TW202301428A - Negative ion irradiation device and control method thereof wherein the negative ion irradiation device includes a control unit and a gas supply unit - Google Patents

Negative ion irradiation device and control method thereof wherein the negative ion irradiation device includes a control unit and a gas supply unit Download PDF

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TW202301428A
TW202301428A TW111134662A TW111134662A TW202301428A TW 202301428 A TW202301428 A TW 202301428A TW 111134662 A TW111134662 A TW 111134662A TW 111134662 A TW111134662 A TW 111134662A TW 202301428 A TW202301428 A TW 202301428A
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plasma
irradiation device
compound semiconductor
negative ion
ion irradiation
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TWI823563B (en
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北見尚久
酒見俊之
山本哲也
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日商住友重機械工業股份有限公司
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    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
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    • C23C14/32Vacuum evaporation by explosion; by evaporation and subsequent ionisation of the vapours, e.g. ion-plating
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/30Electron-beam or ion-beam tubes for localised treatment of objects
    • H01J37/317Electron-beam or ion-beam tubes for localised treatment of objects for changing properties of the objects or for applying thin layers thereon, e.g. for ion implantation
    • H01J37/3171Electron-beam or ion-beam tubes for localised treatment of objects for changing properties of the objects or for applying thin layers thereon, e.g. for ion implantation for ion implantation
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    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/22Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material characterised by the process of coating
    • C23C14/54Controlling or regulating the coating process
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    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/58After-treatment
    • C23C14/5826Treatment with charged particles
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/30Electron-beam or ion-beam tubes for localised treatment of objects
    • H01J37/304Controlling tubes by information coming from the objects or from the beam, e.g. correction signals
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
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Abstract

The present invention provides a negative ion irradiation device and a control method of the negative ion irradiation device that can improve the manufacturing efficiency and the quality of a compound semiconductor. A control unit (50) controls a gas supply unit (40) to supply gas into a vacuum chamber (10). The gas supply unit (40) supplies a gas containing the same element as the ions forming the compound semiconductor (11). Therefore, the same element as the ions forming the compound semiconductor (11) exists in the vacuum chamber (10). Furthermore, the control unit (50) controls a plasma generator (14) to generate a plasma (P) and an electron in the vacuum chamber (10) and stop the generation of the plasma (P) to generate a negative ion by the electron and the gas, and irradiates the compound semiconductor (11) with the negative ion.

Description

負離子照射裝置及負離子照射裝置的控制方法Negative ion irradiation device and control method of negative ion irradiation device

本申請主張基於2018年7月18日申請之日本專利申請第2018-134880號的優先權。該日本申請的全部內容藉由參閱援用於本說明書中。 本發明係有關一種負離子照射裝置及負離子照射裝置的控制方法。 This application claims priority based on Japanese Patent Application No. 2018-134880 filed on July 18, 2018. The entire content of this Japanese application is incorporated in this specification by reference. The invention relates to a negative ion irradiation device and a control method for the negative ion irradiation device.

以往,作為化合物半導體已知有專利文獻1中所記載者。在構成該種化合物半導體之單晶基板上結晶缺陷增加。在專利文獻1中,藉由設計製造方法,試圖減少單晶基板的結晶缺陷。 (先前技術文獻) (專利文獻) 專利文獻1:日本特開2014-22711號公報 Conventionally, what is described in Patent Document 1 is known as a compound semiconductor. Crystal defects increase on the single crystal substrate constituting this compound semiconductor. In Patent Document 1, an attempt is made to reduce crystal defects of a single crystal substrate by devising a manufacturing method. (Prior Art Literature) (patent documents) Patent Document 1: Japanese Patent Laid-Open No. 2014-22711

(本發明所欲解決之課題) 然而,當製造單晶基板時,即使設計製造方法,亦難以防止結晶缺陷的產生。此外,當在單晶基板上產生結晶缺陷時,並不存在用於填補該結晶缺陷之實用的方法。因此,以保持原樣的狀態使用單晶基板的結晶缺陷。單晶基板依據結晶缺陷的量確定等級(品質),並依據等級確定用途。因此,存在如下問題,亦即,由於能夠用於化合物半導體之單晶基板的數量有限,從而導致化合物半導體的製造效率降低。另一方面,存在如下問題,亦即,當將等級低的單晶基板用作化合物半導體時,化合物半導體的品質降低。 因此,本發明的目的為提供一種能夠提高化合物半導體的製造效率及品質之負離子照射裝置及負離子照射裝置的控制方法。 (用以解決課題之手段) 為了解決上述課題,本發明之負離子照射裝置向化合物半導體照射負離子,該負離子照射裝置具備:腔室,在內部進行負離子的生成;氣體供給部,供給包含與形成化合物半導體之離子相同的元素之氣體;電漿生成部,在腔室內生成電漿及電子;配置部,配置化合物半導體;及控制部,進行負離子照射裝置的控制,控制部控制氣體供給部而向腔室內供給氣體,控制部控制電漿生成部而在腔室內生成電漿及電子,並且,藉由停止電漿的生成,由電子和氣體生成負離子,並將該負離子照射到化合物半導體。 在本發明之負離子照射裝置中,控制部控制氣體供給部而向腔室內供給氣體。氣體供給部供給包含與形成化合物半導體之離子相同的元素之氣體。因此,在腔室內存在與形成化合物半導體之離子相同的元素。進而,控制部控制電漿生成部而在腔室內生成電漿及電子,並且,藉由停止電漿的生成,由電子和氣體生成負離子,並將該負離子照射到化合物半導體上。藉此,與形成化合物半導體之離子相同的元素的負離子被照射到化合物半導體。藉此,負離子進入化合物半導體內的來自陰離子之結晶缺陷,從而能夠填補該結晶缺陷。如此能夠填補化合物半導體的結晶缺陷,因此能夠提高化合物半導體的品質。又,在負離子照射前,即使作為化合物半導體的等級不充分之情況下,亦能夠藉由負離子照射提高品質,因此能夠減少預先篩選單晶基板的等級的必要性。藉由以上,能夠提高化合物半導體的製造效率及品質。 本發明之負離子照射裝置的控制方法係向化合物半導體照射負離子之負離子照射裝置的控制方法,負離子照射裝置具備:腔室,在內部進行負離子的生成;氣體供給部,供給包含與形成化合物半導體之離子相同的元素之氣體;電漿生成部,在腔室內生成電漿及電子;配置部,配置化合物半導體;及控制部,進行負離子照射裝置的控制,負離子照射裝置的控制方法包括:氣體供給製程,藉由控制部控制氣體供給部而向腔室內供給氣體;及負離子照射製程,藉由控制部控制電漿生成部而在腔室內生成電漿及電子,並且,藉由停止電漿的生成,由電子和氣體生成負離子,並將該負離子照射到化合物半導體。 藉由本發明之負離子照射裝置的控制方法,能夠獲得與上述負離子照射裝置相同宗旨的作用·效果。 (發明之效果) 藉由本發明,能夠提供一種能夠提高化合物半導體的製造效率及品質之負離子照射裝置及負離子照射裝置的控制方法。 (Problem to be solved by the present invention) However, when manufacturing a single crystal substrate, it is difficult to prevent the generation of crystal defects even if the manufacturing method is devised. Furthermore, when crystal defects are generated on a single crystal substrate, there is no practical method for filling the crystal defects. Therefore, the crystal defects of the single crystal substrate are used as they are. The grade (quality) of the single crystal substrate is determined according to the amount of crystal defects, and the usage is determined according to the grade. Therefore, there is a problem that the production efficiency of the compound semiconductor is lowered due to the limited number of single crystal substrates that can be used for the compound semiconductor. On the other hand, there is a problem that, when a low-grade single crystal substrate is used as a compound semiconductor, the quality of the compound semiconductor decreases. Therefore, an object of the present invention is to provide a negative ion irradiation device and a control method of the negative ion irradiation device capable of improving the production efficiency and quality of compound semiconductors. (means to solve problems) In order to solve the above-mentioned problems, the anion irradiation device of the present invention irradiates negative ions to compound semiconductors, and the negative ion irradiation device includes: a chamber for generating negative ions inside; and a gas supply unit for supplying gas containing the same element as ions forming the compound semiconductor. The plasma generating part generates plasma and electrons in the chamber; the disposing part disposes the compound semiconductor; The plasma generating unit generates plasma and electrons in the chamber, and by stopping the generation of plasma, negative ions are generated from the electrons and gas, and the negative ions are irradiated to the compound semiconductor. In the negative ion irradiation apparatus of this invention, a control part controls a gas supply part, and supplies gas into a chamber. The gas supply unit supplies gas containing the same element as ions forming the compound semiconductor. Therefore, the same elements as ions forming the compound semiconductor exist in the chamber. Furthermore, the control unit controls the plasma generating unit to generate plasma and electrons in the chamber, and by stopping generation of the plasma, negative ions are generated from the electrons and the gas, and the negative ions are irradiated onto the compound semiconductor. Thereby, negative ions of the same element as ions forming the compound semiconductor are irradiated to the compound semiconductor. Thereby, the negative ions enter the crystal defects derived from the negative ions in the compound semiconductor, so that the crystal defects can be filled. Since crystal defects of the compound semiconductor can be filled in this way, the quality of the compound semiconductor can be improved. Also, even if the grade of the compound semiconductor is not sufficient before negative ion irradiation, the quality can be improved by negative ion irradiation, so the necessity of screening the grade of the single crystal substrate in advance can be reduced. Through the above, the production efficiency and quality of compound semiconductors can be improved. The control method of the negative ion irradiation device of the present invention is a control method of the negative ion irradiation device for irradiating negative ions to the compound semiconductor. The negative ion irradiation device is provided with: a chamber for generating negative ions inside; The gas of the same element; the plasma generation part generates plasma and electrons in the chamber; the configuration part arranges the compound semiconductor; and the control part controls the negative ion irradiation device. The control method of the negative ion irradiation device includes: gas supply process, The control part controls the gas supply part to supply gas into the chamber; and the negative ion irradiation process controls the plasma generation part by the control part to generate plasma and electrons in the chamber, and by stopping the generation of plasma, the Electrons and gas generate negative ions, and the negative ions are irradiated to the compound semiconductor. By the control method of the negative ion irradiation device of the present invention, the same purpose and effect as those of the above-mentioned negative ion irradiation device can be obtained. (Effect of Invention) According to the present invention, it is possible to provide a negative ion irradiation device and a control method of the negative ion irradiation device capable of improving the production efficiency and quality of compound semiconductors.

