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TWI887610B - Method for wafer treatment - Google Patents

Method for wafer treatment Download PDF

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TWI887610B
TWI887610B TW112105498A TW112105498A TWI887610B TW I887610 B TWI887610 B TW I887610B TW 112105498 A TW112105498 A TW 112105498A TW 112105498 A TW112105498 A TW 112105498A TW I887610 B TWI887610 B TW I887610B
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laser process
laser
depth
sub
focal depth
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TW112105498A
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TW202435290A (en
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鄭樵陽
劉祥益
燕婕 黎
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華旭矽材股份有限公司
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Abstract

A method for wafer treatment includes providing a wafer including a main surface, a surface layer and a base layer; and performing at least one laser process to irradiate the whole surface layer with laser to thereby generate a plurality of defect regions in the surface layer, and the defect regions form at least one array of defect regions.

Description

晶圓處理方法Wafer processing method

本發明是關於一種晶圓處理方法,且特別是針對晶圓內部的處理方法。 The present invention relates to a wafer processing method, and in particular to a processing method for the inside of a wafer.

在半導體製程中,通常包含施行磊晶製程,以在晶圓上形成磊晶層,磊晶層可以是半導體層,包含應力緩衝層、高電阻層、載子傳輸層及/或蓋層,但不限定於此。接著,再施行適當的半導體製程,例如薄膜製程、蝕刻製程、圖案化製程、摻雜製程等,以形成半導體元件,然而,尤其是異質磊晶(heteroepitaxy)或摻雜濃度相差二個數量級以上的同質磊晶(homoepitaxy),當完成磊晶製程後,通常皆會在晶圓與磊晶層的界面產生相當的應力,此應力通常源自於晶圓與磊晶層之間的晶格常數(lattice constant)的失配或是熱膨脹係數(coefficient of thermal expansion,CTE)的失配。 In the semiconductor manufacturing process, an epitaxial process is usually performed to form an epitaxial layer on a wafer. The epitaxial layer can be a semiconductor layer, including a stress buffer layer, a high resistance layer, a carrier transport layer and/or a capping layer, but is not limited thereto. Then, appropriate semiconductor processes, such as thin film processes, etching processes, patterning processes, doping processes, etc., are performed to form semiconductor devices. However, especially heteroepitaxy or homoepitaxy with doping concentrations that differ by more than two orders of magnitude, after the epitaxial process is completed, considerable stress is usually generated at the interface between the wafer and the epitaxial layer. This stress usually comes from the mismatch of the lattice constant or the mismatch of the coefficient of thermal expansion (CTE) between the wafer and the epitaxial layer.

舉例而言,對於以磊晶製程在矽晶圓上形成氮化鎵磊晶層的情形,因矽與氮化鎵之間的晶格失配(lattice mismatch)為17%、熱膨脹係數失配(thermal mistach)為54%,此使得矽晶圓的表面產生彎曲,而於磊晶層中產生應力、晶格缺陷或裂痕。所述缺陷與應力除了會導致磊晶完後之晶圓產生大幅度的彎曲與易脆之特性,而導致後續元件製程加工困難;同時亦會影響後續半導體元件的電子遷移率、崩潰電壓或其他電性表現,進而降低半導體元件的可靠性。 For example, when forming a gallium nitride epitaxial layer on a silicon wafer using an epitaxial process, the lattice mismatch between silicon and gallium nitride is 17% and the thermal expansion coefficient mismatch is 54%, which causes the surface of the silicon wafer to bend and generates stress, lattice defects or cracks in the epitaxial layer. The defects and stress will not only cause the wafer to bend significantly and become brittle after epitaxial deposition, making subsequent device processing difficult, but will also affect the electron mobility, breakdown voltage or other electrical properties of subsequent semiconductor devices, thereby reducing the reliability of semiconductor devices.

為了解決前述問題,可以在晶圓與磊晶層間設置具備超晶格(super lattice)結構或是晶格常數漸變結構(gradient layer)的緩衝磊晶層,但這將會增加額外的製程複雜度,另一方面,能同時與晶圓及磊晶層匹配的材料過於限定,反而降低製程的彈性,因此,業界需要一種可以釋放晶圓與磊晶層間應力的處理方法。 To solve the above problems, a buffer epitaxial layer with a super lattice structure or a lattice constant gradient structure (gradient layer) can be set between the wafer and the epitaxial layer, but this will increase the complexity of the process. On the other hand, the materials that can match the wafer and the epitaxial layer at the same time are too limited, which will reduce the flexibility of the process. Therefore, the industry needs a processing method that can release the stress between the wafer and the epitaxial layer.

為達成上述目的,本發明提供一種晶圓處理方法,其包含提供晶圓,晶圓包含主表面、表面層及主體層,其中表面層位於主表面及主體層之間;以及施行至少一雷射製程,以雷射全面照射表面層,藉以在表面層中產生複數個缺陷區域,多個缺陷區域構成至少一缺陷陣列。本發明所指之缺陷區域可能為晶格常數變異之同材料單晶、多晶形貌、非晶矽,微小氣泡、汽化區或空缺(cavity),並可構成缺陷陣列。 To achieve the above-mentioned purpose, the present invention provides a wafer processing method, which includes providing a wafer, the wafer including a main surface, a surface layer and a main layer, wherein the surface layer is located between the main surface and the main layer; and performing at least one laser process to fully irradiate the surface layer with a laser, thereby generating a plurality of defect regions in the surface layer, and the plurality of defect regions constitute at least one defect array. The defect region referred to in the present invention may be a single crystal of the same material with a variation in lattice constant, a polycrystalline morphology, amorphous silicon, a tiny bubble, a vaporization region or a cavity, and may constitute a defect array.

本發明之晶圓處理方法所形成的缺陷陣列可有效吸收後續在晶圓上設置的磊晶層的應力,具有步驟簡單、成本低的優點。 The defect array formed by the wafer processing method of the present invention can effectively absorb the stress of the epitaxial layer subsequently set on the wafer, and has the advantages of simple steps and low cost.

100:晶圓 100: Wafer

100A:主體層 100A: Main layer

100B:表面層 100B: Surface layer

100T:主表面 100T: Main surface

110:未處理區域 110: Unprocessed area

200:第一缺陷區域 200: First defect area

200a:第一子缺陷區域 200a: First sub-defect area

200b:第二子缺陷區域 200b: Second sub-defect area

200c:第三子缺陷區域 200c: The third sub-defect area

202:第二缺陷區域 202: Second defect area

302:第一水平面 302: First horizontal plane

304:第二水平面 304: Second level

306:第三水平面 306: The third level

A1:第一缺陷陣列 A1: The first defect array

A2:第二缺陷陣列 A2: The second defect array

a1:陣列單位長度 a1: array unit length

a2:陣列單位寬度 a2: array unit width

F:焦點 F: Focus

G:雷射產生裝置 G: Laser generating device

G1:第一雷射產生裝置 G1: First laser generating device

G2:第二雷射產生裝置 G2: Second laser generating device

H1:第一深度 H1: First Depth

H2:第二深度 H2: Second Depth

L:雷射 L:Laser

La:光點 La: light spot

Lv:聚焦深度 Lv: Focus depth

Lv1:第一聚焦深度 Lv1: First focus depth

Lv2:第二聚焦深度 Lv2: Second focus depth

Lv3:第三聚焦深度 Lv3: Third focus depth

P:掃描路徑 P: Scan path

P1:第一掃描路徑 P1: First scanning path

P2:第二掃描路徑 P2: Second scanning path

T:掃描寬度 T: Scan width

θ1:雷射夾角 θ 1 : Laser angle

θ2:夾角 θ 2 : Angle

D1:第一方向 D1: First direction

D2:第二方向 D2: Second direction

X:X軸 X: X axis

Y:Y軸 Y:Y axis

Z:Z軸 Z:Z axis

S1-S2:步驟 S1-S2: Steps

圖1為本發明一實施例施行第一雷射製程的立體示意圖。 Figure 1 is a three-dimensional schematic diagram of the first laser process performed in an embodiment of the present invention.

