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JP4363637B2 - Tempered glass with heterogeneous phase formed by laser irradiation and glass composition suitable for the tempering method - Google Patents

Tempered glass with heterogeneous phase formed by laser irradiation and glass composition suitable for the tempering method Download PDF

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JP4363637B2
JP4363637B2 JP2004104452A JP2004104452A JP4363637B2 JP 4363637 B2 JP4363637 B2 JP 4363637B2 JP 2004104452 A JP2004104452 A JP 2004104452A JP 2004104452 A JP2004104452 A JP 2004104452A JP 4363637 B2 JP4363637 B2 JP 4363637B2
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glass
plate glass
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mechanical strength
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JP2005289682A (en
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瑞樹 西
宏幸 多門
晋司 西川
雅貴 田原
佳則 赤松
憲太郎 堤
素雄 朝倉
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Central Glass Co Ltd
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    • 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
    • C03C3/00Glass compositions
    • C03C3/04Glass compositions containing silica
    • C03C3/076Glass compositions containing silica with 40% to 90% silica, by weight
    • C03C3/083Glass compositions containing silica with 40% to 90% silica, by weight containing aluminium oxide or an iron compound
    • C03C3/085Glass compositions containing silica with 40% to 90% silica, by weight containing aluminium oxide or an iron compound containing an oxide of a divalent metal
    • C03C3/087Glass compositions containing silica with 40% to 90% silica, by weight containing aluminium oxide or an iron compound containing an oxide of a divalent metal containing calcium oxide, e.g. common sheet or container glass
    • 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
    • C03C23/00Other surface treatment of glass not in the form of fibres or filaments

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  • Chemical & Material Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • General Chemical & Material Sciences (AREA)
  • Geochemistry & Mineralogy (AREA)
  • Materials Engineering (AREA)
  • Organic Chemistry (AREA)
  • Surface Treatment Of Glass (AREA)
  • Glass Compositions (AREA)

Description

本発明は、強化ガラス、特にレーザー照射で異質相が形成されてなる強化ガラスに関する。   The present invention relates to a tempered glass, particularly a tempered glass in which a heterogeneous phase is formed by laser irradiation.

板ガラスの機械的強度を大きくする強化ガラスの製造方法として、風冷強化法、化学強化法等が実施されており、当該方法で得られた強化ガラスは、各種製品でガラス部材として使用されている。   As a method for producing tempered glass for increasing the mechanical strength of plate glass, air-cooled tempering method, chemical tempering method and the like are carried out, and the tempered glass obtained by the method is used as a glass member in various products. .

風冷強化法は、板ガラスを、ガラス軟化点温度付近の高温で加熱する必要があるため、板ガラスの形状制御が問題となる場合があり寸法精度の厳しい用途にはコストが高くなる、軟化点温度の高いガラス組成の場合、加熱温度を相当に高くする必要があり設備等にコストがかかる、さらに薄い厚み(例えば、2mm以下)のガラスの強度化が難しい等の問題があった。   In the air-cooling tempering method, it is necessary to heat the plate glass at a high temperature near the glass softening point temperature, so the shape control of the plate glass may be a problem. In the case of a high glass composition, there is a problem that it is necessary to make the heating temperature considerably high, which increases the cost of equipment and the like, and it is difficult to strengthen the glass having a thinner thickness (for example, 2 mm or less).

化学強化法は、イオン交換処理が必要なため、板ガラスの組成が限定される、イオン交換を行うための薬液の管理にコストがかかる、部分的な強化が難しい等の問題があった。   Since the chemical strengthening method requires ion exchange treatment, the composition of the plate glass is limited, management of the chemical solution for performing ion exchange is costly, and partial strengthening is difficult.

最近、ガラス組成、ガラス厚み等に依存せず、ガラスを強化できる可能性のある手法が特許文献1によって提案された。当該手法は、超短パルスレーザー光の集光照射によって板ガラスの内部に異質相が点状、線状、又は網目状に形成するものである。特許文献1では、ソーダ石灰珪酸塩ガラスをレーザー処理することで、機械的強度が最高で1.5倍向上することが確認されている。
特開2003−286048号公報
Recently, Patent Document 1 has proposed a method that can reinforce glass without depending on glass composition, glass thickness, and the like. According to this method, a heterogeneous phase is formed in the shape of dots, lines, or meshes inside a plate glass by focused irradiation of ultrashort pulse laser light. In Patent Document 1, it is confirmed that the mechanical strength is improved up to 1.5 times by laser treatment of soda-lime silicate glass.
JP 2003-286048 A

近年、各種製品は、軽量化の傾向にあり、当然ガラス部材も軽量化が必要となる。特にプラズマディスプレイ(PDP)、液晶ディスプレイ、有機ELディスプレイ等のガラス部材が大部分を占める表示装置では、軽量化達成のためには、ガラス部材の軽量化は不可避である。ガラス部材の軽量化のためには、機械的強度を保持しつつガラス厚を薄くすることを満足させる必要がある。本発明は、薄い板ガラスであっても機械的強度が向上され、且つ表示装置等の製造時における加熱処理後も機械的強度が保持されうる強化ガラスを提供することを課題とする。   In recent years, various products have been in a trend of weight reduction, and naturally, glass members also need to be lightened. In particular, in a display device in which a glass member such as a plasma display (PDP), a liquid crystal display, or an organic EL display occupies most, it is inevitable to reduce the glass member in order to achieve a reduction in weight. In order to reduce the weight of the glass member, it is necessary to satisfy that the glass thickness is reduced while maintaining the mechanical strength. An object of the present invention is to provide a tempered glass that has improved mechanical strength even if it is a thin plate glass and that can maintain mechanical strength even after heat treatment during manufacturing of a display device or the like.

