JPH0782126B2 - Multi-layer partial reflection film - Google Patents
Multi-layer partial reflection filmInfo
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- JPH0782126B2 JPH0782126B2 JP23370886A JP23370886A JPH0782126B2 JP H0782126 B2 JPH0782126 B2 JP H0782126B2 JP 23370886 A JP23370886 A JP 23370886A JP 23370886 A JP23370886 A JP 23370886A JP H0782126 B2 JPH0782126 B2 JP H0782126B2
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- refractive index
- film
- layer
- partial reflection
- multilayer
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Description
【発明の詳細な説明】 産業上の利用分野 本発明は多層部分反射膜に関するものであり、更に詳し
くは主にレーザ用光学部品として使用される部分反射鏡
に用いられる多層部分反射膜に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a multilayer partial reflection film, and more particularly to a multilayer partial reflection film mainly used for a partial reflection mirror used as an optical component for laser. is there.
従来の技術 近年、レーザ技術およびその応用に関する目醒しい発展
に伴って、レーザ用光学部品の開発・研究が盛んに行な
われてきた。特にレーザ発振器等に用いられる部分反射
鏡(出力鏡ともいう)と称せられるものは、レーザ発振
波長において共振器の設計に応じた適当な反射率(また
は透過率)を有し、レーザ光量の出力を調節する機能を
有している。この部分反射鏡は、一般に光学基板の両面
に誘電体多層膜を被覆して作製されるものであり、その
構成は出力側の基板面に反射防止膜が、共振器側の基板
面には所望する反射率を有する部分反射膜が被覆された
ものとなっている。2. Description of the Related Art In recent years, with the remarkable development of laser technology and its application, development and research of optical components for laser have been actively conducted. Particularly, what is called a partial reflection mirror (also called an output mirror) used in a laser oscillator or the like has an appropriate reflectance (or transmittance) according to the design of the resonator at the laser oscillation wavelength, and outputs the laser light amount. It has the function of adjusting. This partial reflecting mirror is generally manufactured by coating both surfaces of an optical substrate with a dielectric multilayer film. Its structure is such that an antireflection film is formed on the output side substrate surface and a desired resonator side substrate surface is formed. The partial reflection film having the above reflectance is coated.
このような部分反射膜としては従来より誘電体交互多層
膜が用いられており、これは屈折率の異なる2種類の薄
膜、すなわち、低屈折率層および高屈折率層をそれぞれ
λ/4(λ;レーザ発振波長)の光学厚さで交互積層した
ものを基本構造として有し、その構成層数を適当に決定
した時、その構成層のうちの適当な一層(最上層または
最下層の場合が多い)の層厚を調節することにより目的
とする反射率を得るようにしたものである。As such a partial reflection film, a dielectric alternating multi-layer film has been conventionally used. This is two kinds of thin films having different refractive indexes, that is, a low refractive index layer and a high refractive index layer each having λ / 4 (λ A layered structure having an optical thickness of a laser oscillation wavelength) is alternately laminated as a basic structure, and when the number of constituent layers is appropriately determined, an appropriate one of the constituent layers (in the case of the uppermost layer or the lowermost layer, The target reflectance is obtained by adjusting the layer thickness (of a large number).
第2図に従来の多層部分反射膜構造の1例の概略図を示
す。これは、基板上に最下層を層厚調節層とし、その他
をλ/4交互多層膜として積層した多層部分反射膜の1例
である。FIG. 2 shows a schematic view of an example of a conventional multilayer partial reflection film structure. This is an example of a multilayer partial reflection film in which the lowermost layer is a layer thickness adjusting layer and the others are laminated as a λ / 4 alternating multilayer film on a substrate.
発明が解決しようとする問題点 以上述べたように、レーザ光学部品、特に部分反射鏡に
用いられる多層部分反射膜に関して広範な研究が行なわ
れ、その1例として特に第2図に示されるような構成の
多層部分反射膜が提案されてきた。DISCLOSURE OF THE INVENTION Problems to be Solved by the Invention As described above, extensive research has been conducted on laser optical components, particularly multilayer partial reflection films used for partial reflection mirrors, and one example thereof is shown in FIG. Multilayer partially reflective films of construction have been proposed.
