JPS6050294B2 - Demultiplexer - Google Patents
DemultiplexerInfo
- Publication number
- JPS6050294B2 JPS6050294B2 JP7132878A JP7132878A JPS6050294B2 JP S6050294 B2 JPS6050294 B2 JP S6050294B2 JP 7132878 A JP7132878 A JP 7132878A JP 7132878 A JP7132878 A JP 7132878A JP S6050294 B2 JPS6050294 B2 JP S6050294B2
- Authority
- JP
- Japan
- Prior art keywords
- prism
- optical fiber
- light
- wavelength
- rod lens
- 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.)
- Expired
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29346—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating by wave or beam interference
- G02B6/29361—Interference filters, e.g. multilayer coatings, thin film filters, dichroic splitters or mirrors based on multilayers, WDM filters
- G02B6/2937—In line lens-filtering-lens devices, i.e. elements arranged along a line and mountable in a cylindrical package for compactness, e.g. 3- port device with GRIN lenses sandwiching a single filter operating at normal incidence in a tubular package
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Spectrometry And Color Measurement (AREA)
Description
【発明の詳細な説明】
この発明は、1本の光ファイバ中を伝送されてきた少な
くとも2波長成分を含む光を、波長成分によつて分割し
、2本の光ファイバに分けて伝送させる光ファイバ分波
装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention is directed to splitting light containing at least two wavelength components transmitted through one optical fiber according to the wavelength components, and transmitting the light through two optical fibers. This invention relates to fiber demultiplexing equipment.
従来のこの種の装置について説明する。説明を簡単にす
るため、1本の光ファイバ中を伝送されてきた波長λ1
およびλ2の光を分波する場合について述べる。第1図
に従来の分波装置の一例を第2図にその断面図を示す。
1、2は屈折率がロッド中心からの距離のほぼ2乗に比
例して減少するような分布をもつ屈折率分布型ロッドレ
ンズであり、その長さはロッドレンズの焦点面がロッド
の端面に位置するような長さ(114周期長)である。A conventional device of this type will be explained. To simplify the explanation, the wavelength λ1 transmitted through one optical fiber is
A case will be described in which the light of λ2 and λ2 are demultiplexed. FIG. 1 shows an example of a conventional demultiplexing device, and FIG. 2 shows a sectional view thereof.
1 and 2 are gradient index rod lenses with a distribution in which the refractive index decreases approximately in proportion to the square of the distance from the rod center, and the length is such that the focal plane of the rod lens is at the end surface of the rod. It has a length (114 period length) such that
3は波長λ1の光を透過し、波長λ。の光を反射するよ
うな多層膜フィルタである。通常フィルタ3はロッドレ
ンズ1あるいは2の端面にコーティングされている。4
、5、6は入出力用の光ファイバであり、その端面4s
、5s、6sはロッドレンズの焦点面上に各々配設され
ている。3 transmits light of wavelength λ1, and wavelength λ. It is a multilayer filter that reflects the light of Usually, the filter 3 is coated on the end face of the rod lens 1 or 2. 4
, 5 and 6 are optical fibers for input and output, and their end faces 4s
, 5s, and 6s are respectively arranged on the focal plane of the rod lens.
この従来の分波装置の動作を装置の断面図(第2図)に
従つて説明する。光ファイバ4の中に伝送されてきた波
長λ、、およびλ。の光は光線7によつJて示されるよ
うに、ロッドレンズ1によつて平行光線に変換され多層
膜フィルタ3に入射する。このうち、波長λ、の光は多
層膜フィルタ3を透過し光線8によつて示されるごとく
ロッドレンズ2によつて絞られ光ファイバ6へ入射する
。一方波7長λ2の光は支線9によつて示されるごとく
、多層膜フィルタ3によつて反射されロッドレンズ1に
よつて絞られた光ファイバ5へ入射する。このように光
ファイバ4中を伝送されてきた波長λ1およびλ2の光
は分波されそれぞれ光ファイバ5,6へ送り込まれる。
しかしながら、一般に多層膜フィルタの特性は完全でな
く、例えば第3図に示すような特性をもつている。第3
図は、波長λ1に対し透明な帯域透過型フィルタの特性
の一例を示したものである。このように、帯域透過型フ
ィルタでは、所要波長λ1における透過率はほS゛10
0%に近いものが得られるが、その他の波長領域におい
ても若干の透過率を持つのが普通である。このため第2
図に示した従来の分波装置においてフィルタ3として第
3図に示したような特性の帯域透過形フィルタを用いた
場合、第2図の光線10に示すごとく無視できない量の
波長λ2の光が多層膜フィルタ3を透過し光ファイバ6
へ送り込まれる。このため光ファイバ6には波長λ1の
光の他にフィルタ3の不完全性によつて漏れ込んだ波長
λ2の光も入射するための性能のよい分波器を得ること
が困難であつた。なお、光ファイバ6へ入射する波長λ
2の光を減少させるためロッドレンズ1と2の間に複数
枚のフィルタを挿入することが考えられるがこの場合、
フィルタを重ねることによつて波長λ1の光の反射量が
増加しこれらの光が光ファイバ5へ入射するので望まし
くない。このようにこの従来の分波装置単独では多層膜
フィルタの不完全性による分波特性の劣化はさけられな
いものであり不都合であつた。この発明は、従来の分波
装置のこの欠点を除去し簡単な構成て高性能の分波特性
をもつ分波装置を得るため、2つの屈折率分布型ロッド
レンズの.間にプリズムを介在させ、プリズムとロッド
レンズの隙間2ケ所に各々多層膜フィルタとはさみこん
だ構造としたもので以下図面に従い詳細に説明する。第
