TWM364878U - Image forming apparatus for coating substrate - Google Patents

Image forming apparatus for coating substrate Download PDF

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Publication number
TWM364878U
TWM364878U TW97215929U TW97215929U TWM364878U TW M364878 U TWM364878 U TW M364878U TW 97215929 U TW97215929 U TW 97215929U TW 97215929 U TW97215929 U TW 97215929U TW M364878 U TWM364878 U TW M364878U
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Taiwan
Prior art keywords
light
film
coated substrate
substrate
image
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TW97215929U
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Chinese (zh)
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Chi-Sheng Hsieh
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Chi-Sheng Hsieh
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Priority to TW97215929U priority Critical patent/TWM364878U/en
Publication of TWM364878U publication Critical patent/TWM364878U/en

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Description

M364878 八、新型說明: 【新型所屬之技術領域】 本新型涉及-種成像裝置,侧是涉及-種鍍有對可見光呈現高 *反射、低穿透與對紅外呈現高穿透的多層介電質膜層成像。 …【先前技術】 近年來’全球各地治安雜、歐美地區的恐怖活動摊造成政府 _ a共权施上要女裝更多的文全監視攝職(知⑶⑽camera),用以 對惡徒進行適當的防患與嚇阻,例如在社區、都會區街道、賣場與其 他的公共場所等’遇有竊盜、性侵或重大事件時可由監麵影機所攝 錄的影像加以觀察與還原真相狀況。 但是’科技的進步連帶使得竊賊惡徒或恐怖份子們的惡行知識與 技巧也有所進步’明顯的例子是偷竊破壞監視攝影機或刻意迴避各處 監視地點。因此,防盜監視型的偽裝隱藏(c〇ncea|ed Camera)攝影 φ 裝置是現在歐美與全球其他國家地區迫切需求的安全裝置,尤其是對 於美國911事件後的公共安全防護領域,與美國國土安全部宣告的「公 共安全重於個人隱私」更為明顯。 對於偽裝隱藏攝影裝置,有利用一透明基材鍍上金屬薄膜的遮罩 用以遮住攝影機,入射光入射到金屬薄膜時分為兩道光,大部份的一 道光在金屬薄膜正表面反射呈現亮麗鏡面可以隱藏遮住攝影機,另外 小部份的一道光在金屬薄膜表面透射進入攝影機鏡頭成像。為了減少 遮罩造成的反光又再次入射到攝影機鏡頭形成重疊的鬼影,影響成像 品質,常加入一因應的金屬抗反射膜層。 5 M364878 例如’本人於2007年創作的中華民國新型專利證號 銘半球型罩攝影裝置」、與2007年創作的中國大陸公開的實用新型專 利200720154044.5「具減反射膜鍍鋁鏡面的攝影用半球型遮罩」等, 均是在一透明基板的正面鍍高反射的金屬薄膜,藉正面入射光的反射 ••用以遮住(隱藏)攝影機,以及在一透明基板的背面鍍抗反射的金屬 薄膜,用以吸收與減少鍍膜遮罩内的反光,以免影響鍍膜遮罩内攝影 機攝影的品質。 鍍反射膜,主要是增加光學表面的反射率❶一般可分為兩大類, 一類是金屬反射膜’一類是全介電質反射膜。此外,還有把兩者結合 起來的金屬介電質反射膜。 金屬反射膜的優點是製備工藝簡單,工作的波長範圍寬;缺點是 光損耗大,反射率不可能很高。 金屬膜(Metalliccoatings)反射帶比較寬,對入射光角度相對不 敏感。金屬膜對紅外有吸收帶,不利紅外夜視攝影。 多層介電質(dielectric coatings)膜,在特定波長可以達到很高 的反射率,對入射光小角度不敏感,當大角度變化時(如45度),反 射率將變化很大。一般說來,介電膜比金屬膜反射率高,牢固度好, 抗損傷力強,在可見光與紅外呈透明狀。 6 M364878 【新型内容】 本創作所要解決的問題有: (1) 如何提尚鍍膜基板的反射率,以及可同時提高其穿透率? (2) 如何使鍍膜基板在紅外範圍的有很高(观以上)的穿透 •.率? (3) 如何使賴基板的背面具有衰減反光姐,改善鍛膜基板 背面取像單元的成像品質? 本創作所採取的技術方案是: 在-透明基材上錄有-多層介電質膜與_金屬膜層取代先前技術 上透明基材上所鍍有的金屬膜。 透明基材,透明基材大約可分為光學級的透明玻璃與透明樹脂兩 大類。透明基材首先必須有高透明度,必然要求表面質量要求嚴格, •盡量不要有任何斑紋、氣孔、泛白、霧暈、黑點、變色、粗糙光澤不 佳等缺陷《>可見光與紅外在透明基材的透明性,一般同樣是受到「光」 的反射、穿透、吸收、與散射等因素影響。 在一透明基材上鍍有一多層介電質膜與一金屬膜層。 多層介電質膜’今日在薄膜光學上,我們很容易由向量法或導納 軌跡法在光學級透明基板上,鍍折射率高低交互變化的多層四分之一 波膜堆,可獲得預期的穿透率T%。而且理論上也同時可以證明用相 同多膜層數,四分之一波膜堆比非四分之一波膜堆所得到的反射率 7 M364878 R°/〇要高。而膜層數越多則反射率也越大。也就是說,很容易控制穿 透與反射的分光比例。在目前現有可用的鍍膜材料中,在可見光區高 折射率小於等於2.4而低折射率大於等於1. 35,所以單一的四分之一 …波膜堆的高反射帶的寬度是有限的。因此,要滿足本實施例在可見光 …區能夠像金屬膜一樣有較寬的反射帶,有必要將介電質膜高反射帶拓 寬。有關鍍膜的設計基本上可從標準膜系開始著手,例如高反射鏡不 管波寬大小或單或雙波數,都一律以四分之一波膜堆基礎來設計。 當初始設計無法滿足需求的光學成效時,就利用目前商用設計的 電腦軟體來優化或合成。 如後面實施例的圖四所示,本實施例多層介電質膜中採用的鍍模 材料是氧化物膜’以Ti3〇5與Si〇2兩種折射率高低不同的膜材在鍍膜 機内交替蒸鍍18層。 _ 金屬膜層,本實施例金屬膜層中採用的鍍模材料有吸收入射光的 金屬鉻Cr。 請參閱圖一為本創作裝置設計的示意圖。 如圖一所示包含有一鍍膜基材1、一殼體2與一 CCD攝影機3。 鍵膜基材1又包含有一透明基材la、一多層介電質膜層(以下簡 稱介電質膜層Mb與—金屬膜層lce 殼體2為一不透光容器,殼體2有一開口侧,開口侧放置有一鍍 8 M364878 膜基材1 ’殼體2内部收納有一 CCD攝影機3,其中CCD攝影機3 的鏡頭31對準鍍膜基材1的背表面(錢有金屬膜層ic的面)。 圖一所示也包含有便利說明的代表性光線,例如入射光L1、反射 光Lla、以及透射光Lib、Lie、Lid、與Lie等。 如圖一所示,入射光L1入射到鍍膜基材1產生一分光效果。入射 光L1分一部份在鍍膜基材1正表面反射為反射光Lia,另分一部分穿 參透鍵膜基材1後變成透射光Lie進入CCD攝影機3的鏡頭31成像。 假設入射光L1的光能量比為1〇〇〇/0。 當反射光Lla>入射光L1的50%時,則可在鍍膜基材1正表面形 成一明顯亮麗的反光鏡面(人眼正看似像一面鏡子)。 本創作期望作到链膜基材1正表面呈現高反射的亮麗鏡面。所 以,本創作設計條件是將Lla設定為60% (大於50%)。M364878 VIII. New description: [New technical field] The new type relates to an imaging device, and the side is related to a multi-layer dielectric coated with high reflection, low penetration and high penetration to visible light. Film imaging. ...[Previous technology] In recent years, 'there are horrific activities in the world, and the terrorist activities in Europe and the United States have caused the government to _ a total of power to apply for more women’s full surveillance surveillance (known (3) (10) camera), to appropriate for the villains Prevention and deterrence, such as in the community, metropolitan streets, stores and other public places, etc. In the event of theft, sexual assault or major events, the images recorded by the surveillance cameras can be observed and restored. . But the advancement of technology has led to improvements in the evil knowledge and skills of thieves or terrorists. A clear example is the theft of surveillance cameras or the deliberate avoidance of surveillance sites. Therefore, the anti-theft surveillance type camouflage hidden (c〇ncea|ed Camera) photography φ device is an urgently needed security device in Europe and the United States and other countries in the world, especially for the public security protection field after the 9/11 incident in the United States, and the US homeland security. The announcement that "public safety is more important than personal privacy" is more obvious. For the camouflage hidden photographic device, a mask coated with a transparent film on a transparent substrate is used to cover the camera. When the incident light is incident on the metal film, it is divided into two lights, and most of the light is reflected on the front surface of the metal film. The bright mirror can hide the camera, and a small part of the light is transmitted through the surface of the metal film into the camera lens. In order to reduce the reflection caused by the mask and again incident on the camera lens to form overlapping ghosts, affecting the image quality, a corresponding metal anti-reflection film layer is often added. 5 M364878 For example, 'The Republic of China's new patent certificate No. Hemispherical hood photographic device created in 2007', and the Chinese utility model patent published in 2007, 200720154044.5 "Photographic hemisphere with anti-reflection film aluminized mirror surface A mask, etc., is a highly reflective metal film on the front side of a transparent substrate, which is reflected by frontal incident light. • Used to cover (hide) the camera, and to plate an anti-reflective metal film on the back side of a transparent substrate. It is used to absorb and reduce the reflection in the coating mask, so as not to affect the quality of the camera photography in the coating mask. The reflective film is mainly used to increase the reflectivity of the optical surface. Generally, it can be divided into two categories, one is a metal reflective film, and the other is a full dielectric reflective film. In addition, there is a metal dielectric reflective film that combines the two. The metal reflective film has the advantages of simple preparation process and wide working wavelength range; the disadvantage is that the optical loss is large and the reflectance is not high. Metallic coatings are relatively wide and are relatively insensitive to incident light angles. The metal film has an absorption band for the infrared, which is disadvantageous for infrared night vision photography. Dielectric coatings can achieve high reflectance at specific wavelengths and are insensitive to small angles of incident light. When large angles change (eg, 45 degrees), the reflectivity will vary greatly. Generally speaking, the dielectric film has higher reflectance than the metal film, has good firmness, strong damage resistance, and is transparent in visible light and infrared. 