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    • 6. 发明授权
    • Antireflection film and optical element coated with the antireflection film
    • 防反射膜和涂有抗反射膜的光学元件
    • US06396626B1
    • 2002-05-28
    • US09654040
    • 2000-09-01
    • Minoru OtaniKenji AndoYasuyuki SuzukiRyuji BiroHidehiro Kanazawa
    • Minoru OtaniKenji AndoYasuyuki SuzukiRyuji BiroHidehiro Kanazawa
    • F21V904
    • G02B1/115
    • The antireflection film of the present invention comprises an alternately multi-layered film of 10 layers formed on a base member and having antireflection characteristics in two wavelength regions including a first wavelength (&lgr;1) of 248 nm and a second wavelength (&lgr;2) of 633 nm as central wavelengths, respectively, the multi-layered film of 10 layers comprising: low-refractive index layers arranged at odd-numbered positions from a side opposite to the base member and having a refractive index of 1.45 to 1.52 at the first wavelength (&lgr;1); and high-refractive index layers arranged at even-numbered positions from the side opposite to the base member and having a refractive index of 1.65 to 1.80 at the first wavelength (&lgr;1), wherein layers arranged at the first, second and third positions from the side opposite to the base member each have an optical thickness ranging from 0.21&lgr;1 to 0.28&lgr;1.
    • 本发明的抗反射膜包括在基体上形成的具有抗反射特性的10层的交替层叠的膜,其包括248nm的第一波长(lambd1)和633nm的第二波长(lambd2)的两个波长区域 作为中心波长的10层的多层膜包括:从与基底构件相反的一侧排列在奇数位置的折射率低的第一波长的折射率为1.45〜1.52的低折射率层(lambd1 ); 以及高折射率层,其从与所述基底构件相反的一侧布置在偶数位置处,并且在所述第一波长(lambd1)处具有1.65至1.80的折射率,其中从所述第一波长 与基底构件相对的一侧的光学厚度各自具有从0.21lambd1到0.28lambd1的光学厚度。
    • 7. 发明授权
    • Anti-reflection film and optical system using the same
    • 防反射膜和使用其的光学系统
    • US5885712A
    • 1999-03-23
    • US822469
    • 1997-03-21
    • Minoru OtaniKenji AndoYasuyuki SuzukiRyuji BiroHidehiro Kanazawa
    • Minoru OtaniKenji AndoYasuyuki SuzukiRyuji BiroHidehiro Kanazawa
    • G02B1/11B32B7/02C03C17/34B32B17/06
    • C03C17/3417C03C17/3452
    • An anti-reflection film is arranged by alternately stacking a plurality of high-refractive index layers containing Al.sub.2 O.sub.3 and a plurality of low-refractive index layers containing SiO.sub.2 on a transparent substrate in turn from the substrate side to the air side, and satisfies:1.45.ltoreq.ns.ltoreq.1.651.60.ltoreq.na.ltoreq.1.850.31.lambda.0.ltoreq.d1.ltoreq.0.42.lambda.00.38.lambda.0.ltoreq.d2.ltoreq.0.45.lambda.00.20.lambda.0.ltoreq.d3.ltoreq.0.31.lambda.00.18.lambda.0.ltoreq.d4.ltoreq.0.28.lambda.00.20.lambda.0.ltoreq.d5.ltoreq.0.30.lambda.00.20.lambda.0.ltoreq.d6.ltoreq.0.30.lambda.0where ns and na are the refractive indices of the low-refractive index layer and the high-refractive index layer for light components falling with the wavelength range from 190 nm to 250 nm, di (unit: nm) is the optical film thickness of the i-th layer when the high- and low-refractive index layers are counted from the substrate side to the air side, and .lambda.0 (nm) is the reference wavelength within the wavelength range from 190 nm to 250 nm.
    • 通过在透明基板上从基板侧至空气侧交替层叠多个含有Al 2 O 3和多个含有SiO 2的低折射率层的高折射率层,并且满足:1.45 0.30λ0其中ns和na是 di(单位:nm)的波长范围为190nm至250nm的光成分的低折射率层和高折射率层的折射率为di(单位:nm)时的第i层的光学膜厚度, 从基板侧向空气侧计数高折射率层和低折射率层,λ0(nm)是在190nm〜250nm的波长范围内的基准波长。
    • 10. 发明申请
    • MULTILAYER FILM REFLECTOR
    • 多层膜反射器
    • US20090252977A1
    • 2009-10-08
    • US12416544
    • 2009-04-01
    • Seiken MatsumotoKenji AndoHidehiro KanazawaKoji TeranishiTakayuki MiuraKyoko Nagata
    • Seiken MatsumotoKenji AndoHidehiro KanazawaKoji TeranishiTakayuki MiuraKyoko Nagata
    • B32B15/04
    • B82Y10/00G02B5/0891G21K1/062G21K2201/067
    • A stress distribution resulting from variation in in-plane film quality of a stress relaxation layer and a reflective layer is eliminated. A reflective layer is stacked on a substrate via a stress relaxation layer. The stress relaxation layer has a stress relaxation portion having a uniform film thickness distribution to cancel the internal stress of the reflective layer, and a stress distribution eliminating portion with a film thickness distribution approximated to a second order even function. The stress is substantially proportional to the film thickness. Thus, formation of a given film thickness distribution allows the stress distribution to be controlled. However, changing the film thickness distribution based on a design value may degrade the optical characteristics. Thus, the film thickness distribution of the stress distribution eliminating portion, which serves to eliminate the stress distribution, is approximated to the second order even function. This enables aberration associated with the film thickness distribution to be reduced by adjusting an optical system.
    • 消除了由应力松弛层和反射层的面内膜质量的变化引起的应力分布。 反射层通过应力松弛层堆叠在基板上。 应力缓和层具有均匀的薄膜厚度分布的应力松弛部,以抵消反射层的内部应力,以及具有近似于二次偶次函数的膜厚分布的应力分布消除部。 应力基本上与膜厚成正比。 因此,形成给定的膜厚度分布允许控制应力分布。 然而,基于设计值改变膜厚度分布可能降低光学特性。 因此,用于消除应力分布的应力分布消除部分的膜厚度分布近似于二阶偶函数。 通过调整光学系统,能够降低与膜厚分布有关的像差。