TWI868470B - Magnetron sputtering device - Google Patents
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- C23—COATING 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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- C23C14/35—Sputtering by application of a magnetic field, e.g. magnetron sputtering
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Abstract
Description
本申請涉及半導體製造技術領域,尤其涉及一種磁控濺射設備。The present application relates to the field of semiconductor manufacturing technology, and in particular to a magnetron sputtering device.
在半導體晶片的制程中,晶圓上需要構造出溝槽,並通過物理氣相沉積(Physical Vapor Deposition,簡稱PVD)製程在溝槽內沉積金屬線路,這些金屬線路可將電晶體等元件串連起來形成積體電路。在具體的沉積過程中,需要基於磁控濺射技術將靶材濺射出的粒子沉積至晶圓的溝槽中。In the process of manufacturing semiconductor chips, trenches need to be constructed on the wafer, and metal circuits are deposited in the trenches through the physical vapor deposition (PVD) process. These metal circuits can connect transistors and other components in series to form integrated circuits. In the specific deposition process, the particles sputtered from the target material need to be deposited into the trenches of the wafer based on magnetron sputtering technology.
但是,靶材濺射出的粒子是呈無規則的散射狀態,這些粒子難以對準落入溝槽實現沉積,進而表現出溝槽的開口被封堵、存在沉積空洞、粒子運動至晶圓之外等現象。However, the particles sputtered from the target are in an irregular scattered state. It is difficult for these particles to align and fall into the grooves for deposition, resulting in the blocking of the groove openings, the existence of deposition voids, and the movement of particles outside the wafer.
本申請公開一種磁控濺射設備,以優化靶材濺射出的粒子的沉積品質。This application discloses a magnetron sputtering device to optimize the deposition quality of particles sputtered from a target material.
為了解決上述問題,本申請採用下述技術方案:In order to solve the above problems, this application adopts the following technical solutions:
本申請提供一種磁控濺射設備,其包括:製程腔室;靶材,設置於該製程腔室內的頂部;承載基座,用於承載晶圓,該承載基座設置於該製程腔室內,且位於該靶材的下方;導向裝置,設置於該靶材與該承載基座之間,該導向裝置被配置為在該製程腔室內形成電場或磁場,該電場或磁場用於調整該靶材濺射出的粒子的運動軌跡,以使該粒子趨於垂直地沉積於該晶圓上。The present application provides a magnetron sputtering device, which includes: a process chamber; a target material, which is arranged at the top of the process chamber; a supporting base, which is used to support a wafer, and the supporting base is arranged in the process chamber and is located below the target material; a guiding device, which is arranged between the target material and the supporting base, and the guiding device is configured to form an electric field or a magnetic field in the process chamber, and the electric field or the magnetic field is used to adjust the movement trajectory of particles sputtered by the target material so that the particles tend to be deposited vertically on the wafer.
本申請採用的技術方案能夠達到以下有益效果:The technical solution adopted in this application can achieve the following beneficial effects:
在本申請實施的磁控濺射設備中,導向裝置能夠在製程腔室內形成電場或磁場,由電場或磁場產生電場力或磁場力來調節靶材濺射出的粒子的運動軌跡,使得粒子的運動軌跡相對於晶圓表面呈垂直關係,以使粒子能夠趨於垂直地沉積於晶圓上,這樣不僅增加了粒子落入晶圓的數量,減少了靶材的浪費,還使得粒子垂直落入至晶圓溝槽的底部,有效改善了粒子異常沉積而封堵溝槽開口以及存在沉積空洞的問題,最終達到提升粒子的沉積品質的效果。In the magnetron sputtering equipment implemented in the present application, the guiding device can form an electric field or a magnetic field in the process chamber, and the electric field or the magnetic field generates an electric field force or a magnetic field force to adjust the movement trajectory of the particles sputtered from the target material, so that the movement trajectory of the particles is perpendicular to the wafer surface, so that the particles tend to be deposited vertically on the wafer, which not only increases the number of particles falling into the wafer and reduces the waste of target materials, but also makes the particles fall vertically to the bottom of the wafer groove, effectively improving the problem of abnormal particle deposition and blocking the groove opening and the existence of deposition voids, and ultimately achieving the effect of improving the deposition quality of the particles.
以下揭露提供用於實施本揭露之不同構件之許多不同實施例或實例。下文描述組件及配置之特定實例以簡化本揭露。當然,此等僅為實例且非意欲限制。舉例而言,在以下描述中之一第一構件形成於一第二構件上方或上可包含其中該第一構件及該第二構件經形成為直接接觸之實施例,且亦可包含其中額外構件可形成在該第一構件與該第二構件之間,使得該第一構件及該第二構件可不直接接觸之實施例。另外,本揭露可在各個實例中重複參考數字及/或字母。此重複出於簡化及清楚之目的且本身不指示所論述之各個實施例及/或組態之間的關係。The following disclosure provides many different embodiments or examples for implementing the different components of the present disclosure. Specific examples of components and configurations are described below to simplify the present disclosure. Of course, these are only examples and are not intended to be limiting. For example, a first component formed above or on a second component in the following description may include an embodiment in which the first component and the second component are formed to be in direct contact, and may also include an embodiment in which an additional component may be formed between the first component and the second component so that the first component and the second component may not be in direct contact. In addition, the present disclosure may repeatedly refer to numbers and/or letters in each example. This repetition is for the purpose of simplification and clarity and does not itself indicate the relationship between the various embodiments and/or configurations discussed.
此外,為便於描述,諸如「下面」、「下方」、「下」、「上方」、「上」及類似者之空間相對術語可在本文中用於描述一個元件或構件與另一(些)元件或構件之關係,如圖中圖解說明。空間相對術語意欲涵蓋除在圖中描繪之定向以外之使用或操作中之裝置之不同定向。設備可以其他方式定向(旋轉90度或按其他定向)且因此可同樣解釋本文中使用之空間相對描述詞。Additionally, for ease of description, spatially relative terms such as "below," "beneath," "lower," "above," "upper," and the like may be used herein to describe the relationship of one element or component to another element or components as illustrated in the figures. Spatially relative terms are intended to encompass different orientations of the device in use or operation in addition to the orientation depicted in the figures. The device may be otherwise oriented (rotated 90 degrees or at other orientations) and the spatially relative descriptors used herein interpreted similarly.
儘管陳述本揭露之寬泛範疇之數值範圍及參數係近似值,然儘可能精確地報告特定實例中陳述之數值。然而,任何數值固有地含有必然由於見於各自測試量測中之標準偏差所致之某些誤差。再者,如本文中使用,術語「大約」通常意謂在一給定值或範圍之10%、5%、1%或0.5%內。替代地,術語「大約」意謂在由此項技術之一般技術者考量時處於平均值之一可接受標準誤差內。除在操作/工作實例中以外,或除非以其他方式明確指定,否則諸如針對本文中揭露之材料之數量、時間之持續時間、溫度、操作條件、數量之比率及其類似者之全部數值範圍、數量、值及百分比應被理解為在全部例項中由術語「大約」修飾。相應地,除非相反地指示,否則本揭露及隨附發明申請專利範圍中陳述之數值參數係可根據需要變化之近似值。至少,應至少鑑於所報告有效數位之數目且藉由應用普通捨入技術解釋各數值參數。範圍可在本文中表達為從一個端點至另一端點或在兩個端點之間。本文中揭露之全部範圍包含端點,除非另有指定。Although the numerical ranges and parameters setting forth the broad scope of the present disclosure are approximate, the numerical values set forth in the specific examples are reported as accurately as possible. However, any numerical value inherently contains certain errors necessarily due to the standard deviation found in the respective testing measurements. Furthermore, as used herein, the term "approximately" generally means within 10%, 5%, 1%, or 0.5% of a given value or range. Alternatively, the term "approximately" means within an acceptable standard error of the mean when considered by one of ordinary skill in the art. Except in the operating/working examples, or unless otherwise explicitly specified, all numerical ranges, quantities, values and percentages for the amount of materials disclosed herein, the duration of time, temperature, operating conditions, the ratio of quantities and the like should be understood as being modified by the term "approximately" in all instances. Accordingly, unless otherwise indicated, the numerical parameters set forth in the present disclosure and the accompanying invention claims are approximate values that may vary as needed. At least, each numerical parameter should be interpreted in view of the number of reported significant digits and by applying ordinary rounding techniques. Ranges may be expressed herein as from one end point to another or between two end points. All ranges disclosed herein include endpoints unless otherwise specified.
以下結合附圖,詳細說明本申請各個實施例公開的技術方案。The following is a detailed description of the technical solutions disclosed in each embodiment of this application in conjunction with the accompanying drawings.
為了優化靶材濺射出的粒子的沉積品質,本申請實施例提供一種磁控濺射設備。如圖1~圖9所示,本申請實施例的磁控濺射設備包括製程腔室100、靶材T、承載基座200和導向裝置400。In order to optimize the deposition quality of particles sputtered from the target material, the present application embodiment provides a magnetron sputtering device. As shown in FIG. 1 to FIG. 9 , the magnetron sputtering device of the present application embodiment includes a process chamber 100 , a target material T, a support base 200 and a guide device 400 .
其中,製程腔室100是該磁控濺射設備的基礎構件,其能夠作為部分其他構件的安裝基礎,且對設置於製程腔室100內的構件起到保護作用。製程腔室100內部具有製程空間,製程空間為晶圓W的處理提供特定的製程環境。The process chamber 100 is a basic component of the magnetron sputtering device, which can serve as a mounting base for some other components and protect the components disposed in the process chamber 100. The process chamber 100 has a process space inside, and the process space provides a specific process environment for processing the wafer W.
靶材T設置於製程腔室100的頂部,本申請實施例對靶材T的具體材質不限制,其可以為銅、鋁等。The target material T is disposed at the top of the process chamber 100. The embodiment of the present application does not limit the specific material of the target material T, and it can be copper, aluminum, etc.
承載基座200設置於製程腔室100內,其用於承載晶圓W,承載基座200可以設置有固定元件(例如卡盤元件),固定元件用於將晶圓W固定在承載基座200上,以避免晶圓W在製程處理過程中出現移位。同時承載基座200位於靶材T的下方,具體而言,靶材T和承載基座200在沿製程腔室100的高度方向由上至下依次佈置,且二者相對設置,如此,在靶材T濺射出粒子後,粒子能夠順利落在承載基座200的晶圓W上。The support base 200 is disposed in the process chamber 100 and is used to support the wafer W. The support base 200 may be provided with a fixing element (such as a chuck element), and the fixing element is used to fix the wafer W on the support base 200 to prevent the wafer W from shifting during the process. At the same time, the support base 200 is located below the target material T. Specifically, the target material T and the support base 200 are arranged in sequence from top to bottom along the height direction of the process chamber 100, and the two are arranged oppositely, so that after the target material T sputters out particles, the particles can smoothly fall on the wafer W of the support base 200.
