Particles and Nuclei: Volume 2, Part 2


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The divisible atom

Charged meteoric particles as ice nuclei in the mesosphere. Part 2 : A feasibility study

Fluctuations in nuclear reactions - Ericson, T. Faessler, A.. Faessler eds. An attempt of a theory of beta radiation. Nuclear Shell Structure - Feenberg, Eugene et al. Fermi, E.. University of Chicago Press, Chicago. Feldman, G. Feynman, R. The salient features of charge density distributions of medium and heavy even-even nuclei determined from a systematic analysis of elastic electron scattering form factors - Friedrich, J.

Gasiorowicz, S.. Behavior of neutral particles under charge conjugation - Gell-Mann, Murray et al.


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  • Precision measurement of the mass difference between light nuclei and anti-nuclei;

Gell-Mann, M.. Mulvey eds. Press, Oxford. Status of neutrino masses and mixing - Giunti, Carlo Eur. Goldhaber, M.. Helicity of Neutrinos - Goldhaber, M. Golub, R.. Gottfried, K..

THE STRUCTURE OF THE NUCLEUS

Neutron electric dipole moment, ultracold neutrons and polarized He-3 - Golub, R. Measurement of the A-dependence of deep inelastic electron scattering - Gomez, J. Deep inelastic e p scattering in perturbation theory - Gribov, V. Griffiths, D. CERN Cour. Grupen, C.. Haxel, O..

THE STRUCTURE OF THE NUCLEUS

B46 , Phys. Herzberg, G.. Observation of a Dimuon Resonance at 9. Hoyle, F.. Nuclear and nucleon scattering of high-energy electrons - Hofstadter, R. Hughes, E. Kayser, B.. Dietz, H. Klapdor-Kleingrothaus A.. Kleinknecht, K.. Comments Nucl. Kopfermann, H.. Kossel, W.. Heavy Quark Systems - Kwong, Waikwok et al. Langacker, P.. World Scientific. Langacker eds. Lederman, L. Cool, R. Marshak eds. Lederer, C. Leo, W. The parton model and perturbation theory - Lipatov, L.


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  4. The measurement of the beta asymmetry in the decay of polarized neutrons - Liaud, P. Lohrmann, E..

    Aufl Stuttgart. The sizes of atoms, nuclei, and nucleons are measured by firing a beam of electrons at an appropriate target. The higher the energy of the electrons, the farther they penetrate before being deflected by the electric charges within the atom. For example, a beam with an energy of a few hundred electron volts eV scatters from the electrons in a target atom. The way in which the beam is scattered electron scattering can then be studied to determine the general distribution of the atomic electrons.

    At energies of a few hundred megaelectron volts MeV; 10 6 eV , electrons in the beam are little affected by atomic electrons; instead, they penetrate the atom and are scattered by the positive nucleus. Therefore, if such a beam is fired at liquid hydrogen , whose atoms contain only single protons in their nuclei, the pattern of scattered electrons reveals the size of the proton. At energies greater than a gigaelectron volt GeV; 10 9 eV , the electrons penetrate within the protons and neutrons, and their scattering patterns reveal an inner structure.

    Thus, protons and neutrons are no more indivisible than atoms are; indeed, they contain still smaller particles, which are called quarks. Quarks are as small as or smaller than physicists can measure. Similar experiments show that electrons too are smaller than it is possible to measure. Subatomic particle. Article Media.

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    Discovery of the electron and nucleus

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    Particles and Nuclei: Volume 2, Part 2 Particles and Nuclei: Volume 2, Part 2
    Particles and Nuclei: Volume 2, Part 2 Particles and Nuclei: Volume 2, Part 2
    Particles and Nuclei: Volume 2, Part 2 Particles and Nuclei: Volume 2, Part 2
    Particles and Nuclei: Volume 2, Part 2 Particles and Nuclei: Volume 2, Part 2
    Particles and Nuclei: Volume 2, Part 2 Particles and Nuclei: Volume 2, Part 2
    Particles and Nuclei: Volume 2, Part 2 Particles and Nuclei: Volume 2, Part 2
    Particles and Nuclei: Volume 2, Part 2 Particles and Nuclei: Volume 2, Part 2
    Particles and Nuclei: Volume 2, Part 2 Particles and Nuclei: Volume 2, Part 2

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