以下,參閱添附之圖式並對本發明的一實施形態之負離子照射裝置進行說明。另外,在圖式中,對相同要素標註相同符號並省略重複說明。 首先,參閱圖1及圖2,對本發明的實施形態之負離子照射裝置的構成進行說明。圖1及圖2係表示本實施形態之負離子照射裝置的構成之概略剖視圖。圖1表示電漿生成時的動作狀態,圖2表示電漿停止時的動作狀態。 如圖1及圖2所示,本實施形態的負離子照射裝置1係將用於所謂的離子電鍍法之成膜技術應用於負離子照射之裝置。另外,為了便於說明,圖1及圖2中示出XYZ座標系統。Y軸方向係後述之輸送化合物半導體之方向。X軸方向係化合物半導體的厚度方向。Z軸方向係與Y軸方向及X軸方向正交之方向。 負離子照射裝置1可以為如下所謂的臥式負離子照射裝置,亦即,以化合物半導體11的板厚方向成為大致鉛直方向之方式將化合物半導體11配置於真空腔室10內並輸送。此時,Z軸及Y軸方向為水平方向,X軸方向成為鉛直方向且板厚方向。另外,負離子照射裝置1亦可以為如下所謂的立式負離子照射裝置,亦即,以化合物半導體11的板厚方向成為水平方向(圖1及圖2中為X軸方向)之方式,在使化合物半導體11直立或從使其直立之狀態傾斜之狀態下,將化合物半導體11配置於真空腔室10內並輸送。此時,X軸方向為水平方向且化合物半導體11的板厚方向,Y軸方向為水平方向,Z軸方向成為鉛直方向。本發明的一實施形態之負離子照射裝置在下文中以臥式負離子照射裝置為例進行說明。 負離子照射裝置1具備真空腔室10、輸送機構(配置部)3、電漿生成部14、氣體供給部40、電路部34、電壓施加部90及控制部50。 真空腔室10係用於收納化合物半導體11並進行成膜處理之構件。真空腔室10具有用於輸送化合物半導體11之輸送室10a、用於生成負離子之生成室10b及將從電漿槍7以射束狀照射之電漿P收納到真空腔室10之電漿口10c。輸送室10a、生成室10b及電漿口10c彼此連通。輸送室10a沿既定的輸送方向(圖中的箭頭A)(沿Y軸)被設定。又,真空腔室10由導電性材料構成且與接地電位連接。輸送室10a中設置有用於加熱化合物半導體11之加熱部30。加熱部30設置於比在輸送室10a中與生成室10b的連通部更靠輸送方向的上游側。因此,來自生成室10b之負離子被照射到已加熱之狀態的化合物半導體11。 生成室10b作為壁部10W具有:沿著輸送方向(箭頭A)之一對側壁、沿著與輸送方向(箭頭A)交叉之方向(Z軸方向)之一對側壁10h、10i及與X軸方向交叉而配置之底面壁10j。 輸送機構3沿輸送方向(箭頭A)輸送以與生成室10b對置之狀態保持化合物半導體11之化合物半導體保持構件16。輸送機構3作為配置化合物半導體11之配置部發揮功能。例如,化合物半導體保持構件16係保持化合物半導體11的外周邊緣之框體。輸送機構3由設置於輸送室10a內之複數個輸送輥15構成。輸送輥15沿輸送方向(箭頭A)以等間隔配置,且支承化合物半導體保持構件16之同時沿輸送方向(箭頭A)輸送。 另外,化合物半導體11為板狀的基板。對於化合物半導體11的材質等如後述說明。 接著,對電漿生成部14的構成進行詳細說明。電漿生成部14在真空腔室10內生成電漿及電子。電漿生成部14具有電漿槍7、轉向線圈5及爐缸機構2。 電漿槍7例如為壓力梯度型的電漿槍,其主體部分經由設置於生成室10b的側壁之電漿口10c與生成室10b連接。電漿槍7在真空腔室10內生成電漿P。在電漿槍7中所生成之電漿P以射束狀從電漿口10c出射到生成室10b內。藉此,在生成室10b內生成電漿P。 電漿槍7的一端被陰極60封閉。在陰極60與電漿口10c之間同心地配置有第1中間電極(柵格)61及第2中間電極(柵格)62。在第1中間電極61內內置有用於收斂電漿P之環狀永久磁鐵61a。在第2中間電極62內亦為了收斂電漿P而內置有電磁體線圈62a。 電漿槍7在生成負離子時,在生成室10b內間歇地生成電漿P。具體而言,藉由後述控制部50使電漿槍7被控制成在生成室10b內間歇地生成電漿P。關於該控制,在控制部50的說明中進行詳細敘述。 轉向線圈5設置於安裝有電漿槍之電漿口10c的周圍。轉向線圈5將電漿P引導至生成室10b內。轉向線圈5藉由轉向線圈用電源(未圖示)被激磁。 爐缸機構2係將來自電漿槍的電漿P引導至所期望的位置之機構。爐缸機構2具有主爐缸17及環爐缸6。當使用負離子照射裝置1進行成膜時,主爐缸17作為保持成膜材料之陽極而發揮功能。但是,當進行負離子生成時,電漿被引導至環爐缸6,以使電漿P不被引導至成膜材料。因此,負離子照射裝置1不進行成膜而只進行負離子照射時,成膜材料可以不被主爐缸17保持。或者,爐缸機構2只要具有只引導電漿P之構成即可。 環爐缸6為具有用於感應電漿P之電磁體之陽極。環爐缸6配置於主爐缸17的填充部17a的周圍。環爐缸6具有環狀的線圈9、環狀的永久磁鐵部20及環狀的容器12,線圈9及永久磁鐵部20容納於容器12中。在本實施形態中,從輸送機構3觀察時在X軸負方向上依次設置有線圈9、永久磁鐵部20,但亦可以在X軸負方向上依次設置有永久磁鐵部20、線圈9。 氣體供給部40配置於真空腔室10的外部。氣體供給部40通過設置於生成室10b的側壁(例如側壁10h)之氣體供給口41,向真空腔室10內供給氣體。關於氣體的具體例如後述說明。 氣體供給口41的位置較佳為生成室10b與輸送室10a的邊界附近的位置。此時,由於能夠將來自氣體供給部40的氣體供給到生成室10b與輸送室10a的邊界附近,因此在該邊界附近進行後述說明之負離子的生成。 因此,能夠將生成之負離子適宜地注入於輸送室10a內的化合物半導體11。另外,氣體供給口41的位置不限於生成室10b與輸送室10a的邊界附近。 電路部34具有可變電源80、第1配線71、第2配線72、電阻器R1~R4及短路開關SW1、SW2。 可變電源80夾著位於接地電位之真空腔室10,向電漿槍7的陰極60施加負電壓,且向爐缸機構2的主爐缸17施加正電壓。藉此,可變電源80在電漿槍7的陰極60與爐缸機構2的主爐缸17之間產生電位差。 第1配線71電連接電漿槍7的陰極60與可變電源80的負電位側。第2配線72電連接爐缸機構2的主爐缸17(陽極)與可變電源80的正電位側。 電阻器R1的一端與電漿槍7的第1中間電極61電連接,並且另一端經由第2配線72與可變電源80電連接。亦即,電阻器R1在第1中間電極61與可變電源80之間串列連接。 電阻器R2的一端與電漿槍7的第2中間電極62電連接,並且另一端經由第2配線72與可變電源80電連接。亦即,電阻器R2在第2中間電極62與可變電源80之間串列連接。 電阻器R3的一端與生成室10b的壁部10W電連接,並且另一端經由第2配線72與可變電源80電連接。亦即,電阻器R3在生成室10b的壁部10W與可變電源80之間串列連接。 電阻器R4的一端與環爐缸6電連接,並且另一端經由第2配線72與可變電源80電連接。亦即,電阻器R4在環爐缸6與可變電源80之間串列連接。 短路開關SW1、SW2分別為藉由接收來自控制部50的指令訊號來切換成ON/OFF(開啟/關閉)狀態之切換部。 短路開關SW1與電阻器R2並列連接。短路開關SW1在生成電漿P時呈OFF狀態。藉此,第2中間電極62與可變電源80經由電阻器R2彼此電連接,因此電流難以在第2中間電極62與可變電源80之間流動。其結果,來自電漿槍7的電漿P被出射到真空腔室10內。另外,當將來自電漿槍7的電漿P出射到真空腔室10內時,可以代替使電流難以流向第2中間電極62之情況而使電流難以流向第1中間電極61。此時,短路開關SW1不與第2中間電極62側連接而連接於第1中間電極61側。 另一方面,當停止電漿P時,短路開關SW1呈ON狀態。藉此,第2中間電極62與可變電源80之間的電連接發生短路,因此電流在第2中間電極62與可變電源80之間流動。亦即,短路電流流向電漿槍7。其結果,來自電漿槍7的電漿P不被出射到真空腔室10內。 當生成負離子時,藉由控制部50以既定間隔切換短路開關SW1的ON/OFF狀態,藉此,在真空腔室10內間歇地生成來自電漿槍7的電漿P。亦即,短路開關SW1係切換向真空腔室10內的電漿P的供給和切斷之切換部。 短路開關SW2與電阻器R4並列連接。短路開關SW2藉由將電漿P引導至主爐缸17側還是引導至環爐缸6側而由控制部50切換ON/OFF狀態。若短路開關SW2呈ON狀態,則由於環爐缸6與可變電源80之間的電連接發生短路,因此相較於主爐缸17,電流更容易流向環爐缸6。藉此,電漿P容易被引導至環爐缸6。另一方面,若短路開關SW2呈OFF狀態,則環爐缸6與可變電源80經由電阻器R4電連接,因此相較於環爐缸6,電流更容易流向主爐缸17,從而電漿P容易被引導至主爐缸17側。另外,當生成負離子時,短路開關SW2保持在ON狀態。當負離子照射裝置1不進行成膜時,短路開關SW2可以保持在ON狀態。 電壓施加部90能夠向成膜後的化合物半導體(對象物)11施加正電壓。電壓施加部90具備偏壓電路35及滑接線18。 偏壓電路35係用於對成膜後的化合物半導體11施加正的偏壓的電路。偏壓電路35具有對化合物半導體11施加正的偏壓(以下,簡稱為“偏壓”)之偏壓電源27、電連接偏壓電源27與滑接線18之第3配線73及設置於第3配線73之短路開關SW3。偏壓電源27施加作為週期性地增加或減少之矩形波之電壓訊號(週期性電訊號)來作為偏壓。偏壓電源27構成為能夠藉由控制部50的控制來改變所施加之偏壓的頻率。第3配線73的一端與偏壓電源27的正電位側連接,並且另一端與滑接線18連接。藉此,第3配線73電連接滑接線18與偏壓電源27。 短路開關SW3藉由第3配線73在滑接線18與偏壓電源27的正電位側之間串聯連接。短路開關SW3係切換有無對滑接線18施加偏壓之切換部。短路開關SW3藉由控制部50切換其ON/OFF狀態。短路開關SW3在負離子生成時在既定時序呈ON狀態。若短路開關SW3呈ON狀態,則滑接線18與偏壓電源27的正電位側彼此電連接,對滑接線18施加偏壓。 另一方面,短路開關SW3在負離子生成時的既定時序呈OFF狀態。若短路開關SW3呈OFF狀態,則滑接線18與偏壓電源27彼此電切斷,且未對滑接線18施加偏壓。 滑接線18為對化合物半導體保持構件16進行供電之架線。滑接線18在輸送室10a內沿輸送方向(箭頭A)延伸而設置。滑接線18藉由與設置於化合物半導體保持構件16之供電刷42接觸而通過供電刷42對化合物半導體保持構件16進行供電。滑接線18例如由不銹鋼製的金屬絲等構成。 控制部50為控制負離子照射裝置1整體之裝置,具備統括管理裝置整體之ECU[Electronic Control Unit:電子控制單元]。ECU為具有CPU[Central Processing Unit:中央處理單元]、ROM[Read Only Memory:唯讀記憶體]、RAM[Random Access Memory:隨機存取記憶體]、CAN[Controller Area Network:控制器區域網路]通訊電路等之電子控制單元。在ECU中,例如藉由將儲存於ROM之程式加載到RAM,並由CPU執行加載到RAM之程式來實現各種功能。ECU可以由複數個電子單元構成。 控制部50配置於真空腔室10的外部。又,控制部50具備控制基於氣體供給部40之氣體供給之氣體供給控制部51、控制基於電漿生成部14之電漿P的生成之電漿控制部52及控制基於電壓施加部90之電壓的施加之電壓控制部53。 氣體供給控制部51控制氣體供給部40而向生成室10b內供給氣體。接著,控制部50的電漿控制部52將電漿生成部14控制成在生成室10b內間歇地生成來自電漿槍7的電漿P。例如,控制部50以既定間隔切換短路開關SW1的ON/OFF狀態,藉此在生成室10b內間歇地生成來自電漿槍7的電漿P。 當短路開關SW1呈OFF狀態時(圖1的狀態),來自電漿槍7的電漿P被出射到生成室10b內,因此在生成室10b內生成電漿P。電漿P將中性粒子、正離子、負離子(當存在氧氣等負性氣體時)及電子作為構成物質。因此,在生成室10b內生成電子。當短路開關SW1呈ON狀態時(圖2的狀態),由於來自電漿槍7的電漿P不會出射到生成室10b內,因此生成室10b內的電漿P的電子溫度急劇下降。因此,電子容易附著於供給到生成室10b內之氣體的粒子。藉此,在生成室10b內有效地生成負離子。 控制部50控制基於電壓施加部90之電壓的施加。控制部50在既定時序(例如,停止電漿P之時序)藉由電壓施加部90施加電壓。另外,藉由控制部50預先設定開始基於電壓施加部90的電壓的施加之時序。藉由電壓施加部90對化合物半導體11賦予正的偏壓,從而真空腔室10內的負離子被引導至化合物半導體11。藉此,負離子照射到化合物半導體。 在此,對化合物半導體11與負離子之間的關係進行說明。化合物半導體11由陽離子(Cation)和陰離子(Anion)形成。相對於該種化合物半導體11照射包含與形成該化合物半導體11之陰離子相同的元素之負離子。又,藉由氣體供給部40供給之氣體包含與形成化合物半導體11之陰離子相同的元素。另外,氣體還包含Ar等稀有氣體。 例如,化合物半導體11由ZnO、Ga 2O 3等形成時,照射O -等負離子。氣體供給部40的氣體包含O 2等。化合物半導體11由AlN、GaN等形成時,照射NH -等氮化物的負離子。另外,所注入之H藉由退火被去除。氣體供給部40的氣體包含NH 2、NH 4等。此外,化合物半導體11由SiC等形成時,照射C -、Si -等負離子。氣體供給部40的氣體包含C 2H 6、SiH 4等。 另外,化合物半導體11為SiC時,Si亦能夠作為負離子,因此陽離子側亦能夠作為負離子進行照射。 另外,電子親和力容易成為正的原子,分子容易成為負離子。因此,當該種原子、分子的陰離子包含於化合物半導體11時,可以照射包含相同原子、分子之負離子。例如,作為容易負離子化者,可列舉H、He、C、O、F、Si、S、Cl、Br、I、H 2、O 2、Cl 2、Br 2、I 2、CH、OH、CN、HCl、HBr、NH 2、N 2O、NO 2、CCl 4、SF 6等。 接著,參閱圖3,對負離子照射裝置1的控制方法進行說明。圖3係表示本實施形態之負離子照射裝置1的控制方法之流程圖。另外,在此,化合物半導體11由ZnO形成,以照射O -的負離子之情況為例進行說明。 如圖3所示,負離子照射裝置1的控制方法包括氣體供給製程S10、電漿生成製程S20(負離子照射製程的一部分)及電壓施加製程S30(負離子照射製程的一部分)。各製程由控制部50執行。 首先,控制部50的氣體供給控制部51控制氣體供給部40而向真空腔室10內供給氣體(氣體供給製程S10)。藉此,成為在真空腔室10的生成室10b內存在O 2的氣體之狀態。然後,執行電漿生成製程S20。 控制部50的電漿控制部52藉由控制電漿生成部14而在真空腔室10內生成電漿P及電子,並且,藉由停止電漿P的生成,由電子和氣體生成負離子(電漿生成製程S20)。若在真空腔室10的生成室10b內生成電漿P及電子,則藉由電漿P進行“O 2+e -→2O+e -”之反應。然後,若停止電漿P的生成,則在生成室10b內,電子溫度急劇降低,從而進行“O+e -→O -”之反應。在執行電漿生成製程S20之後的既定時序執行電壓施加製程S30。另外,嚴格來講,在電漿生成期間亦生成負離子,且照射負離子時,還照射電漿生成時所生成之負離子。 控制部50的電壓控制部53控制電壓施加部90並對化合物半導體11施加偏壓(電壓施加製程S30)。藉此,生成室10b內的O -的負離子81朝向化合物半導體11側,並且照射到該化合物半導體11(參閱圖2及圖4)。 接著,對本實施形態之負離子照射裝置1及其控制方法的作用·效果進行說明。 在本實施形態之負離子照射裝置1中,控制部50控制氣體供給部40而向真空腔室10內供給氣體。氣體供給部40供給包含與形成化合物半導體11之離子相同的元素之氣體。因此,在真空腔室10內存在與形成化合物半導體11之離子相同的元素。進而,控制部50藉由控制電漿生成部14而在真空腔室10內生成電漿P及電子,並且,藉由停止電漿P的生成,由電子和氣體生成負離子,並將該負離子照射到化合物半導體11上。 例如,如圖4(a)所示,與形成化合物半導體11之離子相同的元素的負離子81被照射到化合物半導體11。負離子81從化合物半導體11的表面11a進入內部。藉此,負離子81進入化合物半導體11內的來自陰離子之結晶缺陷85,從而如圖4(b)所示,能夠填補該結晶缺陷85。 在此,參閱圖5及圖6,對相對於化合物半導體11照射負離子的優點進行說明。在圖5及圖6中,示出形成化合物半導體11之陽離子86及陰離子87的離子鍵結構造。圖5係作為比較例,示意地表示對化合物半導體注入正離子83時的樣子之圖。如圖5所示,若對化合物半導體11注入正離子83,則存在正離子83必須在陽離子86與陰離子87的庫侖力的影響中通過,因此難以平滑地進入化合物半導體11內部之問題。又,若藉由正離子83的注入而產生作為二次電子的電子82的釋放,則導致基板進行充電之問題。 相對於此,若朝向化合物半導體11之負離子81(參閱圖6(a))到達該化合物半導體11,則如圖6(b)所示,藉由碰撞電子82容易脫離。因此,負離子81作為電子82已脫離之中性狀態的粒子81a進入到離子鍵結之中。中性狀態的粒子81a不受陽離子86與陰離子87的庫侖力的影響而能夠平滑地進入化合物半導體11內部。因此,負離子81的能量可以為例如70eV以下的低能量。又,當注入負離子81時,亦不會產生基板的充電。另外,負離子81被注入到藉由加熱部30(參閱圖1)已加熱之狀態的化合物半導體11。因此,所期望的元素藉由濃度擴散而進入化合物半導體11的深處,又,藉由熱處理去除多餘的元素,因此粒子81a能夠只填補結晶缺陷。 此外,例如,作為比較例,在使用負離子源照射負離子時,能夠照射負離子之面積較小。另一方面,如本實施形態般,具備電漿生成部14之負離子照射裝置1能夠對化合物半導體11大面積地照射負離子。 此外,例如,作為比較例,當僅照射單一能量的負離子時,負離子只進入化合物半導體11的既定深度位置,因此不能夠在深度方向的廣範圍內填補結晶缺陷。另一方面,根據本實施形態之負離子照射裝置1,由於能夠生成能量範圍寬的的負離子,因此能夠在深度方向的廣範圍內填補結晶缺陷。 如上所述,本實施形態之負離子照射裝置1能夠填補化合物半導體11的結晶缺陷,因此能夠提高化合物半導體11的品質。又,在負離子照射前,即使作為化合物半導體11的等級不充分之情況下,亦能夠藉由負離子照射提高品質,因此能夠減少預先篩選單晶基板的等級的必要性。藉由以上,能夠提高化合物半導體的製造效率及品質。 本實施形態之負離子照射裝置1的控制方法包括:氣體供給製程S10,控制氣體供給部40而向真空腔室10內供給氣體;負離子照射製程(電漿生成製程S20、電壓施加製程S30),控制電漿生成部14,在真空腔室10內生成電漿P及電子,並且,藉由停止電漿P的生成,由電子和氣體生成負離子,並將該負離子照射到化合物半導體11。 