しかしながら、分光透過スペクトル特性においては、こ
のような多層部分反射膜は使用波長でのみ所望の反射率
を満足するものであり、必ずしもその波長において透過
率が極値となっているとは限らないため、実際の光学膜
製造時において膜厚制御が不十分であるとその透過率は
所望値から外れ、目的値を満足しない結果になりかねな
い。更に、このような部分反射膜はレーザ発振波長の変
動に対して、その分光特性からみて透過率安定性に欠け
るという欠点を有していた。However, in the spectral transmission spectrum characteristics, such a multilayer partial reflection film satisfies the desired reflectance only at the wavelength used, and the transmittance does not always have the extreme value at that wavelength. However, if the film thickness is not sufficiently controlled during the actual production of the optical film, the transmittance may deviate from the desired value, and the desired value may not be satisfied. Further, such a partial reflection film has a drawback that it lacks transmittance stability in view of its spectral characteristics with respect to variations in laser oscillation wavelength.
このような問題点は、上記多層部分反射膜構造が完全な
λ/4交互多層膜となっておらず、目標反射率を満足させ
るため、適当な一層を調整膜として選び、その光学厚さ
をλ/4と異なる値に設定していることに起因すると考え
られる。Such a problem is that the above-mentioned multilayer partial reflection film structure is not a perfect λ / 4 alternating multilayer film, and in order to satisfy the target reflectance, an appropriate layer is selected as the adjustment film and its optical thickness is adjusted. It is considered that this is due to the setting to a value different from λ / 4.
そこで、本発明の目的は、上記のような欠点のない、使
用波長において所望の反射率を有し、かつ分光透過スペ
クトルが使用波長において極値となるような多層部分反
射膜を提供するものである。Therefore, an object of the present invention is to provide a multilayer partial reflection film which does not have the above-mentioned drawbacks, has a desired reflectance at a use wavelength, and has a spectral transmission spectrum having an extreme value at a use wavelength. is there.
問題点を解決するための手段 本発明者等は、従来の多層部分反射膜における上記の如
き諸欠点を解決すべく種々検討、研究を重ねた結果、従
来の多層部分反射膜における低屈折率層を等価な屈折率
を有し且つ3膜からなる等価屈折率層でおきかえ、等価
屈折率を任意に調節しながら、λ/4交互多層膜の構成を
とることが本発明の目的達成に有利であることを見出し
本発明を完成した。Means for Solving the Problems The inventors of the present invention have conducted various studies and researches to solve the above-mentioned drawbacks in the conventional multilayer partial reflection film, and as a result, have achieved a low refractive index layer in the conventional multilayer partial reflection film. It is advantageous to achieve the object of the present invention to replace ## EQU3 ## with an equivalent refractive index layer consisting of three films, and adjust the equivalent refractive index arbitrarily to form a λ / 4 alternating multilayer film. The present invention was completed by finding out that there is.
すなわち、本発明の多層部分反射膜は、屈折率nSの基板
上に、各々、使用波長λに対してλ/4の光学厚さで交互
に積層された少なくとも1層の屈折率nxの低屈折率層と
少なくとも1層の屈折率nHの高屈折率層とから構成され
た多層部分反射膜であって、上記低屈折率層の各々が、
屈折率nLの中間膜と、該中間膜を挟む2層の屈折率nHの
調整膜から構成されていることを特徴とする。That is, the multilayer partially reflective film of the present invention has a refractive index n x of at least one layer alternately laminated on the substrate having a refractive index n S with an optical thickness of λ / 4 with respect to the working wavelength λ. A multilayer partial reflection film comprising a low refractive index layer and at least one high refractive index layer having a refractive index n H , wherein each of the low refractive index layers comprises:
It is characterized in that it is composed of an intermediate film having a refractive index n L and two adjustment films having a refractive index n H sandwiching the intermediate film.
