TWI383173B - Film stacked structure - Google Patents
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Description
本發明涉及一種膜堆結構,尤指一種應用於分光棱鏡上之膜堆結構。 The invention relates to a membrane stack structure, in particular to a membrane stack structure applied to a beam splitting prism.
目前,光學鍍膜已經被廣泛地運用於投影機、傳統相機、數碼相機、手機、天文望遠鏡所用之鏡頭組、濾光片等,用來使得這些光學元件能夠實現不同之光學功能,例如:吸收紫外線、減反射、彩色濾光、紅外光截止等。 At present, optical coatings have been widely used in projectors, conventional cameras, digital cameras, mobile phones, lens sets used in astronomical telescopes, filters, etc., to enable these optical components to achieve different optical functions, such as: UV absorption , anti-reflection, color filter, infrared cut-off, etc.
如圖1所示,本發明涉及一種應用於分光棱鏡1中之膜堆結構2。該分光棱鏡1用於各種光學儀器之顏色分離系統。外界光線進入分光棱鏡1後以45度角入射到鍍有膜堆結構2之表面3上,在透射波長範圍內之光線透過該膜堆結構2由分光棱鏡1之上表面4射出,在反射波長範圍內之光線被該膜堆結構2反射由分光棱鏡1之側面5射出從而達到分光濾波之效果。 As shown in FIG. 1, the present invention relates to a film stack structure 2 applied to a beam splitting prism 1. The dichroic prism 1 is used in a color separation system of various optical instruments. After the external light enters the dichroic prism 1, it is incident on the surface 3 coated with the film stack structure 2 at an angle of 45 degrees, and the light in the transmission wavelength range is transmitted through the film stack structure 2 from the upper surface 4 of the beam splitting prism 1 at the reflection wavelength. The light in the range is reflected by the film stack structure 2 and is emitted from the side surface 5 of the beam splitting prism 1 to achieve the effect of spectral filtering.
現有之膜堆結構2通常使用高、低折射率材料交互層疊之週期性結構。該膜堆結構2可表示為(HL) n ,其中,H代表高折射率膜層,L代表低折射率膜層。H和L前面之係數之比表示各自折射率膜層之光學厚度比,該光學厚度之物理意義為膜層物理厚度與膜層折射率之乘積,光學厚度1等於參考波長之1/4。上標n表示(HL) n 結構之週期數。該高折射率材料之折射率大於2.1而低折射率材料 之折射率低於1.5。 Existing membrane stack structures 2 typically use a periodic structure in which high and low refractive index materials are alternately laminated. The film stack structure 2 can be represented by ( HL ) n , where H represents a high refractive index film layer and L represents a low refractive index film layer. The ratio of the coefficients of the front of H and L represents the optical thickness ratio of the respective refractive index film layers, the physical meaning of which is the product of the physical thickness of the film layer and the refractive index of the film layer, and the optical thickness 1 is equal to 1/4 of the reference wavelength. The superscript n represents the number of cycles of the ( HL ) n structure. The high refractive index material has a refractive index greater than 2.1 and the low refractive index material has a refractive index less than 1.5.