藉由本實施形態之負離子照射裝置1的控制方法,能夠獲得與上述負離子照射裝置1相同宗旨的作用·效果。 以上,對本實施形態的一實施形態進行了說明,但本發明並不限定於上述實施形態,可以在不改變各申請專利範圍所記載之宗旨之範圍內進行變形或應用於其他實施形態中。 又,在上述實施形態中,對還具備作為離子電鍍型的成膜裝置的功能之負離子照射裝置進行了說明,但是,負離子照射裝置亦可以不具有成膜裝置的功能。因此,電漿P可以被引導至例如與電漿槍對置之壁部的電極等中。 例如,在上述實施形態中,將電漿槍7設為壓力梯度型的電漿槍,但是只要能夠在真空腔室10內生成電漿即可,則電漿槍7並不限於壓力梯度型的電漿槍。 又,在上述實施形態中,電漿槍7與引導電漿P之位置(爐缸機構2)的組在真空腔室10內僅設置有一組,但亦可設置複數組。又,對於一個位置,可以從複數個電漿槍7供給電漿P。 Hereinafter, a negative ion irradiation device according to an embodiment of the present invention will be described with reference to the attached drawings. In addition, in the drawings, the same reference numerals are attached to the same elements, and overlapping explanations are omitted. First, referring to FIG. 1 and FIG. 2, the structure of the negative ion irradiation apparatus which concerns on embodiment of this invention is demonstrated. 1 and 2 are schematic cross-sectional views showing the configuration of a negative ion irradiation device according to this embodiment. FIG. 1 shows the state of operation when plasma is generated, and FIG. 2 shows the state of operation when plasma is stopped. As shown in FIG. 1 and FIG. 2, the negative ion irradiation apparatus 1 of this embodiment is a device which applies the film-forming technology used for the so-called ion plating method to negative ion irradiation. In addition, for convenience of explanation, an XYZ coordinate system is shown in FIGS. 1 and 2 . The Y-axis direction is the direction in which the compound semiconductor will be described later. The X-axis direction is the thickness direction of the compound semiconductor. The Z-axis direction is a direction perpendicular to the Y-axis direction and the X-axis direction. The anion irradiation apparatus 1 may be a so-called horizontal anion irradiation apparatus in which the compound semiconductor 11 is arranged and transported in the vacuum chamber 10 so that the thickness direction of the compound semiconductor 11 becomes substantially vertical. At this time, the Z-axis and Y-axis directions are horizontal directions, and the X-axis direction is a vertical direction and a plate thickness direction. In addition, the negative ion irradiation device 1 may also be a so-called vertical negative ion irradiation device in which the compound semiconductor 11 is placed in a horizontal direction (X-axis direction in FIGS. 1 and 2 ) so that the thickness direction of the compound semiconductor 11 The compound semiconductor 11 is arranged and transported in the vacuum chamber 10 in a state where the semiconductor 11 is erected or tilted from the erected state. At this time, the X-axis direction is the horizontal direction, the thickness direction of the compound semiconductor 11 is the plate thickness direction, the Y-axis direction is the horizontal direction, and the Z-axis direction is the vertical direction. An anion irradiation device according to an embodiment of the present invention will be described below by taking a horizontal anion irradiation device as an example. The negative ion irradiation device 1 includes a vacuum chamber 10 , a transport mechanism (disposition unit) 3 , a plasma generation unit 14 , a gas supply unit 40 , a circuit unit 34 , a voltage application unit 90 , and a control unit 50 . The vacuum chamber 10 is a member for accommodating the compound semiconductor 11 and performing a film-forming process. The vacuum chamber 10 has a transport chamber 10a for transporting the compound semiconductor 11, a generation chamber 10b for generating negative ions, and a plasma port for receiving the plasma P irradiated in the form of a beam from the plasma gun 7 into the vacuum chamber 10. 10c. The transport chamber 10a, the generation chamber 10b, and the plasma port 10c communicate with each other. The transport chamber 10a is set along a predetermined transport direction (arrow A in the figure) (along the Y axis). Also, the vacuum chamber 10 is made of a conductive material and is connected to a ground potential. A heating unit 30 for heating the compound semiconductor 11 is provided in the transfer chamber 10a. The heating unit 30 is provided on the upstream side in the conveyance direction from the communicating portion with the production chamber 10b in the conveyance chamber 10a. Therefore, negative ions from the generation chamber 10b are irradiated to the compound semiconductor 11 in a heated state. The production chamber 10b has, as a wall portion 10W, a pair of side walls along the conveyance direction (arrow A), a pair of sidewalls 10h, 10i along a direction (Z-axis direction) intersecting the conveyance direction (arrow A), and a pair of sidewalls 10i along the X-axis. Bottom wall 10j arranged in cross direction. The transport mechanism 3 transports the compound semiconductor holding member 16 holding the compound semiconductor 11 in a state facing the production chamber 10b in the transport direction (arrow A). The transport mechanism 3 functions as a disposing unit for disposing the compound semiconductor 11 . For example, the compound semiconductor holding member 16 is a frame holding the outer peripheral edge of the compound semiconductor 11 . The transport mechanism 3 is composed of a plurality of transport rollers 15 installed in the transport chamber 10a. The conveyance rollers 15 are arranged at equal intervals along the conveyance direction (arrow A), and convey along the conveyance direction (arrow A) while supporting the compound semiconductor holding member 16 . In addition, the compound semiconductor 11 is a plate-shaped substrate. The material and the like of the compound semiconductor 11 will be described later. Next, the configuration of the plasma generation unit 14 will be described in detail. The plasma generator 14 generates plasma and electrons in the vacuum chamber 10 . The plasma generator 14 has a plasma gun 7 , a steering coil 5 , and a hearth mechanism 2 . The plasma gun 7 is, for example, a pressure gradient type plasma gun, and its main body is connected to the generation chamber 10b through a plasma port 10c provided on the side wall of the generation chamber 10b. The plasma gun 7 generates plasma P in the vacuum chamber 10 . The plasma P generated in the plasma gun 7 is emitted into the generation chamber 10b from the plasma port 10c in the form of a beam. Thereby, plasma P is generated in the generation chamber 10b. One end of the plasma gun 7 is closed by a cathode 60 . A first intermediate electrode (grid) 61 and a second intermediate electrode (grid) 62 are arranged concentrically between the cathode 60 and the plasma port 10c. A ring-shaped permanent magnet 61 a for converging the plasma P is built in the first intermediate electrode 61 . An electromagnet coil 62 a is also built in the second intermediate electrode 62 for converging the plasma P. When the plasma gun 7 generates negative ions, the plasma P is generated intermittently in the generation chamber 10b. Specifically, the plasma gun 7 is controlled by the control unit 50 described later so that the plasma P is generated intermittently in the generation chamber 10 b. This control will be described in detail in the description of the control unit 50 . The steering coil 5 is arranged around the plasma port 10c where the plasma gun is installed. The steering coil 5 guides the plasma P into the generation chamber 10b. The steering coil 5 is excited by a steering coil power supply (not shown). The hearth mechanism 2 is a mechanism for guiding the plasma P from the plasma gun to a desired position. The hearth mechanism 2 has a main hearth 17 and a ring hearth 6 . When film formation is performed using the negative ion irradiation device 1 , the main furnace 17 functions as an anode for holding film formation materials. However, when generating negative ions, the plasma is guided to the ring hearth 6 so that the plasma P is not