TWI470662B - Ion gun - Google Patents

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TWI470662B
TWI470662B TW98141369A TW98141369A TWI470662B TW I470662 B TWI470662 B TW I470662B TW 98141369 A TW98141369 A TW 98141369A TW 98141369 A TW98141369 A TW 98141369A TW I470662 B TWI470662 B TW I470662B
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filament
ion beam
ion
cathode
ion gun
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TW98141369A
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Chinese (zh)
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TW201110181A (en
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Yusuke Osada
Tadahisa Shiono
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Showa Shinku Kk
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Description

離子槍Ion gun

本發明係關於離子槍,特別是有關作為離子槍之陰極的燈絲之改良。This invention relates to ion guns, and more particularly to improvements in filaments that are cathodes of ion guns.

離子槍一般係使用於壓電元件之頻率調整裝置等,其原理是在離子槍內部產生電漿,從該電漿引出離子予以加速,藉此形成離子束。The ion gun is generally used for a frequency adjusting device of a piezoelectric element or the like. The principle is that plasma is generated inside the ion gun, and ions are extracted from the plasma to accelerate, thereby forming an ion beam.

專利文獻1揭示有一種離子槍,其係配置有複數個離子束引出孔,用於射出具有對應的電流密度峰值之離子束。Patent Document 1 discloses an ion gun in which a plurality of ion beam extraction holes are disposed for emitting an ion beam having a corresponding current density peak.

專利文獻2揭示有將複數燈絲配置於長邊方向之構成。根據該構成,只要各燈絲之發熱量相同,則熱陰極亦即陰極之熱分布均勻,可期待被射出之離子束的電流密度也均勻化。Patent Document 2 discloses a configuration in which a plurality of filaments are arranged in the longitudinal direction. According to this configuration, as long as the heat generation amount of each of the filaments is the same, the heat distribution of the cathode, that is, the cathode, is uniform, and the current density of the ion beam to be emitted is also expected to be uniform.

[專利文獻1]日本特開2006-100205號公報[Patent Document 1] Japanese Patent Laid-Open Publication No. 2006-100205

[專利文獻2]日本特開2007-311118號公報[Patent Document 2] Japanese Patent Laid-Open Publication No. 2007-311118

但是,如專利文獻2之構成,則必須使複數電源對應於複數燈絲而設置,離子槍之構成將複雜化、大型化,並且有變成高成本之問題。However, as in the configuration of Patent Document 2, it is necessary to provide a plurality of power sources corresponding to the plurality of filaments, and the configuration of the ion gun is complicated and large, and there is a problem that the cost is high.

因此,如上述之整齊排列有複數之離子束引出孔的離子槍中,係以將離子束電流密度變成不均勻之問題(特別是端部側之電流密度變小)藉由簡單且方便之構成予以解決作為課題。Therefore, in the ion gun in which the plurality of ion beam extraction holes are arranged neatly in the above manner, the problem that the ion beam current density becomes uneven (especially, the current density at the end side becomes small) is simple and convenient. It is solved as a problem.

本發明之第1側面係一種離子槍,其係具備:電漿產生手段,由陰極(10)及陽極(20)構成;以及柵極(30),用於從電漿產生手段所產生的電漿引出離子束;陰極係由架設在一對燈絲電極(13)間的燈絲(12)所構成,柵極係具有與燈絲平行排列的複數個離子束引出孔(31),包含該燈絲兩端部(12a)之每單位空間的發熱量,係大於包含燈絲中央部(12b)之每單位空間的發熱量。A first aspect of the present invention is an ion gun comprising: a plasma generating means comprising a cathode (10) and an anode (20); and a grid (30) for generating electricity from a plasma generating means The slurry extracts an ion beam; the cathode is composed of a filament (12) disposed between a pair of filament electrodes (13), and the gate has a plurality of ion beam extraction holes (31) arranged in parallel with the filament, including the ends of the filament The amount of heat generated per unit space of the portion (12a) is greater than the amount of heat generated per unit space including the central portion (12b) of the filament.

