TW201833635A - Glass substrate for display and method for manufacturing glass substrate for display provides a glass substrate for stripping the electrified display - Google Patents

Glass substrate for display and method for manufacturing glass substrate for display provides a glass substrate for stripping the electrified display Download PDF

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TW201833635A
TW201833635A TW107105521A TW107105521A TW201833635A TW 201833635 A TW201833635 A TW 201833635A TW 107105521 A TW107105521 A TW 107105521A TW 107105521 A TW107105521 A TW 107105521A TW 201833635 A TW201833635 A TW 201833635A
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glass
glass substrate
display
manufacturing
ribbon
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TWI741148B (en
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安田興平
井川信彰
林泰夫
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日商旭硝子股份有限公司
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    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • G02F1/133Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/1333Constructional arrangements; Manufacturing methods
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03CCHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
    • C03C15/00Surface treatment of glass, not in the form of fibres or filaments, by etching
    • CCHEMISTRY; METALLURGY
    • C03GLASS; MINERAL OR SLAG WOOL
    • C03BMANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
    • C03B18/00Shaping glass in contact with the surface of a liquid
    • C03B18/02Forming sheets
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/13Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on liquid crystals, e.g. single liquid crystal display cells
    • G02F1/133Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/1333Constructional arrangements; Manufacturing methods
    • G02F1/133302Rigid substrates, e.g. inorganic substrates

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  • Physics & Mathematics (AREA)
  • Chemical & Material Sciences (AREA)
  • Nonlinear Science (AREA)
  • Mathematical Physics (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Engineering & Computer Science (AREA)
  • Materials Engineering (AREA)
  • Organic Chemistry (AREA)
  • Inorganic Chemistry (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • General Chemical & Material Sciences (AREA)
  • Geochemistry & Mineralogy (AREA)
  • Glass Compositions (AREA)
  • Surface Treatment Of Glass (AREA)
  • Re-Forming, After-Treatment, Cutting And Transporting Of Glass Products (AREA)
  • Liquid Crystal (AREA)

Abstract

The invention provides a glass substrate for stripping the electrified display and a manufacturing method of the glass substrate. The invention discloses a glass substrate for a display. The glass substrate is characterized in the average fluorine concentration (mol%) of 0 to 10 nm formed on the surface of the glass, which is opposite to the surface of the semiconductor element forming surface of the glass substrate, is set to be F0 to 10 nm. When the average fluorine concentration of 100 to 400 nm formed from the surface of the glass is set as F100 to 400 nm, F0-10 nm/F100-400 nm ≥ 3, and the surface roughness Ra of the glass surface opposite to the surface of the semiconductor element forming surface is 0.3 nm or more.

Description

顯示器用玻璃基板、及顯示器用玻璃基板之製造方法Glass substrate for display and manufacturing method of glass substrate for display

本發明係關於一種顯示器用玻璃基板、及顯示器用玻璃基板之製造方法。The present invention relates to a glass substrate for a display and a method for manufacturing a glass substrate for a display.

於平板顯示器(FPD)中,使用在玻璃基板上形成有透明電極、半導體元件等者作為基板。例如於液晶顯示器(LCD)中,使用在玻璃基板上形成有透明電極、TFT(Thin Film Transistor,薄膜電晶體)等者作為基板。 於玻璃基板上之透明電極、半導體元件等之形成係於如下狀態下進行:將玻璃基板之與半導體元件形成面相反側之玻璃表面藉由真空吸附而固定於吸附台上。但是,於將形成有透明電極、半導體元件等之玻璃基板自吸附台加以剝離時,玻璃基板帶電,而發生TFT等半導體元件之靜電破壞。 為了抑制剝離帶電之產生,而對連接於吸附台之側之玻璃基板之表面進行表面粗糙化處理,減小玻璃基板與吸附台之接觸面積。作為表面粗糙化處理之方法,例如已知有將玻璃基板之表面藉由大氣壓電漿製程進行化學處理之方法(專利文獻1)。 [先前技術文獻] [專利文獻] [專利文獻1]國際公開第2010/128673號In a flat panel display (FPD), a substrate in which a transparent electrode, a semiconductor element, or the like is formed on a glass substrate is used. For example, in a liquid crystal display (LCD), a transparent electrode, a TFT (Thin Film Transistor), or the like is formed on a glass substrate as a substrate. The formation of transparent electrodes, semiconductor elements, and the like on a glass substrate is performed in a state where the glass surface of the glass substrate opposite to the semiconductor element formation surface is fixed on the adsorption table by vacuum adsorption. However, when a glass substrate on which a transparent electrode, a semiconductor element, or the like is formed is peeled off from an adsorption stage, the glass substrate is charged, and electrostatic destruction of a semiconductor element such as a TFT occurs. In order to suppress the occurrence of peeling and charging, the surface of the glass substrate connected to the side of the adsorption table is subjected to a surface roughening treatment to reduce the contact area between the glass substrate and the adsorption table. As a method of surface roughening treatment, for example, a method of chemically treating the surface of a glass substrate by an atmospheric piezoelectric slurry process is known (Patent Document 1). [Prior Art Literature] [Patent Literature] [Patent Literature 1] International Publication No. 2010/128673

[發明所欲解決之問題] 但是,先前方法並未考慮玻璃基板與吸附台之功函數之差,因而有不充分地抑制剝離帶電之產生,而引起半導體元件之靜電破壞之情況。 本發明係鑒於上述問題而成者,其提供一種於自吸附台加以剝離時不易產生剝離帶電之顯示器用玻璃基板、及其製造方法。 [解決問題之技術手段] 本發明提供一種顯示器用玻璃基板,其特徵在於:於將自玻璃基板之與半導體元件形成面相反側之玻璃表面起深度0~10 nm之氟濃度(mol%)之平均值設為F0-10 nm ,並將自該玻璃表面起深度100~400 nm之氟濃度(mol%)之平均值設為F100-400 nm 時,F0-10 nm /F100-400 nm ≧3,且與上述半導體元件形成面相反側之玻璃表面之表面粗糙度Ra為0.3 nm以上。 又,本發明提供一種顯示器用玻璃基板之製造方法,其特徵在於:具有對在熱處理裝置內被搬送之板玻璃之一表面供給含有氟化氫(HF)之氣體之程序,並且 上述板玻璃之一表面為玻璃基板之與半導體元件形成面相反側之玻璃表面, 上述含有HF之氣體之HF濃度為0.5~30 vol%, 供給上述含有HF之氣體時之玻璃表面溫度為500~900℃。 [發明之效果] 本發明之顯示器用玻璃基板於自吸附台加以剝離時不易產生剝離帶電。[Problems to be Solved by the Invention] However, in the previous method, the difference between the work function of the glass substrate and the adsorption table was not taken into consideration, and thus the generation of peeling and charging was not sufficiently suppressed, which may cause electrostatic destruction of the semiconductor element. The present invention has been made in view of the above-mentioned problems, and provides a glass substrate for a display that is less prone to peeling and charging when peeled from a suction table, and a method for manufacturing the same. [Technical means to solve the problem] The present invention provides a glass substrate for a display, which is characterized in that a fluorine concentration (mol%) of 0 to 10 nm in depth is formed from a glass surface on the opposite side of the glass substrate from the semiconductor element formation surface. The average value is set to F 0-10 nm , and the average value of the fluorine concentration (mol%) at a depth of 100 to 400 nm from the glass surface is set to F 100-400 nm , F 0-10 nm / F 100- 400 nm ≧ 3, and the surface roughness Ra of the glass surface on the opposite side of the semiconductor element formation surface is 0.3 nm or more. In addition, the present invention provides a method for manufacturing a glass substrate for a display, which is characterized by having a procedure for supplying a gas containing hydrogen fluoride (HF) to one surface of a sheet glass to be transported in a heat treatment device, and one surface of the above sheet glass. The glass surface on the opposite side of the semiconductor element formation surface of the glass substrate, the HF concentration of the HF-containing gas is 0.5 to 30 vol%, and the glass surface temperature when the HF-containing gas is supplied is 500 to 900 ° C. [Effects of the Invention] When the glass substrate for a display of the present invention is peeled off from an adsorption stage, it is unlikely to be charged with peeling.