guided to the film-forming material. Therefore, when the negative ion irradiation device 1 performs only negative ion irradiation without film formation, the film formation material need not be held by the main hearth 17 . Alternatively, the hearth mechanism 2 may be configured to guide only the plasma P. The ring hearth 6 is the anode with electromagnets for inducing the plasma P. The ring hearth 6 is disposed around the filling portion 17 a of the main hearth 17 . The ring hearth 6 has an annular coil 9 , an annular permanent magnet portion 20 , and an annular container 12 , and the coil 9 and the permanent magnet portion 20 are accommodated in the container 12 . In this embodiment, the coil 9 and the permanent magnet portion 20 are sequentially provided in the X-axis negative direction when viewed from the conveying mechanism 3 , but the permanent magnet portion 20 and the coil 9 may be sequentially provided in the X-axis negative direction. The gas supply unit 40 is arranged outside the vacuum chamber 10 . The gas supply part 40 supplies gas into the vacuum chamber 10 through the gas supply port 41 provided in the side wall (for example, side wall 10h) of the generation chamber 10b. Specific examples of the gas will be described later. The position of the gas supply port 41 is preferably a position near the boundary between the generation chamber 10b and the transfer chamber 10a. At this time, since the gas from the gas supply unit 40 can be supplied to the vicinity of the boundary between the generation chamber 10b and the transfer chamber 10a, negative ions to be described later are generated near the boundary. Therefore, the generated negative ions can be suitably implanted into the compound semiconductor 11 in the transport chamber 10a. In addition, the position of the gas supply port 41 is not limited to the vicinity of the boundary between the generation chamber 10b and the transfer chamber 10a. The circuit unit 34 has a variable power supply 80 , a first wiring 71 , a second wiring 72 , resistors R1 to R4 , and short-circuit switches SW1 and SW2 . The variable power supply 80 sandwiches the vacuum chamber 10 at the ground potential, applies a negative voltage to the cathode 60 of the plasma gun 7 , and applies a positive voltage to the main furnace 17 of the furnace mechanism 2 . Thereby, the variable power supply 80 generates a potential difference between the cathode 60 of the plasma gun 7 and the main well 17 of the well mechanism 2 . The first wiring 71 electrically connects the cathode 60 of the plasma gun 7 and the negative potential side of the variable power supply 80 . The second wiring 72 electrically connects the main well 17 (anode) of the well mechanism 2 and the positive potential side of the variable power supply 80 . One end of the resistor R1 is electrically connected to the first intermediate electrode 61 of the plasma gun 7 , and the other end is electrically connected to the variable power source 80 via the second wiring 72 . That is, the resistor R1 is connected in series between the first intermediate electrode 61 and the variable power source 80 . One end of the resistor R2 is electrically connected to the second intermediate electrode 62 of the plasma gun 7 , and the other end is electrically connected to the variable power source 80 via the second wiring 72 . That is, the resistor R2 is connected in series between the second intermediate electrode 62 and the variable power source 80 . One end of the resistor R3 is electrically connected to the wall portion 10W of the production chamber 10 b, and the other end is electrically connected to the variable power supply 80 via the second wiring 72 . That is, the resistor R3 is connected in series between the wall portion 10W of the generation chamber 10b and the variable power supply 80 . One end of the resistor R4 is electrically connected to the ring hearth 6 , and the other end is electrically connected to the variable power supply 80 via the second wiring 72 . That is, the resistor R4 is connected in series between the ring hearth 6 and the variable power supply 80 . The short-circuit switches SW1 and SW2 are switching parts that are switched to an ON/OFF (opened/closed) state by receiving a command signal from the control part 50, respectively. The short-circuit switch SW1 is connected in parallel with the resistor R2. The short-circuit switch SW1 is in an OFF state when plasma P is generated. Thereby, since the second intermediate electrode 62 and the variable power source 80 are electrically connected to each other via the resistor R2 , current hardly flows between the second intermediate electrode 62 and the variable power source 80 . As a result, the plasma P from the plasma gun 7 is emitted into the vacuum chamber 10 . In addition, when the plasma P from the plasma gun 7 is emitted into the vacuum chamber 10 , instead of making it difficult for the current to flow to the second intermediate electrode 62 , it is possible to make it difficult for the current to flow to the first intermediate electrode 61 . At this time, the short-circuit switch SW1 is not connected to the second intermediate electrode 62 side but is connected to the first intermediate electrode 61 side. On the other hand, when the plasma P is stopped, the short-circuit switch SW1 is turned ON. As a result, the electrical connection between the second intermediate electrode 62 and the variable power source 80 is short-circuited, so that a current flows between the second intermediate electrode 62 and the variable power source 80 . That is, a short-circuit current flows to the plasma gun 7 . As a result, the plasma P from the plasma gun 7 is not emitted into the vacuum chamber 10 . When negative ions are generated, the ON/OFF state of the short-circuit switch SW1 is switched by the control unit 50 at predetermined intervals, whereby the plasma P from the plasma gun 7 is intermittently generated in the vacuum chamber 10 . That is, the short-circuit switch SW1 is a switching unit for switching supply and cutoff of the plasma P in the vacuum chamber 10 . The short-circuit switch SW2 is connected in parallel with the resistor R4. The ON/OFF state of the short circuit switch SW2 is switched by the control unit 50 depending on whether the plasma P is guided to the main well 17 side or to the ring well 6 side. When the short-circuit switch SW2 is in the ON state, since the electrical connection between the ring well 6 and the variable power supply 80 is short-circuited, current flows more easily to the ring well 6 than to the main well 17 . Thereby, the plasma P is easily guided to the ring hearth 6 . On the other hand, if the short-circuit switch SW2 is in the OFF state, the ring hearth 6 is electrically connected to the variable power supply 80 via the resistor R4. Therefore, compared with the ring hearth 6, the current flows to the main hearth 17 more easily, so that the plasma P is easily guided to the main hearth 17 side. In addition, when negative ions are generated, the short-circuit switch SW2 is kept in the ON state. When the negative ion irradiation device 1 is not performing film formation, the short-circuit switch SW2 may be kept in the ON state. The voltage applying unit 90 can apply a positive voltage to the formed compound semiconductor (object) 11 . The voltage application unit 90 includes a bias circuit 35 and trolley wires 18 . The bias circuit 35 is a circuit for applying a positive bias to the formed compound semiconductor 11 . The bias circuit 35 has a bias power supply 27 for applying a positive bias voltage (hereinafter referred to simply as "bias") to the compound semiconductor 11, a third wiring 73 electrically connecting the bias power supply 27 and the trolley wire 18, and a third wiring 73 provided on the first wiring. 