Near-field electron laser

Abstract

A near-field electron laser includes a light source and a sealed container. The interior of the sealed container is filled with an electron gas, the light source produces incident light, under the irradiation of the incident light, electrons will be forced to vibrate, and emit secondary electromagnetic waves, so that the vibrating electrons are in the near-field of each other; the incident light causes an attractive force to be produced among the vibrating electrons, and under the action of the electric field intensity of the incident light and the attractive force, the electrons will vibrate in the same radial straight line and in the same direction, and have a constant frequency, amplitude, and phase difference; the interference effects of the radiation of the vibrating electrons are used to obtain a stronger directionality and intensity to form a laser light.

Claims

1. A near-field electron laser producing laser light from the near-field energy of vibrating electrons, comprising a light source and a sealed container; wherein the working medium of the laser is electron; the interior of the sealed container is filled with an electron gas, the light source produces an incident light which is a parallel monochromatic light or a laser light, the average distance between electrons in the sealed container is much smaller than the wavelength of the incident light, the electron number density is much greater than the negative third power of the wavelength of the incident light, and the product of the number of electrons in the sealed container and the distance between the electrons is much greater than the wavelength of the incident light, so that the vibrating electrons are in the near-field of each other; the electric field intensity direction of the incident light and the electric moments of the vibrating electrons are in the same radial straight line and in the same direction, and there exists a radial attractive force among the vibrating electrons; the radial attractive force among the vibrating electrons is controlled by controlling the charge amount and amplitude of an accelerating charge that produces the incident light and the distance between the light source and the vibrating electrons, so that the average kinetic energy of the electrons for thermal motion is reduced to nearly zero, and cause the electrons to vibrate in the same radial straight line and in the same direction and have a constant frequency, amplitude and phase difference, and the interference effects of the radiation of various vibrating electrons are used to obtain a stronger directionality and intensity to form a laser light; the incident light is produced by a vibrating electric dipole with a radiated electric field of {right arrow over (E(t))}: $\stackrel{.fwdarw.}{E\left(t\right)}=\frac{\mathrm{Qa}}{4{\mathrm{.Math.}}_0{c}^{2}R}{}^2\cos t$ where Q is charge amount, a is amplitude, is frequency, .sub.0 is a vacuum dielectric constant, c is a vacuum light speed, and R is the distance from an observation point to the centre of the vibrating electric dipole.

2. The near-field electron laser according to claim 1, wherein the sealed tube is evacuated first to remove impurities in the sealed tube, so that the pressure in the sealed tube is lower than 1 P.sub.a, and then the electron gas is injected; during the injection of the electron gas, the electron gas is irradiated with light to produce an attractive force among the vibrating electrons and facilitate the injection of the electron gas; the sealed tube is made of glass or plastic.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) The sole FIGURE is a schematic diagram of the near-field electron laser according to an embodiment of the present application.

DETAILED DESCRIPTION OF EMBODIMENTS

(2) A specific embodiment is described below, but specific implementations are not limited to this example.

(3) Referring to the FIGURE, if there is air inside a sealed container, the thermal kinetic energy of molecules in the air will affect the radiation intensity and directionality of a laser, therefore, the sealed container needs to be evacuated first so that the pressure in the sealed container is lower than 1 P.sub.a. After the vacuum is evacuated, an electron gas is injected, and during the injection of the electron gas, the electron gas is irradiated with light to produce an attractive force among vibrating electrons and facilitate the injection of the electron gas.

(4) To cause the vibrating electrons to be in the near-field of each other, the average distance between the electrons in the sealed container should be much smaller than the wavelength r<< of the incident light. Because there is the following relationship between the average distance r between the electrons and the electron number density n.sub.d:
rn.sub.d(62)

(5) Therefore, there is the following relationship between the electron number density n.sub.d and the wavelength of incident light:
n.sub.d>>.sup.3(64)

(6) That is, the electron number density is much greater than the negative cubic of the wavelength of the incident light. A required number of electrons can be known from the wavelength of the incident light.

(7) Because electrons are produced from gas ionization, a hydrogen molecule contains 2 electrons, and there are 6.02310.sup.23 hydrogen molecules per mole of hydrogen, the number of moles of hydrogen that need to be ionized can be known from the wavelength of the incident light.

(8) Because the interior of the sealed container is filled with the electron gas, the sealed container should be made of glass or plastic. The sealed tube is wrapped with a heat insulation material outside.

(9) After the electron gas is injected, the electrons are irradiated with the incident light so that the vibrating electrons are in the near-field of each other, and the electric field intensity direction of the incident light and the electric moments of the vibrating electron are in the same radial straight line and in the same direction. The radiation intensity and directionality of the laser can be enhanced by increasing the frequency of the incident light, increasing the charge amount Q and amplitude of the accelerating charge that produces the incident light, decreasing the distance between the vibrating electrons and the accelerating charge that produces the incident light, and increasing the number of vibrating electrons.

REFERENCE DOCUMENTS

(10) 1. BingXin Gong, 2013, The light controlled fusion, Annals of Nuclear Energy, 62 (2013), 57-60. 2. Guo Shuohong, Electrodynamics, Second Edition, Higher Education Press, 210-211.