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Beyond the Cookie Cutter Paradigm
Beyond the Cookie Cutter Paradigm

"The physical vacuum ?"... or "Ether!" "Weak force" decay. Before me
"The physical vacuum ?"... or "Ether!" "Weak force" decay. Before me

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... of Ramsey spectroscopy, recall that for a single particle the precession angle ( v 0 2 v )T that is measured in the Ramsey method is, in the rotating frame, just the phase factor e 2i( v 0 2 v )T that the excited state ue& acquires relative to the ground state ug& during the freed precession period ...
Monday, Nov. 14, 2016
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... • One of the clearest conservation rule is the lepton number conservation – While photon and meson numbers are not conserved Monday, Nov. 14, 2016 ...
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... What Happens to the Beam as it Encounters the Step Potential? This largely depends on if the energy of the particles relative to Vo. Consider Case of when E < Vo When the energy of the incoming particle is less than the potential, classically we expect all particles to reflect back. Lets look at wh ...
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... n  the atom absorbs a higher-energy photon of ultraviolet radiation. n  Then, the atom emits two lower-energy photons, at least one of which is in the visible range. n  Consequently, by shinning ultraviolet “black light” on the fluorescent material, it glows with a bright color. ...
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Geiger–Marsden experiment



The Geiger–Marsden experiment(s) (also called the Rutherford gold foil experiment) were a landmark series of experiments by which scientists discovered that every atom contains a nucleus where its positive charge and most of its mass are concentrated. They deduced this by measuring how an alpha particle beam is scattered when it strikes a thin metal foil. The experiments were performed between 1908 and 1913 by Hans Geiger and Ernest Marsden under the direction of Ernest Rutherford at the Physical Laboratories of the University of Manchester.
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