6 M364878 [New Content] The problems to be solved in this creation are as follows: (1) How to improve the reflectivity of the coated substrate and increase its penetration rate at the same time? (2) How to make the coated substrate have a high penetration (above) in the infrared range? (3) How to make the back side of the substrate have attenuated reflective light, and improve the image quality of the image pickup unit on the back surface of the forged film substrate? The technical solution adopted by this creation is: On the transparent substrate, a multi-layer dielectric film and a metal film layer are substituted for the metal film plated on the transparent substrate of the prior art. Transparent substrates, transparent substrates can be divided into two categories: optical grade transparent glass and transparent resin. The transparent substrate must first have high transparency, and the surface quality requirements must be strict. • Try not to have any defects such as streaks, pores, whitening, halo, black spots, discoloration, poor luster, etc. > Visible light and infrared are transparent The transparency of the substrate is generally affected by factors such as reflection, penetration, absorption, and scattering of "light." A multilayer dielectric film and a metal film layer are plated on a transparent substrate. Multilayer Dielectric Films Today, in thin film optics, we can easily apply a multi-layer quarter-wave film stack with high refractive index and high refractive index on the optical grade transparent substrate by vector method or admittance trajectory method. The penetration rate is T%. In theory, it is also proved that the same multi-layer number is used, and the quarter-wave film stack has a higher reflectance than the non-quarter-wave film stack of 7 M364878 R°/〇. The more the number of layers, the greater the reflectivity. In other words, it is easy to control the split ratio of penetration and reflection. In the currently available coating materials, the high refractive index in the visible light region is 2.4 or less and the low refractive index is 1.35 or more, so the width of the high reflection band of the single quarter film stack is limited. Therefore, in order to satisfy the present embodiment, it is possible to have a wide reflection band like a metal film in the visible light region, and it is necessary to broaden the high reflection band of the dielectric film. The design of the coating can basically be started from the standard film system. For example, high reflection mirrors are designed on the basis of a quarter-wave film stack, regardless of the width or single or double wave number. When the initial design fails to meet the optical performance of the demand, it is optimized or synthesized using current commercially designed computer software. As shown in FIG. 4 of the following embodiment, the plating material used in the multilayer dielectric film of the present embodiment is an oxide film, and the film having different refractive indices of Ti3〇5 and Si〇2 is alternated in the coating machine. Evaporation of 18 layers. _ Metal film layer, the plating material used in the metal film layer of this embodiment has metal chromium Cr which absorbs incident light. Please refer to Figure 1 for a schematic diagram of the design of the authoring device. As shown in Fig. 1, a coated substrate 1, a casing 2 and a CCD camera 3 are included. The key film substrate 1 further comprises a transparent substrate 1a and a multilayer dielectric film layer (hereinafter referred to as a dielectric film layer Mb and a metal film layer 1ce, the housing 2 is an opaque container, and the housing 2 has On the open side, the open side is placed with a plated 8 M364878 film substrate 1 'The inside of the casing 2 houses a CCD camera 3, wherein the lens 31 of the CCD camera 3 is aligned with the back surface of the coated substrate 1 (the face having the metal film layer ic) Fig. 1 also includes representative light rays which are conveniently described, such as incident light L1, reflected light Lla, and transmitted light Lib, Lie, Lid, and Lie, etc. As shown in Fig. 1, incident light L1 is incident on the coating film. The substrate 1 generates a light splitting effect. The incident light L1 is partially reflected on the front surface of the coated substrate 1 as reflected light Lia, and a part of the light penetrates through the key film substrate 1 and becomes a transmitted light Lie into the lens 31 of the CCD camera 3. It is assumed that the light energy ratio of the incident light L1 is 1 〇〇〇 / 0. When the reflected light Lla > 50% of the incident light L1, a significantly bright mirror surface (human eye) can be formed on the front surface of the coated substrate 1 It looks like a mirror.) This creation is expected to be made on the front surface of the chain film substrate 1. Bright specular highly reflective now. So, this is a creative design conditions Lla set to 60% (greater than 50%).

Lie進入CCD攝影機3的鏡頭31,使CCD攝影機3可以成像。 本創作設計條件是將Lie設定為15%。 也就是說,本創作假設入射光L1為100%時,設計條件是反射光 Lla為60%與透射光Lie為15%。 如圖一,入射光L1為1〇〇〇/0時,反射光Lla為60%與透射光Lie 為15%;則入射光L1在鍍膜基材1上被吸收(光能損失)了 25。/。(為 100%-60%-15%)。 9 M364878 現在’本創作設計條件是反射光Lla & 6〇%、吸收率為25%與透 射光Lie為15%後’有兩個問題待解決: (一) 如何確定透射光L1e的15%能滿足CCD攝職3的成像 條件?以及; ,_ (二) 如何控制鍍膜基材1的吸收率2504 ? 在本創作設計中作以下試驗,用以解說(-)透射光Lie的15% ®能滿足CCD攝影機3成像條件的問題: 實驗室内架設有六支大小不等的曰光燈組,在鍵膜基材)前欲攝 取之物體的環境經由一般照度計顯示照度約28〇Lux。本創作實施例所 採用的彩色CCD攝影機3是-般普通型日製s〇ny的影像感測器 (image sensor),廠商規格書標示最底感應照度1Lux。試驗時穿透 的透射光Lie約有42Lux (即280Lux乘以15%),由彩色CCD攝影 _機3影像輸出端(Video output)可以顯示出物體的影像,一般感應 照度在十倍于最低照度以上時所攝取的影像品質都很不錯。 在實驗室内照度調降至約1〇〇Lux的照度環境下,穿透鍍膜基材i 背後彩色CCD攝影機3的鏡頭31約有i〇〇|_ux*15%=15Lux的進光 量’由彩色CCD攝影機3影像輸出端也可以顯示出物體的影像。 當實驗室_度調_約5GLux町時,麵呈現的物鱧影像是 由彩色轉成黑白(俗稱曰夜型),更甚至有時(稍低階產品)呈現的影 像是具有白點班或不清楚、在a5Lux時一般彩色CCD攝影機3看不 M364878 清物體影像。 所以,所謂Lie的透光率百分比率T% (Transmittance °/〇)設定 為15%時,並非一定剛剛好是15% !尤其對更高階彩色CCD攝影機 3的影像感測器來說,可以設定在10。/。或是更低。目前高階的Sony 彩色CCD攝影機3最低照度有標示在0.005Lux者。 也就是說,使用越高階的彩色攝影機可以採用越低的透光率Lie φ需求。 本創作實施例考慮成本問題,所採用的是一般中低階價位的彩色 攝影機(Color CCD)。又實施試驗發現採用Color Cmos時的透光率 Lie則要調整為25%到35%之間比較適合。 以目前市售的普通型彩色攝影機的影像感測器(Image Sensor) 可感測的最低照度,大約在1Lux。有的高階(High end)型約在 籲0.01〜0.001LUX之間,也有稱為星光級的其低照度約〇_〇〇2Lux。就以 市售低階Cmos的影像感測器也約在2Lux左右。對2Lux的影像感測 器而言,在實驗室内調至約280Lux的照度環境下,上述的42Lu>((即 280Lux乘以15%)進光量對其2Lux的感測度足足有餘。 當所需環境的環境照度下降到影像感測器不足感測時,攝影機的 影像輸出端(Video out)輸出的影像常在影像顯示器(Monitor)上顯 示出帶有雪花狀的斑點造成不良的成像品質,或是無法成像。 這時可在所需環境下(1)更換為更高階(低照度)的攝影機, 11 M364878 或是(2)增加輔助光源(增加入射光L1強度)可以改善成像品質。 這也就是說,透射光Lie為15%,並非一定要剛剛好是15%的理由! 所以,透射光Lie的15%能否滿足CCD攝影機3的成像條件, 入射光L1的大小(強弱)與CCD攝影機3的影像感測器品質均是關 鍵因素8 當然,透射光Lie大於15%時,也就是說越大越可取得更佳成像 φ品質。若越接近入射光100%乃最理想最好,但透射光Lie提高,就 使反射光Lla降低。因為對L1來說Lla與Lie互為反比,Lla大Lie 則小,Lla小Lie則大。反射光Lla降低其鏡面反射效果就變差,失 去隱藏裝飾意義。