圖2為本發明一實施例的施行雷射製程的立體示意圖。 Figure 2 is a three-dimensional schematic diagram of the laser process of an embodiment of the present invention.

圖3為本發明一實施例施行第一雷射製程的剖面示意圖。 Figure 3 is a cross-sectional schematic diagram of the first laser process performed in an embodiment of the present invention.

圖4為本發明一實施例於施行第一雷射製程後的剖面示意圖。 Figure 4 is a schematic cross-sectional view of an embodiment of the present invention after the first laser process is performed.

圖5為本發明另一實施例於施行第一雷射製程後的剖面示意圖。 Figure 5 is a cross-sectional schematic diagram of another embodiment of the present invention after the first laser process is performed.

圖6為本發明另一實施例於施行第一雷射製程後的剖面示意圖。 Figure 6 is a cross-sectional schematic diagram of another embodiment of the present invention after the first laser process is performed.

圖7為本發明一實施例施行第一雷射製程及第二雷射製程的立體示意圖。 Figure 7 is a three-dimensional schematic diagram of the first laser process and the second laser process in an embodiment of the present invention.

圖8為本發明一實施例於施行第一雷射製程及第二雷射製程後的剖面示意圖。 FIG8 is a schematic cross-sectional view of an embodiment of the present invention after the first laser process and the second laser process are performed.

圖9為本發明一實施例之缺陷陣列的俯視示意圖。 Figure 9 is a top view schematic diagram of a defect array of an embodiment of the present invention.

圖10為本發明不同實施例施行雷射製程的雷射掃描路徑俯視圖。 FIG. 10 is a top view of the laser scanning path of the laser process in different embodiments of the present invention.

圖11為本發明的晶圓處理方法的流程圖。 Figure 11 is a flow chart of the wafer processing method of the present invention.

為使熟習本發明所屬技術領域之一般技藝者能更進一步了解本發明,下文特列舉本發明之數個較佳實施例,並配合所附圖式,詳細說明本發明的構成內容及所欲達成之功效。並且,熟習本發明所屬技術領域之一般技藝者亦能在不脫離本發明的精神下,參考以下所舉實施例,而將數個不同實施例中的特徵進行替換、重組、混合以完成其他實施例。 In order to enable a person skilled in the art who is familiar with the technical field to which the present invention belongs to further understand the present invention, several preferred embodiments of the present invention are listed below, and the components and intended effects of the present invention are described in detail with the accompanying drawings. Moreover, a person skilled in the art who is familiar with the technical field to which the present invention belongs can also refer to the following embodiments without departing from the spirit of the present invention, and replace, reorganize, and mix the features in several different embodiments to complete other embodiments.

圖1繪示本發明一實施例施行第一雷射製程的立體示意圖。其中,晶圓100包含主表面100T、表面層100B及主體層100A,其中表面層100B位於主表面100T及主體層100之間。晶圓100的材質例如是矽、碳化矽、氮化鎵、氮化鋁、砷化鎵、磷化銦、藍寶石等一種或多種元素組成的單晶晶圓基板又或者是上述材質堆疊組合成之複合式單晶晶圓,但不限於此。另一方面,根據不同需求,晶圓100可以摻雜不同濃度的摻質,摻質例如是IIIA族或VA族元素,摻雜濃度可為10^16原子/立方公分至10^18原子/立方公分,但不限於此。根據晶圓100的材質具有不同的剛性表現,晶圓100的厚度可為0.3毫米至1.5毫米。本文中的表面層100B的厚度會根據後續形成在主表面100T上的磊晶層的主體材質、摻雜濃度或磊晶厚度而定,舉例而言,若晶圓100與其上形成的磊晶層的晶格常數及熱膨 脹係數差異越大或兩者的摻雜濃度差異越大,晶格失配的情況越嚴重,此時的表面層100B的厚度越大,於一實施例中,表面層100B的厚度可為50微米至500微米。應說明的是,晶圓100之表面層100B在施行雷射製程前實質上為一均質結構,也就是說,表面層100B之各個區域具有實質相同的晶格大小、晶面、晶型及/或摻雜濃度。 FIG1 is a three-dimensional schematic diagram of a first laser process according to an embodiment of the present invention. The wafer 100 includes a main surface 100T, a surface layer 100B and a main layer 100A, wherein the surface layer 100B is located between the main surface 100T and the main layer 100. The material of the wafer 100 is, for example, a single crystal wafer substrate composed of one or more elements such as silicon, silicon carbide, gallium nitride, aluminum nitride, gallium arsenide, indium phosphide, sapphire, or a composite single crystal wafer composed of the above materials stacked together, but is not limited thereto. On the other hand, according to different requirements, the wafer 100 can be doped with different concentrations of dopants, such as group IIIA or group VA elements, and the doping concentration can be 10^16 atoms/cm3 to 10^18 atoms/cm3, but is not limited thereto. According to the different rigidity performance of the material of the wafer 100, the thickness of the wafer 100 can be 0.3 mm to 1.5 mm. The thickness of the surface layer 100B herein is determined according to the main material, doping concentration or epitaxial thickness of the epitaxial layer subsequently formed on the main surface 100T. For example, if the difference in lattice constant and thermal expansion coefficient between the wafer 100 and the epitaxial layer formed thereon is greater or the difference in doping concentration between the two is greater, the lattice mismatch is more serious, and the thickness of the surface layer 100B is greater at this time. In one embodiment, the thickness of the surface layer 100B may be 50 microns to 500 microns. It should be noted that the surface layer 100B of the wafer 100 is substantially a homogeneous structure before the laser process is performed, that is, each region of the surface layer 100B has substantially the same lattice size, crystal plane, crystal type and/or doping concentration.

本實施例施行之第一雷射製程沿著平行於第一方向D1的多道路徑,針對表面層100B全面施行第一雷射製程。例如藉由雷射產生裝置G產生雷射L,而以雷射L照射晶圓100之表面層100B,以於表面層100B中形成複數個第一缺陷區域(未繪示),多個第一缺陷區域構成第一缺陷陣列(未繪示)。 The first laser process implemented in this embodiment is performed along multiple paths parallel to the first direction D1, and the first laser process is fully performed on the surface layer 100B. For example, the laser generating device G generates laser L, and the laser L is used to irradiate the surface layer 100B of the wafer 100 to form a plurality of first defect regions (not shown) in the surface layer 100B, and the plurality of first defect regions constitute a first defect array (not shown).

應說明的是,本文所述的缺陷區域(包含第一缺陷區域、第二缺陷區域、第三缺陷區域或其他任何的缺陷區域),係表示該區域內的缺陷密度、空隙(void)數量、晶界數量及/或晶型會不同於表面層100B的其他區域。 It should be noted that the defect region described herein (including the first defect region, the second defect region, the third defect region or any other defect region) means that the defect density, the number of voids, the number of grain boundaries and/or the crystal type in the region are different from other regions of the surface layer 100B.

應說明的是,本文所述將雷射照射於某層,係表示雷射的焦點在該層內。舉例來說,當雷射L照射於表面層100B,係表示雷射產生裝置G所射出的雷射L的焦點在表面層100B中。 It should be noted that, when the laser is irradiated on a certain layer, it means that the focus of the laser is in the layer. For example, when the laser L is irradiated on the surface layer 100B, it means that the focus of the laser L emitted by the laser generating device G is in the surface layer 100B.

