Structure of emitter electrode for enhancing ion currents
11309159 · 2022-04-19
Assignee
Inventors
- Wei-Chaio Lai (Citong Township, TW)
- Chun-Yueh Lin (Keelung, TW)
- Ing-Shouh Hwang (New Taipei, TW)
- Wei-Tse Chang (Taoyuan, TW)
- Ching-Yu Hsiao (Taoyuan, TW)
- Yu-Fong Yu (New Taipei, TW)
- Zong-Yu Yang (Jinning Township, TW)
Cpc classification
International classification
Abstract
The present invention discloses a structure of an emitter electrode for enhancing ion currents, including a tip end part and a shank part. The tip end part has a pinpoint, a first diameter, and a radius of curvature. 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.
Claims
1. A structure of an emitter electrode for enhancing ion currents, comprising: a tip end part, formed at a front end of the structure of the emitter electrode, having a pinpoint, a first diameter, and a radius of curvature; and a shank part, formed in a rear of the tip end part at the front end of the structure of the emitter electrode; wherein 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 first distance between the first position and the pinpoint is 300 times of the first diameter; wherein the radius of curvature of the tip end part ranges from 50 nanometers to 5 micrometers; wherein the first diameter is 2 times of the radius of curvature.
2. The structure as claimed in claim 1, wherein there is at least one first node position between a second position and a third position of the shank part and a second diameter corresponding to the at least one first node position is less than 1.2 times of the first diameter; wherein a second distance between the pinpoint and the second position is 3 times of the first diameter and a third distance between the pinpoint and the third position is 60 times of the first diameter.
3. The structure as claimed in claim 2, wherein a third diameter of the shank part between the pinpoint and the second position is less than 1.2 times of the first diameter.
4. The structure as claimed in claim 1, wherein there is at least one second node position between a fourth position and the first position of the shank part and a fourth diameter corresponding to the at least one second node position is less than 2 times of the first diameter; wherein a fourth distance between the pinpoint and the fourth position is 18 times of the first diameter.
5. The structure as claimed in claim 4, wherein a fifth diameter of the shank part between the pinpoint and the fourth position is less than 2 times of the first diameter.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
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DETAILED DESCRIPTION OF THE INVENTION
(11) Referring to
(12) Referring to
(13) Referring to
(14) 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,
(15) Referring to
(16) Referring to
(17) 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.
(18) TABLE-US-00001 TABLE 1 angle ion effective radius of the current captured refrigerator of shank @1e.sup.−4 gas temperature curvature part ion torr area (k) (nm) (°) source (pA) (μm.sup.2) (a) 25 90.55 ~16 He 10.6 2.3334 (b) 29 82.35 ~0 He 53.3 12.3763
(19) 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.
(20) 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.