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  2. Alpha-particle spectroscopy - Wikipedia

    en.wikipedia.org/wiki/Alpha-particle_spectroscopy

    Note that the decay energy will be divided between the alpha-particle and the heavy recoiling daughter so that the kinetic energy of the alpha particle (T α) will be slightly less: T α = (234.043 601 / 238.050 788 2) 4.2699 = 4.198 MeV, (note this is for the 238g U to 234g Th reaction, which in this case has the branching ratio of 79%).

  3. Alpha particle - Wikipedia

    en.wikipedia.org/wiki/Alpha_particle

    Secondly, he found the charge-to-mass ratio of alpha particles to be half that of the hydrogen ion. Rutherford proposed three explanations: 1) an alpha particle is a hydrogen molecule (H 2) with a charge of 1 e; 2) an alpha particle is an atom of helium with a charge of 2 e; 3) an alpha particle is half a helium atom with a charge of 1 e.

  4. Alpha particle X-ray spectrometer - Wikipedia

    en.wikipedia.org/wiki/Alpha_particle_X-ray...

    This makes it possible to calculate the mass of the nucleus hit by the alpha particle. Light elements absorb more energy of the alpha particle, while alpha particles are reflected by heavy nuclei nearly with the same energy. The energy spectrum of the scattered alpha particle shows peaks from 25% up to nearly 100% of the initial alpha particles.

  5. Geiger–Nuttall law - Wikipedia

    en.wikipedia.org/wiki/Geiger–Nuttall_law

    In practice, this means that alpha particles from all alpha-emitting isotopes across many orders of magnitude of difference in half-life, all nevertheless have about the same decay energy. Formulated in 1911 by Hans Geiger and John Mitchell Nuttall as a relation between the decay constant and the range of alpha particles in air, [ 1 ] in its ...

  6. Rutherford backscattering spectrometry - Wikipedia

    en.wikipedia.org/wiki/Rutherford_backscattering...

    Rutherford backscattering spectrometry (RBS) is an analytical technique used in materials science.Sometimes referred to as high-energy ion scattering (HEIS) spectrometry, RBS is used to determine the structure and composition of materials by measuring the backscattering of a beam of high energy ions (typically protons or alpha particles) impinging on a sample.

  7. Bragg peak - Wikipedia

    en.wikipedia.org/wiki/Bragg_peak

    Energy lost by charged particles is inversely proportional to the square of their velocity, which explains the peak occurring just before the particle comes to a complete stop. [4] In the upper figure, it is the peak for alpha particles of 5.49 MeV moving through air.

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  9. Range (particle radiation) - Wikipedia

    en.wikipedia.org/wiki/Range_(particle_radiation)

    The range depends on the type of particle, on its initial energy and on the material through which it passes. For example, if the ionising particle passing through the material is a positive ion like an alpha particle or proton , it will collide with atomic electrons in the material via Coulombic interaction .