JPH07101736A - Molding glass material and method for manufacturing optical glass element - Google Patents
Molding glass material and method for manufacturing optical glass elementInfo
- Publication number
- JPH07101736A JPH07101736A JP25156893A JP25156893A JPH07101736A JP H07101736 A JPH07101736 A JP H07101736A JP 25156893 A JP25156893 A JP 25156893A JP 25156893 A JP25156893 A JP 25156893A JP H07101736 A JPH07101736 A JP H07101736A
- Authority
- JP
- Japan
- Prior art keywords
- molding
- glass material
- optical
- effective surface
- diameter
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Classifications
-
- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B11/00—Pressing molten glass or performed glass reheated to equivalent low viscosity without blowing
- C03B11/06—Construction of plunger or mould
- C03B11/08—Construction of plunger or mould for making solid articles, e.g. lenses
-
- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03B—MANUFACTURE, SHAPING, OR SUPPLEMENTARY PROCESSES
- C03B2215/00—Press-moulding glass
- C03B2215/72—Barrel presses or equivalent, e.g. of the ring mould type
Landscapes
- Engineering & Computer Science (AREA)
- Chemical & Material Sciences (AREA)
- Manufacturing & Machinery (AREA)
- Materials Engineering (AREA)
- Organic Chemistry (AREA)
- Surface Treatment Of Glass (AREA)
- Glass Compositions (AREA)
Abstract
(57)【要約】
【目的】 成形用ガラス素材と上下型に偏心が生じた場
合でも、良好な光学性能を得ることを可能とした光学素
子成形技術(成形用ガラス素材、光学ガラス素子の製造
方法等)を提供する。
【構成】 胴型内径をφC、上下型のうち光学有効面径
の大きい型の光学有効面径をφA、成形用ガラス素材の
外径をφS、成形用ガラス素材の有効面径をφSSとし
た時、φA<φSS≦φSであり、かつ、φC−[φS
−{(φS−φSS)/2}]≦(φC−φA)/2を
満たす成形用ガラス素材を用いる。
【効果】 成形用ガラス素材の有効面以外の面が光学ガ
ラス素子の光学有効面に回り込むことがなく、成形用ガ
ラス素材の有効面以外の面を有効面と同様な高精度に加
工する必要がなくなり、位置決め装置も必要なくなる。
(57) [Abstract] [Purpose] Optical element molding technology (manufacturing of glass material for molding and optical glass element) that enables good optical performance even when eccentricity occurs between the molding glass material and the upper and lower molds. Method). [Structure] Inner diameter of barrel mold is φC, optical effective surface diameter of upper and lower molds is φA, outer diameter of molding glass material is φS, effective surface diameter of molding glass material is φSS When φA <φSS ≦ φS, and φC− [φS
A glass material for molding which satisfies − {(φS−φSS) / 2} ≦ (φC−φA) / 2 is used. [Effect] The surface other than the effective surface of the molding glass material does not wrap around the optically effective surface of the optical glass element, and it is necessary to process the surface other than the effective surface of the molding glass material with the same high precision as the effective surface. It eliminates the need for positioning devices.
Description
【0001】[0001]
【産業上の利用分野】本発明は、光学機器に使用される
レンズ、プリズム等の高精度光学ガラス素子を精密ガラ
ス成形法により形成するための成形用ガラス素材、光学
ガラス素子の製造方法及び光学ガラス素子に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a molding glass material for forming a high-precision optical glass element such as a lens or a prism used in optical equipment by a precision glass molding method, a method for producing an optical glass element, and an optical glass element. Regarding glass elements.
【0002】[0002]
【従来の技術】近年、高精度光学レンズ、特に非球面ガ
ラスレンズ等の製造法として、研磨工程無しの一発成形
により、形成する試みが多くなされ、具現化されつつあ
る。2. Description of the Related Art In recent years, many attempts have been made to realize high-precision optical lenses, particularly aspherical glass lenses, etc. by one-shot molding without a polishing step, and these are being realized.
【0003】その成形法の一つとして、ガラス素材を変
形可能な温度、例えば軟化点近傍の温度に加熱し、押圧
成形等の手段を用いて成形する方法がある(例えば、特
開昭61ー21927号公報、特開昭62−18212
2号公報)。As one of the molding methods, there is a method of heating a glass material to a temperature at which it can be deformed, for example, a temperature near its softening point, and molding it by means such as press molding (see, for example, JP-A-61-161). 21927, JP-A-62-18212.
No. 2).
【0004】この方法には、良好な面粗度及び適切な形
状を有した成形用ガラス素材が必要である。以下、図面
を用いて従来の光学ガラス素子の製造方法の一例につい
て説明する。This method requires a glass molding material having a good surface roughness and an appropriate shape. An example of a conventional method for manufacturing an optical glass element will be described below with reference to the drawings.
【0005】図5は、従来の成形用ガラス素材、片面は
平面、他方はR曲面形状を成形して光学ガラス素子を加
圧変形させた状態を示す断面図である。20、21はそ
れぞれ上型と下型、22は胴型、25は光学ガラス素
子、23、24は加熱加圧機構を備えたプレスヘッドの
一部である。FIG. 5 is a cross-sectional view showing a conventional glass material for molding, one surface of which is a flat surface and the other of which is an R-curved surface and the optical glass element is deformed under pressure. Reference numerals 20 and 21 are upper and lower dies, 22 is a barrel die, 25 is an optical glass element, and 23 and 24 are parts of a press head having a heating and pressing mechanism.