本発明の部分反射膜の反射率Rは、基板の屈折率nS、低
屈折率層の屈折率nXおよび高屈折率の屈折率nHを用いて
下記一般式(I)、(II)によって決定される。すなわ
ち、nS、nX、nHとの間に、 上記低屈折率層nxと上記高屈折率層nHとの交互多層膜系
において、各構成層を個々に数えた全層数Nが偶数であ
るとき、 上記低屈折率層nxと上記高屈折率層nHとの交互多層膜系
において、各構成層を個々に数えた全層数Nが奇数であ
るとき、 の関係式が成立する。The reflectance R of the partially reflective film of the present invention is represented by the following general formulas (I) and (II) using the refractive index n S of the substrate, the refractive index n X of the low refractive index layer and the refractive index n H of the high refractive index. Determined by That is, in the alternating multilayer film system of the low refractive index layer n x and the high refractive index layer n H between n S , n X , and n H , the total number of layers N obtained by individually counting each constituent layer is N. Is an even number, In the alternate multilayer film system of the low refractive index layer n x and the high refractive index layer n H , when the total number N of the individual constituent layers is an odd number, The relational expression of is established.
従って、所望の反射率Rに対し、上記低屈折率層の屈折
率nXは上記一般式(I)または(II)により導かれる。Therefore, with respect to the desired reflectance R, the refractive index n X of the low refractive index layer is derived by the general formula (I) or (II).
ただし、層数Nは必ずしも一義的に決定されるものでは
なく、薄膜形成における難易性または膜の光学特性等に
より最適数を決定するものである。However, the number N of layers is not necessarily uniquely determined, but the optimal number is determined depending on the difficulty in forming a thin film, the optical characteristics of the film, and the like.
一方、低屈折率層は対称3層膜であることが好ましく、
低屈折率層を構成するこれらの中間膜の膜厚dlおよび2
層の調整膜の膜厚daは、それぞれ、次式; および、 により決定される。On the other hand, the low refractive index layer is preferably a symmetrical three-layer film,
The film thicknesses d l and 2 of these intermediate films constituting the low refractive index layer
The film thickness d a of the layer adjusting film is calculated by the following equation; and, Determined by
またこのようなレーザ部品、特にレーザ発振器の部分反
射鏡に要求される反射率は共振器の設計仕様にもよるが
通常50%〜90%の範囲内にあり、このような反射率を限
るため下記のような構成が考えられる。The reflectance required for such a laser component, especially for a partial reflector of a laser oscillator, is usually within the range of 50% to 90%, though it depends on the design specifications of the resonator. The following configurations are possible.
すなわち、上記高屈折率層としては、主に通常ZnSe(nH
=2.40)、ZnS(nH=2.19)、As2S3(nH=2.38)または
CdTe(nH=2.69)等から成る膜が使用され、低屈折率層
を構成する低屈折率膜としては、ThF4(nL=1.35)、Pb
F2(nL=1.55)、SrF2(nL=1.36)またはBaF2(nL=1.
41)等から成る膜が使用される。それぞれの層の屈折率
としては目標反射率の特定の値に対し、層数等地の条件
にもよるが、2.19≦nH≦2.69、1.35≦nL≦1.55のものが
一般に使用される。また、低屈折率層の屈折率nXはnL≦
nX≦nHの範囲の値が可能である。That is, as the high refractive index layer, mainly ZnSe (n H
= 2.40), ZnS (n H = 2.19), As 2 S 3 (n H = 2.38) or
A film made of CdTe (n H = 2.69) or the like is used. As the low refractive index film constituting the low refractive index layer, ThF 4 (n L = 1.35), Pb
F 2 (n L = 1.55), SrF 2 (n L = 1.36) or BaF 2 (n L = 1.
41) Membranes composed of etc. are used. The refractive index of each layer is generally 2.19 ≦ n H ≦ 2.69, 1.35 ≦ n L ≦ 1.55, although it depends on the specific value of the target reflectance and the number of layers and the like. Further, the refractive index n X of the low refractive index layer is n L ≦
Values in the range n X ≤ n H are possible.
同様の考え方から上記多層膜を支持する基板としてはZn
Se、GaAs、CdTeまたはGe等が目的に応じて使用される。From the same viewpoint, Zn is used as a substrate for supporting the above-mentioned multilayer film.
Se, GaAs, CdTe, Ge or the like is used according to the purpose.