應說明的是,本發明所施行的雷射製程係為了在晶圓100內部(例如表面層100B)形成缺陷陣列,因此,所施行的雷射製程的雷射波長需具備穿透或部分穿透晶圓的特性,使得雷射在抵達預定深度前,其能量不會大幅被晶圓吸收或反射。舉例來說,當晶圓的材質為矽,所施行的雷射製程的雷射波長需大於1300奈米。 It should be noted that the laser process implemented in the present invention is to form a defect array inside the wafer 100 (e.g., the surface layer 100B). Therefore, the laser wavelength of the laser process implemented must have the property of penetrating or partially penetrating the wafer, so that the energy of the laser will not be greatly absorbed or reflected by the wafer before reaching the predetermined depth. For example, when the material of the wafer is silicon, the laser wavelength of the laser process implemented must be greater than 1300 nanometers.

在圖1中,雷射L與晶圓100的主表面100T有一雷射夾角θ1,於一實施例中,第一雷射製程的雷射夾角可為30°至90°。 In FIG. 1 , the laser L has a laser angle θ 1 with the main surface 100T of the wafer 100 . In one embodiment, the laser angle of the first laser process may be 30° to 90°.

圖2繪示本發明一實施例的雷射製程的立體示意圖,並進一步放大雷射產生裝置G所射出的雷射L。雷射產生裝置G可沿著掃描路徑P及其他掃描路徑 施行雷射製程。雷射產生裝置G所射出的雷射L具有一焦點F,而雷射L在晶圓100的最外側暴露面(例如主表面100T)具有一光點(spot)La。應注意的是,雖然圖2的雷射L的焦點F位於晶圓100的最外側暴露面之上,但當雷射L的焦點F位於最外側暴露面(例如主表面100T)之下,晶圓100的最外側暴露面仍會具有光點La。 FIG2 is a three-dimensional schematic diagram of a laser process of an embodiment of the present invention, and further magnifies the laser L emitted by the laser generating device G. The laser generating device G can perform a laser process along the scanning path P and other scanning paths. The laser L emitted by the laser generating device G has a focus F, and the laser L has a spot La on the outermost exposed surface of the wafer 100 (e.g., the main surface 100T). It should be noted that although the focus F of the laser L in FIG2 is located above the outermost exposed surface of the wafer 100, when the focus F of the laser L is located below the outermost exposed surface (e.g., the main surface 100T), the outermost exposed surface of the wafer 100 will still have a spot La.

圖3繪示本發明一實施例施行第一雷射製程的剖面示意圖,第一雷射製程的聚焦深度Lv可位於主表面100T下之0.01微米至50微米。於一實施例中,第一雷射製程的脈衝頻率為1kHz至2MHz,或是10kHz至100kHz,但不限定於此。根據不同需求,脈衝頻率可以依照材料種類、缺陷區域的橫向尺寸而予以調整。脈衝寬度可為100飛秒至500奈秒,或0.2奈秒(即200皮秒)至10奈秒,但不限定於此。當雷射的脈衝寬度較短時,例如300皮秒,可以搭配較高的脈衝頻率,例如MHz以上。第一雷射製程之脈衝能量(pulse energy)可為600uJ/pulse至20uJ/pulse。應說明的是,本發明所稱的脈衝能量(pulse energy)為雷射於每一脈衝所傳遞的能量,而晶圓被照射面在單位時間內所接受的能量不僅與脈衝能量有關,亦與脈衝寬度與脈衝頻率相關。具體而言,晶圓被照射面在單位時間內所接受的能量(uJ/ns)可藉由將脈衝能量除以脈衝寬度而得。對於給定功率的雷射設備,當提升脈衝頻率時,會導致脈衝能量降低。此外,若將雷射脈衝寬度從奈秒(nanosecond)之等級調整為皮秒(picosecond)或是飛秒(femtosecond)之等級,則雷射波峰功率(peak power)會越高,即越容易製造出高缺陷密度陣列,因此用於製造出缺陷陣列的雷射脈衝能量也與晶圓表面粗糙度有著一定的關係。 FIG3 is a schematic cross-sectional view of an embodiment of the present invention performing the first laser process. The focal depth Lv of the first laser process may be located at 0.01 micrometers to 50 micrometers below the main surface 100T. In one embodiment, the pulse frequency of the first laser process is 1 kHz to 2 MHz, or 10 kHz to 100 kHz, but is not limited thereto. According to different requirements, the pulse frequency may be adjusted according to the type of material and the lateral size of the defective area. The pulse width may be 100 femtoseconds to 500 nanoseconds, or 0.2 nanoseconds (i.e., 200 picoseconds) to 10 nanoseconds, but is not limited thereto. When the pulse width of the laser is shorter, such as 300 picoseconds, it may be combined with a higher pulse frequency, such as above MHz. The pulse energy of the first laser process can be 600uJ/pulse to 20uJ/pulse. It should be noted that the pulse energy referred to in the present invention is the energy delivered by the laser in each pulse, and the energy received by the irradiated surface of the wafer per unit time is not only related to the pulse energy, but also to the pulse width and pulse frequency. Specifically, the energy (uJ/ns) received by the irradiated surface of the wafer per unit time can be obtained by dividing the pulse energy by the pulse width. For a laser device of a given power, when the pulse frequency is increased, the pulse energy will be reduced. In addition, if the laser pulse width is adjusted from the nanosecond level to the picosecond or femtosecond level, the laser peak power will be higher, which means it will be easier to produce a high defect density array. Therefore, the laser pulse energy used to produce a defect array also has a certain relationship with the surface roughness of the wafer.

圖4繪示本發明一實施例於施行第一雷射製程後的剖面示意圖,其中,在晶圓100之表面層100B具有複數個第一缺陷區域200,本實施例之第一缺陷區域200皆位在同一水平面上,例如平行於由X軸和Y軸所定義出的平面,換句話說,本實施例的聚焦深度(平行於Z軸)為定值。需注意的是,圖4所示的第一缺陷區域200不僅只分布於圖4所示的剖面(即平行於X軸和Z軸的垂直面),第一 缺陷區域200亦可分布於平行於X軸和Z軸的其他多個垂直面。因此,當俯視觀察時,位於相同水平面上的多個第一缺陷區域200構成第一缺陷陣列,第一缺陷陣列具有第一深度H1,具體而言,第一深度H1係為第一缺陷陣列位於主表面100T下之深度,第一深度H1可為0.01微米至50微米。 FIG4 is a schematic cross-sectional view of an embodiment of the present invention after the first laser process is performed, wherein a plurality of first defect regions 200 are provided on the surface layer 100B of the wafer 100. The first defect regions 200 of the present embodiment are all located on the same horizontal plane, for example, parallel to the plane defined by the X-axis and the Y-axis. In other words, the focal depth (parallel to the Z-axis) of the present embodiment is a constant. It should be noted that the first defect regions 200 shown in FIG4 are not only distributed in the cross-sectional view shown in FIG4 (i.e., the vertical plane parallel to the X-axis and the Z-axis), but the first defect regions 200 may also be distributed in other multiple vertical planes parallel to the X-axis and the Z-axis. Therefore, when viewed from above, a plurality of first defect regions 200 located on the same horizontal plane constitute a first defect array, and the first defect array has a first depth H1. Specifically, the first depth H1 is the depth of the first defect array below the main surface 100T, and the first depth H1 can be 0.01 microns to 50 microns.