本発明者は、超短パルスレーザー光の集光照射によって板ガラスの内部に、板ガラスの平面視において異質相が点状、線状、又は網目状に形成された強化ガラスにおいて、機械的強度向上の効果の大きいガラス系を見出した。   The inventor has improved the mechanical strength of the tempered glass in which a heterogeneous phase is formed in the shape of dots, lines, or meshes in a plan view of the plate glass by condensing irradiation with an ultrashort pulse laser beam. We found a glass system with great effect.

本発明の強化ガラスは、超短パルスレーザー光の集光照射によって板ガラスの内部に異質相が、板ガラスの平面視において、点状、線状、又は網目状に形成された強化ガラス(以後、超短パルスレーザー光の集光照射によって板ガラスを強化する方法を「レーザー強化」、該方法で強化された板ガラスを「レーザー強化ガラス」とする)であり、レーザーが照射される板ガラスが、歪点が560℃以上、室温から300℃における線膨張係数が84〜88 (×10−7/℃)以上の性状を有することを特徴とする。又、前記超短パルスレーザー光は、ピコ秒からフェムト秒のパルスレーザー光であることが好ましい。 The tempered glass of the present invention is a tempered glass (hereinafter referred to as super The method of strengthening a plate glass by condensing irradiation of a short pulse laser beam is “laser strengthening”, and the plate glass strengthened by the method is called “laser strengthened glass”). The linear expansion coefficient from 560 ° C. to room temperature to 300 ° C. is 84 to 88 (× 10 −7 / ° C.) or more. The ultrashort pulse laser light is preferably a picosecond to femtosecond pulse laser light.

上記性状を有する板ガラスは、いわゆる高歪点ガラスといわれるものである。当該性状を有する板ガラスが、レーザー強化による強度向上に効果を呈するかの要因は不明であるが、レーザー照射によってガラス内部に高密度化された異質相が形成される際の当該局部で熱収縮が小さいからだと推測される。   The plate glass having the above properties is so-called high strain point glass. The factor of whether the glass sheet having the properties exhibits an effect of improving the strength by laser strengthening is unclear, but heat shrinkage occurs locally in the local area when a dense heterogeneous phase is formed inside the glass by laser irradiation. Presumably because it is small.

板ガラスが上記性状を有するために、板ガラスの組成が重量%表示で、SiO52〜54%、Al7〜11%、ZrO 0〜5%、MgO 1〜5%、CaO 5〜9%、SrO 0〜5%、BaO 8〜14%、MgO+CaO+SrO+BaO 20〜25%、TiO 0〜1%、LiO 0〜5%、NaO 2〜6%、KO 7〜11%、及びLiO+NaO+KO 13〜15%の組成を有することが好ましい。 Since the plate glass has the above-mentioned properties, the composition of the plate glass is expressed by weight%, SiO 2 52 to 54%, Al 2 O 3 7 to 11%, ZrO 2 0 to 5%, MgO 1 to 5%, CaO 5 to 5%. 9%, SrO 0-5%, BaO 8-14%, MgO + CaO + SrO + BaO 20-25%, TiO 2 0-1%, Li 2 O 0-5%, Na 2 O 2-6%, K 2 O 7-11 %, And Li 2 O + Na 2 O + K 2 O 13-15%.

本発明のレーザー強化ガラスは、加熱によって異質相が緩和する等の影響を受けにくいので(例えば、異質相が形成された板ガラスを550℃で加熱しても異質相は板ガラス中に残存する)、表示装置を作製する際の加熱工程を経ても機械的強度が保持されやすい利点を有する。   Since the laser tempered glass of the present invention is not easily affected by the heterogeneous phase being relaxed by heating (for example, the heterogeneous phase remains in the plate glass even when the plate glass on which the heterogeneous phase is formed is heated at 550 ° C.). There is an advantage that the mechanical strength is easily maintained even after a heating step in manufacturing the display device.

本発明のレーザー照射よって得られた強化ガラスは、薄い厚みの板ガラスであっても、機械的強度が向上されているので、ガラス部品の軽量化に貢献し、例えば、表示装置等の軽量化に奏功する。   Even if the tempered glass obtained by the laser irradiation of the present invention is a thin glass plate, the mechanical strength is improved, contributing to the weight reduction of glass parts, for example, the weight reduction of display devices and the like. To be successful.

本発明の強化ガラスは、超短パルスレーザー光の集光照射によって板ガラスの内部に異質相が点状、線状、又は網目状に形成されたレーザー強化ガラスである。当該レーザー強化ガラスは、表面から目的とする深さに、レーザー光を集光させることで得られる。   The tempered glass of the present invention is a laser tempered glass in which a heterogeneous phase is formed in a dot shape, a line shape, or a mesh shape inside a plate glass by focused irradiation of an ultrashort pulse laser beam. The said laser tempered glass is obtained by condensing a laser beam to the target depth from the surface.

レーザー光は例えばNd−YAGレーザー励起のTiサファイアレーザーによる、ピコ秒からフェムト秒の超短パルスレーザー光であることが好ましい。パルスレーザー光のパルス幅は、好ましくは数百フェムト秒以下である。   The laser beam is preferably an ultrashort pulse laser beam of picosecond to femtosecond, for example, by a Ti sapphire laser excited by Nd-YAG laser. The pulse width of the pulse laser beam is preferably several hundred femtoseconds or less.

レーザー光の波長は可視から近赤外の範囲で、板ガラスの吸収が少ない波長を用いることが望ましい。好ましくは400nmから1000nmの範囲である。 また、パルスレーザー光のエネルギーは、数nJ〜1mJであることが好ましく、板ガラスにアブレーションを生じさせない程度のエネルギーで、できるだけ高エネルギーにすることが望ましい。   The wavelength of the laser light is preferably in the range from visible to near infrared, and the wavelength at which the glass sheet absorbs little is used. Preferably it is the range of 400 nm to 1000 nm. Further, the energy of the pulse laser beam is preferably several nJ to 1 mJ, and it is desirable that the energy is as high as possible without causing ablation on the plate glass.