3 The short-circuit switch SW3 of the wiring 73. The bias power supply 27 applies a voltage signal (periodic electric signal) that is a rectangular wave that increases or decreases periodically as a bias voltage. The bias power supply 27 is configured to be able to change the frequency of the applied bias voltage under the control of the control unit 50 . One end of the third wiring 73 is connected to the positive potential side of the bias power supply 27 , and the other end is connected to the trolley wire 18 . Thereby, the third wiring 73 electrically connects the trolley wire 18 and the bias power supply 27 . The short-circuit switch SW3 is connected in series between the trolley wire 18 and the positive potential side of the bias power supply 27 via the third wiring 73 . The short-circuit switch SW3 is a switching section for switching whether or not a bias voltage is applied to the trolley wire 18 . The ON/OFF state of the short-circuit switch SW3 is switched by the control unit 50 . The short-circuit switch SW3 is turned ON at a predetermined timing when negative ions are generated. When the short-circuit switch SW3 is in the ON state, the trolley wire 18 and the positive potential side of the bias power supply 27 are electrically connected to each other, and a bias voltage is applied to the trolley wire 18 . On the other hand, the short-circuit switch SW3 is in an OFF state at a predetermined timing when negative ions are generated. When the short-circuit switch SW3 is in the OFF state, the trolley wire 18 and the bias power supply 27 are electrically disconnected from each other, and no bias is applied to the trolley wire 18 . The trolley wire 18 is a wire for supplying power to the compound semiconductor holding member 16 . The trolley wire 18 is extended in the conveyance direction (arrow A) in the conveyance chamber 10a, and is provided. The sliding wire 18 supplies power to the compound semiconductor holding member 16 through the power supply brush 42 by coming into contact with the power supply brush 42 provided on the compound semiconductor holding member 16 . The trolley wire 18 is made of, for example, a stainless steel wire or the like. The control unit 50 is a device that controls the negative ion irradiation device 1 as a whole, and includes an ECU [Electronic Control Unit] that manages the whole device. ECU has CPU[Central Processing Unit: Central Processing Unit], ROM[Read Only Memory: Read Only Memory], RAM[Random Access Memory: Random Access Memory], CAN[Controller Area Network: Controller Area Network ]Electronic control units for communication circuits, etc. In the ECU, for example, various functions are realized by loading programs stored in ROM into RAM, and executing the programs loaded into RAM by CPU. An ECU may consist of a plurality of electronic units. The control unit 50 is disposed outside the vacuum chamber 10 . Furthermore, the control unit 50 includes a gas supply control unit 51 for controlling the gas supply by the gas supply unit 40, a plasma control unit 52 for controlling the generation of plasma P by the plasma generation unit 14, and a voltage control unit 90 for controlling the voltage. The applied voltage control part 53. The gas supply control unit 51 controls the gas supply unit 40 to supply gas into the generation chamber 10b. Next, the plasma control unit 52 of the control unit 50 controls the plasma generation unit 14 to intermittently generate the plasma P from the plasma gun 7 in the generation chamber 10 b. For example, the control unit 50 switches the ON/OFF state of the short-circuit switch SW1 at predetermined intervals, whereby the plasma P from the plasma gun 7 is intermittently generated in the generation chamber 10 b. When the short-circuit switch SW1 is OFF (the state of FIG. 1 ), the plasma P from the plasma gun 7 is emitted into the generation chamber 10b, so that the plasma P is generated in the generation chamber 10b. Plasma P has neutral particles, positive ions, negative ions (when there is a negative gas such as oxygen) and electrons as constituent substances. Accordingly, electrons are generated in the generation chamber 10b. When the short-circuit switch SW1 is ON (the state in FIG. 2 ), since the plasma P from the plasma gun 7 is not emitted into the generation chamber 10b, the electron temperature of the plasma P in the generation chamber 10b drops sharply. Therefore, electrons tend to attach to the particles of the gas supplied into the generation chamber 10b. Thereby, negative ions are efficiently generated in the generation chamber 10b. The control unit 50 controls the application of the voltage by the voltage application unit 90 . The control unit 50 applies a voltage through the voltage applying unit 90 at a predetermined timing (for example, timing of stopping the plasma P). In addition, the timing at which the application of the voltage by the voltage application unit 90 is started is set in advance by the control unit 50 . When a positive bias is applied to the compound semiconductor 11 by the voltage applying unit 90 , negative ions in the vacuum chamber 10 are guided to the compound semiconductor 11 . Thereby, negative ions are irradiated to the compound semiconductor. Here, the relationship between the compound semiconductor 11 and negative ions will be described. The compound semiconductor 11 is formed of cations (Cations) and anions (Anions). The compound semiconductor 11 is irradiated with negative ions containing the same element as the anion forming the compound semiconductor 11 . Also, the gas supplied by the gas supply unit 40 contains the same element as the anion forming the compound semiconductor 11 . In addition, the gas also contains rare gases such as Ar. For example, when the compound semiconductor 11 is formed of ZnO, Ga 2 O 3 or the like, negative ions such as O are irradiated. The gas of the gas supply unit 40 contains O 2 and the like. When the compound semiconductor 11 is formed of AlN, GaN, etc., negative ions of nitride such as NH - are irradiated. In addition, the implanted H is removed by annealing. The gas in the gas supply unit 40 contains NH 2 , NH 4 , and the like. In addition, when the compound semiconductor 11 is formed of SiC or the like, negative ions such as C , Si −, etc. are irradiated. The gas in the gas supply unit 40 contains C 2 H 6 , SiH 4 , and the like. In addition, when the compound semiconductor 11 is SiC, Si can also serve as negative ions, so the cation side can also be irradiated as negative ions. In addition, electron affinity tends to become positive atoms, and molecules tend to become negative ions. Therefore, when the anions of such atoms and molecules are contained in the compound semiconductor 11, negative ions containing the same atoms and molecules can be irradiated. For example, those that are easily negatively ionized include H, He, C, O, F, Si, S, Cl, Br, I, H 2 , O 2 , Cl 2 , Br 2 , I 2 , CH, OH, CN , HCl, HBr, NH 2 , N 2 O, NO 2 , CCl 4 , SF 6 etc. Next, referring to FIG. 3 , a method of controlling the negative ion irradiation device 1 will be described. Fig. 3 is a flow chart showing the control method of the negative ion irradiation device 1 of the present embodiment. In addition, here, the compound semiconductor 11 is formed of ZnO, and the case where negative ions of O are irradiated will be described as an example. As shown in FIG. 3 , the control method of the negative ion irradiation device 1 includes a gas supply process S10, a plasma generation process S20 (a part of the negative ion irradiation process), and a voltage application process S30 (a part of the negative ion irradiation process). Each process is executed by the control unit 50 . First, the gas supply control unit 51 of the control unit 50 controls the gas supply unit 40 to supply gas into the vacuum chamber 10 (gas supply process S10 ). As a result, the gas of O 2 is present in the generation chamber 10 b of the vacuum chamber 10 . Then, a plasma generation process S20 is performed. The