本発明の多層部分反射膜は、使用波長における薄膜及び
基板の屈折率が明確にわかっていれば、その波長におい
ては本発明の目的を達成することが可能であるが、赤外
のみならず、可視域に及ぶ広範囲な光学膜の対象波長域
でこの多層部分反射膜に上記分光特性をもたせることが
可能なため、種々のレーザ発振器の部分反射膜に応用す
ることができる。例えば、CO2レーザ、COレーザまたはY
AGレーザ等に応用できる。The multilayer partial reflection film of the present invention, if the refractive index of the thin film and the substrate at the wavelength used is clearly known, it is possible to achieve the object of the present invention at that wavelength, not only infrared, Since the multilayer partial reflection film can have the above-mentioned spectral characteristics in a target wavelength range of an optical film in a wide visible range, it can be applied to a partial reflection film of various laser oscillators. For example, CO 2 laser, CO laser or Y
It can be applied to AG laser, etc.
作用 かくして、本発明の多層部分反射膜は、屈折率nXを有す
る低屈折率層と屈折率nHを有する高屈折率層をλ/4の光
学厚さで交互に積層した構成を有することを特徴として
いる。Operation Thus, the multilayer partially reflective film of the present invention has a structure in which a low refractive index layer having a refractive index n X and a high refractive index layer having a refractive index n H are alternately laminated with an optical thickness of λ / 4. Is characterized by.
所望の波長λに対してλ/4の光学厚さを有し、それぞれ
屈折率がnL、nHである2種の層を、各層を個々に数えて
全層数Nだけ屈折率nSの透明基板に交互に積層した多層
膜において、その反射率Rは、一般に、下記の式A、B
により表すことができる。但し、式Aは、全層数Nが偶
数の場合を、式Bは、全層数Nが奇数の場合をそれぞれ
表す。Two layers having an optical thickness of λ / 4 with respect to a desired wavelength λ and having refractive indices n L and n H , respectively, are individually counted and the refractive index n S is equal to the total number N of layers. In the multilayer film alternately laminated on the transparent substrate, the reflectance R is generally expressed by the following formulas A and B.
Can be represented by However, Formula A represents a case where the total number N of layers is an even number, and Formula B represents a case where the total number N of layers is an odd number.
式A、式Bから判るように、各式はその何れの項にも波
長λを含んでおらず、反射率Rは屈折率nS、nL、nHおよ
び全層数Nの関数である。従って、反射率Rは波長依存
性がなく(dR/dλ=0)、波長λの近傍では反射率Rは
極値特性を有する。しかしながら、このことは、反射率
Rが、各屈折率と層数との値により決定されるので、所
望の値に任意に設定できないということを意味してい
る。 As can be seen from the equations A and B, each equation does not include the wavelength λ in any of the terms, and the reflectance R is a function of the refractive indices n S , n L and n H and the total number N of layers. . Therefore, the reflectance R has no wavelength dependence (dR / dλ = 0), and the reflectance R has an extreme value characteristic in the vicinity of the wavelength λ. However, this means that the reflectance R cannot be arbitrarily set to a desired value because the reflectance R is determined by the values of each refractive index and the number of layers.
これに対して、本発明に係る多層部分反射膜は、各層が
λ/4の厚さを有し且つ互いに異なる屈折率nL、nHを有す
るという多層構造という基本構造のもとで、対称3層膜
なる下位構造を有する屈折率nxの低屈折率層を用いるこ
とにより、屈折率、層数により反射率が離散的な値にな
り任意の反射率を設定することができないという従来の
欠点を、波長λにおける反射率の極致特性を損なうこと
なく解決している。On the other hand, the multilayer partially reflective film according to the present invention is symmetric under the basic structure of a multilayer structure in which each layer has a thickness of λ / 4 and has different refractive indices n L and n H. By using a low-refractive index layer having a lower refractive index n x having a three-layer film, the reflectance becomes a discrete value depending on the refractive index and the number of layers, and it is impossible to set an arbitrary reflectance. The drawback is solved without impairing the extreme characteristic of the reflectance at the wavelength λ.
このような構成により、上記多層部分反射膜の反射率R
は、上記式(I)または(II)で与えられるように屈折
率nX、nH、nSおよび層数Nで決定される値をとり、分光
透過スペクトルにおいては透過率が極値となり作用波長
付近での波長依存性は極めて小さくなる。With such a configuration, the reflectance R of the multilayer partial reflection film is
Is a value determined by the refractive indices n X , n H , n S and the number of layers N as given by the above formula (I) or (II), and the transmittance becomes an extreme value in the spectral transmission spectrum, and acts. The wavelength dependence near the wavelength becomes extremely small.