レーザー光は、レンズ等により板ガラスの内部へ集光させる。レ−ザ−光の単位面積当たりのエネルギ−にもよるが、異質相を形成するためには、集光は直径100μm以下のスポット状とすることが好ましい。レーザー光の集光点を板ガラスの内部で移動させることにより、板ガラスに異質相を連続的に形成する。又は、レーザー光の集光点を固定し、板ガラスを移動させて、板ガラスに異質相を形成する。   The laser light is condensed inside the plate glass by a lens or the like. Although depending on the energy per unit area of the laser light, in order to form a heterogeneous phase, it is preferable that the condensed light is spot-shaped with a diameter of 100 μm or less. The heterogeneous phase is continuously formed on the plate glass by moving the condensing point of the laser light inside the plate glass. Or the condensing point of a laser beam is fixed, plate glass is moved, and a heterogeneous phase is formed in plate glass.

レーザー光を集光させる位置は、板ガラスの入射面から裏面の間で、任意の位置で選択でき、好ましくは、ガラス表面から垂直方向に250μm〜500μmの位置にする。本発明のガラス組成系においては、レーザー照射により形成される異質相のガラス厚み方向の中心位置が、板ガラス表面から垂直方向に250μm〜500μmの位置に形成されると機械的強度向上に特に効果が高いことを見出した。機械的強度向上を考慮すると、この位置は260〜330μmの範囲、さらには270μm〜310μmの範囲に設定することが好ましい。   The position for condensing the laser beam can be selected at an arbitrary position between the incident surface and the back surface of the plate glass, and is preferably set to a position of 250 μm to 500 μm in the vertical direction from the glass surface. In the glass composition system of the present invention, when the center position in the glass thickness direction of the heterogeneous phase formed by laser irradiation is formed at a position of 250 μm to 500 μm in the vertical direction from the plate glass surface, it is particularly effective for improving the mechanical strength. Found it expensive. Considering the improvement in mechanical strength, this position is preferably set in the range of 260 to 330 μm, more preferably in the range of 270 μm to 310 μm.

板ガラスの断面視において、最近接の異質相間の平均距離を50μm以下の距離とすることにより板ガラスの機械的強度が向上する。この平均距離を50μm以下とすることにより、板ガラス破壊時のクラック伝播方向を異質相によって変化させる効果が高くなり、板ガラスの機械的強度が向上するものと推察される。この平均距離を短くしていくと、機械的強度の向上に奏するが、強化ガラスの製造コストが高くなるので、この平均距離は、0.1μm以上とすることが好ましい。   In the cross-sectional view of the plate glass, the mechanical strength of the plate glass is improved by setting the average distance between the nearest heterogeneous phases to a distance of 50 μm or less. By setting this average distance to 50 μm or less, it is presumed that the effect of changing the crack propagation direction at the time of breaking the plate glass by the heterogeneous phase is increased, and the mechanical strength of the plate glass is improved. If this average distance is shortened, the mechanical strength is improved. However, the manufacturing cost of tempered glass is increased, and therefore this average distance is preferably 0.1 μm or more.

尚、上記平均距離は次ぎの測定で得られたものとして定義される。板ガラスの断面を顕微鏡によって、100〜500倍で拡大して観察したときに像内の現れた異質相について、それぞれの最近接の異質相との距離を測定し得られた値を平均する。他の断面位置についても同様の測定を行い、少なくとも10箇所の断面位置で得られたそれぞれの平均値を、さらに平均して得られたものを板ガラスの断面視における最近接の異質相間の平均距離とする。そして上記断面は、板ガラスを平面視したときの異質相が点状のパターンの場合は、隣接する異質相が含まれるように切断された面であり、線状及び網目状のパターンの場合は、線に対して垂直に切断された面である。   The average distance is defined as that obtained by the next measurement. When the cross-section of the plate glass is observed with a microscope at a magnification of 100 to 500 times, the heterogeneous phases appearing in the image are averaged from the values obtained by measuring the distance from each of the closest heterogeneous phases. The same measurement was performed for other cross-sectional positions, and the average values obtained at the average of the cross-sectional positions of at least 10 locations were further averaged, and the average distance between the adjacent heterogeneous phases in the cross-sectional view of the plate glass was obtained. And And the cross section is a surface cut so that the adjacent heterogeneous phase is included when the heterogeneous phase when the plate glass is viewed in plan is a dot pattern, and in the case of a linear and mesh pattern, A plane cut perpendicular to the line.

さらに、レーザー照射により形成される異質相のガラス厚み方向の長さを、50μm〜500μmとすると機械的強度向上に特に効果が高いことが見出された。異質相の長さが50μm未満では、機械的強度の向上に効果が少なく、他方、500μm超では、焦点深度のさらに長い集光レンズを用いて異質相を形成するため、ガラスを変質する高いエネルギー密度をもったレーザー光が表面を照射する場合があり、この場合にはガラス表面が粗く研削されるなど大きなダメージを受けるため機械的が低下する。そして、機械的強度向上を考慮すると、異質相のガラス厚み方向の長さを60〜330μmとすることが好ましい。   Furthermore, it has been found that when the length of the heterogeneous phase formed by laser irradiation in the thickness direction of the glass is 50 μm to 500 μm, the effect of improving the mechanical strength is particularly high. When the length of the heterogeneous phase is less than 50 μm, the effect of improving the mechanical strength is small. On the other hand, when the heterogeneous phase exceeds 500 μm, the heterogeneous phase is formed by using a condensing lens having a longer focal depth, and thus the high energy for altering the glass. In some cases, laser light having a density irradiates the surface. In this case, mechanical damage is reduced because the glass surface is subjected to large damage such as rough grinding. And considering the mechanical strength improvement, it is preferable that the length of the heterogeneous phase in the glass thickness direction is 60 to 330 μm.