plasma control unit 52 of the control unit 50 generates plasma P and electrons in the vacuum chamber 10 by controlling the plasma generation unit 14, and by stopping the generation of the plasma P, negative ions (electrons) are generated from the electrons and the gas. Pulp generation process S20). When plasma P and electrons are generated in the generation chamber 10 b of the vacuum chamber 10 , a reaction of “O 2 +e →2O+e ” proceeds by the plasma P. Then, when the generation of the plasma P is stopped, the temperature of the electrons in the generation chamber 10b drops sharply, and a reaction of "O+e - →O - " proceeds. The voltage application process S30 is performed at a predetermined timing after the plasma generation process S20 is performed. In addition, strictly speaking, negative ions are also generated during plasma generation, and when negative ions are irradiated, negative ions generated during plasma generation are also irradiated. The voltage control unit 53 of the control unit 50 controls the voltage application unit 90 and applies a bias voltage to the compound semiconductor 11 (voltage application process S30 ). Thereby, the negative ions 81 of O in the generation chamber 10 b are directed toward the compound semiconductor 11 side, and are irradiated to the compound semiconductor 11 (see FIGS. 2 and 4 ). Next, the operation and effect of the negative ion irradiation device 1 and its control method of the present embodiment will be described. In the negative ion irradiation apparatus 1 of the present embodiment, the control unit 50 controls the gas supply unit 40 to supply gas into the vacuum chamber 10 . The gas supply unit 40 supplies a gas containing the same element as the ions forming the compound semiconductor 11 . Therefore, the same elements as ions forming the compound semiconductor 11 exist in the vacuum chamber 10 . Furthermore, the control unit 50 generates plasma P and electrons in the vacuum chamber 10 by controlling the plasma generation unit 14, and by stopping the generation of the plasma P, negative ions are generated from the electrons and the gas, and the negative ions are irradiated. to the compound semiconductor 11. For example, as shown in FIG. 4( a ), negative ions 81 of the same element as ions forming the compound semiconductor 11 are irradiated to the compound semiconductor 11 . Negative ions 81 enter inside from the surface 11 a of the compound semiconductor 11 . Thereby, the negative ions 81 enter into the crystal defect 85 derived from the anion in the compound semiconductor 11, and as shown in FIG. 4(b), the crystal defect 85 can be filled. Here, the advantages of irradiating the compound semiconductor 11 with negative ions will be described with reference to FIGS. 5 and 6 . 5 and 6 show the ionic bond structure of cations 86 and anions 87 forming the compound semiconductor 11 . FIG. 5 is a diagram schematically showing a state when positive ions 83 are implanted into a compound semiconductor as a comparative example. As shown in FIG. 5 , when positive ions 83 are implanted into the compound semiconductor 11 , the positive ions 83 must pass under the influence of the Coulomb force of the cations 86 and anions 87 , making it difficult to smoothly enter the compound semiconductor 11 . In addition, if electrons 82 as secondary electrons are released by the injection of positive ions 83 , there will be a problem that the substrate is charged. On the other hand, when negative ions 81 (see FIG. 6( a )) directed toward the compound semiconductor 11 reach the compound semiconductor 11 , as shown in FIG. 6( b ), they are easily detached by colliding electrons 82 . Therefore, negative ions 81 enter into ionic bonds as particles 81a in which electrons 82 have left the neutral state. The particles 81 a in the neutral state can smoothly enter the interior of the compound semiconductor 11 without being affected by the Coulomb force of the cations 86 and the anions 87 . Therefore, the energy of negative ions 81 may be as low as 70 eV or less, for example. Also, when the negative ions 81 are injected, the substrate will not be charged. In addition, negative ions 81 are implanted into the compound semiconductor 11 in a state heated by the heating unit 30 (see FIG. 1 ). Therefore, the desired element is penetrated deep into the compound semiconductor 11 by concentration diffusion, and the excess element is removed by heat treatment, so that the particles 81a can fill only crystal defects. In addition, for example, as a comparative example, when negative ions are irradiated using a negative ion source, the area that can be irradiated with negative ions is small. On the other hand, the negative ion irradiation device 1 including the plasma generation unit 14 can irradiate the compound semiconductor 11 with negative ions over a large area as in the present embodiment. In addition, for example, as a comparative example, when only negative ions of a single energy are irradiated, the negative ions enter only a predetermined depth position of the compound semiconductor 11, and therefore crystal defects cannot be filled in a wide range in the depth direction. On the other hand, according to the negative ion irradiation device 1 of the present embodiment, since negative ions having a wide energy range can be generated, crystal defects can be filled in a wide range in the depth direction. As described above, the negative ion irradiation device 1 according to the present embodiment can fill the crystal defects of the compound semiconductor 11, so that the quality of the compound semiconductor 11 can be improved. Also, even if the grade of the compound semiconductor 11 is not sufficient before negative ion irradiation, the quality can be improved by negative ion irradiation, so the necessity of screening the grade of the single crystal substrate in advance can be reduced. Through the above, the production efficiency and quality of compound semiconductors can be improved. The control method of the negative ion irradiation device 1 of the present embodiment includes: gas supply process S10, controlling the gas supply part 40 to supply gas into the vacuum chamber 10; negative ion irradiation process (plasma generation process S20, voltage application process S30), controlling The plasma generation unit 14 generates plasma P and electrons in the vacuum chamber 10 , stops generation of the plasma P, generates negative ions from the electrons and gas, and irradiates the compound semiconductor 11 with the negative ions. By the control method of the negative ion irradiation device 1 of the present embodiment, the same functions and effects as those of the above-mentioned negative ion irradiation device 1 can be obtained. One embodiment of the present embodiment has been described above, but the present invention is not limited to the above-mentioned embodiment, and can be modified or applied to other embodiments without changing the gist described in each claim. In addition, in the above-mentioned embodiment, the negative ion irradiation device also has the function as the ion plating type film formation device has been described, however, the negative ion irradiation device may not have the function of the film formation device. Thus, the plasma P can be guided, for example, into an electrode or the like of a wall portion opposite to the plasma gun. For example, in the above-mentioned embodiment, the plasma gun 7 is set as a pressure gradient type plasma gun, but as long as the plasma can be generated in the vacuum chamber 10, the plasma gun 7 is not limited to the pressure gradient type. plasma gun. In addition, in the above embodiment, only one set of the plasma gun 7 and the position for guiding the plasma P (heart mechanism 2 ) is provided in the vacuum chamber 10 , but plural sets may be provided. Also, plasma P may be supplied from a plurality of plasma guns 7 to one position.