すなわち、屈折率nLの低屈折率膜を中間膜として、その
両側を2層の屈折率nHの調整膜にて挟んだ屈折率nXを有
する3層の低屈折率層を用いることにより、所望の反射
率がいかなる値に設定されようとも、層数Nを選び、屈
折率nXを設定することにより、所望値に一致させること
ができる。That is, by using a low-refractive-index film having a refractive index n L as an intermediate film and three low-refractive-index layers having a refractive index n X sandwiched on both sides by two adjusting films having a refractive index n H , No matter what value the desired reflectance is set to, it is possible to match the desired value by selecting the number N of layers and setting the refractive index n X.
また、本発明の反射膜は従来の多層部分反射膜における
λ/4幕でない調節層を設けることのない完全なるλ/4交
互多層膜構造であるため、使用波長近傍における透過ス
ペクトルの安定性が良好である。Further, since the reflective film of the present invention has a complete λ / 4 alternating multilayer film structure without providing the adjustment layer other than the λ / 4 curtain in the conventional multilayer partial reflective film, the stability of the transmission spectrum in the vicinity of the used wavelength is improved. It is good.
実施例 以下、実施例により本発明の方法を更に具体的に説明す
るが、本発明の範囲は以下の実施例により何等制限され
ない。Examples Hereinafter, the method of the present invention will be described more specifically with reference to Examples, but the scope of the present invention is not limited to the following Examples.
実施例 第1図は、本発明の部分反射膜の概略縦断面図である。Example FIG. 1 is a schematic vertical sectional view of a partially reflective film of the present invention.
第1図に図示する本実施例の部分反射膜は、低屈折率層
Xと高屈折率層Hとが基板側より光学厚さλ/4で交互に
積層した構造となっている。基板は屈折率nS=2.40のセ
レン化亜鉛(ZnSe)で形成されている。低屈折率層X
は、四フッ化トリウム(ThF4)(nL=1.35)の中間膜
と、その両側のZnSe(na=2.40)の調整膜とから構成さ
れている。一方、高屈折率層は、ZnSe(nH=2.40)から
形成されている。The partially reflective film of this embodiment shown in FIG. 1 has a structure in which low refractive index layers X and high refractive index layers H are alternately laminated from the substrate side with an optical thickness of λ / 4. The substrate is made of zinc selenide (ZnSe) having a refractive index n S = 2.40. Low refractive index layer X
Is composed of an intermediate film of thorium tetrafluoride (ThF 4 ) (n L = 1.35) and adjustment films of ZnSe (n a = 2.40) on both sides thereof. On the other hand, the high refractive index layer is formed of ZnSe (n H = 2.40).
このような構造の部分反射膜において、所定の反射率を
有するように、低屈折率層および高屈折率層の合計層数
Nと屈折率nXを決定し、さらに低屈折率層を形成する低
屈折率膜および調整膜の厚さを波長λ=10.6μmに対し
て決定し、第1表に示す。In the partial reflection film having such a structure, the total number N of the low refractive index layer and the high refractive index layer and the refractive index n X are determined so as to have a predetermined reflectance, and the low refractive index layer is further formed. The thicknesses of the low refractive index film and the adjustment film were determined for the wavelength λ = 10.6 μm and are shown in Table 1.
層数2、4および6の部分反射膜の中より、反射率が40
%、70%および90%の場合を選び、その分光透過スペク
トルを従来の多層部分反射膜と比較して第3〜5図に示
した。 The reflectance is 40 out of the partial reflection films with 2, 4 and 6 layers.
%, 70% and 90% were selected, and their spectral transmission spectra are shown in FIGS. 3 to 5 in comparison with the conventional multilayer partial reflection film.
なお、基板の他面側の反射防止膜はシュスター(Shuste
r)の条件式を使った{ThF4/ZnSe}系2層膜構造を採用
した。The antireflection film on the other side of the substrate is a Shuste (Shuste)
We adopted the {ThF 4 / ZnSe} -based two-layer film structure using the conditional expression of r).