【0006】成形用ガラス素材25を、上型20、下型
21、胴型22の中に供給し、加熱加圧機構を備えたプ
レスヘッド23、24で加熱して押圧成形する。変形が
終了した後は上型20、下型21、胴型22、光学ガラ
ス素子25を徐々に冷却し、光学ガラス素子25が取り
出し可能な温度以下になると上型20を開き、光学ガラ
ス素子25を取り出す。The glass material 25 for molding is supplied into the upper mold 20, the lower mold 21, and the body mold 22, and heated by press heads 23 and 24 equipped with a heating and pressing mechanism to press-mold. After the deformation is completed, the upper mold 20, the lower mold 21, the body mold 22, and the optical glass element 25 are gradually cooled, and when the temperature is below the temperature at which the optical glass element 25 can be taken out, the upper mold 20 is opened, and the optical glass element 25 is opened. Take out.
【0007】[0007]
【発明が解決しようとする課題】上記の成形方法におい
て、胴型内径に比べて成形用ガラス素材外径がある程度
以上小さいと、成形用ガラス素材と上下型に偏心が生じ
る。偏心が生じると、成形用ガラス素材の有効面以外の
面が光学ガラス素子の光学有効面まで回り込んでくる。In the above molding method, when the outer diameter of the glass material for molding is smaller than the inner diameter of the barrel by a certain degree or more, the glass material for molding and the upper and lower molds are eccentric to each other. When the eccentricity occurs, the surface other than the effective surface of the molding glass material wraps around to the optically effective surface of the optical glass element.
【0008】前述した光学ガラス素子の光学有効面と
は、光学ガラス素子において実際に光学ガラス素子に要
求される光学性能を生み出すために最小限必要とされる
光学作用面のことであり、また、光学ガラス素材の有効
面とは光学ガラス素子と同等の面粗度を有した面のこと
である。The above-mentioned optically effective surface of the optical glass element is the minimum required optical action surface for producing the optical performance actually required for the optical glass element in the optical glass element, and The effective surface of the optical glass material is a surface having the same surface roughness as that of the optical glass element.
【0009】その面粗度の一例を具体的に述べれば、研
磨加工面の場合、Rmax=0.01μm以下が用いられることが
多いが、勿論、光学ガラス素子により必要な面粗度が異
なるので、一律に断言することはできない。To give a concrete example of the surface roughness, in the case of a polished surface, Rmax = 0.01 μm or less is often used. Of course, since the required surface roughness differs depending on the optical glass element, You can't affirm uniformly.
【0010】成形用ガラス素材の有効面以外の面が光学
ガラス素子の光学有効面として成形されると、外観上は
勿論のこと透過率の低下など光学ガラス素子としての性
能に悪影響を及ぼす。When a surface other than the effective surface of the glass material for molding is molded as an optically effective surface of the optical glass element, not only the appearance but also the performance of the optical glass element is adversely affected by a decrease in transmittance.
【0011】また、それらを防止するために、成形用ガ
ラス素材と型の位置決め機構を設けたり、成形用ガラス
素材の有効面以外の面を有効面と同様の面粗度に加工し
た成形用ガラス素材を用いたりすると、成形用ガラス素
材や成形された光学ガラス素子のコストアップの要因と
なる。In order to prevent them, a molding glass material and a mold positioning mechanism are provided, and a surface of the molding glass material other than the effective surface is processed to have the same surface roughness as the effective surface. If a material is used, the cost of the glass material for molding and the molded optical glass element increases.
【0012】また、胴型内径と成形用ガラス素材外径の
差が殆ど無いと見なせる程に小さい場合には、型の形状
や成形用ガラス素材の形状によって、型の光学機能面と
成形用ガラス素材の有効面間にある密閉空間部分の気体
が抜けない、あるいは変形量が十分に確保できない等の
問題が生じ、光学有効面の転写が不完全になり、良好な
光学ガラス素子を得ることが出来なかった。When the difference between the inner diameter of the barrel die and the outer diameter of the forming glass material is so small that there is almost no difference, the optical functional surface of the die and the forming glass may be changed depending on the shape of the die and the forming glass material. There is a problem that the gas in the closed space between the effective surfaces of the material does not escape, or the amount of deformation cannot be secured sufficiently, the transfer of the optically effective surface becomes incomplete, and a good optical glass element can be obtained. I could not do it.
【0013】[0013]
【課題を解決するための手段】上記課題を解決するため
に本発明は、胴型内径をφC、一対の上下型のうち光学
有効面径が大きい型の光学有効面径をφA、成形用ガラ
ス素材の外径をφS、成形用ガラス素材の有効面径をφ
SSとした時、それらの関係が、φA<φSS≦φSで
あり、かつ、φC−[φS−{(φS−φSS)/
2}]≦(φC−φA)/2である成形用ガラス素材を
用いるものである。In order to solve the above-mentioned problems, the present invention is directed to a cylindrical mold inner diameter of φC, a pair of upper and lower molds having a larger optically effective surface diameter, and an optically effective surface diameter of φA. The outer diameter of the material is φS, and the effective surface diameter of the glass material for molding is φ
When SS, the relation between them is φA <φSS ≦ φS, and φC− [φS − {(φS−φSS) /
2}] ≦ (φC−φA) / 2 is used.