本申請實施例的磁控濺射設備還包括磁控濺射組件300,磁控濺射組件300用於作用靶材T而濺射出粒子。磁控濺射元件300可以包括驅動機構320和與之連接的磁控管310,磁控管310設置於靶材T背離承載基座200的一側,在驅動機構320的作用下,磁控管310作旋轉運動。在進行磁控濺射製程時,製程腔室100內通入製程氣體(通常為氬氣)後,直流電源向靶材T施加直流偏壓,使靶材T相對於接地的製程腔室100呈負偏壓,如此會激發製程氣體放電而產生等離子體,帶正電的等離子體會被吸引至負偏壓的靶材T上,當等離子體的能量足夠大時會轟擊靶材T的表面,進而使靶材T濺射出粒子;基於靶材T的材質會濺射出相應的金屬粒子,例如銅粒子、鋁粒子等。The magnetron sputtering device of the embodiment of the present application further includes a magnetron sputtering assembly 300, which is used to act on the target material T to sputter out particles. The magnetron sputtering element 300 may include a driving mechanism 320 and a magnetron 310 connected thereto, and the magnetron 310 is arranged on a side of the target material T away from the carrier 200, and under the action of the driving mechanism 320, the magnetron 310 performs a rotational motion. During the magnetron sputtering process, after the process gas (usually argon) is introduced into the process chamber 100, a DC power supply applies a DC bias to the target material T, so that the target material T is negatively biased relative to the grounded process chamber 100, which will stimulate the process gas to discharge and generate plasma. The positively charged plasma will be attracted to the negatively biased target material T. When the energy of the plasma is large enough, it will bombard the surface of the target material T, thereby causing the target material T to sputter out particles; based on the material of the target material T, corresponding metal particles, such as copper particles, aluminum particles, etc., will be sputtered.
製程氣體放電產生的等離子體對靶材T的轟擊區域、角度等因素都是隨機的,因此靶材T濺射出的粒子是呈無規則散射狀態,這樣會導致部分粒子濺射至晶圓W區域之外,進而造成靶材T的浪費,其餘的部分粒子即便是能夠落在晶圓W範圍內,多數也會與晶圓W表面呈傾斜角度入射而難以沉積入晶圓W的溝槽內,甚至會在溝槽開口周圍不斷堆積而將開口封堵,進一步地增大粒子的入槽難度。隨著技術的進步,半導體晶片的特徵尺寸被設置得越來越小,這使得晶圓W上溝槽的開口進一步縮小,深寬比進一步增大,上述的問題會更為嚴重。The impact area and angle of the plasma generated by the process gas discharge on the target material T are random, so the particles sputtered by the target material T are in a state of irregular scattering, which will cause some particles to sputter outside the wafer W area, thereby causing waste of the target material T. Even if the remaining particles can fall within the range of the wafer W, most of them will be incident at an oblique angle to the surface of the wafer W and will be difficult to deposit in the grooves of the wafer W. They may even continue to accumulate around the opening of the groove and block the opening, further increasing the difficulty of particles entering the groove. With the advancement of technology, the feature size of semiconductor chips is set to be smaller and smaller, which makes the opening of the trench on the wafer W further reduced and the aspect ratio further increased, and the above-mentioned problem will become more serious.
針對上述問題,本申請實施例的磁控濺射設備是通過設置導向裝置400來解決的。In view of the above problems, the magnetron sputtering device of the embodiment of the present application solves the problems by providing a guiding device 400.
在本申請實施例中,導向裝置400設置於靶材T與承載基座200之間,導向裝置400被配置為在製程腔室100內形成電場或磁場,電場或磁場用於調節靶材濺射出的粒子的運動軌跡,以使粒子趨於垂直地沉積於晶圓W上。In the present application embodiment, the guiding device 400 is disposed between the target material T and the supporting base 200. The guiding device 400 is configured to form an electric field or a magnetic field in the process chamber 100. The electric field or the magnetic field is used to adjust the movement trajectory of the particles sputtered from the target material so that the particles tend to be deposited vertically on the wafer W.
應理解的是,粒子是由靶材T濺射而出並落在晶圓W上,靶材T與承載基座200之間的區域即為濺射區域,導向裝置400設置於靶材T與承載基座200之間,這使得導向裝置400在濺射區域內形成電場或磁場,進而可對濺射區域內的粒子產生導向作用。It should be understood that particles are sputtered from the target material T and fall onto the wafer W. The area between the target material T and the supporting base 200 is the sputtering area. The guiding device 400 is arranged between the target material T and the supporting base 200, which enables the guiding device 400 to form an electric field or a magnetic field in the sputtering area, thereby producing a guiding effect on the particles in the sputtering area.
若導向裝置400用於形成電場,則形成的電場使得其中的粒子受到電場力,在電場力的作用下,粒子的運動軌跡即可被改變;若導向裝置400用於形成磁場,則形成的磁場使得其中的粒子受到磁場力,在磁場力的作用下,粒子的運動軌跡即可被改變。If the guiding device 400 is used to form an electric field, the formed electric field causes the particles therein to be subjected to an electric field force, and under the action of the electric field force, the movement trajectory of the particles can be changed; if the guiding device 400 is used to form a magnetic field, the formed magnetic field causes the particles therein to be subjected to a magnetic field force, and under the action of the magnetic field force, the movement trajectory of the particles can be changed.
借助導向裝置400,可通過產生電場力或磁場力來調節靶材濺射出的粒子的運動軌跡,即起到對粒子的導向作用,使得濺射至晶圓W之外的粒子被導向至落入晶圓W,且使得這部分粒子以及原本就落入晶圓W的粒子的運動軌跡均相對於晶圓表面呈垂直關係,換句話說,導向裝置400使得粒子以趨於0°的入射角落入至晶圓W上,粒子的入射角即是指粒子的運動軌跡與晶圓W表面的法線的夾角。從靶材T濺射的粒子整體情況來看,粒子由之前的無規則散射狀態轉變為較為彙聚並垂直向下入射晶圓W的狀態。With the help of the guide device 400, the movement trajectory of the particles sputtered from the target material can be adjusted by generating an electric field force or a magnetic field force, that is, the particles are guided so that the particles sputtered outside the wafer W are guided to fall into the wafer W, and the movement trajectory of these particles and the particles that originally fell into the wafer W are perpendicular to the wafer surface. In other words, the guide device 400 allows the particles to fall onto the wafer W at an incident angle tending to 0°. The incident angle of the particles refers to the angle between the movement trajectory of the particles and the normal of the surface of the wafer W. From the overall situation of the particles sputtered from the target material T, the particles change from the previous irregular scattering state to a state of being more concentrated and incident on the wafer W vertically downward.
如此情況下,靶材T濺射出的粒子落入至晶圓W的數量會顯著增多,這樣不僅能夠減少靶材T的浪費,也能夠增加粒子落入溝槽的數量,一定程度上減少了沉積空洞的出現;同時,由於有更多的粒子趨於垂直地落入晶圓W,這些粒子不會像傾斜入射的粒子沉積在溝槽的開口處,也不會在通過開口後沉積在開口附近的側壁上,其能夠垂直落入至溝槽的底部,以確保溝槽內各處均填充有粒子,進而提升溝槽內粒子沉積的均勻性,有效避免了出現沉積空洞,還能夠避免粒子在溝槽開口處異常沉積而封堵開口。基於上述的有益效果,本申請實施例的導向裝置400能夠有效地提升粒子的沉積品質。In this case, the number of particles sputtered from the target material T that fall into the wafer W will increase significantly, which can not only reduce the waste of the target material T, but also increase the number of particles falling into the grooves, which to a certain extent reduces the occurrence of deposition voids; at the same time, since more particles tend to fall vertically into the wafer W, these particles will not be as obliquely incident as particles The particles are deposited at the opening of the groove, and will not be deposited on the side wall near the opening after passing through the opening. They can fall vertically to the bottom of the groove to ensure that the groove is filled with particles everywhere, thereby improving the uniformity of particle deposition in the groove, effectively avoiding the occurrence of deposition voids, and preventing particles from abnormally depositing at the opening of the groove and blocking the opening. Based on the above beneficial effects, the guiding device 400 of the embodiment of the present application can effectively improve the deposition quality of particles.
需要說明的是,由於電場力能夠同時改變粒子的速度的方向和大小,則本申請實施例的導向裝置形成的電場為定向電場,以在同一方向上調節粒子的運動軌跡;由於磁場力僅改變粒子速度的方向,而不改變粒子的速度的大小,本申請實施例的導向裝置形成的磁場並不局限為定向磁場,也可以為非定向磁場。It should be noted that, since the electric field force can change the direction and magnitude of the particle's velocity at the same time, the electric field formed by the guiding device of the embodiment of the present application is a directional electric field, so as to adjust the particle's movement trajectory in the same direction; since the magnetic field force only changes the direction of the particle's velocity but does not change the magnitude of the particle's velocity, the magnetic field formed by the guiding device of the embodiment of the present application is not limited to a directional magnetic field, but can also be a non-directional magnetic field.
由上述說明可知,在本申請實施例的磁控濺射設備中,導向裝置400能夠在製程腔室100內形成電場或磁場,由電場或磁場產生電場力或磁場力來調節靶材濺射出的粒子的運動軌跡,使得粒子的運動軌跡相對於晶圓表面呈垂直關係,以使粒子能夠趨於垂直地沉積於晶圓W上,這樣不僅增加了粒子落入晶圓W的數量,減少了靶材T的浪費,還使得粒子垂直落入至晶圓W溝槽的底部,有效改善了粒子異常沉積而封堵溝槽開口以及存在沉積空洞的問題,最終達到提升粒子的沉積品質的效果。As can be seen from the above description, in the magnetron sputtering equipment of the embodiment of the present application, the guiding device 400 can form an electric field or a magnetic field in the process chamber 100, and the electric field or the magnetic field generates an electric field force or a magnetic field force to adjust the movement trajectory of the particles sputtered by the target material, so that the movement trajectory of the particles is perpendicular to the wafer surface, so that the particles can tend to be deposited vertically on the wafer W. This not only increases the number of particles falling into the wafer W and reduces the waste of the target material T, but also makes the particles fall vertically to the bottom of the trench of the wafer W, effectively improving the problem of abnormal particle deposition and blocking the trench opening and the existence of deposition voids, and ultimately achieving the effect of improving the deposition quality of the particles.
