The present invention relates to a structure, particularly to a structure of an emitter electrode for enhancing ion currents.
Gas field ions are generated by gas atoms and gas molecules ionized in an electrical field above a surface of an emitter electrode. The gas atoms and the gas molecules are originally of electrical neutrality. When the gas atoms and the gas molecules approach the emitter electrode in a pin shape, the gas atoms and gas molecules are attracted and polarized by the electrical field and captured because of the heat exchange principle. Ultimately, the gas atoms and the gas molecules are attracted to a pinpoint of the emitter electrode because of a potential energy well. After that, the gas atoms and the gas molecules attracted to the pinpoint of the emitter electrode ionize as the gas field ions in the electrical field are above the pinpoint. In other words, the larger the effective captured gas area is, the higher the ion currents are. Thereby, the structure of the emitter electrode will affect cumulation of the gas field ions.
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Thereby, since to increase the ion currents relates to the structure of the emitter electrode, how to design the structure of the emitter electrode to enhance the ion current is an urgent subject to tackle.
For the problems mentioned above, the present invention discloses a structure of the emitter electrode for enhancing ion currents, including a tip end part and a shank part. The tip end part is formed at a front end of the structure of the emitter electrode and has a pinpoint, a first diameter, and a radius of curvature. The shank part is formed in the rear of the tip end part at the front end of the structure of the emitter electrode. A length of the tip end part with the shank part is from the pinpoint to a first position of the shank part and a distance between the first position and the pinpoint is 300 times the first diameter. The radius of curvature of the tip end part ranges from 50 nanometers to 5 micrometers. The first diameter is 2 times the radius of curvature. Thereby, the ion currents generated by the structure of the emitter electrode of the present invention can be enhanced.
As mentioned above, the structure of the emitter electrode of the present invention has the features including a large radius of curvature of the tip end part, and a long length and a flat angle of the shank part. Thereby, the ion currents can be significantly increased from the scale of pico-amperes to the scale of nano-amperes.
Referring to
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As mentioned above, the ion currents generated by the structure of the emitter electrode 2 relates to the angle θ. That is, the smaller the angle θ is, the higher the ion currents are. The angle θ corresponds to the diameter of the shank part 22. In fact, the method for manufacturing the structure of the emitter electrode 2 cannot extend the length of the shank part 22 without any limits to generate a uniform diameter of the shank part 22 to form a smaller angle θ. In other words, during the manufacturing process, the diameter of the shank part 22 corresponding to different length intervals is not constant. That is, the diameter of the shank part 22 at different length intervals is not uniform. However,
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Referring to Table 1 below, Table 1 shows the simulation and experiment result for the structure of the emitter electrode at different angles of the shank part. As mentioned above, the structure of the emitter electrode for enhancing ion currents 2 of the present invention has three features, including large radius of curvature R of the tip end part 21, and long length and flat angle of the shank part 22. The result proves that the smaller the angle of the shank part 22 of the emitter electrode 2 is, the larger the effective captured gas area is and the higher the ion currents are, wherein the tolerance with the radius of curvature R of the tip end part 21 can be ignored. Furthermore, according to the result, it shows that the ion currents generated by utilizing the structure of the emitter electrode of the present invention increases approximately 5 times.
In summary, the structure of the emitter electrode for enhancing ion currents of the present invention has the features including large radius of curvature of the tip end part, long length of the shank part and flat angle of the shank part. Thereby, the ion current can be significantly increased from the scale of pico-amperes to the scale of the nano-amperes.
Even though numerous characteristics and advantages of the present invention have been set forth in the foregoing description, together with details of the structure and function of the invention, the disclosure is illustrative only. Changes may be made in detail, especially in matters of shape, size, and arrangement of parts within the principles of the invention to the full extent indicated by the broad general meaning of the terms in which the appended claims are expressed.
Number | Date | Country | |
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63069813 | Aug 2020 | US |