Source: https://patents.google.com/patent/JP5807854B2/en
Timestamp: 2020-01-27 04:18:21
Document Index: 81869917

Matched Legal Cases: ['art 23', 'art 22', 'art 22', 'art 23', 'arts 22', 'art 21', 'arts 22', 'art 53', 'art 51', 'art 52', 'art 52', 'art 51', 'art 52', 'art 53']

JP5807854B2 - plasma generator - Google Patents
plasma generator Download PDF
JP5807854B2
JP5807854B2 JP2010267354A JP2010267354A JP5807854B2 JP 5807854 B2 JP5807854 B2 JP 5807854B2 JP 2010267354 A JP2010267354 A JP 2010267354A JP 2010267354 A JP2010267354 A JP 2010267354A JP 5807854 B2 JP5807854 B2 JP 5807854B2
JP2010267354A
JP2012119145A (en
洋通 豊田
信福 野村
2010-11-30 Application filed by 国立大学法人愛媛大学 filed Critical 国立大学法人愛媛大学
2010-11-30 Priority to JP2010267354A priority Critical patent/JP5807854B2/en
2012-06-21 Publication of JP2012119145A publication Critical patent/JP2012119145A/en
2015-11-10 Publication of JP5807854B2 publication Critical patent/JP5807854B2/en
The present invention relates to a plasma antenna electrode that receives microwaves and generates plasma, and a plasma generation apparatus including the same.
Currently, as a method for generating plasma, there is known a method of generating plasma by irradiating an antenna electrode made of a conductor with microwaves and generating a standing wave on the antenna electrode. For example, Japanese Unexamined Patent Application Publication No. 2006-179221 (Patent Document 1) describes a plurality of rod-shaped antenna electrodes. A technique for generating plasma is used in various fields such as a vapor deposition technique in the semiconductor field.
Japanese Patent Laid-Open No. 2006-179211
However, the plasma generated from the conventional rod-shaped antenna electrode is not so large, and it has been necessary to arrange a large amount of antenna electrode in order to apply it to the vapor deposition technique. In addition, when the plasma is small, it is difficult to apply the plasma to other fields (for example, an atmospheric pressure plasma apparatus).
The present invention has been made in view of such circumstances, and an object of the present invention is to provide a plasma antenna electrode capable of generating a plasma larger than a rod-shaped antenna electrode and a plasma generation apparatus including the same. .
The plasma antenna electrode of the present invention is a plasma antenna electrode that receives microwaves to generate plasma, a main receiving unit that receives microwaves, a first electrode unit that extends from one end of the main receiving unit, And a second electrode portion extending from the other end of the main receiving portion and having a distal end spaced apart and close to the tip of the first electrode portion, and the main receiving portion of the conductor mainly receives the microwave. Thus, a standing wave is generated.
According to this configuration, when the conductor (mainly the main receiving unit) receives (captures) the microwave, a standing wave is generated in the conductor. And since the front-end | tip of a 1st electrode part and the front-end | tip of a 2nd electrode part are spaced apart and close, the electric field (vibration resonance electric field of a plasma and an electrode) resonates between each other, and it is larger than a rod shape between the said front-end | tips. Plasma is generated. That is, according to the present invention, plasma larger than that of the rod-shaped antenna electrode can be generated.
Here, it is preferable that the first electrode portion and the second electrode portion have sharp tips. According to this configuration, plasma can be generated more reliably.
The main receiver is preferably linear. Microwaves can be easily received at a straight line portion extending in the propagation direction, and the microwave can be received more reliably by adopting this configuration. Further, the conductor may be C-shaped (annular), and in this case, creation is easy.
Here, the length of the conductor (that is, the plasma antenna electrode) preferably satisfies (λ / 2) × n (n: positive odd number), where λ is the wavelength of the received microwave. Note that satisfying (λ / 2) × n (n: positive odd number) means that an error of about ± 5 mm and peripheral values are included.
According to this configuration, the polarity of the tip of the first electrode portion and the polarity of the tip of the second electrode portion can be reliably reversed by a standing wave generated in the conductor. That is, when the tip of the first electrode portion is positive, the tip of the second electrode portion is negative. When the tip of the first electrode portion is negative, the tip of the second electrode portion is positive. Thereby, a larger plasma is generated between the electrode tips.