【0014】[0014]
【作用】前述した関係を満たす成形用ガラス素材によ
り、成形用ガラス素材と上下型に偏心が生じた場合で
も、光学ガラス素子の光学有効面に成形用ガラス素材の
有効面以外の面の回り込みがなくなり、良好な光学有効
面を有した光学ガラス素子を得ることが出来る。[Function] With the molding glass material satisfying the above-mentioned relationship, even when eccentricity occurs between the molding glass material and the upper and lower molds, the wraparound of the surface other than the effective surface of the molding glass material on the optically effective surface of the optical glass element. It is possible to obtain an optical glass element having a good optically effective surface.
【0015】[0015]
【実施例】以下、本発明の成形用ガラス素材と光学ガラ
ス素子の製造方法と光学ガラス素子の実施例について図
面を参照しながら説明する。EXAMPLES Examples of the glass material for molding, the method for producing an optical glass element and the optical glass element of the present invention will be described below with reference to the drawings.
【0016】(実施例1)図1は、本発明の第1の実施
例の説明図であり、成形用ガラス素材を上下型間に保持
した状態及び光学ガラス素子が示されている。(Embodiment 1) FIG. 1 is an explanatory view of a first embodiment of the present invention, showing a state in which a glass material for molding is held between upper and lower molds and an optical glass element.
【0017】図1において、1は上型、2は下型、3は
胴型、6は成形用ガラス素材、4、5は加熱加圧機構を
備えたプレスヘッドの一部、7は光学ガラス素子であ
る。In FIG. 1, 1 is an upper mold, 2 is a lower mold, 3 is a barrel mold, 6 is a glass material for molding, 4 and 5 are a part of a press head having a heating and pressing mechanism, and 7 is an optical glass. It is an element.
【0018】本実施例では、成形された光学ガラス素子
7の外径を規制する胴型内径φCはφ6mmである。上
型1の光学機能面径φBu及び下型2の光学機能面径φ
Bdはφ5.5mm、上型1の光学有効面径φAuはφ
4.3mm、下型2の光学有効面径φAdはφ4.5m
mである。In the present embodiment, the inner diameter φC of the barrel die for controlling the outer diameter of the molded optical glass element 7 is φ6 mm. Optical functional surface diameter φBu of upper mold 1 and optical functional surface diameter φ of lower mold 2
Bd is φ5.5 mm, the optical effective surface diameter φAu of the upper mold 1 is φ
4.3 mm, lower die 2 has an optically effective surface diameter φAd of φ4.5 m
m.
【0019】また、上型1の曲率半径は8mm、下型2
の曲率半径は12mmで光学機能面径φBu=φBd=
φ5.5mmまで加工されており、それより外周は平坦
部となっている。The radius of curvature of the upper mold 1 is 8 mm, and the lower mold 2 is
Has a radius of curvature of 12 mm and an optical functional surface diameter φBu = φBd =
It is processed up to φ 5.5 mm, and the outer circumference is flat from that.
【0020】前述した上下型の光学有効面とは、成形転
写された光学ガラス素子の光学有効面に対応して実際に
光学ガラス素子に要求される光学性能を生み出すために
最小限必要とされる面のことである。The above-mentioned upper and lower optically effective surfaces are the minimum required to produce the optical performance actually required for the optical glass element corresponding to the optically effective surface of the molded and transferred optical glass element. It is a face.
【0021】また、前述した光学機能面とは、図1
(a)で示すように光学有効面を含み、光学有効面から
平坦面までの曲面を加えた面までのことである。平坦面
がない場合は、胴型内径と摺動収納する上下型の外径部
分までが光学機能面である。Further, the above-mentioned optical function surface is as shown in FIG.
As shown in (a), it is a surface including an optically effective surface and a surface obtained by adding a curved surface from the optically effective surface to a flat surface. If there is no flat surface, the inner diameter of the barrel die and the outer diameter portion of the upper and lower dies that are slidably housed are the optically functional surfaces.
【0022】上型1、下型2の光学有効面径φAu、φ
Adは勿論のこと、光学有効面径φAu、φAdから光
学機能面径φBu、φBdまでを球面でなく非球面に加
工しても良い。Optical effective surface diameters φAu, φ of the upper mold 1 and the lower mold 2.
Not only Ad but also the optically effective surface diameters φAu and φAd to the optically functional surface diameters φBu and φBd may be processed into aspherical surfaces instead of spherical surfaces.
【0023】形状精度は上型1、下型2ともPV=λ/
8(λ=633nm)以下である。成形用ガラス素材6
の形状(図4(a)に断面図を示す)は、両端面ともに
平面で光学ガラス素子7と同等の面粗度Rmax=0.
01μm以下に仕上げられているが、外周面(有効面以
外の面)は研削面であり、面粗度はRmax=約1μ
m、外径φSと有効面径φSSは等しくφ5.4mmで
作成してある。The shape accuracy is PV = λ / for both the upper mold 1 and the lower mold 2.
It is 8 (λ = 633 nm) or less. Molding glass material 6
4 (a cross-sectional view is shown in FIG. 4A), both end faces are flat and have a surface roughness Rmax = 0.
The outer peripheral surface (the surface other than the effective surface) is a ground surface, and the surface roughness is Rmax = about 1 µm.
m, the outer diameter φS and the effective surface diameter φSS are equal to each other and are made to be φ5.4 mm.
【0024】よって、本実施例では、上下型のうち光学
有効面径が大きい型の光学有効面径φAd=φA=φ
4.5mm、上下型のうち光学機能面径が小さい型の光
学機能面径φBu=φBd=φB=φ5.5mm、φS
=φSS=5.4mm、φC=φ6mmとなり、本発明
の寸法関係の範囲内である。Therefore, in this embodiment, the optical effective surface diameter φAd = φA = φ of the upper and lower dies having the larger optical effective surface diameter.
