TWI269888B - Splitter with zero optical path difference in light-focusing path of optics imagery system - Google Patents

Splitter with zero optical path difference in light-focusing path of optics imagery system Download PDF

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TWI269888B
TWI269888B TW94106590A TW94106590A TWI269888B TW I269888 B TWI269888 B TW I269888B TW 94106590 A TW94106590 A TW 94106590A TW 94106590 A TW94106590 A TW 94106590A TW I269888 B TWI269888 B TW I269888B
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Taiwan
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light
mirror
optical
path
hole
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TW94106590A
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Chinese (zh)
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TW200632375A (en
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Da-Jung Shen
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Da-Jung Shen
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Abstract

This invention relates to an optics imagery system. It focuses a splitter with zero optical path difference in light-focusing path. It is constituted from a splitter inserted between an object lens of a light-focusing path and a focal point F'. The splitter is a reflector with a through hole at its center. The axis line of the through hole coincides with the optical axis. It forms an acute angle with the reflection plane of the reflector, and the reflector with the through hole is removed from the light path such that light beams passing through the object lens fully come in the light path for visual observation to provide sufficient luminance inside the visual field. When the reflector with the through hole, it removes from the light path splits light beams to follow two paths. One of the two paths goes through the through hole at the center of the reflector to reach the object lens for visual observation, while the other path through the reflection of plane outside the through hole, it reaches an image sensor for digital photographing. When it moves in and out the light-focusing path in a transition process, the splitter is zero optical path difference. Eventually, it avoids the object lens refocusing.

Description

'1269888 修」 曰 五、發明說明(1) 【發明所屬之技術領域】 本發明係提供一種夯璺古 差分光裝置,π用於望遠鏡广:會:光路中的無光程 以無光程差分光為其特徵,在^、兄、瞄準鏡等器材上, 方便。 使目現硯察和數位照相之切換更加 【先前技術】 在普通光學目苗準的望遠鏡中, 和捕捉Μ票,這種望遠鏡只能用於直目鏡中觀察 路原理如第一圖所示,係以平 :不照相,其光 點F,的焦平面上,人眼3在目物鏡1成像在位於焦 日^在目鏡2中進行瞄準 為了使望遠鏡不僅具有瞄準 =不。 能,需要在第-圖的焦點F,前播入::分二:兼具照相的功 光面上分成二路,其中,—路透射到目J H線在分 準觀察’ “-路則反射至影像傳感器7:如第二於圖人:猫 圖,射入平行光線通過物鏡丨後,合/鏡^的光路原理 F,的焦平面上,第_ i j傻\ s水成像在通過焦點 圖不在物鏡1和焦點F’間插入一傳統的立t路原理圖, 該分光鏡由二塊直角鏡6膠 =鏡分光鏡, *分光膜5,使光線在分光面上間=面上錢 -路反射。而加人立方稜鏡分光鏡後-路透射,另 射率η,與空氣的折射#n不同(一般情況於刀光稜鏡的折 η接近1 ’而玻璃的折射率〇,約為h5左’,氣的折射率 」,因此在光路[1269888 修修] 曰五、发明说明(1) [Technical Field of the Invention] The present invention provides an ancient differential optical device, π is used for telescopes:: no optical path in the optical path with no optical path difference Light is its characteristic, convenient in equipment such as ^, brother, sight, etc. To make the switching between digital observation and digital photography more [previous technique] In the telescope of ordinary optical target, and to capture the ticket, this telescope can only be used in the observation of the straight eyepiece as shown in the first figure. Line up: not photographed, its focal point F, on the focal plane, the human eye 3 is imaged in the objective lens 1 at the focus of the day ^ in the eyepiece 2 to aim in order to make the telescope not only have aiming = no. Yes, need to be in the focus of the first picture F, before the broadcast:: two: the photographic light surface is divided into two, where - the road is transmitted to the eye JH line in the observation of the observation - "- road reflection To the image sensor 7: as the second picture: cat picture, after entering the parallel light through the objective lens, the optical path principle F of the combination / mirror ^, on the focal plane, the first _ ij silly \ s water imaging in the through focus map A conventional vertical t-way schematic is not inserted between the objective lens 1 and the focal point F'. The spectroscope consists of two right-angle mirrors 6 glue = mirror spectroscope, * split film 5, so that the light is on the spectroscopic surface = face money - Road reflection. Adding a cubic 稜鏡 splitter post-channel transmission, the other rate η, is different from the air refraction #n (generally the η of the knife 接近 is close to 1 ' and the refractive index of the glass is 〇, about For h5 left ', the refractive index of gas", so in the light path