其中,燈絲兩端部為捲繞成線圈狀之構成亦可,兩端部被彎曲之構成亦可。In addition, the both ends of the filament may be configured to be wound into a coil shape, and the both end portions may be curved.

本發明之第2側面係一種離子槍,其係具備:電漿產生手段,由陰極(10)及陽極(20)構成;以及柵極(30),用於從電漿產生手段所產生的電漿引出離子束;陰極係由架設在一對燈絲電極間的燈絲(12)所構成,柵極係具有與燈絲平行排列的複數個離子束引出孔(31),相對於該燈絲中央部,兩端側係緻密地捲繞著。A second aspect of the invention is an ion gun comprising: a plasma generating means comprising a cathode (10) and an anode (20); and a grid (30) for generating electricity from the plasma generating means The slurry extracts an ion beam; the cathode system is composed of a filament (12) spanned between a pair of filament electrodes, and the gate has a plurality of ion beam extraction holes (31) arranged in parallel with the filament, with respect to the central portion of the filament, two The end side is densely wound.

針對整齊排列有複數個離子束引出孔的離子槍,可藉由簡單且便宜的構成解決離子束端部側之電流密度減少的問題,使離子束之電流密度均勻化。With respect to the ion gun in which a plurality of ion beam extraction holes are arranged neatly, the current density of the ion beam can be made uniform by a simple and inexpensive configuration, and the current density of the ion beam can be made uniform.

第1圖之離子槍100係具備:架設在一對燈絲電極13之間的燈絲11(陰極10)、與燈絲11平行地對向配置之陽極20、具有複數個離子束引出孔31之柵極30、以及將陰極10及陽極20密閉於內部並且使複數個離子束引出孔31露出之本體40。陰極10和陽極20係構成電漿產生手段,並且連接在分別的電源(不圖示)。又,本體40係具備:氣體導入口41,用於導入放電氣體;及遮蔽板42,用於防止陰極10和陽極20之間不必要的放電。The ion gun 100 of Fig. 1 includes a filament 11 (cathode 10) spanned between a pair of filament electrodes 13, an anode 20 disposed in parallel with the filament 11, and a gate having a plurality of ion beam extraction holes 31. 30. The body 40 in which the cathode 10 and the anode 20 are sealed inside and the plurality of ion beam extraction holes 31 are exposed. The cathode 10 and the anode 20 constitute a plasma generating means and are connected to respective power sources (not shown). Further, the main body 40 includes a gas introduction port 41 for introducing a discharge gas, and a shielding plate 42 for preventing unnecessary discharge between the cathode 10 and the anode 20.

如第2A圖及第2B圖所示,柵極30的複數個離子束引出孔31係於藉由環狀的陽極20所隔成之區域內部,整齊排列在與燈絲11同一方向。As shown in FIGS. 2A and 2B, the plurality of ion beam extraction holes 31 of the gate electrode 30 are arranged inside the region partitioned by the annular anode 20, and are aligned in the same direction as the filament 11.

離子槍之動作係首先將氬等放電氣體從氣體導入口41導入本體40之內部。分別在陰極10施加負電壓、在陽極20施加正電壓,藉由其電位差進行放電而產生電漿。在柵極30施加電壓時,藉由複數個離子束引出孔31從電漿引出離子予以加速,形成離子束。The operation of the ion gun first introduces a discharge gas such as argon into the inside of the body 40 from the gas introduction port 41. A negative voltage is applied to the cathode 10, a positive voltage is applied to the anode 20, and discharge is generated by the potential difference to generate a plasma. When a voltage is applied to the gate electrode 30, ions are extracted from the plasma by a plurality of ion beam extraction holes 31 to form an ion beam.