[顯示器用玻璃基板] 以下,對本發明之實施形態之顯示器用玻璃基板進行說明。 關於本實施形態之顯示器用玻璃基板,其玻璃組成並無特別限定,可為鈉鈣矽酸鹽玻璃、鋁矽酸鹽玻璃、硼矽酸玻璃、無鹼玻璃等範圍廣泛之玻璃組成。 一般而言,關於接觸帶電,若物質彼此之功函數之差較大則容易產生。所謂功函數係指對於將處於固體內之電子取出至固體外、準確為取出至真空中所需之最小限度之能量之大小。因電子自功函數較小之物質向較大之物質遷移,而產生帶電。玻璃基板因與吸附台之功函數之差而帶電。 因此,本申請發明者等人為了減少玻璃基板之帶電量,而著眼於玻璃基板之功函數。然而,測定玻璃基板之功函數之方法尚未確立。 本申請發明者等人經過努力研究,發現玻璃基板之表面附近和內部之氟原子濃度差係與玻璃基板和吸附台之功函數之差相關。 即,藉由在玻璃基板之表面附近使陰電性較高之氟原子高濃度化,會引起能階變化,從而使玻璃基板之功函數變化。 一般認為玻璃基板之帶電量取決於玻璃基板與吸附台之功函數之差(高電阻絕緣玻璃之接觸帶電特性,北林宏佳、藤井治久,電學論A,125卷2號,179-184頁,2005年),藉由使氟原子侵入玻璃基板之表面附近會縮小該差。 關於本實施形態之顯示器用玻璃基板,於將自玻璃基板之與半導體元件形成面相反側之玻璃表面起深度0~10 nm之氟濃度(mol%)之平均值設為F0-10 nm ,且將自該玻璃表面起深度100~400 nm之氟濃度(mol%)之平均值設為F100-400 nm 時,F0-10 nm /F100-400 nm ≧3。 藉此,玻璃基板與吸附台之功函數之差變小,而可抑制玻璃基板之剝離帶電。 此處,將玻璃基板之表面附近之氟濃度設為上述F0-10 nm ,且將玻璃基板之內部之氟濃度設為上述F100-400 nm 之原因如下。 接觸帶電之電子遷移主要發生於自玻璃基板表面起深度0~10 nm之區域,且受到該區域與深度100~400 nm之區域之相互作用所控制。 再者,上述F0-10 nm 及F100-400 nm 係藉由X射線光電子光譜分析(XPS)而測定。 關於本實施形態之顯示器用玻璃基板,較佳為F0-10 nm /F100-400 nm ≧5,更佳為F0-10 nm /F100-400 nm ≧10。 若玻璃基板之表面附近與玻璃基板之內部之氟原子濃度差過大,則霧度惡化,故而欠佳。 F0-10 nm /F100-400 nm ≦150能夠抑制霧度之惡化,故而較佳,更佳為F0-10 nm /F100-400 nm ≦100。 又,玻璃表面之表面粗糙度越大,玻璃基板與吸附台之接觸面積變得越小,而不易引起電子之遷移,因此可抑制玻璃基板之剝離帶電(高電阻絕緣玻璃之接觸帶電特性,北林宏佳、藤井治久,電學論A,125卷2號,179-184頁,2005年)。 關於本實施形態之顯示器用玻璃基板,玻璃基板之與半導體元件形成面相反側之玻璃表面的表面粗糙度Ra為0.3 nm以上。 藉此,玻璃基板與吸附台之功函數之差變小,而可抑制玻璃基板之剝離帶電。 表面粗糙度Ra係利用原子力顯微鏡(AFM)而測定。 表面粗糙度Ra較佳為0.7 nm以上。 但若表面粗糙度Ra過大,則有在玻璃表面產生較大之缺陷,導致玻璃基板之強度降低之虞。於表面粗糙度Ra為5 nm以下之情形時,玻璃表面不產生較大之缺陷,而無玻璃基板之強度降低之虞,故而較佳。表面粗糙度Ra更佳為2 nm以下。 關於本實施形態之顯示器用玻璃基板,較佳為藉由下述實施例中所記載之程序所測得之剝離帶電量為-10 kV以上。 藉此,防止顯示器用玻璃基板上所形成之半導體元件之靜電破壞。 剝離帶電量更佳為-7 kV以上,進而較佳為-5 kV以上。 若對藉由光電子產量能譜分析(PYS)測定所獲得之照射光能量、與光電子釋出數量之平方根進行繪圖,則於照射光能量達到某一數值之時間點,光電子釋出數量之平方根急遽增加。此時成為閾值之照射光能量為功函數。若進一步增加照射能量,則光電子釋出數量之平方根會線性增加。 本申請發明者等人經過努力研究,結果發現該線性增加之斜率、與玻璃基板之剝離帶電量之間存在關聯性。 關於本實施形態之顯示器用玻璃基板,較佳為於將藉由光電子產量能譜分析(PYS)測定所獲得之照射光能量設為X(eV),且將光電子釋出數量之平方根設為Y時,X為5.5~6.0 eV時之Y之斜率ΔY/ΔX為10以上。玻璃基板之功函數小於5.5 eV。X為5.5~6.0 eV之區域係Y線性增加之區域。 斜率ΔY/ΔX近似地表示5.5~6.0 eV時之電子之狀態密度。認為斜率ΔY/ΔX越大,玻璃基板變得越不易接收電子,越不易帶電。 本實施形態之顯示器用玻璃基板更佳為ΔY/ΔX≧20,進而較佳為ΔY/ΔX≧50。 本實施形態之顯示器用玻璃基板之尺寸並無特別限定,大型玻璃基板由於會抑制玻璃基板之剝離帶電,故而適宜。具體而言,較佳為2500 mm×2200 mm以上,更佳為3130 mm×2880 mm以上。 板厚亦無特別限定,薄板之玻璃基板由於會抑制玻璃基板之剝離帶電,故而適宜。具體而言,較佳為1.0 mm以下,更佳為0.75 mm以下,進而較佳為0.45 mm以下。 本實施形態之顯示器用玻璃基板較佳為無鹼玻璃。無鹼玻璃較佳為以下述氧化物基準之質量百分率表示而含有50~73%之SiO2 、10.5~24%之Al2 O3 、0.1~12%之B2 O3 、0~8%之MgO、0~14.5%之CaO、0~24%之SrO、0~13.5%之BaO、0~5%之ZrO2 ,且MgO、CaO、SrO及BaO之合計量(MgO+CaO+SrO+BaO)為8~29.5%。 又,無鹼玻璃較佳為以下述氧化物基準之質量百分率表示而含有58~66%之SiO2 、15~22%之Al2 O3 、5~12%之B2 O3 、0~8%之MgO、0~9%之CaO、3~12.5%之SrO、0~2%之BaO,且MgO、CaO、SrO及BaO之合計量(MgO+CaO+SrO+BaO)為9~18%。 又,無鹼玻璃較佳為以下述氧化物基準之質量百分率表示而含有54~73%之SiO2 、10.5~22.5%之Al2 O3 、0.1~5.5%之B2 O3 、0~8%之MgO、0~9%之CaO、0~16%之SrO、0~2.5%之BaO,且MgO、CaO、SrO及BaO之合計量(MgO+CaO+SrO+BaO)為8~26%。 [顯示器用玻璃基板之製造方法] 其次,對本發明之顯示器用玻璃基板之製造方法之構成例進行說明。 圖1係本發明之實施形態之顯示器用玻璃基板之製造方法的說明圖,且係表示熱處理裝置之一構成例的模式圖。 於圖1中所示之熱處理裝置60中,板玻璃20被沿著箭頭方向搬送。搬送機構並無特別限定,例如為未圖示之搬送輥。又,熱處理裝置60及下述熱處理裝置62具備未圖示之加熱器。 此處,板玻璃20之下表面22為顯示器用玻璃基板中之半導體元件形成面,板玻璃20之上表面24為半導體元件形成面之相反側之玻璃表面,如上所述,於形成半導體元件時藉由真空吸附而固定於吸附台上。 圖1中所示之熱處理裝置60具有噴注器70。自噴注器70之供給口71吹送至板玻璃20之上表面24之氣體在相對於板玻璃20之移動方向為正方向或反方向之流路74中移動,並向排氣口75流出。 圖1中所示之噴注器70係氣體之自供給口71向排氣口75之流向被均等地分成相對於板玻璃20之移動方向為正方向與反方向的雙流向型噴注器。 圖2係表示熱處理裝置之另一構成例的模式圖。圖2中所示之熱處理裝置62具有噴注器80。噴注器80為單流向型噴注器。所謂單流向型噴注器係指氣體之自供給口81向排氣口85之流向被固定為相對於板玻璃20之移動方向為正方向或反方向之任一者的噴注器。圖2中所示之噴注器80係氣體之自供給口81向排氣口85之流向84相對於板玻璃20之移動方向為正方向。但並不限於此,氣體之自供給口81向排氣口85之流向亦可相對於板玻璃20之移動方向為反方向。 於本發明之顯示器用玻璃基板之製造方法中,自噴注器70、80之供給口71、81對板玻璃20之上表面24供給含有氟化氫(HF)之氣體。 藉此,半導體元件形成面之相反側之玻璃表面附近之氟濃度與玻璃基板內部之氟濃度相比變高,玻璃基板與吸附台之功函數之差變小,而可抑制玻璃基板之剝離帶電。 於本發明之顯示器用玻璃基板之製造方法中,將供給含有HF之氣體時之玻璃表面溫度、即板玻璃20之上表面24之溫度設為500~900℃。藉由將玻璃表面溫度設為500℃以上,將發揮以下效果。 氟侵入玻璃表面附近,玻璃表面附近之氟濃度與玻璃基板內部之氟濃度相比變高。玻璃表面溫度更佳為550℃以上,進而較佳為600℃以上。 又,藉由將玻璃表面溫度設為900℃以下,將發揮以下效果。 抑制玻璃表面之表面粗糙度Ra變得過大,形成均勻之表面形狀。 玻璃表面溫度更佳為850℃以下,進而較佳為800℃以下。 於本發明之顯示器用玻璃基板之製造方法中,含有HF之氣體就防止熱處理裝置60、62之噴注器70、80等設備之腐蝕之觀點而言使用氮氣(N2 )或稀有氣體等惰性氣體作為載氣,並以與該等載氣之混合氣體之形式供給至板玻璃20之上表面24。 將自噴注器70、80之供給口71、81供給之含有HF之氣體的HF濃度設為0.5~30 vol%。藉由將HF濃度設為0.5 vol%以上,將發揮以下效果。 氟侵入玻璃表面附近,玻璃表面附近之氟濃度與玻璃基板內部之氟濃度相比變高。 HF濃度更佳為2 vol%以上,進而較佳為4 vol%以上。 又,藉由將HF濃度設為30 vol%以下,將發揮以下效果。 可抑制因玻璃表面與HF之反應而於玻璃表面產生缺陷之情況,而抑制玻璃基板之強度降低。HF濃度更佳為26 vol%以下,進而較佳為22 vol%以下。 噴注器70、80之供給口71、81與板玻璃20之上表面24的距離D較佳為5~50 mm。距離D更佳為8 mm以上。又,距離D更佳為30 mm以下,進而較佳為20 mm以下。藉由將距離D設為5 mm以上,即便因例如地震等導致板玻璃20振動,亦可避免板玻璃20之上表面24與噴注器70、80之接觸。另一方面,藉由將距離D設為50 mm以下,可抑制氣體於裝置內部擴散,而使對於所需氣體量而言充分量之氣體到達板玻璃20之上表面24。 噴注器70、80之板玻璃20之移動方向之距離L較佳為100~500 mm。距離L更佳為150 mm以上,進而較佳為200 mm以上。又,距離L更佳為450 mm以下,進而較佳為400 mm以下。藉由將距離L設為100 mm以上,可設置供給口71、81與排氣口75、85。尤佳為噴注器70之距離L為150 mm以上,噴注器80之距離L為100 mm以上。另一方面,藉由將距離L設為500 mm以下,可抑制因噴注器70、80引起之板玻璃20之脫熱量,故而可抑制複數個加熱器之輸出。 噴注器70、80之板玻璃20之寬度方向之距離較佳為具有板玻璃20之該方向之製品區域以上之距離。於線上實施本發明之顯示器用玻璃基板之製造方法之情形時,該距離較佳為3000 mm以上,更佳為4000 mm以上。 又,含有HF之氣體之流速(線速度)較佳為20~300 cm/s。藉由將流速(線速度)設為20 cm/s以上,含有HF之氣體之氣流穩定,而可均勻地處理玻璃表面。流速(線速度)更佳為50 cm/s以上,進而較佳為80 cm/s以上。 又,如下所述於線上實施本發明之顯示器用玻璃基板之製造方法之情形時,藉由將流速(線速度)設為300 cm/s以下,而可於已抑制氣體在緩冷裝置內部之擴散之狀態下使充分量之氣體到達玻璃帶之頂面。流速(線速度)更佳為250 cm/s以下,進而較佳為200 cm/s以下。 本發明之顯示器用玻璃基板之製造方法可於線上實施,亦可於線下實施。本說明書中所謂「線上處理」係指在對藉由浮式法或下拉法等所成形之玻璃帶進行緩冷之緩冷過程中應用本發明之方法之情形。另一方面,所謂「線下處理」係指對經成形並切斷為所需大小之板玻璃應用本發明之方法之情形。因此,本說明書中之板玻璃除包括經成形並切割為所需大小之板玻璃以外,亦包括藉由浮式法或下拉法等所成形之玻璃帶。 本發明之顯示器用玻璃基板之製造方法基於以下原因較佳為於線上實施。 若為線下處理,則需要增加步驟,相對於此,若為線上處理,則無需增加步驟,故而可以低成本進行處理。又,若為線下處理,則含有HF之氣體會於玻璃基板間旋繞至玻璃基板之半導體元件形成面,相對於此,若為玻璃帶之線上處理,則可抑制含有HF之氣體之旋繞。 如顯示器用玻璃基板之板玻璃之製造程序具有如下步驟:熔解步驟,其係將玻璃原料進行熔解而製成熔融玻璃;成形步驟,其係將上述熔解步驟中所獲得之熔融玻璃成形為帶狀而製成玻璃帶;及緩冷步驟,其係對上述成形步驟中所獲得之玻璃帶進行緩冷。作為上述成形步驟,可列舉藉由浮式法所進行之浮式法成形步驟、藉由下拉法所進行之下拉成形步驟。 於線上實施本發明之顯示器用玻璃基板之製造方法之情形時,於上述緩冷步驟中,對玻璃帶之頂面供給含有HF之氣體。 圖3係本發明之實施形態之顯示器用玻璃基板之製造方法的說明圖,且係表示浮式法玻璃製造裝置之概略的剖視圖。 圖3中所示之浮式法玻璃製造裝置100具備:熔解裝置200,其將玻璃原料10進行熔解而製成熔融玻璃12;成形裝置300,其將自熔解裝置200供給之熔融玻璃12成形為帶狀而製成玻璃帶14;及緩冷裝置400,其對在成形裝置300中所成形之玻璃帶14進行緩冷。 熔解裝置200具備:熔解槽210,其收容熔融玻璃12;及燃燒器220,其於收容至熔解槽210內之熔融玻璃12之上方形成火焰。投入至熔解槽210內之玻璃原料10藉由來自燃燒器220所形成之火焰之輻射熱而緩慢地熔化為熔融玻璃12。熔融玻璃12自熔解槽210被連續地供給至成形裝置300。 成形裝置300具備收容熔融錫310之浴槽320。成形裝置300係藉由使連續地供給至熔融錫310上之熔融玻璃12在熔融錫310上沿著特定方向流動而成形為帶狀,從而製成玻璃帶14。成形裝置300內之環境溫度自成形裝置300之入口朝向出口逐漸成為低溫。成形裝置300內之環境溫度係利用設置於成形裝置300內之加熱器(未圖示)等進行調整。玻璃帶14一面於特定方向流動一面被冷卻,於浴槽320之下游區域被自熔融錫310提拉起。自熔融錫310提拉起之玻璃帶14藉由提昇輥510被搬送至緩冷裝置400。 緩冷裝置400對在成形裝置300中所成形之玻璃帶14進行緩冷。緩冷裝置400例如包含:隔熱構造之緩冷爐(Lehr)410;及複數個搬送輥420,該等配設於緩冷爐410內,且於特定方向搬送玻璃帶14。緩冷爐410內之環境溫度自緩冷爐410之入口朝向出口逐漸成為低溫。緩冷爐410內之環境溫度係利用設置於緩冷爐410內之加熱器440等進行調整。自緩冷爐410之出口搬出之玻璃帶14係利用切割機切割為特定尺寸,而作為製品出貨。 於作為製品出貨之前,亦可視需要對玻璃基板之兩表面之至少一面進行研磨,並清洗玻璃基板。再者,於線上實施本發明之顯示器用玻璃基板之製造方法之情形時,玻璃基板之與半導體元件形成面相反側之玻璃表面對應於玻璃帶14之頂面,半導體元件形成面對應於玻璃帶14之底面。 於本發明之顯示器用玻璃基板之製造方法中,藉由使半導體元件形成面之相反側之玻璃表面附近之氟濃度變得高於玻璃基板內部之氟濃度,使玻璃基板、與吸附台之功函數之差變小,而抑制玻璃基板之剝離帶電,故而於實施研磨之情形時,較佳為僅對玻璃帶14之底面進行研磨。對於玻璃基板之半導體元件形成面,一面供給氧化鈰水溶液一面利用研磨具進行研磨。於研磨時,氧化鈰水溶液之一部分旋繞至玻璃基板之與半導體元件形成面相反側之玻璃表面,而成為漿料殘渣。 玻璃基板之清洗係例如藉由淋浴清洗、使用圓盤刷之漿料清洗、漂洗而進行。漿料清洗係藉由在玻璃基板之與半導體元件形成面相反側之玻璃表面一面供給漿料(例如氧化鈰水溶液、碳酸鈣水溶液)一面利用圓盤刷進行研磨,而去除殘留於與半導體元件形成面相反側之玻璃表面之漿料殘渣。 圖3中所示之浮式法玻璃製造裝置100由於在線上實施本發明之顯示器用玻璃基板之製造方法,故而於緩冷裝置400內之玻璃帶14之上方設置噴注器70、80,使用該噴注器70、80對玻璃帶14之頂面供給含有氟化氫(HF)之氣體。再者,圖1、2中所示之熱處理裝置60、62於線上實施本發明之顯示器用玻璃基板之製造方法之情形時,對應於圖3中所示之緩冷裝置400。 又,於圖3中,噴注器70、80係設置於緩冷裝置400內,但關於本發明之另一實施形態之浮式法玻璃製造裝置,若供給含有HF之氣體時之玻璃表面溫度為500~900℃,則亦可將噴注器設置於成形裝置300內。 [實施例] 以下,對本發明之實施例及比較例進行具體說明。再者,本發明並不限於該等記載。 (實驗例1) 於實驗例1中,於線下實施本發明之顯示器用玻璃基板之製造方法。 於實驗例1中,準備如下無鹼玻璃板(520 mm×410 mm×厚度0.5 mm),其含有SiO2 :59.5%、Al2 O3 :17%、B2 O3 :8%、MgO:3.3%、CaO:4%、SrO:7.6%、BaO:0.1%、ZrO2 :0.1%,且為MgO+CaO+SrO+BaO:15%,剩餘量為不可避免雜質,鹼金屬氧化物之含量之合計量為0.1%以下。自圖1中所示之熱處理裝置之噴注器70對無鹼玻璃板之上表面供給含有HF之氣體。圖4係表示實驗例1中之噴注器之狹縫寬度(a)、處理長度(b)、處理寬度(c)之關係的圖。 於實驗例1中,上述a(mm)、b(mm)、c(mm)、及含有HF之氣體之流量(L/min)、處理時間(sec)、線速度(mm/sec)係設為下述表1中所示之條件。 又,噴注器70之供給口71與板玻璃20之上表面的距離D係設定為10 mm。 又,供給含有HF之氣體時之玻璃表面溫度(表2中記為溫度)、HF濃度(vol%)係設為下述表2中所示之條件。