TW201605750A - Methods for separating a glass sheet - Google Patents

Methods for separating a glass sheet Download PDF

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Publication number
TW201605750A
TW201605750A TW104122376A TW104122376A TW201605750A TW 201605750 A TW201605750 A TW 201605750A TW 104122376 A TW104122376 A TW 104122376A TW 104122376 A TW104122376 A TW 104122376A TW 201605750 A TW201605750 A TW 201605750A
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Taiwan
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glass sheet
major surface
predetermined path
carrier substrate
along
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TW104122376A
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Chinese (zh)
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卡諾尙恩馬修
李興華
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康寧公司
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Publication of TW201605750A publication Critical patent/TW201605750A/en

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    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B33/00Severing cooled glass
    • C03B33/09Severing cooled glass by thermal shock
    • C03B33/091Severing cooled glass by thermal shock using at least one focussed radiation beam, e.g. laser beam
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B33/00Severing cooled glass
    • C03B33/02Cutting or splitting sheet glass or ribbons; Apparatus or machines therefor
    • C03B33/0222Scoring using a focussed radiation beam, e.g. laser
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B33/00Severing cooled glass
    • C03B33/02Cutting or splitting sheet glass or ribbons; Apparatus or machines therefor
    • C03B33/023Cutting or splitting sheet glass or ribbons; Apparatus or machines therefor the sheet or ribbon being in a horizontal position
    • C03B33/03Glass cutting tables; Apparatus for transporting or handling sheet glass during the cutting or breaking operations
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B33/00Severing cooled glass
    • C03B33/07Cutting armoured, multi-layered, coated or laminated, glass products
    • C03B33/074Glass products comprising an outer layer or surface coating of non-glass material
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B33/00Severing cooled glass
    • C03B33/02Cutting or splitting sheet glass or ribbons; Apparatus or machines therefor
    • C03B33/04Cutting or splitting in curves, especially for making spectacle lenses
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P40/00Technologies relating to the processing of minerals
    • Y02P40/50Glass production, e.g. reusing waste heat during processing or shaping
    • Y02P40/57Improving the yield, e-g- reduction of reject rates

Abstract

A method of separating a glass sheet comprises providing a glass sheet including a first major surface opposing a second major surface. A layer of adhesive material bonds the second major surface of the glass sheet to a support surface of a carrier substrate and a thickness between the first and second major surfaces of the glass sheet is equal to or less than about 300 [mu]m. The method comprises providing a first defect in the glass sheet and separating the glass sheet into a plurality of sub-sheets by traversing a beam of electromagnetic radiation over the first major surface along a first predetermined path to (a) transform the first defect into a first full body crack and (b) propagate the first full body crack along the first predetermined path, thereby producing a full body separation of the glass sheet while the glass sheet remains bonded to the support surface.

Description

用於分離玻璃板的方法 Method for separating glass sheets

本發明基於專利法主張2014年7月9日所申請之美國臨時申請案第62/022394號的優先權,該申請案的內容為本案所本且係藉由引用形式而整體併入本文中。 The present invention is based on the priority of U.S. Provisional Application No. 62/022,394, filed on Jul. 9, 2014, the disclosure of which is hereby incorporated by reference in its entirety in its entirety.

本發明一般是關於用於分離玻璃板的方法,更特別地,是與用於分離薄玻璃片的方法有關。 The present invention relates generally to a method for separating glass sheets, and more particularly to a method for separating thin glass sheets.

玻璃板常用於例如顯示應用中,舉例而言,如液晶顯示器(LCDs)、電泳顯示器(EPD)、有機發光二極體顯示器(OLEDs)、電漿顯示器面板(PDPs)等。有時,玻璃板被分離為多個子板,這些子板各自該玻璃板移除以用於一特定應用中。 Glass sheets are commonly used, for example, in display applications such as liquid crystal displays (LCDs), electrophoretic displays (EPD), organic light emitting diode displays (OLEDs), plasma display panels (PDPs), and the like. Sometimes the glass sheet is separated into a plurality of daughter boards, each of which is removed for use in a particular application.

玻璃板的切割在傳統上是藉由使用機械工具來完成。一般而言,玻璃板先經劃線,例如藉由使用一劃線工具(舉例而言,例如尖銳的碳化物刀輪)而進行,劃線工具於玻璃板中產生劃痕或中央裂紋,並且伴隨地在切割邊緣對玻璃板產生實質破壞。然而,也存在著使用CO2雷射輻射來加熱玻璃板並經由溫度梯度產生張應力以產生劃痕之替代製程。在雷射劃線期間,在玻璃板上會產生一初始缺陷,進以產生一中央裂紋(也稱為部分裂口,或簡稱為裂口)。裂口接著藉由形成為橫跨玻璃板整個表面間之 光束的雷射光、隨後以冷卻噴嘴產生一冷卻區域而傳播。以雷射光束加熱玻璃板,並且在之後立即以冷卻劑與倚淬冷,這產生了熱梯度與對應的應力場,用於裂口的傳播。當完成劃線,接著即對玻璃板施加彎折或剪應力,使裂口完成它的傳播而貫穿玻璃板的厚度。 The cutting of glass sheets has traditionally been accomplished by the use of mechanical tools. In general, the glass sheet is first scribed, for example by using a scribing tool, such as, for example, a sharp carbide cutter wheel, which produces scratches or central cracks in the glass sheet, and Concomitantly, the glass sheet is substantially destroyed at the cutting edge. However, there are alternative processes that use CO 2 laser radiation to heat the glass sheet and generate tensile stress via a temperature gradient to create scratches. During laser scribing, an initial defect is created on the glass sheet to create a central crack (also known as a partial crack, or simply a split). The breach is then propagated by laser light that is formed as a beam of light across the entire surface of the glass sheet, followed by a cooling zone that creates a cooling zone. The glass plate is heated with a laser beam and immediately quenched with a coolant and a sink, which creates a thermal gradient and a corresponding stress field for the propagation of the crack. When the scribing is completed, then the glass sheet is subjected to bending or shearing stress so that the crack completes its propagation and penetrates the thickness of the glass sheet.

雖然上述雷射劃線技術會比機械劃線製程產生較少破壞,但雷射劃線製程仍會對玻璃板產生破壞,例如,特別是在涉及施加彎折或剪應力的機械分離製程中。在對雷射入射側評估張應力對壓縮應力的關係時,這可能會產生邊緣強度的差異。此外,對於雷射與機械劃線技術兩者而言,玻璃板的分離需要至少兩個步驟,包括產生劃痕,然後對玻璃板施加應力(例如彎折應力),以沿著劃痕線分離玻璃板。此外,劃線技術一般會產生碎片,碎片可能會污染子板。因此,提供一種可對子板提供最小邊緣破壞和分離製程中受碎片污染達最低之簡化的分離製程是有利的。 While the laser scribing technique described above produces less damage than the mechanical scribing process, the laser scribing process can still cause damage to the glass sheet, for example, particularly in mechanical separation processes involving the application of bending or shear stress. This may result in a difference in edge strength when evaluating the relationship between tensile stress and compressive stress on the incident side of the laser. Furthermore, for both laser and mechanical scribing techniques, the separation of the glass sheets requires at least two steps, including the creation of scratches, which are then stressed (eg, bending stress) to separate along the score line. glass plate. In addition, scribing techniques typically produce debris that can contaminate the daughterboard. Accordingly, it would be advantageous to provide a simplified separation process that provides minimal edge damage to the daughterboard and minimal debris contamination during the separation process.

提出了用於分離玻璃板之方法,所提出方法可提供一種簡化的分離製程,並可進一步提供具有最小邊緣破壞及受分離製程中碎片污染達最低之子板。 A method for separating glass sheets is proposed which provides a simplified separation process and further provides a daughterboard with minimal edge damage and minimal debris contamination during the separation process.

在一第一構想中,一種用於分離玻璃板的方法包括:步驟(I)提供一玻璃板,該玻璃板包括一第一主要表面和與該第一主要表面相對的一第二主要表面;一黏著材料層係將該玻璃板的該第二主要表面接合至一載體基板的 一支撐表面,且該第一主要表面與該第二主要表面之間的一厚度等於或小於約300微米。該方法進一步包括步驟(II)於該玻璃板中提供一第一缺陷;及步驟(III)將該玻璃板分離為複數個子板。步驟(III)是藉由使一電磁輻射束沿一第一預定路徑於該第一主要表面上往復移動而進行,以:(a)將該第一缺陷轉換為與該玻璃板的該第一主要表面和該第二主要表面交錯的一第一完整本體裂紋;及(b)使該第一完整本體裂紋沿著該第一預定路徑傳播,藉此沿著該第一預定路徑產生該玻璃板之一完整本體分離,而該玻璃板的該第二主要表面仍保持接合至該載體基板的該支撐表面。 In a first concept, a method for separating a glass sheet includes: step (I) providing a glass sheet, the glass sheet including a first major surface and a second major surface opposite the first major surface; An adhesive material layer bonding the second major surface of the glass sheet to a carrier substrate a support surface, and a thickness between the first major surface and the second major surface is equal to or less than about 300 microns. The method further includes the step (II) of providing a first defect in the glass sheet; and the step (III) separating the glass sheet into a plurality of daughter boards. Step (III) is performed by reciprocating a beam of electromagnetic radiation on the first major surface along a first predetermined path to: (a) convert the first defect to the first with the glass sheet a first complete body crack interleaved between the major surface and the second major surface; and (b) propagating the first intact body crack along the first predetermined path, thereby generating the glass sheet along the first predetermined path One of the complete bodies separates while the second major surface of the glass sheet remains bonded to the support surface of the carrier substrate.