如圖2所示,其為參考波長為550nm,入射角為45度時週期數為18之膜堆結構2(HL)18之透射光譜圖。其中,實線為自然光之透射光譜線,虛線為平行偏振光(P-Polarized)之透射光譜線,點劃線為垂直偏振光(S-Polarized)之透射光譜線。該垂直偏振光為線偏振光,其偏振面垂直於由濾光片表面法線和入射光線所決定之平面。該平行偏振光為線偏振光,其偏振面平行於垂直偏振光之偏振面。自然光可看成係振幅相同之平行偏振光(P-Polarized)與垂直偏振光(S-Polarized)之疊加。因為波長相同之垂直偏振光與平行偏振光對於同一種材料所呈現之折射率不同,所以會導致透過該膜堆結構2(HL)18之平行偏振光譜特性與垂直偏振光譜特性產生偏移,即圖2中之虛曲線和點劃線在波長方向上出現平移,該平行偏振光透射光譜線之半值波長(透過率為50%時所對應之波長)與垂直偏振光透射光譜線之半值波長相差70nm以上。此時,混合後自然光之透射光譜線會在半值波長處出現非線性之不平滑部分影響了分光濾波之效果。 As shown in FIG. 2, it is a transmission spectrum diagram of a membrane stack structure 2 ( HL ) 18 having a reference wavelength of 550 nm and an angle of incidence of 45 degrees. The solid line is the transmission spectrum line of natural light, the broken line is the transmission spectrum line of parallel polarized light (P-Polarized), and the dotted line is the transmission spectrum line of S-Polarized. The vertically polarized light is linearly polarized light having a plane of polarization perpendicular to a plane defined by the normal to the surface of the filter and the incident ray. The parallel polarized light is linearly polarized light whose plane of polarization is parallel to the plane of polarization of the vertically polarized light. Natural light can be seen as a superposition of parallel polarized light (P-Polarized) and vertically polarized light (S-Polarized). Since the vertically polarized light of the same wavelength and the parallel polarized light exhibit different refractive indices for the same material, the parallel polarization spectral characteristics and the vertical polarization spectral characteristics transmitted through the film stack structure 2 ( HL ) 18 are shifted, that is, The dashed curve and the dotted line in Fig. 2 show a shift in the wavelength direction, and the parallel polarized light transmits the half value wavelength of the spectral line (the wavelength corresponding to the transmittance of 50%) and the half value of the vertical polarized light transmission spectral line. The wavelengths differ by 70 nm or more. At this time, the non-smooth part of the transmission spectrum line of the natural light after mixing at the half-value wavelength affects the effect of the spectral filtering.
因為光學系統中之光源所發出之平行光通常存在一定之角度誤差,所以分光濾波膜堆之透射光譜特性隨入射光線角度之變化情況也成為考察分光濾波膜堆品質好壞之標準之一。 Because the parallel light emitted by the light source in the optical system usually has a certain angular error, the variation of the transmission spectral characteristics of the spectral filter film stack with the incident light angle has become one of the criteria for examining the quality of the spectral filter film stack.
現以入射角分別為53度和37度為例,考察該膜堆結構2 (HL)18之透射光譜特性隨入射光線角度之變化情況。如圖3、圖4所示,其中,實線為自然光之透射光譜線,虛線為平行偏振光之透射光譜線,點劃線為垂直偏振光之透射光譜線。從圖3中可知,當入射角度較大(入射角為53度)時,該膜堆結構2(HL)18之自然光透射光譜線之非線性不平滑部分更為明顯,而且反射波長範圍之反射率也降低許多。從圖3和圖4之對比中可發現,該膜堆結構2之透射光譜特性隨角度變化明顯,若以透過率為30%時所對應之波長做比較,入射角為53度時之自然光透射光譜線與入射角為37度時之自然光透射光譜線相差80nm。 Taking the incident angles of 53 degrees and 37 degrees as examples, the variation of the transmission spectrum characteristics of the film structure 2 ( HL ) 18 with the angle of incident light is investigated. As shown in FIG. 3 and FIG. 4 , the solid line is the transmission spectrum line of natural light, the broken line is the transmission spectrum line of parallel polarized light, and the dotted line is the transmission spectrum line of the vertically polarized light. As can be seen from Fig. 3, when the incident angle is large (incident angle is 53 degrees), the nonlinear non-smooth portion of the natural light transmission spectral line of the stack structure 2 ( HL ) 18 is more pronounced, and the reflection wavelength range is reflected. The rate is also much lower. From the comparison of Fig. 3 and Fig. 4, it can be found that the transmission spectrum characteristic of the film stack structure 2 changes significantly with the angle. If the wavelength corresponding to the transmittance is 30%, the natural light transmission when the incident angle is 53 degrees is observed. The spectral line differs from the natural light transmission spectral line at an incident angle of 37 degrees by 80 nm.
綜上所述,現有之膜堆結構2(HL)18因高、低折射率材料之折射率存在較大差異從而導致其出現分光濾波之效果較差,透射光譜特性隨角度變化明顯以及在大角度入射時反射波段之反射率下降等缺點。 In summary, the existing membrane stack structure 2 ( HL ) 18 has a poor difference in refractive index of the high and low refractive index materials, resulting in poor spectral filtering effect, and the transmission spectral characteristics vary significantly with angle and at large angles. Disadvantages such as a decrease in the reflectance of the reflection band at the time of incidence.