於表2中,例1、2為比較例,例3、4為實施例。 於供給含有HF之氣體後,將玻璃表面溫度以相同溫度保持5 min後,以30 min冷卻至常溫。 其後,實施以下所示之評價。 [玻璃基板之表面附近與內部之F濃度(F0-10 nm 、F100-400 nm )] 根據以下程序測定F0-10 nm 及F100-400 nm 。 將藉由上述程序所獲得之玻璃基板切割為寬度10 mm×長度10 mm,利用X射線光電子光譜裝置(ULVAC-PHI公司製造,ESCA5500)測定自玻璃基板之玻璃表面起深度0、2、5、7、10 nm之F濃度(mol%)。將深度0、2、5、7、10 nm之F濃度之測定值進行平均化,而算出深度0~10 nm之F濃度之平均值F0-10 nm 。自玻璃基板表面起至深度10 nm為止之研削係利用C60 離子束進行濺鍍蝕刻。 又,利用X射線光電子光譜裝置(ULVAC-PHI公司製造,ESCA5500)測定自玻璃基板之玻璃表面起深度100、101、112、123、134、145、156、167、178、189、200、211、222、266、310、354、398、400 nm之F濃度(mol%)。將深度100~400 nm之F濃度之測定值進行平均化,而算出深度100~400 nm之F濃度之平均值F100-400 nm 。 將例4中之自玻璃板之表面起之深度與玻璃板中之氟濃度的關係示於圖5。 [玻璃表面之平均表面粗糙度Ra] 將藉由上述程序所獲得之玻璃基板切割為寬度5 mm×長度5 mm,藉由以下方法測定玻璃基板之玻璃表面之平均表面粗糙度Ra(算術平均表面粗糙度Ra(JIS B0601-2013))。使用原子力顯微鏡(製品名:SPI-3800N,Seiko Instruments公司製造)觀察玻璃基板之玻璃表面。懸臂係使用SI-DF40P2。觀察係使用動態力模式以掃描速率1 Hz對掃描區域5 μm×5 μm進行(區域內資料數量:256×256)。基於該觀察,算出各測定點之平均表面粗糙度Ra。計算軟體係使用原子力顯微鏡所附帶之軟體(軟體名:SPA-400)。 [玻璃基板之剝離帶電量] 藉由以下方法測定藉由上述程序所獲得之玻璃基板之剝離帶電量。使寬度410 mm×長度520 mm×厚度0.5 mm之玻璃基板接觸SUS304製之真空吸附台後,重複玻璃基板之吸附與解除110個循環。其後,使用頂起銷自真空吸附台將玻璃基板剝離。利用表面電位計(製品名:MODEL 341B,TREK JAPAN公司製造)測定玻璃基板離開真空吸附台而上升5 cm為止之表面電位之變化。將測定結果之峰值設為剝離帶電量。 [PYS測定(ΔY/ΔX)] 關於例4,藉由下述程序實施光電子產量能譜分析(PYS)測定,而求出照射光能量X、與光電子釋出數量之平方根Y的斜率(ΔY/ΔX)。 準備寬度20 mm×長度20 mm×厚度0.5 mm之玻璃基板。紫外線之照射面係設為玻璃基板之與半導體元件形成面相反側之玻璃表面。照射面之光電子釋出數量係使用大氣中光電子光譜測定裝置AC-5(理研計器公司製造)而測定。照射紫外線強度係設為2000 nW。紫外線係於照射光能量X為4.2~6.2 eV之範圍內以0.1 eV為單位進行照射。光電子之計數時間設定為每0.1 eV為5秒。 將表示例4中之照射光能量X、與光電子釋出數量之平方根Y的關係之圖表示於圖6(a)。圖6(b)係照射光能量X為5.5~6.0 eV時之圖6(a)之放大圖。斜率ΔY/ΔX係將X為5.5~6.0 eV時之描點圖藉由最小平方法進行線性近似而算出。 (實驗例2) 於實驗例2中,於線上實施本發明之顯示器用玻璃基板之製造方法。 於實驗例2中,使用圖3中所示之浮式法玻璃製造裝置100製造厚度0.5 mm之如下無鹼玻璃板,其含有SiO2 :59.5%、Al2 O3 :17%、B2 O3 :8%、MgO:3.3%、CaO:4%、SrO:7.6%、BaO:0.1%、ZrO2 :0.1%,且為MgO+CaO+SrO+BaO:15%,剩餘量為不可避免雜質,鹼金屬氧化物之含量之合計量為0.1%以下。 於使用熔解裝置200將玻璃原料10進行熔解而製成熔融玻璃12後,將熔融玻璃12供給至成形裝置300,將熔融玻璃12成形為帶狀而獲得玻璃帶14。自成形裝置300之出口抽出玻璃帶14後,於緩冷裝置400內進行緩冷。 於緩冷裝置400內之玻璃帶14之溫度為500℃之位置,設置玻璃帶14之移動方向之距離L為300 mm之噴注器70。 圖4係表示實驗例2中之噴注器之狹縫寬度(a)、處理長度(b)、處理寬度(c)之關係的圖。 於實驗例2中,上述a(mm)、b(mm)、c(mm)、及含有HF之氣體之流量(L/min)、處理時間(sec)、線速度(mm/sec)係設為下述表1中所示之條件。 又,噴注器70之供給口71與板玻璃20之上表面的距離D係設定為10 mm。 又,供給含有HF之氣體時之玻璃表面溫度(表3中記為溫度)、HF濃度(vol%)係設為下述表3中所示之條件。於表3中,例11為比較例,例12、13為實施例。 將所獲得之玻璃板藉由與實驗例1相同之程序進行評價。將例11中之玻璃板之自表面起之深度與玻璃板中之氟濃度的關係示於圖5。 將表示例11、13中之照射光能量X與光電子釋出數量之平方根Y的關係之圖表示於圖6(a)、圖6(b)。 [表1] [表2] [表3] 於F0-10 nm /F100-400 nm <3或Ra未達0.3 nm之例1、2、例11中,剝離帶電量未達-10 kV。相對於此,於F0-10 nm /F100-400 nm ≧3且Ra為0.3 nm以上之例3、4、例12、13中,剝離帶電量得到抑制而為-10 kV以上。又,於例11中,ΔY/ΔX<10,相對於此,於例4、例12、13中,ΔY/ΔX≧10。 以上,參照特定之實施態樣詳細地說明了本發明,但從業者明瞭可在不脫離本發明之精神與範圍之情況下施加各種變更或修正。 本申請係基於2017年2月21日提出申請之日本專利申請2017-029636者,並將其內容作為參照而併入本文中。[Glass substrate for display] Hereinafter, a glass substrate for a display according to an embodiment of the present invention will be described. As for the glass substrate for a display of this embodiment, the glass composition is not particularly limited, and may be a wide range of glass compositions such as soda lime silicate glass, aluminosilicate glass, borosilicate glass, and alkali-free glass. Generally speaking, with regard to contact charging, it is easy to occur if the difference in work function between substances is large. The so-called work function refers to the minimum amount of energy required to take out the electrons inside the solid to the outside, which is exactly the amount of energy required to take out into the vacuum. Charges are generated by the migration of a substance with a smaller electron self-work function to a larger substance. The glass substrate is charged due to the difference in work function between the glass substrate and the adsorption table. Therefore, in order to reduce the charge amount of the glass substrate, the inventors of the present application paid attention to the work function of the glass substrate. However, a method for measuring the work function of a glass substrate has not been established. Through intensive research, the inventors of the present application found that the difference between the fluorine atom concentration near and inside the glass substrate is related to the difference between the work functions of the glass substrate and the adsorption table. That is, by increasing the concentration of fluorine atoms having a high anion conductivity near the surface of the glass substrate, the energy level changes, and the work function of the glass substrate is changed. It is generally believed that the charge of a glass substrate depends on the difference between the work function of the glass substrate and the adsorption table (contact charging characteristics of high-resistance insulating glass, Hiroshi Kitabayashi, Zhiji Fujii, Electricity Theory A, Vol. 2, No. 2, 179-184, 2005 This difference is narrowed by allowing fluorine atoms to penetrate into the vicinity of the surface of the glass substrate. Regarding the glass substrate for a display of this embodiment, the average value of the fluorine concentration (mol%) at a depth of 0 to 10 nm from the glass surface of the glass substrate on the side opposite to the semiconductor element formation surface is set to F 0-10 nm , When the average value of the fluorine concentration (mol%) at a depth of 100 to 400 nm from the glass surface is set to F 100-400 nm , F 0-10 nm / F 100-400 nm ≧ 3. Thereby, the difference between the work function of the glass substrate and the adsorption stage becomes small, and peeling and charging of the glass substrate can be suppressed. Here, the reason why the fluorine concentration near the surface of the glass substrate is set to the above-mentioned F 0-10 nm , and the fluorine concentration inside the glass substrate is set to the above-mentioned F 100-400 nm is as follows. The contact-charged electron migration mainly occurs in a region with a depth of 0 to 10 nm from the surface of the glass substrate, and is controlled by the interaction between this region and a region with a depth of 100 to 400 nm. The F 0-10 nm and F 100-400 nm are measured by X-ray photoelectron spectroscopy (XPS). The glass substrate for a display of this embodiment is preferably F 0-10 nm / F 100-400 nm ≧ 5, and more preferably F 0-10 nm / F 100-400 nm ≧ 10. If the difference in fluorine atom concentration between the vicinity of the surface of the glass substrate and the inside of the glass substrate is too large, the haze will be deteriorated, which is unfavorable. F 0-10 nm / F 100-400 nm ≦ 150 can suppress the deterioration of haze, so it is better, more preferably F 0-10 nm / F 100-400 nm ≦ 100. In addition, the greater the surface roughness of the glass surface, the smaller the contact area between the glass substrate and the adsorption stage, and the less likely it is to cause the migration of electrons, so the peeling and charging of the glass substrate can be suppressed (contact charging characteristics of high-resistance insulating glass, Beilin Hongjia, Zhikui Fujii, Electrics A, Vol. 125, No. 2, 179-184, 2005). Regarding the glass substrate for a display of this embodiment, the surface roughness Ra of the glass surface of the glass substrate on the side opposite to the semiconductor element formation surface is 0.3 nm or more. Thereby, the difference between the work function of the glass substrate and the adsorption stage becomes small, and peeling and charging of the glass substrate can be suppressed. The surface roughness Ra is measured using an atomic force microscope (AFM). The surface roughness Ra is preferably 0.7 nm or more. However, if