在第一構想的一個示例中,步驟(II)進一步包括於玻璃板中提供一第二缺陷,且將該玻璃板分離為複數個子板之步驟(III)係進一步包括使一電磁輻射束於該第一主要表面上沿著一第二預定路徑往復移動,以:(a)將該第二缺陷轉換為與該第一主要表面和該第二主要表面交錯的一第二完整本體裂紋;及(b)使該第二完整本體裂紋沿著該第二預定路徑傳播,藉此沿著該第二預定路徑產生該玻璃板之一完整本體分離,而該玻璃板的該第二主要表面仍保持接合至該載體基板的該支撐表面。在一個示例中,該第二預定路徑係與該第一預定路徑交錯。 In an example of the first concept, the step (II) further includes providing a second defect in the glass sheet, and the step (III) of separating the glass sheet into the plurality of sub-boards further comprises: causing an electromagnetic radiation beam to be Reciprocating along a second predetermined path on the first major surface to: (a) convert the second defect into a second complete body crack interleaved with the first major surface and the second major surface; and b) propagating the second complete body crack along the second predetermined path, thereby producing a complete body separation of the glass sheet along the second predetermined path, while the second major surface of the glass sheet remains bonded To the support surface of the carrier substrate. In one example, the second predetermined path is interleaved with the first predetermined path.

在該第一構想的另一實例中。該方法進一步包括步驟(IV):藉由於該玻璃板的該第二主要表面與該載體基板的該支撐表面中至少其一中產生一曲度,自該載體基 板釋放至少一個子板的至少一部分。在一個示例中,步驟(IV)包括自該載體玻璃完全釋放至少一個子板,同時保持該曲度。在另一示例中,步驟(IV)包括藉由使該複數個子板的其中一個子板的一邊緣部分上升遠離該載體玻璃,在該玻璃板的該第二主要表面中產生一雙重彎曲曲度。 In another example of this first concept. The method further includes the step (IV) of generating a curvature from at least one of the second major surface of the glass sheet and the support surface of the carrier substrate, from the carrier base The board releases at least a portion of at least one of the daughter boards. In one example, step (IV) includes completely releasing at least one daughterboard from the carrier glass while maintaining the curvature. In another example, step (IV) includes creating a double bend curvature in the second major surface of the glass sheet by raising an edge portion of one of the plurality of daughter boards away from the carrier glass .

在第一構想的另外一個示例中,該方法進一步包括步驟(IV)於該載體基板中提供一第二缺陷;及步驟(V)藉由使一電磁輻射束沿著一第二預定路徑而相對於該載體基板往復移動,使該載體基板分離為複數個子載體基板。在一個示例中,第一預定路徑係與第二預定路徑對齊。在另一示例中,在步驟(V)中使雷射束往復移動係沿著第二預定路徑於該載體基板中產生一劃線。在一個特定示例中,步驟(V)係進一步對載體基板施加一彎折力,以使載體基板沿著該劃線而分離為複數個子載體基板。在另外的示例中,在步驟(V)中使電磁輻射往復移動係使第二缺陷轉換為延伸貫穿載體基板之一第二完整本體裂紋,且使該第二裂紋沿著該第二預定路徑傳播係沿著該第二預定路徑產生該載體基板之一完整本體分離。在另一示例中,步驟(V)所提供的每一個子載體基板係與複數個子板中的一單一對應者接合。在一個特定示例中,該方法進一步包括步驟(IV):自對應的子載體基板釋放其中一個子板。 In another example of the first concept, the method further includes the step (IV) of providing a second defect in the carrier substrate; and the step (V) of causing a beam of electromagnetic radiation to be relatively along a second predetermined path The carrier substrate is reciprocated to separate the carrier substrate into a plurality of sub-carrier substrates. In one example, the first predetermined path is aligned with the second predetermined path. In another example, reciprocating the laser beam in step (V) produces a scribe line in the carrier substrate along a second predetermined path. In one particular example, step (V) further applies a bending force to the carrier substrate to separate the carrier substrate along the scribe line into a plurality of sub-carrier substrates. In a further example, reciprocating the electromagnetic radiation in step (V) converts the second defect into a second complete body crack extending through one of the carrier substrates and causing the second crack to propagate along the second predetermined path A complete body separation of the carrier substrate is produced along the second predetermined path. In another example, each of the sub-carrier substrates provided in step (V) is bonded to a single one of the plurality of daughter boards. In one particular example, the method further includes the step (IV) of releasing one of the daughter boards from the corresponding sub-carrier substrate.

前述第一構想係可單獨提供,或與上述第一構想中的任一或多個示例組合提供。 The foregoing first concept may be provided separately or in combination with any one or more of the above-described first concepts.

在一第二構想中,用於分離一玻璃板之方法包括步驟(I)提供一玻璃板,該玻璃板包括一第一主要表面、與該第一主要表面相對的一第二主要表面,且該第一主要表面和該第二主要表面之間的厚度係等於或小於約300微米。玻璃板的第二主要表面係接合至一載體基板的一支撐表面。該方法進一步包括步驟(II):於該玻璃板中提供一第一缺陷;及步驟(III):將該玻璃板分離為複數個子板。步驟(III)是藉由使電磁輻射束於該第一主要表面上沿一第一預定路徑往復移動而進行,以:(a)將該第一缺陷轉換為與該玻璃板的第一主要表面及第二主要表面交錯的一第一完整本體裂紋;及(b)使該第一完整本體裂紋沿著該第一預定路徑傳播,藉此產生該玻璃板沿該第一預定路徑之一完整本體分離,同時該玻璃板的該第二主要表面仍保持接合至該載體基板的該支撐表面。該方法進一步包括步驟(IV):藉由於該玻璃板的該第二主要表面和該載體基板的該支撐表面之至少其一中產生一曲度而自該載體基板釋放至少一個子板的至少一部分。 In a second concept, a method for separating a glass sheet includes the step (I) of providing a glass sheet, the glass sheet including a first major surface, a second major surface opposite the first major surface, and The thickness between the first major surface and the second major surface is equal to or less than about 300 microns. The second major surface of the glass sheet is bonded to a support surface of a carrier substrate. The method further includes the step (II) of providing a first defect in the glass sheet; and the step (III): separating the glass sheet into a plurality of daughter boards. Step (III) is performed by reciprocating the electromagnetic radiation beam on the first major surface along a first predetermined path to: (a) convert the first defect into a first major surface with the glass sheet And a first complete body crack interleaved with the second major surface; and (b) propagating the first complete body crack along the first predetermined path, thereby generating a complete body of the glass sheet along the first predetermined path Separating while the second major surface of the glass sheet remains bonded to the support surface of the carrier substrate. The method further includes the step (IV) of releasing at least a portion of the at least one daughterboard from the carrier substrate by creating a curvature in at least one of the second major surface of the glass sheet and the support surface of the carrier substrate .

在該第二構想的一個示例中,步驟(IV)進一步包括:自該載體玻璃完全釋放至少一個子板,同時仍保持該曲度。 In one example of the second concept, step (IV) further comprises: completely releasing at least one daughterboard from the carrier glass while still maintaining the curvature.

在該第二構想的另一示例中,步驟(IV)包括藉由使使該複數個子板的其中一個子板的一邊緣部分上升遠離該載體玻璃,在該玻璃板的該第二主要表面中產生一雙重彎曲曲度。 In another example of the second concept, the step (IV) includes, by causing an edge portion of one of the plurality of daughter boards to rise away from the carrier glass, in the second major surface of the glass sheet Produces a double curvature.

在該第二構想的又一示例中,步驟(IV)使相鄰的一對子板的至少一對面向邊緣表面沿著第一主要表面的方向移動遠離彼此,以於該隊面向邊緣表面之間產生一側向間隙。 In still another example of the second concept, the step (IV) moves at least one pair of facing edge surfaces of the adjacent pair of daughter boards away from each other in a direction of the first major surface, so that the team faces the edge surface A lateral gap is created.

在該第二構想的另外一個示例中,步驟(II)進一步包括於該玻璃板中提供一第二缺陷,且使該玻璃板分離為複數個子板之步驟(III)進一步包括使一電磁輻射束於該第一主要表面上方沿一第二預定路徑上方往復移動,以:(a)將該第二缺陷轉化為與該玻璃板的該第一主要表面及該第二主要表面交錯的一第二完整本體裂紋;及(b)沿該第二預定路徑傳播該第二完整本體裂紋。因此,步驟(III)係沿著該第二預定路徑產生玻璃板之完整本體分離,同時玻璃板的第二主要表面仍保持接合至載體基板的支撐表面。在一個示例中,第二預定路徑可與第一預定路徑交錯。 In another example of the second concept, the step (II) further includes providing a second defect in the glass sheet, and the step (III) of separating the glass sheet into the plurality of sub-plates further comprises: causing an electromagnetic radiation beam Reciprocating over the first major surface along a second predetermined path to: (a) convert the second defect into a second interlaced with the first major surface and the second major surface of the glass sheet a complete body crack; and (b) propagating the second complete body crack along the second predetermined path. Thus, step (III) produces a complete body separation of the glass sheet along the second predetermined path while the second major surface of the glass sheet remains bonded to the support surface of the carrier substrate. In one example, the second predetermined path can be interleaved with the first predetermined path.

在該第二構想的另外一個示例中,步驟(I)包括利用一黏著材料層將該玻璃板的該第二主要表面接合至該載體基板的該支撐表面之步驟。 In another example of the second concept, step (I) includes the step of bonding the second major surface of the glass sheet to the support surface of the carrier substrate using an adhesive layer.

前述第二構想係可單獨提供,或與上述第二構想中的任一或多個示例組合提供。 The foregoing second concept may be provided separately or in combination with any one or more of the above-described second concepts.