異質相は、板ガラスの平面視において、点状、線状、又は網目状の形に、板ガラスの内部に形成されることが好ましい。又、3次元的に形成されてもよい。   The heterogeneous phase is preferably formed inside the plate glass in the shape of dots, lines, or meshes in plan view of the plate glass. Further, it may be formed three-dimensionally.

本発明のレーザー強化で使用されるガラスは、その性状において、歪点が560℃以上、室温から 300℃における線膨張係数が84〜88 (×10−7/℃)であり 、表示装置での応用を考慮すると、250℃における体積抵抗率が10Ω・cm以上であることが好ましい。 The glass used in the laser strengthening of the present invention has a strain point of 560 ° C. or higher and a linear expansion coefficient from room temperature to 300 ° C. of 84 to 88 (× 10 −7 / ° C.). In consideration of application, the volume resistivity at 250 ° C. is preferably 10 9 Ω · cm or more.

当該性状を有する板ガラスのガラス組成物としては、重量%表示で、SiO52〜54%、Al7〜11%、ZrO 0〜5%、MgO 1〜5%、CaO 5〜9%、SrO 0〜5%、BaO 8〜14%、MgO+CaO+SrO+BaO 20〜25%、TiO 0〜1%、LiO 0〜5%、NaO 2〜6%、KO 7〜11%、及びLiO+NaO+KO 13〜15%の組成を有することが好ましい。 The glass composition of the glass sheet having the properties, in weight percentages, SiO 2 52~54%, Al 2 O 3 7~11%, ZrO 2 0~5%, 1~5% MgO, CaO 5~9 %, SrO 0-5%, BaO 8-14%, MgO + CaO + SrO + BaO 20-25%, TiO 2 0-1%, Li 2 O 0-5%, Na 2 O 2-6%, K 2 O 7-11% And Li 2 O + Na 2 O + K 2 O preferably have a composition of 13-15%.

上記ガラス組成物において、SiOはガラスの主成分であり、重量%において52%未満ではガラスの歪点が低下し、化学的耐久性が悪化する傾向がある。他方54%を越えるとガラス融液の高温粘度が高くなり、フロート法成形が難しくなる。従って、52〜54%、好ましくは、53〜54%の範囲とすることがよい。 In the above glass composition, SiO 2 is a main component of glass. If the weight percentage is less than 52%, the strain point of the glass tends to be lowered and the chemical durability tends to deteriorate. On the other hand, if it exceeds 54%, the high-temperature viscosity of the glass melt increases, and float molding becomes difficult. Therefore, it is good to set it as 52 to 54%, preferably 53 to 54%.

Al7%未満であるとガラスの歪点が低下する傾向がある。他方11%を超えるとガラス融液の高温粘度が高くなり、失透傾向が増大し、フロート法成形が難しくなる。従って7〜11%、好ましくは、8〜11%の範囲とすることがよい。 Al 2 O 3 strain point of the glass is less than 7% tends to decrease. On the other hand, if it exceeds 11%, the high-temperature viscosity of the glass melt increases, the tendency to devitrification increases, and float molding becomes difficult. Therefore, it is 7 to 11%, preferably 8 to 11%.

ZrOは必須成分ではないが、ガラスの歪点を上昇させ、失透の発生を抑える作用を有するので5%以下の範囲で含有させることが好ましい。該成分は、5%を超えると、失透傾向が増大するので、ガラスの溶融やフロート法成形が難しくなる。 ZrO 2 is not an essential component, but it has an effect of raising the strain point of the glass and suppressing the occurrence of devitrification, so it is preferably contained in a range of 5% or less. If the component exceeds 5%, the tendency to devitrification increases, so that it becomes difficult to melt the glass or form the float process.

MgOは他の二価成分酸化物に比べ歪点を上昇させる作用を有するが、1%未満ではその作用が不充分である。他方5%を超えると失透傾向が大きくなる。従って1〜5%、好ましくは2〜4%の範囲とすることがよい。   MgO has an effect of increasing the strain point as compared with other divalent component oxides, but if less than 1%, the effect is insufficient. On the other hand, if it exceeds 5%, the tendency of devitrification increases. Therefore, the content should be in the range of 1 to 5%, preferably 2 to 4%.

CaOは、BaOとの共存下でガラス融液の高温粘度を下げる作用を有するが、5%未満ではその作用が不充分であり、他方9%を超えると失透傾向が大きくなる傾向がある。従って、5〜9%、好ましくは6〜8%の範囲とすることがよい。   CaO has the effect of lowering the high-temperature viscosity of the glass melt in the presence of BaO, but if it is less than 5%, the effect is insufficient, while if it exceeds 9%, the tendency to devitrification tends to increase. Therefore, it is good to set it as 5 to 9%, Preferably it is 6 to 8% of range.

BaOは前記のごとくCaOとの共存下でガラス融液の高温粘度を下げ失透の発生を抑制する作用を有するが、8%未満では失透を抑制する作用が不充分であり、他方14%を超えるとガラスの歪点が低下し過ぎる傾向がある。従って、8〜14%、好ましくは9〜13%の範囲とすることがよい。   BaO has the effect of reducing the high-temperature viscosity of the glass melt and suppressing the occurrence of devitrification in the presence of CaO as described above, but if it is less than 8%, the effect of suppressing devitrification is insufficient, while the other 14% If it exceeds 1, the strain point of the glass tends to decrease too much. Therefore, it is good to set it as 8 to 14%, preferably 9 to 13%.