4.5 mm, of the upper and lower molds, which has a smaller optical function surface diameter, has an optical function surface diameter φBu = φBd = φB = φ5.5 mm, φS
= ΦSS = 5.4 mm and φC = φ6 mm, which are within the range of the dimensional relationship of the present invention.
【0025】また、光学ガラス素子7の中心厚は3.0
mmであり、成形用ガラス素材6の厚みは3.12mm
に作成されている。また成形用ガラス素材6の材料とし
ては、SF4(Tg=430℃)を用いた。The center thickness of the optical glass element 7 is 3.0.
mm, and the thickness of the glass material for molding 6 is 3.12 mm.
Has been created in. SF4 (Tg = 430 ° C.) was used as the material of the glass material 6 for molding.
【0026】成形用ガラス素材6を成形用ガラス素材6
の有効面径φSSと上下型の光学有効面径φAu、φA
dが対向するよう上型1、下型2、胴型3の間に配置す
る。プレスヘッド4、5によりそれらを加熱する。Forming glass material 6 Forming glass material 6
Effective surface diameter φSS and upper and lower optical effective surface diameters φAu, φA
It is arranged between the upper die 1, the lower die 2 and the body die 3 so that d faces each other. The press heads 4, 5 heat them.
【0027】成形用ガラス素材6が成形可能な温度に到
達すると、プレスヘッド4、5により加圧を行い所定量
変形させる。成形温度は520℃、加圧力は450Kg
f/cm2とした。When the molding glass material 6 reaches a temperature at which it can be molded, it is pressed by the press heads 4 and 5 to be deformed by a predetermined amount. Molding temperature is 520 ℃, pressure is 450 Kg
It was set to f / cm 2 .
【0028】光学ガラス素子7の中心厚は胴型3の端面
と上型1、下型2の胴型3の端面と対向する面が当接す
ることにより決定している。他の方法で光学ガラス素子
の中心厚を決定しても良い。The center thickness of the optical glass element 7 is determined by the contact between the end surface of the barrel die 3 and the surfaces of the upper die 1 and the lower die 2 which face the end faces of the barrel die 3. The center thickness of the optical glass element may be determined by other methods.
【0029】変形が終了した後、プレスヘッド4、5に
より、冷却を行う。光学ガラス素子7が取りだし可能な
温度420℃以下になると上型1、胴型3を分解し、光
学ガラス素子7を取り出す。光学ガラス素子7の形状精
度は上下面ともPV=λ/5以下を示し、型精度を良好
に転写していた。After the deformation is completed, the press heads 4 and 5 perform cooling. When the temperature at which the optical glass element 7 can be taken out falls below 420 ° C., the upper mold 1 and the barrel mold 3 are disassembled, and the optical glass element 7 is taken out. The shape accuracy of the optical glass element 7 was PV = λ / 5 or less on both upper and lower surfaces, and the mold accuracy was well transferred.
【0030】また、図1(b)に示すように、成形用ガ
ラス素材6が一方に偏り外周面が胴型3の内壁に接触し
ても、対向する側の成形用ガラス素材6の外周面と胴型
3の内壁との最大隙間Lsは、Ls=φC−[φS−
{(φS−φSS)/2}]=6−[5.4−{(5.
4−5.4)/2}]=0.6mmであり、胴型3の内
壁から、上型1の光学有効面径φAuまでの距離Lku
=(φC−φAu)/2=(6−4.3)/2=0.8
5mm、下型2の光学有効面径φAdまでの距離Lkd
=(φC−φAd)/2=(6−4.5)/2=0.7
5mmより小さいため、すなわち、本発明に規定の寸法
関係であるため、図1(c)に示すように光学ガラス素
子7の光学有効面径φAu、φAdに成形用ガラス素材
6の有効面径φSS以外の面が回り込むこと無く常に良
好な転写面を有した光学ガラス素子7が得られた。Further, as shown in FIG. 1B, even if the molding glass material 6 is biased to one side and the outer peripheral surface comes into contact with the inner wall of the barrel mold 3, the outer peripheral surface of the molding glass material 6 on the opposite side is opposed. The maximum gap Ls between the inner wall of the body mold 3 and Ls = φC− [φS−
{(ΦS-φSS) / 2}] = 6- [5.4-{(5.
4-5.4) / 2}] = 0.6 mm, and the distance Lku from the inner wall of the barrel die 3 to the optically effective surface diameter φAu of the upper die 1.
= (ΦC−φAu) / 2 = (6−4.3) /2=0.8
5 mm, distance Lkd to the optically effective surface diameter φAd of the lower mold 2
= (ΦC−φAd) / 2 = (6-4.5) /2=0.7
Since it is smaller than 5 mm, that is, because of the dimensional relationship specified in the present invention, the optical effective surface diameters φAu and φAd of the optical glass element 7 are changed to the effective surface diameter φSS of the molding glass material 6 as shown in FIG. It was possible to obtain the optical glass element 7 which always had a good transfer surface without wrapping around other surfaces.