10‧‧‧玻璃板 10‧‧‧ glass plate

12‧‧‧第一主要表面 12‧‧‧ first major surface

14‧‧‧第二主要表面 14‧‧‧ second major surface

16‧‧‧邊緣 16‧‧‧ edge

18‧‧‧邊緣 18‧‧‧ edge

20‧‧‧邊緣 20‧‧‧ edge

22‧‧‧邊緣 22‧‧‧ edge

24‧‧‧載體基板 24‧‧‧ Carrier substrate

26‧‧‧第一主要表面 26‧‧‧First major surface

28‧‧‧第二主要表面 28‧‧‧ second major surface

30‧‧‧邊緣 30‧‧‧ edge

32‧‧‧邊緣 32‧‧‧ edge

34‧‧‧邊緣 34‧‧‧ edge

36‧‧‧邊緣 36‧‧‧ edge

40‧‧‧黏著材料層 40‧‧‧Adhesive material layer

42‧‧‧玻璃-載體組件 42‧‧‧Glass-carrier assembly

44‧‧‧第一缺陷 44‧‧‧First defect

46‧‧‧第二缺陷 46‧‧‧second defect

48‧‧‧電磁輻射束 48‧‧‧Electromagnetic radiation beam

50‧‧‧第一預定路徑 50‧‧‧First scheduled path

52‧‧‧雷射輻射裝置 52‧‧‧Laser radiation device

54‧‧‧加熱區域 54‧‧‧heating area

56‧‧‧冷卻裝置 56‧‧‧Cooling device

58‧‧‧冷卻流體 58‧‧‧Cooling fluid

60‧‧‧冷卻區域 60‧‧‧Cooling area

64‧‧‧第一完整本體裂紋 64‧‧‧First complete body crack

68‧‧‧子板 68‧‧‧Slate board

70‧‧‧子板 70‧‧‧ daughter board

78‧‧‧第二預定路徑 78‧‧‧second scheduled path

82‧‧‧第二完整本體裂紋 82‧‧‧Second complete body crack

86‧‧‧子板 86‧‧‧Slate board

88‧‧‧子板 88‧‧‧Slate board

90‧‧‧子板 90‧‧‧ daughter board

92‧‧‧子板 92‧‧‧Slate board

102‧‧‧第三缺陷 102‧‧‧ third defect

112‧‧‧第三預定路徑 112‧‧‧ third scheduled path

116‧‧‧裂紋 116‧‧‧ crack

118‧‧‧劃痕線 118‧‧‧Scratch line

120‧‧‧子載體基板 120‧‧‧Subcarrier substrate

122‧‧‧子載體基板 122‧‧‧Subcarrier substrate

124‧‧‧子載體基板 124‧‧‧Subcarrier substrate

126‧‧‧子載體基板 126‧‧‧Subcarrier substrate

130‧‧‧子組件 130‧‧‧Subcomponents

132‧‧‧子組件 132‧‧‧Subcomponents

134‧‧‧子組件 134‧‧‧Subcomponents

136‧‧‧子組件 136‧‧‧Subcomponents

142‧‧‧邊緣部分 142‧‧‧Edge section

144‧‧‧邊緣表面 144‧‧‧Edge surface

146‧‧‧邊緣表面 146‧‧‧Edge surface

150‧‧‧邊緣 150‧‧‧ edge

152‧‧‧邊緣 152‧‧‧ edge

156‧‧‧間隙 156‧‧‧ gap

參照如附圖式來研讀本發明之下述詳細內容,即可更加理解本發明的上述特徵、構想與優點,其中:第1圖為一玻璃板的透視圖;第2圖為一載體基板的透視圖; 第3圖為接合至載體基板以形成玻璃-載體組件之玻璃板的透視圖;第4圖說明了於玻璃板中提供第一與第二缺陷之步驟;第5圖說明了使一電磁輻射束沿著第一預定路徑於玻璃板上往復移動之步驟;第6圖說明了沿著第一預定路徑之玻璃板中完整本體切割;第7圖說明使電磁輻射束沿一第二預定路徑於玻璃板上往復移動之一例示步驟;第8圖說明沿著第二預定路徑之玻璃板中完整本體切割;第9圖說明在載體基板中形成一第三缺陷之一例示步驟;第10圖說明使雷射束沿一第三預定路徑於載體基板上往復移動以形成一完整本體裂紋之例示步驟;第11圖說明使雷射束沿著第三預定路徑於載體基板上往復移動以形成一部分裂紋之例示步驟;第12圖說明分離為複數個子組件的玻璃-載體組件;第13圖說明了自該複數個子組件中其一釋放一子板之步驟;第14圖說明了於玻璃板的一第二主要表面中產生曲度之步驟; 第15圖說明了於載體基板的一支撐表面中產生曲度之步驟;及第16圖是在第15圖所述步驟中之玻璃-載體組件的放大圖。 Read with reference to the appended drawings the present invention detailed below, to better understand the present invention, the above-described features, and advantages contemplated, in which: FIG. 1 is a perspective view of a first glass plate; FIG. 2 is a second carrier substrate perspective view; FIG. 3 is bonded to a carrier substrate to form a glass - a perspective view of the carrier assembly of the glass sheet; Fig. 4 illustrates the step of providing the first and second defects in the glass plate; FIG. 5 illustrates the pair a step of reciprocating the beam of electromagnetic radiation along the first predetermined path on the glass sheet; Figure 6 illustrates the complete body cutting in the glass sheet along the first predetermined path; and Figure 7 illustrates the beam of electromagnetic radiation along a second predetermined path of reciprocating movement on a glass plate shows an example of the step; FIG. 8 illustrate a second glass plate is cut along the predetermined path of the complete body; FIG. 9 shows an example of the steps described a third defects formed in the carrier substrate; 10 FIG explaining a laser beam to reciprocate on the carrier substrate to form a complete embodiment shown the body of a crack along a third predetermined path step; FIG. 11 described so that the laser beam is moved reciprocally along a predetermined path in a third substrate on the carrier Forms part of the cracking step illustrated embodiment; FIG. 12 is a description of glass separated plurality of sub-components - carrier assembly; FIG. 13 illustrates the steps from one of the plurality of subassemblies in the release of a daughter board; FIG. 14 illustrates a glass sheet a step of generating second main surface of curvature; FIG. 15 illustrates the step of generating the curvature of the surface of the carrier on a supporting substrate; and FIG. 16 is a glass in the first step of FIG. 15 - carrier assembly Magnified view.

現將於下文中參照如附圖式來更完整說明本發明,在圖式中繪示了所主張發明的例示具體實施例。盡可能在任何時候都使用相同的元件符號來表示相同或類似的部件。然而,所主張發明也可具現為許多不同形式,且不應被解釋為受限於本文所提出的具體實施例。這些例示具體實施例是為了使本發明說明書更為徹底與完整以及對熟習該領域技術之人士傳達所主當發明的範疇而提供。 The invention will now be described more fully hereinafter with reference to the accompanying drawings, in which FIG. Whenever possible, the same component symbols are used to denote the same or similar components. However, the claimed invention may be embodied in many different forms and should not be construed as being limited to the specific embodiments set forth herein. These exemplary embodiments are provided to provide a thorough and complete description of the invention and the scope of the invention as disclosed herein.

第1圖所示,一例示方法包括提供一玻璃板10,該玻璃板10包括一第一主要表面12及與該第一主要表面12相對的一第二主要表面14。在玻璃板10的第一主要表面12與第二主要表面14之間的厚度T1可等於或小於約300微米,例如等於或小於約280微米,例如等於或小於約230微米,例如等於或小於約180微米,例如等於或小於約100微米,例如等於或小於約50微米。玻璃板10可包括至少一個邊緣,以提供曲線形(例如橢圓形、圓形等)之多邊形(舉例而言,例如方形等之矩形)。舉例而言,如圖所示,玻璃板10可進一步包括四個邊緣16182022,這些邊緣定義了排列為所述方形之第一主要表面12的邊界,然在其他示例中,也可提供其他的矩形形狀。 As shown in FIG. 1, an exemplary method comprises providing a glass sheet 10, the glass plate 12 and 10 includes the first major surface 12 a first major surface opposite a second major surface 14. The thickness T1 between the first major surface 12 and the second major surface 14 of the glass sheet 10 can be equal to or less than about 300 microns, such as equal to or less than about 280 microns, such as equal to or less than about 230 microns, such as equal to or less than about 180 microns, for example equal to or less than about 100 microns, such as equal to or less than about 50 microns. The glass sheet 10 can include at least one edge to provide a polygonal shape (e.g., a rectangle such as a square or the like) that is curved (e.g., elliptical, circular, etc.). For example, as shown, the glass sheet 10 can further include four edges 16 , 18 , 20 , 22 that define the boundaries of the first major surface 12 that are arranged in the square, although in other examples, Other rectangular shapes are also available.

轉參第2圖,例示方法係進一步包括提供一載體基板24,該載體基板可由廣泛範圍的材料提供,例如玻璃、陶瓷、玻璃陶瓷或其他材料。根據製程技術或其他需求而定,載體基板24可為透光或不透光,且因此呈現至少部分透明或完全透明、半透明或不透明。載體基板24包括一第一主要表面26、一相對的第二主要表面28以及在第一與第二主要表面2628之間的厚度T2。在某些示例中,厚度T2係視情況為大於或等於500微米。 Referring to Figure 2 , the exemplary method further includes providing a carrier substrate 24 that can be provided by a wide range of materials, such as glass, ceramic, glass ceramic or other materials. Depending on the process technology or other needs, the carrier substrate 24 can be light transmissive or opaque, and thus exhibits at least partially transparent or completely transparent, translucent or opaque. The carrier substrate 24 includes a first major surface 26 , an opposing second major surface 28, and a thickness T2 between the first and second major surfaces 26 , 28 . In some examples, the thickness T2 is optionally greater than or equal to 500 microns.

第2圖中進一步所說明,載體基板24進一步包括定義了第二主要表面28的邊界之邊緣30323436。在某些示例中,載體基板24具有與玻璃板10幾何形狀類似或相同的周邊形狀。舉例而言,所述載體基板24具有與玻璃板10的外方形相同的外方形。在其他示例中,雖非完全相同,但載體基板24會具有幾何上與玻璃板10相似的形狀。舉例而言,載體基板24具有稍微較大、但幾何上與玻璃板10的形狀相似的形狀。提供較大的載體基板24有助於保護玻璃板10的邊緣免受破壞。在某些示例中,載體基板24也具有實質上大於玻璃板10之形狀。在另外一些示例中,載體基板24也具有小於玻璃板10的形狀。 As further illustrated in FIG. 2 , carrier substrate 24 further includes edges 30 , 32 , 34 , 36 that define the boundaries of second major surface 28 . In some examples, carrier substrate 24 has a perimeter shape that is similar or identical to the geometry of glass sheet 10 . For example, the carrier substrate 24 has the same outer square shape as the outer square of the glass sheet 10 . In other examples, although not identical, the carrier substrate 24 will have a shape that is geometrically similar to the glass sheet 10 . For example, the carrier substrate 24 has a shape that is slightly larger but geometrically similar to the shape of the glass sheet 10 . Providing a larger carrier substrate 24 helps protect the edges of the glass sheet 10 from damage. In some examples, the carrier substrate 24 also has a shape that is substantially larger than the glass sheet 10 . In other examples, the carrier substrate 24 also has a shape that is smaller than the glass sheet 10 .