有鑒於此,有必要提供具有較理想分光濾波效果之膜堆結構。 In view of this, it is necessary to provide a film stack structure having a better spectral filtering effect.
一種膜堆結構,該膜堆結構包括一個透明基底和疊於其上之週期性膜堆。該週期性膜堆之週期性結構為交互層疊之高折射率膜層和中間折射率膜層,該中間折射率膜層之折射率範圍為1.71至1.79或1.81至1.86。 A membrane stack structure comprising a transparent substrate and a periodic membrane stack superposed thereon. The periodic structure of the periodic film stack is an alternately laminated high refractive index film layer and an intermediate refractive index film layer having a refractive index ranging from 1.71 to 1.79 or 1.81 to 1.86.
相較於先前之技術,該膜堆結構採用了中間折射率膜層 代替現有之膜堆結構中之低折射率膜層,減少了週期性膜堆結構中兩種折射率膜層之間之折射率差值,縮短了透射垂直偏振光譜和透射平行偏振光譜之差距,達到改善分光濾波鏡之透射光譜特性之目之。 Compared to the prior art, the membrane stack structure uses an intermediate refractive index film layer Replacing the low refractive index film layer in the existing film stack structure, the refractive index difference between the two refractive index film layers in the periodic film stack structure is reduced, and the difference between the transmission vertical polarization spectrum and the transmission parallel polarization spectrum is shortened. The purpose of improving the transmission spectrum characteristics of the spectroscopic filter is achieved.
請參閱圖5,其為本發明所提供之膜堆結構10示意圖。該膜堆結構10包括透明基底102和疊於其上之週期性膜堆104。該週期性膜堆104之週期性結構為交互層疊之高折射率膜層106和中間折射率層108。該週期性膜堆104之週期性結構可表示為(HM) n ,其中,H代表一個高折射率膜層106,M代表一個中間折射率膜層104,H和M前面之係數之比代表各折射率膜層之光學厚度比,上標n表示該週期性結構之週期數。 Please refer to FIG. 5 , which is a schematic diagram of a membrane stack structure 10 provided by the present invention. The film stack structure 10 includes a transparent substrate 102 and a periodic film stack 104 stacked thereon. The periodic structure of the periodic film stack 104 is an alternating layer of the high refractive index film layer 106 and the intermediate refractive index layer 108. The periodic structure of the periodic film stack 104 can be expressed as ( HM ) n , where H represents a high refractive index film layer 106, M represents an intermediate refractive index film layer 104, and the ratio of coefficients in front of H and M represents each The optical thickness ratio of the refractive index film layer, the superscript n indicates the number of cycles of the periodic structure.
該週期性膜堆104(HM) n 之高折射率膜層106和中間折射率膜層108之光學厚度相同。該週期性膜堆104(HM) n 之週期數根據需要透射和反射之波長範圍而設定。於本實施例中,該週期性膜堆104(HM) n 之週期數為18,其透射之波長範圍為480nm至670nm,反射之波長範圍為400nm至440nm。 The high refractive index film layer 106 and the intermediate refractive index film layer 108 of the periodic film stack 104 ( HM ) n have the same optical thickness. The number of cycles of the periodic film stack 104 ( HM ) n is set according to the wavelength range in which transmission and reflection are required. In this embodiment, the periodic film stack 104 ( HM ) n has a period of 18, a wavelength range of 480 nm to 670 nm, and a wavelength range of 400 nm to 440 nm.
