TW201621979A - Wafer tray for MOCVD reaction system - Google Patents

Wafer tray for MOCVD reaction system Download PDF

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TW201621979A
TW201621979A TW104128059A TW104128059A TW201621979A TW 201621979 A TW201621979 A TW 201621979A TW 104128059 A TW104128059 A TW 104128059A TW 104128059 A TW104128059 A TW 104128059A TW 201621979 A TW201621979 A TW 201621979A
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wafer
wafer carrier
sub
gas
recessed
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TWI590300B (en
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Takiguchi Haruhisa
Ning Zhou
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Advanced Micro Fab Equip Inc
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Abstract

The present invention provides a wafer tray for a MOCVD reaction system. An upper surface of said wafer tray includes a first sub-surface and a second sub-surface. A first structure on which wafers are placed is arranged on the first sub-surface. A second structure is installed on the second sub-surface. Said second structure enlarges the area of the second sub-surface such that a reaction rate constant between the reaction gas and the second sub-surface of the wafer tray is equal to the reaction rate constant between the reaction gas and the wafer surface. As such, with the wafer tray provided by this invention, the gas concentration above the wafer perimeter close to a front end of the gas rotation direction is ensured to be equal to the gas concentrations above other areas. Thus, the reaction rates on the entire wafer surface can be ensured to be identical, which in turn assures that the crystal materials grown on the entire surface of the wafer have the same thickness.

Description

用於MOCVD反應系統的晶圓載盤Wafer carrier for MOCVD reaction system

本發明涉及半導體加工設備領域,尤其一種用於MOCVD反應系統的晶圓載盤。The present invention relates to the field of semiconductor processing equipment, and more particularly to a wafer carrier for an MOCVD reaction system.

對於生長的薄層晶體材料,其重要的指標是厚度的均勻性和組分比例的均勻性。為了保證生長的晶體材料達到這些指標,在MOCVD技術中,必須使晶體材料在整個晶圓表面上具有均勻的生長速率。For the growth of thin layer crystalline materials, important indicators are the uniformity of the thickness and the uniformity of the composition ratio. In order to ensure that the growing crystalline material meets these specifications, in MOCVD technology, it is necessary to have a uniform growth rate of the crystalline material over the entire wafer surface.

由於晶體材料在晶圓表面上的生長速率與晶圓上方的反應氣體的濃度呈正比。為了保證晶體材料在整個晶圓表面上具有均勻的生長速率,就需要整個晶圓表面上方的反應氣體的濃度在各個晶圓表面位置處保持一致。Since the growth rate of the crystalline material on the surface of the wafer is proportional to the concentration of the reactive gas above the wafer. In order to ensure a uniform growth rate of the crystal material over the entire wafer surface, it is required that the concentration of the reactive gas over the entire wafer surface be uniform at the respective wafer surface locations.

需要說明的是,在採用MOCVD技術對晶圓表面上生長晶體材料時,要將晶圓放置在晶圓載盤上的用於放置晶圓的凹槽內。由於晶圓載盤的材料與晶圓的材料不同,使得晶圓載盤表面消耗反應氣體的反應常數小於晶圓表面消耗反應氣體的反應常數,由於晶圓載盤和晶圓表面上方的氣體濃度是相同的,所以導致晶圓載盤表面與氣體的反應速率小於晶圓表面與氣體的反應速率,從而導致晶圓載盤表面消耗的氣體量小於晶圓表面消耗的氣體量,進而使得反應後的晶圓載盤表面上方的反應氣體濃度大於晶圓表面上方的反應氣體濃度。It should be noted that when the crystal material is grown on the surface of the wafer by MOCVD technology, the wafer is placed in a groove on the wafer carrier for placing the wafer. Since the material of the wafer carrier is different from the material of the wafer, the reaction constant of the reaction gas on the wafer carrier surface is smaller than the reaction constant of the reaction gas on the wafer surface, because the gas concentration above the wafer carrier and the wafer surface is the same. Therefore, the reaction rate between the surface of the wafer carrier and the gas is smaller than the reaction rate between the surface of the wafer and the gas, so that the amount of gas consumed on the surface of the wafer carrier is smaller than the amount of gas consumed on the surface of the wafer, thereby causing the surface of the wafer carrier after the reaction. The concentration of the reaction gas above is greater than the concentration of the reactant gas above the surface of the wafer.

而在實際MOCVD技術過程中,晶圓載盤是轉動的,這就相當於晶圓載盤上方的氣體流是旋轉氣體流。因而流向晶圓表面的氣體流可以等效為兩個方向的氣體流,一個是來自頂部的竪直流向的氣體流,該氣體流由氣體噴淋頭噴出;另外一個是從晶圓載盤流向晶圓邊緣的水平方向的氣體流。由於晶圓載盤表面上方的氣體濃度大於晶圓表面上方的氣體濃度,所以,靠近氣體旋轉方向前端的晶圓邊緣的氣體濃度大於晶圓其它區域的氣體濃度,又因為,生長速率與氣體濃度成正比關係,所以,靠近氣體旋轉方向前端的晶圓邊緣的生長速率大於晶圓其它區域的生長速率。第1圖為形成生長速率不均勻的原因的簡易圖。In the actual MOCVD technology process, the wafer carrier is rotated, which is equivalent to the flow of gas above the wafer carrier is a rotating gas flow. Thus, the flow of gas to the surface of the wafer can be equivalent to a gas flow in two directions, one being a vertical direct flow of gas from the top, which is ejected by a gas showerhead; the other is flowing from the wafer carrier to the crystal. The horizontal flow of gas at the edge of the circle. Since the gas concentration above the wafer carrier surface is greater than the gas concentration above the wafer surface, the gas concentration at the edge of the wafer near the front end of the gas rotation direction is greater than the gas concentration in other regions of the wafer, and because the growth rate and gas concentration are In a proportional relationship, the growth rate of the edge of the wafer near the front end of the gas rotation direction is greater than the growth rate of other areas of the wafer. Fig. 1 is a simplified diagram showing the cause of uneven growth rate.

為了解決上述技術問題,本發明採用了如下技術方案:In order to solve the above technical problems, the present invention adopts the following technical solutions:

一種用於MOCVD反應系統的晶圓載盤,所述晶圓載盤的上表面包括第一子表面和第二子表面,在所述第一子表面上設置有用於放置晶圓的第一結構,在所述第二子表面上設置有第二結構,所述第二結構能夠增大所述第二子表面的面積,使反應氣體與晶圓載盤的第二子表面的反應速率常數等於反應氣體與晶圓表面的反應速率常數。A wafer carrier for an MOCVD reaction system, the upper surface of the wafer carrier including a first sub-surface and a second sub-surface, on which the first structure for placing a wafer is disposed, The second sub-surface is provided with a second structure capable of increasing the area of the second sub-surface such that the reaction rate constant of the reaction gas and the second sub-surface of the wafer carrier is equal to the reaction gas and The reaction rate constant of the wafer surface.