1:負離子照射裝置(負離子照射裝置) 3:輸送機構(配置部) 7:電漿槍 10:真空腔室 11:化合物半導體 14:電漿生成部 40:氣體供給部 50:控制部 P:電漿 1: Negative ion irradiation device (negative ion irradiation device) 3: Conveying mechanism (configuration department) 7: Plasma Gun 10: Vacuum chamber 11: Compound semiconductor 14: Plasma Generation Department 40: Gas supply part 50: Control Department P: Plasma

[圖1]係表示本發明的實施形態之負離子照射裝置的構成之概略剖視圖,且係表示電漿生成時的動作狀態之圖。 [圖2]係表示圖1的負離子照射裝置的構成之概略剖視圖,且係表示電漿停止時的動作狀態之圖。 [圖3]係表示本實施形態之負離子照射裝置的控制方法之流程圖。 [圖4]係示意地表示負離子被照射到化合物半導體時的樣子之圖。 [圖5]係作為比較例,示意地表示對化合物半導體注入正離子時的樣子之圖。 [圖6]係示意地表示對化合物半導體注入負離子時的樣子之圖。 [ Fig. 1 ] is a schematic cross-sectional view showing the structure of a negative ion irradiation device according to an embodiment of the present invention, and is a diagram showing an operating state when plasma is generated. [ Fig. 2 ] is a schematic cross-sectional view showing the structure of the negative ion irradiation device in Fig. 1 , and is a diagram showing the operating state when the plasma is stopped. [FIG. 3] It is a flow chart which shows the control method of the negative ion irradiation apparatus of this embodiment. [ Fig. 4 ] is a diagram schematically showing how a compound semiconductor is irradiated with negative ions. [ Fig. 5 ] is a diagram schematically showing the state when positive ions are implanted into a compound semiconductor as a comparative example. [ Fig. 6 ] is a diagram schematically showing a state when negative ions are implanted into a compound semiconductor.

