Newton's and Fresnel's Diffraction Experiments The Continuation of Newton's Diffraction
Experiments Diffraction of Light at Slit and Hindrance Interference-Angle Condition, Diffraction and
Imagery Diffraction One After Another and with
Intermediate Imagery Diminishing of Frequency of Light after
Diffraction Inner and Outer Diffraction-Fringes at
Circular Openings Superposition of Interference and Diffraction Diffraction Experiments with Inhomogeneous
Illumination Experiments with Polarized Light at Slit and
Double-Slit The Background of Diffraction-Figures Trial for Interpretation of Newton's Diffraction
Experiments Consequences for Photons out of Newton's
Diffraction Experiments Consequences for Structure of Electrons out of
that of Photons The Thermally Conditioned Electromagnetic Field Diffraction and Light-Emission of Electrons Energy-Steps of Electrons in Magnetic Eigen-Field Faraday's Electro-tonic States Near-Field Optics with Regard to Newton's
Diffraction-Experiments Consideration of Magnetic Moment of Electron
in Quantum Theories |
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Consideration of Magnetic Moment of Electron in Quantum Theories
In previous papers were shown that the consideration of magnetic moments delivered new aspects by introducing into spin and Bohr's atomic model. In this paper could be shown that with 'on electrons coupled magnetic current-tubes' in quantum-field theory as well as vivid consideration of magnetic moment of electron and Lorentz-force can give the same results. This shows that quantum-theory is necessary for completion. Einstein was right that he marked Heisenberg-Bohr's quantum theory as incomplete. General is shown that the designation of wave is to change for field, in light and also in matter.. .....ConclusionAs already described in section I, the Copenhagen interpretation is by consideration of Newton's diffraction experiments without physical basis. Out of these and newer experiments is deduced that also the foundation of the whole quantum-theory is to inspect. The consideration of magnetic moment of electron demands the definition of spin instead of formal magnetic spin-quantum numbers to replace by spin- or better vortex-aggregates. Therefore the structure of vortex-pair for photon and the structure of vortex-twin for electron are offered. Quantum-electro-dynamics has instead of second quantization to consider the building of photons within the so called life-time. Here is to calculate really the magnetic moment of electron circulating round the nucleus and not to interpret formal as coupled magnetic stream-sheet. References[1] A. J. Fresnel, Oeuvres complétes 1. Paris 1866; Abhandlungen über die Beugung des Lichtes. Ostwalds Klassiker Nr. 215, Engelmann, Leipzig 1926. [2] L. de Broglie, J. Phys. Radium 8 (1927) 225-241. [3] H. Nieke, Newtons Beugungsexperimente und ihre Weiterführung. Halle 1997, Comp. Print 1, Arbeit 1 (Vorhanden in vielen deutschen Universitätsbibliotheken); Newton's Diffraction Experiments and their Continuation. Halle 1997, comp. print 3, paper 1 (Available in some university libraries). [4] As [3], paper 2. [5] I. Newton, Opticks, or a Treatise of the Reflexions, Refractions, Inflexions and Colours of Light. London 1704; Opera quae exstant omnis, Tom IV. London 1782; Optics. Reprint, Bruxelles 1966; Optik II + III, Übers. W. Abendroth, Ostwald's Klassiker Nr. 97, Engelmann, Leipzig 1898; Neuauflage Bd. 96/97, Vieweg, Braunschweig 1983. Optique, Trac. J. P. Marat 1787; Reproduction Bourgois, Paris 1989. [6] As [3], paper 12. [7] E. Schrödinger, Ann. Physik IV 81 (1926) 109. [8] W. Heisenberg, Introduction to Unifom Field Theory of Elementary Particles. Interscience, New York 1966; Einführung in die einheitliche Feldtheorie der Elementarteilchen. Hirzel, Stuttgart 1967, S. 116. [9] As [3], paper 14. [10] W, Pauli, Aufsätze und Vorträge über Physik und Erkenntnistheorie. Vieweg, Braunschweig 1961, S. 120-146 (Nobelvortrag 1946); Z. Physik 31 (1925) 373, 765. Collected and Selected Papers. New York 1964. [11] As [3], paper 17. [12] M. Düren, Phys. BI. 52 (1996) Nr.3, 243-6; Desy Hermes 95 - 02 (1995). [13] As [3], paper 6. [14] As [3], paper 13. [15] S.-S. Chern a. J. Simons, Proc. Nat. Acad. Sci. USA. 68 (1971) 791; Ann. of Math. 99 (1974) 48-69 S.-S. Chern, Selected Papers Vol. 1. Springer, New York, ... 1980. paper 103 p. 444-465. [16] S.-S. Chern, Complex Manifolds without Potential Theory. Second edition, Universaltext, Springer, Berlin u.a. 1995, § 7, p.148-154 u. 157. [17] C. Rebbi a. G. Soliani, Solitons and Particle Physics. World Scientific, Singapore 1985. [18] W. Weller, Phys. BI. 52 (1996) 121-4. [19] G. Dunne, Self-Dual Cern-Simons Theories. Lecture Notes Physics M 36 Springer, Berlin 1995. [20] E. Guadagnini, The Link Invariants of the Chern-Simons Field Theory. De Gruyter, Berlin 1993, p. 5 [21] F. Ehrenhaft, Acta physica austrica 4 (1951) 461-88; 5 (1952) 12-29. [22] O. Carnal u. J. Mlynek, Phys. Bl. 47 (1991) Nr. 5, 379-81; Phys. Rev. Lett. 66 (1991) Nr. 21, 2689-96. [23] J. L. Staudenmann, S. A. Werner, R. Colelia a. A. W. Overhauser, Phys. Rev. A 21 (1980) 1419-38. [24] J. S. Bell, Speakable and unspeakable in quantum mechanics. Cambridge Univ. Press Cambridge a. o. 1987. Nr. 17 p. 159-168; Foundations of Physics 12 (1982) 989-99. [25] As [24] Nr. 1, p. 1-13, Nr. 4, p. 29-39; Rev. Mod. Phys. 38 (1966) 447-52 In German: M. Baumann u. R. U. Sexl, Deutungen der Quantentheorie. Vieweg, Braunschweig/Wiesbaden 1987, S. 193-205. [26] E. Schrödinger, Ann. Physik (4) 82 (1927) 257. [27] D. Bohm, Phys. Rev. 85 (1952) 166-179. [28] Y. Aharonova, a. A. Casher, Phys, Rev. Lett. 53 (1984) 319. [29] Y. Aharonov a. D. Bohm, Phys. Rev. 115 (1959) 485; Y. Imry u. R. A. Web, Spectrum d. Wiss. 1989 Juni 88-95. Sc. Am. (USA) 1989, April 36. [29] Y. Aharonov a. A. Casher, Phys. Rev. Lett. 53 (1984) 319. [30] K. Zeiske, G. Zinner, F. Riehle u. J. Helmcke, Phys. Bl. 51 (1995) Nr. 12, 1188-9; Appl. Phys. B 60 (1995) 205. [31] M. Boz, V. Fainberg, N. K.Pak, Ann. Phys. N.Y. 246 (1996) 374. [32] F. Hund, Materie als Feld. Springer, Berlin, Göttingen, Heidelberg 1954.
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