This is a U.S. National Stage under 35 U.S.C 371 of the International Application PCT/CN2018/075293, filed Feb. 5, 2018, which claims priority under 35 U.S.C. 119(a-d) to CN 201710244250.3, filed Apr. 14, 2017.
The present invention relates to the field of chemical vapor deposition technology. In particular, a microwave resonant cavity and a corresponding reactor relate to the field of plasma chemical vapor deposition technology
Using microwave energy to generate plasma, materials such as diamond and graphene can be fulfilled by microwave plasma chemical vapor deposition (CVD) method. Since the plasma is generated in an electrodeless discharge process, it is relatively pure. When materials are prepared by hot filament CVD method or direct current arc plasma jet CVD method, they are often contaminated by the evaporation of the hot metal filament or the tungsten electrode. Compared with the radiofrequency CVD method, the microwave plasma CVD method has a relatively concentrated discharge region, a higher energy density, and a faster deposition rate. Therefore, this method has received extensive attention and has been widely used in the fields of research and preparation of high-quality diamond materials.
The resonant cavity is the main component of the microwave plasma CVD reactor. However, two tricky problems still remain. On one hand, the cavity structure of the microwave plasma CVD reactor often has a low focusing ability. Therefore, improving the focusing ability to form a strongly focused electric field and generate high-density plasma is preferred to develop new resonant cavity structures. On the other hand, the resonant cavity is less flexible. It should be combined with a specific coupling mechanism and a dielectric window in a microwave plasma CVD reactor. For example, an ellipsoidal resonant cavity needs to be equipped with a coaxial probe antenna as a coupling mechanism and a quartz bell jar as a dielectric window; a cylindrical resonant cavity is generally equipped with a coaxial probe antenna as a coupling mechanism and a quartz plate as a dielectric window; a butterfly resonant cavity needs to be equipped with a coaxial circumferential antenna as a coupling mechanism and a quartz ring as a dielectric window.
In order to overcome the two problems mentioned above, the present invention proposes a novel resonant cavity by utilizing the principle of reflection and interference of electromagnetic waves. The novel resonant cavity has a strong electric field focusing ability and can match different coupling mechanisms and dielectric windows to build microwave plasma CVD reactors.
The present invention provides a plasma chemical vapor deposition reactor with a microwave resonant cavity for the purposes of improving the focusing ability and configuration flexibility.
Based on the above purposes, a rotary body is adopted for the microwave resonant cavity, which is formed by two isosceles triangles intersecting at the vertex angles with a Boolean union operation. Inside the rotary body, there are an upper cavity and a lower cavity. The base angles of the two triangles are 50°˜75°. Between 2nλ˜(2n+0.5) λ, the base lengths of the two triangles are equal or have an nλ difference, where n is an integer, λ is the microwave wavelength. The distance between the centroids of the upper and the lower isosceles triangles is 0˜4/5λ.
Further, an upper cylindrical cavity is provided in the middle part of the rotary body, and a lower cylindrical cavity is provided at the bottom of the lower cavity.
The plasma chemical vapor deposition reactor comprises a microwave coupling mechanism, a dielectric window, a substrate holder, a tuning mechanism, air inlet and outlet holes, and the microwave resonant cavity described above.
Further, in the plasma chemical vapor deposition reactor, the bases of the two isosceles triangles forming the microwave resonant cavity are equal in length. The top of the upper cavity is provided with a coaxial probe coupling antenna. A frequency tuning plate is set at the bottom of the lower cavity, and a microwave shielding elastic piece is placed between the frequency tuning plate and the lower cavity wall. The foot of the quartz bell jar dielectric window is placed on the frequency tuning plate and well-sealed. The top contour of the quartz bell jar dielectric window is higher than the interface of the upper and lower cavities. The substrate holder is set in the middle of the frequency tuning plate. An air inlet and two air outlets on both sides of the substrate holder are given in the frequency tuning plate.