第5頁 Π69888 案號 94106590 五、發明說明(2) 中’若分光鏡的厚度為L n’ = L/1· 5=0· 67L ,與不 n,即成像面向後 度越大,光程差也越大, 數位望遠鏡可以利用 與焦點F’間插入一立方稜 分光鏡分光面上分成二路 準觀察,另一路反射到光 二圖所示。在立方稜鏡分 —種是將分光鏡固定在會 動或轉動機構將分光鏡安 光路來實現單純觀察與瞄 “ 針對現有技術,從分 光鏡有以下之問題點: 其一,所需尺寸大, 作’且精密的稜鏡材料成 其二’鍍分光模易產 其三,因尺寸大,移 光程差。 ^立方稜鏡分光鏡的 =論目苗準觀察或照相分光 鏡的光線就要分為二部分 二能損失較大,將會影響 使用目苗準照相功能時需 修正 ’通過厚度為L玻 加入分光鏡時的 移〇 · 3 3 L的距離· 成像面需移動的 以上分光原理來 鏡分光鏡,使透 ,一路透射到達 學影像傳感器, 光鏡的設置上, 聚光路中,第二 置在望遠鏡中, 準照相之間的功 光鏡本身來看, 璃的光程為L / 光程差AzL-L/ 3該分光棱鏡的厚 距離也越大。 實現,即在物鏡 過物鏡的光線在 目鏡’由人眼目苗 用於照相,如第 有兩種方式,第 種疋採用一個移 透過移入、移出 能切換。 採用立方稜鏡分 分光面,鍍分光模,不容易 本相當1¾。 生顏色失真及光線的損耗。 入、移出光路時,备 曰產生較大的 兩種設置方式來看, 鏡均固定在光路中,;接種方式 ,分別用於瞄準觀R 7水透過物 卞現祭和昭如 ^ 觀察和照相的效果。Μ 使 將分光鏡移入光跋 種方式 路,而在使用單Page 5 Π 69888 Case No. 94106590 V. Invention Description (2) If the thickness of the beam splitter is L n' = L/1· 5=0·67L, and no n, that is, the larger the image orientation, the optical path The difference is also greater. The digital telescope can be divided into two directions by using a cubic prism beam splitter between the focus F' and the other side to reflect the light. In the cube, the spectroscope is fixed in the moving or rotating mechanism to separate the optical path of the spectroscope to achieve simple observation and aiming. For the prior art, the following problems are solved from the spectroscope: First, the required size is large. , 'and the precision of the bismuth material into the second' plated optical mode is easy to produce three, due to the large size, the optical path is poor. ^Cubic 稜鏡 稜鏡 = 论 论 论 论 论 论 论 论 论 论 论 论 论 论 论 论It is necessary to divide into two parts and the second energy loss is large, which will affect the use of the target seeding function. It is necessary to correct the movement when the thickness of the beam is added to the beam splitter. · 3 3 L distance · The above splitting of the imaging surface to be moved The principle is to mirror the beam splitter, make it transparent, all the way to reach the image sensor, the light mirror is set, the spotlight is in the way, the second is placed in the telescope, and the light path between the quasi-photographs itself, the optical path of the glass is L / optical path difference AzL-L / 3 The thicker distance of the dichroic prism is also greater. Realization, that is, the light in the objective lens of the objective lens in the eyepiece 'is used by the human eye seedlings, as the first two ways, the first kind Using a shift The shifting can be switched. The splitting of the split surface and the splitting of the optical mode are not easy. The color distortion and the loss of light. When entering and removing the optical path, the preparation of the larger two ways is The mirrors are fixed in the light path; the inoculation method is used to aim at the R 7 water permeate and the effect of observation and photography. Μ Move the spectroscope into the light path, and use the single