在一些可選的實施例中,導向裝置400包括多個主體件,多個主體件由上至下依次間隔設置,每個主體件均開設有多個用於使粒子穿過的通孔;多個主體件上的各個通孔一一對應;每個主體件均為導電體,多個主體件的電勢由上至下依次遞減,以在各相鄰的兩個主體件之間形成子電場,該子電場用於調整經過的粒子的運動軌跡。具體而言,如此設置下,多個主體件均具備導電性能,因此能夠通過向多個主體件施加電壓,而在各相鄰的兩個主體件的相對側端面之間形成子電場;由於多個主體件的電勢由上至下依次遞減,則各子電場的方向是由上至下。如此情況下,在粒子由上而下依次通過各子電場進行導向之後,粒子會被多次導向,下方的子電場可以彌補上方的子電場對粒子施加導向作用的不足,以確保粒子最終被導向為趨於垂直落入晶圓W。In some optional embodiments, the guiding device 400 includes a plurality of main parts, which are arranged in sequence from top to bottom, and each main part is provided with a plurality of through holes for particles to pass through; the through holes on the plurality of main parts correspond to each other one by one; each main part is a conductor, and the electric potential of the plurality of main parts decreases in sequence from top to bottom to form a sub-electric field between each two adjacent main parts, and the sub-electric field is used to adjust the movement trajectory of the passing particles. Specifically, under such a configuration, the plurality of main parts all have conductive properties, so that a sub-electric field can be formed between the opposite side surfaces of each two adjacent main parts by applying voltage to the plurality of main parts; since the potential of the plurality of main parts decreases from top to bottom, the direction of each sub-electric field is from top to bottom. In this case, after the particles are guided from top to bottom through each sub-electric field in turn, the particles will be guided multiple times, and the sub-electric field below can make up for the lack of guiding effect of the sub-electric field above on the particles, so as to ensure that the particles are finally guided to fall vertically into the wafer W.
由於每個主體件均開設有多個用於使粒子穿過的通孔,各相鄰的兩個主體件的實體重合區域(非通孔區域)的電場強度無疑較高,該區域的等勢面較為密集,而各通孔的對應區域電場強度無疑較低,該區域的等勢面較為稀疏;整體來看,如圖3所示,圖3中虛線即表示等勢面。Since each main body has multiple through holes for particles to pass through, the electric field intensity of the solid overlapping area (non-through hole area) of each adjacent main body is undoubtedly higher, and the equipotential surfaces in this area are denser, while the electric field intensity of the corresponding area of each through hole is undoubtedly lower, and the equipotential surfaces in this area are sparser; overall, as shown in Figure 3, the dotted line in Figure 3 represents the equipotential surface.
靶材T濺射出的粒子帶正電荷,其在子電場中所受到的電場力是垂直於等勢面的,也即粒子會朝等勢面的法線方向偏轉,因此粒子在電場力的持續作用下會呈現出圖3中的運動軌跡,圖3中實線即表示粒子的運動軌跡。需要說明的是,由於粒子在自重和電場力的作用下會受到加速作用,其在各相鄰的兩個主體件之間的上下半區內會存在通行時間的差異,也即粒子在各相鄰的兩個主體件之間的上半區的通行時間會多於其在各相鄰的兩個主體件之間的下半區的通行時間,因此,粒子在各相鄰的兩個主體件之間的上半區受電場力產生的偏轉較大,而其在各相鄰的兩個主體件之間的下半區受電場力產生的偏轉較小,如此以無規則散射狀態入射的粒子均會以趨於垂直晶圓W的角度從導向裝置400出射,粒子之間會呈相互平行的狀態。The particles ejected from the target material T are positively charged, and the electric field force they experience in the sub-electric field is perpendicular to the equipotential surface, that is, the particles will deflect in the normal direction of the equipotential surface. Therefore, under the continuous action of the electric field force, the particles will show the movement trajectory shown in Figure 3. The solid line in Figure 3 represents the movement trajectory of the particles. It should be noted that, since the particles are accelerated due to their own weight and the electric field force, there will be a difference in the travel time between the upper and lower halves of each adjacent main body, that is, the travel time of the particles in the upper half between each adjacent main body will be longer than the travel time in the lower half between each adjacent main body. Therefore, the deflection of the particles caused by the electric field force in the upper half between each adjacent main body is larger, while the deflection of the particles in the lower half between each adjacent main body is smaller. In this way, particles incident in a state of irregular scattering will all be emitted from the guiding device 400 at an angle tending to be perpendicular to the wafer W, and the particles will be parallel to each other.
通過調節各子電場的強度,即可對粒子在濺射區域所受到的電場力的大小進行調節,由於粒子的運動軌跡與其受到的電場力大小直接相關,當電場力較大或較小都難以使得粒子趨於垂直落入晶圓W,因此可以對導向裝置400進行預先測試,通過觀察粒子通過導向裝置400的運動軌跡,來將各子電場的強度調節至合適範圍。By adjusting the strength of each sub-electric field, the magnitude of the electric field force to which the particles are subjected in the sputtering region can be adjusted. Since the movement trajectory of the particle is directly related to the magnitude of the electric field force to which it is subjected, it is difficult for the particle to fall vertically into the wafer W when the electric field force is large or small. Therefore, the guiding device 400 can be pre-tested, and the strength of each sub-electric field can be adjusted to an appropriate range by observing the movement trajectory of the particle through the guiding device 400.
以主體件為兩個為例,如圖1~圖3所示,本申請實施例提供第一種導向裝置400,其主體件為兩個,分別為第一主體件410和第二主體件420,第一主體件410和第二主體件420由上至下依次間隔設置,開設在第一主體件410上的通孔為第一通孔H1,開設在第二主體件420上的通孔為第二通孔H2,多個第一通孔H1與多個第二通孔H2一一對應,可選的,沿製程腔室100的高度方向(即,豎直方向)上,第一通孔H1和第二通孔H2的投影能夠相互重合。Taking two main parts as an example, as shown in Figures 1 to 3, the embodiment of the present application provides a first guiding device 400, which has two main parts, namely a first main part 410 and a second main part 420. The first main part 410 and the second main part 420 are arranged in sequence from top to bottom. The through hole opened on the first main part 410 is the first through hole H1, and the through hole opened on the second main part 420 is the second through hole H2. The multiple first through holes H1 correspond to the multiple second through holes H2 one by one. Optionally, along the height direction (i.e., the vertical direction) of the process chamber 100, the projections of the first through hole H1 and the second through hole H2 can overlap with each other.
同時,第一主體件410和第二主體件420均為導電體,第一主體件410被配置為處於第一電勢U1,第二主體件420被配置為處於第二電勢U2,且第一電勢U1大於第二電勢U2,以在第一主體件410和第二主體件420之間形成第一子電場。At the same time, the first main body 410 and the second main body 420 are both conductors, the first main body 410 is configured to be at a first potential U1, the second main body 420 is configured to be at a second potential U2, and the first potential U1 is greater than the second potential U2 to form a first sub-electric field between the first main body 410 and the second main body 420.
具體而言,如此設置下,第一主體件410和第二主體件420均具備導電性能,因此能夠通過向第一主體件410和第二主體件420施加電壓,而在第一主體件410和第二主體件420的相對側端面之間形成第一子電場;由於第一電勢U1大於第二電勢U2,則第一子電場的方向是由第一主體件410朝向第二主體件420的端面至第二主體件420朝向第一主體件410的端面。Specifically, under such a configuration, the first main body 410 and the second main body 420 both have conductive properties, so that a first sub-electric field can be formed between the opposite side end surfaces of the first main body 410 and the second main body 420 by applying a voltage to the first main body 410 and the second main body 420; since the first potential U1 is greater than the second potential U2, the direction of the first sub-electric field is from the end surface of the first main body 410 toward the second main body 420 to the end surface of the second main body 420 toward the first main body 410.
由於第一通孔H1和第二通孔H2的存在,第一主體件410和第二主體件420的實體重合區域的電場強度無疑較高,該區域的等勢面較為密集,而第一通孔H1和第二通孔H2的對應區域電場強度無疑較低,該區域的等勢面較為稀疏;整體來看,如圖3所示,圖3示出了第一子電場的等勢面分佈形貌,圖3中虛線即表示等勢面。Due to the existence of the first through hole H1 and the second through hole H2, the electric field strength in the physically overlapping area of the first main body 410 and the second main body 420 is undoubtedly higher, and the equipotential surfaces in this area are relatively dense, while the electric field strength in the corresponding area of the first through hole H1 and the second through hole H2 is undoubtedly lower, and the equipotential surfaces in this area are relatively sparse; overall, as shown in Figure 3, Figure 3 shows the equipotential surface distribution morphology of the first sub-electric field, and the dotted line in Figure 3 represents the equipotential surface.
靶材T濺射出的粒子帶正電荷,其在第一子電場中所受到的電場力是垂直於等勢面的,也即粒子會朝等勢面的法線方向偏轉,因此粒子在電場力的持續作用下會呈現出圖3中的運動軌跡,圖3中實線即表示粒子的運動軌跡。需要說明的是,由於粒子在自重和電場力的作用下會受到加速作用,其在第一主體件410和第二主體件420之間的上下半區內會存在通行時間的差異,也即粒子在第一主體件410和第二主體件420之間的上半區的通行時間會多於其在第一主體件410和第二主體件420之間的下半區的通行時間,因此,粒子在第一主體件410和第二主體件420之間的上半區受電場力產生的偏轉較大,而其在第一主體件410和第二主體件420之間的下半區受電場力產生的偏轉較小,如此以無規則散射狀態入射的粒子均會以趨於垂直晶圓W的角度從導向裝置400出射,粒子之間會呈相互平行的狀態。The particles sputtered from the target material T carry positive charge, and the electric field force they are subjected to in the first sub-electric field is perpendicular to the equipotential surface, that is, the particles will be deflected in the normal direction of the equipotential surface. Therefore, under the continuous action of the electric field force, the particles will show the motion trajectory shown in Figure 3. The solid line in Figure 3 represents the motion trajectory of the particles. It should be noted that, since the particles are accelerated due to their own weight and the electric field force, there will be a difference in the passage time between the upper and lower halves between the first main body 410 and the second main body 420, that is, the passage time of the particles in the upper half between the first main body 410 and the second main body 420 will be longer than the passage time in the lower half between the first main body 410 and the second main body 420. Therefore, the deflection of the particles caused by the electric field force in the upper half between the first main body 410 and the second main body 420 is larger, while the deflection of the particles caused by the electric field force in the lower half between the first main body 410 and the second main body 420 is smaller. In this way, the particles incident in a randomly scattered state will all be emitted from the guiding device 400 at an angle tending to be perpendicular to the wafer W, and the particles will be parallel to each other.
本申請實施例未限制第一主體件410被配置為處於第一電勢U1以及第二主體件420被配置為處於第二電勢U2的具體實現方式,舉例來說,可通過電場載入元件來實現,電場載入元件可以包括第一直流電源和第二直流電源,第一直流電源與第一主體件410電連接並形成通路,第二直流電源與第二主體件420電連接並形成通路,且第一直流電源向第一主體件410施加第一電壓,且第一主體件410處於第一電勢U1,第二直流電源向第二主體件420施加第二電壓,且第二主體件420處於第二電勢U2;或者,電場載入元件包括直流電源和電連接件(通常為導線),直流電源分別與第一主體件410和第二主體件420電連接,且電連接件也與第一主體件410和第二主體件420電連接,進而使得直流電源、第一主體件410、第二主體件420和電連接件構成回路,直流電源向第一主體件410和第二主體件420施加電壓,並使得第一主體件410處於第一電勢U1、第二主體件420處於第二電勢U2。The embodiment of the present application does not limit the specific implementation method of the first main body 410 being configured to be in the first potential U1 and the second main body 420 being configured to be in the second potential U2. For example, it can be implemented by an electric field loading element. The electric field loading element may include a first DC power supply and a second DC power supply. The first DC power supply is electrically connected to the first main body 410 to form a path, and the second DC power supply is electrically connected to the second main body 420 to form a path. The first DC power supply applies a first voltage to the first main body 410, and the first main body 410 is in the first potential U1, and the second DC power supply applies a first voltage to the second main body 420. The second voltage is applied to the first main body 410, and the second main body 420 is at a second potential U2; or, the electric field loading element includes a DC power supply and an electrical connector (usually a wire), the DC power supply is electrically connected to the first main body 410 and the second main body 420 respectively, and the electrical connector is also electrically connected to the first main body 410 and the second main body 420, so that the DC power supply, the first main body 410, the second main body 420 and the electrical connector form a loop, the DC power supply applies a voltage to the first main body 410 and the second main body 420, and the first main body 410 is at a first potential U1, and the second main body 420 is at a second potential U2.