4図は、本発明による光分波装置の一実施例jであり、
第5図はその断面図である。The operation of this conventional demultiplexing device will be explained with reference to a cross-sectional view of the device (FIG. 2). The wavelengths λ, and λ transmitted into the optical fiber 4. The light 7 is converted into a parallel light beam by the rod lens 1 and enters the multilayer filter 3, as shown by the light ray J. Of these, the light having the wavelength λ passes through the multilayer filter 3 and is focused by the rod lens 2 as shown by the light ray 8, and enters the optical fiber 6. On the other hand, as shown by a branch line 9, the light having the wavelength 7 and the wavelength λ2 is reflected by the multilayer filter 3 and enters the optical fiber 5 which is condensed by the rod lens 1. The lights of wavelengths λ1 and λ2 thus transmitted through the optical fiber 4 are demultiplexed and sent to the optical fibers 5 and 6, respectively.
However, in general, the characteristics of a multilayer filter are not perfect, and have characteristics as shown in FIG. 3, for example. Third
The figure shows an example of the characteristics of a bandpass filter that is transparent to wavelength λ1. In this way, in the bandpass filter, the transmittance at the required wavelength λ1 is approximately S゛10
Although a transmittance close to 0% can be obtained, it usually has a slight transmittance in other wavelength regions as well. For this reason, the second
In the conventional demultiplexing device shown in the figure, when a band pass filter with the characteristics shown in FIG. The optical fiber 6 passes through the multilayer filter 3.
sent to. For this reason, it has been difficult to obtain a duplexer with good performance so that, in addition to the light of wavelength λ1, the light of wavelength λ2 that has leaked into the optical fiber 6 due to the imperfection of the filter 3 is inputted into the optical fiber 6. Note that the wavelength λ incident on the optical fiber 6
It is conceivable to insert multiple filters between rod lenses 1 and 2 in order to reduce the light of 2, but in this case,
By overlapping the filters, the amount of light reflected at wavelength λ1 increases and these lights enter the optical fiber 5, which is undesirable. As described above, using this conventional demultiplexing device alone is inconvenient because deterioration of the demultiplexing characteristics due to imperfections in the multilayer filter cannot be avoided. In order to eliminate this drawback of the conventional demultiplexing device and obtain a demultiplexing device with a simple configuration and high performance demultiplexing characteristics, this invention uses two gradient index rod lenses. It has a structure in which a prism is interposed between them, and a multilayer film filter is sandwiched between two gaps between the prism and the rod lens, and will be described in detail below with reference to the drawings. FIG. 4 shows an embodiment j of an optical demultiplexing device according to the present invention,
FIG. 5 is a sectional view thereof.
説明を簡単にするため、本分波装置を用いて光ファイバ
を伝送されてきた波長λ1およびλ2の光を本分波装置
により分波し、2本の光ファイバに送り込む場合につい
て述べる。1,2は114周期長の屈折率4分布形ロッ
ドレンズ、3,12は波長λ1の光を透過し波長λ2の
光を反射する多層膜フィルタ4,5,6は入出力用光フ
ァイバでその端面4s,5s,6sはそれぞれロッドレ
ンズ1,2の焦点面に配設されている。To simplify the explanation, a case will be described in which the present demultiplexer is used to demultiplex the lights of wavelengths λ1 and λ2 transmitted through the optical fibers, and the demultiplexers are sent into two optical fibers. Reference numerals 1 and 2 are 4-distribution index rod lenses with a period length of 114, and multilayer filters 4, 5, and 6, which transmit light with wavelength λ1 and reflect light with wavelength λ2, are optical fibers for input and output. The end surfaces 4s, 5s, and 6s are arranged at the focal planes of the rod lenses 1 and 2, respectively.