較佳地,所述設置有所述第二結構的第二子表面的面積與所述未設置有所述第二結構的第二子表面的面積的比值範圍在1.05~1.15之間。Preferably, the ratio of the area of the second sub-surface provided with the second structure to the area of the second sub-surface not provided with the second structure ranges between 1.05 and 1.15.

較佳地,所述第二結構為凹陷結構和/或突起結構。Preferably, the second structure is a recessed structure and/or a raised structure.

較佳地,所述第二結構為複數個,當所述第二結構為凹陷結構時,每一個所述凹陷結構為凹陷腔體,所述凹陷腔體的形狀為半球;當所述第二結構為突起結構時,每一個所述突起結構的形狀為半球。Preferably, the second structure is plural. When the second structure is a recessed structure, each of the recessed structures is a recessed cavity, and the shape of the recessed cavity is a hemisphere; When the structure is a protruding structure, each of the protruding structures has a shape of a hemisphere.

較佳地,所述半球的半徑與深度相同,或者所述半球的半徑大於深度。Preferably, the radius of the hemisphere is the same as the depth, or the radius of the hemisphere is greater than the depth.

較佳地,當所述第二結構為凹陷結構時,所述凹陷結構為凹溝,當所述第二結構為突起結構時,所述突起結構為突出條。Preferably, when the second structure is a concave structure, the concave structure is a concave groove, and when the second structure is a protruding structure, the protruding structure is a protruding strip.

較佳地,所述凹陷結構為多條環狀凹溝,每條環狀凹溝與所述晶圓載盤的中心相同。Preferably, the recessed structure is a plurality of annular grooves, each annular groove being the same as the center of the wafer carrier.

較佳地,所述突起結構為多條環狀突出條,每條環狀突出條與所述晶圓載盤的中心相同。Preferably, the protruding structure is a plurality of annular protruding strips, each annular protruding strip being the same as the center of the wafer carrier.

較佳地,所述凹陷結構為多條凹溝,所述突起結構為多條突出條,每條所述突出條或每條所述凹溝從所述晶圓載盤的中心沿徑向方向延伸。Preferably, the recessed structure is a plurality of recessed grooves, and the protruding structure is a plurality of protruding strips, each of the protruding strips or each of the recessed grooves extending in a radial direction from a center of the wafer carrier .

較佳地,沿徑向方向延伸的所述突出條或所述凹溝向同一方向傾斜。Preferably, the protruding strips or the grooves extending in the radial direction are inclined in the same direction.

較佳地,所述第一結構為複數個,在部分所述第一結構的內部設置有所述第二結構。Preferably, the first structure is plural, and the second structure is disposed inside a part of the first structure.

一種用於MOCVD反應系統的晶圓載盤,所述晶圓載盤的上表面包括多個向下凹陷的安裝區,所述安裝區用於安裝待處理晶圓,所述安裝區之間包括隔離區,以使所述安裝區之間互相隔離,所述隔離區的上表面包括至少一個凹陷結構或突起結構,所述凹陷結構或突起結構使得所述隔離區上表面的面積與所述隔離區向下投影的平面面積的比值在1.05-1.15之間。A wafer carrier for an MOCVD reaction system, the upper surface of the wafer carrier includes a plurality of downwardly recessed mounting regions for mounting wafers to be processed, and an isolation region between the mounting regions So that the mounting regions are isolated from each other, the upper surface of the isolation region includes at least one recessed structure or a protruding structure, the recessed structure or the protruding structure such that the area of the upper surface of the isolation region and the isolation region The ratio of the planar area of the lower projection is between 1.05 and 1.15.

相較於現有技術,本發明具有以下有益效果:Compared with the prior art, the present invention has the following beneficial effects:

本發明提供的用於MOCVD反應系統的晶圓載盤,在未設置用於放置晶圓的第一結構的第二子表面上設置有第二結構,該第二結構能夠增大第二子表面的面積。相較於未設置第二結構的第二子表面的面積,本發明提供的晶圓載盤的第二子表面的面積較大,該增大的表面積能夠增大晶圓載盤表面與反應氣體的反應速率常數。藉由調整第二子表面的面積能夠使晶圓載盤表面與反應氣體的反應速率常數等於晶圓表面與反應氣體的反應速率常數,從而能夠使晶圓載盤表面與氣體的反應速率等於晶圓表面與氣體的反應速率,從而使得晶圓載盤表面消耗的氣體量等於晶圓表面消耗的氣體量,進一步使得反應後的晶圓載盤表面上方的反應氣體濃度等於晶圓表面上方的反應氣體濃度。因而也就不會出現濃度較大的晶圓載盤表面上方的氣體向晶圓表面上方擴散的現象,從而不會導致靠近氣體旋轉方向前端的晶圓邊緣上方的氣體濃度大於晶圓其它區域上方的氣體濃度。因而,藉由本發明提供的晶圓載盤,能夠保證靠近氣體旋轉方向前端的晶圓邊緣上方的氣體濃度與其它區域上方的氣體濃度相等,從而能夠保證晶圓整個表面上的反應速率均相等,進一步保證生長在晶圓整個表面上的晶體材料的厚度相同。The wafer carrier for an MOCVD reaction system provided by the present invention is provided with a second structure on a second sub-surface on which the first structure for placing the wafer is not disposed, the second structure capable of increasing the second sub-surface area. Compared with the area of the second sub-surface where the second structure is not disposed, the second sub-surface of the wafer carrier provided by the present invention has a larger area, and the increased surface area can increase the reaction between the surface of the wafer carrier and the reaction gas. Rate constant. By adjusting the area of the second sub-surface, the reaction rate constant of the wafer carrier surface and the reaction gas can be made equal to the reaction rate constant of the wafer surface and the reaction gas, so that the reaction rate between the wafer carrier surface and the gas can be equal to the wafer surface. The reaction rate with the gas is such that the amount of gas consumed on the surface of the wafer carrier is equal to the amount of gas consumed on the surface of the wafer, further allowing the concentration of the reactive gas above the surface of the wafer carrier after the reaction to be equal to the concentration of the reactive gas above the surface of the wafer. Therefore, the phenomenon that the gas above the surface of the wafer carrier having a large concentration spreads above the surface of the wafer does not occur, so that the gas concentration above the edge of the wafer near the front end of the gas rotation direction is not greater than that above the other areas of the wafer. Gas concentration. Therefore, the wafer carrier provided by the present invention can ensure that the gas concentration above the edge of the wafer near the front end of the gas rotation direction is equal to the gas concentration above the other regions, thereby ensuring that the reaction rates on the entire surface of the wafer are equal, further Ensure that the thickness of the crystalline material grown on the entire surface of the wafer is the same.

正如背景技術部分所述,MOCVD是以III族、II族元素的有機化合物和V、VI族元素的氫化物等作為晶體生成源材料,以熱分解反應方式在晶圓上進行氣相外延、生長各種III-V族、II-VI族化合物半導體以及它們的多元固熔體的薄層晶體材料。As described in the background section, MOCVD is a crystal generation source material of an organic compound of a group III or a group II element and a hydride of a group V or a group VI element, and is subjected to vapor phase epitaxy and growth on a wafer by thermal decomposition reaction. A variety of III-V, II-VI compound semiconductors and their thin-layer crystalline materials of multiple solid solution.