該透明基底102之材料可為透明玻璃或塑膠材質,如無色高度透明之冕玻璃(B270)或者青板玻璃。高折射率膜層106之折射率大於2.1,其材料可為二氧化鈦、五氧化二鉭和五氧化二鈮中之一種。中間折射率膜層108之折射 率範圍為1.71至1.79或1.81至1.86,其材料可為德國默克公司生產之中間折射率材料M2或M3。除了本實施方式所提到之材料外,其他能滿足各膜層折射率要求之材料也可採用,各膜層通過物理氣相沉積之方法制得。 The material of the transparent substrate 102 can be a transparent glass or plastic material, such as a colorless and highly transparent bismuth glass (B270) or a slate glass. The high refractive index film layer 106 has a refractive index greater than 2.1, and the material thereof may be one of titanium dioxide, tantalum pentoxide, and tantalum pentoxide. Refraction of the intermediate refractive index film layer 108 The rate ranges from 1.71 to 1.79 or from 1.81 to 1.86, and the material may be the intermediate refractive index material M2 or M3 produced by Merck & Co., Germany. In addition to the materials mentioned in the present embodiment, other materials which can satisfy the refractive index requirements of the respective film layers can be used, and each film layer is obtained by a physical vapor deposition method.
請參閱圖6,其為週期性膜堆104(HM)18在參考波長為475nm,入射角為45度條件下之透射光譜圖。其中,實線為自然光之透射光譜線,虛線為平行偏振光之透射光譜線,點劃線為垂直偏振光之透射光譜線。對比圖6與圖2可知該週期性膜堆104(HM)18透射之平行偏正光譜線與垂直偏振光譜線之半值波長差值僅為40nm。相較於現有膜堆結構2(HL)18,本發明提供之週期性膜堆104(HM)18大大地減少了平行偏振光譜線和垂直偏振光譜線之偏移效應,使得透過該週期性膜堆104(HM)18之自然光之光譜特性在半值波長處之非線性不平滑部分得到較大之改善,提高了該週期性膜堆104(HM)18之分光濾波效果。 Please refer to FIG. 6 , which is a transmission spectrum diagram of the periodic film stack 104 ( HM ) 18 at a reference wavelength of 475 nm and an incident angle of 45 degrees. The solid line is the transmission spectrum line of natural light, the broken line is the transmission spectrum line of parallel polarized light, and the dotted line is the transmission spectrum line of vertically polarized light. Comparing FIG. 6 with FIG. 2, it can be seen that the half-value wavelength difference between the parallel positive polarization spectrum and the vertical polarization spectral line transmitted by the periodic film stack 104 ( HM ) 18 is only 40 nm. Compared to the prior art stack structure 2 ( HL ) 18 , the periodic film stack 104 ( HM ) 18 provided by the present invention greatly reduces the offset effect of the parallel polarization spectral line and the vertical polarization spectral line, so that the periodic film is transmitted through the periodic film. The spectral characteristics of the natural light of the stack 104 ( HM ) 18 are greatly improved at the half-value wavelength, and the spectral filtering effect of the periodic film stack 104 ( HM ) 18 is improved.
請參閱圖7和圖8,其為本發明提供之週期性膜堆104(HM)18在參考波長為475nm,入射角分別為53度和37度條件下之透射光譜圖。其中,實線為自然光之透射光譜線,虛線為平行偏振光之透射光譜線,點劃線為垂直偏振光之透射光譜線。對比圖7和圖3可知,本發明提供之週期性膜堆104(HM)18在較大入射角(入射角為53 度)時平行偏振光與垂直偏振光透射光譜之偏移情況相較於現有膜堆2(HL)18有了較大之改善。其次,在反射波長範圍內,本發明提供之週期性膜104(HM)18依然能保持較高之反射率有效地改善了現有膜堆2(HL)18在較大入射角時反射波長範圍內反射率升高之問題。對比圖7、圖8、圖3與圖4可知,本發明提供之週期性膜堆104(HM)18在入射角為37度時之平行偏振光與垂直偏振光透射光譜之偏移情況相較於現有膜堆2(HL)18有了較大之改善,且在入射角度由37至53之變化範圍內,本發明提供之週期性膜堆104(HM)18之透射光譜特性隨入射角度之變化較小,可較大之入射角範圍獲得較好之透射光譜特性。 Please refer to FIG. 7 and FIG. 8 , which are transmission spectrum diagrams of the periodic film stack 104 ( HM ) 18 provided by the present invention at a reference wavelength of 475 nm and incident angles of 53 degrees and 37 degrees, respectively. The solid line is the transmission spectrum line of natural light, the broken line is the transmission spectrum line of parallel polarized light, and the dotted line is the transmission spectrum line of vertically polarized light. 