また11は頂角が45の直角プリズムである。光ファイ
バ4を伝送されてきた波長λ1およびλ2の光はロッド
レンズ1によつて光線7によつて示されるように平行光
束に変換され多層膜フィルタ3へ入射する。多層膜フィ
ルタ3によつて波長屓の光は反射されロッドレンズ1に
よつて絞られ光ファイバ5へ入射する。この場合多層膜
フィルタとして第3図に示したような特性の帯域透過型
フィルタを用いれば、つこのフィルタによる波長λ1の
光の反射量はきわめて小さくできるので光ファイバ5へ
の波長λ1の光の漏れ込みはきわめて小さくすることが
できる。一方、多層膜フィルタ3と透過した光には波長
λ1の光(光線8によつて示す)とフィルタ37の不完
全性による波長λ2の光(光線10によつて示す)が含
まれる。これらの光は、プリズムの斜面によつて全反射
され多層膜フィルタ12へ入射する。このうち波長λ1
の光は多層膜フィルタ12を透過しロッドレンズ13に
よつて絞られ光Jファイバ6へ入射する。この場合、フ
ィルタの不完全性によつてフィルタを透過する波長λ2
の光は多層膜フィルタ3と多層膜フィルタ12によつて
2回フィルタリングされていることに留意すれば十分小
さくすることができる。あるいは多層膜フィルタ12と
して波長λ2の光をほS゛100%反射する帯域阻止形
フィルタを用いると一層効果的である。帯域阻止形フィ
ルタの特性は、通常第6図に示すように、所要波長にお
いてほS]00%の反射率をもつが他の波長においても
若干の反射率をもつている。このような帯域阻止形フィ
ルタを多層膜フィルタ12に用いれば波長λ2の光はこ
のフィルタ12によつてほS゛100%反射されるので
光ファイバ6への波長λ2の光をよソー層小さくするこ
とが可能である。さて多層膜フィルタ12によつて反射
された波長λ2の光(光線10)およびこのフィルタの
不完全性のため生じる波長λ1の光(光線11)は光線
10,14に示されるごとくプリズム側面より空間に放
射され失なわれるので光ファイバ5,6に入射し本分波
装置の特性をそこなうことはない。このように本発明に
よる分波装置では多層膜フィルタの不完全性による所要
波長以外の反射あるいは透過光を、ロッドレンズの間に
プリズムを介在させることによつて分波特性をそこなう
ことなく取り除くことができる。この実施例では、プリ
ズムとして頂角が45゜の直角プリズムを用いる場合に
ついて述べたがこれは特に頂角が45゜である必要もな
く又直角プリズムである必要もない。Further, 11 is a right angle prism with an apex angle of 45. The lights of wavelengths λ1 and λ2 transmitted through the optical fiber 4 are converted by the rod lens 1 into a parallel beam of light as shown by the light ray 7, and then enter the multilayer filter 3. The light of different wavelengths is reflected by the multilayer film filter 3, focused by the rod lens 1, and enters the optical fiber 5. In this case, if a bandpass filter with the characteristics shown in FIG. 3 is used as the multilayer filter, the amount of light with wavelength λ1 reflected by this filter can be made extremely small, so that the amount of light with wavelength λ1 entering the optical fiber 5 can be reduced. Leakage can be made extremely small. On the other hand, the light transmitted through the multilayer filter 3 includes light with a wavelength λ1 (indicated by ray 8) and light with a wavelength λ2 (indicated by ray 10) due to imperfections in the filter 37. These lights are totally reflected by the slope of the prism and enter the multilayer filter 12 . Of these, the wavelength λ1
The light passes through the multilayer filter 12, is focused by the rod lens 13, and enters the optical J fiber 6. In this case, the wavelength λ2 transmitted through the filter due to the imperfection of the filter
The light can be made sufficiently small by keeping in mind that the light is filtered twice by the multilayer filter 3 and the multilayer filter 12. Alternatively, it is more effective to use a band-elimination filter that reflects almost 100% of the light with wavelength λ2 as the multilayer filter 12. As shown in FIG. 6, the characteristic of a band-elimination filter is that it usually has a reflectance of approximately S]00% at a desired wavelength, but also has a slight reflectance at other wavelengths. If such a band-elimination filter is used as the multilayer filter 12, almost 100% of the light with the wavelength λ2 will be reflected by the filter 12, so the light with the wavelength λ2 to the optical fiber 6 can be made smaller by a relatively small layer. Is possible. Now, the light of wavelength λ2 (ray 10) reflected by the multilayer filter 12 and the light of wavelength λ1 (ray 11) generated due to the imperfection of this filter are emitted from the side of the prism as shown by rays 10 and 14. Since the light is radiated to the optical fibers 5 and 6 and is lost, the light does not enter the optical fibers 5 and 6 and impair the characteristics of the demultiplexer. As described above, in the demultiplexing device according to the present invention, reflected or transmitted light of wavelengths other than the required wavelength due to imperfections in the multilayer filter can be removed without damaging the demultiplexing characteristics by interposing a prism between the rod lenses. be able to. In this embodiment, a case has been described in which a right-angle prism with an apex angle of 45 degrees is used as the prism, but the apex angle does not particularly need to be 45 degrees, nor does it need to be a right-angle prism.