ΙΒΒ 第6頁 ill ^1269888 五、發明說明(3) 純觀察功能時可將分光鏡移出 失,使單純觀察變的更加、、主姑 。這樣雖能減少光能損 出,在目視觀察光路中產光,由於分光鏡的移入、移 調焦。顯然兩種方式均存在明:=生又使目鏡需要重新 【發明内容】 、 、失。 本發明之主要目的,在於 光路中的無光程差分光裝置,、直係:=學成像系統會聚 和移出過程中,於物鏡與目鏡:間反射鏡移: 論用於觀察或照相切換過程中生變化隹不 使用上更為簡易方便。 兄白不而要重新調焦, 為了達成上述之目的,本發明係提供一 統會聚光路中的益光裎#八亦壯 種先子成像糸 鏡與焦點之間的;光鏡構:入會聚光路物 反射鏡中心有,,該通孔的射鏡盘; 射鏡的反射面成銳角設置,另該通孔二=2二 與物鏡成像光束在反射鏡上所截光斑面^ ^的區域面積 圍内。 咐筑上所截元斑面積之比在5%〜30%範 【實施方式】 有關本發明之特徵及技術内容,請參閱以下之 ’而所附圖式僅提供參考與說明’並非對本 發明加以限制者。 τ伞 请茶閱第七圖所示,係為本發明應用於數位望 的無光程差分光裝置,由一插入會聚光路物鏡丨與焦點兄丁 F之間的分光鏡所構成,本實施例之分光鏡係為一反射鏡 m 第7頁 1269888 修正 案號 94106590 五、發明說明(4) J,如第四圖及第五圖所示,該反射鏡8中心設有一 ’ 通孔9的轴線與光轴12重合,並與反射鏡8的反射面 ^45度夾角。該反射鏡8係可由平板破璃或其他材料所製 成,其反射面鍍有全反射膜10(如第四圖所示);而註$ 接收器7係設於反射鏡8鍍有全反射膜丨〇之一側邊上,Λ =該 =射鏡8中心通孔9的孔徑d尺寸,按照通孔9所圍設成的: 域面積和物鏡i成像光束在反射鏡8上所截光斑面積之比值 ,一般在5%〜30%範圍内,通常皆取1〇%左右,因在5%〜3〇% 之範圍内時,方能確保分光後之影像接收器7上之光亮度 均勻;當該比值大於30%以上時,影像接收器7上的成彳象"會 因通孔9孔徑的增加而產生切割現象,(即通孔9過大切割曰 了主要光線),而呈現光線亮、暗不均勻的差異,並造成 像場中央之影像遺失或令像場之四角產生缺角現象,根本 不能應用在影像系統上;此外,其比值大於3〇%以上時, 更將使付反射鏡8之體積加大、重量變重、成本高、製作 困難、、等諸多問題。另當該比值小於以内時,將導致 衫像接收杰7然法成像’在影像糸統上無任何利用價值。 為了使數位遂鏡同時具有單獨觀察和聪準照相兩種功 能,該反射鏡8由一移動或轉動機構支撐,並在移入和移 出光路二種工作狀態之間進行切換。 本發明工作原理是:將中心有通孔9之反射鏡8移入光 路,如第六圖A所示,光路中心部份的光線通過中心通孔 9,到達焦面,如圖中的陰影部分。其餘大部分光線由反 射鏡8之中心通孔9外的光斑反射面反射,構成另一路光ΙΒΒ Page 6 ill ^1269888 V. Inventive Note (3) When the pure observation function is used, the spectroscope can be removed and lost, so that the observation alone becomes more and more, and the aunt. In this way, although the light energy loss can be reduced, the light is generated by visual observation of the light path, and the beam splitter is moved in and out. Obviously, there are two ways to know: = and the eyepiece needs to be re-invented [invention], and lost. The main object of the present invention is to provide a light-path differential optical device in an optical path, a direct system: a convergence and removal process of the imaging system, and an objective lens and an eyepiece: an inter-mirror shift: in the process of observation or photography switching It is easier and more convenient to use it without change. In order to achieve the above objectives, the present invention provides a combination of the 糸 裎 八 八 八 八 八 八 八 八 八 ; ; ; ; ; ; ; ; 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间 之间The center of the object mirror has, the mirror plate of the through hole; the reflecting surface of the mirror is set at an acute angle, and the through hole 2=2 2 and the area of the area where the objective lens imaging beam is cut on the mirror ^ ^ Inside. The ratio of the area of the cut surface of the ridge is 5% to 30%. [Embodiment] For the features and technical contents of the present invention, please refer to the following ', and the drawings only provide a reference and explanation'. Limiter. τ Umbrella please refer to the seventh figure, which is a non-optical-path differential optical device applied to the digital position of the present invention, which is composed of a spectroscope inserted between the objective lens of the converging optical path and the focal point F, this embodiment The beam splitter is a mirror m. Page 7 1269888 Amendment No. 94106590 V. Invention Description (4) J. As shown in the fourth and fifth figures, the mirror 8 is provided with a 'through hole 9' axis. The line coincides with the optical axis 12 and is at an angle of 45 degrees to the reflecting surface of the mirror 8. The mirror 8 can be made of flat glass or other materials, and its reflecting surface is plated with a total reflection film 10 (as shown in the fourth figure); and the receiver 7 is provided with a total reflection of the mirror 8 On one side of the diaphragm, Λ = the size of the aperture d of the central through hole 9 of the mirror 8 is surrounded by the through hole 9 : the area of the area and the spot of the objective lens i imaging beam on the mirror 8 The ratio of the area is generally in the range of 5% to 30%, and is usually about 1%, and the brightness of the image receiver 7 after the splitting is uniform can be ensured in the range of 5% to 3%. When the ratio is greater than 30%, the image formation on the image receiver 7 will cause a cutting phenomenon due to an increase in the aperture of the through hole 9, (ie, the through hole 9 is too large to cut the main light), and the light is present. The difference between bright and dark unevenness, and the loss of the image in the center of the image field or the cornering of the four corners of the image field cannot be applied to the image system at all; in addition, when the ratio is greater than 3〇%, it will be paid more. The mirror 8 has a large volume, a heavy weight, a high cost, difficulty in production, and the like. In addition, when the ratio is less than or less, it will cause the shirt to be imaged without any use value on the image system. In order to have both the digital observation and the smart camera function, the mirror 8 is supported by a moving or rotating mechanism and switches between two operating states of moving in and out of the optical path. The working principle of the invention is to move the mirror 8 with the through hole 9 in the center into the optical path. As shown in Fig. A, the light in the central portion of the optical path passes through the central through hole 9 to reach the focal plane, as shown in the shaded portion in the figure. Most of the remaining light is reflected by the spot reflection surface outside the center through hole 9 of the mirror 8, forming another path of light.