the surface roughness Ra is too large, a large defect may be generated on the glass surface, which may cause a reduction in the strength of the glass substrate. In the case where the surface roughness Ra is 5 nm or less, no large defects are generated on the glass surface, and there is no risk of reducing the strength of the glass substrate, so it is preferable. The surface roughness Ra is more preferably 2 nm or less. As for the glass substrate for a display of this embodiment, it is preferable that the peeling charge amount measured by the procedure described in the following examples is -10 kV or more. This prevents electrostatic damage to the semiconductor element formed on the glass substrate for a display. The peeling charge amount is more preferably -7 kV or more, and even more preferably -5 kV or more. If the irradiation light energy obtained by the photoelectron yield spectroscopy (PYS) measurement and the square root of the photoelectron emission quantity are plotted, the square root of the photoelectron emission quantity at the time point when the irradiation light energy reaches a certain value is urgent. increase. The energy of the irradiated light which becomes the threshold at this time is a work function. If the irradiation energy is further increased, the square root of the number of photoelectron emission will increase linearly. Through intensive research, the inventors of the present application found that there is a correlation between the slope of the linear increase and the peeling charge of the glass substrate. Regarding the glass substrate for a display of this embodiment, it is preferable that the irradiation light energy obtained by the photoelectron yield spectrum analysis (PYS) measurement is set to X (eV), and the square root of the number of photoelectron emission is set to Y At this time, the slope ΔY / ΔX of Y when X is 5.5 to 6.0 eV is 10 or more. The work function of the glass substrate is less than 5.5 eV. A region where X is 5.5 to 6.0 eV is a region where Y linearly increases. The slope ΔY / ΔX approximately represents the state density of the electrons at 5.5 to 6.0 eV. It is considered that the larger the slope ΔY / ΔX, the more difficult it becomes for the glass substrate to receive electrons, and the less likely it is to be charged. The glass substrate for a display of this embodiment is more preferably ΔY / ΔX ≧ 20, and more preferably ΔY / ΔX ≧ 50. The size of the glass substrate for a display of this embodiment is not particularly limited, and large glass substrates are suitable because they suppress the peeling and charging of the glass substrate. Specifically, it is preferably 2500 mm × 2200 mm or more, and more preferably 3130 mm × 2880 mm or more. The thickness of the plate is also not particularly limited, and a thin glass substrate is suitable because it can suppress the peeling and charging of the glass substrate. Specifically, it is preferably 1.0 mm or less, more preferably 0.75 mm or less, and still more preferably 0.45 mm or less. The glass substrate for a display of this embodiment is preferably an alkali-free glass. The alkali-free glass is preferably expressed in terms of mass percentages based on the following oxides and contains 50 to 73% of SiO 2 , 10.5 to 24% of Al 2 O 3 , 0.1 to 12% of B 2 O 3 , and 0 to 8%. MgO, 0 to 14.5% CaO, 0 to 24% SrO, 0 to 13.5% BaO, 0 to 5% ZrO 2 , and the total amount of MgO, CaO, SrO, and BaO (MgO + CaO + SrO + BaO) is 8 to 29.5% . The alkali-free glass is preferably expressed in terms of mass percentages based on the following oxides and contains 58 to 66% of SiO 2 , 15 to 22% of Al 2 O 3 , and 5 to 12% of B 2 O 3 , 0 to 8 % Of MgO, 0 to 9% of CaO, 3 to 12.5% of SrO, 0 to 2% of BaO, and the total amount of MgO, CaO, SrO, and BaO (MgO + CaO + SrO + BaO) is 9 to 18%. The alkali-free glass is preferably expressed in terms of mass percentages of the following oxide standards and contains 54 to 73% of SiO 2 , 10.5 to 22.5% of Al 2 O 3 , 0.1 to 5.5% of B 2 O 3 , and 0 to 8 % MgO, 0-9% CaO, 0-16% SrO, 0-2.5% BaO, and the total amount of MgO, CaO, SrO, and BaO (MgO + CaO + SrO + BaO) is 8-26%. [Manufacturing method of glass substrate for display] Next, a configuration example of a manufacturing method of the glass substrate for display of the present invention will be described. FIG. 1 is an explanatory diagram of a method for manufacturing a glass substrate for a display according to an embodiment of the present invention, and is a schematic diagram showing a configuration example of a heat treatment apparatus. In the heat treatment apparatus 60 shown in FIG. 1, the plate glass 20 is carried in the direction of the arrow. The transport mechanism is not particularly limited, and it is, for example, a transport roller (not shown). The heat treatment apparatus 60 and the heat treatment apparatus 62 described below include heaters (not shown). Here, the lower surface 22 of the plate glass 20 is a semiconductor element formation surface in a glass substrate for a display, and the upper surface 24 of the plate glass 20 is a glass surface on the opposite side of the semiconductor element formation surface. As described above, when forming a semiconductor element It is fixed on the adsorption table by vacuum adsorption. The heat treatment apparatus 60 shown in FIG. 1 has an injector 70. The gas blown from the supply port 71 of the injector 70 to the upper surface 24 of the plate glass 20 moves in the flow path 74 which is a forward direction or a reverse direction with respect to the moving direction of the plate glass 20 and flows out to the exhaust port 75. The injector 70 shown in FIG. 1 is a dual-flow type injector in which the flow direction of the gas from the supply port 71 to the exhaust port 75 is equally divided into a forward direction and a reverse direction with respect to the moving direction of the plate glass 20. FIG. 2 is a schematic diagram showing another configuration example of the heat treatment apparatus. The heat treatment apparatus 62 shown in FIG. 2 has an injector 80. The injector 80 is a single-flow type injector. The single-flow type injector refers to an injector in which the flow direction of the gas from the supply port 81 to the exhaust port 85 is fixed to be either the forward direction or the reverse direction with respect to the moving direction of the plate glass 20. The flow direction 84 of the injector 80 shown in FIG. 2 from the supply port 81 to the exhaust port 85 of the gas is positive with respect to the moving direction of the plate glass 20. However, the flow direction of the gas from the supply port 81 to the exhaust port 85 may be opposite to the moving direction of the plate glass 20. In the method for manufacturing a glass substrate for a display of the present invention, a gas containing hydrogen fluoride (HF) is supplied to the upper surface 24 of the plate glass 20 from the supply ports 71 and 81 of the injectors 70 and 80. Thereby, the fluorine concentration near the glass surface on the opposite side of the semiconductor element formation surface becomes higher than the fluorine concentration inside the glass substrate, the difference in work function between the glass substrate and the adsorption table becomes smaller, and peeling and charging of the glass substrate can be suppressed . In the method for manufacturing a glass substrate for a display of