7 and FIG. 3, the periodic film stack 104 ( HM ) 18 provided by the present invention is compared with the shift of the parallel polarized light and the vertical polarized light transmission spectrum at a large incident angle (incident angle of 53 degrees). The existing membrane stack 2 ( HL ) 18 has been greatly improved. Secondly, in the reflection wavelength range, the periodic film 104 ( HM ) 18 provided by the present invention can still maintain a high reflectivity and effectively improve the reflection wavelength range of the existing film stack 2 ( HL ) 18 at a large incident angle. The problem of increased reflectivity. 7 , FIG. 8 , FIG. 3 and FIG. 4 , the periodic film stack 104 ( HM ) 18 provided by the present invention has a shift of parallel polarized light and a vertically polarized light transmission spectrum at an incident angle of 37 degrees. The existing film stack 2 ( HL ) 18 has a large improvement, and the transmission spectrum characteristic of the periodic film stack 104 ( HM ) 18 provided by the present invention varies with the incident angle in the range of the incident angle from 37 to 53. The change is small, and a better transmission spectrum characteristic can be obtained with a larger incident angle range.
相較於現有之技術,本發明提供之週期性膜堆(HM) n 通過利用中間折射率材料替代現有膜層結構(HL) n 中之低折射率材料,使得不同折射率膜層之折射率差值縮小從而有效地減少分光濾波膜層在45度角入射時透射光譜之半值波長處平行偏振光譜和垂直偏振光譜之偏移量,改善了現有膜層結構(HL) n 在較大入射角時反射波長範圍內反射率下降之情況並且減少了分光濾波膜層在入射角變化時之透射光譜偏移量。 Compared with the prior art, the periodic film stack ( HM ) n provided by the present invention replaces the low refractive index material in the existing film structure ( HL ) n by using an intermediate refractive index material, so that the refractive index of the different refractive index film layers The difference is reduced to effectively reduce the offset between the parallel polarization spectrum and the vertical polarization spectrum at the half-value wavelength of the transmission spectrum of the spectral filter film at an angle of 45 degrees, which improves the existing film structure ( HL ) n at a large incidence. The reflectance decreases in the wavelength range of the reflection angle and reduces the transmission spectral shift of the spectrally-filtered film layer when the incident angle changes.
綜上所述,本發明確已符合發明專利之要件,遂依法提 出專利申請。惟,以上所述者僅為本發明之較佳實施方式,自不能以此限制本案之申請專利範圍。舉凡熟悉本案技藝之人士援依本發明之精神所作之等效修飾或變化,皆應涵蓋於以下申請專利範圍內。 In summary, the present invention has indeed met the requirements of the invention patent, and Patent application. However, the above description is only a preferred embodiment of the present invention, and it is not possible to limit the scope of the patent application of the present invention. Equivalent modifications or variations made by persons skilled in the art in light of the spirit of the invention are intended to be included within the scope of the following claims.
1‧‧‧分光棱鏡 1‧‧‧Splitting prism
2‧‧‧膜堆結構 2‧‧‧membrane structure
4‧‧‧分光棱鏡上表面 4‧‧‧Splitting prism upper surface
3‧‧‧鍍有膜堆結構之表面 3‧‧‧ Surface coated with membrane stack structure
5‧‧‧分光棱鏡側面 5‧‧‧Split prism side
10‧‧‧膜堆結構 10‧‧‧membrane structure
102‧‧‧透明基底 102‧‧‧Transparent substrate
104‧‧‧週期性膜堆 104‧‧‧Recurrent membrane stack
106‧‧‧高折射率膜層 106‧‧‧High refractive index film
108‧‧‧中間折射率膜層 108‧‧‧Intermediate refractive index film
圖1為分光棱鏡之結構示意圖。 1 is a schematic view showing the structure of a beam splitting prism.
圖2為入射角為45度,參考波長為550nm時,膜堆結構(HL)18之透射光譜圖。 2 is a transmission spectrum diagram of the film stack structure ( HL ) 18 when the incident angle is 45 degrees and the reference wavelength is 550 nm.