第一缺陷區域200係為透過雷射改質的特定區域,根據雷射所施予的能量和時間,第一缺陷區域200的缺陷密度、空隙數量、晶界數量及/或晶型可不同於表面層100B的其他區域。根據本發明一實施例,缺陷區域200的晶型和晶界數量與晶圓100之表面層100B的晶型和晶界數量不同,例如第一缺陷區域200的晶型為多晶型,且具有較多晶界,但第一缺陷區域200之外的表面層100B的晶型為單晶,且幾乎不存在晶界,又或者第一缺陷區域200的晶體與成分態樣不同於晶圓100,但不限於此。第一缺陷區域200的晶型與晶圓100之表面層100B的晶型可以不同,例如第一缺陷區域200的晶型為多晶(polycrystalline)或非晶質(amorphous),晶圓100之表面層100B的晶型為單晶(single crystal),但不限於此。 The first defect region 200 is a specific region modified by laser. According to the energy and time of the laser, the defect density, the number of voids, the number of grain boundaries and/or the crystal type of the first defect region 200 may be different from other regions of the surface layer 100B. According to an embodiment of the present invention, the crystal type and the number of grain boundaries of the defect region 200 are different from those of the surface layer 100B of the wafer 100. For example, the crystal type of the first defect region 200 is polycrystalline and has more grain boundaries, but the crystal type of the surface layer 100B outside the first defect region 200 is single crystal and has almost no grain boundaries, or the crystal and composition of the first defect region 200 are different from those of the wafer 100, but it is not limited thereto. The crystal type of the first defect region 200 and the crystal type of the surface layer 100B of the wafer 100 may be different. For example, the crystal type of the first defect region 200 is polycrystalline or amorphous, and the crystal type of the surface layer 100B of the wafer 100 is single crystal, but it is not limited thereto.

根據雷射所施予的能量及光點尺寸直徑,各第一缺陷區域200的投影面積可為1平方微米至104平方微米。 According to the energy and spot size diameter of the laser, the projection area of each first defect region 200 can be 1 square micron to 10 4 square microns.

相鄰的第一缺陷區域200可彼此分離。根據一實施例,第一缺陷區域200係沿著X軸斷續分布,使得相鄰的第一缺陷區域200不直接接觸。藉由設置第一缺陷區域200,例如是設置斷續且週期性分布的第一缺陷區域200,兩相鄰的第一缺陷區域200之間會存在未處理區域110(例如未經雷射處理的區域),如此可以使得位於同一水平面的多個第一缺陷區域200及相鄰的未處理區域110產生緩衝應力的效果,而可作為後續磊晶成長的應力緩衝層。 Adjacent first defect regions 200 can be separated from each other. According to one embodiment, the first defect regions 200 are intermittently distributed along the X axis so that adjacent first defect regions 200 do not directly contact each other. By providing the first defect regions 200, for example, discontinuous and periodically distributed first defect regions 200, there will be an untreated region 110 (for example, a region not treated by laser) between two adjacent first defect regions 200, so that multiple first defect regions 200 and adjacent untreated regions 110 located on the same horizontal plane can produce a stress buffering effect, and can serve as a stress buffer layer for subsequent epitaxial growth.

根據一實施例,相鄰的第一缺陷區域200可彼此部分接觸,使得各第一缺陷區域200沿著至少一方向連續分布。在此實施例,相鄰的第一缺陷區域200可以視為由第一子缺陷區(圖未示)和第二子缺陷區(圖未示)沿著至少一方向交替 排列而成,且第一子缺陷區的晶格缺陷密度、晶格常數、晶面及/或晶型會不同於第二子缺陷區的晶格缺陷密度、晶格常數、晶面及/或晶型。此時,只要子缺陷區域的至少其中一者具有週期性分布,則其所構成的缺陷陣列即可吸收晶圓100與磊晶層之界面產生的應力。 According to one embodiment, adjacent first defect regions 200 may partially contact each other, so that each first defect region 200 is continuously distributed along at least one direction. In this embodiment, adjacent first defect regions 200 can be regarded as being formed by alternating first sub-defect regions (not shown) and second sub-defect regions (not shown) along at least one direction, and the lattice defect density, lattice constant, crystal plane and/or crystal type of the first sub-defect region are different from the lattice defect density, lattice constant, crystal plane and/or crystal type of the second sub-defect region. At this time, as long as at least one of the sub-defect regions has a periodic distribution, the defect array formed by them can absorb the stress generated at the interface between the wafer 100 and the epitaxial layer.

圖5繪示本發明另一實施例於施行第一雷射製程後的剖面示意圖,本實施例與圖4所示之第一雷射製程大致相同,差異在於本實施例之第一雷射製程包含依序且循環施行的第一子雷射製程、第二子雷射製程及第三子雷射製程,以分別產生子缺陷區域200a、200b、200c。第一子雷射製程具有第一聚焦深度Lv1、第二子雷射製程具有第二聚焦深度Lv2,第三子雷射製程具有第三聚焦深度Lv3,第一聚焦深度Lv1大於第二聚焦深度Lv2,第二聚焦深度Lv2大於第三聚焦深度Lv3,且第一聚焦深度Lv1、第二聚焦深度Lv2及第三聚焦深度Lv3位於主表面100T下之0.01微米至10微米。於一實施例中,第一聚焦深度Lv1與第二聚焦深度Lv2相差1微米至3微米,第二聚焦深度Lv2與第三聚焦深度Lv3相差1微米至3微米。此外,第一子雷射製程、第二子雷射製程及第三子雷射製程的其他雷射參數,例如脈衝能量、脈衝寬度、光點尺寸等,可以相同或不同,端視實際需求。 FIG5 is a cross-sectional schematic diagram of another embodiment of the present invention after the first laser process is performed. This embodiment is substantially the same as the first laser process shown in FIG4 , except that the first laser process of this embodiment includes a first sub-laser process, a second sub-laser process, and a third sub-laser process that are sequentially and cyclically performed to generate sub-defect regions 200a, 200b, and 200c, respectively. The first sub-laser process has a first focus depth Lv1, the second sub-laser process has a second focus depth Lv2, and the third sub-laser process has a third focus depth Lv3. The first focus depth Lv1 is greater than the second focus depth Lv2, the second focus depth Lv2 is greater than the third focus depth Lv3, and the first focus depth Lv1, the second focus depth Lv2, and the third focus depth Lv3 are located at 0.01 micrometers to 10 micrometers below the main surface 100T. In one embodiment, the first focus depth Lv1 differs from the second focus depth Lv2 by 1 micron to 3 microns, and the second focus depth Lv2 differs from the third focus depth Lv3 by 1 micron to 3 microns. In addition, other laser parameters of the first sub-laser process, the second sub-laser process, and the third sub-laser process, such as pulse energy, pulse width, spot size, etc., can be the same or different, depending on actual needs.

在圖5中,每三個子缺陷區域200a、200b、200c構成類似於梯狀的規律性單元,此規律單元可沿著X軸延伸。複數個第一子缺陷區域200a可以位於相同深度,且分布在平行於X軸和Y軸的第一水平面302上,而構成第一子缺陷陣列。類似的,複數個第二子缺陷區域200b和複數個第三子缺陷區域200c會分別位於相同深度,且分別分布在平行於X軸和Y軸的第二水平面304及第三水平面306上,而構成第二子缺陷陣列及第三子缺陷陣列。第一缺陷陣列的第一深度係第一子缺陷陣列、第二子缺陷陣列及第三子缺陷陣列的平均深度,即第一聚焦深度Lv1、第二聚焦深度Lv2及第三聚焦深度Lv3的平均值。 In FIG5 , every three sub-defect regions 200a, 200b, and 200c form a regular unit similar to a ladder, and the regular unit may extend along the X-axis. The plurality of first sub-defect regions 200a may be located at the same depth and distributed on a first horizontal plane 302 parallel to the X-axis and the Y-axis to form a first sub-defect array. Similarly, the plurality of second sub-defect regions 200b and the plurality of third sub-defect regions 200c may be located at the same depth, and distributed on a second horizontal plane 304 and a third horizontal plane 306 parallel to the X-axis and the Y-axis to form a second sub-defect array and a third sub-defect array. The first depth of the first defect array is the average depth of the first sub-defect array, the second sub-defect array, and the third sub-defect array, that is, the average of the first focus depth Lv1, the second focus depth Lv2, and the third focus depth Lv3.