其中,針對陽極20予以補充。第9圖(a)~(d)係顯示陽極的形狀(皆為俯視圖)變化者。第9圖(a)係第2圖所示之環狀型者,但其他還有如(b)之在長邊方向分割者,如(c)之形者,如(d)之在寬方向分割者等。又,不限於方形,也可以是橢圓形。此外,亦可不設陽極20而將本體40本身當作陽極。Among them, the anode 20 is supplemented. Fig. 9 (a) to (d) show changes in the shape of the anode (both in plan view). Fig. 9(a) is a ring type shown in Fig. 2, but others are also divided in the long side direction as in (b), as in (c) The shape, such as (d) is divided in the wide direction, and so on. Further, it is not limited to a square shape, and may be an elliptical shape. Further, the body 40 itself may be used as an anode without providing the anode 20.

又,針對複數個離子束引出孔31予以補充。第10圖(a)~(e)係顯示複數個離子束引出孔31之變化者。如此地,除了第2圖(亦即,第10圖(d))所顯示者之外 ,離子束引出孔31可獲得各種形態。本說明書及申請專利範圍所說的「複數個離子束引出孔」係包含上述例示之全部態樣及其類似之態樣。Further, a plurality of ion beam extraction holes 31 are supplemented. Fig. 10 (a) to (e) show changes in a plurality of ion beam extraction holes 31. Thus, except as shown in Figure 2 (ie, Figure 10 (d)) The ion beam extraction hole 31 can be obtained in various forms. The "plurality of ion beam extraction holes" as used in the specification and claims refers to all aspects of the above-described examples and the like.

總之,如第1圖之離子槍也是耐於實用者,但熱陰極亦即燈絲11端部之温度仍低於燈絲電極13之散熱,因此從端部側之離子束引出孔31所射出之離子束的電流密度會有減少之情形。In short, the ion gun as shown in Fig. 1 is also resistant to practical use, but the temperature of the hot cathode, that is, the end of the filament 11 is still lower than that of the filament electrode 13, so that the ion emitted from the ion beam extraction hole 31 on the end side The current density of the beam will be reduced.

第3圖係顯示此構成中的距離柵極面25mm之位置,亦即配置有處理基板的位置中的離子束之電流密度者。如圖示,各峰值係對應於各離子束引出孔31,相對於中心附近的電流密度峰值,端部側的電流密度峰值略微減少。如此地,在第1圖之構成中,離子束電流密度會有變成不均勻者之情形。Fig. 3 is a view showing a position in the configuration of 25 mm from the gate surface, that is, a current density of an ion beam in a position where the substrate is processed. As shown in the figure, each peak line corresponds to each ion beam extraction hole 31, and the peak value of the current density on the end side is slightly decreased with respect to the current density peak near the center. As described above, in the configuration of Fig. 1, the ion beam current density may become uneven.

因此,第4A圖係顯示進一步改良後的本發明之離子槍200。離子槍200的陽極20、柵極30及本體40之構成係與前述第1圖、第2圖、第9圖及第10圖同樣,因此賦予相同符號而省略其說明。Thus, Figure 4A shows a further improved ion gun 200 of the present invention. The configuration of the anode 20, the gate electrode 30, and the body 40 of the ion gun 200 is the same as that of the first, second, ninth, and ninth drawings, and therefore the same reference numerals will be given thereto, and the description thereof will be omitted.

第4A圖中,熱陰極亦即陰極10係由一對架設在燈絲電極13之間的燈絲12構成。此外,第4A圖中也是陰極10和陽極20構成電漿產生手段,且連接在分別的電源(不圖示)。In Fig. 4A, the hot cathode, i.e., the cathode 10, is composed of a pair of filaments 12 spanned between the filament electrodes 13. Further, in Fig. 4A, the cathode 10 and the anode 20 also constitute a plasma generating means, and are connected to respective power sources (not shown).

為了方便說明,如第4B圖所示,將燈絲12當作由端部12a和中央部12b構成者。端部12a係捲繞成線圈狀,相較於以往的燈絲11,端部之發熱量變大。藉此,即使燈絲12因燈絲電極13而被散熱,端部12a的温度仍可維持於預定之高温。For convenience of explanation, as shown in Fig. 4B, the filament 12 is constituted by the end portion 12a and the central portion 12b. The end portion 12a is wound in a coil shape, and the amount of heat generated at the end portion is increased as compared with the conventional filament 11. Thereby, even if the filament 12 is dissipated by the filament electrode 13, the temperature of the end portion 12a can be maintained at a predetermined high temperature.