SrOは必須成分ではないが、CaO及びBaOとの共存下でガラス融液の高温粘度を下げる作用を有する。尚、SrOの含有量は、5%以下の範囲とすることが好ましく、5%を超えると歪点が低下し過ぎ、又線膨張係数を過大とする傾向がある。   SrO is not an essential component, but has the effect of lowering the high-temperature viscosity of the glass melt in the presence of CaO and BaO. The SrO content is preferably in the range of 5% or less, and if it exceeds 5%, the strain point tends to be too low and the linear expansion coefficient tends to be excessive.

さらに、上記組成範囲内において、アルカリ土類金属酸化物(CaO、MgO、BaO、SrO)の合計を20〜25%の範囲とすることによって、ガラスの溶融性を良好な範囲に維持しつつ、粘度−温度勾配を適度として成形性を良好とし、耐熱性、化学的耐久性等に優れ、適切な範囲の線膨張係数を有するガラスを得ることができる。アルカリ土類金属酸化物の合計が25%を越えると、特に線膨張係数が上昇するとともに失透傾向が増大し、化学的耐久性が低下する傾向がある。20%未満では、高温粘度が上昇して溶融および成形を困難とし、線膨張係数が低下する傾向がある。   Furthermore, within the above composition range, by keeping the total of alkaline earth metal oxides (CaO, MgO, BaO, SrO) in the range of 20 to 25%, while maintaining the glass meltability in a good range, A glass having a suitable viscosity-temperature gradient, good moldability, excellent heat resistance, chemical durability, and the like, and an appropriate range of linear expansion coefficient can be obtained. When the total of the alkaline earth metal oxides exceeds 25%, the linear expansion coefficient increases, the tendency to devitrification increases, and the chemical durability tends to decrease. If it is less than 20%, the high-temperature viscosity tends to increase, making melting and molding difficult, and the linear expansion coefficient tends to decrease.

TiOは必須成分ではないが、ガラスの化学的耐久性を向上させ、又ガラス溶融に際して失透傾向を低減させるために1%以下導入することが好ましい。ただし1%を越えて導入するとガラスが着色する傾向があるので好ましくない。 NaOはKOとともにガラス溶融剤として作用し、又ガラスの線膨張係数を適度な大きさに維持するために不可欠である。NaOが2%未満であると線膨張係数が低くなり過ぎる傾向があり、6%を超えると歪点が低下し過ぎる傾向がある。従って、2〜6%、好ましくは、3〜5%の範囲とするとよい。 Although TiO 2 is not an essential component, it is preferably introduced in an amount of 1% or less in order to improve the chemical durability of the glass and reduce the tendency to devitrification when the glass is melted. However, if it exceeds 1%, the glass tends to be colored, which is not preferable. Na 2 O acts as a glass melting agent together with K 2 O, and is indispensable for maintaining the linear expansion coefficient of the glass at an appropriate size. When Na 2 O is less than 2%, the linear expansion coefficient tends to be too low, and when it exceeds 6%, the strain point tends to be too low. Therefore, it is good to set it as 2 to 6%, Preferably it is 3 to 5% of range.

Oは、上記理由及びNaOとの混合アルカリ効果によりアルカリイオンの移動を抑制し、ガラスの体積抵抗率を高める。7%未満であるとそれら作用が不充分であり、11%を超えると線膨張係数が過大となり、又歪点も低下し過ぎる傾向があるため、7〜11%、好ましくは、8〜10%の範囲とするとよい。 K 2 O suppresses the migration of alkali ions due to the above reasons and the mixed alkali effect with Na 2 O, and increases the volume resistivity of the glass. If it is less than 7%, these effects are insufficient, and if it exceeds 11%, the linear expansion coefficient becomes excessive and the strain point tends to decrease too much, so that it is 7 to 11%, preferably 8 to 10%. It is good to be in the range.

LiOは必須成分ではないが、ガラスの高温粘度を下げ、ガラス原料の溶融を促進する。但し、5%を越えて含有させるとガラスの歪点が低下し過ぎる傾向があるので、5%以下の範囲で導入するのが望ましい。 Li 2 O is not an essential component, but lowers the high temperature viscosity of the glass and promotes melting of the glass raw material. However, if the content exceeds 5%, the strain point of the glass tends to be lowered too much, so it is desirable to introduce it in a range of 5% or less.

前記アルカリ成分(NaO、KO、LiO)の量に関し、その合計量を13〜15%にすることにより、歪点、線膨張係数、高温粘度および失透温度を適切な範囲に維持することができる。アルカリ成分の合計量が13%未満では線膨張係数が低下し、失透傾向が増大する傾向にある。15%を越えると歪点が低下し過ぎるうえに、体積抵抗率が低下する。従って、13〜15%の範囲とするとよい。 Regarding the amount of the alkali components (Na 2 O, K 2 O, Li 2 O), the total amount is set to 13 to 15%, so that the strain point, linear expansion coefficient, high temperature viscosity, and devitrification temperature are in an appropriate range. Can be maintained. When the total amount of the alkali components is less than 13%, the linear expansion coefficient decreases and the tendency to devitrification tends to increase. If it exceeds 15%, the strain point is lowered too much and the volume resistivity is lowered. Therefore, it is good to set it as 13 to 15% of range.

又、前記アルカリ成分において、KO/NaO重量比を2.0以上とすると、ガラス中でのアルカリイオンの移動が抑制され、体積抵抗率を上昇させる作用を有するようになり好ましい。 Further, in the alkaline component and the K 2 O / Na 2 O weight ratio is 2.0 or more, the movement of the alkali ions in the glass is suppressed, preferably it takes on the effect of increasing the volume resistivity.