要は多層膜フィルタ12によつて反射された光が再び光
ファイバ5あるいは6へ入射することがないようプリズ
ムが挿入されておれば本発明の効果が得られることは前
述の説明から容易に理解できよう。但しプリズムとして
頂角が45゜の直角プリズムを用いた場合は、2つのロ
ッドレンズのなす角が直交し又、多層膜フィルタ3およ
び12への光線の入射角が等しくなるので光学設計およ
び機構設計上有利である。また、屈折率分布型ロッドレ
ンズ1,2として114周期長のものを用いたが、頭ノ
ドレンズもこの長さに限らす要は光ファイバ4,5,6
の端面4s,5s,6sが各々ロッドレンズの焦点面に
来るように配設されておればよい。但しロッドレンズが
lハ周期長の場合は焦点面とロッドレンズ端面が一致し
従つて光ファイバ4,5,6の端面4s,5s,6sと
ロッドレンズの端面に密着できるのでフレネル反射の低
減にきわめて有利てある。また光ファイバ4,5,6と
して複数本の光ファイバを束ねた光ファイバ束を用いる
こともできるのは明らかである。なお以上は、2つの波
長の光を分波する場合について設明したが、この発明は
これに限らず3つ以上の波長の光を波長によつて2分割
する場合に使用しても同様の効果を得ることができる。In short, it is easy to understand from the above explanation that the effects of the present invention can be obtained as long as a prism is inserted to prevent the light reflected by the multilayer filter 12 from entering the optical fiber 5 or 6 again. I can do it. However, if a right-angle prism with an apex angle of 45° is used as the prism, the angles formed by the two rod lenses will be orthogonal, and the incident angles of the light rays to the multilayer filters 3 and 12 will be equal, so optical design and mechanical design will be difficult. It is advantageous. Furthermore, although we used gradient index rod lenses 1 and 2 with a period length of 114, the length of the head throat lens should also be limited to this length.
It is only necessary that the end surfaces 4s, 5s, and 6s of the rod lenses are arranged so that they are in the focal plane of the rod lens. However, when the rod lens has a period length of l, the focal plane and the end surface of the rod lens coincide, and therefore the end surfaces 4s, 5s, 6s of the optical fibers 4, 5, 6 can be brought into close contact with the end surfaces of the rod lens, which reduces Fresnel reflection. It is extremely advantageous. It is also obvious that an optical fiber bundle obtained by bundling a plurality of optical fibers can be used as the optical fibers 4, 5, and 6. Although the above description has been made for the case of splitting light of two wavelengths, this invention is not limited to this, and the same invention can be applied to the case of splitting light of three or more wavelengths into two depending on the wavelength. effect can be obtained.
以上のように、本発明による分波装置では2つの屈折率
分布型ロッドレンズの間にプリズムを介在させプリズム
とロッドレンズの間に各々多層膜フィルタをはさみ込む
構造になつているから多層膜フィルタの不完全性による
不要な透過光あるいは反射光を取り除くことができ、良
好な分波特性の分波器を得ることができる利点がある。As described above, the demultiplexing device according to the present invention has a structure in which a prism is interposed between two gradient index rod lenses, and a multilayer filter is sandwiched between the prism and the rod lens. This has the advantage that unnecessary transmitted light or reflected light due to imperfections can be removed, and a demultiplexer with good demultiplexing characteristics can be obtained.