圖6繪示本發明另一實施例於施行第一雷射製程後的剖面示意圖。如圖6所示,本實施例與圖5所示之第一雷射製程大致相同,第一雷射製程同樣可包含依序且循環施行的第一子雷射製程、第二子雷射製程及第三子雷射製程,以分別產生子缺陷區域200a、200b、200c。第一子缺陷區域200a、第二子缺陷區域200b及第三子缺陷區域200c會構成類似於波浪狀的規律性單元,此規律單元可沿著X軸延伸。舉例來說,第一子雷射製程形成的一第一缺陷區域200a可構成波浪狀單元的波谷,而第三子雷射製程形成的第三缺陷區域200c可構成波浪狀單元的波峰。 FIG6 is a cross-sectional schematic diagram of another embodiment of the present invention after the first laser process is performed. As shown in FIG6, this embodiment is substantially the same as the first laser process shown in FIG5. The first laser process may also include a first sub-laser process, a second sub-laser process, and a third sub-laser process that are performed sequentially and cyclically to generate sub-defect regions 200a, 200b, and 200c, respectively. The first sub-defect region 200a, the second sub-defect region 200b, and the third sub-defect region 200c may form a regular unit similar to a wave shape, and the regular unit may extend along the X-axis. For example, a first defect region 200a formed by the first sub-laser process may form a trough of the wave-shaped unit, and a third defect region 200c formed by the third sub-laser process may form a peak of the wave-shaped unit.

當缺陷陣列由聚焦深度不同的複數缺陷區域所構成時(例如梯狀規律性單元或波浪狀規律性直列),對於後續形成磊晶層後,晶圓與磊晶層界面之應力可以有效分散,進而避免應力累積於磊晶層內,或避免造成晶圓之主表面彎曲甚至破裂。 When the defect array is composed of multiple defect areas with different focus depths (such as ladder-shaped regular units or wavy regular straight lines), the stress at the interface between the wafer and the epitaxial layer can be effectively dispersed after the epitaxial layer is subsequently formed, thereby avoiding stress accumulation in the epitaxial layer or causing the main surface of the wafer to bend or even break.

圖7繪示本發明一實施例施行第一雷射製程及第二雷射製程的立體示意圖。在施行第一雷射製程的過程中,雷射會沿著平行於第一方向D1的多道路徑(例如第一掃描路徑P1及相平行的其他路徑)全面照射表面層100B;在施行第二雷射製程的過程中,雷射會沿著平行於第二方向D2的多道路徑(例如第二掃描路徑P2及相平行的其他路徑)全面照射表面層100B。根據一實施例,例如藉由第一雷射產生裝置G1產生雷射L,而以雷射L照射晶圓100之表面層100B,形成複數個第一缺陷區域(未繪示),多個第一缺陷區域在一水平面上構成第一缺陷陣列(未繪示);第二雷射產生裝置G2產生雷射L,而以雷射L照射晶圓100之表面層100B,形成複數個第二缺陷區域(未繪示),多個第二缺陷區域在一水平面上構成第二缺陷陣列(未繪示)。 FIG7 is a three-dimensional schematic diagram of the first laser process and the second laser process according to an embodiment of the present invention. In the process of performing the first laser process, the laser will fully irradiate the surface layer 100B along multiple paths parallel to the first direction D1 (e.g., the first scanning path P1 and other parallel paths); in the process of performing the second laser process, the laser will fully irradiate the surface layer 100B along multiple paths parallel to the second direction D2 (e.g., the second scanning path P2 and other parallel paths). According to one embodiment, for example, a first laser generating device G1 generates laser L, and the laser L is used to irradiate the surface layer 100B of the wafer 100 to form a plurality of first defect regions (not shown), and the plurality of first defect regions form a first defect array (not shown) on a horizontal plane; a second laser generating device G2 generates laser L, and the laser L is used to irradiate the surface layer 100B of the wafer 100 to form a plurality of second defect regions (not shown), and the plurality of second defect regions form a second defect array (not shown) on a horizontal plane.

在圖7中,沿著第一方向D1延伸的掃描路徑P1與沿著第二方向D2延伸的掃描路徑P2之間具有夾角θ2,夾角θ2可為30°至90°。 In FIG. 7 , a scanning path P1 extending along the first direction D1 and a scanning path P2 extending along the second direction D2 have an angle θ 2 therebetween. The angle θ 2 may be 30° to 90°.

類似於圖4之實施例,第二雷射製程可沿著第二方向D2施行,其聚焦深度可位於主表面下之0.01微米至10微米,且聚焦深度為定值,第一雷射製程與第二雷射製程的聚焦深度可彼此相同或不同。 Similar to the embodiment of FIG. 4 , the second laser process can be performed along the second direction D2, and its focal depth can be 0.01 microns to 10 microns below the main surface, and the focal depth is a constant value. The focal depths of the first laser process and the second laser process can be the same or different.

根據一實施例,第一雷射製程與第二雷射製程會依序且循環施行。舉例來說,當沿著某一道路徑(例如第一掃描路徑P1)施行第一雷射製程之後,會沿著另一道路徑(例如第二掃描路徑P2)施行第二雷射製程,之後循環施行上述製程。 According to one embodiment, the first laser process and the second laser process are performed sequentially and cyclically. For example, after the first laser process is performed along a certain path (e.g., the first scanning path P1), the second laser process is performed along another path (e.g., the second scanning path P2), and then the above processes are performed cyclically.

類似於圖5之實施例,第二雷射製程可包含依序且循環施行的第四子雷射製程、第五子雷射製程及第六子雷射製程,第四子雷射製程具有第四聚焦深度、第五子雷射製程具有第五聚焦深度,第六子雷射製程具有第六聚焦深度,第四聚焦深度大於第五聚焦深度,第五聚焦深度大於第六聚焦深度,且第四聚焦深度、第五聚焦深度及第六聚焦深度位於主表面100T下之0.01微米至10微米。對應形成的複數第四子缺陷區域在一水平面上構成第四子缺陷陣列,複數第五子缺陷區域在一水平面上構成第五子缺陷陣列,複數第六子缺陷區域在一水平面上構成第六子缺陷陣列。第四子缺陷陣列、第五子缺陷陣列及第六子缺陷陣列可共同構成第二缺陷陣列。第一雷射製程之第一聚焦深度、第二聚焦深度及第三聚焦深度之任一者不同於第二雷射製程之第四聚焦深度、第五聚焦深度及第六聚焦深度之任一者。 Similar to the embodiment of FIG. 5 , the second laser process may include a fourth sub-laser process, a fifth sub-laser process, and a sixth sub-laser process that are sequentially and cyclically performed, the fourth sub-laser process has a fourth focal depth, the fifth sub-laser process has a fifth focal depth, the sixth sub-laser process has a sixth focal depth, the fourth focal depth is greater than the fifth focal depth, the fifth focal depth is greater than the sixth focal depth, and the fourth focal depth, the fifth focal depth, and the sixth focal depth are located 0.01 micrometers to 10 micrometers below the main surface 100T. The correspondingly formed plurality of fourth sub-defect regions constitute a fourth sub-defect array on a horizontal plane, the plurality of fifth sub-defect regions constitute a fifth sub-defect array on a horizontal plane, and the plurality of sixth sub-defect regions constitute a sixth sub-defect array on a horizontal plane. The fourth sub-defect array, the fifth sub-defect array, and the sixth sub-defect array may together constitute a second defect array. Any one of the first focal depth, the second focal depth, and the third focal depth of the first laser process is different from any one of the fourth focal depth, the fifth focal depth, and the sixth focal depth of the second laser process.