第3圖所示,玻璃板10的第二主要表面14係接合至載體基板24的一支撐表面(例如第一主要表面26),因而形成一玻璃-載體組件42。黏著材料層40係用以將第二玻璃板10的第二主要表面14接合至載體基板24的支撐表面26。此外,也可使用其他接合技術(例如,氫 鍵結)來將玻璃板10的第二主要表面14接合至載體基板24的支撐表面26As shown in FIG . 3 , the second major surface 14 of the glass sheet 10 is bonded to a support surface (e.g., the first major surface 26 ) of the carrier substrate 24 , thereby forming a glass-carrier assembly 42 . Adhesive material layer 40 is used to bond second major surface 14 of second glass sheet 10 to support surface 26 of carrier substrate 24 . In addition, other bonding techniques (eg, hydrogen bonding) may also be used to bond the second major surface 14 of the glass sheet 10 to the support surface 26 of the carrier substrate 24 .

第1圖第3圖可知,玻璃板10和載體基板24的主要表面12142628在形狀上皆為方形,並且具有相同的面積。然而,如上文中關於邊緣所述內容,主要表面12142628可具有不同形狀,例如除了方形以外之矩形、曲線形(例如圓形、橢圓形等)。此外,如先前所述,玻璃板10的第一及第二主要表面1214可具有與載體基板24的第一及第二主要表面2628不同的形狀或面積。舉例而言,載體基板24的第一和第二主要表面2628可為矩形,並且具有比方形的玻璃板10之第一和第二主要表面1214更大的面積。因此,遇到外部物體的首先是載體基板24,藉此可保護玻璃板10的邊緣。載體基板24的第一與第二主要表面2628也可以是矩形且具有比方形的玻璃板10之第一和第二主要表面1214更小的面積。 As can be seen from Figures 1 to 3 , the major surfaces 12 , 14 , 26 , 28 of the glass sheet 10 and the carrier substrate 24 are all square in shape and have the same area. However, as described above with respect to the edges, the major surfaces 12 , 14 , 26 , 28 may have different shapes, such as rectangular, curved (e.g., circular, elliptical, etc.) in addition to square. Moreover, as previously described, the first and second major surfaces 12 , 14 of the glass sheet 10 can have a different shape or area than the first and second major surfaces 26 , 28 of the carrier substrate 24 . For example, the first and second major surfaces 26 , 28 of the carrier substrate 24 can be rectangular and have a larger area than the first and second major surfaces 12 , 14 of the square glass sheet 10 . Therefore, the first encounter with the external object is the carrier substrate 24 , whereby the edge of the glass sheet 10 can be protected. The first and second major surfaces 26 , 28 of the carrier substrate 24 may also be rectangular and have a smaller area than the first and second major surfaces 12 , 14 of the square glass sheet 10 .

例示方法可進一步包括於玻璃板10中提供一第一缺陷44與一第二缺陷46,如第4圖所示。第一和第二缺陷4446可利用各種方法而產生。舉例而言,第一與第二缺陷4446可藉由雷射脈衝或藉由例如劃片、劃線刀輪、鑽石尖刀、壓痕器等機械工具而產生。第一和第二缺陷4446係形成於玻璃板10的任一邊緣16182022上,或是第一和第二缺陷4446可形成於遠離邊緣16182022之玻璃板10的第一主要表面12上。在這個示例中,第一 缺陷44是形成在玻璃板10的邊緣16上,而第二缺陷46是形成在玻璃板10的邊緣22上。 It illustrates a method may further comprise providing a first defect a second defect 46 and 44, as shown in FIG. 4, the glass sheet 10. The first and second defects 44 , 46 can be produced using a variety of methods. For example, the first and second defects 44 , 46 may be generated by laser pulses or by mechanical means such as dicing, scribing cutter wheels, diamond sharpeners, indenters, and the like. The first and second defects 44 , 46 are formed on either edge 16 , 18 , 20 , 22 of the glass sheet 10 , or the first and second defects 44 , 46 may be formed away from the edges 16 , 18 , 20 , The first major surface 12 of the glass sheet 10 of 22 . In this example, the first defect 44 is formed on the edge 16 of the glass sheet 10 and the second defect 46 is formed on the edge 22 of the glass sheet 10 .

例示方法可進一步包括將玻璃板10分離為複數個子板。舉例而言,藉由使電磁輻射束48沿一第一預定路徑50於第一主要表面12上移動,如第5圖所示,玻璃板10係分離為複數個子板。在本示例中,第一預定路徑50包括在第一缺陷44處從玻璃板10的邊緣16延伸至玻璃板10的邊緣20之一直線。然而,在其他示例中,第一預定路徑50會包括曲線。此外,第一預定路徑50是在第一缺陷44的位置處從玻璃板10的邊緣16延伸至玻璃板10的任何其他邊緣。更甚者,第一預定路徑50可包含一封閉路徑,該封閉路徑完全地侷限於第一主要表面12的邊界內,使得該封閉路徑會與玻璃板10的任何邊緣交錯。第一預定路徑50包含沿著或橫越玻璃板10的第一主要表面12而延伸的任何路徑。 The exemplary method can further include separating the glass sheet 10 into a plurality of daughter boards. For example, by moving the electromagnetic radiation beam 48 over the first major surface 12 along a first predetermined path 50 , as shown in FIG . 5 , the glass sheet 10 is separated into a plurality of daughter boards. In the present example, a first predetermined path 50 includes a first defect 44 extends from an edge of the glass sheet 16 to the edge 10 of glass sheet 10, one 20 in a straight line. However, in other examples, the first predetermined path 50 will include a curve. Furthermore, the first predetermined path 50 is extended to any other edge of the glass 10 from the edge 16 of glass sheet 10 at a position 44 of the first defect. Still further, the first predetermined path 50 can include a closed path that is completely confined within the boundaries of the first major surface 12 such that the closed path can be staggered with any edge of the glass sheet 10 . The first predetermined path 50 includes any path that extends along or across the first major surface 12 of the glass sheet 10 .

可使用可移動之雷射輻射裝置52來產生電磁輻射束48及使電磁輻射束48沿著第一預定路徑50往復移動。隨著電磁輻射束48沿著第一預定路徑50往復移動,在第一主要表面12上會形成一加熱區域54。電磁輻射束48可視情況接以一冷卻裝置56,冷卻裝置56係於電磁輻射束48的加熱之後,沿著第一預定路徑50對玻璃板10施用一冷卻流體58,如第5圖進一步所示。冷卻流體58可為液體或氣體或液體與氣體的組合。冷卻流體58的施用係於第一主要表面12上產生一冷卻區域60,該冷卻區域60在溫度上係 低於加熱區域54。此溫度差異的結果是,在玻璃板10中產生一熱應力,熱應力使第一缺陷44轉化為與玻璃板10的第一主要表面12和第二主要表面14交錯的第一完整本體裂紋64。第一完整本體裂紋64接著會隨著電磁輻射束48與冷卻流體58沿第一預定路徑50的往復移動而沿著第一預定路徑50傳播。如圖所示,視情況,第一完整本體裂紋64產生但不傳播至載體基板24中。如第6圖所示,一旦電磁輻射束48與冷卻流體58完全橫越第一預定路徑50,即從第一主要表面12到第二主要表面14、沿著第一預定路徑50產生玻璃板10之完整本體分離,因而使玻璃板10分離為兩個子板6870。此外,因為玻璃板10的第二主要表面14在分離期間與分離之後仍保持接合至載體基板24的支撐表面26,這兩個子板6870係仍保持為沿著它們的分離線實質上彼此接觸或彼此靠近。 The movable laser radiation device 52 can be used to generate the electromagnetic radiation beam 48 and to reciprocate the electromagnetic radiation beam 48 along the first predetermined path 50 . As the beam of electromagnetic radiation 48 reciprocates along the first predetermined path 50 , a heated region 54 is formed on the first major surface 12 . After the beam of electromagnetic radiation 48 optionally connected to a cooling device 56, cooling device 56 based on the heating electromagnetic radiation beam 48, 58, as further shown in FIG. 5 along a first cooling fluid 10 is administered a predetermined path 50 to the glass sheet . Cooling fluid 58 can be a liquid or a gas or a combination of liquid and gas. Cooling fluid administration system 58 is to generate a cooling zone 12 on the first major surface 60, 60 in the cooling area is less than a temperature of the heating zone 54. As a result of this temperature difference, a thermal stress is generated in the glass sheet 10 that converts the first defect 44 into a first complete body crack 64 that is interleaved with the first major surface 12 and the second major surface 14 of the glass sheet 10 . . The first complete body crack 64 then propagates along the first predetermined path 50 as the electromagnetic radiation beam 48 and the cooling fluid 58 reciprocate along the first predetermined path 50 . As shown, the first complete body crack 64 is generated but not propagated into the carrier substrate 24 , as appropriate. As shown in FIG . 6 , once the electromagnetic radiation beam 48 and the cooling fluid 58 completely traverse the first predetermined path 50 , i.e., from the first major surface 12 to the second major surface 14 , along the first predetermined path 50, the glass sheet 10 is produced. The complete body separation thus separates the glass sheet 10 into two daughter boards 68 , 70 . Moreover, because the second major surface 14 of the glass sheet 10 remains bonded to the support surface 26 of the carrier substrate 24 during and after separation, the two daughter boards 68 , 70 remain substantially along their separation line. Get in touch with each other or close to each other.