Here, the antenna electrode for plasma of the present invention may include a plurality of the conductors, and the plurality of conductors may be arranged such that the main receiving portions intersect each other. Thereby, the plasma antenna electrode can generate a large plasma regardless of the propagation direction of the received microwave. In this configuration, it is preferable that all the tips are spaced apart from each other and close to each other. By arranging the spaces between the tips to overlap, the electric field between them is strengthened, and a larger plasma can be generated.
Here, the plasma generation apparatus of the present invention includes a microwave irradiation apparatus that irradiates a microwave and the above-described plasma antenna electrode, and the plasma antenna electrode receives a microwave and generates a standing wave. Features. In this plasma generator, a larger plasma can be generated.
In the plasma generator of the present invention, it is preferable that the main receiver has a linear shape, and the microwave irradiator irradiates microwaves parallel to the main receiver with respect to the plasma antenna electrode. As a result, the plasma antenna electrode efficiently receives the microwave and generates a large plasma.
Further, the plasma antenna electrode may be formed on the same plane, and the microwave irradiation apparatus may be configured to irradiate the plasma antenna electrode with the microwave parallel to the plane. Also by this, the plasma antenna electrode efficiently receives the microwave, and a large plasma is generated.
The present invention can also be configured as follows. That is, the present invention is a plasma antenna electrode that receives microwaves and generates plasma, and includes a plate-shaped main receiving unit that receives microwaves, and a first electrode unit that extends upward from the surface of the main receiving unit. A conductor having a second electrode portion extending upward from the surface of the main receiving portion and having a tip spaced apart and close to the tip of the first electrode portion; and a first electrode portion provided on the surface of the main receiving portion. And a non-conductive covering member that covers the second electrode portion so that only the tip is exposed, and the main receiving portion of the conductor mainly receives the microwave and generates a standing wave. . According to this configuration, large plasma can be generated between the tips of the first electrode portion and the second electrode portion even in the conductive liquid.
According to the present invention, a large plasma can be generated from one antenna electrode.
It is a schematic cross section which shows the structure of the plasma generator 1 of 1st embodiment. It is a model front view which shows the antenna electrode 2 for plasmas of 1st embodiment. It is a schematic plan view which shows the antenna electrode for plasma 2 of 1st embodiment. 4 is a schematic diagram showing a configuration of Experimental Example 1. FIG. It is a figure which shows the result of Experimental example 2. It is a model front view which shows the antenna electrode 2 for plasma in angle (theta) 0 degree. It is a model front view which shows the antenna electrode 2 for plasma of a deformation | transformation aspect. It is a model front view which shows the antenna electrode 2 for plasma of a deformation | transformation aspect. It is a model perspective view which shows the antenna electrode 20 for plasma of a deformation | transformation aspect. 10 is a schematic diagram showing a configuration of Experimental Example 6. FIG. 10 is a schematic diagram showing a configuration of Experimental Example 6. FIG. It is a model front view which shows the antenna electrode 5 for plasma of 2nd embodiment.
Next, the present invention will be described in more detail with reference to embodiments.
A first embodiment will be described with reference to FIGS. In addition, about drawing, it represents typically so that a structure can be grasped | ascertained, and the dimension is expanded and reduced partially.
As shown in FIG. 1, the plasma generator 1 includes a plasma antenna electrode 2, an outer container 3, and a microwave irradiation device 4.
As shown in FIGS. 2 and 3, the plasma antenna electrode 2 is made of an elongated plate-like conductor (here, tungsten), and is formed in a rice ball shape (triangular corners are round) as a whole. The total length of the plasma antenna electrode 2 is approximately ½ (approximately 61 mm) of the wavelength λ of the microwave to be received (here, frequency 2.45 GHz). The plasma antenna electrode 2 has a width d of about 3 mm and a thickness t of about 0.5 mm. The wavelength λ of the propagating microwave is obtained by λ = (c / f) × ε r −1/2 (c: speed of light, f: frequency, ε r : relative dielectric constant).