如何拿捏主要是視使用環境照度與取像單元品質而 定。 接下來,說明(二)如何控制鍍膜基材1吸收率在25%的問題。 事實上,如圖一所示鍍膜基材1的光學現象並非僅有反射光Lla、 與透射光Lib、Lie、Lid、Lie等這樣簡單。例如像Lib在透明基材 la與介電質膜層lb之間的介面也會有無數的反射光反射到介電質膜 la内,再經透明基材la透射出去等等涉及複雜數學計算。為簡化說 明就將這些無數的反射光、透射光等複雜數學計算給予省略。 如圖一,反射光L1的光能量穿透到透明基材la後剩餘為Lib, Lib再穿透到介電質膜層lb後剩餘為Lie,Lie再穿透到金屬膜層lc 後剩餘為Lie。最後,在殼體2内有入射光L1轉變成的透射光Lie。 12 M364878 這透射光Lie就是攝影機3成像所須的光源。 簡單以數學式表示鍍膜基材1的吸收率A%為: A%=L1b+L1c+L1d=25%。 ' 也就是說,考慮到透明基材la、介電質膜層lb與金屬膜層lc等 各介質内的吸收或光能損失就可’對於很複雜的各介質與各介質介面 上的光學現象則因影響本實施例所涉及的成像品質不明顯,故可忽略 鲁不計。 由於透明基材la的透明需求、介電質膜層ib膜材的對可見光與 紅外的呈現的透明,對上述的A%=L1b+L1c+L1d=25%,可簡化為; A0/〇= L1d=25%。 也就是說,控制金屬膜層lc的鍍膜厚度就可控制鍍膜基材1的吸 _收率A%。 在一透明基材la上鍍完一多層介電質膜ib與一金屬膜層lc後, 經曰本Hitachi光譜儀U-4100測試與自動繪出的光譜圖如圖四曲線 4A1所示,在可見光400nm〜700nm部份的穿透率τ%平均在27.1%, 反射率R%平均約在56% (如圖五)。而在紅外780nm〜1,000nm部 份的穿透率T%平均約在75%。 也就是說,一透明基材la上鍍完一多層介電質膜ib與一金屬膜 層lc後形成的鍍膜基板1,對一單純的入射光來說此鍍膜基板1 : 13 M364878 (1) 其56%的反射率R%在此鍍膜基板1的正面形成一鏡面高 反射(好像一面鏡子)9 (2) 其27%的穿透率T%使鍍膜基板1背面的攝影機成像。 .- (3 )其17% ( 100%-56%-27% )的吸收率使鍍膜基板1背面不 必要的反光被吸收以免反光成像造成鬼影而影響攝影品質》 (4)其75%的紅外穿透率T%,使鍍膜基板1背面的攝影機可以 鲁攝取紅外影像。 由(1)~(4)的參數可知本創作所採取的技術方案所預期的功效。 其中,如(3)其17%的吸收率實際上是鍍金屬膜層1c的關係。 如果鍍膜基板1僅鍍上一多層介電質膜lb而不鍍金屬膜層時,這 17%的損耗(一)可加入在此鍍膜基板i的56%反射率r%上,使此 反射率變成73% (56%+17%)、或(二)可加入在此鍍膜基板1的 籲27%的穿透率τ%上,使此穿透率變成44% (27%+17。/〇)、或(三) 可分別(等比例或不等比例)加入在此鍍膜基板i的反射率R%與穿 透率T%上。這也就是鍍多層介電質膜比鍍金屬膜層的另一好處。 問題是,又要解決鍍膜基板1的背面具有衰減反光功效,改善鍍 膜基板1背面取像單元成像品質的問題? 在後面實施例介紹有二個方法: 第- ’在攝影鏡頭31外圍套入一不透光的黑色軟套32,把鍍膜基 14 M364878 板1背面的反光擋住。 第二,在鍍膜基板1背面安置於一殼體2,並在殼體2的内部表面 形成有黑色或深色的粗糙表面,用以吸收與散射掉穿透鍍膜基板1背 面的反光。 所以,在鍍膜基板1上不採取鍍金屬膜時’也可以採用上述的 二個方法。 ® 本創作所採取的技術方案與特徵的技術效果: 本創作的效果之一,對同一入射光而言,因為金屬膜對光能損耗 相對較大,故以鍍多層介電質膜取代鍍金屬膜可以提高其反射率,使 鍵膜基板的正表面呈現亮麗高反射鏡面,用以隱藏裝飾鍍膜基板背表 面的取像單元。 本創作的效果之二,經過鍍膜基板1透射的可見光與紅外均可使 _鍵膜基板1背表面的取像單元3成像。 +本創作的效果之三’義基板1背;所產生不必要的反光給予 衰減(吸收)掉’用以改善取像單元3的成像品質與隱藏取像單元3 15 M364878 【實施方式】 本實施例的名詞定義如下: 的透明破螭與透明 (1)透明基材la,透明基材ia可分為光學級 樹脂兩大類。 透明基材la的解釋: 透明基材la中光學級的透明玻璃適合採用平 因可容純«贱合採肝錄、㈣料平喊脂Lie enters the lens 31 of the CCD camera 3 so that the CCD camera 3 can be imaged. This creative design condition is to set Lie to 15%. That is to say, this creation assumes that the incident light L1 is 100%, and the design conditions are that the reflected light Lla is 60% and the transmitted light Lie is 15%. As shown in Fig. 1, when the incident light L1 is 1 〇〇〇/0, the reflected light L1a is 60% and the transmitted light Lie is 15%; the incident light L1 is absorbed on the coated substrate 1 (light energy loss) by 25. /. (100%-60%-15%). 9 M364878 Now 'this design condition is that the reflected light Lla & 6〇%, the absorption rate is 25% and the transmitted light Lie is 15%'. There are two problems to be solved: (1) How to determine 15% of the transmitted light L1e Can you meet the imaging conditions of CCD Care 3? And, (2) How to control the absorption rate of the coated substrate 1 2504? In the original design, the following experiment was carried out to explain (-) that 15% of the transmitted light Lie can meet the imaging conditions of the CCD camera 3: The experimental indoor frame is provided with six illuminating light sets of different sizes, and the environment of the object to be ingested before the key film substrate) shows an illuminance of about 28 〇 Lux through a general illuminometer. The color CCD camera 3 used in the present embodiment is an image sensor of a general-purpose Japanese-style s〇ny, and the manufacturer's specification indicates the lowest-intensity illuminance 1 Lux. The transmitted light Lie penetrated during the test is about 42 Lux (that is, 280 Lux multiplied by 15%), and the image of the object can be displayed by the color CCD camera. The general induction illuminance is ten times the minimum illuminance. The quality of the images taken above was very good. In the illuminance environment in which the illuminance is reduced to about 1 〇〇 Lux in the laboratory, the lens 31 of the color CCD camera 3 behind the coated substrate i is approximately i 〇〇 | _ ux * 15% = 15 Lux light amount 'by color The image output of the CCD camera 3 can also display an image of the object. When the laboratory _ _ _ about 5 GLux town, the object image presented by the face is changed from color to black and white (commonly known as day and night type), and even sometimes (slightly lower order products) images are white spots or It is not clear that in the case of a5Lux, the general color CCD camera 3 does not see the M364878 clear object image. Therefore, when the light transmittance percentage ratio T% (Transmittance °/〇) of Lie is set to 15%, it is not necessarily just 15%! Especially for the image sensor of the higher-order color CCD camera 3, it can be set. At 10. /. Or lower. At present, the high-end Sony color CCD camera 3 has the lowest illumination of 0.005 Lux. That is to say, the lower the light transmittance Lie φ demand can be employed using a higher order color camera. The present embodiment considers the cost problem, and adopts a color camera (Color CCD) of a general low-end price. Further experiments have shown that the light transmittance when using Color Cmos Lie is adjusted to be between 25% and 35%. The minimum illuminance that can be sensed by the Image Sensor of a commercially available color camera is about 1 Lux. Some high-end types are between 0.01 and 0.001 LUX, and there are also low-illuminances called 星_〇〇2 Lux. The image sensor of the commercially available low-order Cmos is also around 2 Lux. For the 2Lux image sensor, in the illuminance environment adjusted to about 280Lux in the laboratory, the 42Lu>((ie 280Lux multiplied by 15%) light input amount is more than 2Lux. When the ambient illumination of the environment drops to the sense of insufficient image sensor, the image output from the video output of the camera often displays a snowflake-like spot on the image display (Monitor), resulting in poor imaging quality. Or can't image. At this time, you can change the image to a higher-order (low-illuminance) camera in the required environment (11), 11 M364878 or (2) increase the auxiliary light source (increasing the intensity of the incident light L1) to improve the image quality. That is to say, the transmitted light Lie is 15%, which is not necessarily just 15% of the reason! Therefore, 15% of the transmitted light Lie can satisfy the imaging condition of the CCD camera 3, the size (intensity) of the incident light L1 and the CCD camera 3 image sensor quality is a key factor 8 Of course, when the transmitted light Lie is greater than 15%, that is, the larger the image, the better the image quality can be achieved. If the closer to the incident light 100% is the best, but the transmission Light Lie , the reflected light Lla is lowered. Because L1 and Lie are inversely proportional to L1, Lla is small and Lla is small. Lla reduces the specular reflection effect and loses the hidden decorative meaning. The pinch is mainly determined by the ambient illuminance and the quality of the image taking unit. Next, it is explained how to control the absorption rate of the coated substrate 1 at 25%. In fact, the optical properties of the coated substrate 1 as shown in Fig. The phenomenon is not only the reflected light Lla, but also the transmitted light Lib, Lie, Lid, Lie, etc. For example, the interface between the transparent substrate la and the dielectric film layer lb, such as Lib, may also have numerous reflected light reflected to Complex dielectric calculations are involved in the dielectric film la, and then transmitted through the transparent substrate 1a. For the sake of simplicity, these complicated mathematical calculations such as reflected light and transmitted light are omitted. Figure 1 shows the reflected light L1. After the light energy penetrates into the transparent substrate la, Lib remains, Lib penetrates to the dielectric film layer lb and remains Lie, and Lie penetrates into the metal film layer lc and remains Lie. Finally, in the shell 2 There is a transmitted light Lie into which the incident light L1 is converted. 