the present invention, the glass surface temperature when the gas containing HF is supplied, that is, the temperature of the upper surface 24 of the plate glass 20 is set to 500 to 900 ° C. By setting the glass surface temperature to 500 ° C or higher, the following effects are exhibited. The fluorine invades near the glass surface, and the fluorine concentration near the glass surface becomes higher than the fluorine concentration inside the glass substrate. The glass surface temperature is more preferably 550 ° C or higher, and even more preferably 600 ° C or higher. In addition, by setting the glass surface temperature to 900 ° C or lower, the following effects are exhibited. The surface roughness Ra of the glass surface is suppressed from becoming too large, and a uniform surface shape is formed. The glass surface temperature is more preferably 850 ° C or lower, and even more preferably 800 ° C or lower. In the method for manufacturing a glass substrate for a display of the present invention, an inert gas such as nitrogen (N 2 ) or a rare gas is used for the gas containing HF from the viewpoint of preventing the corrosion of the heat treatment devices 60, 62, and the injectors 70 and 80. The gas is used as a carrier gas and is supplied to the upper surface 24 of the plate glass 20 in the form of a mixed gas with the carrier gas. The HF concentration of the HF-containing gas supplied from the supply ports 71 and 81 of the injectors 70 and 80 is set to 0.5 to 30 vol%. By setting the HF concentration to 0.5 vol% or more, the following effects are exhibited. The fluorine invades near the glass surface, and the fluorine concentration near the glass surface becomes higher than the fluorine concentration inside the glass substrate. The HF concentration is more preferably 2 vol% or more, and even more preferably 4 vol% or more. In addition, by setting the HF concentration to 30 vol% or less, the following effects are exhibited. It is possible to suppress the occurrence of defects on the glass surface due to the reaction between the glass surface and HF, and to suppress the decrease in the strength of the glass substrate. The HF concentration is more preferably 26 vol% or less, and still more preferably 22 vol% or less. The distance D between the supply ports 71 and 81 of the injectors 70 and 80 and the upper surface 24 of the plate glass 20 is preferably 5 to 50 mm. The distance D is more preferably 8 mm or more. The distance D is more preferably 30 mm or less, and further preferably 20 mm or less. By setting the distance D to 5 mm or more, even if the plate glass 20 is vibrated due to, for example, an earthquake, contact between the upper surface 24 of the plate glass 20 and the injectors 70 and 80 can be avoided. On the other hand, by setting the distance D to 50 mm or less, it is possible to suppress the gas from diffusing inside the device, and allow a sufficient amount of gas to reach the upper surface 24 of the plate glass 20 for the required amount of gas. The distance L in the moving direction of the plate glass 20 of the injectors 70 and 80 is preferably 100 to 500 mm. The distance L is more preferably 150 mm or more, and further preferably 200 mm or more. The distance L is more preferably 450 mm or less, and further preferably 400 mm or less. By setting the distance L to 100 mm or more, the supply ports 71 and 81 and the exhaust ports 75 and 85 can be provided. Particularly preferably, the distance L of the injector 70 is 150 mm or more, and the distance L of the injector 80 is 100 mm or more. On the other hand, by setting the distance L to 500 mm or less, the heat loss of the plate glass 20 caused by the injectors 70 and 80 can be suppressed, and the output of a plurality of heaters can be suppressed. The distance in the width direction of the plate glass 20 of the injectors 70 and 80 is preferably the distance above the product area having the plate glass 20 in that direction. When the manufacturing method of the glass substrate for a display of the present invention is implemented online, the distance is preferably 3000 mm or more, and more preferably 4000 mm or more. The flow velocity (linear velocity) of the HF-containing gas is preferably 20 to 300 cm / s. By setting the flow velocity (linear velocity) to 20 cm / s or more, the gas flow of the gas containing HF is stable, and the glass surface can be treated uniformly. The flow velocity (linear velocity) is more preferably 50 cm / s or more, and still more preferably 80 cm / s or more. When the method for manufacturing a glass substrate for a display of the present invention is implemented on-line as described below, by setting the flow velocity (linear velocity) to 300 cm / s or less, it is possible to suppress the presence of gas in the slow cooling device. In a diffused state, a sufficient amount of gas reaches the top surface of the glass ribbon. The flow velocity (linear velocity) is more preferably 250 cm / s or less, and still more preferably 200 cm / s or less. The manufacturing method of the glass substrate for a display of the present invention can be implemented on-line or off-line. The "on-line processing" in this specification refers to a case where the method of the present invention is applied in a slow cooling process of slow cooling a glass ribbon formed by a float method or a down-draw method. On the other hand, the "off-line treatment" refers to a case where the method of the present invention is applied to a sheet glass that is formed and cut to a desired size. Therefore, the sheet glass in this specification includes not only sheet glass that is formed and cut to a desired size, but also glass ribbons formed by a float method or a down-draw method. The method for manufacturing a glass substrate for a display of the present invention is preferably implemented on-line for the following reasons. In the case of offline processing, additional steps are required, while in the case of online processing, no additional steps are required, so processing can be performed at low cost. In addition, in the case of off-line processing, a gas containing HF is wound between the glass substrates to the semiconductor element formation surface of the glass substrate. In contrast, in the case of on-line processing of a glass ribbon, the swirling of the gas containing HF can be suppressed. For example, the manufacturing process of plate glass for display glass substrates has the following steps: a melting step, which fuses glass raw materials to make molten glass; a forming step, which shapes the molten glass obtained in the above melting step into a ribbon shape A glass ribbon is made; and a slow cooling step, which is a slow cooling of the glass ribbon obtained in the above-mentioned forming step. Examples of the forming step include a float forming step performed by a float method and a down forming step performed by a down method. When the manufacturing method of the glass substrate for a display of this invention is implemented online, in the said slow cooling process, the top surface of a glass ribbon is supplied with the gas containing HF. FIG. 3 is an explanatory view of a method for manufacturing a glass substrate for a display according to an embodiment of the present invention, and is a schematic cross-sectional view showing a float glass manufacturing apparatus. The float glass manufacturing apparatus 100 shown in