下面以氮化鎵GaN晶體材料的生長為例結合第2圖至第3圖說明晶體材料GaN在晶圓上的生長機制。第2圖為在氣相中氣體流動和化學反應機構示意圖;第3圖是GaN在晶圓表面上生長的反應機構示意圖。需要說明的是,MOCVD技術可以實現在晶圓表面上生長多種晶體材料,不限於本發明實施例所述的氮化鎵晶體。The growth mechanism of the crystalline material GaN on the wafer will be described below by taking the growth of the gallium nitride GaN crystal material as an example in conjunction with FIGS. 2 to 3. Figure 2 is a schematic diagram of the gas flow and chemical reaction mechanism in the gas phase; Figure 3 is a schematic diagram of the reaction mechanism of GaN growth on the wafer surface. It should be noted that the MOCVD technology can realize the growth of a plurality of crystal materials on the surface of the wafer, and is not limited to the gallium nitride crystal described in the embodiments of the present invention.

如第2圖所示,氣體源三甲基鎵TMG與氣體載體H2或N2從噴淋頭噴出,在溫度達到大約100℃時,TMG開始熱分解生成單甲基鎵MMG。當溫度升到大約500℃時,TMG在化學界面層CBL(chemical boundary layer)開始分解生成單甲基鎵MMG。在溫度高於500℃時,MMG與NH3 反應生成氣體GaN。氣體GaN擴散進入靠近晶圓表面的區域,其擴散係數為As shown in Fig. 2, the gas source trimethylgallium TMG and the gas carrier H2 or N2 are ejected from the shower head, and when the temperature reaches about 100 ° C, TMG starts to thermally decompose to form monomethyl gallium MMG. When the temperature rises to about 500 ° C, TMG begins to decompose at the chemical boundary layer CBL to form monomethyl gallium MMG. At temperatures above 500 ° C, MMG reacts with NH 3 to form gaseous GaN. Gas GaN diffuses into a region near the surface of the wafer with a diffusion coefficient of .

如第3圖所示,氣體GaN擴散到表面反應界面,在該表面反應界面處,部分氣體GaN分子發生固化沉積到晶圓表面上。As shown in Fig. 3, the gas GaN diffuses to the surface reaction interface where a portion of the gas GaN molecules are solidified and deposited on the surface of the wafer.

當達到穩定狀態時,從噴流頭噴出的氣體GaN的流量與在晶圓表面消耗的GaN的流量相等。用公式表示如下:; 其中,為氣體擴散係數;為在化學界面層上方的氣相分子濃度;為在晶圓表面上方的氣體濃度;為晶圓表面上的異質反應速率常數; GaN(g):氣相GaN; GaN(s):固相GaN。When the steady state is reached, the flow rate of the gas GaN ejected from the jet head is equal to the flow rate of GaN consumed on the surface of the wafer. Formulated as follows: ; ; ; among them, Is the gas diffusion coefficient; Is the gas phase molecular concentration above the chemical interface layer; For the gas concentration above the wafer surface; Is the heterogeneous reaction rate constant on the wafer surface; GaN (g): vapor phase GaN; GaN (s): solid phase GaN.

需要說明的是,晶體材料的生長速率與氣相分子濃度、以及成正比。It should be noted that the growth rate of the crystal material and the gas phase molecular concentration, as well as In direct proportion.

用於MOCVD反應系統包括晶圓載盤,其上表面上設置有用於放置晶圓的凹槽。當採用MOCVD反應系統在晶圓上生長晶體材料時,需要將晶圓放置在晶圓載盤的用於放置晶圓的凹槽內。由於凹槽僅占晶圓載盤的部分區域,所以,MOCVD技術過程中,未設置凹槽的那部分區域的晶圓載盤的上表面也被反應氣體所籠罩。為了描述方便,將設置有用於放置晶圓的凹槽的表面定義為第一子表面,將除所述第一子表面的上表面的其它表面定義為第二子表面。當MOCVD技術進行時,反應氣體籠罩在整個晶圓載盤的上表面上方。這樣在晶體生長在晶圓表面上的同時,晶體也會在晶圓載盤的第二子表面上生長。其反生長機制示意圖如第4圖所示。設定:分別為從反應氣體氣相區域流向晶圓載盤和晶圓的氣體流量;分別為在晶圓載盤表面和晶圓表面上發生反應所消耗的氣體流量;為氣體擴散係數;為在化學界面層上方的氣相分子濃度;分別為在晶圓載盤和晶圓表面上方的氣體濃度;分別為晶圓載盤和晶圓表面上的異質反應速率常數。 在晶圓載盤的第二子表面上方:(1)(2) 在晶圓表面上方:(3)(4) 一般情况下,>>,那麽,(5)(6); 又因為在穩定狀態下,流入的氣體流量等於消耗的氣體流量,所以,(7) 一般情况下,,所以,(8)。The MOCVD reaction system includes a wafer carrier on which an upper surface is provided with a recess for placing a wafer. When a crystal material is grown on a wafer using an MOCVD reaction system, the wafer needs to be placed in a recess of the wafer carrier for placing the wafer. Since the groove only occupies a part of the wafer carrier, the upper surface of the wafer carrier in the portion where the groove is not provided is also covered by the reaction gas during the MOCVD technique. For convenience of description, a surface provided with a groove for placing a wafer is defined as a first sub-surface, and other surfaces other than an upper surface of the first sub-surface are defined as a second sub-surface. When the MOCVD technique is performed, the reactive gas is enveloped over the upper surface of the entire wafer carrier. Thus, while the crystal is grown on the surface of the wafer, the crystal also grows on the second subsurface of the wafer carrier. The schematic diagram of its anti-growth mechanism is shown in Figure 4. set up: , The flow of gas from the gas phase region of the reactive gas to the wafer carrier and the wafer, respectively; , The flow of gas consumed by the reaction on the wafer carrier surface and the wafer surface, respectively; Is the gas diffusion coefficient; Is the gas phase molecular concentration above the chemical interface layer; , The gas concentration above the wafer carrier and wafer surface; , The heterogeneous reaction rate constants on the wafer carrier and wafer surface, respectively. Above the second subsurface of the wafer carrier: (1) (2) Above the wafer surface: (3) (4) Under normal circumstances, >> or , then, (5) (6); and because in steady state, the inflowing gas flow rate is equal to the gas flow rate consumed, therefore, (7) Under normal circumstances, < ,and so, > (8).