通過調節第一子電場的強度,即可對粒子在濺射區域所受到的電場力的大小進行調節,由於粒子的運動軌跡與其受到的電場力大小直接相關,當電場力較大或較小都難以使得粒子趨於垂直落入晶圓W,因此可以對導向裝置400進行預先測試,通過觀察粒子通過導向裝置400的運動軌跡,來將第一子電場的強度調節至合適範圍。By adjusting the strength of the first sub-electric field, the magnitude of the electric field force to which the particles are subjected in the sputtering region can be adjusted. Since the movement trajectory of the particles is directly related to the magnitude of the electric field force to which they are subjected, it is difficult for the particles to fall vertically into the wafer W when the electric field force is large or small. Therefore, the guiding device 400 can be pre-tested, and the strength of the first sub-electric field can be adjusted to an appropriate range by observing the movement trajectory of the particles passing through the guiding device 400.
本申請實施例的導向裝置400還可以通過其他的方式來調節粒子所受到的導向作用,在另外的實施方式中,如圖8所示,本申請實施例的導向裝置400,其主體件為三個,分別為第一主體件410、第二主體件420和第三主體件430,第一主體件410、第二主體件420和第三主體件430由上至下依次間隔設置,開設在第一主體件410上的通孔為第一通孔H1,開設在第二主體件420上的通孔為第二通孔H2,開設在第三主體件430上的通孔為第三通孔(圖中未示出),多個第一通孔、多個第二通孔和多個第三通孔一一對應,可選的,沿製程腔室100的高度方向(即,豎直方向)上,第一通孔H1、第二通孔H2和第三通孔的投影都能夠相互重合。The guiding device 400 of the embodiment of the present application can also adjust the guiding effect on the particles in other ways. In another embodiment, as shown in FIG. 8 , the guiding device 400 of the embodiment of the present application has three main parts, namely a first main part 410, a second main part 420 and a third main part 430. The first main part 410, the second main part 420 and the third main part 430 are arranged in sequence from top to bottom, and are opened in the first main part. The through hole on the main body 410 is the first through hole H1, the through hole opened on the second main body 420 is the second through hole H2, and the through hole opened on the third main body 430 is the third through hole (not shown in the figure). The multiple first through holes, the multiple second through holes and the multiple third through holes correspond to each other one by one. Optionally, along the height direction (i.e., the vertical direction) of the process chamber 100, the projections of the first through hole H1, the second through hole H2 and the third through hole can overlap with each other.
同時,第一主體件410、第二主體件420和第三主體件430為導電體,第一主體件410被配置為處於第一電勢U1,第二主體件420被配置為處於第二電勢U2,第三主體件430被配置為處於第三電勢,且第一電勢U1大於第二電勢U2,第三電勢小於第二電勢U2,以在第一主體件410和第二主體件420之間形成第一子電場,在第二主體件420和第三主體件430之間形成第二子電場。At the same time, the first main body 410, the second main body 420 and the third main body 430 are conductors, the first main body 410 is configured to be at a first potential U1, the second main body 420 is configured to be at a second potential U2, the third main body 430 is configured to be at a third potential, and the first potential U1 is greater than the second potential U2, and the third potential is less than the second potential U2, so as to form a first sub-electric field between the first main body 410 and the second main body 420, and form a second sub-electric field between the second main body 420 and the third main body 430.
具體而言,如此設置下,第一主體件410、第二主體件420和第三主體件430均具備導電性能,因此能夠通過向第一主體件410、第二主體件420和第三主體件430施加電壓,而在第一主體件410和第二主體件420的相對側端面之間形成第一子電場,在第二主體件420和第三主體件430的相對側端面之間形成第二子電場;由於第一電勢U1大於第二電勢U2,則第一子電場的方向是由第一主體件410朝向第二主體件420的端面至第二主體件420朝向第一主體件410的端面;由於第二電勢U2大於第三電勢,則第二子電場的方向是由第二主體件420朝向第三主體件430的端面至第三主體件430朝向第二主體件420的端面;第二子電場與第一子電場的屬性相同,第二子電場的等勢面分佈形貌也如圖3所示。如此情況下,在粒子通過第一子電場進行導向之後,粒子通過第二子電場會被二次導向,第二子電場可以彌補第一子電場對粒子施加導向作用的不足,以確保粒子最終被導向為趨於垂直落入晶圓W。Specifically, under such a configuration, the first main body 410, the second main body 420 and the third main body 430 all have conductive properties. Therefore, by applying voltage to the first main body 410, the second main body 420 and the third main body 430, a first sub-electric field can be formed between the opposite side end surfaces of the first main body 410 and the second main body 420, and a second sub-electric field can be formed between the opposite side end surfaces of the second main body 420 and the third main body 430. Since the first potential U1 is greater than the second potential U2, Since the second electric potential U2 is greater than the third electric potential, the direction of the first sub-electric field is from the end surface of the first main body 410 toward the second main body 420 to the end surface of the second main body 420 toward the first main body 410; since the second electric potential U2 is greater than the third electric potential, the direction of the second sub-electric field is from the end surface of the second main body 420 toward the third main body 430 to the end surface of the third main body 430 toward the second main body 420; the second sub-electric field has the same properties as the first sub-electric field, and the equipotential surface distribution morphology of the second sub-electric field is also shown in FIG3. In this case, after the particles are guided by the first sub-electric field, the particles will be guided for the second time by the second sub-electric field, and the second sub-electric field can make up for the lack of the first sub-electric field in guiding the particles, so as to ensure that the particles are finally guided to fall vertically into the wafer W.
如圖1、圖2、圖4和圖5所示,本申請實施例提供第二種導向裝置400,其包括多個主體件和至少一個磁場形成元件,多個主體件由上至下依次間隔設置,每個主體件均開設有多個用於使粒子穿過的通孔;多個主體件上的各個通孔一一對應;多個主體件均為導磁體,各相鄰的兩個主體件對應設置有一個磁場形成元件,用於磁化對應的相鄰兩個主體件,並使對應的相鄰兩個主體件分別形成相異的兩個磁極,以在各相鄰的兩個主體件之間形成子磁場。As shown in Figures 1, 2, 4 and 5, the embodiment of the present application provides a second guiding device 400, which includes multiple main parts and at least one magnetic field forming element. The multiple main parts are arranged in sequence from top to bottom, and each main part is provided with multiple through holes for particles to pass through; the through holes on the multiple main parts correspond to each other; the multiple main parts are magnetic conductors, and each two adjacent main parts are correspondingly provided with a magnetic field forming element, which is used to magnetize the corresponding two adjacent main parts and make the corresponding two adjacent main parts form two different magnetic poles respectively, so as to form a sub-magnetic field between each two adjacent main parts.
具體而言,如此設置下,多個主體件均具備導磁性能,磁場形成元件用於磁化對應的相鄰兩個主體件,以在相鄰兩個主體件的相對側端面之間形成子磁場。該子磁場的磁場方向與相鄰兩個主體件內部的磁疇方向有關,而相鄰兩個主體件內部的磁疇方向與磁場形成元件具體的磁化作用有關,如圖5所示,圖5中虛線即表示磁感線,對於各相鄰的兩個主體件,上方的子主體件上形成N磁極,下方的主體件上形成S磁極,因此子磁場的磁場方向也是由上方的子主體件至下方的主體件。當然,本申請實施例未限制各相鄰的兩個主體件上分別形成的磁極的具體類型,在另外的實施方式中,上方的子主體件上可形成S磁極,下方的主體件上可形成N磁極。Specifically, under such a configuration, multiple main parts all have magnetic conductivity, and the magnetic field forming element is used to magnetize the corresponding two adjacent main parts to form a sub-magnetic field between the opposite side end surfaces of the two adjacent main parts. The magnetic field direction of the sub-magnetic field is related to the magnetic field direction inside the two adjacent main parts, and the magnetic field direction inside the two adjacent main parts is related to the specific magnetization effect of the magnetic field forming element, as shown in Figure 5. The dotted line in Figure 5 represents the magnetic flux lines. For each of the two adjacent main parts, an N magnetic pole is formed on the upper sub-main part, and an S magnetic pole is formed on the lower main part. Therefore, the magnetic field direction of the sub-magnetic field is also from the upper sub-main part to the lower main part. Of course, the embodiment of the present application does not limit the specific types of magnetic poles formed on each of the two adjacent main parts. In another embodiment, an S magnetic pole can be formed on the upper sub-main part, and an N magnetic pole can be formed on the lower main part.
需要說明的是,本申請實施例的導向裝置所形成的磁場力主要是指洛倫茲力,洛倫茲力僅改變粒子的速度方向,而不會改變粒子的速度大小,因此其僅改變粒子的運動方向而不會對粒子做功。It should be noted that the magnetic field force formed by the guiding device of the embodiment of the present application mainly refers to the Lorentz force, which only changes the direction of the particle's velocity but does not change the magnitude of the particle's velocity. Therefore, it only changes the direction of the particle's movement but does not do work on the particle.
由於每個主體件均開設有多個用於使粒子穿過的通孔,各相鄰的兩個主體件的實體重合區域(非通孔區域)的磁場強度較高,而通孔的對應區域的磁場強度較低,具體可參見圖5示出的子磁場中磁感線的分佈形貌。Since each main body is provided with a plurality of through holes for particles to pass through, the magnetic field strength in the solid overlapping area (non-through hole area) of each adjacent main body is relatively high, while the magnetic field strength in the corresponding area of the through hole is relatively low. For details, please refer to the distribution morphology of magnetic flux lines in the sub-magnetic field shown in FIG5 .