FIG. 3 includes a melting device 200 that melts glass raw material 10 to produce molten glass 12 and a molding device 300 that shapes molten glass 12 supplied from the melting device 200 into The ribbon is formed into a glass ribbon 14; and a slow cooling device 400 for slow cooling the glass ribbon 14 formed in the molding device 300. The melting device 200 includes a melting tank 210 that contains the molten glass 12 and a burner 220 that forms a flame above the molten glass 12 that is contained in the melting tank 210. The glass raw material 10 put into the melting tank 210 is slowly melted into the molten glass 12 by the radiant heat from the flame formed by the burner 220. The molten glass 12 is continuously supplied from the melting tank 210 to the forming apparatus 300. The molding apparatus 300 includes a bath 320 that accommodates molten tin 310. The molding apparatus 300 forms the glass ribbon 14 by flowing the molten glass 12 continuously supplied onto the molten tin 310 into a band shape by flowing on the molten tin 310 in a specific direction. The ambient temperature in the forming apparatus 300 becomes gradually lower from the inlet to the outlet of the forming apparatus 300. The ambient temperature in the molding apparatus 300 is adjusted by a heater (not shown) or the like provided in the molding apparatus 300. The glass ribbon 14 is cooled while flowing in a specific direction, and is pulled up from the molten tin 310 in a region downstream of the bath 320. The glass ribbon 14 pulled up from the molten tin 310 is transferred to the slow cooling device 400 by a lift roller 510. The slow cooling device 400 slow-cools the glass ribbon 14 formed in the forming device 300. The slow cooling device 400 includes, for example, a slow cooling furnace (Lehr) 410 with a heat insulation structure, and a plurality of conveying rollers 420, which are arranged in the slow cooling furnace 410 and convey the glass ribbon 14 in a specific direction. The ambient temperature in the slow cooling furnace 410 gradually decreases from the inlet to the outlet of the slow cooling furnace 410. The ambient temperature in the slow cooling furnace 410 is adjusted using a heater 440 or the like provided in the slow cooling furnace 410. The glass ribbon 14 carried out from the exit of the slow cooling furnace 410 is cut to a specific size by a cutter and shipped as a product. Before shipment as a product, at least one of the two surfaces of the glass substrate may be polished and the glass substrate may be cleaned as necessary. Furthermore, when the manufacturing method of the glass substrate for a display of the present invention is implemented online, the glass surface of the glass substrate opposite to the semiconductor element formation surface corresponds to the top surface of the glass ribbon 14, and the semiconductor element formation surface corresponds to the glass ribbon. Underside of 14. In the method for manufacturing a glass substrate for a display of the present invention, by making the fluorine concentration near the glass surface on the opposite side of the semiconductor element formation surface higher than the fluorine concentration inside the glass substrate, the function of the glass substrate and the adsorption stage is improved. The difference in the functions becomes smaller, and the peeling and charging of the glass substrate is suppressed. Therefore, when polishing is performed, it is preferable to polish only the bottom surface of the glass ribbon 14. The semiconductor element formation surface of the glass substrate was polished with a polishing tool while supplying a cerium oxide aqueous solution. During grinding, a part of the cerium oxide aqueous solution was spirally wound onto the glass surface of the glass substrate on the side opposite to the semiconductor element formation surface, and became a slurry residue. The glass substrate is cleaned, for example, by shower cleaning, slurry cleaning using a disc brush, and rinsing. Slurry cleaning is performed by supplying a slurry (e.g., cerium oxide aqueous solution, calcium carbonate aqueous solution) on the glass surface of the glass substrate on the side opposite to the surface on which the semiconductor element is formed, and grinding with a disc brush to remove residues remaining on the semiconductor element Sludge residue on the glass surface on the opposite side. Since the float glass manufacturing apparatus 100 shown in FIG. 3 implements the manufacturing method of the glass substrate for a display of the present invention on-line, injectors 70 and 80 are provided above the glass ribbon 14 in the slow cooling apparatus 400 and used. The injectors 70 and 80 supply a gas containing hydrogen fluoride (HF) to the top surface of the glass ribbon 14. In addition, when the heat treatment apparatuses 60 and 62 shown in FIGS. 1 and 2 implement the manufacturing method of the glass substrate for a display of this invention on line, it corresponds to the slow cooling apparatus 400 shown in FIG. In FIG. 3, the injectors 70 and 80 are installed in the slow cooling device 400. However, regarding the float glass manufacturing device according to another embodiment of the present invention, the glass surface temperature when a gas containing HF is supplied When the temperature is 500 to 900 ° C, the injector may be installed in the molding apparatus 300. [Examples] Examples and comparative examples of the present invention will be specifically described below. The present invention is not limited to these descriptions. (Experimental Example 1) In Experimental Example 1, the manufacturing method of the glass substrate for a display of the present invention was carried out offline. In Experimental Example 1, the following alkali-free glass plate (520 mm × 410 mm × thickness 0.5 mm) was prepared, which contained SiO 2 : 59.5%, Al 2 O 3 : 17%, B 2 O 3 : 8%, and MgO: 3.3%, CaO: 4%, SrO: 7.6%, BaO: 0.1%, ZrO 2 : 0.1%, and MgO + CaO + SrO + BaO: 15%, the remaining amount is unavoidable impurities, and the total content of alkali metal oxides is 0.1% the following. A gas containing HF is supplied from the injector 70 of the heat treatment apparatus shown in FIG. 1 to the upper surface of the alkali-free glass plate. FIG. 4 is a diagram showing the relationship between the slit width (a), the processing length (b), and the processing width (c) of the injector in Experimental Example 1. FIG. In Experimental Example 1, the a (mm), b (mm), c (mm), and the flow rate (L / min), processing time (sec), and linear velocity (mm / sec) of the gas containing HF are set. The conditions are shown in Table 1 below. The distance D between the supply port 71 of the injector 70 and the upper surface of the plate glass 20 is set to 10 mm. The glass surface temperature (referred to as the temperature in Table 2) and the HF concentration (vol%) when the gas containing HF was supplied were set to the conditions shown in Table 2 below. In Table 2, Examples 1 and 2 are comparative examples, and Examples 3 and 4 are examples. After supplying the gas containing HF, the glass surface temperature was kept at the same temperature for 5 minutes, and then cooled to normal temperature in 30 minutes. Then, the evaluation shown below was performed. [F concentration (F 0-10 nm , F 100-400 nm ) near and inside the glass substrate] The F 0-10 nm and F 100-400 nm were measured according to the following procedure. The glass substrate obtained by the above procedure was cut into a width of 10 mm × length of 10 mm, and an X-ray photoelectron spectroscopy device (manufactured by ULVAC-PHI Corporation, ESCA5500) was used to measure the depths of 0, 2, 5, and 5 from the glass surface of the glass substrate. 