在實際MOCVD技術過程中,晶圓載盤是轉動的,這就相當於晶圓載盤上方的氣體流是旋轉氣體流。因而流向晶圓表面的氣體流可以等效為兩個方向的氣體流,一個是來自頂部的竪直流向的氣體流,該氣體流由氣體噴淋頭噴出;另外一個是從晶圓載盤流向晶圓邊緣的水平方向的氣體流。由於晶圓載盤表面上方的氣體濃度大於晶圓表面上方的氣體濃度,所以,靠近氣體旋轉方向前端的晶圓邊緣的氣體濃度大於晶圓其它區域的氣體濃度,又因為,生長速率與氣體濃度成正比關係,所以,靠近氣體旋轉方向前端的晶圓邊緣的生長速率大於晶圓其它區域的生長速率,這種現象可以稱為“leading edge”。In the actual MOCVD process, the wafer carrier is rotated, which is equivalent to the flow of gas above the wafer carrier being a rotating gas stream. Thus, the flow of gas to the surface of the wafer can be equivalent to a gas flow in two directions, one being a vertical direct flow of gas from the top, which is ejected by a gas showerhead; the other is flowing from the wafer carrier to the crystal. The horizontal flow of gas at the edge of the circle. Since the gas concentration above the wafer carrier surface is greater than the gas concentration above the wafer surface, the gas concentration at the edge of the wafer near the front end of the gas rotation direction is greater than the gas concentration in other regions of the wafer, and because the growth rate and gas concentration are In a proportional relationship, the growth rate of the edge of the wafer near the front end of the gas rotation direction is greater than the growth rate of other areas of the wafer. This phenomenon can be called "leading edge".

為了防止靠近氣體旋轉方向前端的晶圓邊緣的生長速率大於晶圓其它區域的生長速率,需要抑制晶圓載盤上方的氣體較大的濃度。這就需要使晶圓載盤消耗與晶圓相同量的氣體量。也就是說,需要使反應氣體與晶圓載盤的反應速率等於反應氣體與晶圓的反應速率。由於在反應前,晶圓載盤表面上方的氣體濃度與晶圓表面上方的氣體濃度相等,所以要使兩者的反應速率相等,需要使反應氣體與晶圓載盤表面反應的速率常數等於反應氣體與晶圓表面反應的速率常數。In order to prevent the growth rate of the wafer edge near the front end of the gas rotation direction from being greater than the growth rate of other regions of the wafer, it is necessary to suppress a large concentration of gas above the wafer carrier. This requires the wafer carrier to consume the same amount of gas as the wafer. That is, it is necessary to make the reaction rate of the reaction gas and the wafer carrier equal to the reaction rate of the reaction gas and the wafer. Since the gas concentration above the wafer carrier surface is equal to the gas concentration above the wafer surface before the reaction, so that the reaction rates of the two are equal, the rate constant for reacting the reaction gas with the wafer carrier surface is equal to the reaction gas and The rate constant of the wafer surface reaction.

為了實現上述目的,本發明提供了一種用於MOCVD反應系統的晶圓載盤。如第5圖所示,晶圓載盤500的上表面包括第一子表面和第二子表面,在第一子表面上設置有用於放置晶圓的第一結構501,在第二子表面上設置有第二結構502,該第二結構502能夠增大第二子表面的面積,從而使本發明實施例設置有第二結構502的第二子表面的面積大於未設置第二結構502的第二子表面的面積。相較於常規結構的第二子表面與反應氣體的反應速率常數,設置有第二結構的第二子表面與反應氣體的反應速率常數增大,並且能夠使該反應速率常數等於晶圓表面與反應氣體的反應速率常數。需要說明的是,常規結構的第二子表面為平整表面。In order to achieve the above object, the present invention provides a wafer carrier for an MOCVD reaction system. As shown in FIG. 5, the upper surface of the wafer carrier 500 includes a first sub-surface and a second sub-surface, on the first sub-surface, a first structure 501 for placing a wafer, and a second sub-surface disposed on the second sub-surface There is a second structure 502, which can increase the area of the second sub-surface, so that the area of the second sub-surface provided with the second structure 502 in the embodiment of the present invention is larger than the second area in which the second structure 502 is not disposed. The area of the subsurface. Compared with the reaction rate constant of the second sub-surface of the conventional structure and the reaction gas, the reaction rate constant of the second sub-surface provided with the second structure and the reaction gas is increased, and the reaction rate constant can be made equal to the wafer surface and The reaction rate constant of the reaction gas. It should be noted that the second sub-surface of the conventional structure is a flat surface.

需要說明的是,本發明實施例所述的晶圓載盤的上表面是指在MOCVD技術時朝向反應氣體的表面。在本發明實施例中,晶圓載盤的材質可以為石墨。It should be noted that the upper surface of the wafer carrier according to the embodiment of the present invention refers to the surface facing the reaction gas in the MOCVD technology. In the embodiment of the present invention, the material of the wafer carrier may be graphite.

由於晶圓載盤的第二子表面的面積增大,從而增大了晶圓載盤表面與反應氣體的反應速率常數。藉由調整第二子表面的面積能夠使晶圓載盤表面與反應氣體的反應速率常數等於晶圓表面與反應氣體的反應速率常數,從而能夠使晶圓載盤表面與氣體的反應速率等於晶圓表面與氣體的反應速率,從而使得晶圓載盤表面消耗的氣體量等於晶圓表面消耗的氣體量,進一步使得反應後的晶圓載盤表面上方的反應氣體濃度等於晶圓表面上方的反應氣體濃度。因而也就不會出現濃度較大的晶圓載盤表面上方的氣體向晶圓表面上方擴散的現象,從而不會導致靠近氣體旋轉方向前端的晶圓邊緣上方的氣體濃度大於晶圓其它區域上方的氣體濃度。因而,藉由本發明提供的晶圓載盤,能夠保證靠近氣體旋轉方向前端的晶圓邊緣上方的氣體濃度與其它區域上方的氣體濃度相等,從而能夠保證晶圓整個表面上的反應速率均相等,進一步能夠保證生長在晶圓整個表面上的晶體材料的厚度相同。As the area of the second sub-surface of the wafer carrier increases, the reaction rate constant of the wafer carrier surface and the reactive gas is increased. By adjusting the area of the second sub-surface, the reaction rate constant of the wafer carrier surface and the reaction gas can be made equal to the reaction rate constant of the wafer surface and the reaction gas, so that the reaction rate between the wafer carrier surface and the gas can be equal to the wafer surface. The reaction rate with the gas is such that the amount of gas consumed on the surface of the wafer carrier is equal to the amount of gas consumed on the surface of the wafer, further allowing the concentration of the reactive gas above the surface of the wafer carrier after the reaction to be equal to the concentration of the reactive gas above the surface of the wafer. Therefore, the phenomenon that the gas above the surface of the wafer carrier having a large concentration spreads above the surface of the wafer does not occur, so that the gas concentration above the edge of the wafer near the front end of the gas rotation direction is not greater than that above the other areas of the wafer. Gas concentration. Therefore, the wafer carrier provided by the present invention can ensure that the gas concentration above the edge of the wafer near the front end of the gas rotation direction is equal to the gas concentration above the other regions, thereby ensuring that the reaction rates on the entire surface of the wafer are equal, further It is ensured that the thickness of the crystal material grown on the entire surface of the wafer is the same.