【0031】本実施例の上型1、下型2の形状、光学機
能面径φBu、φBdが胴型内径φCより小さく光学機
能面径φBu、φBdが凹面形状を有し、図4(a)の
ような両端面が平面形状の成形用ガラス素材を用いる場
合、上下型のうち光学有効面径が大きい型の光学有効面
径φA、上下型のうち光学機能面径が小さい型の光学機
能面径φB、成形用ガラス素材の外径φS、成形用ガラ
ス素材の有効面径φSSの関係が、φA<φSS≦φS
≦φBにしておくことが望ましい。The shapes of the upper mold 1 and the lower mold 2 of this embodiment, the optical function surface diameters φBu and φBd are smaller than the barrel mold inner diameter φC, and the optical function surface diameters φBu and φBd have a concave shape, as shown in FIG. When a glass material for molding whose both end surfaces are flat is used, the optical effective surface diameter φA of the upper and lower molds having the larger optically effective surface diameter, and the optical functional surface of the lower mold having the smaller optically functional surface diameter. The relationship among the diameter φB, the outer diameter φS of the glass material for molding, and the effective surface diameter φSS of the glass material for molding is φA <φSS ≦ φS
It is desirable that ≦ φB.
【0032】φSがφBより大きくなると、φSとφC
の間隔が小さくなり、変形量が十分でなく成形用ガラス
素材6の有効面径φSSと型の光学機能面径φBの間の
密閉空間の気体が抜けにくく、転写不良の生じる原因と
なる。When φS becomes larger than φB, φS and φC
Is small, the amount of deformation is not sufficient, and the gas in the closed space between the effective surface diameter φSS of the molding glass material 6 and the optically functional surface diameter φB of the mold is difficult to escape, which causes transfer failure.
【0033】しかし、図4(d)のような形状をした成
形用ガラス素材を用いた場合であれば、密閉空間は存在
しなくなるのでφA<φSS≦ φSの関係でも転写不
良が発生することは無い。However, if the glass material for molding having the shape as shown in FIG. 4 (d) is used, the sealed space will not exist, so that transfer failure will not occur even if φA <φSS ≦ φS. There is no.
【0034】(実施例2)図2は、本発明の第2の実施
例の説明図であり、成形用ガラス素材13を上下型8、
9間に保持した状態を示すものである。11、12は加
熱加圧機構を備えたプレスヘッドの一部である。(Embodiment 2) FIG. 2 is an explanatory view of the second embodiment of the present invention, in which a glass material 13 for molding is used for the upper and lower molds 8,
9 shows a state of being held for 9 seconds. Reference numerals 11 and 12 are parts of a press head provided with a heating / pressurizing mechanism.
【0035】上型8、下型9は、所望の光学性能が得ら
れるように凸形状に加工されている(従って、凹レンズ
が成形される)。上型8、下型9の光学機能面径φB
u、φBdは、胴型内径φCと同じ径φ8mmに、また
上型8の曲率半径は6mm、下型9の曲率半径は7.5
mmに加工されており、光学有効面径φAu、φAdは
それよりも小さく上型φ6.0mm、下型φ6.2mm
である。形状精度は上型8、下型9ともPV=λ/8以
下である。The upper mold 8 and the lower mold 9 are processed into convex shapes so that desired optical performance can be obtained (thus, concave lenses are molded). Optical function surface diameter φB of upper mold 8 and lower mold 9
u and φBd have the same diameter φ8 mm as the barrel die inner diameter φC, the radius of curvature of the upper die 8 is 6 mm, and the radius of curvature of the lower die 9 is 7.5.
mm, and the optical effective surface diameters φAu and φAd are smaller than that. Upper die φ6.0 mm, Lower die φ6.2 mm
Is. The shape precision is PV = λ / 8 or less for both the upper mold 8 and the lower mold 9.
【0036】成形用ガラス素材13の形状は、両端面と
もに平面で、この平面部分は光学ガラス素子と同等の面
粗度Rmax=0.01μm以下に仕上げられている
が、外周面は研削面であり、面粗度はRmax=約0.
2μmであり、、外径φSと有効面径φSSは等しく共
にφ7.1mmで作成してあり、本発明に規定の寸法関
係の範囲内である。The shape of the glass material for molding 13 is flat on both end surfaces, and the flat surface portion is finished to have a surface roughness Rmax = 0.01 μm or less equivalent to that of an optical glass element, but the outer peripheral surface is a ground surface. And the surface roughness is Rmax = approximately 0.
The diameter is 2 μm, the outer diameter φS and the effective surface diameter φSS are equal, and both are formed with φ7.1 mm, which is within the range of the dimensional relationship specified in the present invention.
【0037】成形して得られる光学ガラス素子の中心厚
は0.8mmで、成形用ガラス素材13の厚みは2.6
5mmとした。The center thickness of the optical glass element obtained by molding is 0.8 mm, and the thickness of the molding glass material 13 is 2.6.
It was set to 5 mm.
【0038】本実施例においては、第1の実施例と同様
な工程で光学ガラス素子を得る。本実施例では、成形用
ガラス素材13としてSF8(Tg=425℃)を用
い、成形温度は530℃、加圧力は200Kgf/cm
2、取り出し温度は420℃以下で行った。In this embodiment, an optical glass element is obtained by the same steps as in the first embodiment. In this embodiment, SF8 (Tg = 425 ° C.) is used as the glass material 13 for molding, the molding temperature is 530 ° C., and the pressure is 200 Kgf / cm.
2. The take-out temperature was 420 ° C. or lower.
【0039】その結果、得られた光学ガラス素子の形状
精度は上下面ともPV=λ/5以下を示し、型の精度を
良好に転写していた。As a result, the shape accuracy of the obtained optical glass element was PV = λ / 5 or less on both upper and lower surfaces, and the mold accuracy was excellently transferred.