Further, in the plasma chemical vapor deposition reactor, the base of the isosceles triangle forming the upper cavity is longer than that of the isosceles triangle forming the lower cavity. The upper cavity is provided with a coaxial circumferential coupling antenna on the top. The inner side of the top of the upper cavity is provided with a well-sealed quartz ring dielectric window which matches with the coaxial circumferential coupling antenna. In the center of the coaxial circumferential coupling antenna is an air inlet running through the microwave resonant cavity. At the bottom of the lower cavity, a frequency tuning plate is set. Between the frequency tuning plate and the lower cavity wall, a microwave shielding elastic piece is placed. The substrate holder is set in the middle of the frequency tuning plate. Two air outlets on both sides of the substrate holder are given in the frequency tuning plate, and a total air outlet is given at the bottom of the lower cavity.
Further, in the plasma chemical vapor deposition reactor, the base of the isosceles triangle forming the upper cavity is shorter than that of the isosceles triangle forming the lower cavity. The upper cavity is provided with a coaxial probe coupling antenna. A quartz plate dielectric window is horizontally set in the middle of the upper cavity and stuck onto the upper cavity wall. An air inlet is given at the upper cavity wall below the quartz plate dielectric window. A frequency tuning plate is set at the bottom of the lower cavity. Between the frequency tuning plate and the lower cavity wall, a microwave shielding elastic piece is placed. A substrate holder is set in the middle of the frequency tuning plate. On both sides of the substrate holder, two air outlets are given. Besides, a total air outlet at the bottom of the lower cavity is given.
Further, in a structure comprising an upper cylindrical cavity and a lower cylindrical cavity, the plasma chemical vapor deposition reactor is provided, which comprises a microwave coupling mechanism, a dielectric window, a substrate holder, a tuning mechanism, air inlet and outlet holes, and the microwave resonant cavity according to claim 2. The top of the upper cavity is provided with a coaxial circumferential coupling antenna. The inner side of the top of the upper cavity is provided with a well-sealed quartz ring dielectric window which matches with the coaxial circumferential coupling antenna. In the center of the antenna is an air inlet running through the microwave resonant cavity. A central first frequency tuning plate is set in the middle of the lower cylindrical cavity, and a substrate holder is set in the middle of the first frequency tuning plate. A second frequency tuning plate perpendicular to the first frequency tuning plate is set around the substrate holder. Two air outlets are given in the second frequency tuning plate on both sides of the substrate holder, and a total air outlet is given at the bottom of the cavity.
When microwaves are coupled into the microwave resonant cavity from the upper part of the reactor, it is hoped that a highly intensive and uniformly distributed focused electric field can be formed at the bottom center of the resonant cavity. Based on the principle of reflection and interference of electromagnetic waves, the strongly focused electric field in this invention is formed by adjusting the base lengths, the base angles and the centroid distance. According to specific applications, different dielectric windows, microwave coupling modes and reaction gas inlet and outlet modes can be selected in the resonant cavity. With simple structures, the resonant cavity is convenient and flexible.
The foregoing conceptions and their accompanying advantages of this invention will become more readily appreciated after being better understood by referring to the following detailed description, in conjunction with the accompanying drawings, wherein:
In the drawings, the following reference numbers are used: 1—Upper cavity; 2—Lower cavity; 3—Upper cylindrical cavity; 4—Lower cylindrical cavity; 5—Coaxial probe coupling antenna; 6—Frequency tuning plate; 7—Quartz bell jar dielectric window; 8—Substrate holder; 9—Air inlet; 10—Air outlet; 11—Coaxial circumferential coupling antenna; 12—Quartz ring dielectric window; 13—Quartz plate dielectric window; 14—Total outlet; 15—Lifting mechanism of substrate holder; 16—Lifting mechanism of frequency tuning plate; 61—First frequency tuning plate; 62—Second frequency tuning plate; 161—Lifting mechanism of first frequency tuning plate; 162—Lifting mechanism of second frequency tuning plate.