將玻璃板10分離為複數個子板之步驟係進一步包括使電磁輻射束48沿著一第二預定路徑78於第一主要表面12上方往復移動,如第7圖所示。在本示例中的第二預定路徑78包括在第二缺陷46處從玻璃板10的邊緣22延伸至玻璃板10的邊緣18之一直線。此外,如圖所示,第二預定路徑78可與第一預定路徑50交錯。如圖所示,第二預定路徑78也可取向為與第一預定路徑50呈垂直。然而,第二預定路徑78並不需要與第一預定路徑50垂直;反而是,第二預定路徑78可與第一預定路徑50間形成任何角度。此外,在某些示例中,第二預定路徑78會包含曲線而非直線。 另外,第二預定路徑78可於第二缺陷46的位置處從玻璃板10的邊緣22延伸至玻璃板10的任何其他邊緣。更甚者,第二預定路徑78可包含一封閉路徑,該封閉路徑完全侷限於第一主要表面12的邊界內,因此該封閉路徑會與玻璃板10的任何邊緣交錯。第二預定路徑78可包含沿著或橫越玻璃板10的第一主要表面12而延伸且與該第一預定路徑50交錯的任何路徑。 The glass plate 10 is a step of separating the plurality of sub-plate system further comprises an electromagnetic radiation beam 48 to move along a second predetermined path 78 to reciprocate above the first major surface 12, as shown in FIG. 7. In the present example the second predetermined path 78 includes second defect 46 extending from the edge of the glass to the edge of the glass 10 10 22 18 linear one. Moreover, as shown, the second predetermined path 78 can be interleaved with the first predetermined path 50 . As shown, the second predetermined path 78 can also be oriented perpendicular to the first predetermined path 50 . However, the second predetermined path 78 does not need to be perpendicular to the first predetermined path 50 ; instead, the second predetermined path 78 can form any angle with the first predetermined path 50 . Moreover, in some examples, the second predetermined path 78 will include a curve rather than a straight line. Further, the second predetermined path 78 may extend to any other edge of the glass 10 from the edge 22 of glass sheet 10 at a position 46 of the second defect. Still further, the second predetermined path 78 can include a closed path that is completely confined within the boundaries of the first major surface 12 such that the closed path can be staggered with any edge of the glass sheet 10 . The second predetermined path 78 can include any path that extends along or across the first major surface 12 of the glass sheet 10 and that is interleaved with the first predetermined path 50 .

當電磁輻射束48沿著第二預定路徑78往復移動時,會再一次地在第一主要表面12上形成加熱區域54。電磁輻射束48可視情況接以冷卻裝置56,以於電磁輻射束48的加熱之後沿著第二預定路徑78對玻璃板10施用冷卻流體58,因而形成冷卻區域60。在玻璃板10中會產生熱應力,使第二缺陷46轉化為與玻璃板10的第一主要表面12和第二主要表面14交錯的一第二完整本體裂紋82。第二完整本體裂紋82接著會隨電磁輻射束48與冷卻流體58沿第二預定路徑78的往復移動而沿著第二預定路徑78傳播。 When the electromagnetic radiation beam 48 reciprocates along the second predetermined path 78 , the heating region 54 is again formed on the first major surface 12 . The beam of electromagnetic radiation 48 may optionally be coupled to a cooling device 56 to apply a cooling fluid 58 to the glass sheet 10 along a second predetermined path 78 after heating of the beam of electromagnetic radiation 48 , thereby forming a cooling zone 60 . Thermal stress is generated in the glass sheet 10 to convert the second defect 46 into a second complete body crack 82 that is interleaved with the first major surface 12 and the second major surface 14 of the glass sheet 10 . The second complete body crack 82 then propagates along the second predetermined path 78 as the electromagnetic radiation beam 48 and the cooling fluid 58 reciprocate along the second predetermined path 78 .

如圖所示,視情況,第二完整本體裂紋82產生但不傳播至載體基板24中。最後,第二完整本體裂紋82會沿著第二預定路徑78傳播至兩個子板6870的分離線。因為這兩個子板6870係仍沿著它們的分離線保持為實質上彼此接觸或彼此靠近,第二完整本體裂紋82將繼續傳播通過兩個子板6870的分離線,而不需要有另外的缺陷。因此,如第8圖所示,一旦電磁輻射束48與冷卻流體58完全橫越了第二預定路徑78,就會沿著第二預定路徑78產生從 第一主要表面12到第二主要表面14之玻璃板10之完整本體分離,因而將玻璃板10分離為四個子板86889092。沿著第二預定路徑78之此一分離也可稱為交叉切割,因為沿著第二預定路徑78之分離會與玻璃板10沿著第一預定路徑50之分離交叉。由於在分離期間或分離之後,玻璃板10的第二主要表面14仍保持為接合至載體基板24的支撐表面26,因此這四個子板86889092在分離線上仍保持為實質上彼此接觸或彼此靠近。在此示例中,子板86889092的形成需要半數或較少的起始缺陷數。隨著子板數量增加,需要的起始缺陷相對數量即減少。 As shown, the second complete body crack 82 is generated but not propagated into the carrier substrate 24 , as appropriate. Finally, the second complete body crack 82 propagates along the second predetermined path 78 to the separation line of the two daughter boards 68 , 70 . Because the two daughter boards 68 , 70 are still held substantially in contact with each other or close to each other along their separation line, the second complete body crack 82 will continue to propagate through the separation lines of the two daughter boards 68 , 70 without Need to have additional defects. Thus, as shown in FIG . 8 , once the electromagnetic radiation beam 48 and the cooling fluid 58 have completely traversed the second predetermined path 78 , a second predetermined path 78 is created along the second predetermined path 78 from the first major surface 12 to the second major surface 14. The complete body of the glass sheet 10 is separated, thereby separating the glass sheet 10 into four sub-boards 86 , 88 , 90 , 92 . This separation along the second predetermined path 78 may also be referred to as cross-cutting because the separation along the second predetermined path 78 may intersect the separation of the glass sheet 10 along the first predetermined path 50 . Since the second major surface 14 of the glass sheet 10 remains bonded to the support surface 26 of the carrier substrate 24 during or after separation, the four daughter boards 86 , 88 , 90 , 92 remain substantially separate on the separation line. Get in touch with each other or close to each other. In this example, the formation of daughter boards 86 , 88 , 90 , 92 requires half or less of the number of initial defects. As the number of daughter boards increases, the relative amount of initial defects required decreases.

雖然所述例示方法是沿著兩個預定分離路徑來分離玻璃板10,但在其他示例中,該方法可沿著任何數量的預定分離路徑分離玻璃板10。在這些示例中,可類似地為每一個預定路徑形成一缺陷,並對玻璃板10類似地施用電磁輻射束48與視情況之冷卻流體58,以將缺陷轉化為裂紋,並使裂紋沿著對應的預定路徑傳播。若預定路徑恰巧與玻璃板10的兩個子板之間的分離線交叉,則裂紋將繼續傳播通過分離線,這是因為子板係因玻璃板10和載體基板24的接合而保持為熱接觸之故。 While the illustrated method separates the glass sheets 10 along two predetermined separation paths, in other examples, the method can separate the glass sheets 10 along any number of predetermined separation paths. In these examples, a defect can be similarly formed for each predetermined path, and a beam of electromagnetic radiation 48 and optionally a cooling fluid 58 are applied similarly to the glass sheet 10 to convert the defect into a crack and cause the crack to follow The scheduled path is spread. If the predetermined path happens to intersect the separation line between the two daughter boards of the glass sheet 10 , the crack will continue to propagate through the separation line because the daughter board remains in thermal contact due to the bonding of the glass sheet 10 and the carrier substrate 24 . The reason.

當玻璃板10已經分離為所需數量的子板,即可以各種方式自玻璃-載體組件42釋放一或多個子板。舉例而言,第9圖第13圖說明了自玻璃-載體組件42釋放一或多個子板的一種方式。如第9圖所示,在玻璃板10已經分離為四個子板86889092之後,該方法可包括於載體 基板24中提供一第三缺陷102之步驟。第三缺陷102係形成於載體基板24的任一邊緣30323436上,或是該第三缺陷102可形成於遠離邊緣30323436之載體基板24的第二主要表面28上。基於說明目的,第三缺陷102係呈現為形成在載體基板24的邊緣30上。 When the glass sheet 10 has been separated into the desired number of daughter boards, one or more daughter boards can be released from the glass-carrier assembly 42 in a variety of ways. For example, Figures 9 through 13 illustrate one manner of releasing one or more daughter boards from the glass-carrier assembly 42 . As shown in FIG. 9 , after the glass sheet 10 has been separated into four sub-boards 86 , 88 , 90 , 92 , the method can include the step of providing a third defect 102 in the carrier substrate 24 . Third defect 102 is formed based on either edge 30 of the carrier substrate 24, 32, 34, 36, or the third defect 102 may be formed away from the edge 30 in the second primary, 32, carriers 34, 36 of the substrate 24 On the surface 28 . For purposes of illustration, the third defect 102 is presented as being formed on the edge 30 of the carrier substrate 24 .

在已經形成第三缺陷102之後,藉由使電磁輻射束48沿著一第三預定路徑112相對於載體基板24往復移動,載體基板24係分離為複數個子載體基板,如第10圖所示。較佳的是,第三預定路徑112與第一預定路徑50對齊,並且包括在第三缺陷102的位置處從載體基板24的邊緣30延伸至載體基板24的邊緣34之一直線。然而,第三預定路徑112可包含延伸於載體基板24的第二主要表面28上之任何路徑。 After the third defect 102 has been formed, the electromagnetic radiation by the beam 48 with respect to the carrier substrate 24 reciprocates, the carrier substrate 24 is separated into a plurality of sub-based carrier substrate, as shown in FIG. 10 along a third predetermined path 112. Preferably, the third predetermined path 112 is aligned with the first predetermined path 50 and includes a line extending from the edge 30 of the carrier substrate 24 to the edge 34 of the carrier substrate 24 at the location of the third defect 102 . However, the third predetermined path 112 can include any path that extends over the second major surface 28 of the carrier substrate 24 .