The plasma antenna electrode 2 includes a main receiving unit 21, a first electrode unit 22, and a second electrode unit 23. The main receiver 21 has a linear shape and is a part that mainly receives microwaves in the plasma antenna electrode 2.
The first electrode unit 22 extends from one end of the main receiver 21 in a direction intersecting the main receiver 21. In other words, the first electrode portion 22 extends from one end of the main receiving portion 21 such that the direction from the end of the first electrode portion 22 toward the tip is different from the extending direction of the main receiving portion 21. Specifically, the angle formed by the first electrode portion 22 and the main receiving portion 21 (the same angle as θ described above) is an acute angle (here, approximately 40 to 45 degrees). The tip of the first electrode portion 22 has a sharp shape.
The second electrode portion 23 extends from one end of the main receiving portion 21 in a direction intersecting the main receiving portion 21 so that the tip approaches the tip of the first electrode portion 22. In other words, the second electrode portion 23 extends from the other end of the main receiving portion 21 such that the direction from the end of the second electrode portion 23 toward the tip is different from the extending direction of the portion 21. The angle formed between the second electrode portion 23 and the main receiving portion 21 is the same as the angle formed between the first electrode portion 22 and the main receiving portion 21. The length of the 2nd electrode part 23 is the same as the length of the 1st electrode part 22, and it can be said that it is a substantially isosceles triangle as a whole. The tip of the second electrode portion 23 has a sharp shape. In the present embodiment, the separation distance between the tips of the electrodes 22 and 23 (distance between tips) is set to approximately 3 mm.
The main receiving unit 21, the first electrode unit 22, and the second electrode unit 23 are formed so as to be located on substantially the same plane. In the present embodiment, the angle formed between the first electrode part 22 and the main receiver 21 and the angle formed between the second electrode part 23 and the main receiver 21 may be slightly different. Further, the length of the first electrode portion 22 and the length of the second electrode portion 23 may be slightly different. Further, the sharp shape may be a shape in which the thickness t (plate thickness) is constant and the width d becomes thinner toward the tip.
The outer container 3 is a housing having an internal space, and accommodates the plasma antenna electrode 2 and the microwave irradiation device 4 therein. The outer container 3 has a pipe 31 communicating with the inside. An inert gas supply device (not shown) is provided outside the outer container 3, and an inert gas such as nitrogen or argon is supplied into the outer container 3 through the pipe 31. Here, a pedestal 32 is provided in the outer container 3, and the plasma antenna electrode 2 is disposed on the pedestal 32.
The microwave irradiation device 4 is a device that irradiates microwaves, and here, a magnetron is used. The microwave irradiation device 4 is disposed in the outer container 3 and irradiates microwaves having a frequency of 2.45 GHz.
A plasma generation experiment was performed using the plasma generator 1. As shown in FIG. 4, a microwave oven A (power 750 W) was used as the outer container 3 and the microwave irradiation device 4. That is, the casing of the microwave oven A is the outer container 3, and the magnetron (frequency 2.45 GHz) in the microwave oven is the microwave irradiation device 4. In addition, the turntable in the microwave oven is in a removed state (that is, a state in which it does not rotate).
First, the beaker B is prepared, and the plasma antenna electrode 2 is placed in the beaker B so that the main receiving unit 21 is in contact with the bottom surface of the beaker B and the tips of the electrode units 22 and 23 are located above the main receiving unit 21. installed. Thereafter, argon gas was injected into the beaker B, and the beaker B was sealed. Subsequently, the beaker B was placed in the microwave oven A.
Here, the beaker B was arranged so that the main receiving portion 21 of the plasma antenna electrode 2 was parallel to the microwave irradiation direction (propagation direction). Since the magnetron which is the microwave irradiation device 4 is arranged on the right side surface (see FIG. 1) in the microwave oven A, the microwave irradiation direction is a direction from the right side surface in the microwave oven A toward the left side surface. . That is, the beaker B is disposed so that the extending direction of the main receiving unit 21 is the left-right direction when viewed from the front of the microwave oven A. In this arrangement, the plasma antenna electrode 2 (the main receiving unit 21, the first electrode unit 22, and the second electrode unit 23) formed on one virtual plane is microscopic from a direction parallel to the virtual plane. Waves will be irradiated.