第5圖係顯示第4A圖之離子槍200中的距離柵極面25mm之位置,亦即配置有處理基板的位置中的離子束之電流密度者。第5圖中也是電流密度之峰值對應於各離子束引出孔31。與第3圖比較即可明瞭,端部側之電流密度峰值相對於離子束中心附近之電流密度峰值的降低被減輕,可使離子束電流密度涵蓋其長邊方向為大致均勻者。Fig. 5 is a view showing the position of the ion gun 200 of Fig. 4A which is 25 mm from the gate surface, that is, the current density of the ion beam in the position where the substrate is processed. Also in Fig. 5, the peak of the current density corresponds to each ion beam extraction hole 31. As can be seen from comparison with Fig. 3, the peak of the current density at the end side is reduced with respect to the peak of the current density near the center of the ion beam, and the ion beam current density can be made to be substantially uniform in the longitudinal direction.

此外,藉由調節在端部12a之捲繞數或捲繞密度,可調整該離子束電流密度之分布。Further, the distribution of the ion beam current density can be adjusted by adjusting the number of windings or the winding density at the end portion 12a.

例如,如第6A圖,可使捲繞成線圈狀的燈絲12於其捲繞中具有粗密,亦可使靠近端部側之捲繞為密,使靠近中心部之捲繞為疏。又,如第6B圖,亦可使燈絲端部之捲繞徑大於燈絲中心部之捲繞徑。又,如第6C圖,可使捲繞成線圈狀的燈絲12於其捲繞徑具有傾斜,亦可使靠近端部側之捲繞徑變大,使靠近中心部之捲徑變小。For example, as shown in Fig. 6A, the filament 12 wound in a coil shape can be made thick in winding, or the winding near the end side can be made dense, and the winding near the center portion can be made thin. Further, as shown in Fig. 6B, the winding diameter of the end portion of the filament may be made larger than the winding diameter of the central portion of the filament. Further, as shown in Fig. 6C, the filament 12 wound in a coil shape can be inclined in the winding diameter, and the winding diameter near the end portion can be increased, and the winding diameter close to the center portion can be made small.

如第7圖所示,本發明之核心在於包含燈絲端部12a之每單位空間A的發熱量大於包含燈絲中央部12b之每單位空間B的發熱量。因而,實施形態不限於第4B圖之構成,如以下之變形例亦包含在本發明。As shown in Fig. 7, the core of the present invention is that the amount of heat generated per unit space A including the filament end portion 12a is larger than the amount of heat generated per unit space B including the filament center portion 12b. Therefore, the embodiment is not limited to the configuration of Fig. 4B, and the following modifications are also included in the present invention.

例如,如第8A圖及第8B圖所示,亦可使燈絲端部12a彎曲以增加端部側之發熱量。此外,各圖不一定要依照顯示之尺寸。For example, as shown in Figs. 8A and 8B, the filament end portion 12a may be bent to increase the amount of heat generation at the end side. In addition, the figures do not have to follow the dimensions shown.

又,亦可使燈絲12的阻抗值曲線傾斜,使端部側的阻抗值高於中心部側的阻抗值,增加端部側的發熱量。Moreover, the impedance value curve of the filament 12 can be inclined, and the impedance value at the end portion side is higher than the impedance value at the center portion side, and the amount of heat generation at the end portion side is increased.

10...陰極10. . . cathode

11、12...燈絲11,12. . . filament

12a...燈絲端部12a. . . Filament end

12b...燈絲中央部12b. . . Central part of the filament

13...燈絲電極13. . . Filament electrode

20...陽極20. . . anode

30...柵極30. . . Gate

31...離子束引出孔31. . . Ion beam extraction hole

40...本體40. . . Ontology

41...氣體導入口41. . . Gas inlet

42...遮蔽板42. . . Masking board

100、200...離子槍100, 200. . . Ion gun

第1圖係顯示本發明之離子槍之圖。Fig. 1 is a view showing the ion gun of the present invention.