2 M364878 This transmitted light Lie is the light source required for imaging of the camera 3. The mathematical expression of the absorptivity A% of the coated substrate 1 is: A%=L1b+L1c+L1d=25%. The absorption or loss of light energy in each medium such as the transparent substrate la, the dielectric film layer 1b and the metal film layer lc can be affected by the optical phenomenon on the complicated medium and each medium interface. The image quality involved is not obvious, so it can be ignored. Due to the transparent requirements of the transparent substrate la, the transparency of the visible film and infrared of the dielectric film ib film, the above A%=L1b+L1c+ L1d=25%, which can be simplified as; A0/〇= L1d=25%. That is, controlling the thickness of the plating film of the metal film layer lc can control the absorption rate A% of the plating substrate 1. After plating a multilayer dielectric film ib and a metal film layer lc on a transparent substrate 1a, the spectrum of the Hitachi spectrometer U-4100 is tested and automatically plotted as shown in FIG. 4 curve 4A1. The transmittance τ% of the visible light range of 400 nm to 700 nm averaged 27.1%, and the reflectance R% averaged about 56% (Fig. 5). On the other hand, the transmittance T% of the infrared 780 nm to 1,000 nm portion is about 75% on average. That is, a coated substrate 1 formed by plating a multilayer dielectric film ib and a metal film layer lc on a transparent substrate 1a, for a simple incident light, the coated substrate 1: 13 M364878 (1 The 56% reflectance R% forms a specular high reflection on the front surface of the coated substrate 1 (like a mirror) 9 (2) Its 27% transmittance T% images the camera on the back side of the coated substrate 1. .- (3) The absorption rate of 17% (100%-56%-27%) causes unnecessary reflection on the back side of the coated substrate 1 to be absorbed to avoid ghosting and affecting the quality of photography. (4) 75% of it The infrared transmittance T% enables the camera on the back of the coated substrate 1 to capture infrared images. From the parameters of (1) to (4), the expected efficacy of the technical solution adopted by this creation can be known. Among them, as in (3), the absorption rate of 17% is actually the relationship of the metal plating layer 1c. If the coated substrate 1 is plated with only one multi-layer dielectric film lb without a metallization layer, the 17% loss (a) can be added to the 56% reflectance r% of the coated substrate i to make this reflection The rate becomes 73% (56% + 17%), or (2) can be added to the 27% transmittance τ% of the coated substrate 1 so that the transmittance becomes 44% (27% + 17%). 〇), or (3) may be separately added (equal or unequal ratio) to the reflectance R% and the transmittance T% of the coated substrate i. This is another benefit of plating a multilayer dielectric film over a metallized layer. The problem is that it is necessary to solve the problem that the back surface of the coated substrate 1 has an attenuating reflection effect and the image quality of the image pickup unit on the back side of the coated substrate 1 is improved. In the following embodiments, there are two methods: First - ” An opaque black soft cover 32 is placed around the photographic lens 31 to block the reflection of the back surface of the coated substrate 14 M364878. Secondly, a casing 2 is disposed on the back surface of the coated substrate 1, and a black or dark rough surface is formed on the inner surface of the casing 2 for absorbing and scattering the reflection of the back surface of the coated substrate 1. Therefore, when the metal plating film is not used on the coated substrate 1, the above two methods can also be employed. ® The technical effect of the technical solutions and features adopted by this creation: One of the effects of this creation is that for the same incident light, because the metal film has a relatively large loss of light energy, the plating of the multilayer dielectric film is used instead of the metal plating. The film can increase the reflectance thereof, so that the front surface of the key film substrate presents a bright high mirror surface for hiding the image capturing unit of the back surface of the decorative coated substrate. The second effect of the present invention is that the visible light and the infrared light transmitted through the coated substrate 1 can image the image capturing unit 3 on the back surface of the key film substrate 1. + The effect of the creation of the third substrate is the back of the substrate; the unnecessary reflection is given to the attenuation (absorption) to improve the imaging quality of the image capturing unit 3 and the hidden image capturing unit 3 15 M364878 [Embodiment] This embodiment The nouns of the examples are defined as follows: transparent ruthenium and transparent (1) transparent substrate la, transparent substrate ia can be divided into two major categories of optical grade resin. Explanation of the transparent substrate la: The transparent glass of the optical grade in the transparent substrate la is suitable for the use of flatness and can be purely purely «贱合采肝录, (4)

透明玻璃,透明玻璃有青、或白板玻额Βκ_7等I 玻璃測試效果較佳。 *中以白板 透麵脂,透明樹脂是具光散射少的非結晶體。例如透明 工業用樹脂。 • 透明樹脂或一般透明高分子聚合物,其内部有微細界面,也會發 生光散射,其典型就是結晶結構。 例如同樣是H2〇構成的水和冰。水是透明的,冰多半不透明, 這是因為冰是結晶體,會發生光散射使光透過齡^水是非結晶體, 發生光散射少,故呈現透明。Transparent glass, clear glass with blue, or whiteboard glass forehead Β __7, etc. I glass test effect is better. *In the whiteboard, the transparent resin is a non-crystalline body with less light scattering. For example, transparent industrial resins. • Transparent resin or general transparent polymer with a fine interface inside and light scattering, which is typically a crystalline structure. For example, it is also water and ice composed of H2〇. Water is transparent, and ice is mostly opaque. This is because ice is a crystal, and light scattering occurs. Light is transmitted through the age. Water is amorphous, and light scattering is small, so it is transparent.