更進一步地說,第二子表面的面積也不是越大越好,如果第二子表面的面積太大,有可能會出現,晶圓載盤表面與反應氣體的反應速率常數大於晶圓表面與反應氣體的反應速率常數,從而也會出現反應速率不均勻的現象。所以,作為本發明的一個優選實施例,將設置有第二結構的第二子表面的面積與未設置有第二結構的第二子表面的面積的比值限定在一定範圍內。經過試驗驗證,該面積比值的範圍優選在1.05~1.15之間。在該範圍內,晶圓載盤表面與反應氣體的反應速率常數與晶圓表面與反應氣體的反應速率常數大致相同,進而能夠保證晶圓載盤消耗的氣體量與晶圓表面消耗的氣體量大致相同,能夠取得較好的效果。Furthermore, the area of the second sub-surface is not as large as possible. If the area of the second sub-surface is too large, it may occur that the reaction rate constant of the wafer carrier surface and the reaction gas is larger than the surface of the wafer and the reaction gas. The reaction rate constant, and thus the phenomenon of uneven reaction rate. Therefore, as a preferred embodiment of the present invention, the ratio of the area of the second sub-surface provided with the second structure to the area of the second sub-surface not provided with the second structure is limited to a certain range. It has been experimentally verified that the area ratio is preferably in the range of 1.05 to 1.15. Within this range, the reaction rate constant of the wafer carrier surface and the reaction gas is substantially the same as the reaction rate constant of the wafer surface and the reaction gas, thereby ensuring that the amount of gas consumed by the wafer carrier is substantially the same as the amount of gas consumed on the wafer surface. Can achieve better results.

另外,一般情况下,晶圓載盤的面積明顯大於一個晶圓的面積,所以,如第5圖所示,在晶圓載盤500上可以設置有多個第一結構501,用於放置多個晶圓。該第一結構501通常為凹槽結構。為了增大第二子表面的面積,可以在第二子表面上設置多個第二結構502。In addition, in general, the area of the wafer carrier is significantly larger than the area of one wafer. Therefore, as shown in FIG. 5, a plurality of first structures 501 may be disposed on the wafer carrier 500 for placing a plurality of crystals. circle. The first structure 501 is generally a groove structure. In order to increase the area of the second sub-surface, a plurality of second structures 502 may be disposed on the second sub-surface.

作為本發明的更為具體的實施例,能夠增大晶圓載盤第二子表面面積502的第二結構可以為凹陷結構,也可以為突起結構,或者兩者的結合因而藉由凹陷結構和/或突起結構能夠增大第二子表面的面積。As a more specific embodiment of the present invention, the second structure capable of increasing the second sub-surface area 502 of the wafer carrier may be a recessed structure, a protruding structure, or a combination of the two, and thus by a recessed structure and/or Or the raised structure can increase the area of the second sub-surface.

也可以這麽理解上述晶圓載盤的結構:在晶圓載盤500的上表面包括多個向下凹陷的安裝區501(相當於第一結構),該安裝區501用於安裝待處理的晶圓,在多個安裝區501之間包括隔離區,隔離區使得不同安裝區501之間相互隔離。所述隔離區的上表面包括至少一個凹陷結構或突起結構502(相當於第二結構),該凹陷結構或突起結構502使得隔離區上表面的面積與所述隔離區向下投影的平面面積的比值在1.05~1.15之間。The structure of the wafer carrier can also be understood as follows: the upper surface of the wafer carrier 500 includes a plurality of downwardly recessed mounting regions 501 (corresponding to the first structure) for mounting the wafer to be processed. An isolation area is included between the plurality of mounting areas 501, the isolation areas separating the different mounting areas 501 from each other. The upper surface of the isolation region includes at least one recessed structure or protrusion structure 502 (corresponding to the second structure), the recessed structure or protrusion structure 502 such that the area of the upper surface of the isolation region and the planar area of the isolation region projected downward The ratio is between 1.05 and 1.15.

在本發明實施例中,第二結構502可以藉由多種具體結構和形狀來實現,具體參見以下實施例。In the embodiment of the present invention, the second structure 502 can be implemented by using various specific structures and shapes. For details, refer to the following embodiments.

第6A圖是本發明實施例一提供的晶圓載盤的結構示意圖,第6B圖是本發明實施例一的晶圓載盤上的第二結構的結構示意圖。6A is a schematic structural view of a wafer carrier according to Embodiment 1 of the present invention, and FIG. 6B is a schematic structural view of a second structure on a wafer carrier according to Embodiment 1 of the present invention.

如第6A圖所示,實施例一提供的晶圓載盤的上表面包括第一子表面和第二子表面,其中,在第一子表面上設置有12個用於放置晶圓的凹槽601,在第二子表面上設置有多個凹陷腔體602。其中,凹陷腔體602的形狀為半球,單個凹陷腔體602的放大示意圖如第6B圖所示。需要說明的是,在本發明實施例中,第一子表面和第二子表面的劃分是根據其上設置的結構來劃分的。在本發明實施例中,晶圓載盤的直徑可以為500毫米。凹槽601可以設置為用於放置4英寸的晶圓的凹槽。As shown in FIG. 6A, the upper surface of the wafer carrier provided in the first embodiment includes a first sub-surface and a second sub-surface, wherein 12 recesses 601 for placing the wafer are disposed on the first sub-surface. A plurality of recessed cavities 602 are disposed on the second sub-surface. The shape of the recessed cavity 602 is a hemisphere, and an enlarged schematic view of the single recessed cavity 602 is shown in FIG. 6B. It should be noted that, in the embodiment of the present invention, the division of the first sub-surface and the second sub-surface is divided according to the structure disposed thereon. In an embodiment of the invention, the wafer carrier may have a diameter of 500 mm. The groove 601 can be provided as a groove for placing a 4 inch wafer.

如第6B圖所示的半球形狀的凹陷腔體602,其半徑與深度可以相等,或者,半徑略大於深度。作為本發明的更具體實施例,半球形狀的凹陷腔體602的半徑可以為1毫米。假設該半球的半徑為r,深度為d,則該半球的表面積P可以藉由以下方式計算得到:The hemispherical shaped cavity 602 as shown in FIG. 6B may have a radius and a depth equal to each other, or a radius slightly larger than the depth. As a more specific embodiment of the present invention, the hemispherical shaped recessed cavity 602 may have a radius of 1 mm. Assuming that the radius of the hemisphere is r and the depth is d, the surface area P of the hemisphere can be calculated by: .

採用本發明實施例所述的晶圓載盤,晶圓載盤表面與反應氣體的反應速率常數等於晶圓表面與反應氣體的反應速率常數。從而使得反應後在晶圓載盤表面上方的氣體濃度與晶圓表面上方的氣體濃度相等,從而抑制了“leading edge”的發生,保證了晶圓整個表面上的氣體濃度相等,進而保證了在整個晶圓表面上的晶體生長具有相同的生長速率,從而能夠在晶圓表面生長的晶體具有均勻的厚度。According to the wafer carrier of the embodiment of the invention, the reaction rate constant of the surface of the wafer carrier and the reaction gas is equal to the reaction rate constant of the surface of the wafer and the reaction gas. Therefore, the gas concentration above the wafer carrier surface after the reaction is equal to the gas concentration above the wafer surface, thereby suppressing the occurrence of "leading edge" and ensuring equal gas concentration on the entire surface of the wafer, thereby ensuring the entire The crystal growth on the surface of the wafer has the same growth rate, so that crystals grown on the surface of the wafer have a uniform thickness.

