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The Crystal Structure of Beryllium and of Beryllium Oxide
Author(s) -
L. W. McKeehan
Publication year - 1922
Publication title -
proceedings of the national academy of sciences
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 5.011
H-Index - 771
eISSN - 1091-6490
pISSN - 0027-8424
DOI - 10.1073/pnas.8.9.270
Subject(s) - induced pluripotent stem cell , beryllium , in vitro , biophysics , stem cell , fluorescence , regenerative medicine , chemistry , fluorescence microscope , myocyte , biomedical engineering , microbiology and biotechnology , nanotechnology , materials science , biology , medicine , biochemistry , physics , embryonic stem cell , organic chemistry , quantum mechanics , gene
before collision. No drop is seen at 5.4 volts which would correspond to the loss of 10.4 volts which is normally assumed to take place at ionization. From curves of such nature for different velocities of impact, it has been possible to determine more surely than heretofore the energy losses at electron impact. The outstanding results of the investigation are: 1. The discovery by Mohler, Foote and Meggers of a resonance potentialt nvolving an energy loss of 6.7 volts was confirmed. The work from which these investigators were able to deduce the existence of this critical potential seemed subject to some very serious difficulties in interpretation. These difficulties have been cleared up. The 6.7 volt type of collision does not occur for electrons with energies less than 8.5 volts, but at voltages above the ionization point it is the most important type of resonating collision. 2. Indications were also found that a collision involving an energy loss of about 5.7 volts also occurs in mercury. This is in-agreement with the fact that absorption lines have been found by previous investigators in the mercury spectrum in a region which through the quantum relation corresponds to this potential. 3. Little has been hitherto known about the nature of the ionizing collision. The present method has cast some light on this matter. The results obtained indicate that at such a collision the impinging electron loses all of its energy, and also that the electron which is the product of the ionization leaves the parent atom with negligible energy. This conclusion is at variance with the usual conception of the ionization process.

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