隨著電磁輻射束48沿著第三預定路徑112往復移動,在載體基板24的第二主要表面28上會形成加熱區域54。電磁輻射束48可接以一冷卻裝置56,以於電磁輻射束48的加熱之後,沿著第三預定路徑112對載體基板24施用一冷卻流體58,因而形成冷卻區域60。在載體基板24中會產生熱應力,使第三缺陷102轉化為裂紋116,裂紋116接著會隨電磁輻射束48與冷卻流體58的往復移動而沿著第三預定路徑112傳播。在本具體實施例中,裂紋116是延伸貫穿載體基板24的整體厚度T2之一完整本體裂紋,因此沿著第三預定路徑112產生載體基板24之一完整本體分離。然而,在其他具體實施例中,裂紋116係一部分裂紋, 其僅傳播而部分貫穿載體基板24的厚度T2,因而沿著第三預定路徑112形成一劃痕118,如第11圖所示。在這類具體實施例中,接著對載體基板24施加彎折力,以使載體基板24沿著所形成之劃痕118分離為複數個子載體基板。除了使用電磁輻射以外,也可藉由使用機械劃線技術或其他方式來分離載體基板24。用以分離載體基板24與玻璃板10的方法不需要是相同的。 As the beam of electromagnetic radiation 48 reciprocates along the third predetermined path 112 , a heated region 54 is formed on the second major surface 28 of the carrier substrate 24 . The electromagnetic radiation beam 48 can be coupled to a cooling device 56 to apply a cooling fluid 58 to the carrier substrate 24 along the third predetermined path 112 after heating of the electromagnetic radiation beam 48 , thereby forming a cooling region 60 . In the carrier substrate 24 generates heat stress, the third defect 102 into a crack 116, 116 will then crack with an electromagnetic beam of radiation 48 and 112 spread the cooling fluid 58 is reciprocated along a third predetermined path. In the present embodiment, the crack 116 is a complete body crack extending through one of the overall thicknesses T2 of the carrier substrate 24 , thus creating a complete body separation of the carrier substrate 24 along the third predetermined path 112 . However, in other embodiments, a portion of crack 116 based cracks which propagate only partially through the thickness T2 of the carrier substrate 24, thereby forming a scratch 118, as shown in FIG. 11 along a third predetermined path 112. In such embodiments, the bending force is then applied to the carrier substrate 24, the substrate 24 so that the carrier scratches formed along the separated plurality of sub-carrier substrate 118 is. In addition to the use of electromagnetic radiation, the carrier substrate 24 can also be separated by using mechanical scribing techniques or other means. The method for separating the carrier substrate 24 from the glass sheet 10 need not be the same.

利用劃片及/或上述完整本體切割技術,可將載體基板24分離為任何數量的子載體基板。舉例而言,第12圖說明了在載體基板24已經沿著與第一和第二預定路徑5078(玻璃板10係沿其而分離)的兩個預定路徑分離之後的玻璃-載體組件42。如圖所示,載體基板24已經分離為四個子載體基板120122124126。因此,玻璃-載體組件42係分離為四個子組件130132134136,其中每一個子載體基板120122124126係與複數個子板86889092中的一單一對應子板接合,以形成四個子組件130132134136中其一。這些子組件130132134136中的每一個係用於個別的應用。此外,因為每一個子板86889092都是一個別子組件130132134136的一部分,因此每一個子板86889092都可自其對應的子載體基板120122124126釋放,沒有使子板邊緣與剩餘子板產生接觸而破壞邊緣的風險。舉例而言,第13圖說明了自子載體基板120釋放子組件130的子板86之步驟。子組件130已經與剩餘的 子組件132134136隔離,因此,可在不生使子板86的邊緣接觸剩餘子板889092的風險下釋放子板86The carrier substrate 24 can be separated into any number of sub-carrier substrates using dicing and/or the above-described complete body cutting technique. For example, Figure 12 illustrates the glass-carrier assembly 42 after the carrier substrate 24 has been separated along two predetermined paths from the first and second predetermined paths 50 , 78 (to which the glass sheet 10 is separated). . As shown, the carrier substrate 24 has been separated into four sub-carrier substrates 120 , 122 , 124 , 126 . Therefore, the glass - based carrier assembly 42 is separated into four sub-assemblies 130, 132, 134, 136, wherein each sub-carrier substrate 120, 122, 124, 126 lines and a plurality of daughter boards 86, 88, 90, 92 in a single The corresponding daughter boards are joined to form one of the four sub-assemblies 130 , 132 , 134 , 136 . Each of these sub-components 130 , 132 , 134 , 136 is for an individual application. Moreover, since each of the daughter boards 86 , 88 , 90 , 92 is part of one of the other sub-components 130 , 132 , 134 , 136 , each of the daughter boards 86 , 88 , 90 , 92 can be from its corresponding sub-carrier The substrates 120 , 122 , 124 , 126 are released without the risk of damaging the edges of the daughterboard edges in contact with the remaining daughterboards. For example, Figure 13 illustrates the steps of releasing the daughter board 86 of the subassembly 130 from the subcarrier substrate 120 . Sub-assembly 130 has 132, 134, 136 isolated from the rest of the subassembly, thus, may be born without edge sub-plate 86 makes contact with the remaining sub-plate 88, the sub-plate 86 is released at risk 90, 92.

雖然上述釋放步驟涉及了在玻璃板10已經分離之後再將載體基板24分離為複數個子載體,但在其他示例中,釋放步驟亦可在玻璃板10被分離之前即先將載體基板24分離為複數個子載體。此外,在其他示例中,劃線是先形成於載體基板24中,然後進行玻璃板10的分離,接著對載體基板24施加彎折應力以使載體基板24沿著劃線分離為複數個子載體。 Although the above releasing step involves separating the carrier substrate 24 into a plurality of sub-carriers after the glass sheet 10 has been separated, in other examples, the releasing step may also separate the carrier substrate 24 into plural numbers before the glass sheet 10 is separated. Subcarrier. Further, in other examples, first scribe line is formed in the carrier substrate 24, the glass plate 10 is then separated, bending stress is then applied to the carrier substrate 24 so that the carrier substrate 24 is separated into a plurality of sub carrier along the score line.

第14圖第16圖說明了從玻璃-載體組件42釋放一或多個子板、但不包含將載體基板24分離為子載體基板之替代步驟。舉例而言,在玻璃-載體組件42的玻璃板10已經分離為複數個子板之後,該方法可包括藉由在玻璃板10的第二主要表面14及載體基板24的支撐表面26之至少其一中產生一曲度而自載體基板24分離至少一個子板的至少一部分之步驟。舉例而言,第14圖第15圖說明在玻璃板10已經分離為四個子板86889092之後的玻璃-載體組件42。如第14圖所示,藉由使複數個子板的其中一個子板86的一邊緣部分142上升遠離載體基板24,在玻璃板10的第二主要表面14中產生一雙重彎曲曲度。在僅一個示例中,邊緣部分142係上升遠離而使得相鄰子板8692的相向邊緣表面144146在邊緣部分142升離的同時立即開始移動遠離彼此。舉例而言,在一個示例中,雙重彎曲曲度係使得相向的邊緣表面144146能在邊緣部分142 升離時保持呈實質上彼此平行。由於相向的邊緣表面保持為實質上平行,相向的邊緣表面144146係可於邊緣部分142升離時立即開始移動遠離彼此。然而,會存在有相向的邊緣表面144146在邊緣部分142被升離時呈現稍微不平行的具體實施例。雙重彎曲曲度使邊緣表面144146可於邊緣部分142被升離時保持為實質上平行或稍微不平行,以使子板86自載體基板24撕離。在此方式中,藉由使邊緣部分142上升遠離載體基板24,即可避免子板86的邊緣150152摩擦邊緣表面146。因此,其他釋放技術對於邊緣表面146之破壞即得以避免。子板86是在保持此雙重彎曲曲度下自載體基板24完全釋放。然而,也會有僅在子板86的一部分自載體基板24釋放時保持該雙重彎曲曲度之具體實施例。同時,可視情況地使用其他單一彎曲幾何形狀、以及從外邊緣(而不是如第14圖所示內邊緣表面144)開始釋放子板86之幾何形狀,以使子板86自載體基板24釋放。 Figures 14 through 16 illustrate an alternative step of releasing one or more daughter plates from the glass-carrier assembly 42 but without separating the carrier substrate 24 into sub-carrier substrates. For example, after the glass sheet 10 of the glass-carrier assembly 42 has been separated into a plurality of daughter boards, the method can include at least one of the second major surface 14 of the glass sheet 10 and the support surface 26 of the carrier substrate 24 . The step of separating at least a portion of the at least one daughterboard from the carrier substrate 24 is produced in a curvature. For example, Figures 14 and 15 illustrate the glass-carrier assembly 42 after the glass sheet 10 has been separated into four daughter sheets 86 , 88 , 90 , 92 . As shown in Figure 14, by making a plurality of sub-sub-plate wherein a plate portion 142 rising edge 86 away from the carrier substrate 24, to produce a double curvature in the bent glass sheet 10 of the second major surface 14. In just one example, the edge portions 142 are raised away such that the opposing edge surfaces 144 , 146 of the adjacent daughter boards 86 , 92 begin to move away from each other as the edge portions 142 are lifted off. For example, in one example, the double bend curvature is such that the opposing edge surfaces 144 , 146 can remain substantially parallel to each other as the edge portion 142 is lifted off. Since the opposing edge surfaces remain substantially parallel, the opposing edge surfaces 144 , 146 can begin to move away from each other as soon as the edge portion 142 is lifted off. However, there may be specific embodiments in which the opposing edge surfaces 144 , 146 appear slightly non-parallel when the edge portion 142 is lifted off. The double bend curvature causes the edge surfaces 144 , 146 to remain substantially parallel or slightly non-parallel when the edge portion 142 is lifted away to tear the daughterboard 86 away from the carrier substrate 24 . In this manner, by raising the edge portion 142 away from the carrier substrate 24 , the edges 150 , 152 of the daughterboard 86 can be prevented from rubbing against the edge surface 146 . Therefore, damage to the edge surface 146 by other release techniques is avoided. The daughter board 86 is completely released from the carrier substrate 24 while maintaining this double bending curvature. However, there may be specific embodiments for maintaining the double bend curvature only when a portion of the daughter board 86 is released from the carrier substrate 24 . At the same time, other single curved geometries can be used as appropriate, and the geometry of the daughterboard 86 can be released from the outer edge (rather than the inner edge surface 144 as shown in FIG . 14 ) to release the daughterboard 86 from the carrier substrate 24 .