【0040】また、図1(b)と同様に、故意に成形用
ガラス素材13を一方に偏らせた場合(言い換えれば、
成形用ガラス素材13と上型8、下型9に偏心が生じた
場合)でも、成形用ガラス素材13の有効面径φSS以
外の面が光学ガラス素子の光学有効面径φAu、φAd
に転写されることは無く、成形用ガラス素材13の有効
面径φSS内で光学ガラス素子の光学有効面径φAu、
φAdを形成した良好な光学性能の光学ガラス素子が成
形できた。Further, as in the case of FIG. 1B, when the glass material 13 for molding is intentionally biased to one side (in other words,
Even when the molding glass material 13 and the upper mold 8 and the lower mold 9 are decentered), the surfaces other than the effective surface diameter φSS of the molding glass material 13 are the optical effective surface diameters φAu and φAd of the optical glass element.
, The optical effective surface diameter φAu of the optical glass element within the effective surface diameter φSS of the molding glass material 13,
An optical glass element having good optical performance in which φAd was formed could be molded.
【0041】本実施例では、成形用ガラス素材13が一
方に偏り成形用ガラス素材13の外周面が胴型10の内
壁に接触した時、対向する側の成形用ガラス素材13の
外周面と胴型10の内壁との最大隙間は0.9mmであ
り、胴型10の内壁から下型9の光学有効面径φAdま
での距離0.9mmと同じである。In this embodiment, when the forming glass material 13 is biased to one side and the outer peripheral surface of the forming glass material 13 comes into contact with the inner wall of the barrel mold 10, the outer peripheral surface of the forming glass material 13 on the opposite side and the body. The maximum gap with the inner wall of the mold 10 is 0.9 mm, which is the same as the distance 0.9 mm from the inner wall of the barrel mold 10 to the optically effective surface diameter φAd of the lower mold 9.
【0042】一方、押圧成形することにより、成形前の
成形用ガラス素材の有効面径φSSは大きく広がること
が確認されており、従って本実施例において光学ガラス
素子の光学有効面に成形用ガラス素材13の有効面以外
の面(外周面)が回り込むことはない。On the other hand, it has been confirmed that the effective surface diameter φSS of the glass material for molding before molding is largely expanded by the press molding. Therefore, in this embodiment, the glass material for molding is formed on the optically effective surface of the optical glass element. The surface (outer peripheral surface) other than the effective surface of 13 does not go around.
【0043】(実施例3)図3は、本発明の第3の実施
例を示すもので、成形用ガラス素材19を上下型14、
15間に保持した状態を示す。16は胴型、19は成形
用ガラス素材、17、18は加熱加圧機構を備えたプレ
スヘッドの一部である。(Embodiment 3) FIG. 3 shows a third embodiment of the present invention.
The state of being held between 15 is shown. Reference numeral 16 is a barrel mold, 19 is a glass material for molding, and 17 and 18 are parts of a press head having a heating and pressing mechanism.
【0044】上型14は曲率半径8.0mmの凸形状に
加工されている。上型14の光学機能面径φBuは胴型
16の内径φCと同じφ13mmで、光学有効面径φA
uはφ8.24mmである。The upper mold 14 is processed into a convex shape having a radius of curvature of 8.0 mm. The optical functional surface diameter φBu of the upper die 14 is 13 mm which is the same as the inner diameter φC of the barrel die 16, and the optically effective surface diameter φA.
u is φ8.24 mm.
【0045】下型15の光学機能面径φBdはφ12m
mで、光学有効面径φAdはφ10.8mm、曲率半径
は40.0mmである。形状精度は上型14、下型15
ともPV=λ/8以下である。The optical functional surface diameter φBd of the lower mold 15 is φ12 m.
m, the optically effective surface diameter φAd is φ10.8 mm, and the radius of curvature is 40.0 mm. Shape accuracy is upper mold 14, lower mold 15
Both are PV = λ / 8 or less.
【0046】成形用ガラス素材19の形状は、両端面と
もに平面の円板形状で、この平面部は光学ガラス素子と
同等の面粗度Rmax=0.01μm以下に仕上げられ
ているが、外周面は面粗度がRmax=0.8μm程度
の研削面である。また、外径φSと有効面径φSSは等
しくφ11.9mmで作成してあり、本発明に規定の寸
法関係を満たしている。光学ガラス素子の中心厚1.2
mmを得るため、成形用ガラス素材19の厚みは2.9
3mmとした。The shape of the glass material for molding 19 is a disk shape with both end surfaces being flat, and this flat surface portion is finished to have a surface roughness Rmax = 0.01 μm or less equivalent to that of an optical glass element, but the outer peripheral surface. Is a ground surface having a surface roughness of Rmax = 0.8 μm. Further, the outer diameter φS and the effective surface diameter φSS are made equal to each other by φ11.9 mm, which satisfies the dimensional relationship prescribed in the present invention. Center thickness of optical glass element 1.2
In order to obtain mm, the thickness of the glass material for molding 19 is 2.9.
It was 3 mm.
【0047】第1の実施例と同様な工程で光学ガラス素
子を得た。光学ガラス素子の形状精度は上下面ともPV
=λ/4以下を示し、型精度を良好に転写していた。An optical glass element was obtained by the same steps as in the first example. The shape accuracy of the optical glass element is PV on both the upper and lower surfaces.
= Λ / 4 or less, and the mold precision was transferred well.
【0048】さらに図4(b)、(c)に示す外周面と
有効面をC面、R面で連結した形状を有する成形用ガラ
ス素材を作成した。いずれも外径φSはφ12mm、面
取り部分は0.1mm(それぞれC0.1mm、R0.
