LIGHT-CONTROLLED SUPERCONDUCTOR

Abstract

A light-controlled superconductor uses electrons as carriers, which includes a light source and a sealed tube, wherein the sealed tube is made of glass or plastic. The sealed tube is filled with electron gas, and the light source produces incident light, and under the irradiation of the incident light, electrons will be forced to vibrate and behave similarly to vibrating electric dipoles, and emit secondary electromagnetic waves, so that the average distance between the electrons in the sealed tube is much smaller than the wavelength of the incident light, causing the vibrating electrons to be in a near-field of each other. When the electric field intensity direction of the incident light and the electric moments of two vibrating electrons are in the same radial straight line and are in the same direction, there exists an attractive force among the vibrating electrons.

Claims

1. A light-controlled superconductor, characterized in that the light-controlled superconductor uses electrons as carriers, which comprises a light source and a sealed tube, wherein the sealed tube is made of glass or plastic and is filled with electron gas; the average distance between electrons in the sealed tube is much smaller than the wavelength of incident light, and an electron number density is much greater than the negative third power of the wavelength of the incident light, so that vibrating electrons are in a near-field of each other; the light source produces the incident light, and the electrons are irradiated with the incident light, so that an attractive force is produced between 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 thermal motions of the electrons decreases to nearly zero, and the resistance of the electron gas is zero, and the electron gas transitions from a normal state to a superconducting state to realize superconductivity; the electron number density is controlled by controlling the frequency of the incident light, thereby controlling a superconducting current density; it is also possible to use nucleons or other charged particles as carriers for the light-controlled superconductor.

2. The light-controlled superconductor according to claim 1, characterized in that the sealed tube is evacuated first to remove impurities in the sealed tube, so that a pressure intensity in the sealed tube is less than 1 P.sub.a, and then the electron gas is injected; and when the electron gas is injected, the electron gas is first irradiated with a low-frequency electromagnetic wave, the electron gas is then irradiated with a high-frequency electromagnetic wave, so that the attractive force among the vibrating electrons becomes greater, and the average distance between the electrons in the sealed tube becomes smaller; the sealed tube is made of glass or plastic, and the sealed tube is wrapped with a heat insulation material outside.

Description

DETAILED DESCRIPTION OF EMBODIMENTS

[0055] A specific embodiment is described below, but specific implementations are not limited to this example.

[0056] If there is air in a sealed tube, the thermal kinetic energy of molecules in the air will affect the transition of an electron gas from a normal state to a superconducting state, therefore, the sealed tube needs to be evacuated first, so that the pressure in the sealed tube is lower than 1 P.sub.a. After the evacuation, the electron gas is injected, and in order to allow the vibrating electrons to be in a near-field of each other, the average distance between electrons in the sealed tube should be much smaller than the wavelength of incident light, r<<. Because there is the following relationship between the average distance r between electrons and a particle number density n.sub.d:

[00027]$\begin{array}{cc}r{n}_d^{-\frac{1}{3}}& \left(31\right)\end{array}$

[0057] Therefore, there is the following relationship between the particle number density n.sub.d and the wavelength of the incident light:

[00028]$\begin{array}{cc}{n}_d>>{}^{-\frac{1}{3}}& \left(60\right)\end{array}$

[0058] That is, the third power of the particle number density is much greater than the wavelength of the incident light. A required particle number density can be known from the wavelength of the incident light.

[0059] 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.

[0060] The sealed tube is made of glass or plastic, and the sealed tube is wrapped with a heat insulation material outside to prevent the electron gas from absorbing heat to change from the superconducting state to the normal state.

[0061] When the electron gas is injected, the electron gas is first irradiated with a low-frequency electromagnetic wave, and the electron gas is then irradiated with a high-frequency electromagnetic wave, so that the attractive force among vibrating electrons becomes greater, and the average distance between the electrons in the sealed tube becomes smaller.

[0062] From formulas (2) and (16), it can be seen that the attractive force F.sub.N between the vibrating electrons increases with the increase of A and and increases with the decrease of the distance r, and A increases with the increase of Q and A increases with the decrease of R. Therefore, controlling the charge amount Q and amplitude a of an accelerating charge that produces the incident light and the distance R can control the radial attractive force among the vibrating electrons, thereby controlling the average kinetic energy of the thermal motions of the electrons to realize superconductivity.

[0063] At the same time, it can be known according to formula (54) that the electron number density is controlled by controlling the frequency of the incident light, thereby controlling a superconducting current density. This light-controlled superconductor may also use nucleons or other charged particles as carriers.

REFERENCE DOCUMENTS

[0064] 1, [0065] BingXin Gong, 2013, The light controlled fusion, Annals of Nuclear Energy, 62 (2013), 57-60.