Here, the start button of the microwave oven A was pushed, and the microwave was irradiated from the magnetron. Thereafter, plasma was generated between the tip of the first electrode portion 22 and the tip of the second electrode portion 23. Plasma was generated approximately 100 mm upward from between the tips of the electrode portions 22 and 23. In the rod-shaped antenna electrode fixed upright on a conventional pedestal, plasma was generated only about 5 mm from the tip of the antenna electrode under the same conditions.
Thus, according to the plasma antenna electrode 2 of the present embodiment, larger plasma can be generated. According to the present embodiment, a portion where the potential is 0 is generated in the central portion of the main receiving unit 21, and the tip of each electrode unit 22, 23 is plus and minus above the portion, so A large plasma is generated toward In the present embodiment, since the entire length of the plasma antenna electrode 2 is ½ of the microwave wavelength λ, a standing wave can be generated more reliably in the electrode. At the tips of the first electrode portion 22 and the second electrode portion 23, plus and minus are alternately switched, a strong electric field is generated between the tips, and a large plasma is generated. Each of the electrode portions 22 and 23 also receives microwaves to some extent.
Here, in Experimental Example 1, the material of the plasma antenna electrode 2 was copper, and the distance between the tips of the electrodes 22 and 23 was changed. According to this, as shown in FIG. 5, strong plasma was generated particularly in the range of about 0.2 mm to 10 mm as shown in FIG. In FIG. 5, ◯ represents that plasma of approximately 10 mm or more was generated, Δ represents that it was difficult to generate plasma, and × represents that plasma was not generated. When the distance between the tips was 0, no plasma was generated. When the distance between the tips was less than 0.2 mm, the experiment could not be performed because the electrode could not be manufactured by design. However, if the distance was not 0, it can be predicted that a strong electric field is generated between the tips and strong plasma is generated. In this way, the distance between the tips of the plasma antenna electrode 2 is not limited to 0 and may be close.
Further, as shown in FIG. 2, the distance between the tips was fixed to 3 mm, and the angle θ formed by the tips of the electrode portions 22 and 23 with respect to the installation surface was changed. Regarding the angle θ, the one in which only the tips of the electrode portions 22 and 23 are bent is excluded. That is, except that θ is 0 degree, the angles are formed by the electrode portions 22 and 23 and the main receiving portion 21, and the electrode portions 22 and 23 are not bent. When θ is 0 degree, as shown in FIG. 6, the electrode parts 22 and 23 are bent from the end of the main receiving part 21 at half or less of the entire length of the electrode parts 22 and 23, and the angle θ is set to 0 degree. According to this, when the angle θ is small (for example, approximately 60 degrees or less, specifically, 20 degrees, 30 degrees, 40 degrees, 60 degrees), strong plasma is easily generated. Plasma was hardly generated at 80 degrees and 90 degrees. This is presumably because the length of the main receiver 21 increases as the angle θ decreases, and microwaves can be received more reliably under the condition that the total length of the plasma antenna electrode 2 is constant.
Moreover, it experimented by changing the full length of the antenna electrode 2 for plasma around 61 mm. As a result, strong plasma was generated at about 56 mm to 66 mm. In other words, it was found that the overall length of the plasma antenna electrode 2 is preferably λ / 2 and its periphery. Note that plasma is generated at approximately 55 mm and 54 mm, and the preferable overall length can be said to be approximately 0.9 × (λ / 2) or more and 1.1 × (λ / 2) or less.
Theoretically, the total length of the plasma antenna electrode 2 that easily generates a strong electric field is an odd multiple (positive integer) of λ / 2 (including peripheral values). By setting an odd multiple of λ / 2, the tips of the electrode portions 22 and 23 are likely to have opposite polarities when a standing wave is generated. When the tips have opposite polarities, the electric field between the tips becomes strong, and a strong plasma is likely to be generated.