第2A圖係柵極的構成之說明圖。Fig. 2A is an explanatory view showing the configuration of the gate.

第2B圖係柵極的構成之說明圖。Fig. 2B is an explanatory view showing the configuration of the gate.

第3圖係本發明之說明圖。Figure 3 is an explanatory view of the present invention.

第4A圖係顯示本發明之離子槍之圖。Fig. 4A is a view showing the ion gun of the present invention.

第4B圖係顯示本發明之燈絲之圖。Figure 4B is a diagram showing the filament of the present invention.

第5圖係本發明之說明圖。Figure 5 is an explanatory view of the present invention.

第6A圖係顯示本發明之燈絲之變形例圖。Fig. 6A is a view showing a modification of the filament of the present invention.

第6B圖係顯示本發明之燈絲之變形例圖。Fig. 6B is a view showing a modification of the filament of the present invention.

第6C圖係顯示本發明之燈絲之變形例圖。Fig. 6C is a view showing a modification of the filament of the present invention.

第7圖係本發明之說明圖。Figure 7 is an explanatory view of the present invention.

第8A圖係顯示本發明之燈絲之變形例圖。Fig. 8A is a view showing a modification of the filament of the present invention.

第8B圖係顯示本發明之燈絲之變形例圖。Fig. 8B is a view showing a modification of the filament of the present invention.

第9圖係本發明之補充圖。Figure 9 is a supplementary diagram of the present invention.

第10圖係本發明之補充圖。Figure 10 is a supplementary diagram of the present invention.

10...陰極10. . . cathode

12...燈絲12. . . filament

13...燈絲電極13. . . Filament electrode

20...陽極20. . . anode

30...柵極30. . . Gate

40...本體40. . . Ontology

41...氣體導入口41. . . Gas inlet

42...遮蔽板42. . . Masking board

200...離子槍200. . . Ion gun

Claims (4)

一種離子槍,其係具備:電漿產生手段,由陰極(10)及陽極(20)構成;及柵極(30),用於從該電漿產生手段所產生的電漿引出離子束;該陰極係由架設在一對燈絲電極間的燈絲(12)所構成,該柵極係具有與該燈絲平行排列的複數個離子束引出孔(31),包含該燈絲兩端部(12a)之每單位空間的發熱量,係大於包含該燈絲中央部(12b)之每單位空間的發熱量。An ion gun comprising: a plasma generating means comprising a cathode (10) and an anode (20); and a grid (30) for extracting an ion beam from the plasma generated by the plasma generating means; The cathode system is composed of a filament (12) spanned between a pair of filament electrodes, the grid having a plurality of ion beam extraction holes (31) arranged in parallel with the filament, comprising each of the two ends (12a) of the filament The amount of heat generated per unit space is greater than the amount of heat generated per unit space including the central portion (12b) of the filament. 如申請專利範圍第1項之離子槍,其中,前述燈絲兩端部被捲繞成線圈狀。An ion gun according to claim 1, wherein both ends of the filament are wound into a coil shape. 如申請專利範圍第1項之離子槍,其中,前述燈絲兩端部被彎曲。The ion gun of claim 1, wherein the ends of the filament are bent. 一種離子槍,其係具備:電漿產生手段,由陰極(10)及陽極(20)構成;及柵極(30),用於從該電漿產生手段所產生的電漿引出離子束;該陰極係由架設在一對燈絲電極間的燈絲(12)所構成,該柵極係具有與該燈絲平行排列的複數個離子束引出孔(31),相對於該燈絲中央部,兩端側係緻密地捲繞著。An ion gun comprising: a plasma generating means comprising a cathode (10) and an anode (20); and a grid (30) for extracting an ion beam from the plasma generated by the plasma generating means; The cathode system is composed of a filament (12) spanned between a pair of filament electrodes, the gate having a plurality of ion beam extraction holes (31) arranged in parallel with the filament, and the two ends are opposite to the central portion of the filament Wrapped densely.
TW98141369A 2008-12-24 2009-12-03 Ion gun TWI470662B (en)

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