靶材T濺射出的粒子帶正電荷,其在子磁場中運動時,會受到垂直於運動方向和磁場方向的磁場力,而磁場力的具體方向可通過左手定則來判斷。在磁場力的作用下,粒子會沿著磁感線的方向螺旋運動,具體可參見圖6,圖6僅用於示出粒子形成螺旋運動的原理,並不代表粒子呈圖6中所示的運動軌跡;同時,基於磁場強度的分佈,粒子在螺旋運動時會朝向磁場強度較低的區域逐漸偏移,粒子會大致呈現出圖5中的運動軌跡,圖5中實線即表示粒子的運動軌跡。直至粒子運動至通孔的中軸線附近,此時粒子所受的磁場力最小,其受到的磁場力改變其速度方向的作用趨於可忽略不計;具體地,粒子的射出速度V'的方向與射入速度V的方向存在區別,射出速度V'的方向位於通孔的軸線方向,因此,粒子不再做螺旋運動而從通孔垂直向下出射。由此可見,粒子通過導向裝置後就趨於垂直落入晶圓W。The particles sputtered from the target material T carry positive charge. When they move in the sub-magnetic field, they will be subject to a magnetic field force perpendicular to the direction of movement and the direction of the magnetic field. The specific direction of the magnetic field force can be determined by the left-hand rule. Under the action of the magnetic field force, the particles will spirally move along the direction of the magnetic flux lines. For details, please refer to Figure 6. Figure 6 is only used to illustrate the principle of the particles forming spiral motion, and does not mean that the particles present the motion trajectory shown in Figure 6; at the same time, based on the distribution of the magnetic field intensity, the particles will gradually deviate towards the area with lower magnetic field intensity during the spiral motion, and the particles will roughly present the motion trajectory in Figure 5. The solid line in Figure 5 represents the motion trajectory of the particles. Until the particle moves to the vicinity of the central axis of the through hole, the magnetic field force on the particle is minimal, and the effect of the magnetic field force on the particle changing its velocity direction tends to be negligible; specifically, the direction of the particle's ejection velocity V' is different from the direction of the injection velocity V, and the direction of the ejection velocity V' is in the axis direction of the through hole, so the particle no longer makes a spiral motion but is ejected vertically downward from the through hole. It can be seen that the particle tends to fall vertically into the wafer W after passing through the guide device.
通過調節磁場形成元件載入的子磁場的強度,即可對粒子在濺射區域所受到的磁場力的大小進行調節,由於粒子的運動軌跡與其受到的磁場力大小直接相關,當磁場力較大會造成耗能嚴重,而磁場力較小難以使得粒子趨於垂直落入晶圓W,因此可以對導向裝置進行預先測試,通過觀察粒子通過導向裝置的運動軌跡,來將磁場形成組件載入的子磁場的強度調節至合適範圍。By adjusting the intensity of the sub-magnetic field loaded by the magnetic field forming component, the magnitude of the magnetic field force to which the particles are subjected in the sputtering area can be adjusted. Since the movement trajectory of the particles is directly related to the magnitude of the magnetic field force to which they are subjected, a larger magnetic field force will cause serious energy consumption, while a smaller magnetic field force will make it difficult for the particles to fall vertically into the wafer W. Therefore, the guiding device can be pre-tested, and the intensity of the sub-magnetic field loaded by the magnetic field forming component can be adjusted to an appropriate range by observing the movement trajectory of the particles passing through the guiding device.
本申請實施例未限制磁場形成元件的具體類型,其可以為永磁鐵,只要能夠對多個主體件產生磁化作用的元件即可。在另外的實施方式中,上述磁場形成元件包括多個電磁鐵元件,該磁場形成元件中的全部電磁鐵元件均設置於與該磁場形成元件對應的相鄰兩個主體件之間,且沿主體件的圓周方向均勻佈置;磁場形成元件中的全部電磁鐵元件通過相同的磁極端與該磁場形成元件對應的相鄰兩個主體件中的一者連接,以使所連接的其中一主體件上形成第一磁極,磁場形成元件中的全部電磁鐵元件通過相同的另一磁極端與該磁場形成組件對應的相鄰兩個主體件中的另一者連接,以使所連接的另一主體件上形成第二磁極。上述電磁鐵元件通過通斷電即可對子磁場進行控制,改變通入電流的大小即可控制子磁場的磁場強度,還可以通過改變電流方向(包括改變電磁鐵中線圈的纏繞方向)來改變子磁場的磁場方向,因此電磁鐵類型的磁場形成元件無疑具有更便捷的操作性。The embodiment of the present application does not limit the specific type of the magnetic field forming element, which can be a permanent magnet as long as it can produce a magnetizing effect on multiple main parts. In another embodiment, the magnetic field forming element includes a plurality of electromagnetic iron elements, all of which are disposed between two adjacent main parts corresponding to the magnetic field forming element and are evenly arranged along the circumferential direction of the main parts; all of the electromagnetic iron elements in the magnetic field forming element are connected to one of the two adjacent main parts corresponding to the magnetic field forming element through the same magnetic pole end so that a first magnetic pole is formed on one of the connected main parts, and all of the electromagnetic iron elements in the magnetic field forming element are connected to the other of the two adjacent main parts corresponding to the magnetic field forming assembly through the same other magnetic pole end so that a second magnetic pole is formed on the other connected main part. The above-mentioned electromagnetic element can control the sub-magnetic field by turning on and off the power. The magnetic field strength of the sub-magnetic field can be controlled by changing the size of the input current. The magnetic field direction of the sub-magnetic field can also be changed by changing the direction of the current (including changing the winding direction of the coil in the electromagnetic). Therefore, the electromagnetic type magnetic field forming element is undoubtedly more convenient to operate.
以主體件為兩個為例,本申請實施例的導向裝置400,其兩個主體件分別為第一主體件410和第二主體件420,第一主體件410和第二主體件420由上至下依次間隔設置,開設在第一主體件410上的通孔為第一通孔H1,開設在第二主體件420上的通孔為第二通孔H2,多個第一通孔H1與多個第二通孔H2一一對應,可選的,沿製程腔室100的高度方向(即,豎直方向)上,第一通孔H1和第二通孔H2的投影能夠相互重合。Taking two main parts as an example, the guiding device 400 of the embodiment of the present application has two main parts, namely a first main part 410 and a second main part 420. The first main part 410 and the second main part 420 are arranged in sequence from top to bottom. The through hole opened on the first main part 410 is the first through hole H1, and the through hole opened on the second main part 420 is the second through hole H2. The multiple first through holes H1 correspond to the multiple second through holes H2 one by one. Optionally, along the height direction (i.e., the vertical direction) of the process chamber 100, the projections of the first through hole H1 and the second through hole H2 can overlap with each other.
同時,第一主體件410和第二主體件420均為導磁體,磁場形成元件440為一個,用於磁化第一主體件410和第二主體件420,並使第一主體件410上形成第一磁極,以及使第二主體件420上形成第二磁極,且第一磁極和第二磁極相異,以在第一主體件410和第二主體件420之間形成第一子磁場。At the same time, the first main body 410 and the second main body 420 are both magnetic conductors, and the magnetic field forming element 440 is one, which is used to magnetize the first main body 410 and the second main body 420, and form a first magnetic pole on the first main body 410, and form a second magnetic pole on the second main body 420, and the first magnetic pole and the second magnetic pole are different, so as to form a first sub-magnetic field between the first main body 410 and the second main body 420.
具體而言,如此設置下,第一主體件410和第二主體件420均具備導磁性能,磁場形成元件440即可順利磁化第一主體件410和第二主體件420,而在第一主體件410和第二主體件420的相對側端面之間形成第一子磁場。第一子磁場的磁場方向與第一主體件410和第二主體件420內部的磁疇方向有關,而第一主體件410和第二主體件420內部的磁疇方向與磁場形成元件440具體的磁化作用有關,以圖5示出的實施方式為例,其示出了第一子磁場的磁感線分佈形貌,圖5中虛線即表示磁感線,磁場形成組件440磁化第一主體件410,並在第一主體件410上形成N磁極,磁場形成元件440磁化第二主體件420,並在第二主體件420上形成S磁極,因此第一子磁場的磁場方向也是由第一主體件410至第二主體件420。Specifically, under such a setting, the first main body 410 and the second main body 420 both have magnetic conductivity, and the magnetic field forming element 440 can smoothly magnetize the first main body 410 and the second main body 420, and form a first sub-magnetic field between the relative side end surfaces of the first main body 410 and the second main body 420. The magnetic field direction of the first sub-magnetic field is related to the magnetic flux direction inside the first main body 410 and the second main body 420, and the magnetic flux direction inside the first main body 410 and the second main body 420 is related to the specific magnetization effect of the magnetic field forming element 440. Taking the implementation method shown in Figure 5 as an example, it shows the magnetic flux line distribution morphology of the first sub-magnetic field. The dotted lines in Figure 5 represent the magnetic flux lines. The magnetic field forming component 440 magnetizes the first main body 410 and forms an N magnetic pole on the first main body 410. The magnetic field forming element 440 magnetizes the second main body 420 and forms an S magnetic pole on the second main body 420. Therefore, the magnetic field direction of the first sub-magnetic field is also from the first main body 410 to the second main body 420.
當然,本申請實施例未限制第一主體件410和第二主體件420上分別形成的磁極的具體類型,在另外的實施方式中,第一主體件410上可形成S磁極,第二主體件420上可形成N磁極。Of course, the embodiment of the present application does not limit the specific types of magnetic poles formed on the first main body 410 and the second main body 420 respectively. In another embodiment, an S magnetic pole can be formed on the first main body 410 and an N magnetic pole can be formed on the second main body 420.
需要說明的是,本申請實施例的導向裝置400所形成的磁場力主要是指洛倫茲力,洛倫茲力僅改變粒子的速度方向,而不會改變粒子的速度大小,因此其僅改變粒子的運動方向而不會對粒子做功。It should be noted that the magnetic field force formed by the guiding device 400 of the embodiment of the present application mainly refers to the Lorentz force, which only changes the velocity direction of the particle but does not change the velocity magnitude of the particle. Therefore, it only changes the movement direction of the particle but does not do work on the particle.
由於第一通孔H1和第二通孔H2的存在,第一主體件410和第二主體件420的實體重合區域的磁場強度較高,而第一通孔H1和第二通孔H2的對應區域的磁場強度較低,具體可參見圖5示出的第一子磁場中磁感線的分佈形貌。Due to the existence of the first through hole H1 and the second through hole H2, the magnetic field strength in the physically overlapping area of the first main body 410 and the second main body 420 is relatively high, while the magnetic field strength in the corresponding area of the first through hole H1 and the second through hole H2 is relatively low. For details, please refer to the distribution morphology of the magnetic flux lines in the first sub-magnetic field shown in FIG. 5 .