In Experimental Example 1, the experiment was performed by changing the arrangement position of the plasma antenna electrode 2 with respect to the microwave propagation direction. According to this, the strongest plasma was generated when the main receiver 21 was parallel to the propagation direction of the microwave (that is, Experimental Example 1). Next, when the main receiver 21 was tilted 45 degrees with respect to the propagation direction of the microwave, although strong plasma was generated, it was smaller than the parallel case. Next, when the main receiver 21 was tilted 90 degrees with respect to the propagation direction of the microwave (that is, when it was orthogonal), no plasma was generated. That is, it is most preferable that the extending direction of the main receiver 21 and the propagation direction of the microwave are parallel.
<Deformation mode>
Here, the plasma antenna electrode 2 is not limited to the above shape. The plasma antenna electrode 2 only needs to be spaced apart and close to each other, for example, an annular shape (substantially C-shaped) as shown in FIG. 7, a rectangular shape as shown in FIG. 6, or as shown in FIG. Such a chestnut shape (for example, the main receiver 21 is linear and the electrode portions 22 and 23 are convex arcs: included in the C-shape) may be used. In the case of FIG. 7, for example, approximately half or more of the upper and lower heights can be referred to as electrode portions 22 and 23. In the case of FIG. 8 as well, in addition to the above, more than half of the height may be referred to as electrode portions 22 and 23. The plasma antenna electrode 2 is not limited to a plate shape, and may be formed using, for example, a rod-shaped material (conductor).
Further, as shown in FIG. 9, a plurality of plasma antenna electrodes 2 may be combined to form one plasma antenna electrode 20. The plasma antenna electrode 20 is formed by joining the central portions of two main receivers 21 so that the main receivers 21 are orthogonal to each other. The joining can be performed using, for example, welding or an adhesive. The four electrode portions 22 and 23 of the plasma antenna electrode 20 are separated from each other and close to each other.
According to this configuration, no matter which direction the plasma antenna electrode 20 is arranged, at least one of the two main receivers 21 is in a position not orthogonal to the microwave propagation direction. That is, strong plasma can be generated between the tips of the electrode portions 22 and 23 regardless of the arrangement direction of the plasma antenna electrode 20 with respect to the microwave propagation direction. Furthermore, since the tips overlap each other, a stronger electric field is generated and a stronger plasma is generated.
The microwave irradiation device 4 is not limited to a magnetron, and may be a microwave vacuum tube such as a klystron, or a semiconductor element such as a gun diode.
Further, the plasma generator 1 and the plasma antenna electrode 2 are not limited to gas phase plasma. For example, even when the plasma antenna electrode 2 is disposed in an organic solvent such as normal dodecane (n-dodecane), plasma can be easily generated according to this embodiment. That is, the plasma generator 1 and the plasma antenna electrode 2 are effective because they can generate plasma in liquid. In the present embodiment, in-liquid plasma is possible and effective as long as it is in a non-conductive liquid such as waste oil or silicon oil, as with an organic solvent. In the case of normal dodecane, since the relative dielectric constant ε r is 1.777, the wavelength λ of the propagating microwave is changed, and the total length of the plasma antenna electrode 2 is preferably λ / 2 (approximately 45.9 mm). .
Moreover, the plasma generator 1 of this embodiment can be utilized as an atmospheric pressure plasma CVD apparatus. Since the conventional atmospheric pressure plasma CVD apparatus uses a rod-shaped antenna electrode, there is a problem that plasma is small and hardly occurs. However, according to the present embodiment, stronger plasma can be easily generated, and for example, a thin film can be easily formed in a semiconductor process.
An example of an atmospheric pressure plasma CVD apparatus is a diamond synthesis apparatus. The diamond synthesizer can be configured, for example, by arranging a substrate (for example, a silicon wafer) above the plasma antenna electrode 2 in the plasma generator 1 of FIG. Then, the plasma antenna electrode 2 and the substrate are disposed in a container (beaker or the like), and a mixed gas of methane gas and hydrogen is injected, and the container is disposed in the outer container 3. When this is irradiated with microwaves, strong plasma is generated and diamond is deposited on the substrate. Thus, the plasma generator 1 of this embodiment is also suitable for an atmospheric pressure plasma CVD apparatus. The plasma antenna electrodes 2 and 20 are also suitable as antenna electrodes for an atmospheric pressure plasma CVD apparatus.