Ί269888 五、發明說明(5) . 、= 如第六圖B所示陰影部分。從第六圖A及B比較可以看 〜’兩路光線從分光面到達成像面的距離相等,即L j L 2。當單獨用於目視瞄準觀察時,將反射鏡8移出光 I立此日守通過物鏡1 2 3的光線不受反射鏡8中心通孔9限制, _^成像在目鏡2 (如第七圖所示)視場内’能夠獲得足書 路儿又D ▲用於照相時,將中心有通孔9的反射鏡8移入光 此日守’光線分成兩部分,通過中心通孔9部分的光線 八並在目鏡2視~ ’用於目視觀察,見第六圖A中的陰影部 其餘部分光線經反射面反射,有左右的光能射二二 立傳感器7,有足夠的光能用於照相,見第六圖b中的 = ^ 甲心有通孔9的反射鏡8移入和移出光路的整個過 壬中,目視觀察光路的光程不發生變化,因而可得一 1 ^ 程差的分光裝置。 …、尤 八第〇圖為第七圖中的A向分光光束分布圖,圖中陰$ 砟7刀表示反射光束截面1 1。 本發明除了用於數位望遠鏡外,也能用於 會聚亦改rb 、土 、他類似的 路中’達到分光切換時無光程差的目的。 此外’依據本發明之光學成像系統會聚光路 程差分光萝罟 ^ _ 略干的無光 刀7t衣置,至少具有以下諸多之優點: 造生產、只要 射膜即矸進行 反射膜,不產 一塊中間有通 光路分光。 生分光顏色失 之分光鏡易於製 ’ 一面鍍有全反 之分光鏡只鍍全Ί 269888 V. Inventive Note (5) . , = As shown in the shaded part of Figure B. From the comparison of the sixth figure A and B, it can be seen that the distance between the two paths of light from the spectroscopic surface to the imaging surface is equal, that is, L j L 2 . When used alone for visual aiming observation, the mirror 8 is moved out of the light I. The light passing through the objective lens 1 2 3 is not restricted by the central through hole 9 of the mirror 8, and is imaged in the eyepiece 2 (as shown in the seventh figure). In the field of view, 'there is a book that can be obtained. D ▲ is used for photography. The mirror 8 with the through hole 9 in the center is moved into the light. The light is divided into two parts, and the light passing through the center through hole 9 is eight. In the eyepiece 2 view ~ 'for visual observation, see the rest of the shaded light in the sixth picture A is reflected by the reflective surface, there are left and right light energy to shoot the two vertical sensor 7, there is enough light for photography, see In the sixth figure b, the mirror 8 having the through hole 9 is moved into and out of the entire optical path of the optical path, and the optical path of the optical path is not visually observed, so that a spectroscopic device with a step of 1 ^ can be obtained. ..., especially the eighth diagram is the distribution diagram of the A-direction beam splitter in the seventh diagram, in which the yin 砟7 knife represents the reflected beam section 1 1 . In addition to being used for digital telescopes, the present invention can also be used for convergence and rb, soil, and his similar roads to achieve the goal of no optical path difference when splitting. In addition, the optical imaging system according to the present invention can collect the light path differential light 罟 罟 ^ _ slightly dry matt knives 7t clothing, at least has the following advantages: production, as long as the film is 矸 矸 reflective film, does not produce a middle There is a light path splitting. The splitter color is lost, the spectroscope is easy to make ‘ one side is plated with all-reflective beamsplitter only plated