在本發明實施例中,多個凹陷腔體在第二子表面上的分布呈三次對稱軸分布,將形成三次對稱軸分布的三個凹陷腔體稱為一個第二結構單元,一個第二結構單元在第二子表面上的配置如第6C圖所示。其中,凹陷腔體分別位於等邊三角形的頂點上,假設三角形的等效邊長為a,凹陷腔體的半徑為r,深度為d,則一個第二結構單元的面積的計算公式如下:(9)。In the embodiment of the present invention, the distribution of the plurality of concave cavities on the second sub-surface is distributed in a cubic symmetry axis, and the three concave cavities forming the third symmetry axis distribution are referred to as a second structural unit, and a second structure. The configuration of the unit on the second sub-surface is as shown in Fig. 6C. Wherein, the concave cavity is respectively located at the apex of the equilateral triangle, and if the equivalent side length of the triangle is a, the radius of the concave cavity is r, and the depth is d, the calculation formula of the area of a second structural unit is as follows: (9).

需要說明的是,三角形的等效邊長a決定了各個凹陷腔體在晶圓載盤表面上之間的距離。It should be noted that the equivalent side length a of the triangle determines the distance between each recessed cavity on the surface of the wafer carrier.

本發明實施例對第二結構單元的各個參數(三角形的等效邊長a、半球的半徑r和深度d)進行了調整,從而得到多個面積比值(ratio),具體如表1所示。表1所示的面積比值ratio是設置有第二結構的第二子表面與未設置第二結構的第二子表面的面積比,也就是第二子表面與第二子表面向下投影得到的平面的面積比值。表1 In the embodiment of the present invention, each parameter of the second structural unit (the equivalent side length a of the triangle, the radius r of the hemisphere and the depth d) is adjusted to obtain a plurality of area ratios, as shown in Table 1. The area ratio ratio shown in Table 1 is an area ratio of the second sub-surface provided with the second structure and the second sub-surface not provided with the second structure, that is, the second sub-surface and the second sub-surface are projected downward. The area ratio of the plane. Table 1

另外,氣體在凹陷腔體602內的雷諾指數有可能達到200,因而在該凹陷腔體內可能會産生湍流,從而進一步增大氣體的消耗量,使得晶圓載盤的表面與反應氣體的反應速率常數增大。上述實施例一所述的凹陷腔體為半球,實際上,本發明實施例所述的凹陷腔體也可以是其它形狀,如圓柱形的、倒圓錐形、溝槽或者其它不規則凹陷形狀,只要凹陷腔體的形狀能夠改變氣流在載盤表面的路徑均屬本發明內容。In addition, the Reynolds index of the gas in the recessed cavity 602 may reach 200, so turbulence may be generated in the recessed cavity, thereby further increasing the gas consumption, so that the reaction rate constant of the surface of the wafer carrier and the reaction gas is constant. Increase. The recessed cavity of the first embodiment is a hemisphere. In fact, the recessed cavity according to the embodiment of the present invention may also have other shapes, such as a cylindrical shape, an inverted conical shape, a groove or other irregular concave shape. It is within the scope of the present invention that the shape of the recessed cavity can change the path of the airflow over the surface of the carrier.

上述實施例一提供的晶圓載體中的第二結構為半球狀的凹陷腔體,實際上,所述第二結構也可以為形狀為半球的突起結構。該半球狀的突起結構的結構示意圖如第6D圖。該半球狀的突起結構的半徑r和深度d與半球狀的凹陷腔體的半徑r和深度d相同。為了簡要起見,在此不再詳細描述。The second structure in the wafer carrier provided in the first embodiment is a hemispherical concave cavity. In fact, the second structure may also be a hemispherical protrusion structure. A schematic structural view of the hemispherical projection structure is shown in Fig. 6D. The radius r and the depth d of the hemispherical protrusion structure are the same as the radius r and depth d of the hemispherical recessed cavity. For the sake of brevity, it will not be described in detail here.

實施例一所述的第二結構為半球狀的凹陷腔體或半球狀的突起結構。實際上,作為本發明的另一實施例,第二結構還可以為凹溝或突出條。具體參見實施例二。當第二結構為凹溝或突出條時,該凹溝或突出條的數量、深度、寬度確定第二子表面的面積。 實施例二The second structure described in the first embodiment is a hemispherical concave cavity or a hemispherical protrusion structure. In fact, as another embodiment of the present invention, the second structure may also be a groove or a protruding strip. See the second embodiment for details. When the second structure is a groove or a protruding strip, the number, depth, and width of the groove or the protruding strip determine the area of the second sub-surface. Embodiment 2

如第7A圖所示,在晶圓載盤700的上表面的第一子表面上設置有12個用於放置晶圓的第一結構701,該第一結構701可以為凹槽。在第二子表面上設置有多條環形凹溝或突出條702。在本發明實施例中,每條環形凹溝或突出條702與晶圓載盤700的中心重合。也就是說,晶圓載盤700與環境凹溝或突出條702構成同心圓。As shown in FIG. 7A, on the first sub-surface of the upper surface of the wafer carrier 700, there are disposed 12 first structures 701 for placing wafers, and the first structures 701 may be grooves. A plurality of annular grooves or protruding strips 702 are disposed on the second sub-surface. In the embodiment of the invention, each annular groove or protruding strip 702 coincides with the center of the wafer carrier 700. That is, the wafer carrier 700 is concentric with the environmental grooves or protruding strips 702.

實施例二所述的凹溝或突出條702為環形的,實際上,上述所述的凹溝或突出條702還可以為從晶圓載盤的中心沿徑向方向向晶圓載盤的四周延伸,如第7B圖所示。The groove or protruding strip 702 of the second embodiment is annular. In fact, the groove or protruding strip 702 may extend from the center of the wafer carrier to the periphery of the wafer carrier in a radial direction. As shown in Figure 7B.

為了使得晶圓載盤在轉動的過程中,有利於氣體的流動,上述所述的凹溝或突出條702還可以向同一個方向傾斜,如同風車的葉輪。In order to facilitate the flow of the gas during the rotation of the wafer carrier, the grooves or protruding strips 702 described above may also be inclined in the same direction as the impeller of the windmill.