在工業用塑料中透明性好的樹脂大約有:PMMA(透明度93%)、 PC (透明度 88% )、PS (透明度 89〇/〇 )、CR-39 (透明度 90% )、SAN 16 M364878 樹脂(透明度90%)、MS樹脂(透明度90%)、聚-4甲基戊烯-(ΤΡΧ) (透明度>90%)。另外,像聚甲烯酸曱酯、苯乙烯共聚物(MAS)、 PET、PP以及PVC等透明度均很好。 上述這些汎用透明樹脂中,其透光性不僅包含波長在 380nm〜780nm的可見光’實際上也涵蓋波長在780nm〜1000nm的 近紅外領域。 • 可見光與紅外在透明樹脂的透明性,一般同樣是受到「光」的反 射、穿透、吸收、與散射等因素影響。 當光進入透明樹脂時,一部份會在表面反射而損失。反射的例子 通常是以光的折射率nl (=1)由空氣垂直射入折射率n2的聚合物時, 所算出的表面反射率R%是以(η-l)的平方除以(n+l)的平方表示 之。資料顯示,透明壓克力(有機玻璃)pmma 籲(Polymethylmethacrylate)的折射率是L49,算出表面反射率RO/〇 約為4%。 PMMA的全透光率約為93%,這種光的損失大部份是表面來回 二次反射造成的,而吸收和散射等内部的損失則非常小。 當光碰到透明樹脂分子後,分子將吸收其能量而發生旋轉運動, 引起光吸收於是降低透紐,在光魏關時發生的散射也會就大大 降低透光性。由於透明樹脂内㈣有的散射係與折射率8乘方成正 比,與波長4乘方成反比,因此,折射率低的材料散射損失少,在波 17 M364878 長較長的可見光領域,散射的影響較小。在波長較長的紅外領域,散 射的影響幾乎小到等於零。這論點是支持本實施例僅就涉及對光的反 射、穿透與吸收等解釋而不論述較複雜的散射現象。 而且’透明樹脂或一透明高分子聚合物在製造過程產生或是參入 的一些異物,也會因為散射而降低透光性。由製造廠商資料顯示,光 學級的PMMA的異物僅有一般成型用pmmA的十分之一,異物粒徑 魯在0.5叩~0.〇7抑時,光學級PMMA的異物量約為600〜2000個/g, 一般級PMMA的異物量約為4000〜20000個/g。這也就是本實施例建 議使用光學級PMMA的原因。在實際應用上,有時因為環境的溫度和 溼度的變動,也大大影響折射率。一般來說,透明樹脂的折射率愈大, 則反射率會大。透明樹脂的構造不均勻,光學上引起微觀上折射率的 不均而有散射的現象,光學級的折射率則比較均勻。 目前,壓克力PMMA (聚曱基丙烯酸曱酯)在塑料中透明度首屈一 馨指,在澆鑄板的厚度為1〇〇mm時也可完全透視物體。它又可以用染 料自由著色、而且表面光澤度很好、對人體無毒性。 曰本三菱Rayon製的PMMA的分光光線透過率在紫外線從 250nm附近上升,在可見光領域完全不吸收。 PMMA是屬於一種非結晶性塑料(Am〇「ph〇us),高分子鏈凌亂排 列糾纏,未形成井然有序的排列結構,在凝固過程中沒有晶核及晶粒 生長過程,僅是自由的高分子鏈被"凍結"(frozen)的現象。所以多具 高透明外觀。雜·歸聚合體皆有良好的光透性、其材f的密度 18 M364878 性也較低;至於,結晶形(Crystalline)聚合體由於球晶和不定形區域 的折射率不同,其光透性較差,材質密度較大,不適合本實施例使用。 PMMA壓克力板有良好的加工性能,既可採用熱成型(包括模 壓、吹塑和真空吸塑),也可用機械加工方式鑽、車、切割等。用微電 腦控制的機械切刮和雕刻不僅使加工精度大提高,而且還可製作出用 傳統方式無法完成的圖案和造型。另外還可接著、塗裝、與鍍膜等, _非常適合本發明實施例的使用。以上論點也就是本實施例建議使用光 學級PMMA的原因。 比PMMA透明度稍差一點點(透光度約88%)的聚碳酸樹脂PC (Polycarbonate) ’也是本實施例應用的另一個透明樹脂。 兩者比較不同點如下: PMMA缺點:吸水率高、耐熱性稍差、較不耐衝擊、較容易起燃。 PC缺點:成形性差。 瞻 因為PC的黏度較高,成形溫度也高些。但不需要特別困難的成 形技術。 對透明基材la,本實施例採用的鍍膜方式在真空蒸鍍中,透明玻 璃的耐溫約300°C,PC的耐溫約ll〇°C與PMMA的耐溫約70°C中, 以PMMA的冷處理較具困難’但這對有鍍膜經驗與較佳設備的廠商而 言並無技術上的困難。本實施例所鍍的鍍膜基材1中,起始的透明基 材la是採用透明玻璃比較容易蒸鍍,稍有經驗再採取PC、接著再採 用比較困難(溫度太高會變形,溫度太低則膜層附著力不好)的 19 M364878 PMMA。 (2)介電質膜層lb,介電質膜層lb的膜材包含氧化物膜。 介電質膜層lb的解釋: 本實施例採用膜材的要求是:在可見光與紅外範圍都是透明的。 例如 Ti〇2、Ti2〇5、Ti3〇5、Nb2〇5、Zr〇2、Hf〇2、Si〇2 等若無離子源助鍍(IAD) 透明基板la適宜者加高溫到250°C~300°C,並在抽真空後加以約15mPa 春之氧氣下蒸鍍,可得到堅固透明的氧化膜。但如透明基材1&為pc基 板或PMMA基板,如果要得到良好的膜質必須補以離子源助鍍。 光學鍍膜技術和其他科技一樣於近年來有著快速的發展。鍍膜技 術有很多種,大體上可分為利用液體與氣體成型兩類。前者大都涉及 化學變化,例如常見的溶膠法(S0|_ge丨)。後者有些是利用化學作用, 有些則是屬於物理作用。 験請參閱圖二為薄膜(鍵膜膜材)反射率與光學厚度的變化關係圖。 由光學薄膜干涉現象可知,當光垂直入射單層膜時,且光學厚度 Nd (為薄膜反射率與薄膜厚度的乘積)為(2;ι〇/2)、λ〇、(3λ〇/2)… 膜層對波長的反光強度不變;若光學厚度Nd為(λ()/4)、(3;U/4)、 (5 λq/4)…,反射率將為極大值或極小值,且其值決定於骐的折射率 η是大於還是小於基板的折射率nS。當n > nS時,反射率為極大值, 在η < nS時,反射率為極小值,如圖二所示。由圖二可見,一層光 學厚度為入射光波長四分之一奇數倍,讓反射波形成破壞性干涉,即 20 M364878 可得反射率為〇之抗反射效果。但對其他波長的反射率並非為〇,因 而為了在可見光範圍可得到寬廣的反射率通常都是多層架構,適當選 擇膜層的折神無層設計就可得騎㈣反射率。由圖二可見,一 層光學厚度為四分之-波長,且折射__義,可作為抗反射膜, ••使表面反射率降低,例如在玻璃(ΒΚ7,η=1·53)表面锻上單層說 化鎮(MgF2,η = 1. 38) ’即為-種簡單架構的抗反射膜。相對的, 若在玻璃表面錄上-層折射率足夠高的材料,它將大大增加玻璃表面 的反射率,因此這種薄膜可作為-種很好的分光鏡,單層的二氧化欽 (Τι〇2,η = 2.2)或硫化辞(ZnS,η = 2. 35)薄膜常作為這種用途, 反射率約可達30%左右。 基本上單層膜的疊加就是多層膜。當使用多層薄膜時,可以依照 我們的需要,運用高低折射率薄膜堆疊,做各式各樣的薄膜設計,以 產生我們所要求的光學特性。常見的如抗反射鏡、高反射鏡、截止濾 φ光鏡、帶通濾光鏡、帶止濾光鏡還有與本實施相對應分光鏡效果等等。 而電腦的出現,不但使光學薄膜設計(電腦輔助軟體)更為方便,且 光學薄膜的相關研究更是一日千裡。至今,光學薄膜製作的困難點已 經报少出現在設計上,只要特性要求合理例如本實施例的應用例,總 是能設計出適用的多層膜架構,關鍵的問題在於薄膜製鍍工藝的改 進,如何精確地控制每一層的厚度和折射率,以得到期望的光學性質 和機械特性’甚至考量製作的量產化及成本的降低,另外如薄膜材料 的開發、先進鐘膜技術的開發與薄膜的量測等,皆非為本實施例的範 21 M364878 圍0 今曰在薄膜光學上,我們很容易由向量法或導納軌跡法在光學級 基板上,鍍折射率高低交互變化的多層四分之一波膜堆,可獲得預期 的穿透率τ%。而且理論上也同時可以證明用相同多膜層數,四分之 一波膜堆比非四分之一波膜堆所得到的反射率R%要高。而膜層數越 多則反射率也越大。也就是說,很容易控制穿透與反射的分光比例。 在目前現有可用的鍍膜材料中,在可見光區高折射率小於等於 2.4而低折射率大於等於1.35,所以單一的四分之一波膜堆的高反射 帶的寬度是有限的。因此,要滿足本實施例在可見光區能夠像金屬膜 一樣有較寬的反射帶,有必要將介電質膜高反射帶拓寬。 拓寬的方法其中之一,是使膜系之每層厚度有規則的遞增(可依 等比級數或等差級數)’如此可使很寬的區域内的任何波長都有足夠多 的膜層,其光學厚度也足夠接近四分之一波。不過如此作成之高反射 區反射率會有許多下降的波紋,必須用優化法(Simplexmethod)再 行優化之。其他的方法還有將一個中心波長稍短之四分之一波膜堆養 加在另一個四分之一波膜堆上。 有關鍍膜的設計基本上可從標準膜系開始著手,例如高反射鏡不 管波寬大小或單或雙波數,都一律以四分之一波膜堆基礎來設計。 當初始設計無法滿足需求的光學成效時,就利用目前商用設計的 電腦軟體來優化或合成。有些優化所用的是數學技巧而且不斷的改進 22 M364878 中。例如最常用的有簡形優化法、最小平方調適法(Least-square fit or damped least squares)及合成法0 (3)金屬膜層lc 金屬膜層lc ’此金屬膜層lc主要功能是設計在「吸收殼體2内 所有的光能」,包含所有入射光穿透錄膜基材1進入殼體2後的多次 反射光。使殼體2内的反射光在金屬膜層lc被吸收掉或衰減掉。 如前述數學式的「L1b+L1c+L1d=25%」成立,由於透明基材ia 的Lib相對很大(吸收幾乎可忽略,即約為Llc+Lld=25%)〇所以, 可知鍍好介電質膜層lb後再鍍金屬膜層lc時,控制金屬膜層lc的 厚度即可掌握這個25%的動向。 如此之後,殼體2内的反射光被此金屬膜層le吸收後產生了兩 個功能: 一是人眼從鍍膜基材1往殼體2内觀看時看不到殼體2内的物品 (例如攝影機3)。因為,若僅透過鍍膜基材1的一透明基材ia與一 介電質膜層lb是很容易看到殼體2内的物品,因為透明基材la是透 明的’而常用的介電質膜層lb在可見光範圍也是呈現透明的,所以 透明基材la與-介電質膜層化在某角度(例如45度視角)是 很容易看到殼體2内的物品,詳述如圖八所示。 二是吸收掉殼體2内的其他反射光,以免這些其他反射光直接或 間接反射進人攝雜3的鏡頭干擾(例如反光)成像品f,詳述如圖 23 M364878 七所示。 一般金屬消光係數越大,光振幅衰減越迅速,進入金屬内部的光 能越少,反射率越高’例如本人的新型專利證號M326646「鍍銘半 球型罩攝影裝置」其中锻銘表面的反射率約55% (其中可見光穿透率Resins with good transparency in industrial plastics are: PMMA (transparency 93%), PC (transparency 88%), PS (transparency 89〇/〇), CR-39 (transparency 90%), SAN 16 M364878 resin ( Transparency 90%), MS resin (transparency 90%), poly-4methylpentene-(ΤΡΧ) (transparency > 90%). In addition, transparency such as decyl methacrylate, styrene copolymer (MAS), PET, PP, and PVC is excellent. Among these general-purpose transparent resins, the light transmittance includes not only visible light having a wavelength of from 380 nm to 780 nm but also a near-infrared field having a wavelength of from 780 nm to 1000 nm. • The transparency of visible light and infrared light in transparent resins is generally affected by factors such as reflection, penetration, absorption, and scattering of “light”. When light enters the transparent resin, some of it will be reflected on the surface and lost. The example of reflection is usually when the refractive index n1 (=1) of the light is perpendicularly incident on the polymer having the refractive index n2, and the calculated surface reflectance R% is divided by the square of (η-l) by (n+ The square of l) is expressed. The data shows that the refractive index of transparent acrylic (Plexiglas) pmma (Polymethylmethacrylate) is L49, and the surface reflectance RO/〇 is calculated to be about 4%. The total light transmittance of PMMA is about 93%. This loss of light is mostly caused by the secondary reflection of the surface back and forth, while the internal loss such as absorption and scattering is very small. When the light hits the transparent resin molecule, the molecule will absorb its energy and rotate, causing the light absorption to reduce the permeability, and the scattering occurring during the light-off will greatly reduce the light transmission. Since the scattering system in the transparent resin (4) is proportional to the refractive index of 8 squares and inversely proportional to the wavelength 4, the scattering loss of the material having a low refractive index is small, and the scattering is in the visible light region where the wavelength of the wave is longer than M. Less affected. In the infrared field with longer wavelengths, the effect of the scattering is almost as small as zero. This argument is to support the fact that this embodiment only deals with the interpretation of reflection, penetration and absorption of light without discussing more complex scattering phenomena. Moreover, some foreign matter generated or incorporated by the transparent resin or a transparent polymer during the manufacturing process also reduces the light transmittance due to scattering. According to the manufacturer's data, the optical grade PMMA foreign matter is only one tenth of the general molding pmmA, and the foreign matter particle size is 0.5叩~0.