第3〜5図のいずれの分光透過スペクトルにおいても、
CO2レーザの発振波長10.6μmにおいては本発明の部分
反射膜は、所望する反射率、即ち40%、70%および90%
の値で極値を示し、この波長で極値をとらない従来の部
分反射膜に比べ安定であることが示された。In any of the spectral transmission spectra shown in FIGS. 3 to 5,
When the oscillation wavelength of the CO 2 laser is 10.6 μm, the partially reflective film of the present invention has a desired reflectance, that is, 40%, 70% and 90%.
The value of shows an extreme value, and it is shown to be more stable than the conventional partial reflection film which does not take an extreme value at this wavelength.
また第6図には本発明の多層部分反射膜を使用したCO2
レーザ用70%部分反射鏡の赤外透過スペクトルを示す。
上記同様CO2レーザの発振波長10.6μmにおいて、所望
する反射率70%の値にてこの部分反射鏡は赤外透過スペ
クトルの極値をとることがわかった。Further, FIG. 6 shows CO 2 using the multilayer partially reflective film of the present invention.
The infrared transmission spectrum of a 70% partial reflection mirror for lasers is shown.
Similar to the above, it was found that this partial reflecting mirror has an extreme value of the infrared transmission spectrum at a desired reflectance of 70% at an oscillation wavelength of a CO 2 laser of 10.6 μm.
発明の効果 以上詳しく説明したように、本発明の多層部分反射膜は
低屈折率層としてλ/4等価3層膜を利用したλ/4交互多
層膜構造であるため、分光透過スペクトルにおける使用
波長で透過率の極値を示し、優れた分光特性を示す。ま
た本発明の多層部分反射膜は使用波長での薄膜材料およ
び基板材料の屈折率がわかっていれば、その波長におい
て所望反射率を有し、かつ分光透過スペクトルで極値を
とりうることが可能である。また、赤外だけでなく可視
域に及ぶ広範囲な対象波長域で本発明の多層部分反射膜
に従って得られる分光特性上の特徴を有することができ
る。EFFECTS OF THE INVENTION As described in detail above, since the multilayer partially reflective film of the present invention has a λ / 4 alternating multilayer film structure using a λ / 4 equivalent three-layer film as a low refractive index layer, it has a wavelength used in the spectral transmission spectrum. Shows the extreme value of transmittance and shows excellent spectral characteristics. Further, if the refractive index of the thin film material and the substrate material at the wavelength used is known, the multilayer partially reflective film of the present invention can have a desired reflectance at that wavelength and can take an extreme value in the spectral transmission spectrum. Is. Further, not only in the infrared but also in a wide range of target wavelengths extending to the visible range, the multi-layer partial reflection film of the present invention can have a characteristic in spectral characteristics.
第1図は、本発明の多層部分反射膜の一つの例を示す模
式断面図であり、 第2図は、公知の多層部分反射膜を示す模式断面図であ
り、 第3図は、本発明および公知の40%部分反射膜の分光透
過スペクトルであり、 第4図は、本発明および公知の70%部分反射膜の分光透
過スペクトルであり、 第5図は、本発明および公知の90%部分反射膜の分光透
過スペクトルであり、 第6図は、本発明の多層部分反射膜を用いて作製された
CO2レーザ用70%部分反射鏡の赤外透過率スペクトルで
ある。 (主な参照番号) H……高屈折率層、L……低屈折率層、 LX……反射率調整層、X……低屈折率層、 a……調整膜、l……中間膜FIG. 1 is a schematic cross-sectional view showing one example of the multilayer partial reflection film of the present invention, FIG. 2 is a schematic cross-sectional view showing a known multilayer partial reflection film, and FIG. 3 is the present invention. FIG. 4 is a spectral transmission spectrum of a known 40% partial reflection film, FIG. 4 is a spectral transmission spectrum of the present invention and a known 70% partial reflection film, and FIG. FIG. 6 is a spectral transmission spectrum of a reflective film, and FIG. 6 was prepared using the multilayer partially reflective film of the present invention.