圖3為入射角為53度,參考波長為483nm時,膜堆結構(HL)18之透射光譜圖。 Fig. 3 is a transmission spectrum diagram of the film stack structure ( HL ) 18 when the incident angle is 53 degrees and the reference wavelength is 483 nm.
圖4為入射角為37度,參考波長為483nm時,膜堆結構(HL)18之透射光譜圖。 4 is a transmission spectrum diagram of the film stack structure ( HL ) 18 when the incident angle is 37 degrees and the reference wavelength is 483 nm.
圖5為本發明提供之週期性膜堆(HM) n 之結構示意圖。 FIG. 5 is a schematic structural view of a periodic film stack ( HM ) n provided by the present invention.
圖6為入射角為45度,參考波長為475nm時,膜堆結構(HM)18之透射光譜圖。 Fig. 6 is a transmission spectrum diagram of the film stack structure ( HM ) 18 when the incident angle is 45 degrees and the reference wavelength is 475 nm.
圖7為入射角為53度,參考波長為475nm時,膜堆結構(HM)18之透射光譜圖。 Fig. 7 is a transmission spectrum diagram of the film stack structure ( HM ) 18 when the incident angle is 53 degrees and the reference wavelength is 475 nm.
圖8為入射角為37度,參考波長為475nm時,膜堆結構(HM)18之透射光譜圖。 Fig. 8 is a transmission spectrum diagram of the film stack structure ( HM ) 18 when the incident angle is 37 degrees and the reference wavelength is 475 nm.
10‧‧‧膜堆結構 10‧‧‧membrane structure
102‧‧‧透明基底 102‧‧‧Transparent substrate
104‧‧‧週期性膜堆 104‧‧‧Recurrent membrane stack
106‧‧‧高折射率膜層 106‧‧‧High refractive index film
108‧‧‧中間折射率膜層 108‧‧‧Intermediate refractive index film
Claims (10)
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TW97125381A TWI383173B (en) | 2008-07-04 | 2008-07-04 | Film stacked structure |
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TW97125381A TWI383173B (en) | 2008-07-04 | 2008-07-04 | Film stacked structure |
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TW201003113A TW201003113A (en) | 2010-01-16 |
TWI383173B true TWI383173B (en) | 2013-01-21 |
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Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
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US6018421A (en) * | 1995-06-28 | 2000-01-25 | Cushing; David Henry | Multilayer thin film bandpass filter |
US6627304B1 (en) * | 1997-04-30 | 2003-09-30 | Leica Microsystems Wetzlar Gmbh | Absorbent thin-film system consisting of metal and dielectric films |
TWI236548B (en) * | 2003-09-10 | 2005-07-21 | Seiko Epson Corp | Color filter substrate and its manufacturing method, electro-optical apparatus, and electronic equipment |
JP2006091859A (en) * | 2004-08-27 | 2006-04-06 | Fuji Photo Film Co Ltd | Anti-reflection film, and polarizing plate and image display device using the same |
TW200804874A (en) * | 2006-07-11 | 2008-01-16 | Murakami Corp | Dielectric multilayer filter |
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2008
- 2008-07-04 TW TW97125381A patent/TWI383173B/en not_active IP Right Cessation
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6018421A (en) * | 1995-06-28 | 2000-01-25 | Cushing; David Henry | Multilayer thin film bandpass filter |
US6627304B1 (en) * | 1997-04-30 | 2003-09-30 | Leica Microsystems Wetzlar Gmbh | Absorbent thin-film system consisting of metal and dielectric films |
TWI236548B (en) * | 2003-09-10 | 2005-07-21 | Seiko Epson Corp | Color filter substrate and its manufacturing method, electro-optical apparatus, and electronic equipment |
JP2006091859A (en) * | 2004-08-27 | 2006-04-06 | Fuji Photo Film Co Ltd | Anti-reflection film, and polarizing plate and image display device using the same |
TW200804874A (en) * | 2006-07-11 | 2008-01-16 | Murakami Corp | Dielectric multilayer filter |
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