1mm)とし、有効面径φSSはφ11.8mm、厚み
は2.88mm、有効面径の面粗度はRmax=0.0
1μm以下、有効面以外の面粗度はRmax=3μmで
ある。Further, a glass material for molding having a shape in which the outer peripheral surface and the effective surface shown in FIGS. 4 (b) and 4 (c) were connected by the C surface and the R surface was prepared. In both cases, the outer diameter φS is φ12 mm, and the chamfered portion is 0.1 mm (C0.1 mm, R0.
1 mm), the effective surface diameter φSS is φ11.8 mm, the thickness is 2.88 mm, and the surface roughness of the effective surface diameter is Rmax = 0.0.
The surface roughness is 1 μm or less, and the surface roughness other than the effective surface is Rmax = 3 μm.
【0049】また図4(d)に示す成形用ガラス素材を
作成したが、これは、両凸Rの形状で、外径φSと有効
面径φSSは等しくφ11.95mm、曲率半径は両面
とも38.0mm、中心厚3.37mmである。Further, a glass material for molding shown in FIG. 4 (d) was prepared, which has a biconvex R shape, and the outer diameter φS and the effective surface diameter φSS are equal to each other and the radius of curvature is 38 mm on both sides. The thickness is 0.0 mm and the center thickness is 3.37 mm.
【0050】これらの成形用ガラス素材について同様に
成形を行った。いずれの形状の光学用ガラス素材も本発
明に規定の寸法関係を満たしており、故意に成形用ガラ
ス素材を片方に偏らせた場合でも、成形用ガラス素材の
有効面以外の面が光学ガラス素子の光学有効面に回り込
んで転写されることは無く、成形用ガラス素材の有効面
径φSS内で光学ガラス素子の光学有効面を形成した良
好な光学性能の光学ガラス素子を得ることができた。Molding was performed in the same manner for these glass materials for molding. The optical glass material of any shape satisfies the dimensional relationship specified in the present invention, and even if the molding glass material is intentionally biased to one side, the surface other than the effective surface of the molding glass material is an optical glass element. It was possible to obtain an optical glass element having good optical performance in which the optical effective surface of the optical glass element was formed within the effective surface diameter φSS of the molding glass material without being transferred to the optical effective surface of .
【0051】尚、本実施例で挙げた成形用ガラス素材以
外の形状においても、本発明に規定の関係を満たしてい
れば良好な転写面を有した光学ガラス素子が得られるこ
とは言うまでもない。It is needless to say that an optical glass element having a good transfer surface can be obtained even if the shape other than the glass material for molding mentioned in this embodiment satisfies the relationship prescribed in the present invention.
【0052】例えば、図4(c)の様にR面取りをした
形状において、R面取り部を鏡面加工し、有効面部φS
Sを外径φSと同一径にしても問題無い。また、成形後
に胴型内径で規制された光学ガラス素子の外径を心取り
加工等を施して光学ガラス素子として用いても何等問題
はない。For example, as shown in FIG. 4 (c), in the shape with R chamfering, the R chamfered portion is mirror-finished to obtain an effective surface portion φS.
There is no problem even if S has the same diameter as the outer diameter φS. Further, there is no problem even if the outer diameter of the optical glass element, which is regulated by the inner diameter of the barrel mold, is subjected to centering processing or the like after molding and used as the optical glass element.
【0053】[0053]
【発明の効果】本発明によれば、成形用ガラス素材と上
下型に偏心が生じた場合でも、成形用ガラス素材の有効
面以外の面が光学ガラス素子の光学有効面に回り込むこ
とがなく、成形用ガラス素材の有効面のみで光学ガラス
素子の光学有効面が形成できる。According to the present invention, even when eccentricity occurs between the molding glass material and the upper and lower molds, a surface other than the effective surface of the molding glass material does not wrap around the optical effective surface of the optical glass element. The optical effective surface of the optical glass element can be formed only by the effective surface of the glass material for molding.
【0054】このため、成形用ガラス素材の有効面以外
の面を有効面と同様な面粗度に加工していない成形用ガ
ラス素材を用いることが可能となり成形用ガラス素材が
安価になる。For this reason, it becomes possible to use a glass material for molding in which the surfaces other than the effective surface of the glass material for molding are not processed to the same surface roughness as the effective surface, and the glass material for molding becomes inexpensive.
【0055】また、偏心を防止するための成形用ガラス
素材の位置決め装置なども必要なく工程が容易になり、
さらには光学ガラス素子の低価格化が可能となる。Further, since a molding glass material positioning device for preventing eccentricity is not required, the process is simplified,
Further, the cost of the optical glass element can be reduced.
【図1】本発明の第1実施例の説明図FIG. 1 is an explanatory diagram of a first embodiment of the present invention.
【図2】本発明の第2実施例の説明図FIG. 2 is an explanatory diagram of a second embodiment of the present invention.
【図3】本発明の第3実施例の説明図FIG. 3 is an explanatory diagram of a third embodiment of the present invention.
【図4】本発明の成形用ガラス素材の実施例を示す断面
図FIG. 4 is a sectional view showing an example of the glass material for molding of the present invention.
【図5】従来の光学ガラス素子の成形技術の説明図FIG. 5 is an explanatory view of a conventional molding technique for an optical glass element.