図面の簡単な説明第1図は従来の分波装置を示す図、第
2図は第1図に示した従来の分波装置の断面図、第3図
は帯域透過形フィルタの特性の一例を示す図、第4図は
本発明による分波装置の一実施例を示す図、第5図は第
4図に示した本発明による分波装置の一実施例の断面図
、第6図は帯域阻止形フィルタの特性の一例を示す図で
ある。Brief Description of the Drawings Figure 1 shows a conventional demultiplexer, Figure 2 is a sectional view of the conventional demultiplexer shown in Figure 1, and Figure 3 shows an example of the characteristics of a band-pass filter. FIG. 4 is a diagram showing an embodiment of the demultiplexing device according to the present invention, FIG. 5 is a sectional view of an embodiment of the demultiplexing device according to the present invention shown in FIG. 4, and FIG. FIG. 3 is a diagram showing an example of characteristics of a blocking filter.
図中1,2は屈折率分布形ロッドレンズ、3は多層膜フ
ィルタ、4,5,6は入出力用光ファイバ、7は入力用
光ファイバからロッドレンズ内に放射された波長λ1
とλ2の光線の一例、8は多層膜フィルタ3を透過した
波長λ,の光線の一例、9は多層膜フィルタ3により反
射された波長λ。In the figure, 1 and 2 are gradient index rod lenses, 3 is a multilayer filter, 4, 5, and 6 are input/output optical fibers, and 7 is a wavelength λ1 emitted from the input optical fiber into the rod lens.
and λ2, 8 is an example of a light beam of wavelength λ transmitted through the multilayer filter 3, and 9 is a wavelength λ reflected by the multilayer filter 3.
Claims (1)
てきた少なくとも2波長成分以上の光を波長により分割
し2本の光ファイバあるいは光ファイバ束に送り込む分
波装置において、2つの1/4周期長以下の長さの屈折
率分布形ロッドレンズをその端面間にプリズムを介在さ
せて配設し、プリズムと各々のロッドレンズの間に多層
膜フィルタをはさみ込み、1つのロッドレンズのプリズ
ムとは反対側の焦点面上に2本の光ファイバあるいは光
ファイバ束を、また他のロッドレンズのプリズムとは反
対側の焦点面上に1本の光ファイバあるいは光ファイバ
束を配設したことを特徴とする分波装置。 2 頂角が45゜の直角プリズムの直角をはさむ2面に
それぞれロッドレンズを配設したことを特徴とする特許
請求の範囲第1項記載の分波装置。 3 その焦点面に2本の光ファイバを配設したロッドレ
ンズとプリズムの間に帯域透過形フィルタを又、他のロ
ッドレンズとプリズムの間に帯域阻止形フィルタをはさ
み込んだことを特徴とする特許請求の範囲第1項記載の
分波装置。[Scope of Claims] 1. A demultiplexing device that splits light of at least two wavelength components transmitted through one optical fiber or optical fiber bundle according to wavelength and sends it to two optical fibers or optical fiber bundles. A gradient index rod lens having a length of 1/4 period length or less is arranged with a prism interposed between its end faces, and a multilayer film filter is sandwiched between the prism and each rod lens. Two optical fibers or optical fiber bundles are arranged on the focal plane of the lens opposite to the prism, and one optical fiber or optical fiber bundle is arranged on the focal plane of the other rod lens opposite to the prism. A demultiplexing device characterized by: 2. The demultiplexing device according to claim 1, characterized in that a rod lens is disposed on each of two surfaces sandwiching a right angle of a right angle prism having an apex angle of 45 degrees. 3 A band transmission filter is sandwiched between a prism and a rod lens with two optical fibers arranged on its focal plane, and a band rejection filter is sandwiched between another rod lens and the prism. A demultiplexing device according to claim 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7132878A JPS6050294B2 (en) | 1978-06-13 | 1978-06-13 | Demultiplexer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7132878A JPS6050294B2 (en) | 1978-06-13 | 1978-06-13 | Demultiplexer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS54162589A JPS54162589A (en) | 1979-12-24 |
| JPS6050294B2 true JPS6050294B2 (en) | 1985-11-07 |
Family
ID=13457362
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7132878A Expired JPS6050294B2 (en) | 1978-06-13 | 1978-06-13 | Demultiplexer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6050294B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63161994U (en) * | 1987-04-03 | 1988-10-21 |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5857770A (en) * | 1997-03-24 | 1999-01-12 | Ford Motor Company | Laser illuminated vehicle lighting system utilizing a turning prism |
-
1978
- 1978-06-13 JP JP7132878A patent/JPS6050294B2/en not_active Expired
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63161994U (en) * | 1987-04-03 | 1988-10-21 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS54162589A (en) | 1979-12-24 |
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