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Quantum dynamics and isotope effects of hydrogen
Quantum dynamics and isotope effects of hydrogen

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Correlations and Counting Statistics of an Atom Laser

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Surface Enhanced Raman Scattering Spectroscopy

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Probing a scattering resonance in Rydberg molecules with a Bose

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Spontaneous emission of an atom in front of a mirror

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Nonlinear atom optics - University of Arizona

... instigated the analogous field of nonlinear atom optics in which the atomic field effectively interacts with itself. It is well known that photons do not interact with each other in free space. In order to achieve the wave-mixing phenomena that are the hallmark of nonlinear optics, it is necessary t ...
my title - Ohio University Physics and Astronomy
my title - Ohio University Physics and Astronomy

... Yet, the atom still prefers to travel along the CP row and in doing so it moves away from the tip shortly after such an intersection (Fig. 4). At one point it can no longer continue to move along the CP row because of the large tip-atom distance. Then the atom stops traveling and rest for some time, ...
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The von Neumann entanglement entropy for Wigner

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Chapter 4 MANY PARTICLE SYSTEMS

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The Two Slit Experiment

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Lecture 6, Parity and Charge Conjugation

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From the Mendeleev periodic table to particle physics and - Hal-SHS

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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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