在圖7中,施行第一雷射製程及第二雷射製程之態樣包含同時施行,再選擇性地施行退火(annealing)處理,以雷射照射晶圓100的主表面100T或表面層100B,藉此改變表面層100B的結晶性,或者先施行第一雷射製程,接著選擇性地施行第一退火處理,以藉由退火處理消除雷射製程產生之應力,之後再施行第二雷射製程,接著選擇性地施行第二退火處理,以防止應力的累積。應說明的是,雖然特定波長的雷射製程可穿透晶圓,但無可避免地會造成穿透路徑 上的晶格產生些微偏移(例如小於5Å),由於第二雷射製程前有施行第一退火處理,可以確保前述些微偏移的晶格修復至雷射製程前的晶格狀態,以控制第二雷射製程的準確度。 In FIG. 7 , the first laser process and the second laser process are performed simultaneously, and then an annealing treatment is selectively performed to irradiate the main surface 100T or the surface layer 100B of the wafer 100 with a laser, thereby changing the crystallinity of the surface layer 100B, or the first laser process is performed first, and then a first annealing treatment is selectively performed to eliminate the stress generated by the laser process by the annealing treatment, and then the second laser process is performed, and then a second annealing treatment is selectively performed to prevent the accumulation of stress. It should be noted that although the laser process of a specific wavelength can penetrate the wafer, it will inevitably cause a slight shift in the lattice on the penetration path (for example, less than 5Å). Since the first annealing treatment is performed before the second laser process, it can ensure that the slightly shifted lattice is restored to the lattice state before the laser process to control the accuracy of the second laser process.

於一實施例中,第一雷射製程與第二雷射製程具有相同的脈衝能量,因此,所形成的第一缺陷區域及第二缺陷區域具有實質相同或近似的缺陷密度、空隙數量、晶界數量及/或晶型形貌。此外,端視實際需求,第一雷射製程及第二雷射製程的雷射參數,例如脈衝能量、脈衝寬度及光點尺寸等,可以相同或不同。 In one embodiment, the first laser process and the second laser process have the same pulse energy, so the first defect region and the second defect region formed have substantially the same or similar defect density, number of voids, number of grain boundaries and/or crystal morphology. In addition, depending on actual needs, the laser parameters of the first laser process and the second laser process, such as pulse energy, pulse width and spot size, can be the same or different.

圖8繪示本發明一實施例於施行第一雷射製程及第二雷射製程後的剖面示意圖,其中,在晶圓100之表面層100B具有複數個第一缺陷區域200,多個複數第一缺陷區域200會分布在一水平面上,而構成第一缺陷陣列A1,第一缺陷陣列A1具有第一深度H1,晶圓100之表面層100B另具有複數個第二缺陷區域202,多個複數第二缺陷區域202會分布在另一水平面上,而構成第二缺陷陣列A2,第二缺陷陣列A2具有第二深度H2。在本實施例中,第一深度H1不同於第二深度H2,且第一深度H1大於第二深度H2。需注意的是,圖8所示的第一缺陷區域200和第二缺陷區域202不僅只分布於圖8所示的剖面(即平行於X軸和Z軸的垂直面),第一缺陷區域200和第二缺陷區域202亦可分布於平行於X軸和Z軸的其他多個垂直面。 FIG8 is a schematic cross-sectional view of an embodiment of the present invention after the first laser process and the second laser process are performed, wherein a plurality of first defect regions 200 are provided on the surface layer 100B of the wafer 100, and the plurality of first defect regions 200 are distributed on a horizontal plane to form a first defect array A1, and the first defect array A1 has a first depth H1. The surface layer 100B of the wafer 100 also has a plurality of second defect regions 202, and the plurality of second defect regions 202 are distributed on another horizontal plane to form a second defect array A2, and the second defect array A2 has a second depth H2. In this embodiment, the first depth H1 is different from the second depth H2, and the first depth H1 is greater than the second depth H2. It should be noted that the first defect region 200 and the second defect region 202 shown in FIG. 8 are not only distributed in the cross-section shown in FIG. 8 (i.e., the vertical plane parallel to the X-axis and the Z-axis), but the first defect region 200 and the second defect region 202 may also be distributed in other multiple vertical planes parallel to the X-axis and the Z-axis.

於另一實施例中,第一缺陷陣列A1之第一深度H1可與第二缺陷陣列A2之第二深度H2相同,第一缺陷陣列A1的任一第一缺陷區域200不與第二缺陷陣列A2的任一第二缺陷區域202接觸,且任二相鄰的第一缺陷區域200之間可存在一第二缺陷區域202。 In another embodiment, the first depth H1 of the first defect array A1 may be the same as the second depth H2 of the second defect array A2, any first defect region 200 of the first defect array A1 does not contact any second defect region 202 of the second defect array A2, and a second defect region 202 may exist between any two adjacent first defect regions 200.

應說明的是,由於施行第一雷射製程的第一方向與施行第二雷射製程的第二方向並非互相平行,且第一雷射產生裝置及第二雷射產生裝置的掃描 間距可根據欲形成的缺陷陣列進行調整,也就是說,在晶圓100的俯視方向上,部分第一缺陷區域200與第二缺陷區域202可以不重疊。 It should be noted that since the first direction of the first laser process and the second direction of the second laser process are not parallel to each other, and the scanning intervals of the first laser generating device and the second laser generating device can be adjusted according to the defect array to be formed, that is, in the top view direction of the wafer 100, part of the first defect area 200 and the second defect area 202 may not overlap.

類似地,根據不同需求,本發明之晶圓處理方法還包含沿著第三方向施行第三雷射製程以在表面層100B中形成複數個第三缺陷區域,以在某一水平面上構成第三缺陷陣列,使得晶圓100之表面層100B同時具有第一缺陷陣列、第二缺陷陣列及第三缺陷陣列。 Similarly, according to different requirements, the wafer processing method of the present invention further includes performing a third laser process along a third direction to form a plurality of third defect regions in the surface layer 100B to form a third defect array on a certain horizontal plane, so that the surface layer 100B of the wafer 100 has the first defect array, the second defect array and the third defect array at the same time.

圖9繪示本發明一實施例之缺陷陣列的俯視示意圖,其中,該缺陷陣列具有陣列單位長度a1及陣列單位寬度a2,陣列單位長度a1平行於Y軸,陣列單位寬度a2平行於X軸,本實施例之陣列單位長度a1及陣列單位寬度a2相同,因此,圖9之缺陷陣列可視為由多個缺陷方格單元所構成。於另一實施例中,陣列單位長度a1大於陣列單位寬度a2,如此一來,缺陷陣列可視為由多個缺陷矩形單元所構成。於再一實施例中,陣列單位長度a1與Y軸之間有30°至60°之夾角,陣列單位寬度a2平行於X軸,如此一來,缺陷陣列可視為由多個缺陷平行四邊形單元所構成。 FIG9 is a top view schematic diagram of a defect array according to an embodiment of the present invention, wherein the defect array has an array unit length a1 and an array unit width a2, the array unit length a1 is parallel to the Y axis, and the array unit width a2 is parallel to the X axis. The array unit length a1 and the array unit width a2 of this embodiment are the same, so the defect array of FIG9 can be regarded as being composed of a plurality of defective square grid units. In another embodiment, the array unit length a1 is greater than the array unit width a2, so that the defect array can be regarded as being composed of a plurality of defective rectangular units. In another embodiment, the array unit length a1 has an angle of 30° to 60° with the Y axis, and the array unit width a2 is parallel to the X axis. In this way, the defect array can be regarded as composed of multiple defect parallelogram units.