実施例1
板ガラスには、板ガラスには、室温から300℃における線膨張係数が85.4(×10−7/℃)、歪点が603℃、体積抵抗率が109.9Ω・cmの性状を有し、重量%で、SiOが54%、Alが9%、ZrOが3.7%、MgOが3.0%、CaOが7.7%、BaOが9.6%、NaOが4.2%、KOが8.8%の組成を有し、10mm×50mm角で、2.3mm厚サイズのものを準備した。
Example 1
The plate glass has properties such that the linear expansion coefficient from room temperature to 300 ° C. is 85.4 (× 10 −7 / ° C.), the strain point is 603 ° C., and the volume resistivity is 10 9.9 Ω · cm. In terms of weight percent, SiO 2 is 54%, Al 2 O 3 is 9%, ZrO 2 is 3.7%, MgO is 3.0%, CaO is 7.7%, BaO is 9.6%, Na 2 O is 4.2% K 2 O has a composition of 8.8%, at 10 mm × 50 mm square was prepared ones 2.3mm thickness size.

超短パルスレーザー光は、Nd−YAGレーザー励起のTiサファイアレーザーから発振されたパルス幅100フェムト秒、繰返し周期1kHz、中心波長800nmのフェムト秒レーザー光を利用し、NDフィルターを用いて焦点付近での出力を約100mWに調節した。   The ultrashort pulse laser beam is a femtosecond laser beam with a pulse width of 100 femtoseconds, a repetition period of 1 kHz, and a center wavelength of 800 nm oscillated from an Nd-YAG laser-excited Ti sapphire laser. Was adjusted to about 100 mW.

フェムト秒レーザー光の集光する位置をガラス表面から垂直方向に300μm内部に固定し、超短パルスレーザー光を集光レンズ(オリンパス製対物レンズ、倍率10倍、開口数0.25)で約5μmφのスポット状に集光させた。   The position where the femtosecond laser beam is focused is fixed to 300 μm in the vertical direction from the glass surface, and the ultrashort pulse laser beam is approximately 5 μmφ with a focusing lens (Olympus objective lens, magnification 10 ×, numerical aperture 0.25). The light was condensed into a spot shape.

フェムト秒レーザー光の集光する位置をガラス表面から300μm内部に固定し、板ガラスを、自動ステージを用いて25mm/secの速度で移動させることで、点状の異質相を25μm間隔で形成した。そして、点状の異質相を形成する作業を繰り返し、異質相が、板ガラスの断面視において、平均25μmの間隔で形成されたレーザー強化ガラスを得た。   The position where the femtosecond laser beam was focused was fixed to the inside of 300 μm from the glass surface, and the plate glass was moved at a speed of 25 mm / sec using an automatic stage, thereby forming point-like heterogeneous phases at 25 μm intervals. And the operation | work which forms a dotted | punctate heterogeneous phase was repeated and the laser tempered glass in which the heterogeneous phase was formed in the cross-sectional view of plate glass on the average of 25 micrometers was obtained.

実施例2
板ガラスを、室温から300℃における線膨張係数が87.6(×10−7/℃)、歪点が602℃、体積抵抗率が109.4Ω・cmの性状を有し、重量%で、SiOが53.8%、Alが9.6%、ZrOが2.3%、MgOが2.4%、CaOが7.8%、BaOが10.0%、NaOが4.6%、KOが9.5%の組成を有するものを用いた以外は、実施例1と同様の手順にて、板ガラスの断面視において、間隔が平均25μmで、点状の異質相が形成されたレーザー強化ガラスを得た。
Example 2
The sheet glass has properties such that the linear expansion coefficient from room temperature to 300 ° C. is 87.6 (× 10 −7 / ° C.), the strain point is 602 ° C., and the volume resistivity is 10 9.4 Ω · cm. SiO 2 53.8%, Al 2 O 3 9.6%, ZrO 2 2.3%, MgO 2.4%, CaO 7.8%, BaO 10.0%, Na 2 Except for using O having a composition of 4.6% and K 2 O of 9.5%, in the same manner as in Example 1, in the cross-sectional view of the plate glass, the interval was 25 μm on average and was dotted A laser tempered glass in which a heterogeneous phase was formed was obtained.

実施例3
板ガラスを、室温から300℃における線膨張係数が86.7(×10−7/℃)、歪点が610℃、体積抵抗率が109.7Ω・cmの性状を有し、重量%で、SiOが53.2%、Alが9.3%、ZrOが3.9%、MgOが3.4%、CaOが6.8%、BaOが9.8%、NaOが4.5%、KOが9.1%の組成を有するものを用いた以外は、実施例1と同様の手順にて、板ガラスの断面視において、間隔が平均25μmで、点状の異質相が形成されたレーザー強化ガラスを得た。
Example 3
The sheet glass has properties such that the linear expansion coefficient from room temperature to 300 ° C. is 86.7 (× 10 −7 / ° C.), the strain point is 610 ° C., the volume resistivity is 10 9.7 Ω · cm, and the weight percentage is SiO 2 is 53.2%, Al 2 O 3 is 9.3%, ZrO 2 is 3.9%, MgO is 3.4%, CaO is 6.8%, BaO is 9.8%, Na 2. Except for using O having a composition of 4.5% and K 2 O of 9.1%, in the same procedure as in Example 1, in the cross-sectional view of the plate glass, the interval was 25 μm on average and dotted A laser tempered glass in which a heterogeneous phase was formed was obtained.