1:負離子照射裝置 1: Negative ion irradiation device

2:爐缸機構 2: Hearth mechanism

3:輸送機構(配置部) 3: Conveying mechanism (configuration department)

5:轉向線圈 5: Steering coil

6:環爐缸 6: ring hearth

7:電漿槍 7: Plasma Gun

9:線圈 9: Coil

10:真空腔室 10: Vacuum chamber

10a:輸送室 10a: Transport chamber

10b:生成室 10b: Generation Room

10c:電漿口 10c: plasma port

10h(10W):側壁 10h(10W): side wall

10i(10W):側壁 10i(10W): side wall

10j(10W):底面壁 10j (10W): Bottom wall

11:化合物半導體 11: Compound semiconductor

12:容器 12: container

14:電漿生成部 14: Plasma Generation Department

15:輸送輥 15: Conveyor roller

16:化合物半導體保持構件 16: Compound semiconductor holding member

17:主爐缸 17: Main hearth

17a:填充部 17a: filling part

18(90):滑接線 18 (90): sliding wire

20:永久磁鐵部 20:Permanent magnet part

27:偏壓電源 27: Bias power supply

30:加熱部 30: heating part

34:電路部 34: Circuit Department

35(90):偏壓電路 35(90): Bias circuit

40:氣體供給部 40: Gas supply part

41:氣體供給口 41: Gas supply port

42:供電刷 42: Power supply brush

50:控制部 50: Control Department

51:氣體供給控制部 51: Gas supply control unit

52:電漿控制部 52: Plasma Control Department

53:電壓控制部 53:Voltage Control Department

60:陰極 60: Cathode

61:第1中間電極 61: 1st middle electrode

61a:環狀永久磁鐵 61a: ring permanent magnet

62:第2中間電極 62: The second middle electrode

62a:電磁體線圈 62a: Electromagnet coil

71:第1配線 71: 1st wiring

72:第2配線 72: 2nd wiring

73:第3配線 73: 3rd wiring

80:可變電源 80: variable power supply

A:箭頭 A: arrow

P:電漿 P: Plasma

R1:電阻器 R1: Resistor

R2:電阻器 R2: Resistor

R3:電阻器 R3: Resistor

R4:電阻器 R4: Resistor

SW1:短路開關 SW1: Short circuit switch

SW2:短路開關 SW2: Short circuit switch

SW3:短路開關 SW3: Short circuit switch

Claims (5)

一種負離子照射裝置,其向被照射體照射負離子,前述負離子照射裝置具備: 腔室,能夠配置前述被照射體; 氣體供給部,供給包含與形成前述被照射體之離子相同的元素之氣體;及 電漿生成部,在前述腔室內生成電漿及電子; 前述氣體供給部向前述腔室內供給前述氣體, 前述電漿生成部,係在前述腔室內生成前述電漿及前述電子,並且藉由停止前述電漿的生成,由前述電子和前述氣體生成前述負離子,並將該負離子照射到前述被照射體。 A negative ion irradiation device, which irradiates negative ions to an irradiated body, and the aforementioned negative ion irradiation device has: a chamber capable of disposing the aforementioned irradiated body; a gas supply unit that supplies a gas containing the same element as the ion forming the aforementioned irradiated body; and A plasma generation unit generates plasma and electrons in the chamber; The gas supply unit supplies the gas into the chamber, The plasma generation unit generates the plasma and the electrons in the chamber, stops generation of the plasma, generates the negative ions from the electrons and the gas, and irradiates the negative ions to the irradiated body. 如請求項1之負離子照射裝置,其中 前述被照射體,係在外部事先製造者。 Such as the negative ion irradiation device of claim 1, wherein The aforementioned object to be irradiated is manufactured externally in advance. 如請求項1或2之負離子照射裝置,其中 還具備:對前述被照射體賦予偏壓的電壓施加部。 Such as the negative ion irradiation device of claim 1 or 2, wherein A voltage application unit that applies a bias voltage to the irradiated body is further provided. 如請求項1至3之中任一項之負離子照射裝置,其中 前述被照射體為化合物半導體。 An anion irradiation device according to any one of claims 1 to 3, wherein The aforementioned object to be irradiated is a compound semiconductor. 一種向被照射體照射負離子之負離子照射裝置的控制方法,前述負離子照射裝置具備: 腔室,能夠配置前述被照射體; 氣體供給部,供給包含與形成前述被照射體之離子相同的元素之氣體;及 電漿生成部,在前述腔室內生成電漿及電子; 前述負離子照射裝置的控制方法包括: 氣體供給製程,藉由前述氣體供給部向前述腔室內供給前述氣體;及 負離子照射製程,藉由前述電漿生成部在前述腔室內生成前述電漿及前述電子,並且藉由停止前述電漿的生成,由前述電子和前述氣體生成前述負離子,並將該負離子照射到前述被照射體。 A method for controlling an anion irradiation device for irradiating an irradiated body with negative ions, wherein the anion irradiation device includes: a chamber capable of disposing the aforementioned irradiated body; a gas supply unit that supplies a gas containing the same element as the ion forming the aforementioned irradiated body; and A plasma generation unit generates plasma and electrons in the chamber; The control method of aforementioned negative ion irradiation device comprises: a gas supply process, supplying the aforementioned gas into the aforementioned chamber through the aforementioned gas supply unit; and In the negative ion irradiation process, the plasma and the electrons are generated in the chamber by the plasma generating unit, and by stopping the generation of the plasma, the negative ions are generated from the electrons and the gas, and the negative ions are irradiated onto the The irradiated body.
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