3 Conclusions.3.1 The Hyperfine Structure.The result achieved here with regard to the prediction of the hyperfine spectra, i.e. the 21.1cm line, is in complete agreement with observation, but of course has had the benefit of the adjustment of the semi-empirical parameter dp to ensure this. Consequently, factors which are perhaps more significant than this numerical result, are that it has been possible to identify aspects of the physics which complete the characterisation of hyperfine emissions in the resurrected theory. These factors are listed and briefly discussed below. One aspect of the numerical results that should be mentioned however, is spectral emission "bandwidth". It can be seen from Table A.3 that due to the extra inter-shell transitions introduced by the hyperfine orbitals, each individual emission line of the fine structure spectral signature, acquires a bandwidth. For the orbit shells considered, this ranges from 0.0003Å to 0.0035Å. This range is well within pressure variation and/or Doppler pulse broadening effects, and would not therefore be discernible in experimental results. The factors mentioned above significant to the characterisation of the hyperfine structure are listed as follows. (i) Only one relatively simple mathematical formulation is necessary to represent the complete spectral signature of hydrogen in the resurrected Bohr/Sommerfeld theory, i.e. (2.7) or, fully expanded, [2], Eq.(4.2). Finally, it should be noted that in the literature it is stated that the hyperfine emission of hydrogen, the 21.1cm line, does not appear in laboratory experiments. Clearly, in this theory of atomic structure, this would be due to the absence of the external stimulus that initiates it in inter-stellar hydrogen. 3.2 The Overall Theory. With the inclusion of the hyperfine structure, apart from the additional
analysis discussed in [2] to refine accuracy, the part of the
Bohr/Sommerfeld theory of atomic structure that deals with the prediction of
the wavelengths of spectral signatures, to the level of precision targeted,
is now virtually complete. It only remains to develop a mathematical
formulation to predict relative intensities. However, only hydrogen has been
considered in detail in these series of papers, and while the majority of
the content would be applicable to other outer shell single electron atoms,
derivation of their hyperfine structure, and the finer details of their fine
structure, would require further refinement of the final orbital energy
relationship to take account of their multi-particle nuclei, and possibly,
electron inter-action and electron shielding of the central nuclear charge.
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P.G.Bass, August 2007
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