〇7, the optical grade PMMA foreign matter is about 600~2000. The amount of foreign matter of the general-grade PMMA is about 4,000 to 20,000 pieces/g. This is why this embodiment suggests the use of optical grade PMMA. In practical applications, the refractive index is greatly affected by changes in the temperature and humidity of the environment. In general, the higher the refractive index of the transparent resin, the greater the reflectance. The structure of the transparent resin is not uniform, optically causing unevenness in the refractive index on the microscopic surface, and the refractive index of the optical grade is relatively uniform. At present, acrylic PMMA (poly(decyl methacrylate)) is the first of its kind in plastics. It can also fully see through the object when the thickness of the cast sheet is 1〇〇mm. It can also use the dye to freely color, and the surface gloss is very good and non-toxic to the human body. The spectral light transmittance of PMMA manufactured by Mitsubishi Rayon is increased in the ultraviolet light from around 250 nm, and is not absorbed at all in the visible light field. PMMA belongs to a kind of amorphous plastic (Am〇 “ph〇us”. The polymer chain is disorderly arranged and entangled. It does not form an orderly structure. There is no crystal nucleus and grain growth process during solidification. It is only free. The polymer chain is "frosted" (frozen), so it has a high transparent appearance. The hybrid polymer has good light transmittance, and the density of the material f is also low. Due to the different refractive indices of spherulites and amorphous regions, the crystalline crystals have poor light transmittance and high material density, which is not suitable for use in this embodiment. PMMA acrylic sheets have good processing properties and can be used in heat. Molding (including molding, blow molding and vacuum blistering), can also be drilled, car, cut, etc. by mechanical processing. Micro-computer controlled mechanical cutting and engraving not only improve the processing precision, but also can not be produced in the traditional way. Finished pattern and shape. Further, it can be followed by coating, coating, etc., which is very suitable for the use of the embodiment of the present invention. The above argument is also suggested to use optical grade PMMA in this embodiment. Cause: Polycarbonate PC (Polycarbonate) which is slightly less transparent than PMMA (transparency of about 88%) is another transparent resin used in this embodiment. The difference between the two is as follows: PMMA disadvantage: high water absorption It has a slightly poor heat resistance, is less resistant to impact, and is easier to ignite. PC disadvantage: poor formability. Because of the high viscosity of PC, the forming temperature is also higher. However, it does not require particularly difficult forming technology. The coating method adopted in this embodiment is in vacuum evaporation, the temperature resistance of the transparent glass is about 300 ° C, the temperature resistance of the PC is about ll 〇 ° C and the temperature resistance of the PMMA is about 70 ° C, and the cold treatment with PMMA is more Difficult' but this is not technically difficult for manufacturers with coating experience and better equipment. In the coated substrate 1 coated in this embodiment, the starting transparent substrate la is relatively easy to vaporize using transparent glass. A little experience, then take the PC, and then use the 19 M364878 PMMA which is difficult (the temperature is too high to deform, the temperature is too low, the adhesion of the film is not good). (2) Dielectric film layer lb, dielectric film The film of layer lb contains an oxide film. Explanation of layer lb: The requirements for the use of the film in this embodiment are: transparent in the visible and infrared ranges. For example, Ti〇2, Ti2〇5, Ti3〇5, Nb2〇5, Zr〇2, Hf〇2 For Si〇2, etc., if there is no ion source assisted plating (IAD), the transparent substrate is suitable for high temperature to 250 ° C ~ 300 ° C, and after vacuuming, about 15 mPa of spring oxygen evaporation, a strong transparent oxide film can be obtained. However, if the transparent substrate 1& is a pc substrate or a PMMA substrate, ion source plating must be supplemented if a good film quality is to be obtained. Optical coating technology has been rapidly developed in recent years as well as other technologies. There are many kinds of coating technology, which can be roughly divided into two types: liquid and gas molding. Most of the former involve chemical changes, such as the common sol method (S0|_ge丨). Some of the latter use chemical action, while others are physical.験Please refer to Figure 2 for the relationship between the reflectance of the film (bond film) and the optical thickness. It is known from the optical film interference phenomenon that when the light is perpendicularly incident on the single layer film, and the optical thickness Nd (which is the product of the film reflectance and the film thickness) is (2; ι 〇 / 2), λ 〇, (3 λ 〇 / 2) ... the reflection intensity of the film layer is invariant; if the optical thickness Nd is (λ()/4), (3; U/4), (5 λq/4)..., the reflectance will be a maximum or a minimum value. And its value depends on whether the refractive index η of germanium is larger or smaller than the refractive index nS of the substrate. When n > nS, the reflectance is a maximum value, and at η < nS, the reflectance is a minimum value, as shown in Fig. 2. It can be seen from Fig. 2 that the optical thickness of one layer is an odd multiple of one-fourth of the wavelength of the incident light, which causes the reflected wave to form destructive interference, that is, 20 M364878 can obtain the anti-reflection effect of 〇. However, the reflectance for other wavelengths is not 〇, so in order to obtain a wide reflectance in the visible range, it is usually a multi-layered structure, and the wavy (four) reflectance can be obtained by appropriately selecting the wavy layerless design of the film layer. As can be seen from Fig. 2, a layer of optical thickness is quarter-wavelength, and the refractive index is used as an anti-reflection film. • The surface reflectance is lowered, for example, on the surface of glass (ΒΚ7, η=1·53). Single-layered town (MgF2, η = 1.38) 'is a simple structure of anti-reflection film. In contrast, if a material with a sufficiently high refractive index is recorded on the surface of the glass, it will greatly increase the reflectivity of the glass surface, so the film can be used as a good spectroscope, a single layer of dioxygen 〇2, η = 2.2) or vulcanized (ZnS, η = 2.35) films are often used for this purpose, with a reflectivity of about 30%. Substantially the superposition of a single layer of film is a multilayer film. When using multilayer films, we can use a combination of high and low refractive index films to create a wide range of film designs to produce