実施例4
板ガラスを、室温から300℃における線膨張係数が87.3(×10−7/℃)、歪点が595℃、体積抵抗率が109.8Ω・cmの性状を有し、重量%で、SiOが53.6%、Alが10.4%、MgOが3.6%、CaOが8.0%、BaOが11.2%、NaOが4.2%、KOが8.8%の組成を有するものを用いた以外は、実施例1と同様の手順にて、板ガラスの断面視において、間隔が平均25μmで、点状の異質相が形成されたレーザー強化ガラスを得た。
Example 4
The plate glass has properties such that the linear expansion coefficient from room temperature to 300 ° C. is 87.3 (× 10 −7 / ° C.), the strain point is 595 ° C., the volume resistivity is 10 9.8 Ω · cm, and the weight% SiO 2 53.6%, Al 2 O 3 10.4%, MgO 3.6%, CaO 8.0%, BaO 11.2%, Na 2 O 4.2%, K except that 2 O was used having a composition of 8.8% at the same manner as in example 1, in a cross-sectional view of the glass sheet, a laser distance on average 25 [mu] m, dotted heterogeneous phase is formed A tempered glass was obtained.

実施例5
板ガラスを、室温から300℃における線膨張係数が86.2(×10−7/℃)、歪点が600℃、体積抵抗率が109.2Ω・cmの性状を有し、重量%で、SiOが53.9%、Alが10.5%、ZrOが1.0%、MgOが3.0%、CaOが7.9%、BaOが9.1%、NaOが4.8%、KOが9.8%の組成を有するものを用いた以外は、実施例1と同様の手順にて、板ガラスの断面視において、間隔が平均25μmで、線状の異質相が形成されたレーザー強化ガラスを得た。
Example 5
The plate glass has properties such that the linear expansion coefficient from room temperature to 300 ° C. is 86.2 (× 10 −7 / ° C.), the strain point is 600 ° C., and the volume resistivity is 10 9.2 Ω · cm. SiO 2 53.9%, Al 2 O 3 10.5%, ZrO 2 1.0%, MgO 3.0%, CaO 7.9%, BaO 9.1%, Na 2 Except for using O having a composition of 4.8% and K 2 O having a composition of 9.8%, the same procedure as in Example 1 was used, and the interval was 25 μm on average in the cross-sectional view of the plate glass. A laser tempered glass in which a heterogeneous phase was formed was obtained.

比較例1
板ガラスには、室温から 300℃における熱膨張係数が88.0(×10−7/℃)、歪点が520℃、体積抵抗率が107.1Ω・cmの性状を有し、重量%で、SiOが70.6%、Alが2.0%、MgOが3.6%、CaOが9.5%、NaO+KOが14.3%の組成を有するものを用いた。
Comparative Example 1
The plate glass has properties such that the thermal expansion coefficient from room temperature to 300 ° C. is 88.0 (× 10 −7 / ° C.), the strain point is 520 ° C., and the volume resistivity is 10 7.1 Ω · cm. And having a composition of 70.6% SiO 2 , 2.0% Al 2 O 3 , 3.6% MgO, 9.5% CaO and 14.3% Na 2 O + K 2 O Using.

超短パルスレーザー光は、Nd−YAGレーザー励起のTiサファイアレーザーから発振されたパルス幅100フェムト秒、繰返し周期1kHz、中心波長800nmのフェムト秒レーザー光を利用し、NDフィルターを用いて焦点付近での出力を約9mWに調節した。   The ultrashort pulse laser beam is a femtosecond laser beam with a pulse width of 100 femtoseconds, a repetition period of 1 kHz, and a center wavelength of 800 nm oscillated from an Nd-YAG laser-excited Ti sapphire laser. Was adjusted to about 9 mW.

フェムト秒レーザー光の集光する位置をガラス表面から垂直方向に200μm内部に固定し、超短パルスレーザー光を集光レンズ(オリンパス製対物レンズ、倍率40倍、開口数0.55)で約5μmφのスポット状に集光させた。   The position where the femtosecond laser beam is focused is fixed to 200 μm inside in the vertical direction from the glass surface, and the ultrashort pulse laser beam is approximately 5 μmφ with a focusing lens (Olympus objective lens, magnification 40 ×, numerical aperture 0.55). The light was condensed into a spot shape.

フェムト秒レーザー光の集光する位置をガラス表面から200μm内部に固定し、板ガラスを、自動ステージを用いて25mm/secの速度で移動させることで、点状の異質相を、25μm間隔で形成した。そして、点状の異質相を形成する作業を繰り返し、、板ガラスの断面視において、点状の異質相が平均25μmの間隔で形成されたレーザー強化ガラスを得た。
[レーザー強化ガラスの機械的強度の評価]
実施例1乃至5、及び比較例1で得られたレーザー強化ガラスについて、支点間距離30mm、荷重点間距離10mm、荷重速度0.5mm/minの条件で4点曲げ強度試験を行い、破壊時の負荷荷重を測定し、レーザー強化前の板ガラスとそれと比較し、レーザー強化による機械的強度の増加率を求めた。結果を表1に示す。
A spot-like heterogeneous phase was formed at intervals of 25 μm by fixing the position where the femtosecond laser beam was focused to 200 μm inside from the glass surface and moving the plate glass at a speed of 25 mm / sec using an automatic stage. . And the operation | work which forms a dotted | punctate heterogeneous phase was repeated and the laser tempered glass in which the dotted | punctate heterogeneous phase was formed in the space | interval of 25 micrometers on average was obtained in the cross sectional view of plate glass.
[Evaluation of mechanical strength of laser tempered glass]
The laser tempered glass obtained in Examples 1 to 5 and Comparative Example 1 was subjected to a 4-point bending strength test under the conditions of a distance between fulcrums of 30 mm, a distance between load points of 10 mm, and a load speed of 0.5 mm / min. The load was measured and compared with the plate glass before laser strengthening to determine the rate of increase in mechanical strength due to laser strengthening. The results are shown in Table 1.

実施例1乃至5、及び比較例1のそれぞれにおいて、レーザー強化によって、機械的強度の向上が確認された。そして、実施例1乃至5のレーザー強化ガラスは、比較例1より機械的強度が向上することが確認された。   In each of Examples 1 to 5 and Comparative Example 1, improvement in mechanical strength was confirmed by laser strengthening. And it was confirmed that the laser-strengthened glass of Examples 1 to 5 has improved mechanical strength as compared with Comparative Example 1.