7. F concentration (mol%) at 10 nm. The measured values of the F concentration at the depths of 0, 2, 5, 7, and 10 nm were averaged to calculate the average value of the F concentration at the depth of 0 to 10 nm, F 0 to 10 nm . The grinding from the surface of the glass substrate to a depth of 10 nm is performed by sputtering etching using a C 60 ion beam. The X-ray photoelectron spectroscopy device (manufactured by ULVAC-PHI, ESCA5500) was used to measure the depth from the glass surface of the glass substrate to 100, 101, 112, 123, 134, 145, 156, 167, 178, 189, 200, 211, F concentration (mol%) of 222, 266, 310, 354, 398, 400 nm. The measured values of the F concentration at a depth of 100 to 400 nm are averaged, and the average value of the F concentration at a depth of 100 to 400 nm is calculated as F 100 to 400 nm . The relationship between the depth from the surface of the glass plate and the fluorine concentration in the glass plate in Example 4 is shown in FIG. 5. [Average surface roughness Ra of glass surface] The glass substrate obtained by the above procedure was cut into a width of 5 mm × length 5 mm, and the average surface roughness Ra (arithmetic average surface) of the glass surface of the glass substrate was measured by the following method. Roughness Ra (JIS B0601-2013)). The glass surface of the glass substrate was observed using an atomic force microscope (product name: SPI-3800N, manufactured by Seiko Instruments). The cantilever system uses SI-DF40P2. The observation system uses dynamic force mode to scan 5 μm × 5 μm in the scanning area at a scanning rate of 1 Hz (the number of data in the area: 256 × 256). Based on this observation, the average surface roughness Ra of each measurement point is calculated. The calculation software system uses software (software name: SPA-400) attached to the atomic force microscope. [Peeling Charge of Glass Substrate] The peeling charge of the glass substrate obtained by the above procedure was measured by the following method. After the glass substrate having a width of 410 mm × a length of 520 mm × a thickness of 0.5 mm was brought into contact with a vacuum adsorption table made of SUS304, the adsorption and release of the glass substrate was repeated for 110 cycles. Thereafter, the glass substrate was peeled from the vacuum adsorption stage using a jack pin. A surface potentiometer (product name: MODEL 341B, manufactured by TREK JAPAN) was used to measure the change in the surface potential of the glass substrate up to 5 cm from the vacuum adsorption stage. The peak value of the measurement result was set as the peeling charge amount. [PYS measurement (ΔY / ΔX)] In Example 4, the photoelectron yield spectroscopy (PYS) measurement was performed by the following procedure, and the slope (ΔY / ΔX). Prepare a glass substrate with a width of 20 mm × length of 20 mm × thickness of 0.5 mm. The ultraviolet irradiation surface is a glass surface on the glass substrate, which is opposite to the semiconductor element formation surface. The photoelectron emission amount on the irradiation surface was measured using an atmospheric photoelectron spectrometer AC-5 (manufactured by Riken Keiki Co., Ltd.). The irradiation ultraviolet intensity was set to 2000 nW. The ultraviolet rays are irradiated in units of 0.1 eV within a range of irradiation light energy X of 4.2 to 6.2 eV. The optoelectronic counting time is set to 5 seconds per 0.1 eV. A graph showing the relationship between the irradiation light energy X and the square root Y of the number of photoelectron emission in Example 4 is shown in FIG. 6 (a). FIG. 6 (b) is an enlarged view of FIG. 6 (a) when the irradiation light energy X is 5.5 to 6.0 eV. The slope ΔY / ΔX is calculated by linearly approximating the tracing plot when X is 5.5 to 6.0 eV by the least square method. (Experimental Example 2) In Experimental Example 2, the manufacturing method of the glass substrate for a display of the present invention was implemented on-line. In Experimental Example 2, a float glass glass manufacturing apparatus 100 shown in FIG. 3 was used to manufacture an alkali-free glass plate having a thickness of 0.5 mm and containing SiO 2 : 59.5%, Al 2 O 3 : 17%, and B 2 O. 3 : 8%, MgO: 3.3%, CaO: 4%, SrO: 7.6%, BaO: 0.1%, ZrO 2 : 0.1%, and MgO + CaO + SrO + BaO: 15%. The remaining amount is an inevitable impurity, which is an alkali metal oxide. The total content is 0.1% or less. After the glass raw material 10 is melted using the melting device 200 to prepare a molten glass 12, the molten glass 12 is supplied to a molding device 300, and the molten glass 12 is shaped into a ribbon shape to obtain a glass ribbon 14. After the glass ribbon 14 is withdrawn from the exit of the forming apparatus 300, it is slowly cooled in the slow cooling apparatus 400. In a position where the temperature of the glass ribbon 14 in the slow cooling device 400 is 500 ° C., an injector 70 having a distance L in the moving direction of the glass ribbon 14 of 300 mm is set. FIG. 4 is a diagram showing the relationship between the slit width (a), the processing length (b), and the processing width (c) of the injector in Experimental Example 2. FIG. In Experimental Example 2, the a (mm), b (mm), c (mm), and the flow rate (L / min), processing time (sec), and linear velocity (mm / sec) of the gas containing HF are set. The conditions are shown in Table 1 below. The distance D between the supply port 71 of the injector 70 and the upper surface of the plate glass 20 is set to 10 mm. The glass surface temperature (referred to as the temperature in Table 3) and the HF concentration (vol%) when the gas containing HF was supplied were set to the conditions shown in Table 3 below. In Table 3, Example 11 is a comparative example, and Examples 12 and 13 are examples. The obtained glass plate was evaluated by the same procedure as in Experimental Example 1. The relationship between the depth from the surface of the glass plate and the fluorine concentration in the glass plate in Example 11 is shown in FIG. 5. The graphs showing the relationship between the irradiation light energy X and the square root Y of the number of photoelectron emission in Examples 11 and 13 are shown in Figs. 6 (a) and 6 (b). [Table 1] [Table 2] [table 3] In Examples 1, 2, and 11 where F 0-10 nm / F 100-400 nm <3 or Ra less than 0.3 nm, the peeling charge did not reach -10 kV. In contrast, in Examples 3, 4, 12, and 13 in which F 0-10 nm / F 100-400 nm ≧ 3 and Ra was 0.3 nm or more, the peeling charge was suppressed to be -10 kV or more. In addition, in Example 11, ΔY / ΔX <10, whereas in Examples 4, 12 and 13, ΔY / ΔX ≧ 10. In the above, the present invention has been described in detail with reference to specific embodiments. However, it is apparent to practitioners that various changes or modifications can be made without departing from the spirit and scope of the present invention. This application is based on Japanese Patent Application No. 2017-029636 filed on February 21, 2017, and the contents are incorporated herein by reference.