圖10繪示本發明不同實施例施行雷射製程的雷射掃描路徑俯視圖。本發明施行二個以上之雷射製程的掃描路徑P可彼此相同或不同。如圖10(a)所示,掃描路徑P可沿著Y軸以線狀進行,相鄰二掃描路徑P具有一掃描寬度T,雷射的掃描寬度可為2微米至100微米,雷射的掃描間距為雷射產生裝置射出雷射的間隔距離,於一實施例中,掃描間距為1微米至100微米。如圖10(b)所示,掃描路徑P可沿著X軸以線狀進行;如圖10(c)所示,在施行二個以上之雷射製程的態樣中,先施行之雷射製程之掃描路徑P可沿著Y軸以線狀進行,後施行之雷射製程再沿著X軸以線狀進行,或先施行之雷射製程沿著X軸以線狀進行,後施行之雷射製程再沿著Y軸以線狀進行;如圖10(d)所示,施行三個以上之雷射製程的態樣中,先施行之雷射製程之掃描路徑P可先沿著Y軸以線狀進行,後施行之二 雷射製程再依序沿著另外二個彼此不同的掃描方向進行掃描。 FIG. 10 shows a top view of a laser scanning path for laser processes in different embodiments of the present invention. The scanning paths P for two or more laser processes in the present invention may be the same or different. As shown in FIG. 10( a ), the scanning path P may be linear along the Y axis, and two adjacent scanning paths P have a scanning width T. The scanning width of the laser may be 2 microns to 100 microns. The scanning pitch of the laser is the spacing distance between lasers emitted by the laser generating device. In one embodiment, the scanning pitch is 1 micron to 100 microns. As shown in FIG. 10(b), the scanning path P can be performed linearly along the X axis; as shown in FIG. 10(c), in the case of performing two or more laser processes, the scanning path P of the first laser process can be performed linearly along the Y axis, and the second laser process can be performed linearly along the X axis, or the first laser process can be performed linearly along the X axis, and the second laser process can be performed linearly along the Y axis; as shown in FIG. 10(d), in the case of performing three or more laser processes, the scanning path P of the first laser process can be performed linearly along the Y axis, and the second laser process can be performed sequentially along two other different scanning directions.

圖11繪示本發明的晶圓處理方法的流程圖。在圖11中,晶圓處理方法可包含步驟S1及S2。如圖11所示,在步驟S1中,提供晶圓。在步驟S2中,施行至少一雷射製程,以雷射全面照射表面層,藉以在表面層中產生複數個缺陷,多個缺陷構成至少一缺陷陣列。根據不同需求,在執行步驟S2後,晶圓處理方法更包含施行退火處理,以雷射照射晶圓的主表面或表面層,藉此改變表面層的結晶性。 FIG11 is a flow chart of the wafer processing method of the present invention. In FIG11 , the wafer processing method may include steps S1 and S2. As shown in FIG11 , in step S1, a wafer is provided. In step S2, at least one laser process is performed to fully irradiate the surface layer with laser, thereby generating a plurality of defects in the surface layer, and the plurality of defects constitute at least one defect array. According to different requirements, after executing step S2, the wafer processing method further includes performing an annealing process to irradiate the main surface or the surface layer of the wafer with laser, thereby changing the crystallinity of the surface layer.

根據本發明的上述實施例,係利用施行雷射製程以在晶圓的表面層中形成複數個缺陷,以構成至少一缺陷陣列。當後續在晶圓的主表面上成長磊晶層時,該缺陷陣列有利於緩衝或吸收源自於晶圓與磊晶層之間的晶格常數失配或是熱膨脹係數失配的應力。相較於在晶圓上先設置一緩衝磊晶層以解決前述問題,本發明具有步驟簡單、成本低的優點,且由於不需額外成長緩衝磊晶層,還可以降低半導體元件的厚度甚至降低後續晶圓薄化的程度。 According to the above-mentioned embodiment of the present invention, a laser process is performed to form a plurality of defects in the surface layer of the wafer to form at least one defect array. When an epitaxial layer is subsequently grown on the main surface of the wafer, the defect array is beneficial for buffering or absorbing the stress caused by the lattice constant mismatch or thermal expansion coefficient mismatch between the wafer and the epitaxial layer. Compared with first setting a buffer epitaxial layer on the wafer to solve the above-mentioned problem, the present invention has the advantages of simple steps and low cost, and since there is no need to grow an additional buffer epitaxial layer, the thickness of the semiconductor device can be reduced and even the degree of subsequent wafer thinning can be reduced.

以上所述僅為本發明之較佳實施例,凡依本發明申請專利範圍所做之均等變化與修飾,皆應屬本發明之涵蓋範圍。 The above is only the preferred embodiment of the present invention. All equivalent changes and modifications made within the scope of the patent application of the present invention shall fall within the scope of the present invention.

100:晶圓 100A:主體層 100B:表面層 100T:主表面 G:雷射產生裝置 L:雷射 θ 1:雷射夾角 D1:第一方向 100: wafer 100A: main layer 100B: surface layer 100T: main surface G: laser generating device L: laser θ 1 : laser angle D1: first direction

Claims (10)