[レーザー強化ガラスの加熱処理]
実施例1及び比較例1で得られたレーザー強化ガラスを加熱炉にて550℃に加熱、30分間の保持後、室温まで冷却した。図1乃至4に、異質相部を反射微分干渉顕微鏡で拡大観察したときの図面代用写真を示す。図1は、実施例1で得られた強化ガラスの加熱処理前、図2は、実施例1で得られた強化ガラスの加熱処理後、図3は、比較例1で得られた強化ガラスの加熱処理前、図4は比較例1で得られた強化ガラスの加熱処理後のものである。
[Laser tempered glass heat treatment]
The laser tempered glass obtained in Example 1 and Comparative Example 1 was heated to 550 ° C. in a heating furnace, held for 30 minutes, and then cooled to room temperature. FIGS. 1 to 4 show photographs substituted for drawings when the heterogeneous phase portion is magnified and observed with a reflection differential interference microscope. 1 shows the tempered glass obtained in Example 1 before the heat treatment, FIG. 2 shows the tempered glass obtained in Example 1 after the heat treatment, and FIG. 3 shows the tempered glass obtained in Comparative Example 1. FIG. 4 shows the tempered glass obtained in Comparative Example 1 after the heat treatment before the heat treatment.

実施例1で得られたレーザー強化ガラスは、加熱処理後も点状の異質相は消滅せず、その形状は熱処理前とほぼ同様であったのに対し、比較例1で得られたレーザー強化ガラスは、点状の異質相は熱処理後にほぼ消滅した。本発明のレーザー強化ガラスは、PDP等の加熱工程を伴う表示装置の基板として好適であることが確認された。   In the laser tempered glass obtained in Example 1, the point-like heterogeneous phase did not disappear even after the heat treatment, and its shape was almost the same as that before the heat treatment, whereas the laser tempered glass obtained in Comparative Example 1 In the glass, the point-like heterogeneous phase almost disappeared after the heat treatment. It was confirmed that the laser tempered glass of the present invention is suitable as a substrate of a display device accompanied by a heating process such as PDP.

本実施例1のレーザー強化ガラスの表面を反射微分干渉顕微鏡で200倍に拡大して観察したときの図面代用の写真である。It is a photograph for drawing substitutes when the surface of the laser tempered glass of this Example 1 is magnified 200 times with a reflection differential interference microscope. 本実施例1のレーザー強化ガラスを550℃で加熱処理した後のその表面を反射微分干渉顕微鏡で200倍に拡大して観察したときの図面代用の写真である。It is the photograph instead of drawing when the surface after heat-treating the laser tempered glass of the present Example 1 at 550 degreeC is magnified 200 times with the reflection differential interference microscope. 本比較例1のレーザー強化ガラスの表面を反射微分干渉顕微鏡で200倍に拡大して観察したときの図面代用の写真である。It is the photograph instead of drawing when the surface of the laser tempered glass of this comparative example 1 is magnified 200 times and observed with the reflection differential interference microscope. 本比較例1のレーザー強化ガラスを550℃で加熱処理した後のその表面を反射微分干渉顕微鏡で200倍に拡大して観察したときの図面代用の写真である。It is the photograph instead of drawing when the surface after heat-treating the laser tempered glass of this comparative example 1 at 550 degreeC is magnified 200 times with the reflection differential interference microscope.

Claims (2)

板ガラスの機械的強度を向上させる方法であり、該方法は、ピコ秒からフェムト秒の超短パルスレーザー光の集光照射によって板ガラスの内部に異質相を、板ガラスの平面視において、点状、線状、又は網目状に形成するものであり、レーザーが照射される板ガラスを、歪点が560℃以上、室温から300℃における線膨張係数が84〜88(×10 −7 /℃)の性状を有し、且つ、重量%表示で、SiO 52〜54%、Al 7〜11%、ZrO 0〜5%、MgO 1〜5%、CaO 5〜9%、SrO 0〜5%、BaO 8〜14%、MgO+CaO+SrO+BaO 20〜25%、TiO 0〜1%、Li O 0〜5%、Na O 2〜6%、K O 7〜11%、及びLi O+Na O+K O 13〜15%の組成を有するものとすることを特徴とする板ガラスの機械的強度を向上させる方法 It is a method for improving the mechanical strength of a plate glass, which is a method for producing a heterogeneous phase inside a plate glass by focused irradiation of an ultrashort pulse laser beam of picoseconds to femtoseconds. Jo, or is intended to form a reticulated, the flat glass laser is irradiated, the strain point of 560 ° C. or higher, linear expansion coefficient at 300 ° C. from room temperature properties of 84~88 (× 10 -7 / ℃) has, and, by weight percentages, SiO 2 52~54%, Al 2 O 3 7~11%, ZrO 2 0~5%, MgO 1~5%, CaO 5~9%, SrO 0~5% BaO 8-14%, MgO + CaO + SrO + BaO 20-25%, TiO 2 0-1%, Li 2 O 0-5%, Na 2 O 2-6%, K 2 O 7-11%, and Li 2 O + Na 2 O + K. 2 O 13-15% A method for improving the mechanical strength of plate glass, characterized by having a composition . 請求項1に記載の方法により板ガラスの機械的強度を向上させる工程、及び前記工程で機械的強度の向上がなされた板ガラスを550℃以上で加熱する工程を有することを特徴とする表示装置の製法。 A method for producing a display device, comprising: a step of improving the mechanical strength of a plate glass by the method according to claim 1; and a step of heating the plate glass whose mechanical strength has been improved in the step at 550 ° C. or higher. .
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