Here, a diamond synthesis experiment was conducted using the apparatus shown in FIG. The apparatus shown in FIG. 10 has the same configuration as the plasma generator 1 and uses a microwave oven A2. Four tubes 31 are inserted in the pipe above the microwave oven A2. The two tubes 31 are for supplying and exhausting nitrogen between the outside and the inside of the microwave oven A2, and the remaining two are for supplying and exhausting hydrogen and methane between the outside and the beaker B2. Is.
As shown in FIG. 11, the beaker B2 is provided with two through holes, and the tubes 31 are inserted one by one there. The beaker B <b> 2 was covered and sealed, and supply / exhaust with the outside was performed via the tube 31.
A chestnut-shaped plasma antenna electrode 2 and a substrate holder 33 are installed on a base 32 (made of Teflon (registered trademark)) in the beaker B2. The plasma antenna electrode 2 is installed so that the main receiver 21 is substantially parallel to the microwave irradiation direction. The substrate holder 33 holds the silicon substrate 34 above the plasma antenna electrode 2. The distance between the silicon substrate 34 and the tip of the plasma antenna electrode 2 was about 5 mm.
In this apparatus, the microwave oven A2 was started, and a mixed gas of hydrogen and methane (methane 1%) was flowed at 1000 cc / min into the beaker B2. The inside of the microwave oven A2 was filled with nitrogen gas. The temperature of the silicon substrate 34 was maintained at about 700 ° C. by adjusting the microwave output from the magnetron with a slider. Three minutes after the start of the experiment, a diamond (particle size 5 μm) film was formed on the silicon substrate 34.
The plasma antenna electrode 5 of the second embodiment will be described with reference to FIG. As shown in FIG. 12, the plasma antenna electrode 5 includes a main receiving portion 51, a first electrode portion 52, a second electrode portion 53, and a covering member 54.
The main receiver 51 is a flat conductor (for example, copper or tungsten) having a thickness of about 0.5 mm. The plan view of the main receiver 51 is substantially circular. The first electrode unit 52 is a long plate conductor (for example, copper or tungsten) extending in an arc shape upward from the surface of the main receiving unit 51. The second electrode part 53 is a long plate conductor (for example, copper or tungsten) extending in an arc shape upward from the surface of the main receiving part 51 and the end of the first electrode part 52. That is, each electrode part 52 and 53 is electrically connected (or contacted) to the main receiving part 51. The first and second electrode portions 52 and 53 are integrally formed and have a substantially C-shape as a whole. As in Experimental Example 4, the first and second electrode portions 52 and 53 preferably have a total length of λ / 2 (or an odd multiple of λ / 2) and its periphery.
The covering member 54 is made of a heat-resistant adhesive and has a substantially cylindrical shape on the surface of the main receiver 51. The covering member 54 covers the first and second electrode portions 52 and 53 except for the tips of the first and second electrode portions 52 and 53. That is, the first and second electrode portions 52 and 53 are covered with the covering member 54 and only the tips are exposed. In other words, the first electrode portion 52 includes a first exposed electrode portion (tip portion) and a first covered electrode portion, and the second electrode portion 53 includes a second exposed electrode portion (tip portion) and a second covered electrode. It consists of parts.
Also in the plasma antenna electrode 5, as in the first embodiment, when the microwave was irradiated, a large plasma was generated between the tips of the first and second electrode portions 52 and 53. Further, in the plasma antenna electrode 5 of the second embodiment, the first and second electrode portions 52 and 53 are covered with the covering member 54, and plasma can be generated even in a conductive liquid such as water. When the plasma antenna electrode 5 was placed in water, which is a conductive liquid, and irradiated with microwaves, large plasma was generated. This is because the covering member 54 prevents electromagnetic waves from being absorbed by the conductive liquid when a standing wave is formed in the conductor.