實施例一和實施例二所述的晶圓載盤僅在第二子表面上設置有第二結構。將該種結構的晶圓載盤應用於MOCVD系統時,如果用於放置晶圓的第一結構上均放置了晶圓,能夠保證晶圓載盤表面與氣體的反應速率常數等於晶圓表面與氣體的反應速率常數,進而能夠保證生長在晶圓表面上的晶體材料的厚度均勻性。但是,如果僅在部分第一結構上放置了晶圓,留有部分第一結構閒置,這時,閒置的第一結構相當於晶圓載盤的表面,而這些閒置的第一結構表面與氣體的反應速率常數小於晶圓表面與氣體的反應速率常數,此時,有可能就會出現晶圓表面上的晶體材料的厚度不均勻的情况。為了避免該種情况的出現,本發明還提供了實施例三。 實施例三The wafer carrier of the first embodiment and the second embodiment is provided with the second structure only on the second sub-surface. When the wafer carrier of the structure is applied to the MOCVD system, if the wafer is placed on the first structure for placing the wafer, the reaction rate constant of the surface of the wafer carrier and the gas can be ensured to be equal to the surface of the wafer and the gas. The reaction rate constant, in turn, ensures the uniformity of the thickness of the crystalline material grown on the surface of the wafer. However, if the wafer is placed only on part of the first structure, leaving part of the first structure idle, at this time, the idle first structure corresponds to the surface of the wafer carrier, and the reaction of these idle first structural surfaces with the gas The rate constant is smaller than the reaction rate constant of the wafer surface and the gas. At this time, there is a possibility that the thickness of the crystal material on the wafer surface is not uniform. In order to avoid the occurrence of such a situation, the present invention also provides the third embodiment. Embodiment 3

如第8圖所示,在晶圓載盤800的上表面的第一子表面上設置有多個用於放置晶圓的第一結構801,在第二子表面上設置有多個第二結構802,並且在部分第一結構801的內部也設置有第二結構802’。這樣,當在部分第一結構801上放置晶圓時,將晶圓放置在未設置第二結構的第一結構801上,將設置有第二結構802’的第一結構801閒置,由於這些閒置的第一結構的表面上也設置了第二結構,所以,這些閒置的第一結構的表面與氣體的反應速率常數等於晶圓表面與氣體的反應速率常數,從而能夠保證第一結構部分放置有晶圓時,也能保證生長在晶圓表面上的晶體材料的厚度的均勻性。As shown in FIG. 8, a plurality of first structures 801 for placing wafers and a plurality of second structures 802 are disposed on the second sub-surfaces on the first sub-surface of the upper surface of the wafer carrier 800. And a second structure 802' is also disposed inside the portion of the first structure 801. Thus, when the wafer is placed on the portion of the first structure 801, the wafer is placed on the first structure 801 where the second structure is not disposed, and the first structure 801 provided with the second structure 802' is left idle. The second structure is also disposed on the surface of the first structure, so that the reaction rate constant of the surface of the idle first structure and the gas is equal to the reaction rate constant of the surface of the wafer and the gas, thereby ensuring that the first structural portion is placed The uniformity of the thickness of the crystalline material grown on the wafer surface is also ensured during the wafer.

需要說明的是,在本發明實施例中,所述的第二結構802可以為實施例一或實施例二所述的任一結構,本實施例對第二結構的形式不做限定。It should be noted that, in the embodiment of the present invention, the second structure 802 may be any one of the first embodiment or the second embodiment. The form of the second structure is not limited in this embodiment.

以上所述僅是本發明的優選實施方式,應當指出,對於所屬領域具有通常知識者來說,在不脫離本發明原理的前提下,還可以做出若干改進和潤飾,這些改進和潤飾也應視為本發明的保護範圍。The above description is only a preferred embodiment of the present invention, and it should be noted that those skilled in the art can make several improvements and refinements without departing from the principles of the present invention. It is considered as the scope of protection of the present invention.

500、600、700、800‧‧‧晶圓載盤
501、701、801‧‧‧第一結構
502、802、802'‧‧‧第二結構
601‧‧‧凹槽
602‧‧‧凹陷腔體
702‧‧‧凹溝或突出條
500, 600, 700, 800‧‧‧ wafer carrier
501, 701, 801‧‧‧ first structure
502, 802, 802'‧‧‧ second structure
601‧‧‧ Groove
602‧‧‧ recessed cavity
702‧‧‧ Grooves or protruding strips

第1圖是在晶圓表面上的晶體材料的生長速率不均勻的原因解釋示意圖。Figure 1 is a schematic illustration of the reason why the growth rate of the crystalline material on the surface of the wafer is not uniform.

第2圖至第3圖是為晶體材料GaN反應機構示意圖。2 to 3 are schematic views of a GaN reaction mechanism for a crystalline material.

第4圖是晶體材料GaN在晶圓上的的生長機制示意圖。Figure 4 is a schematic diagram showing the growth mechanism of crystalline material GaN on a wafer.

第5圖是本發明實施例的晶圓載盤的結構示意圖。Fig. 5 is a schematic structural view of a wafer carrier according to an embodiment of the present invention.

第6A圖是本發明實施例一提供的晶圓載盤的結構示意圖。FIG. 6A is a schematic structural view of a wafer carrier according to Embodiment 1 of the present invention.

第6B圖是本發明實施例一提供的一種第二結構的結構示意圖。FIG. 6B is a schematic structural view of a second structure according to Embodiment 1 of the present invention.

第6C圖是本發明實施例一提供的第二結構在晶圓載盤上的配置的結構示意圖。FIG. 6C is a schematic structural diagram of a configuration of a second structure provided on a wafer carrier according to Embodiment 1 of the present invention.

第6D圖是本發明實施例一提供的另外一種第二結構的結構示意圖。FIG. 6D is a schematic structural view of another second structure according to Embodiment 1 of the present invention.

第7A圖是本發明實施例二提供的一種晶圓載盤的結構示意圖。FIG. 7A is a schematic structural view of a wafer carrier according to Embodiment 2 of the present invention.

第7B圖是本發明實施例二提供的另外一種晶圓載盤的結構示意圖。FIG. 7B is a schematic structural view of another wafer carrier according to Embodiment 2 of the present invention.

第8圖是本發明實施例三提供的晶圓載盤的結構示意圖。FIG. 8 is a schematic structural view of a wafer carrier according to Embodiment 3 of the present invention.

500‧‧‧晶圓載盤 500‧‧‧ wafer carrier

501‧‧‧第一結構 501‧‧‧ first structure

502‧‧‧第二結構 502‧‧‧Second structure

Claims (12)