1 上型 2 下型 3 胴型 4 加熱加圧機構を有するプレスヘッドの一部 5 加熱加圧機構を有するプレスヘッドの一部 6 成形用ガラス素材 7 光学ガラス素子 8 上型 9 下型 10 胴型 11 加熱加圧機構を有するプレスヘッドの一部 12 加熱加圧機構を有するプレスヘッドの一部 13 成形用ガラス素材 14 上型 15 下型 16 胴型 17 加熱加圧機構を有するプレスヘッドの一部 18 加熱加圧機構を有するプレスヘッドの一部 19 成形用ガラス素材 20 上型 21 下型 22 胴型 23 加熱加圧機構を有するプレスヘッドの一部 24 加熱加圧機構を有するプレスヘッドの一部 25 光学ガラス素子 1 Upper mold 2 Lower mold 3 Body mold 4 Part of press head having heating / pressurizing mechanism 5 Part of press head having heat / pressurizing mechanism 6 Glass material for molding 7 Optical glass element 8 Upper mold 9 Lower mold 10 Body Mold 11 Part of a press head having a heating and pressing mechanism 12 Part of a press head having a heating and pressing mechanism 13 Glass material for molding 14 Upper mold 15 Lower mold 16 Body mold 17 One of press heads having a heating and pressing mechanism Part 18 Part of a press head having a heating and pressing mechanism 19 Glass material for molding 20 Upper mold 21 Lower mold 22 Body 23 A part of a press head having a heating and pressing mechanism 24 A press head having a heating and pressing mechanism Part 25 Optical glass element
フロントページの続き (72)発明者 春原 正明 大阪府門真市大字門真1006番地 松下電器 産業株式会社内 (72)発明者 片岡 秀直 大阪府門真市大字門真1006番地 松下電器 産業株式会社内Front page continuation (72) Inventor Masaaki Sunohara 1006 Kadoma, Kadoma City, Osaka Prefecture Matsushita Electric Industrial Co., Ltd.
Claims (4)
型の光学有効面径をφA、胴型内径をφC、成形用ガラ
ス素材の外径をφS、成形用ガラス素材の有効面径をφ
SSとした時、それらの関係が、φA<φSS≦φSで
あり、かつ、φC−[φS−{(φS−φSS)/
2}]≦(φC−φA)/2であることを特徴とする成
形用ガラス素材。1. An optical effective surface diameter of a mold having a larger optical effective surface diameter of a pair of upper and lower molds is φA, an inner diameter of a barrel mold is φC, an outer diameter of a molding glass material is φS, and an effective surface diameter of a molding glass material. Φ
When SS, the relation between them is φA <φSS ≦ φS, and φC− [φS − {(φS−φSS) /
2}] ≦ (φC−φA) / 2, a glass material for molding.
型の光学有効面径をφAとし、前述の上下型のうち光学
機能面径の小さい型の光学機能面径をφB、成形用ガラ
ス素材の外径をφS、成形用ガラス素材の有効面径をφ
SSとした時、φA<φSS≦φS≦φBであることを
特徴とする請求項1記載の成形用ガラス素材。2. A mold having a larger optical effective surface diameter of the pair of upper and lower molds has an optical effective surface diameter of φA, and a mold having a smaller optical functional surface diameter of the above-mentioned upper and lower molds has an optical functional surface diameter of φB. The outer diameter of the glass material is φS, and the effective surface diameter of the glass material for molding is φ
The glass material for molding according to claim 1, wherein, when SS, φA <φSS ≦ φS ≦ φB.
型の光学有効面径をφA、胴型内径をφC、成形用ガラ
ス素材の外径をφS、成形用ガラス素材の有効面径をφ
SSとした時、それらの関係が、φA<φSS≦φSで
あり、かつ、φC−[φS−{(φS−φSS)/
2}]≦(φC−φA)/2である成形用ガラス素材を
上下型間に型の光学有効面と成形用ガラス素材の有効面
とが対向するように供給し、前記成形用ガラス素材を軟
化点近傍の温度まで加熱し、上型、下型により押圧成形
を行い、その後、光学ガラス素子がガラス転移点近傍の
温度になるまで冷却した後、光学ガラス素子を取り出す
ことを特徴とする光学ガラス素子の製造方法。3. An optical effective surface diameter of a mold having a larger optical effective surface diameter of a pair of upper and lower molds is φA, an inner diameter of a barrel mold is φC, an outer diameter of a glass material for molding is φS, and an effective surface diameter of a glass material for molding is Φ
When SS, the relation between them is φA <φSS ≦ φS, and φC− [φS − {(φS−φSS) /
2}] ≦ (φC−φA) / 2 is supplied so that the optical effective surface of the mold and the effective surface of the molding glass material face each other between the upper and lower molds, and the molding glass material is An optical device characterized by heating to a temperature near the softening point, press-molding with an upper mold and a lower mold, then cooling the optical glass element to a temperature near the glass transition point, and then taking out the optical glass element. Method for manufacturing glass element.
型の光学有効面径をφA、前述の上下型のうち光学機能
面径の小さい型の光学機能面径をφB、成形用ガラス素
材の外径をφS、成形用ガラス素材の有効面径をφSS
とした時、φA<φSS≦φS≦φBである成形用ガラ
ス素材を用いることを特徴とする請求項3記載の光学ガ
ラス素子の製造方法。4. A molding glass having an optical effective surface diameter of a mold having a larger optical effective surface diameter of a pair of upper and lower molds, and an optical functional surface diameter of a mold having a smaller optical functional surface diameter of the aforesaid upper and lower molds, φB. The outer diameter of the material is φS, the effective surface diameter of the glass material for molding is φSS
4. The method for producing an optical glass element according to claim 3, wherein a glass material for molding with φA <φSS ≦ φS ≦ φB is used.
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