The shape (plan view) of the main receiver 51 is not limited to the above, and may be an ellipse or a polygon such as a rectangle. The main receiver 51 is not limited to a plate shape, and may be a rod shape, a spherical shape, or the like. However, the main receiver 51 is preferably plate-shaped from the standpoint of installation and the like, and the circular shape can generate plasma more stably regardless of the microwave irradiation direction.
Further, the surface area (upper surface) of the main receiver 51 is preferably larger than the bottom area of the covering member 54. Thereby, a microwave can be received more reliably and effectively. The material of the covering member 54 may be a non-conductive material, and may be a resin member. Moreover, the shape of the 1st electrode part 52 and the 2nd electrode part 53 may be a triangle and a chestnut type as shown in FIG.2 and FIG.8.
1: Plasma generator,
2, 20, 5: antenna electrode for plasma,
21, 51: main receiver, 22, 52: first electrode, 23, 53: second electrode,
54: Cover member, 3: Outer container, 4: Microwave irradiation device
A microwave irradiation device for irradiating microwaves;
A main receiver that receives the microwave, a first electrode that extends from one end of the main receiver, and a tip that extends from the other end of the main receiver and is spaced apart and close to the tip of the first electrode A plasma antenna electrode comprising a conductor having a second electrode portion;
The plasma antenna electrode has a plurality of the conductors, the main reception unit mainly receives the microwave, and generates a standing wave in the plasma antenna electrode,
The plasma generating apparatus, wherein the plurality of conductors are arranged such that the main receiving portions of the conductors intersect each other.
The plasma generating apparatus according to claim 1, wherein all the tips are spaced apart from each other and close to each other.
In the plasma antenna electrode, the main receiver mainly receives the microwave, and generates a standing wave in the plasma antenna electrode.
The main receiver has a linear shape,
The said microwave irradiation apparatus irradiates a microwave in parallel with the said main receiving part with respect to the said antenna electrode for plasma, The plasma generator characterized by the above-mentioned.
The main receiving unit, the first electrode unit, and the second electrode unit are formed on the same plane,
The said microwave irradiation apparatus irradiates a microwave parallel to the said plane with respect to the said antenna electrode for plasma, The plasma generator characterized by the above-mentioned.
A main receiving unit that receives the microwave, a first electrode unit that extends upward from the surface of the main receiving unit, and an upper portion that extends upward from the surface of the main receiving unit, with a tip spaced apart and close to the tip of the first electrode unit A conductor having a second electrode portion,
A non-conductive covering member that is provided on the surface of the main receiving portion and covers the first electrode portion and the second electrode portion so that only the tip is exposed;
The plasma generator according to claim 1, wherein the main receiver receives the microwave mainly and generates a standing wave on the conductor.
The first electrode part and the second electrode part are integrally formed,
The total length of the first electrode part and the second electrode part is λ as the wavelength of the received microwave.
(Λ / 2) × n (n: positive odd number)
The plasma generator according to claim 5, wherein
The plasma generator according to any one of claims 1 to 6, wherein the first electrode portion and the second electrode portion have sharp tips.
The length of the conductor is λ as the wavelength of the received microwave.
The plasma generator as described in any one of Claims 1-4 which satisfy | fills.
The first electrode portion extends from one end of the main receiving portion in a direction intersecting the main receiving portion,
The plasma generating apparatus according to any one of claims 1 to 4, wherein the second electrode portion extends from the other end of the main receiving portion in a direction intersecting the main receiving portion.
The plasma generator according to any one of claims 1, 2, and 4, wherein the conductor has a C-shape.
The plasma generating apparatus according to any one of claims 1 to 4 , wherein the plasma antenna electrode is disposed in a non-conductive liquid.
The plasma generator according to any one of claims 1 to 11, which is used as a diamond synthesizer.
JP2010267354A 2010-11-30 2010-11-30 plasma generator Active JP5807854B2 (en)
JP2010267354A JP5807854B2 (en) 2010-11-30 2010-11-30 plasma generator
JP2012119145A JP2012119145A (en) 2012-06-21
JP5807854B2 true JP5807854B2 (en) 2015-11-10
ID=46501759
JP2010267354A Active JP5807854B2 (en) 2010-11-30 2010-11-30 plasma generator
JP (1) JP5807854B2 (en)
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