靶材T濺射出的粒子帶正電荷,其在第一子磁場中運動時,會受到垂直於運動方向和磁場方向的磁場力,而磁場力的具體方向可通過左手定則來判斷。在磁場力的作用下,粒子會沿著磁感線的方向螺旋運動,具體可參見圖6,圖6僅用於示出粒子形成螺旋運動的原理,並不代表粒子呈圖6中所示的運動軌跡;同時,基於磁場強度的分佈,粒子在螺旋運動時會朝向磁場強度較低的區域逐漸偏移,粒子會大致呈現出圖5中的運動軌跡,圖5中實線即表示粒子的運動軌跡。直至粒子運動至第一通孔H1和第二通孔H2的中軸線附近,此時粒子所受的磁場力最小,其受到的磁場力改變其速度方向的作用趨於可忽略不計;具體地,粒子的射出速度V'的方向與射入速度V的方向存在區別,射出速度V'的方向位於第二通孔H2的軸線方向,因此,粒子不再做螺旋運動而從第二通孔H2垂直向下出射。由此可見,粒子通過導向裝置400後就趨於垂直落入晶圓W。The particles sputtered from the target material T are positively charged. When they move in the first sub-magnetic field, they will be subject to a magnetic field force perpendicular to the direction of movement and the direction of the magnetic field. The specific direction of the magnetic field force can be determined by the left-hand rule. Under the action of the magnetic field force, the particles will move in a spiral along the direction of the magnetic flux lines. For details, please refer to Figure 6. Figure 6 is only used to illustrate the principle of the particles forming a spiral motion, and does not mean that the particles present the motion trajectory shown in Figure 6; at the same time, based on the distribution of the magnetic field intensity, the particles will gradually deviate towards the area with lower magnetic field intensity during the spiral motion, and the particles will roughly present the motion trajectory in Figure 5. The solid line in Figure 5 represents the motion trajectory of the particles. Until the particle moves to the vicinity of the central axis of the first through hole H1 and the second through hole H2, the magnetic field force on the particle is minimal, and the effect of the magnetic field force on the particle changing its velocity direction tends to be negligible; specifically, the direction of the particle's ejection velocity V' is different from the direction of the injection velocity V, and the direction of the ejection velocity V' is located in the axis direction of the second through hole H2, so the particle no longer performs a spiral motion but is ejected vertically downward from the second through hole H2. It can be seen that the particle tends to fall vertically into the wafer W after passing through the guide device 400.
通過調節磁場形成元件440載入的第一子磁場的強度,即可對粒子在濺射區域所受到的磁場力的大小進行調節,由於粒子的運動軌跡與其受到的磁場力大小直接相關,當磁場力較大會造成耗能嚴重,而磁場力較小難以使得粒子趨於垂直落入晶圓W,因此可以對導向裝置400進行預先測試,通過觀察粒子通過導向裝置400的運動軌跡,來將磁場形成組件440載入的第一子磁場的強度調節至合適範圍。By adjusting the intensity of the first sub-magnetic field loaded by the magnetic field forming element 440, the magnitude of the magnetic field force to which the particles are subjected in the sputtering area can be adjusted. Since the movement trajectory of the particles is directly related to the magnitude of the magnetic field force to which they are subjected, a larger magnetic field force will cause serious energy consumption, while a smaller magnetic field force will make it difficult for the particles to fall vertically into the wafer W. Therefore, the guiding device 400 can be pre-tested, and the intensity of the first sub-magnetic field loaded by the magnetic field forming component 440 can be adjusted to an appropriate range by observing the movement trajectory of the particles passing through the guiding device 400.
本申請實施例未限制磁場形成元件440的具體類型,其可以為永磁鐵,只要能夠對第一主體件410和第二主體件420產生磁化作用的元件即可。在另外的實施方式中,如圖7所示,本申請實施例的磁場形成元件440可選為電磁鐵元件,電磁鐵元件通過通斷電即可對第一子磁場進行控制,改變通入電流的大小即可控制第一子磁場的磁場強度,還可以通過改變電流方向(包括改變電磁鐵中線圈的纏繞方向)來改變第一子磁場的磁場方向,因此電磁鐵類型的磁場形成元件440無疑具有更便捷的操作性。The embodiment of the present application does not limit the specific type of the magnetic field forming element 440, which can be a permanent magnet, as long as it can generate a magnetization effect on the first main body 410 and the second main body 420. In another embodiment, as shown in FIG7 , the magnetic field forming element 440 of the embodiment of the present application can be selected as an electromagnetic iron element, which can control the first sub-magnetic field by turning on and off the power, and can control the magnetic field strength of the first sub-magnetic field by changing the size of the input current. The magnetic field direction of the first sub-magnetic field can also be changed by changing the direction of the current (including changing the winding direction of the coil in the electromagnetic iron), so the electromagnetic iron type magnetic field forming element 440 undoubtedly has more convenient operation.
無論磁場形成元件440是永磁鐵還是電磁鐵元件,其均可以與第一主體件410和第二主體件420通過直接連接來強化磁化效果。如圖4和圖5所示,磁場形成組件440的N磁極端與第一主體件410連接,第一主體件410被磁化後而形成N磁極,磁場形成元件440的S磁極端與第二主體件420連接,第二主體件420被磁化後而形成S磁極,此時,第一子磁場的磁場方向也是由第一主體件410至第二主體件420。Regardless of whether the magnetic field forming element 440 is a permanent magnet or an electromagnetic iron element, it can be directly connected to the first main body 410 and the second main body 420 to enhance the magnetization effect. As shown in Figures 4 and 5, the N magnetic pole end of the magnetic field forming component 440 is connected to the first main body 410, and the first main body 410 is magnetized to form an N magnetic pole. The S magnetic pole end of the magnetic field forming element 440 is connected to the second main body 420, and the second main body 420 is magnetized to form an S magnetic pole. At this time, the magnetic field direction of the first sub-magnetic field is also from the first main body 410 to the second main body 420.
本申請實施例未限制磁場形成元件440與第一主體件410和第二主體件420的具體連接關係,磁場形成元件440的N磁極端也可以與第二主體件420連接,磁場形成元件440的S磁極端也可以與第一主體件410連接。The embodiment of the present application does not limit the specific connection relationship between the magnetic field forming element 440 and the first main body 410 and the second main body 420. The N magnetic pole end of the magnetic field forming element 440 can also be connected to the second main body 420, and the S magnetic pole end of the magnetic field forming element 440 can also be connected to the first main body 410.
為了避免第一子磁場的各區域磁場強度存在較大的偏差,如圖4所示,本申請實施例的磁場形成元件440為電磁鐵元件,且為多個,全部電磁鐵元件設置於第一主體件410與第二主體件420之間,且沿第一主體件410的邊緣均勻佈置;全部電磁鐵元件通過相同的磁極端與第一主體件410連接,以使第一主體件410上形成第一磁極,全部電磁鐵元件通過相同的另一磁極端與第二主體件420連接,以使第二主體件420上形成第二磁極。In order to avoid large deviations in the magnetic field strength of each region of the first sub-magnetic field, as shown in FIG4 , the magnetic field forming element 440 of the embodiment of the present application is an electromagnetic iron element, and there are multiple electromagnetic iron elements, all of which are disposed between the first main body 410 and the second main body 420, and are evenly arranged along the edge of the first main body 410; all of the electromagnetic iron elements are connected to the first main body 410 through the same magnetic pole end to form a first magnetic pole on the first main body 410, and all of the electromagnetic iron elements are connected to the second main body 420 through the same other magnetic pole end to form a second magnetic pole on the second main body 420.
具體而言,由於全部的電磁鐵元件沿第一主體件410的邊緣均勻佈置,則全部的電磁鐵元件也是沿第二主體件420的邊緣均勻佈置,這樣就使得電磁鐵元件對第一主體件410和第二主體件420內部的磁疇施加分佈較為均勻的磁化作用,進而使得第一子磁場的磁場分佈較為均衡,有利於對粒子進行較為統一規律的調節作用。在本實施例中,全部電磁鐵元件通過N磁極端(或S磁極端)與第一主體件410連接,相應地,全部電磁鐵元件則通過S磁極端(或N磁極端)與第二主體件420連接。Specifically, since all the electromagnetic iron elements are evenly arranged along the edge of the first main body 410, all the electromagnetic iron elements are also evenly arranged along the edge of the second main body 420, so that the electromagnetic iron elements apply a more evenly distributed magnetization effect to the magnetic field inside the first main body 410 and the second main body 420, thereby making the magnetic field distribution of the first sub-magnetic field more balanced, which is conducive to a more uniform and regular regulation of the particles. In this embodiment, all the electromagnetic iron elements are connected to the first main body 410 through the N magnetic pole end (or the S magnetic pole end), and correspondingly, all the electromagnetic iron elements are connected to the second main body 420 through the S magnetic pole end (or the N magnetic pole end).
需要說明的是,本申請實施例未限制磁場形成元件440的具體數量,其可以為四個、七個、十個等。It should be noted that the embodiment of the present application does not limit the specific number of the magnetic field forming elements 440, which can be four, seven, ten, etc.
本申請實施例的導向裝置400還可以通過其他的方式來調節粒子所受到的導向作用,在另外的實施方式中,如圖8所示,本申請實施例的導向裝置400,其主體件為三個,分別為第一主體件410、第二主體件420和第三主體件430,第一主體件410、第二主體件420和第三主體件430由上至下依次間隔設置,開設在第一主體件410上的通孔為第一通孔H1,開設在第二主體件420上的通孔為第二通孔H2,第三主體件430開設有多個第三通孔,多個第一通孔H1、多個第二通孔H2和多個第三通孔一一對應,也即沿製程腔室100的高度方向上,第一通孔H1、第二通孔H2和第三通孔的投影都能夠相互重合。The guiding device 400 of the embodiment of the present application can also adjust the guiding effect on the particles in other ways. In another embodiment, as shown in Figure 8, the guiding device 400 of the embodiment of the present application has three main parts, namely a first main part 410, a second main part 420 and a third main part 430. The first main part 410, the second main part 420 and the third main part 430 are arranged in sequence from top to bottom. The through hole opened on the first main part 410 is the first through hole H1, and the through hole opened on the second main part 420 is the second through hole H2. The third main part 430 is provided with a plurality of third through holes. The plurality of first through holes H1, the plurality of second through holes H2 and the plurality of third through holes correspond to each other one by one, that is, along the height direction of the process chamber 100, the projections of the first through hole H1, the second through hole H2 and the third through hole can overlap with each other.
同時,第一主體件410、第二主體件420和第三主體件430均為導磁體,磁場形成組件為兩個,分別為第一磁場形成元件和第二磁場形成元件,其中,第一磁場形成元件用於磁化第一主體件410和第二主體件420,並使第一主體件410上形成第一磁極,以及使第二主體件420上形成第二磁極,且上述第一磁極與第二磁極相異,以在第一主體件410和第二主體件420之間形成第一子磁場;第二磁場形成元件用於磁化第二主體件420和第三主體件430,並使第二主體件420上形成第二磁極,以及使第三主體件430上形成第三磁極,且第二磁極與第三磁極相異,以在第二主體件420和第三主體件430之間載入第二子磁場。Meanwhile, the first main body 410, the second main body 420 and the third main body 430 are all magnetic conductors, and there are two magnetic field forming components, namely, a first magnetic field forming element and a second magnetic field forming element, wherein the first magnetic field forming element is used to magnetize the first main body 410 and the second main body 420, and to form a first magnetic pole on the first main body 410, and to form a second magnetic pole on the second main body 420, and the first magnetic pole is connected to the magnetic field of the first main body 410. The second magnetic poles are different to form a first sub-magnetic field between the first main body 410 and the second main body 420; the second magnetic field forming element is used to magnetize the second main body 420 and the third main body 430, and to form a second magnetic pole on the second main body 420, and to form a third magnetic pole on the third main body 430, and the second magnetic pole is different from the third magnetic pole to load a second sub-magnetic field between the second main body 420 and the third main body 430.