1 ·本發明 孔的平板破璃 2 ·本發明 3 真現象。 1269888 _案號 94106590_年月日__ 五、發明說明(6) 3 .本發明之分光鏡移入、移出光路時,不產生光程 差,在目視觀察時不需要再重新調焦。 綜上所述,當知本發明之光學成像系統會聚光路中的 無光程差分光裝置已具有產業利用性、新穎性與進步性, 又本發明之構造亦未曾見於同類產品及公開使用,完全符 合發明專利申請要件,爰依專利法提出申請。 惟以上所述僅為本發明之較佳可行實施例,並非因此 即拘限本發明之專利範圍,故舉凡運用本發明說明書及圖 式内容所為之等效結構變化,或直接或間接運用於其他相 ^ 關之技術領域,均同理皆包含於本發明所涵蓋之範圍内, 合予陳明。1 · The flat glass of the hole of the present invention 2 · The present invention 3 true phenomenon. 1269888 _ Case No. 94106590_年月日日__ V. Invention Description (6) 3. When the beam splitter of the present invention moves in and out of the optical path, no optical path difference is generated, and it is not necessary to refocus the lens when visually observed. In summary, it is known that the optical pathless optical device in the optical path of the optical imaging system of the present invention has industrial applicability, novelty and advancement, and the structure of the present invention has not been seen in similar products and is used publicly. In accordance with the requirements of the invention patent application, the application is filed in accordance with the Patent Law. However, the above description is only a preferred embodiment of the present invention, and is not intended to limit the scope of the invention, so that the equivalent structural changes of the present specification and drawings may be applied directly or indirectly to other The technical fields of the related art are all included in the scope of the present invention and are combined with Chen Ming.

第10頁 1269888 j號 94106590 圖式簡單說明 【圖式簡單說明 f一圖係、習知望遠鏡光路原理圖。 弟一圖A係習知移出分光鏡時的望遠鏡光路 ^圖B係、習知移人分光鏡時的望遠鏡光路原 弟一圖 係習知數位望遠鏡原理圖。 第四圖 係本發明有通孔反射鏡的剖視圖。 第五圖 係第四圖的左視圖。 第六圖A係本發明無光程差分光原理圖(一)。 第六圖B係本發明無光程差分光原理圖(二)。 第七圖 係本發明應用於數位望遠鏡時的光路原理圖 第八圖 係第七圖中的Α向分光光束分布圖。 月 曰Page 10 1269888 j No. 94106590 Simple description of the diagram [Simplified description of the diagram f-picture system, the schematic diagram of the light path of the conventional telescope. Figure 1A shows the optical path of the telescope when the spectroscope is removed. Figure B shows the schematic diagram of the telescope optical path when the conventional beam splitter is used. Fourth Figure is a cross-sectional view of a through-hole mirror of the present invention. The fifth figure is the left view of the fourth figure. Fig. 6 is a schematic diagram (1) of the optical pathless differential light of the present invention. Figure 6B is a schematic diagram of the optical pathless differential light of the present invention (2). Fig. 7 is a schematic diagram of the optical path when the present invention is applied to a digital telescope. Fig. 8 is a distribution diagram of the pupil beam splitting beam in the seventh figure. Month