轉參第15圖第16圖,在另外的示例中,係於載體基板24的支撐表面26中產生曲度,以自載體基板24釋放子板86的至少一部分。由第15圖第16圖可知,產生曲度會使相鄰的成對子板8692的一對相向邊緣表面144146沿著第一主要表面12的方向D平移遠離彼此,以於該對相向邊緣表面144146之間產生一側向間隙156。間隙156的存在可避免子板86的邊緣150152在子板86的邊緣部分142升離載體基板24時摩擦邊緣表面146。此 外,可於使邊緣部分142上升遠離載體基板24時進一步於玻璃板10的第二主要表面14中產生雙重或單一彎曲曲度,以助於進一步避免子板86的邊緣150152在子板86的邊緣部分142上升遠離時摩擦邊緣表面146。子板86係自載體基板24完全釋放,同時仍保持載體基板24的支撐表面26中之曲度。然而,也會有僅在子板86的一部分自載體基板24釋放時保持載體基板24的支撐表面26中的曲度之具體實施例。 Transfected with reference to FIG. 15 to FIG. 16, in another example, based on the generated surface of the carrier 26 supports the curvature of substrate 24, at least a portion of the carrier substrate 24 from the sub-plate 86 is released. As can be seen from Figures 15 and 16 , the resulting curvature causes the pair of opposing edge surfaces 144 , 146 of adjacent pairs of daughter plates 86 , 92 to translate away from each other along the direction D of the first major surface 12 . A lateral gap 156 is created between the pair of opposing edge surfaces 144 , 146 . The presence of the gap 156 to avoid edge sub-plate 86 may be 150, 152 at the edge portion 142 of the sub-plate 86 is lifted off the edge 24 when the friction surface 146 of the carrier substrate. In addition, a double or single bending curvature may be created in the second major surface 14 of the glass sheet 10 as the edge portion 142 is raised away from the carrier substrate 24 to help further avoid the edges 150 , 152 of the daughterboard 86 in the daughterboard. The edge portion 142 of the 86 is raised away from the friction edge surface 146 . The daughter board 86 is completely released from the carrier substrate 24 while still maintaining the curvature in the support surface 26 of the carrier substrate 24 . However, there may be specific embodiments for maintaining the curvature in the support surface 26 of the carrier substrate 24 only when a portion of the daughter board 86 is released from the carrier substrate 24 .

雖然第14圖第16圖說明了從玻璃-載體組件42釋放一或多個子板、但不包括將載體基板24分離為子載體基板之步驟,但也會存在從玻璃-載體組件42釋放一或多個子板、並且包括上述將載體基板24分離為子載體基板及於玻璃板10的第二主要表面14與載體基板24的支撐表面26中至少其一中產生一曲度的具體實施例。舉例而言,在玻璃-載體組件42的玻璃板10已經分離為四個子板86889092之後,載體基板24係沿著一單一預定路徑而分離,以產生兩個子組件,其中每一個子組件都包括接合至一子載體的兩個子板。接著於玻璃板10的第二主要比面14和載體基板24的支撐表面26之至少其中一個中產生曲度,以自其中一個子組件移除其中一個子板。 Although Figures 14 through 16 illustrate the release of one or more daughter boards from the glass-carrier assembly 42 , but do not include the step of separating the carrier substrate 24 into sub-carrier substrates, there may be a release from the glass-carrier assembly 42. Or a plurality of daughter boards, and including the above-described embodiment of separating the carrier substrate 24 into the sub-carrier substrate and producing a curvature in at least one of the second major surface 14 of the glass sheet 10 and the support surface 26 of the carrier substrate 24 . For example, after the glass sheet 10 of the glass-carrier assembly 42 has been separated into four daughter boards 86 , 88 , 90 , 92 , the carrier substrate 24 is separated along a single predetermined path to produce two sub-assemblies, wherein Each subassembly includes two daughter boards joined to a subcarrier. A curvature is then produced in at least one of the second major specific face 14 of the glass sheet 10 and the support surface 26 of the carrier substrate 24 to remove one of the daughter boards from one of the subassemblies.

上述例示方法可提供優於一般雷射劃線技術的數項優點。舉例而言,玻璃板之一般雷射劃線技術需要至少兩個步驟,包括產生一劃痕,然後對玻璃板施加一應力,以沿著劃痕線分離玻璃板。同時,在涉及施加彎折或剪應 力之機械分離製程期間會產生機械缺陷。在對雷射入射側評估張應力對壓縮應力的關係時,這可能會產生邊緣強度的差異。然而,上述方法藉由在玻璃板10中產生完整本體裂紋6482(其係於不需要對玻璃板10施加應力之額外步驟下分離玻璃板10)而簡化了分離製程。另一個優點是,上述方法可使得在具有交錯分離線的交叉切割應用期間所產生之邊緣破壞量達到最小。因為在例示方法中的玻璃板10係接合(例如利用黏著劑)至載體基板24,所形成之任何子板將沿著它們的分離線保持實質上彼此接觸或靠近。因此,當任何裂紋被傳播橫越一現有分離線時,即不需要為了使裂紋繼續傳播橫越分線而產生任何邊緣缺陷。的確,如第8圖所示,子板90是在不需要沿其周徑產生任何邊緣缺陷下形成。另外一個優點是,上述方法有助於在藉由將玻璃-載體組件42分離為複數個獨立的子組件(其中每一個子組件都具有一單一子板)、或藉由在玻璃板10的第二主要表面14及載體基板24的支撐表面26之至少其中一個中產生曲度而自載體基板24移除玻璃子板時,避免對玻璃子板產生邊緣破壞。 The above exemplary method can provide several advantages over the general laser scribing technique. For example, a typical laser scribing technique for a glass sheet requires at least two steps, including creating a scratch, and then applying a stress to the glass sheet to separate the glass sheet along the score line. At the same time, mechanical defects can occur during mechanical separation processes involving the application of bending or shear stress. This may result in a difference in edge strength when evaluating the relationship between tensile stress and compressive stress on the incident side of the laser. However, by the method described above to produce a complete body of cracks in the glass sheet 1064, 82 (which need not tied to the glass sheet 10 applied to the glass plate 10 an additional separation step in stress) simplifies the separation process. Another advantage is that the above method minimizes the amount of edge damage generated during cross-cutting applications with staggered separation lines. Because the glass sheets 10 in the exemplary method are bonded (e.g., with an adhesive) to the carrier substrate 24 , any of the daughter sheets formed will remain substantially in contact with or in close proximity along their separation lines. Thus, when any crack is propagated across an existing separation line, there is no need to create any edge defects in order for the crack to continue to propagate across the split line. Indeed, as shown in Figure 8 , the daughterboard 90 is formed without the need to create any edge defects along its circumference. Another advantage is that the above method facilitates the separation of the glass-carrier assembly 42 into a plurality of individual sub-assemblies (each of which has a single sub-plate) or by the glass sheet 10 two support surfaces 14 and the major surface 26 of the carrier substrate 24 wherein at least one of the curvature generated when the carrier substrate 24 and removing the glass from the sub-plate, to avoid damage to the edge of the daughter board glass.

現將說明發明人已經使用上述方法而進行之實驗的實例。 An example of an experiment that the inventors have performed using the above method will now be described.

實例1 Example 1

在一個實例中,將一玻璃板接合至一載體玻璃基板,該玻璃板包括可從紐約州康寧市康寧公司取得之Corning® Willow® Glass,且其所具厚度為130微 米;該載體玻璃基板包括可從紐約州康寧市康寧公司所取得之Corning® EAGLE XG® Glass,且其所具厚度為700微米。載體玻璃基板係塗有電漿聚合化鐵氟龍(-PPT)以增進接合及剝離。然後利用鑽石尖刀或劃線刀輪在玻璃板的邊緣區域中產生缺陷。然後,利用400W RF-激發之CO2雷射進行玻璃板的CO2雷射交叉切割。雷射束會被擴展,並利用非對稱球面透鏡進行聚焦,以於玻璃板的表面上產生一矩形覆蓋區,該矩形覆蓋區的大小大約是45mm長及1.5mm寬。雷射束在它的長軸(45mm)和短軸(1.5mm)上都具有上部帽型強度分佈。切割是沿著覆蓋區的長軸進行。在雷射束之後接以一噴霧,利用去離子水作為冷卻劑來淬冷玻璃板。在交叉切割期間,雷射束與噴霧是在下列條件下操作 In one example, a glass sheet is bonded to a carrier glass substrate comprising Corning® Willow® Glass available from Corning Incorporated, Corning, NY, and having a thickness of 130 microns; the carrier glass substrate includes Corning® EAGLE XG® Glass, available from Corning Incorporated, Corning, NY, and has a thickness of 700 microns. The carrier glass substrate is coated with a plasma polymerized Teflon (-PPT) to enhance bonding and peeling. Defects are then created in the edge regions of the glass sheets using diamond sharpeners or scribing cutter wheels. The CO 2 laser cross-cut of the glass sheets was then performed using a 400 W RF-excited CO 2 laser. The laser beam is expanded and focused using an asymmetric spherical lens to create a rectangular footprint on the surface of the glass sheet that is approximately 45 mm long and 1.5 mm wide. The laser beam has an upper hat-type intensity distribution on both its long axis (45 mm) and short axis (1.5 mm). The cutting is done along the long axis of the footprint. A spray is applied after the laser beam, and deionized water is used as a coolant to quench the glass plate. During cross-cutting, the laser beam and spray are operated under the following conditions

雷射功率:160W Laser power: 160W

水流量:10sccm Water flow: 10sccm

空氣流量:3lpm Air flow: 3lpm

切割速度:250mm Cutting speed: 250mm

利用CO2雷射進行第一次切割,然後進行與第一次切割痕交錯之第二次切割。針對第一次與第二次切割痕都觀察到完整本體裂紋。觀察到第二次切割痕係不受阻礙地傳播通過第一次切割痕。可輕易從載體基板提取出上述交叉切割製程所產生的玻璃子板。 The first cut was performed using a CO 2 laser and then a second cut was made interleaving with the first cut. Complete bulk cracks were observed for both the first and second cut marks. It was observed that the second cut line propagated unimpeded through the first cut mark. The glass sub-board produced by the above cross-cutting process can be easily extracted from the carrier substrate.