具體而言,如此設置下,第一主體件410、第二主體件420和第三主體件430具備導磁性能,第一磁場形成元件即可順利磁化第一主體件410和第二主體件420,而在第一主體件410和第二主體件420的相對側端面之間形成第一子磁場。第二磁場形成元件可順利磁化第二主體件420和第三主體件430,而在第二主體件420和第三主體件430的相對側端面形成第二子磁場;第二子磁場可設置為與第一子磁場的屬性相同,如此第二子磁場的磁感線分佈形貌也可以參照圖5。如此情況下,在粒子通過第一子磁場進行導向之後,粒子通過第二子磁場會被二次導向,第二子磁場可以彌補第一子磁場對粒子導向作用的不足,以確保粒子最終被導向為趨於垂直落入晶圓W。在該實施方式中,由於磁場形成元件440和磁場形成元件共同磁化第二主體件420,因此第二主體件420被磁化的速度會顯著加快。Specifically, under such a configuration, the first main body 410, the second main body 420 and the third main body 430 have magnetic conductivity, and the first magnetic field forming element can smoothly magnetize the first main body 410 and the second main body 420, and form a first sub-magnetic field between the opposite side end surfaces of the first main body 410 and the second main body 420. The second magnetic field forming element can smoothly magnetize the second main body 420 and the third main body 430, and form a second sub-magnetic field on the opposite side end surfaces of the second main body 420 and the third main body 430; the second sub-magnetic field can be configured to have the same properties as the first sub-magnetic field, so the magnetic flux distribution morphology of the second sub-magnetic field can also refer to FIG. 5. In this case, after the particles are guided by the first sub-magnetic field, the particles are guided again by the second sub-magnetic field, and the second sub-magnetic field can make up for the deficiency of the first sub-magnetic field in guiding the particles, so as to ensure that the particles are finally guided to fall vertically into the wafer W. In this embodiment, since the magnetic field forming element 440 and the magnetic field forming element jointly magnetize the second main body 420, the speed at which the second main body 420 is magnetized is significantly accelerated.
在可選的方案中,本申請實施例的第一主體件410和第二主體件420可以均為板狀結構件,且第一主體件410和第二主體件420相互平行。In an optional solution, the first main body 410 and the second main body 420 of the embodiment of the present application can both be plate-shaped structural members, and the first main body 410 and the second main body 420 are parallel to each other.
應理解的是,如此設置下,以導向裝置400用於形成電場(磁場)為例,其形成的電場(磁場)具有一定的規律性,具體可參見圖3(圖5),即在第一通孔H1和第二通孔H2對應的區域的電場(磁場)強度較低,而在第一通孔H1和第二通孔H2周圍的實體重合區域的電場(磁場)強度較高,整個導向裝置400存在規律化的電場(磁場)強度分佈,這樣能夠使得從不同第一通孔H1入射的粒子大致以同樣的角度形態從第二通孔H2出射,進而有利於對導向裝置400形成的電場(磁場)做出整體調節,能夠避免從不同第二通孔H2出射的粒子出射角度存在極大差異,而導致對導向裝置400形成的電場(磁場)做出整體調節而無法兼顧大部分粒子狀態的問題。It should be understood that, under such a setting, taking the guide device 400 used to form an electric field (magnetic field) as an example, the electric field (magnetic field) formed has a certain regularity, as shown in FIG. 3 (FIG. 5), that is, the electric field (magnetic field) intensity in the area corresponding to the first through hole H1 and the second through hole H2 is relatively low, while the electric field (magnetic field) intensity in the solid overlap area around the first through hole H1 and the second through hole H2 is relatively high, and the entire guide device 400 has a regular electric field. (Magnetic field) intensity distribution, so that particles incident from different first through holes H1 can be emitted from the second through holes H2 at roughly the same angle, which is beneficial to the overall adjustment of the electric field (magnetic field) formed by the guiding device 400, and can avoid the problem that there are great differences in the emission angles of particles emitted from different second through holes H2, resulting in the overall adjustment of the electric field (magnetic field) formed by the guiding device 400 and the inability to take into account the states of most particles.
當然,本申請實施例未限制第一主體件410和第二主體件420的具體構型,它們也可以為塊狀結構件等。Of course, the embodiment of the present application does not limit the specific configuration of the first main body 410 and the second main body 420, and they can also be block-shaped structural parts, etc.
無論是第一種導向裝置400,還是第二種導向裝置400,均可以通過增加導向裝置400的數量來強化粒子所受到的導向作用,具體地,如圖9所示,本申請實施例的導向裝置400可以為多個,每個導向裝置400均包括多個主體件(如圖9中的第一主體件410和第二主體件420等),多個導向裝置400由上至下依次間隔設置。Whether it is the first type of guiding device 400 or the second type of guiding device 400, the guiding effect on the particles can be enhanced by increasing the number of guiding devices 400. Specifically, as shown in Figure 9, the guiding device 400 of the embodiment of the present application can be multiple, and each guiding device 400 includes multiple main parts (such as the first main part 410 and the second main part 420 in Figure 9, etc.), and the multiple guiding devices 400 are arranged in sequence from top to bottom.
當導向裝置400用於形成電場時,在相鄰的兩個分屬不同導向裝置的主體件中,位於上方的主體件的電勢大於位於下方的主體件的電勢。具體地,如圖9所示,位於上方的導向裝置400中的第二主體件420的電勢大於位於下方的導向裝置400中的第一主體件410的電勢。在此種結構佈局下,全部導向裝置400形成的各個子電場均是沿製程腔室100的高度方向由上至下,也即全部子電場形成了定向的不間斷的電場組,這樣就使得粒子在從上至下通過多個導向裝置400的過程中,其會受到多個電場作用,以對粒子進行多次導向,後續的電場可彌補之前的電場對粒子施加導向作用的不足,以確保粒子最終被導向為趨於垂直落入晶圓W。When the guide device 400 is used to form an electric field, in two adjacent main parts belonging to different guide devices, the potential of the main part located at the top is greater than the potential of the main part located at the bottom. Specifically, as shown in FIG9 , the potential of the second main part 420 in the guide device 400 located at the top is greater than the potential of the first main part 410 in the guide device 400 located at the bottom. Under this structural layout, all the sub-electric fields formed by the guiding devices 400 are from top to bottom along the height direction of the process chamber 100, that is, all the sub-electric fields form a directional and uninterrupted electric field group. In this way, when the particles pass through multiple guiding devices 400 from top to bottom, they will be affected by multiple electric fields to guide the particles multiple times. The subsequent electric field can make up for the insufficient guiding effect of the previous electric field on the particles to ensure that the particles are finally guided to fall vertically into the wafer W.
當導向裝置400用於形成磁場時,在相鄰的兩個分屬不同導向裝置的主體件上形成的磁極相異。具體地,如圖9所示,位於上方的導向裝置400中的第二主體件420上形成的磁極與位於下方的導向裝置400中的第一主體件410上形成的磁極相異。在此種結構佈局下,不僅在導向裝置400內部形成用於對粒子進行導向調節的子磁場,相鄰導向裝置400之間也能夠形成子磁場,全部導向裝置400形成的子磁場形成了不間斷的磁場組,這樣就使得粒子在從上至下通過多個導向裝置400的過程中,其會受到多個磁場作用,以對粒子進行多次導向,後續的磁場可彌補之前的磁場對粒子施加導向作用的不足,以確保粒子最終被導向為趨於垂直落入晶圓W。When the guide device 400 is used to form a magnetic field, the magnetic poles formed on two adjacent main bodies belonging to different guide devices are different. Specifically, as shown in FIG9 , the magnetic poles formed on the second main body 420 in the upper guide device 400 are different from the magnetic poles formed on the first main body 410 in the lower guide device 400. Under this structural layout, not only is a sub-magnetic field for guiding and adjusting the particles formed inside the guiding device 400, but a sub-magnetic field can also be formed between adjacent guiding devices 400. The sub-magnetic fields formed by all the guiding devices 400 form an uninterrupted magnetic field group, so that the particles will be affected by multiple magnetic fields in the process of passing through multiple guiding devices 400 from top to bottom, so as to guide the particles multiple times. The subsequent magnetic field can make up for the insufficient guiding effect of the previous magnetic field on the particles, so as to ensure that the particles are finally guided to fall vertically into the wafer W.
由於靶材T在濺射粒子時存在不規則性,而通孔的數量較小,會導致粒子無法落入各通孔的幾率,這樣會造成靶材T的浪費、對各通孔的封堵。Since the target material T has irregularities when sputtering particles and the number of through holes is small, there is a probability that particles cannot fall into each through hole, which will cause waste of the target material T and blockage of each through hole.
基於此,在本申請實施例中,每個主體件上的通孔在主體件上呈蜂窩狀佈設,例如,如圖2所示,多個第一通孔H1在第一主體件410上可以呈蜂窩狀佈設,多個第二通孔H2在第二主體件420上可以呈蜂窩狀佈設。應理解的是,基於蜂窩狀的結構,各主體件相當於設置為網孔狀結構件,通孔的數量增加,且分佈緊密,各主體件上孔間的實體部分尺寸較小,如此設置無疑能夠有效確保粒子落入各通孔,而避免粒子沉積在主體件的實體部分。Based on this, in the embodiment of the present application, the through holes on each main body are arranged in a honeycomb shape on the main body. For example, as shown in FIG. 2 , a plurality of first through holes H1 can be arranged in a honeycomb shape on the first main body 410, and a plurality of second through holes H2 can be arranged in a honeycomb shape on the second main body 420. It should be understood that, based on the honeycomb structure, each main body is equivalent to being set as a mesh structure, the number of through holes is increased, and the distribution is dense, and the size of the solid part between the holes on each main body is smaller. Such a setting can undoubtedly effectively ensure that particles fall into each through hole and avoid particles from being deposited in the solid part of the main body.
在通孔為蜂窩狀構型時,每個通孔均可以呈正六邊形,但本申請實施例對通孔的具體形狀不做限制,它們也可以為正五邊形、正八邊形甚至不規則形狀等。When the through holes are in a honeycomb configuration, each through hole may be a regular hexagon, but the embodiment of the present application does not limit the specific shape of the through holes, and they may also be regular pentagons, regular octagons, or even irregular shapes.
本申請實施例未限制通孔的具體孔口寬度尺寸;但是,若通孔的孔口寬度值過大,則會導致減弱導向裝置400對粒子的導向作用,若通孔的孔口寬度值過小,則在長時間使用後粒子極容易封堵住通孔,這樣會使得導向裝置400的功能失效。基於此,在可選的方案中,本申請實施例的通孔的最大孔口寬度值範圍可以為大於等於30mm,且小於等於100mm;具體可選為35mm、50mm、75mm、90mm等。如此設置下,通孔的孔口寬度值既能夠避免其被封堵,又能夠兼顧導向裝置400的導向作用。The embodiment of the present application does not limit the specific aperture width size of the through hole; however, if the aperture width value of the through hole is too large, it will weaken the guiding effect of the guiding device 400 on the particles. If the aperture width value of the through hole is too small, the particles will easily block the through hole after long-term use, which will make the function of the guiding device 400 ineffective. Based on this, in an optional scheme, the maximum aperture width value range of the through hole in the embodiment of the present application can be greater than or equal to 30mm and less than or equal to 100mm; specifically, it can be selected as 35mm, 50mm, 75mm, 90mm, etc. Under such a setting, the aperture width value of the through hole can not only prevent it from being blocked, but also take into account the guiding effect of the guiding device 400.
