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
german
Near-Field Optics with Regard to Newton's Diffraction-Experiments
The phenomenons of diffraction are new built up with regard to Newton's and newly diffraction experiments. By photons with structure and field diffraction is described as change of direction in consequence of interaction of the photon with its asymmetric returning field with use of vortex-dynamics By strong fade out, interaction or origin in smallest particles, can originate photons with an incomplete field. These photons can not interfere with its field and so are not to obey Abbe's formula for resolving power. But every photon completed soon its field and so was near-field optics possible only in shortest distances, as experiments show too.
.....
Comparison with the sound-field
Marti a. Krausch [17] compared near-field optics with phenomena in sound where also appear near-field effects which direct to a higher resolution. But between sound and light are fundamental differences. With our present knowledge sound bases in gaseous medium on periodic stimulations but then on impact-processes. The single gas-molecules move locally only little in propagation-direction till it hits the next molecule. At central impact they can pass down their energy, at eccentric impact only a part of energy is delivered and it results a change of direction. These changes of direction feign to do a Huygens' principle and cause at sound a diffraction as deflection. An interference of one molecule with itself in the form of interaction of molecule with ist field not known in sound. At limitation and periodic stimulation result diffractions which are only restrictively comparable with diffraction of light. If sound comes out of a very small source so have in short distance took place only few impacts and deviations from the original direction hardly make a difference, there exists also in sound a near-field with different properties.
References
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