實例2 Example 2

在另一實例中,將包括Corning® Willow® Glass之一玻璃板接合至包括Corning® EAGLE XG® Glass之一玻璃板,以產生一玻璃-載體組件。載體玻璃基板係塗有PPT以促進接合與剝離。然後利用鑽石尖刀或劃線刀輪在玻璃板的邊緣區域中產生缺陷。利用與實例1中所述相同之參數切割玻璃板。然而,在切割之前,利用雷射束於載體基板上形成劃痕線。接著對玻璃-載體組件施加一彎折應力,以傳播劃痕線的裂紋,並且沿著劃痕線使載體基板破裂。裂紋並不會傳播到玻璃板中。接著在玻璃板中起始一完整本體裂紋,並使其傳播以分離玻璃板。 In another example, a glass sheet comprising one of Corning® Willow® Glass is bonded to a glass sheet comprising one of Corning® EAGLE XG® Glass to produce a glass-carrier assembly. The carrier glass substrate is coated with PPT to promote bonding and peeling. Defects are then created in the edge regions of the glass sheets using diamond sharpeners or scribing cutter wheels. The glass sheets were cut using the same parameters as described in Example 1. However, a scribe line is formed on the carrier substrate using a laser beam prior to dicing. A bending stress is then applied to the glass-carrier assembly to propagate the cracks in the score line and to rupture the carrier substrate along the score line. Cracks do not propagate into the glass sheet. A complete bulk crack is then initiated in the glass sheet and propagated to separate the glass sheets.

實例3 Example 3

在另一實例中,將包括Corning® Willow® Glass之一玻璃板接合至包括Corning® EAGLE XG® Glass之一玻璃板,以產生一玻璃-載體組件。載體玻璃基板係塗有PPT以促進接合與剝離。然後利用鑽石尖刀或劃線刀輪在玻璃板的邊緣區域中產生缺陷。然後利用與實例1中所述相同之參數切割玻璃板。然後,於載體玻璃基板上進行雷射交叉劃線製程。小心地使雷射劃痕線與玻璃板上的切割痕對齊。接著對玻璃-載體組件施加彎折應力,以使載體玻璃沿著劃痕線破裂。 In another example, a glass sheet comprising one of Corning® Willow® Glass is bonded to a glass sheet comprising one of Corning® EAGLE XG® Glass to produce a glass-carrier assembly. The carrier glass substrate is coated with PPT to promote bonding and peeling. Defects are then created in the edge regions of the glass sheets using diamond sharpeners or scribing cutter wheels. The glass sheets were then cut using the same parameters as described in Example 1. Then, a laser cross-hatch process is performed on the carrier glass substrate. Carefully align the laser scratch line with the cut marks on the glass. A bending stress is then applied to the glass-carrier assembly to cause the carrier glass to rupture along the score line.

熟習該領域技術人士將可理解,對於本發明所進行的各種修飾例與變化例皆不背離本發明之精神與範疇。因此,本發明意欲涵蓋在如附申請專利範圍及其等效例的範疇內所提供之各種本發明修飾例與變化例。 It will be understood by those skilled in the art that various modifications and changes may be made without departing from the spirit and scope of the invention. Therefore, the present invention is intended to cover various modifications and variations of the present invention as set forth in the appended claims.

10‧‧‧玻璃板 10‧‧‧ glass plate

12‧‧‧第一主要表面 12‧‧‧ first major surface

14‧‧‧第二主要表面 14‧‧‧ second major surface

16‧‧‧邊緣 16‧‧‧ edge

20‧‧‧邊緣 20‧‧‧ edge

22‧‧‧邊緣 22‧‧‧ edge

24‧‧‧載體基板 24‧‧‧ Carrier substrate

42‧‧‧玻璃-載體組件 42‧‧‧Glass-carrier assembly

46‧‧‧第二缺陷 46‧‧‧second defect

48‧‧‧電磁輻射束 48‧‧‧Electromagnetic radiation beam

50‧‧‧第一預定路徑 50‧‧‧First scheduled path

52‧‧‧雷射輻射裝置 52‧‧‧Laser radiation device

54‧‧‧加熱區域 54‧‧‧heating area

56‧‧‧冷卻裝置 56‧‧‧Cooling device

58‧‧‧冷卻流體 58‧‧‧Cooling fluid

60‧‧‧冷卻區域 60‧‧‧Cooling area

64‧‧‧第一完整本體裂紋 64‧‧‧First complete body crack

Claims (10)

一種用於分離一玻璃板的方法,包括以下步驟:(I)提供一玻璃板,該玻璃板包括一第一主要表面和與該第一主要表面相對的一第二主要表面,其中一黏著材料層係將該玻璃板的該第二主要表面接合至一載體基板的一支撐表面,且該第一主要表面與該第二主要表面之間的一厚度等於或小於約300微米;(II)於該玻璃板中提供一第一缺陷;及(III)藉由使一電磁輻射束沿一第一預定路徑於該第一主要表面上往復移動,將該玻璃板分離為複數個子板,以:(a)將該第一缺陷轉換為與該玻璃板的該第一主要表面和該第二主要表面交錯的一第一完整本體裂紋;及(b)使該第一完整本體裂紋沿著該第一預定路徑傳播,藉此沿著該第一預定路徑產生該玻璃板之一完整本體分離,而該玻璃板的該第二主要表面仍保持接合至該載體基板的該支撐表面。 A method for separating a glass sheet, comprising the steps of: (I) providing a glass sheet, the glass sheet comprising a first major surface and a second major surface opposite the first major surface, wherein an adhesive material Laminating the second major surface of the glass sheet to a support surface of a carrier substrate, and a thickness between the first major surface and the second major surface is equal to or less than about 300 microns; (II) Providing a first defect in the glass sheet; and (III) separating the glass sheet into a plurality of daughter boards by reciprocating a beam of electromagnetic radiation along the first predetermined path along the first predetermined path to: ( a) converting the first defect into a first complete body crack interleaved with the first major surface and the second major surface of the glass sheet; and (b) causing the first complete body crack along the first A predetermined path propagates whereby a complete body separation of the glass sheet is created along the first predetermined path while the second major surface of the glass sheet remains bonded to the support surface of the carrier substrate. 如請求項1所述之方法,其中步驟(II)進一步包括以下步驟:於該玻璃板中提供一第二缺陷,且步驟(III)之將該玻璃板分離為複數個子板係進一步包括以下步驟:使一電磁輻射束沿著一第二預定路徑於該第一 主要表面上往復移動,以:(a)將該第二缺陷轉換為與該第一主要表面和該第二主要表面交錯的一第二完整本體裂紋;及(b)使該第二完整本體裂紋沿著該第二預定路徑傳播,藉此沿著該第二預定路徑產生該玻璃板之一完整本體分離,而該玻璃板的該第二主要表面仍保持接合至該載體基板的該支撐表面。 The method of claim 1, wherein the step (II) further comprises the steps of: providing a second defect in the glass sheet, and separating the glass sheet into a plurality of sub-plate systems in the step (III) further comprises the following steps : causing a beam of electromagnetic radiation to follow the first predetermined path along the second Reciprocatingly moving over the major surface to: (a) convert the second defect into a second complete body crack interleaved with the first major surface and the second major surface; and (b) cause the second complete body crack Propagating along the second predetermined path whereby a complete body separation of the glass sheet is produced along the second predetermined path while the second major surface of the glass sheet remains bonded to the support surface of the carrier substrate. 如請求項2所述之方法,其中該第二預定路徑與該第一預定路徑交錯。 The method of claim 2, wherein the second predetermined path is interleaved with the first predetermined path. 如請求項1所述之方法,進一步包括步驟(IV):藉由於該玻璃板的該第二主要表面與該載體基板的該支撐表面中至少其一中產生一曲度,自該載體基板釋放至少一個子板的至少一部分。 The method of claim 1, further comprising the step (IV) of releasing from the carrier substrate by generating a curvature in at least one of the second major surface of the glass sheet and the support surface of the carrier substrate At least a portion of at least one daughter board. 如請求項4所述之方法,其中步驟(IV)進一步包括以下步驟:自該載體玻璃完全釋放至少一個子板,同時保持該曲度。 The method of claim 4, wherein the step (IV) further comprises the step of completely releasing at least one daughterboard from the carrier glass while maintaining the curvature. 如請求項4所述之方法,其中步驟(IV)包括以下步驟:藉由使該複數個子板的其中一個子板的一邊緣部分上升遠離該載體玻璃,在該玻璃板的該第二主要表面中產生一雙重彎曲曲度。 The method of claim 4, wherein the step (IV) comprises the step of: lifting an edge portion of one of the plurality of daughter boards away from the carrier glass, the second major surface of the glass sheet Produces a double bending curvature. 如請求項1所述之方法,進一步包括以下步驟:(IV)於該載體基板中提供一第二缺陷;及 (V)藉由使一電磁輻射束沿著一第二預定路徑而相對於該載體基板往復移動,使該載體基板分離為複數個子載體基板。 The method of claim 1, further comprising the steps of: (IV) providing a second defect in the carrier substrate; (V) separating the carrier substrate into a plurality of sub-carrier substrates by reciprocating the electromagnetic radiation beam relative to the carrier substrate along a second predetermined path. 如請求項7所述之方法,其中該第一預定路徑與該第二預定路徑對齊。 The method of claim 7, wherein the first predetermined path is aligned with the second predetermined path. 如請求項7所述之方法,其中使在步驟(V)中使該電磁輻射束往復移動係將該第二缺陷轉換為延伸貫穿該載體基板之一第二完整本體裂紋,且使該第二裂紋沿著該第二預定路徑傳播係沿著該第二預定路徑產生該載體基板之一完整本體分離。 The method of claim 7, wherein causing the electromagnetic radiation beam to reciprocate in step (V) converts the second defect into a second complete body crack extending through the carrier substrate, and causing the second A propagation along the second predetermined path along the second predetermined path produces a complete body separation of the carrier substrate. 如請求項4所述之方法,其中步驟(IV)係使一對相鄰子板的至少一對相向邊緣表面沿著該第一主要表面的一方向平移遠離彼此,以於該對相向的邊緣表面之間產生一側向間隙。 The method of claim 4, wherein the step (IV) is to translate at least one pair of opposing edge surfaces of a pair of adjacent daughterboards away from each other along a direction of the first major surface to the opposite edges A lateral gap is created between the surfaces.
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