It is an infrared transmittance spectrum of a 70% partial reflection mirror for CO 2 lasers. (Main reference numbers) H: high refractive index layer, L: low refractive index layer, L X: reflectance adjusting layer, X: low refractive index layer, a: adjusting film, l: intermediate film
Claims (5)
対してλ/4の光学厚さで交互に積層された少なくとも1
層の屈折率nxの低屈折率層と少なくとも1層の屈折率nH
の高屈折率層とから構成された多層部分反射膜であっ
て、上記低屈折率層の各々が、屈折率nLの中間膜と、該
中間膜を挟む2層の屈折率nHの調整膜から構成されてい
ることを特徴とする上記多層部分反射膜。1. At least one layer alternately laminated on a substrate having a refractive index n S with an optical thickness of λ / 4 with respect to a used wavelength λ.
Layer with low refractive index n x and at least one layer with refractive index n H
Of the high refractive index layer, wherein each of the low refractive index layers is an intermediate film having a refractive index n L , and the refractive index n H of two layers sandwiching the intermediate film is adjusted. The multilayer partial reflection film described above, which is formed of a film.
交互多層膜系において、各構成層を個々に数えた全層数
Nが偶数であるとき、所望の反射率Rに対し、上記低屈
折率層が一般式(I); から求められる等価屈折率nXを有することを特徴とする
特許請求の範囲第1項に記載の多層部分反射膜。2. In the alternate multilayer film system of the low refractive index layer n x and the high refractive index layer n H , the desired reflectance is obtained when the total number N of the individual constituent layers is an even number. For R, the low refractive index layer has the general formula (I); The multilayer partial reflection film according to claim 1, which has an equivalent refractive index n X obtained from
交互多層膜系において、各構成層を個々に数えた全層数
Nが奇数であるとき、所望の反射率Rに対し、上記低屈
折率層が一般式(II); から求められる等価屈折率nXを有することを特徴とする
特許請求の範囲第1項に記載の多層部分反射膜。3. In the alternate multilayer film system of the low refractive index layer n x and the high refractive index layer n H , the desired reflectance is obtained when the total number N of the individual constituent layers is an odd number. For R, the low refractive index layer has the general formula (II); The multilayer partial reflection film according to claim 1, which has an equivalent refractive index n X obtained from
特徴とする特許請求の範囲第1〜3項のいずれか1項に
記載の多層部分反射膜。4. The multilayer partial reflection film according to claim 1, wherein the low refractive index layer is a symmetrical three-layer film.
および2層の調整膜の膜厚daがそれぞれ、次式; および、 により決定されることを特徴とする特許請求の範囲第1
〜4項のいずれか1項に記載の多層部分反射膜。5. The film thickness d l of the intermediate film constituting the low refractive index layer
And the film thickness d a of the two-layer adjusting film is respectively the following formula; and, Claim 1 characterized by being determined by
Item 5. The multilayer partial reflection film according to any one of items 4 to 4.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23370886A JPH0782126B2 (en) | 1986-10-01 | 1986-10-01 | Multi-layer partial reflection film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23370886A JPH0782126B2 (en) | 1986-10-01 | 1986-10-01 | Multi-layer partial reflection film |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6388506A JPS6388506A (en) | 1988-04-19 |
| JPH0782126B2 true JPH0782126B2 (en) | 1995-09-06 |
Family
ID=16959305
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP23370886A Expired - Lifetime JPH0782126B2 (en) | 1986-10-01 | 1986-10-01 | Multi-layer partial reflection film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0782126B2 (en) |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4653912B2 (en) * | 2001-08-30 | 2011-03-16 | 光伸光学工業株式会社 | Multi-cavity bandpass filter and manufacturing method thereof |
| JP2003344645A (en) * | 2002-05-27 | 2003-12-03 | Hamamatsu Photonics Kk | Light reflection film and its manufacturing method |
| US7675078B2 (en) | 2005-09-14 | 2010-03-09 | Chunghwa Picture Tubes, Ltd. | Pixel structure |
| US8072402B2 (en) * | 2007-08-29 | 2011-12-06 | Qualcomm Mems Technologies, Inc. | Interferometric optical modulator with broadband reflection characteristics |
| JP2013187212A (en) * | 2012-03-06 | 2013-09-19 | Shimadzu Corp | Compact solid-state laser element |
-
1986
- 1986-10-01 JP JP23370886A patent/JPH0782126B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6388506A (en) | 1988-04-19 |
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