一種晶圓處理方法,包含: 提供一晶圓,所述晶圓包含一主表面、一表面層及一主體層,其中所述表面層位於所述主表面及所述主體層之間; 施行至少一雷射製程,沿著複數個雷射掃描路徑,以雷射全面照射所述表面層,藉以在所述表面層中產生複數個缺陷區域,所述多個缺陷區域構成至少一缺陷陣列,其中,所述雷射製程的聚焦深度位於所述主表面下0.01微米至10微米;以及 在施行所述至少一雷射製程之後,在所述晶圓的所述主表面上成長一磊晶層。 A wafer processing method comprises: Providing a wafer, the wafer comprising a main surface, a surface layer and a main layer, wherein the surface layer is located between the main surface and the main layer; Performing at least one laser process, irradiating the surface layer with a laser along a plurality of laser scanning paths, thereby generating a plurality of defect regions in the surface layer, wherein the plurality of defect regions constitute at least one defect array, wherein the focusing depth of the laser process is located 0.01 micrometers to 10 micrometers below the main surface; and After performing the at least one laser process, growing an epitaxial layer on the main surface of the wafer. 如申請專利範圍第1項所述之晶圓處理方法,其中,施行所述至少一雷射製程包含: 施行一第一雷射製程,以雷射照射所述表面層,使得所述多個缺陷區域沿著一第一方向延伸,雷射的聚焦深度位於所述主表面下之0.01微米至50微米,且所述聚焦深度為定值。 The wafer processing method as described in item 1 of the patent application scope, wherein the implementation of the at least one laser process comprises: Implementing a first laser process, irradiating the surface layer with a laser so that the multiple defect regions extend along a first direction, the laser focus depth is 0.01 micron to 50 microns below the main surface, and the focus depth is a constant value. 如申請專利範圍第1項所述之晶圓處理方法,其中,施行所述至少一雷射製程包含: 施行一第一雷射製程,以雷射照射所述表面層,使得所述多個缺陷區域沿著一第一方向延伸,其中施行所述第一雷射製程包含: 依序且循環施行一第一子雷射製程、一第二子雷射製程及一第三子雷射製程,所述第一子雷射製程具有第一聚焦深度,所述第二子雷射製程具有第二聚焦深度,所述第三子雷射製程具有第三聚焦深度,且所述第一聚焦深度、所述第二聚焦深度及所述第三聚焦深度位於所述主表面下之0.01微米至50微米,其中,所述第一聚焦深度大於所述第二聚焦深度,所述第二聚焦深度大於所述第三聚焦深度。 The wafer processing method as described in item 1 of the patent application, wherein performing the at least one laser process comprises: performing a first laser process to irradiate the surface layer with a laser so that the multiple defect regions extend along a first direction, wherein performing the first laser process comprises: performing a first sub-laser process, a second sub-laser process and a third sub-laser process sequentially and cyclically, wherein the first sub-laser process has a first focal depth, the second sub-laser process has a second focal depth, and the third sub-laser process has a third focal depth, and the first focal depth, the second focal depth and the third focal depth are located at 0.01 micrometers to 50 micrometers below the main surface, wherein the first focal depth is greater than the second focal depth, and the second focal depth is greater than the third focal depth. 如申請專利範圍第1項所述之晶圓處理方法,其中,施行所述至少一雷射製程包含: 施行一第一雷射製程,以雷射照射所述表面層,使得所述多個缺陷區域的一部分沿著一第一方向延伸,雷射的聚焦深度位於所述主表面下之0.01微米至10微米,且所述聚焦深度為定值;以及 施行一第二雷射製程,以雷射照射所述表面層,使得所述多個缺陷區域的另一部分沿著一第二方向延伸,雷射的聚焦深度位於所述主表面下之0.01微米至10微米,且所述聚焦深度為定值, 其中,所述第一方向與所述第二方向之間具有一夾角,所述夾角為30°至90°,所述第一雷射製程的聚焦深度與所述第二雷射製程的聚焦深度彼此相同或不同, 其中,所述第一雷射製程及所述第二雷射製程會依序且循環施行。 The wafer processing method as described in item 1 of the patent application scope, wherein the implementation of the at least one laser process comprises: Implementing a first laser process, irradiating the surface layer with a laser, so that a portion of the multiple defect regions extend along a first direction, the laser focus depth is located at 0.01 microns to 10 microns below the main surface, and the focus depth is a constant value; and Implementing a second laser process, irradiating the surface layer with a laser, so that another portion of the multiple defect regions extend along a second direction, the laser focus depth is located at 0.01 microns to 10 microns below the main surface, and the focus depth is a constant value, wherein there is an angle between the first direction and the second direction, the angle is 30° to 90°, the focus depth of the first laser process and the focus depth of the second laser process are the same or different from each other, wherein the first laser process and the second laser process are implemented sequentially and cyclically. 如申請專利範圍第1項所述之晶圓處理方法,其中,施行所述至少一雷射製程包含: 施行一第一雷射製程,以雷射照射所述表面層,使得所述多個缺陷區域的一部分沿著一第一方向延伸,其中施行所述第一雷射製程包含: 依序且循環施行一第一子雷射製程、一第二子雷射製程及一第三子雷射製程,所述第一子雷射製程具有第一聚焦深度,所述第二子雷射製程具有第二聚焦深度,所述第三子雷射製程具有第三聚焦深度,且所述第一聚焦深度、所述第二聚焦深度及所述第三聚焦深度位於所述主表面下之0.01微米至10微米;以及 施行一第二雷射製程,以雷射照射所述表面層,使得所述多個缺陷區域的另一部分沿著一第二方向延伸,其中施行所述第二雷射製程包含: 依序且循環施行一第四子雷射製程、一第五子雷射製程及一第六子雷射製程,所述第四子雷射製程具有第四聚焦深度,所述第五子雷射製程具有第五聚焦深度,所述第六子雷射製程具有第六聚焦深度,且所述第四聚焦深度、所述第五聚焦深度及所述第六聚焦深度位於所述主表面下之0.01微米至50微米; 其中,所述第一方向與所述第二方向之間具有一夾角,所述夾角為30°至90°, 其中,所述第一聚焦深度大於所述第二聚焦深度,所述第二聚焦深度大於所述第三聚焦深度,所述第四聚焦深度大於所述第五聚焦深度,所述第五聚焦深度大於所述第六聚焦深度,所述第一聚焦深度、所述第二聚焦深度及所述第三聚焦深度之任一者不同於所述第四聚焦深度、所述第五聚焦深度及所述第六聚焦深度之任一者。 The wafer processing method as described in item 1 of the patent application scope, wherein performing the at least one laser process comprises: Performing a first laser process to irradiate the surface layer with a laser so that a portion of the multiple defect regions extend along a first direction, wherein performing the first laser process comprises: Performing a first sub-laser process, a second sub-laser process and a third sub-laser process sequentially and cyclically, wherein the first sub-laser process has a first focus depth, the second sub-laser process has a second focus depth, the third sub-laser process has a third focus depth, and the first focus depth, the second focus depth and the third focus depth are located at 0.01 microns to 10 microns below the main surface; and Performing a second laser process to irradiate the surface layer with a laser so that another portion of the multiple defect regions extend along a second direction, wherein performing the second laser process comprises: A fourth sub-laser process, a fifth sub-laser process and a sixth sub-laser process are sequentially and cyclically performed, wherein the fourth sub-laser process has a fourth focal depth, the fifth sub-laser process has a fifth focal depth, and the sixth sub-laser process has a sixth focal depth, and the fourth focal depth, the fifth focal depth and the sixth focal depth are located at 0.01 micrometers to 50 micrometers below the main surface; wherein there is an angle between the first direction and the second direction, and the angle is 30° to 90°, wherein the first focal depth is greater than the second focal depth, the second focal depth is greater than the third focal depth, the fourth focal depth is greater than the fifth focal depth, the fifth focal depth is greater than the sixth focal depth, and any one of the first focal depth, the second focal depth and the third focal depth is different from any one of the fourth focal depth, the fifth focal depth and the sixth focal depth. 如申請專利範圍第5項所述之晶圓處理方法,其中,所述第一雷射製程的施行時點與所述第二雷射製程的施行時點相同,或是所述第一雷射製程的施行時點早於所述第二雷射製程的施行時點。As described in item 5 of the patent application scope, the wafer processing method, wherein the implementation time of the first laser process is the same as the implementation time of the second laser process, or the implementation time of the first laser process is earlier than the implementation time of the second laser process. 如申請專利範圍第4項或第5項所述之晶圓處理方法,其中,所述第一雷射製程與所述第二雷射製程具有相同的脈衝能量。A wafer processing method as described in item 4 or 5 of the patent application scope, wherein the first laser process and the second laser process have the same pulse energy. 如申請專利範圍第1項所述之晶圓處理方法,所述至少一缺陷陣列包含: 一第一缺陷陣列,位於所述主表面下的第一深度;以及 一第二缺陷陣列,位於所述主表面下的第二深度, 其中,所述第一深度不同於所述第二深度。 As described in the wafer processing method of item 1 of the patent application scope, the at least one defect array includes: a first defect array, located at a first depth below the main surface; and a second defect array, located at a second depth below the main surface, wherein the first depth is different from the second depth. 如申請專利範圍第1項所述之晶圓處理方法,其中,在施行所述至少一雷射製程的過程中,各所述雷射的掃描路徑為線狀、掃描間距為1微米至100微米、掃描寬度為2微米至100微米。As described in item 1 of the patent application scope, in the process of implementing the at least one laser process, the scanning path of each laser is linear, the scanning pitch is 1 micron to 100 microns, and the scanning width is 2 microns to 100 microns. 如申請專利範圍第1項所述之晶圓處理方法,另包含: 施行一退火處理,以雷射照射所述晶圓的所述主表面或所述表面層,藉此改變所述表面層的結晶性。 The wafer processing method as described in Item 1 of the patent application scope further comprises: Performing an annealing process by irradiating the main surface or the surface layer of the wafer with a laser to change the crystallinity of the surface layer.
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TW202121519A (en) * 2019-08-06 2021-06-01 美商應用材料股份有限公司 Hybrid wafer dicing approach using a spatially multi-focused laser beam laser scribing process and plasma etch process
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TW202012090A (en) * 2018-07-05 2020-04-01 日商濱松赫德尼古斯股份有限公司 Laser machining device
TW202121519A (en) * 2019-08-06 2021-06-01 美商應用材料股份有限公司 Hybrid wafer dicing approach using a spatially multi-focused laser beam laser scribing process and plasma etch process
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