In a typical embodiment of the present invention, a plasma chemical vapor deposition microwave resonant cavity is a rotary body formed by two isosceles triangles intersecting at the vertex angles with a Boolean union operation, as shown in
The simulated electric field contours of the microwave resonant cavity according to typical embodiments of the present invention are shown in
In a preferred embodiment (see the following embodiment 4), the central part of the rotary body is an upper cylindrical cavity (3), and the bottom part of the lower cavity (2) is a lower cylindrical cavity (4).
A plasma chemical vapor deposition reactor can be constructed by combining the microwave resonant cavity mentioned above with a microwave coupling mechanism, a dielectric window (7), a substrate holder (8), a tuning mechanism, and air inlet hole (9) and outlet holes (10).
The structure and technical effects of the plasma chemical vapor deposition reactor with a microwave resonant cavity according to the present invention will be further described through the following specific embodiments.
It should be noted that there are two common industrial microwave frequencies in the technical field, namely 2.45 GHz and 915 MHz. Corresponding to the two microwave frequencies, the wavelengths are λ1=122.4 mm and λ2=327.9 mm, respectively. In the specific embodiments, the microwave wavelength λ=122.4 mm (the wavelength allowable deviation is ±10 mm) is adopted. For the microwave resonant cavity, the base lengths of the isosceles triangles are 2nλ (2n+0.5) λ, where n is 1 and λ is 122.4 mm, that is, the base lengths are 244.8˜306 mm. The base lengths of the two isosceles triangles are equal or have a difference of λ, that is, the base lengths of the two isosceles triangles are equal or have a difference of 122.4 mm (the allowable deviation is ±10 mm). The centroid distance of the upper and the lower isosceles triangles is 0˜4/5λ, that is, 0˜97.92 mm.
This embodiment refers to
In the specific implementation, the base lengths of the two isosceles triangles are equal, which are 245±5 mm; the centroid of the upper isosceles triangle coincides with that of the lower isosceles triangle, that is, the centroid distance of the two triangles is 0; the base angles of the two isosceles triangles are both 50°.
This embodiment refers to
In the specific implementation, the base length and the base angle of the upper isosceles triangle are 735±5 mm and 55° respectively; for the lower isosceles triangle, they are 490±5 mm and 60° respectively; the centroid distance of the two isosceles triangles is 55±5 mm.
This embodiment refers to
In the specific implementation, the base length and the base angle of the upper isosceles triangle are 790±5 mm and 75°, respectively; for the lower isosceles triangle, they are 1035±5 mm and 55°, respectively; the centroid distance of the two isosceles triangles is 95±5 mm.
This embodiment refers to
In the specific implementation, the base length and the base angle of the upper isosceles triangle are 1244±5 mm and 65° respectively; for the lower isosceles triangle, they are 1000±5 mm and 55° respectively; the diameter and the height of the upper cylindrical cavity (3) are 1110±5 mm and 290±5 mm respectively; for the lower cylindrical cavity (4), they are 850±5 mm and 165±5 mm respectively; the centroid distance of the two isosceles triangles is 35±5 mm.
Number | Date | Country | Kind |
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201710244250.3 | Apr 2017 | CN | national |
Filing Document | Filing Date | Country | Kind |
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PCT/CN2018/075293 | 2/5/2018 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
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WO2018/188406 | 10/18/2018 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
5418430 | Bayliss | May 1995 | A |
6132550 | Shiomi | Oct 2000 | A |
6622650 | Ishii | Sep 2003 | B2 |
6863773 | Emmerich | Mar 2005 | B1 |
20040134431 | Sohn | Jul 2004 | A1 |
20130125817 | van Stralen | May 2013 | A1 |
20140230729 | Brandon | Aug 2014 | A1 |
20170032986 | Engelhardt | Feb 2017 | A1 |
Number | Date | Country | |
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20200105504 A1 | Apr 2020 | US |