在本申請實施例中,多個主體件的設置方式有多種,舉例來說,以主體件為兩個為例,如圖1所示,第一主體件410和第二主體件420的邊緣均外延形成有支撐部,該支撐部延伸至製程腔室100的底壁上。在另外的實施方式中,主體件還可以通過其周向邊緣與製程腔室100的內壁連接。例如,如圖1所示,第一主體件410可以通過其周向邊緣與製程腔室100的內壁連接,第二主體件420可以通過其周向邊緣與製程腔室100的內壁連接。In the embodiment of the present application, there are many ways to arrange the multiple main parts. For example, taking two main parts as an example, as shown in FIG1 , the edges of the first main part 410 and the second main part 420 are both extended to form a support portion, and the support portion extends to the bottom wall of the process chamber 100. In another embodiment, the main part can also be connected to the inner wall of the process chamber 100 through its circumferential edge. For example, as shown in FIG1 , the first main part 410 can be connected to the inner wall of the process chamber 100 through its circumferential edge, and the second main part 420 can be connected to the inner wall of the process chamber 100 through its circumferential edge.
應理解的是,如此設置下,粒子就不會存在從各主體件的周向邊緣與製程腔室100的內壁之間的間隙通過的情況,進而可確保全部粒子均受到導向裝置400的導向作用,以使得全部粒子均趨於垂直落入晶圓W;同時,各主體件上不需要設置額外的連接結構,簡化了各主體件的結構。It should be understood that, under such a configuration, particles will not pass through the gap between the circumferential edge of each main body and the inner wall of the process chamber 100, thereby ensuring that all particles are guided by the guiding device 400 so that all particles tend to fall vertically into the wafer W; at the same time, no additional connection structure is required on each main body, thereby simplifying the structure of each main body.
本申請實施例對電場的強度不做限制,本申請實施例的電場的電場強度範圍可以為大於等於1000V/m,且小於等於100000V/m,此時電場的電場強度範圍較為合適,此處的電場包括前述的由導向裝置產生的子電場。需要說明的是,若電場的電場強度小於1000V/m時,粒子受到的電場力較小而難以被導向至垂直落入晶圓W,若電場的電場強度大於100000V/m時,相鄰的兩個主體件(例如第一主體件410和第二主體件420)會因為電流超載而被擊穿。The embodiment of the present application does not limit the intensity of the electric field. The electric field intensity range of the embodiment of the present application can be greater than or equal to 1000V/m and less than or equal to 100000V/m. At this time, the electric field intensity range of the electric field is more suitable. The electric field here includes the aforementioned sub-electric field generated by the guiding device. It should be noted that if the electric field intensity of the electric field is less than 1000V/m, the electric field force on the particles is relatively small and it is difficult to be guided to fall vertically into the wafer W. If the electric field intensity of the electric field is greater than 100000V/m, two adjacent main parts (such as the first main part 410 and the second main part 420) will be broken down due to current overload.
在可選的方案中,如圖1所示,製程腔室100可以包括外腔體110和保護罩120,保護罩120將濺射區域與外腔體110隔開。如此設置下,保護罩120能夠將濺射製程限定在濺射區域中進行,以阻擋粒子濺射至外腔體110上,進而延長製程腔室100整體的使用壽命。In an optional solution, as shown in FIG1 , the process chamber 100 may include an outer chamber 110 and a protective cover 120, wherein the protective cover 120 separates the sputtering region from the outer chamber 110. In this configuration, the protective cover 120 can confine the sputtering process to the sputtering region to prevent particles from sputtering to the outer chamber 110, thereby extending the service life of the process chamber 100 as a whole.
結合各主體件通過周向邊緣連接製程腔室100的內壁的實施方式,各主體件可以通過周向邊緣直接與保護罩120的內壁連接。In combination with the implementation in which each main body is connected to the inner wall of the process chamber 100 via the peripheral edge, each main body can be directly connected to the inner wall of the protective cover 120 via the peripheral edge.
前述內容概括數項實施例之特徵,使得熟習此項技術者可更佳地理解本揭露之態樣。熟習此項技術者應瞭解,其等可容易地使用本揭露作為用於設計或修改用於實行本文仲介紹之實施例之相同目的及/或達成相同優點之其他製程及結構之一基礎。熟習此項技術者亦應瞭解,此等等效構造不背離本揭露之精神及範疇,且其等可在不背離本揭露之精神及範疇之情況下在本文中作出各種改變、置換及更改。The foregoing summarizes the features of several embodiments so that those skilled in the art can better understand the aspects of the present disclosure. Those skilled in the art should understand that they can easily use the present disclosure as a basis for designing or modifying other processes and structures for implementing the same purpose and/or achieving the same advantages of the embodiments described herein. Those skilled in the art should also understand that such equivalent structures do not depart from the spirit and scope of the present disclosure, and that they can make various changes, substitutions, and modifications herein without departing from the spirit and scope of the present disclosure.
100:製程腔室 110:外腔體 120:保護罩 200:承載基座 300:磁控濺射組件 310:磁控管 320:驅動機構 400:導向裝置 410:第一主體件 420:第二主體件 430:第三主體件 440:第一磁場形成組件 H1:第一通孔 H2:第二通孔 T:靶材 U1:第一電勢 U2:第二電勢 W:晶圓 100: Process chamber 110: External chamber 120: Protective cover 200: Carrier base 300: Magnetron sputtering assembly 310: Magnetron 320: Driving mechanism 400: Guide device 410: First main body 420: Second main body 430: Third main body 440: First magnetic field forming assembly H1: First through hole H2: Second through hole T: Target U1: First potential U2: Second potential W: Wafer
當結合附圖閱讀時,從以下詳細描述最佳理解本揭露之態樣。應注意,根據產業中之標準實踐,各種構件未按比例繪製。事實上,為了論述的清楚起見可任意增大或減小各種構件之尺寸。 圖1為本申請實施例公開的磁控濺射設備的結構示意圖; 圖2為本申請實施例公開的導向裝置的俯視圖; 圖3為圖2中A-A向的第一種導向裝置的剖視圖; 圖4為本申請實施例公開的第二種導向裝置的結構示意圖; 圖5為圖2中A-A向的第二種導向裝置的剖視圖; 圖6為本申請實施例公開的第二種導向裝置對粒子進行導向的原理示意圖; 圖7為本申請實施例公開的磁場形成元件的結構示意圖; 圖8為本申請實施例公開的導向裝置包括三個主體件的結構示意圖; 圖9為本申請實施例公開的磁控濺射設備包括多個導向裝置的結構示意圖。 The present disclosure is best understood from the following detailed description when read in conjunction with the accompanying drawings. It should be noted that, in accordance with standard practice in the industry, the various components are not drawn to scale. In fact, the dimensions of the various components may be arbitrarily increased or decreased for clarity of discussion. Figure 1 is a schematic diagram of the structure of the magnetron sputtering device disclosed in the embodiment of the present application; Figure 2 is a top view of the guiding device disclosed in the embodiment of the present application; Figure 3 is a cross-sectional view of the first guiding device in the A-A direction in Figure 2; Figure 4 is a schematic diagram of the structure of the second guiding device disclosed in the embodiment of the present application; Figure 5 is a cross-sectional view of the second guiding device in the A-A direction in Figure 2; Figure 6 is a schematic diagram of the principle of the second guiding device disclosed in the embodiment of the present application guiding particles; Figure 7 is a schematic diagram of the structure of the magnetic field forming element disclosed in the embodiment of the present application; Figure 8 is a schematic diagram of the structure of the guiding device disclosed in the embodiment of the present application including three main parts; Figure 9 is a schematic diagram of the structure of the magnetron sputtering device disclosed in the embodiment of the present application including multiple guiding devices.
410:第一主體件 410: First main body
420:第二主體件 420: Second main body
H1:第一通孔 H1: First through hole
H2:第二通孔 H2: Second through hole
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| US20110048927A1 (en) * | 2008-06-26 | 2011-03-03 | Naoki Morimoto | Sputtering apparatus and sputtering method |
| JP2016117923A (en) * | 2014-12-19 | 2016-06-30 | 株式会社アルバック | Sputtering apparatus |
| TW201803641A (en) * | 2016-07-20 | 2018-02-01 | 應用材料股份有限公司 | Physical vapor deposition plasma energy control controlled by dynamic magnetron |
| CN111155068A (en) * | 2020-04-02 | 2020-05-15 | 上海陛通半导体能源科技股份有限公司 | Physical vapor deposition pore filling equipment |
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| AU6977998A (en) * | 1997-04-21 | 1998-11-13 | Tokyo Electron Arizona, Inc. | Method and apparatus for ionized sputtering of materials |
| US6692617B1 (en) * | 1997-05-08 | 2004-02-17 | Applied Materials, Inc. | Sustained self-sputtering reactor having an increased density plasma |
| US6579421B1 (en) * | 1999-01-07 | 2003-06-17 | Applied Materials, Inc. | Transverse magnetic field for ionized sputter deposition |
| JP4031691B2 (en) * | 2002-09-20 | 2008-01-09 | 東京エレクトロン株式会社 | Plasma processing apparatus and plasma processing method |
| TWI229908B (en) * | 2004-03-08 | 2005-03-21 | Univ Nat Chiao Tung | Adjustable collimator and sputtering apparatus with the same |
| US7695590B2 (en) * | 2004-03-26 | 2010-04-13 | Applied Materials, Inc. | Chemical vapor deposition plasma reactor having plural ion shower grids |
| JP2015117400A (en) * | 2013-12-17 | 2015-06-25 | 昭和電工株式会社 | Carbon film forming device, carbon film forming method, and method for manufacturing magnetic recording medium |
| KR102383703B1 (en) * | 2016-03-05 | 2022-04-08 | 어플라이드 머티어리얼스, 인코포레이티드 | Methods and apparatus for controlling ion fraction in physical vapor deposition processes |
| JP6122169B1 (en) * | 2016-03-15 | 2017-04-26 | 株式会社東芝 | Processing device and collimator |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| US20110048927A1 (en) * | 2008-06-26 | 2011-03-03 | Naoki Morimoto | Sputtering apparatus and sputtering method |
| JP2016117923A (en) * | 2014-12-19 | 2016-06-30 | 株式会社アルバック | Sputtering apparatus |
| TW201803641A (en) * | 2016-07-20 | 2018-02-01 | 應用材料股份有限公司 | Physical vapor deposition plasma energy control controlled by dynamic magnetron |
| CN111155068A (en) * | 2020-04-02 | 2020-05-15 | 上海陛通半导体能源科技股份有限公司 | Physical vapor deposition pore filling equipment |
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