一種用於MOCVD反應系統的晶圓載盤,其包括:該晶圓載盤的上表面包括一第一子表面和一第二子表面,在該第一子表面上設置用於放置晶圓的一第一結構,在該第二子表面上設置有一第二結構,該第二結構能夠增大該第二子表面的面積,使反應氣體與晶圓載盤的第二子表面的反應速率常數等於反應氣體與晶圓表面的反應速率常數。A wafer carrier for an MOCVD reaction system, comprising: an upper surface of the wafer carrier comprising a first sub-surface and a second sub-surface, wherein a first surface for placing a wafer is disposed on the first sub-surface a structure having a second structure disposed on the second sub-surface, the second structure capable of increasing an area of the second sub-surface such that a reaction rate constant of the reaction gas and the second sub-surface of the wafer carrier is equal to a reactive gas The reaction rate constant with the wafer surface. 如申請專利範圍第1項所述之晶圓載盤,其中設置有該第二結構的第二子表面的面積與未設置有該第二結構的第二子表面的面積的比值範圍在1.05~1.15之間。The wafer carrier according to claim 1, wherein a ratio of an area of the second sub-surface provided with the second structure to an area of the second sub-surface not provided with the second structure is in the range of 1.05 to 1.15. between. 如申請專利範圍第1或2項所述之晶圓載盤,其中該第二結構為凹陷結構、突起結構、或其組合。The wafer carrier of claim 1 or 2, wherein the second structure is a recessed structure, a raised structure, or a combination thereof. 如申請專利範圍第3項所述之晶圓載盤,其中該第二結構為複數個,當該第二結構為凹陷結構時,每個該凹陷結構為凹陷腔體,該凹陷腔體的形狀為半球;當該第二結構為突起結構時,每個該突起結構的形狀為半球。The wafer carrier of claim 3, wherein the second structure is plural, and when the second structure is a recessed structure, each of the recessed structures is a recessed cavity, and the shape of the recessed cavity is Hemisphere; when the second structure is a protruding structure, each of the protruding structures is in the shape of a hemisphere. 如申請專利範圍第4項所述之晶圓載盤,其中該半球的半徑與深度相同,或者該半球的半徑大於深度。The wafer carrier of claim 4, wherein the hemisphere has the same radius or depth, or the hemisphere has a radius greater than the depth. 如申請專利範圍第3項所述之晶圓載盤,其中當該第二結構為凹陷結構時,該凹陷結構為凹溝,當該第二結構為突起結構時,該突起結構為突出條。The wafer carrier of claim 3, wherein when the second structure is a recessed structure, the recessed structure is a groove, and when the second structure is a protruding structure, the protruding structure is a protruding strip. 如申請專利範圍第6項所述之晶圓載盤,其中該凹陷結構為複數個環狀凹溝,每個該環狀凹溝與該晶圓載盤的中心相同。The wafer carrier of claim 6, wherein the recessed structure is a plurality of annular grooves, each of the annular grooves being the same as a center of the wafer carrier. 如申請專利範圍第6項所述之晶圓載盤,其中該突起結構為複數個環狀突出條,每個該環狀突出條與該晶圓載盤的中心相同。The wafer carrier of claim 6, wherein the protruding structure is a plurality of annular protruding strips, each of the annular protruding strips being the same as a center of the wafer carrier. 如申請專利範圍第6項所述之晶圓載盤,其中該凹陷結構為複數個該凹溝,該突起結構為複數個該突出條,每個該突出條或每個該凹溝從該晶圓載盤的中心沿徑向方向延伸。The wafer carrier of claim 6, wherein the recessed structure is a plurality of the grooves, the protruding structure is a plurality of the protruding strips, and each of the protruding strips or each of the grooves is carried from the wafer The center of the disk extends in the radial direction. 如申請專利範圍第9項所述之晶圓載盤,其中沿徑向方向延伸的該突出條或該凹溝向同一方向傾斜。The wafer carrier of claim 9, wherein the protruding strip or the groove extending in a radial direction is inclined in the same direction. 如申請專利範圍第1或2項所述之晶圓載盤,其中該第一結構為複數個,在部分該第一結構的內部設置有該第二結構。The wafer carrier of claim 1 or 2, wherein the first structure is plural, and the second structure is disposed inside a portion of the first structure. 一種用於MOCVD反應系統的晶圓載盤,其中,該晶圓載盤的上表面包括複數個向下凹陷的安裝區,該複數個安裝區用於安裝待處理晶圓,該複數個安裝區之間包括隔離區,以使該複數個安裝區之間互相隔離,該隔離區的上表面包括至少一個凹陷結構或突起結構,該凹陷結構或突起結構使得該隔離區上表面的面積與該隔離區向下投影的平面面積的比值在1.05-1.15之間。A wafer carrier for an MOCVD reaction system, wherein an upper surface of the wafer carrier includes a plurality of mounting regions that are recessed downwardly, the plurality of mounting regions for mounting a wafer to be processed, between the plurality of mounting regions An isolation region is included to isolate the plurality of mounting regions from each other, the upper surface of the isolation region including at least one recessed structure or protrusion structure, the recessed structure or the protrusion structure causing an area of an upper surface of the isolation region and the isolation region The ratio of the planar area of the lower projection is between 1.05 and 1.15.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI643973B (en) * 2017-11-16 2018-12-11 錼創顯示科技股份有限公司 Wafer carrier and metal organic chemical vapor deposition apparatus

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105632984B (en) * 2014-11-24 2018-10-16 中微半导体设备(上海)有限公司 A kind of wafer carrier
USD860146S1 (en) 2017-11-30 2019-09-17 Veeco Instruments Inc. Wafer carrier with a 33-pocket configuration
USD854506S1 (en) 2018-03-26 2019-07-23 Veeco Instruments Inc. Chemical vapor deposition wafer carrier with thermal cover
USD866491S1 (en) 2018-03-26 2019-11-12 Veeco Instruments Inc. Chemical vapor deposition wafer carrier with thermal cover
USD860147S1 (en) 2018-03-26 2019-09-17 Veeco Instruments Inc. Chemical vapor deposition wafer carrier with thermal cover
USD858469S1 (en) 2018-03-26 2019-09-03 Veeco Instruments Inc. Chemical vapor deposition wafer carrier with thermal cover
USD863239S1 (en) 2018-03-26 2019-10-15 Veeco Instruments Inc. Chemical vapor deposition wafer carrier with thermal cover
WO2021120189A1 (en) * 2019-12-20 2021-06-24 苏州晶湛半导体有限公司 Wafer susceptor and chemical vapor deposition equipment

Family Cites Families (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7256375B2 (en) * 2002-08-30 2007-08-14 Asm International N.V. Susceptor plate for high temperature heat treatment
JP2005256137A (en) * 2004-03-15 2005-09-22 Fuji Electric Holdings Co Ltd Chemical vapor deposition system
JP4782788B2 (en) * 2005-07-28 2011-09-28 京セラ株式会社 Sample holder, sample adsorption device using the same, and sample processing method using the same
US8852349B2 (en) * 2006-09-15 2014-10-07 Applied Materials, Inc. Wafer processing hardware for epitaxial deposition with reduced auto-doping and backside defects
CN101487138A (en) * 2008-01-17 2009-07-22 矽延电子实业有限公司 Silicon wafer bearing disk for epitaxial manufacture process
CN102242352A (en) * 2010-05-14 2011-11-16 佛山市奇明光电有限公司 Organometallic chemical vapor deposition machine
TW201239124A (en) * 2011-03-22 2012-10-01 Chi Mei Lighting Tech Corp Wafer susceptor and chemical vapor deposition apparatus
US10854498B2 (en) * 2011-07-15 2020-12-01 Asm Ip Holding B.V. Wafer-supporting device and method for producing same

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI643973B (en) * 2017-11-16 2018-12-11 錼創顯示科技股份有限公司 Wafer carrier and metal organic chemical vapor deposition apparatus

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