Interrelations between Mathematics and Experiment in the Present Structure of Quantum Electrodynamics

DOI: 10.4236/oalib.1102211   PDF   HTML   XML   776 Downloads   1,183 Views   Citations


The electromagnetic interaction of the hydrogen atom is used as an experimental device and the data prove that bound fields and radiation fields are different physical objects. A further analysis proves that there is no direct interaction between radiation fields and there is no self-interaction of fields of an elementary pointlike charge. Therefore, bound fields and radiation fields should be treated differently and radiation fields emitted from two different sources should be treated separately. The fields term of the electromagnetic Lagrangian density Lem=-Fuv Fuv/16π; does not abide by these properties of electromagnetic fields, because Fuv is the sum of all kinds of fields. This is the underlying reason for the infinities of quantum electrodynamics and for the erroneous energy-momentum tensor which is obtained from an analysis of Lem.

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Comay, E. (2015) Interrelations between Mathematics and Experiment in the Present Structure of Quantum Electrodynamics. Open Access Library Journal, 2, 1-6. doi: 10.4236/oalib.1102211.

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[1] Landau, L.D. and Lifshitz, E.M. (2005) The Classical Theory of Fields. Elsevier, Amsterdam.
[2] Weinberg, S. (1995) The Quantum Theory of Fields. Vol. I. Cambridge University Press, Cambridge.
[3] Peskin, M. E. and Schroeder, D. V. (1995) An Introduction to Quantum Field Theory. Addison-Wesley, Reading, MA.
[4] Ryder, L.H. (1997) Quantum Field Theory. Cambridge University Press, Cambridge.
[5] Bjorken, J.D. and Drell, S.D. (1965) Relativistic Quantum Fields. McGraw-Hill, New York.
[6] Dirac, P.A.M. (1963) The Evolution of the Physicist’s Picture of Nature. Scientific American, 208, 45-53.
[7] Feynman, R.P. (1990) QED, The Strange Theory of Light and Matter. Penguin, London.
[8] Pohl, R., et al. (2010) The Size of the Proton. Nature, 466, 213-216.
[9] Jackson, J.D. (1975) Classical Electrodynamics. John Wiley, New York.
[10] Soper, D.E. (1976) Classical Field Theory. Wiley, New York.
[11] Wigner, E. (1960) The Unreasonable Effectiveness of Mathematics in the Natural Sciences. Comm. Communications on Pure and Applied Mathematics, 13, 1-14.
[12] Munoz, G. (1996) Lagrangian Field Theories and Energy-Momentum Tensors. American Journal of Physics, 64, 1153-1157.
[13] Schiff, L.I. (1955) Quantum Mechanics. McGraw-Hill, New York.
[14] Merzbacher, E. (1970) Quantum Mechanics. John Wiley, New York.
[15] Comay, E. (1991) Lorentz Transformation of Electromagnetic Systems and the 4/3 Problem. Zeitschrift für Naturforschung A, 46, 377-383.

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