复JL 明 說 號 符 件1 元明1 要發鏡 主本物 [[ 人眼3 分光膜5 影像傳感器7 通孔9 反射光束截面11 目鏡2 光程差4 直角稜鏡6 反射鏡8 全反射膜1 0 光轴1 2Complex JL Ming said the symbol 1 Yuan Ming 1 to send the mirror main object [[ human eye 3 split film 5 image sensor 7 through hole 9 reflected beam section 11 eyepiece 2 optical path difference 4 right angle 稜鏡 6 mirror 8 total reflection film 1 0 optical axis 1 2

第11頁Page 11

Claims (1)

1269888 -------—Έ. 申请專利範圍 1 · 一種光 置,由一設於 其中,所述分 该通孔的軸線 角,另該通孔 鏡上所截光斑 2.如申請 路中的無光程 反射面之夾角 3·如申請 光路中的無光 構成,且其反 4·如申請 路中的無光程 機構支撐,並 換。 5·如申請 路中的無光程 中。 6·如申請 路中的無光程 積與物鏡成像 學成像 會聚光 光鏡為 與光轴 所圍設 面積之 專利範 差分光 為45 0 專利範 程差分 射面鑛 專利範 差分光 在移入 專利範 差分光 專利範 差分光 光束在 日_ifi___ 系統會聚光路中的無光程差分光裴 路物鏡與其焦點之間的分光鏡構成, 反射鏡,該反射鏡中心有一通孔, 重合’並與反射鏡的反射面形成失 成的區域面積與物鏡成像光束在反射 比在5 %〜3 0 %範圍内。 圍第1項所述之光學成像系統會聚光 裝置,其中該反射鏡之通孔的轴線與 〇 圍第1或2項所述之光學成像系統會聚 光裝置’其中該反射鏡由平板鏡片所 有全反射膜。 圍第1項所述之光學成像系統會聚光 裝置,其中該反射鏡由一移動或轉動 和移出光路二種工作狀態之間進行切 圍第1項所述之光學成像系統會聚光 裝置,其中該反射鏡固定設置在光路 圍第1項所述之光學成像系統會聚光 裝置,其中該通孔所圍設成的區域面 反射鏡上所截光斑面積之比為1 〇 %。1269888 --------Έ. Patent Application No. 1 · An optical device, wherein one is disposed therein, the axis angle of the through hole is divided, and the spot on the through hole mirror is cut. The angle of the non-optical reflection surface in the middle is as follows. For example, the application of the optical path in the light path is not necessary, and the reverse is performed as in the application of the non-optical path mechanism in the road. 5. If you apply for no light path in the road. 6. If the application of the pathless optical product and objective lens imaging is concentrated, the optical lens is the patented differential light with the area enclosed by the optical axis. The patented differential range surface mining patent differential light is transferred into the patent. The parametric differential optical patent differential light beam is formed by a beam splitter between the objective lens and the focus of the optical path in the convergence path of the _ifi___ system. The mirror has a through hole in the center of the mirror, which coincides with and reflects The reflective surface of the mirror forms a region of the lost region and the objective lens imaging beam has a reflectance in the range of 5% to 30,000. The optical imaging system of the first aspect of the present invention, wherein the mirror of the through hole of the mirror and the optical imaging system of the first or second aspect of the mirror converge the light device, wherein the mirror is owned by the flat lens Total reflection film. The optical imaging system of claim 1, wherein the mirror is separated by a moving or rotating and moving out optical path, wherein the optical imaging system concentrating device according to item 1 is The mirror is fixedly disposed in the optical imaging system concentrating device according to item 1 of the optical path, wherein the ratio of the area of the spot on the area mirror surrounded by the through hole is 1%. 第12胃 -1269888 案號94106590 年月日 修正The 12th stomach -1269888 case number 94106590 第3頁Page 3
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