjected to the attraction of a superposed magnet.
2. By postulate (1), the value of A for any particular photon 1 cannot depend on the choice of what to measure at the distant station 2, nor on the outcome of that measurement. Similarly for A , B, B . 3. Hence each of the quantities A, A , B and B exists and takes a value +1 or −1 which is, in the case of A, independent of whether it is B or B which is measured at the distant station, and vice versa. In other words, the value of A which occurs in the product AB is identical to that occurring in AB , etc.