The standard interpretation of Young’s double slit experiment is that the light behaves as waves before and after passing through the diaphragm of the double slit. There is one primary maximum intensity at the central position of the interference pattern. Recently, the photon chamber has been proposed and utilized to study the behavior of photons near the detecting screen. The experiments show that the light, near the screen, behaves as photons propagating along the straight-line trajectories that distribute as waves. In this article, we place the photon chamber near the diaphragm of the double slit. The Experiments show, the first time, that (1) within certain distance from the diaphragm, there is the non-wave pattern (two photon tracks), which indicates that the standard double slit experiments violate the wave interpretations; (2) the light beams behave as photons near the double slit.
The standard interpretation of Young’s double slit experiment is that the light behaves as waves before and after passing through the diaphragm of the double slit. There is one primary maximum intensity at the central position of the interference pattern. Recently, the photon chamber has been proposed and utilized to study the behavior of photons near the detecting screen. The experiments show that the light, near the screen, behaves as photons propagating along the straight-line trajectories that distribute as waves. In this article, we place the photon chamber near the diaphragm of the double slit. The Experiments show, the first time, that (1) within certain distance from the diaphragm, there is the non-wave pattern (two photon tracks), which indicates that the standard double slit experiments violate the wave interpretations; (2) the light beams behave as photons near the double slit.
The standard interpretation of Young’s double slit experiment is that the light behaves as waves before and after passing through the diaphragm of the double slit. There is one primary maximum intensity at the central position of the interference pattern. Recently, the photon chamber has been proposed and utilized to study the behavior of photons near the detecting screen. The experiments show that the light, near the screen, behaves as photons propagating along the straight-line trajectories that distribute as waves. In this article, we place the photon chamber near the diaphragm of the double slit. The Experiments show, the first time, that (1) within certain distance from the diaphragm, there is the non-wave pattern (two photon tracks), which indicates that the standard double slit experiments violate the wave interpretations; (2) the light beams behave as photons near the double slit.
The standard interpretation of Young's double slit experiment is that the light behaves as waves before and after passing through the diaphragm of the double slit. There is one primary maximum intensity at the central position of the interference pattern. Recently, the photon chamber has been proposed and utilized to study the behavior of photons near the detecting screen. The experiments show that the light, near the screen, behaves as photons propagating along the straight-line trajectories that distribute as waves. In this article, we place the photon chamber near the diaphragm of the double slit. The Experiments show that (1) at 2 mm to 150 mm range from the diaphragm, there are two primary maximum intensities, i.e., the pattern is non-interference, which violates the wave interpretations; (2) the light beams behave as photons, which violate the wave particle duality and Bohr's complementarity.
Abstract The standard interpretation of Young’s double slit experiment is that the light behaves as waves before and after passing through the diaphragm of the double slit. There is one primary maximum intensity at the central position of the interference pattern. Recently, the photon chamber has been proposed and utilized to study the behavior of photons near the detecting screen. The experiments show that the light, near the screen, behaves as photons propagating along the straight-line trajectories that distribute as waves. In this article, we place the photon chamber near the diaphragm of the double slit. The Experiments show: (1) at approximate up to 150 mm range from the diaphragm, there are two primary maximum intensities (Figure on the left), which violates the standard wave interpretations (Figure on the right); (2) the light beams behave as photons.
Young’s double slit experiment revived the wave theory of the light. The standard interpretation is that the light behaves as waves before and after passing through the diaphragm of the double slit. Feynman called the double slit experiment the only mystery in quantum mechanics. Recently, the photon chamber has been proposed and utilized to study the behavior of photons near the detecting screen. The experiments show that the light, near the screen, behaves as photons propagating along the straight-line trajectories, and the trajectories distribute as waves. Furthermore, the photon chamber experiments show that, withing a macroscopic distance from the double slit, the pattern is non-interference, which indicates that the standard double slit experiments violate the standard wave interpretations in the area near the diaphragm. In this article, we utilize two new methods to study how the non-interference pattern (near the double slit) evolving to the interference pattern (far from it). The experiments show, the first time, that (1) the shape of the pattern are distance-dependent, when the distance increases, the non-interference pattern evolves to the interference pattern, which indicates that the non-wave nature and the wave distribution coexist in the same wave experiment; (2) the light beams behave as photons near the double slit. The experiments: (1) provide novel phenomena/data for further theoretical development of the established optics and for understanding the nature of the light; (2) show the Feynman’s mystery in the different perspectives; (3) provide three methods that show the non-wave pattern in standard wave experiments and can be utilized to develop the classical optics further.
The standard interpretation of Young’s double slit experiment is that the light behaves as waves before and after passing through the diaphragm of the double slit. There is one primary maximum intensity at the central position of the interference pattern. Recently, the photon chamber has been proposed and utilized to study the behavior of photons near the detecting screen. The experiments show that the light, near the screen, behaves as photons propagating along the straight-line trajectories that distribute as waves. Furthermore, the photon chamber placed near the double slit shows the non-interference pattern. blob:https://www.techrxiv.org/66ec822d-f054-4cc3-8b9e-8ff89d6481e2 In this article we show how the non-interference (non-wave) pattern evolves gradually to the interference pattern: (1) at 50 mm from the diaphragm of the double slit, the non-interference pattern shows and has two primary maximum intensities (Figure (a)); (2) at 150 mm, the two intensities of the non-interference pattern become wider and closer (Figure (b)); (3) at 200 mm, the two intensities of the non-interference pattern merge (Figure (c)); (4) at 400 mm, the non-interference pattern evolves to the interference pattern(Figure (d)). The interpretations of the optics wave and electromagnetic wave theories of the double slit experiments is incomplete. This phenomenon provides information for further theoretical development.
The standard interpretation of Young’s double slit experiment is that the light behaves as waves before and after passing through the diaphragm of the double slit. There is one primary maximum intensity at the central position of the interference pattern. Recently, the photon chamber has been proposed and utilized to study the behavior of photons near the detecting screen. The experiments show that the light, near the screen, behaves as photons propagating along the straight-line trajectories that distribute as waves. Furthermore, the photon chamber placed near the double slit shows the non-interference pattern. blob:https://www.techrxiv.org/66ec822d-f054-4cc3-8b9e-8ff89d6481e2 In this article we show how the non-interference (non-wave) pattern evolves gradually to the interference pattern: (1) at 50 mm from the diaphragm of the double slit, the non-interference pattern shows and has two primary maximum intensities (Figure (a)); (2) at 150 mm, the two intensities of the non-interference pattern become wider and closer (Figure (b)); (3) at 200 mm, the two intensities of the non-interference pattern merge (Figure (c)); (4) at 400 mm, the non-interference pattern evolves to the interference pattern(Figure (d)). The interpretations of the optics wave and electromagnetic wave theories of the double slit experiments is incomplete. This phenomenon provides information for further theoretical development.