10‧‧‧玻璃原料10‧‧‧Glass Raw Materials

12‧‧‧熔融玻璃12‧‧‧ molten glass

14‧‧‧玻璃帶14‧‧‧glass ribbon

20‧‧‧板玻璃20‧‧‧ plate glass

22‧‧‧下表面22‧‧‧ lower surface

24‧‧‧上表面24‧‧‧ Top surface

60、62‧‧‧熱處理裝置60, 62‧‧‧ heat treatment equipment

70、80‧‧‧噴注器70, 80‧‧‧ injector

71、81‧‧‧供給口71, 81‧‧‧ supply port

74、84‧‧‧流路74, 84‧‧‧ stream

75、85‧‧‧排氣口75, 85‧‧‧ exhaust port

100‧‧‧浮式法玻璃製造裝置100‧‧‧ float glass manufacturing equipment

200‧‧‧熔解裝置200‧‧‧ melting device

210‧‧‧熔解槽210‧‧‧ melting tank

220‧‧‧燃燒器220‧‧‧ burner

300‧‧‧成形裝置300‧‧‧forming device

310‧‧‧熔融錫310‧‧‧ Molten Tin

320‧‧‧浴槽320‧‧‧ bath

400‧‧‧緩冷裝置400‧‧‧ Slow cooling device

410‧‧‧緩冷爐410‧‧‧ Slow cooling furnace

420‧‧‧搬送輥420‧‧‧ transporting roller

440‧‧‧加熱器440‧‧‧heater

510‧‧‧提昇輥510‧‧‧Lifting roller

D‧‧‧距離D‧‧‧distance

L‧‧‧距離L‧‧‧ Distance

圖1係本發明之實施形態之顯示器用玻璃基板之製造方法的說明圖,且係表示熱處理裝置之一構成例的模式圖。 圖2係本發明之實施形態之顯示器用玻璃基板之製造方法的說明圖,且係表示熱處理裝置之另一構成例的模式圖。 圖3係本發明之實施形態之顯示器用玻璃基板之製造方法的說明圖,且係表示浮式法玻璃製造裝置之概略的剖視圖。 圖4係表示實施例中之噴注器之狹縫寬度(a)、處理長度(b)、處理寬度(c)之關係的圖。 圖5係表示實施例(例4、例11)中之玻璃板之自表面起之深度、與玻璃板中之氟濃度之關係的圖表。 圖6(a)係表示實施例中之照射光能量X、與光電子釋出數量之平方根Y之關係的圖表。圖6(b)係照射光能量X為5.5~6.0 eV時之圖6(a)之放大圖。FIG. 1 is an explanatory diagram of a method for manufacturing a glass substrate for a display according to an embodiment of the present invention, and is a schematic diagram showing a configuration example of a heat treatment apparatus. FIG. 2 is an explanatory diagram of a method for manufacturing a glass substrate for a display according to an embodiment of the present invention, and is a schematic diagram showing another configuration example of a heat treatment apparatus. 3 is an explanatory diagram of a method for manufacturing a glass substrate for a display according to an embodiment of the present invention, and is a schematic cross-sectional view showing a float glass manufacturing apparatus. FIG. 4 is a diagram showing the relationship between the slit width (a), the processing length (b), and the processing width (c) of the injector in the embodiment. Fig. 5 is a graph showing the relationship between the depth from the surface of the glass plate and the fluorine concentration in the glass plate in Examples (Examples 4 and 11). FIG. 6 (a) is a graph showing the relationship between the irradiated light energy X and the square root Y of the number of photoelectron emission in the example. FIG. 6 (b) is an enlarged view of FIG. 6 (a) when the irradiation light energy X is 5.5 to 6.0 eV.

Claims (6)

一種顯示器用玻璃基板,其特徵在於:於將自玻璃基板之與半導體元件形成面相反側之玻璃表面起深度0~10 nm之氟濃度(mol%)之平均值設為F0-10 nm ,並將自該玻璃表面起深度100~400 nm之氟濃度(mol%)之平均值設為F100-400 nm 時,F0-10 nm /F100-400 nm ≧3,且與上述半導體元件形成面相反側之玻璃表面之表面粗糙度Ra為0.3 nm以上。A glass substrate for a display, characterized in that an average value of a fluorine concentration (mol%) at a depth of 0 to 10 nm from a glass surface on a side of the glass substrate opposite to a surface on which a semiconductor element is formed is set to F 0-10 nm , When the average value of the fluorine concentration (mol%) at a depth of 100 to 400 nm from the glass surface is set to F 100-400 nm , F 0-10 nm / F 100-400 nm ≧ 3, and the same as the above semiconductor device The surface roughness Ra of the glass surface on the opposite side of the formation surface is 0.3 nm or more. 如請求項1之顯示器用玻璃基板,其剝離帶電量為-10 kV以上。For example, the glass substrate for display of claim 1 has a peeling charge of -10 kV or more. 如請求項1或2之顯示器用玻璃基板,其中於將藉由光電子產量能譜分析(PYS)測定所獲得之照射光能量設為X(eV),且將光電子釋出數量之平方根設為Y時,上述X為5.5~6.0 eV時之上述Y之斜率ΔY/ΔX為10以上。For example, the glass substrate for a display according to claim 1 or 2, wherein the irradiation light energy obtained by the photoelectron yield spectroscopy (PYS) measurement is set to X (eV), and the square root of the number of photoelectron emission is set to Y In this case, the slope ΔY / ΔX of the Y when the X is 5.5 to 6.0 eV is 10 or more. 一種顯示器用玻璃基板之製造方法,其特徵在於:具有對在熱處理裝置內被搬送之板玻璃之一表面供給含有氟化氫(HF)之氣體之程序,並且 上述板玻璃之一表面為玻璃基板之與半導體元件形成面相反側之玻璃表面, 上述含有HF之氣體之HF濃度為0.5~30 vol%, 供給上述含有HF之氣體時之玻璃表面溫度為500~900℃。A manufacturing method of a glass substrate for a display is characterized in that it has a procedure for supplying a gas containing hydrogen fluoride (HF) to one surface of a sheet glass to be transported in a heat treatment device, and one surface of the sheet glass is a glass substrate The glass surface on the opposite side of the semiconductor element formation surface has a HF concentration of the HF-containing gas of 0.5 to 30 vol%, and a glass surface temperature when the HF-containing gas is supplied is 500 to 900 ° C. 如請求項4之顯示器用玻璃基板之製造方法,其具有:熔解步驟,其係將玻璃原料進行熔解而製成熔融玻璃;成形步驟,其係將上述熔解步驟中所獲得之熔融玻璃成形為帶狀而製成玻璃帶;及緩冷步驟,其係對上述成形步驟中所獲得之玻璃帶進行緩冷;並且 於上述緩冷步驟中,對上述玻璃帶之頂面供給含有HF之氣體。The method for manufacturing a glass substrate for a display according to claim 4, comprising: a melting step of melting glass raw materials to produce molten glass; and a forming step of forming the molten glass obtained in the above melting step into a ribbon To form a glass ribbon; and a slow cooling step, which is to slowly cool the glass ribbon obtained in the forming step; and to supply a gas containing HF to the top surface of the glass ribbon in the slow cooling step. 如請求項4或5之顯示器用玻璃基板之製造方法,其中上述成形步驟為浮式法成形步驟。The method for manufacturing a glass substrate for a display according to claim 4 or 5, wherein the forming step is a floating method forming step.
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