the optical properties we require. Common examples include anti-reflectors, high-reflectors, cut-off filters, band-pass filters, band-stop filters, and spectroscopic effects corresponding to this implementation. The emergence of computers has not only made optical film design (computer-aided software) more convenient, but also related research on optical films. So far, the difficulty of optical film fabrication has been reported in the design. As long as the characteristics are reasonable, for example, the application examples of the embodiment, the applicable multilayer film structure can always be designed. The key problem is the improvement of the film plating process. How to precisely control the thickness and refractive index of each layer to obtain the desired optical properties and mechanical properties' even to consider the mass production and cost reduction of the production, as well as the development of thin film materials, the development of advanced clock technology and the film Measurement, etc., are not the model 21 M364878. In the film optics, we can easily apply multi-layered four-points with high refractive index on the optical grade substrate by vector method or admittance trajectory method. One of the diaphragm stacks can achieve the expected penetration rate τ%. In theory, it is also proved that the same multi-layer number is used, and the one-quarter diaphragm stack has a higher reflectance R% than the non-quarter-wave stack. The more the number of layers, the greater the reflectivity. That is to say, it is easy to control the split ratio of penetration and reflection. Among the currently available coating materials, the high refractive index in the visible light region is 2.4 or less and the low refractive index is 1.35 or more, so the width of the high reflection band of the single quarter-wave film stack is limited. Therefore, in order to satisfy the present embodiment, it is possible to have a wide reflection band like a metal film in the visible light region, and it is necessary to widen the high reflection band of the dielectric film. One of the methods of broadening is to have a regular increase in the thickness of each layer of the film system (depending on the number of steps or the number of steps) so that there can be enough film at any wavelength in a wide area. The layer, whose optical thickness is also close enough to a quarter wave. However, the high reflectance reflectance thus produced has many falling ripples that must be optimized using the Simplex method. Other methods include stacking a quarter-wave film with a shorter center wavelength on another quarter-wave film stack. The design of the coating can basically be started from the standard film system. For example, high reflection mirrors are designed on the basis of a quarter-wave film stack, regardless of the width or single or double wave number. When the initial design fails to meet the optical performance of the demand, it is optimized or synthesized using current commercially designed computer software. Some optimizations use mathematical techniques and are constantly improving in 22 M364878. For example, the most commonly used are the simple optimization method, the least square adjustment method (Least-square fit or damped least squares) and the synthesis method 0 (3) metal film layer lc metal film layer lc 'the main function of the metal film layer lc is designed in "Absorbing all of the light energy in the casing 2" includes all of the reflected light that passes through the recording film substrate 1 and enters the casing 2. The reflected light in the casing 2 is absorbed or attenuated in the metal film layer lc. As the above formula "L1b+L1c+L1d=25%" holds, since the Lib of the transparent substrate ia is relatively large (absorption is almost negligible, that is, about Llc+Lld=25%), it is known that the plating is good. When the metal film layer lc is plated after the electric film layer 1b, the thickness of the metal film layer lc can be controlled to grasp the 25% movement. After this, the reflected light in the casing 2 is absorbed by the metal film layer to produce two functions: First, the human eye cannot see the contents of the casing 2 when viewed from the coated substrate 1 into the casing 2 ( For example, camera 3). Therefore, if only a transparent substrate ia of the coated substrate 1 and a dielectric film layer 1b are easily visible in the article 2, since the transparent substrate 1a is transparent, the commonly used dielectric The film layer lb is also transparent in the visible light range, so that the transparent substrate la and the dielectric film are layered at an angle (for example, a 45 degree angle of view), and the articles in the casing 2 are easily seen. Shown. The second is to absorb other reflected light in the casing 2, so as to prevent these other reflected light from directly or indirectly reflecting into the lens interference (for example, reflective) image f of the camera 3, as shown in detail in FIG. 23 M364878. Generally, the larger the metal extinction coefficient, the faster the attenuation of the light amplitude, and the less the light energy entering the metal interior, the higher the reflectivity. For example, my new patent number M326646 "plated in the hemispherical hood photographic device" The rate is about 55% (where the visible light transmittance

約為18%)。簡單說,光的物理性質決定於振幅與波長兩因素。振幅 決定了光量的強弱,波長則是區別色彩的特徵與種類,也就是說,振 幅的差異,給予明暗的區別;而波長的差異則給予色相的區別。業者 總是選擇消光係數較大,光學性質較穩定的那些金屬作為鍍金屬膜材 料。例如在紫外區常用的金屬薄膜材料是鋁,在可見光區常用銘和 銀,在紅外區常用金、銀和銅,此外,鉻Cr和鉑也常用作一些特殊 的鍍膜材料。由於鋁、銀、銅等材料在空氣中很容易氧化而降低性能, 所以必須用介電質膜加以保護,常用的保護膜材料有一氧化矽以〇、 氟化鎂MgF2等。 金屬膜層lc既然功能是設計在「吸收殼體2内所有的光能」,所 以金屬膜層lc的膜材則不限於鍍鉻Cr。 請參閱圖三為設計本實施例樣品A的光譜圖。 如圖三所示,本實施例樣品設計的需求是: ㈠在可見光(400nm〜700nm)部份的,希望平均控制在18〇/〇。 (二)在紅外(780nm〜1,000nm)部份的穿透率了%,希望平均控 制在70%以上。 24 M364878 準備-厚度為3_的透明青板朗數片,經清洗與強化處理後 放入鍍膜機進行Mg。鍍膜機内放有三個以上的賴分別裝有漏5、 Si〇2、與Cr等膜材。 圖三中縱座標為穿透率百分比T% (Transmjttance 0/〇)。橫座標 為光譜波長(單位nm)。其他參數為(丨)白光環境、(2 )正面入射角(〇 度)(3)參考波長為450nm.、(4)以四分之一波(qUarter-wave-stack multi-layered)模式設計。 鍵多層介電質膜lb的膜材儘量選擇最少的兩種搭配開始,不容易 找到適當的搭配時則多增加一或兩種以上也可。 本實施纖介電質膜lb是選用兩種折射率高低不同的膜材在鍍 膜機内交替蒸鍍的方式形成。 -般選擇兩種折射率高低不觸膜材中,有常賴氧化物膜,例 如有高折射率的Ti〇2與低折射率的si〇2。 由於Τι〇2容易失氧’且會有不同的結構(例如銳鈦礦咖心 等)。目前電子搶蒸鍍或濺鍍Ti2〇5或Ti3〇5都比Ti〇2穩定。Ti3〇5膜 比Ti〇2膜容易得到較小的吸收與散射。 所以,本實施例現就以Ti3〇5 (取代Ti〇2)與Si〇2兩種折射率高 低不同的膜材在鍍膜機内交替蒸鍍18層。 第一層:鍍Ti3〇5。光學膜厚=〇. 5075 第二層:鍍Si〇2。光學膜厚=0.4615 第三層:鍍Ti3〇5。光學膜厚=2. 0697 第四層:鍍Si〇2。光學膜厚=〇. 3996 25 M364878 第五層:鍍Ti3〇5。光學膜厚=1. 2309 第六層:鍍Si〇2。光學膜厚=0· 9521 第七層:鍍Ti3〇5。光學膜厚=0. 6556 ' 第八層:鍍Si〇2。光學膜厚=1.2178 第九層:鍍Ti3〇5。光學膜厚=1.4742 第十層:鍍Si〇2。光學膜厚=0. 3776 第十一層:鍍Ti3〇5。光學膜厚=4.1621 I 第十二層:鍍Si〇2。光學膜厚=0.8100 第十三層:鍍Ti3〇5。光學膜厚=1. 7303 第十四層:鍍Si〇2。光學膜厚=1.5163 第十五層:鍍Ti3〇5。光學膜厚=1.1209 第十六層:鍍Si〇2。光學膜厚=1.7299 第十七層:鍍Ti3〇5。光學膜厚=1.4229 第十八層:鍍Si〇2。光學膜厚=2. 8657 &鍍完介電質薄膜lb後再鍍金屬薄膜lc,金屬膜材有Cr。 鍵 Cr 一層為 3nm 厚度(Physical thickness )。 完成鏟膜處理後,經日本Hitachi光譜儀U-4100測試如誤差過大 再修正直到誤差在允許範圍内。 其中,樣品A作了兩款分别為樣品Αι與樣品A2。 樣^是在3mm的透明青板破璃的一表面鍍介電質薄膜化,而 在同一表面再鍍金属薄膜lc。所以,樣品A1可稱為翠面鍵膜。 26 M364878 樣时A2是在3mm的透明青板玻璃的_表面鐘介電質薄膜化,而 在另表面链金屬薄膜lc。所以,樣品A2可稱為雙面锻膜。 •最後再經光譜儀U-4100測試電腦繪出如圖四有樣品A1的光譜曲 線4A1與樣品A2的曲線4A2 〇 圖四為樣品A鍍膜完錢的實際光譜圖。 圖四中,縱座標為穿透率百分比T% (Transmjttance %)。橫座 ®標為光譜波長(單位nm)e 如圖四所示’鍍膜完成後的樣品A經光譜儀U-4100測試電腦、命 出的實際光譜曲線,可看出㈣三本實麵樣品A原先設計的模擬光 譜曲線有落差。 原先設計的光譜曲線(如圖三)是希望在可見光4〇〇nm~7〇〇nm 部伤的穿透率T。/。平均控制在18% »而在紅外780nm〜1,000nm部份 ®的穿透率T%平均控制在70%以上。 然而,鍍膜完成後的實際光譜曲線中; 曲線4A1在可見光400nm〜700nm部份的穿透率τ。/。平均(光譜儀 自動計算)在27.1%’往長波方向580nm以後有下降趨勢直到75〇nm 後才上升。而在紅外780nm〜1,000nm部份的穿透率τ%平均(人工目 視估算)約在75%。 曲線4A2在可見光400nm〜700nm部份的穿透率了。/0平均(光譜儀 27 M364878 自動計算)在23%,越往長波方向有上昇趨勢。而在紅外 780nm〜1,000nm部份的穿透率Τ%平均(人工目視估算)約在7〇%以 上。 由曲線4Α1與曲線4Α2看來,鍍雙面與鍍單面的效果差異不很大, 但鍍雙面所花的工時相對多(本實施例鍍雙面時要翻轉再鍍另一面)成 本相對比較高。而且,锻雙面在基板外表面容易沾污與刮傷常需另加 保護膜。又,鍍單面膜時如囷四所示,在可見光部份會有些明顯凸出 的曲線(如在570nm處)’這除了在可見光部份不同顏色的光折射率〇 依序從小變大屬於正色散現象(normal dispersion)以外,鍍介電質膜 層lb與鍵金屬膜(Cr)lc的過於接近疊起,影響到介電質膜比的干涉, 但是由本實關可知’-般CCD攝職在常見的環贼視以非專業 高解析度型)上對攝影成像影響不大(看不出在57〇nm處有色偏現 象)。 _ 如果圖四在可見光部份曲線高凸點與曲線低凹點之間的差距太大 的話,則有可能在差關對應的波長產生此波長對應的色偏。簡單說, 如果這些差關對應驗長大部份落在紐的紅絲圍,則攝影機所 攝取的可見光影像會產生帶有偏「紅」的色彩。 如有必要時,以增加膜層數的設計可以將圖四在可見光部份臀蠻 曲曲的曲雜上下雜平,齡其高凸點與伽點之間的差距,但這 會增加製作成本。本實施的另外例中,若透明基板la採以pMMA時 因為增加膜層數應小心其產生的高溫會使pMMA變形,初步解決的方 28 M364878 式是再鍍下一層時的時間間隔稍拉長一點,使有足夠時間降溫。 在後面的應用實施例以樣品A1與A2的影像測試發現,這些在可 見光部份彎彎曲曲的曲線並無明顯地影響成像的品質(例如色偏現 象)。 事實上,對於像圓三的設計,由於不同的鍍膜機也會有不同的結 果’如前述可以電腦再修正或再多作一兩次鍵膜實作修正。修正後存 籲檔並在往後量產時儘量以同一台鍍膜機生產可取得穩定的產品。 另外’如果鍍Cr層的3nm厚度依最後光譜儀測試,如測試後Lie 的穿透率低於18% (或不符理想),則再將鍍Cr層的厚度減低(或重 新修正)再鍍一次,直到Lie的穿透率接近於18% (或接近理想值)。 當調整好Lie的穿透率後,接下來看看鍍完金屬膜lc後有何效 果? 鲁請參閱圖五為樣品A1的反射光譜圖。 如圖五的反射光譜圖中,縱座標為反射率百分比R〇/〇。橫座標為 光譜波長(單位nm)。 樣品A1的反射光譜圓中,曲線A10為樣品A1的正面(無鍍膜面) 反射光譜曲線。曲線All為樣品A1的背面(艘金屬膜ic面)反射光 譜曲線。 由曲線A10與曲線All雙曲線圖可知,較低反射的曲線A11,的 29 M364878 確鍍金屬膜lc具有抗反射效果。也就是說,cr建到「吸收」的效果, 所以也稱鍍Cr層為金屬膜層。 請參閱圊六為樣品A2的反射光譜圖。 如圖六的反射光譜圖中,縱座標為反射率百分比R%。橫座標為 光譜波長(單位nm)。 樣品A2的反射光譜圖中,曲線A20為樣品A2的正面(鍍介電質 參膜層lb面)反射光譜曲線。曲線A21為樣品A2的背面(鍍金屬膜lc 面)反射光譜曲線。 由曲線A20與曲線A21雙曲線囷可知,較低反射的曲線A21,的 確鍍金屬膜lc具有抗反射效果。也就是說,Cr達到「吸收」的效果。 鍍Cr層的厚度與「吸收」的效果成正比。也就是說,鍍Cr層的 厚度越薄其吸收量越少。 完成上述鑛膜後的鍍膜基材1 (包含一 3mm厚的透明青板玻璃、 一 TisOs與si〇2介電質膜與一鍍金屬Cr膜層),將攝影機3的鏡頭 31對準鍍膜基材1的金屬Cr膜層膜面,以便實施應用。 請參閱囷七為本實施例裝置應用示意圖。 圖七也是為圊一所示之裝置的應用示意圖。 圖七中包含有樣品A1形成的鍍膜基材1、殼體2、攝影機3、與 30 M364878 影像顯示器4。也包含有便利說明的代表性的光線,例如Ll、Lla、Lle、 與 L2a、L2b、L2c 與 L3、L3a、L3b 等。 入射光LI (100%)入射到鍍膜基材1正表面時,如圖五光譜圖所 示其反射光Lla約為56%,如圊四光譜圖所示其穿透鍍膜基材1的透 射光Lie約為27%。 約為56%的反射光Lla在鍍膜基材1正表面呈現亮麗鏡面(乍看 鲁像一面鏡子)。 約為27%的透射光Lie進入攝影鏡頭31成像。 則約有17%(100%-56%-27%)在鍍膜基材1損失(大部份是被鍍Cr 層吸收掉)。 另一入射光L2 (100% )入射到鍍膜基材1正表面時,其穿透鍍膜 基材1的透射光L2a (透射光Lie相同)約為27%。但透射光L2a並 泰無直接進入攝影鏡頭31成像而是在殼體2内反射形成另一反射光 L2b〇 反射光L2b反射到鍍膜基材1背表面時會再產生再一反射光L2c’ 這反射光L2c會反射進入攝影鏡頭31成像,反射光L2c與透射光Lie 一起進入攝影鏡頭31造成重疊的影像,俗稱鬼影影響成像的品質。 反射光L2c反射到鍍膜基材1背表面時約有56%的反射’則其光 能約為入射光L2的15.1%(27%*56%)。 M364878 本實施例測試可知,如果入射光L2過小時(例如為5〇j_ux)則反射 光L2c約為7.5Lux,反射光L2c與透射光Lie —起進入攝影鏡頭31 後’在影像顯示器4上並無顯示出L2c的影像。如果入射光L2過大時 (例如為300Lux)則反射光L2c約為45Lux,反射光L2c與透射光Lie 一起進入攝影鏡頭31造成重疊影像,在影像顯示器4上會很明顯顯示 出L2c的影像。 為了阻止或衣減反射光L2c進入攝影鏡頭31有三個方法: 第一,在攝影鏡頭31外圍套入一不透光的黑色軟套32,把反射光 L2c擋住。這黑色軟套32必須與鍍膜基材丨背表面緊緊貼近不要有透 光的間隙,非直接由攝影鏡頭31前進入的光(例如Ue)以外的雜光 通通被黑色軟套32擋住。這黑色軟套32最好用黑色或深色,如用白 色則會造成白色的反射讓人眼從鍍膜基材丨正表面看到白色的圈套影 子。 上面第-個方法,若套用在目前流行的高速球攝影機(High Speed Dome Camera)’則有一定程度的困難。因為,這類高速球攝 影機的鏡聊份常作冑速紐轉,其躺上的黑色軟套32會被碰擊造 成鍍膜基材1背表面損壞。 第二,在殼趙2的内部表面21形成有黑色或深色的粗輪表面。目 的是吸收與散射掉L2a,使L2b不易形成。也就是說,間接使L2c不 易形成。 32 M364878 上面第二個方法,若鍍膜基材1不是平板狀,而是像本人的新型 專利證號M326646「鍍鋁半球型罩攝影裝置」一般呈現半球狀,則入 射光L2透射到半球狀的鍍膜基材1内時,可能又從鍍膜基材1的另一 側再透射出去,根本沒有透射進入到殼體2的内部表面21。這時如果 有人從L2入射方向看去,就容易看到鍍膜基材丨後的的攝影機3 了。 第二,在攝影鏡頭31前加入一金屬膜層,用以吸收或降低的 光能。 上面第三個方法,是本實施例的設計重點之一。 因此,以如上的第三個方法較適通用,但若能將三個方法合併使 用則在應用上可發揮更不錯的效果。 請參閱圖八為本實施例裝置實驗示意囷。 圖八所示與囷七不同處在於;在圖八中移除了圖七的殼體2。 如圖八所示,入射光L2入射到鍍膜基材1後的透射光L2a並無觸 及物體(例如殼體2)時,L2a就繼續直線往前走直到光能耗盡,就不 會有產生反射L2b的問題。 這時若人眼從L2的方向看鍍膜基材1,會發現鍍膜基材1呈現透 明狀態,人眼容易看到鍍膜基材1背後的物體,尤其是在鍍膜基材1 背後的光照度大於鍍膜基材1前面(與人眼同方向位置)的光照度時, 更是明顯。 33 M364878 當鍍膜基材1的背景環境是深色(例如深藍)或黑色時(例如在 殼體2内),在一般環境下(例如約2〇〇Lux的照度環境)對人眼從鍍膜 基材1的正面觀察,具有50%以上的反射光時就可顯示出鏡面反射的 效果。60%以上的反射光比較像鏡面,7〇%以上的反射光又更像一面 ~鏡子. 圖八是鍍膜基材1完成時的測試工作之一,主要測試鍍膜基材1 鲁背表面的成像效果。這工作是將攝影機3的鏡頭31對準鍍膜基材1 背表面,再將影像顯示器4連接起來,測試透射光Lie的成像效果。 在影像顯示器4顯示的成像效果,如果在一定的環境照度下,主 要取決於透射光Lie的光能大小、以及攝影機3的成像品質。 透射光Lie的光能比(佔入射光L1的百分比)越大則在影像顯示 器4顯示的成像效果越好。 # 但是,透射光L1e的光能比越大,相對的反射光Lla就越小。反 射光Lla越小就越顯不出亮麗的反射鏡面,沒有了亮麗的反射鏡面就 不容易隱藏裝飾鍍膜基材1背後的物體(例如攝影機3),這也就失去 本實施例要達成隱藏裝飾成像的目的。由圖七實際應用上透射光L1e 的光能比在10%〜30%是較經濟的合理選擇。 至於攝影機3的成像品質,主要是指攝影機3的影像感測器的感 應度品質。國内外市場上常用的有許多種款式,包含有日本s〇ny、 Sharp與韓國三星等廠牌,都有生產不同高階end)、低階(L〇w 34 M364878 end)的各型號產品。如囷八本實施例的攝影機3測試了十餘型號的 CCD與Cmos,在不同照度環境也取得不同的成像效果。如果為了節 省購買高階低照度的攝影機,僅購買低階的攝影機,再適當的搭配輔 助光源也是一個替代的方案。 如圖八是鍛膜基材1完成時的測試工作,也就是說鍛膜基材1量 產時可單獨出售鍍膜基材1給攝影機廠商或系統安裴廠商的品質測試 _工作。也就是說’單獨的鍛膜基材1可以當作一關鍵性組件鎖售。 在實際應用裝置上常加入一殻體2以形成一可直接應用與銷售的 產品。 請參閱圖九為内建紅外光源的裝置應用示意圖。 如圖九所示是另一個應用裝置。圖九所示與圖七不同處在於;在 圖九中增加了一紅外光源5以及利於紅外光源5散熱的鋁製的殼體2。 近年國際安全器材展上顯示有日夜型的防盜監視的攝影裝置,大 都以把夜視用的輔助紅外光源與攝影機鏡頭組合在一起後再置入同一 鋁製的殼體2内,用以施工方便。白天(環境光能充足)利用可見光攝 影,夜間(環境光能不足)利用辅助紅外光源攝影。 對於夜視輔助光源常用的有稱為IR-LED的紅外發光二極體,是 市場上最廉價與方便的夜視輔助光源。其中心波長常用的是850nm, 單顆功率約為100mW’廠商在日夜型防盜攝影機成品中,常以12、 24、36顆甚至有一百多棵的丨R-LED圍繞在一電路板的四周,而電路 35 M364878 板的中央有一圓形空洞是直接套在攝影機鏡頭31周圍。 在圖九中所增加的一紅外光源5,同目前市售的小型的防盜監視 的攝影裝置(台灣與中國大陸俗稱槍機)一樣,也是將紅外光源5與 攝影機鏡頭31組合在一起後,再置入同一機殼2内。 紅外光源5也可以設置於機殼2外、或獨立於機殼2。 近年來新出產的搶機,大都採用了單或雙層透明玻璃的防護罩, _圖九是以鍍膜基材1取代其透明玻璃的防護罩。 LED光源所發射的光是紅外範圍的850nm,是人眼可辨識的範圍 内,所以人眼常看到紅色光點(Red glow)業界稱為「紅爆」,是夜 間暴露搶機攝影位置的主要原因。 如圖九所示,新增的紅外光源5在殼髏2内所幅射的紅外線為紅 外L3(其紅外幅射能量假設為100%),紅外L3入射到链膜基材1時, 豢紅外L3在到鍍膜基材1約有75%為紅外透射光L3b(如圖四)與約有 15%為紅外反射光L3a (如圖五),其餘大都被鑛膜基材i的金屬膜lc 吸收掉。 當紅外透射光L3b穿透鍍膜基材1出去入射到物體a,物體a吸收 後再放射出去穿透鍍膜基材1後,成為L3C進入攝影鏡頭31成像(紅 外影像)。 另外,紅外反射光L3a如果沒有黑色軟套32的阻擋,則可能會進 36 M364878 入攝影機鏡頭31成像,在影像顯示器4上顯示出白色曝光區塊’這白 色曝光區塊是紅外光源5輻射紅外的區塊影像。例如若僅有一顆圓形 狀5mm的紅外發光二極體(|R-LED)時,這白色曝光區塊就是一圓 形狀的白色曝光區塊。 .· 若有一物體A在鍍膜基材1前,在可見光L1的入射下’其透射光 Lie進入攝影機鏡頭31成像,最後在影像顯示器4上顯示出物體A的 可見光影像。若攝影機3為彩色攝影機時則這可見光影像為彩色的影 像。若攝影機3為黑白攝影機時則這可見光影像為黑白的影像。 但,若有一物體A在鍍膜基材1前,在紅外光源5發光時,其透 射紅外L3c進入攝影機鏡頭31成像,最後在影像顯示器4上顯示出物 體A的紅外影像。這紅外影像是單色的影像對人眼而言與黑白影像很 相似但不一樣。 _ 若有一物體A在鍍膜基材1前,當有可見光L1的入射與紅外光源 5的發光時,則在影像顯示器4上顯示出物體A的可見光影像與紅外 影像的重疊影像。 這時若可見光影像大於紅外影像,則可見光影像「蓋過」紅外影 像使影像顯示器4上顯示出物體A的可見光影像。 這時若可見光影像小於紅外影像,則紅外影像「蓋過」可見光影 像使影像顯示器4上顯示出物體A的紅外影像。 這時若可見絲像接近料於紅外影像,則可見光影像以及紅外 37 M364878 影像兩者同時存在,使影像顯示器4上顯示出物體A的可見光影像但 帶有類似過度曝光的區塊,造成成像品質不良。 為了避免造成在影像顯示器4上顯示出物體A可見光帶有類似過 度曝光的區塊的影像’通常是以一光敏電阻(CDS)元件做為偵測。 , 當環境照度不足(例如剩餘約1〇Lux)時,因CDS元件啟動控制電路 打開紅外光源5電源發出紅外,這時應是紅外影像大於可見光影像, 使影像顯示器4上顯示出物體A的紅外影像。圖九省略CDS元件乃 因CDS是習知元件。唯一要注意的是;CDS元件接受入射可見光的 方向不要經過鍍膜基材1,因為鍍膜基材1的穿透率只有入射可見光 的15%,與常用CDS元件的安置於透明玻璃内(幾乎接受入射可見 光的90%)不同。如果一定要安置於經過鍍膜基材1的位置時,則必 須調整CDS元件的靈敏度。也就是說,若安置於透明玻璃内CDS元 件調整在10Lux時啟動,則安置於鍍膜基材1後的CDS元件應該調 ¥整在60〜70Lux之間為宜。 目前高階產品都在攝影機3的鏡頭31後與影像感測器前之間的空 間上,加上自動雙濾光片切換裝置。 目前市場上的自動雙濾光片切換裝置,簡單說就是自動切換紅外 截止濾光片丨CF (Infraredcutfiltter)與普通透明玻璃濾光片等兩個濾 光片的裝置。紅外截止濾光片切入到影像感測器前時,阻擋了紅外L3c 的進入,其影像感測器僅感測到可見光Lie。紅外截止濾光片移除離 開影像感測器前時,因其普通透明玻璃濾光片切入的關係,其影像感 38 M364878 測器則可感測到可見光Lie與紅外L3c兩者。 本實施例再依圖九所示將攝影機3,改裝成一具有自動雙濾光片切 換裝置的攝影機3 ’其中把CDS元件安置於殼體2上(不經過艘膜基 材1),也把原CDS元件的設定(在i〇Lux啟動)維持不變更》 .- 結果發現;攝影機3的影像感測器切入普通透明玻璃濾光片時則 可感測到可見光Lie與紅外L3c。主要原因出在,當環境照度約在 籲10Lux時,CDS元件啟動將普通透明玻璃濾光片移入的攝影機3的影 像感測器前,使可見光L1 e與紅外L3c均一啟進入攝影機3的影像感 測器成像。而其中,高階產品的攝影機3其環境照度約在i〇Lux時, CDS元件除了啟動自動雙濾光片以外,同時也啟動了紅外光源5。這 就有機會同時出現可見光Lie與紅外L3c混合的影像(造成類似有點 曝光的影像,除非是屬專業的藝術性攝影,否則不適合防盜攝影監視 用途)。 為了使可見光Lie與紅外L3c兩種影像,沒有機會同時一起顯示 在影像顯示器4上。本實施例再將自動雙濾光片切換裝置的普通透明 玻璃渡光片移除,改換一種稱為紅外通過渡光片IPF (Infrared Pass filtter)者》IPF與ICF作用相反,丨PF僅讓紅外通過而截止可見光Lie 通過。藉由此種自動雙濾光片(IPF與ICF)切換裝置,使得出現可 見光Lie與紅外L3c混合的影像在影像顯示器上出現的機會變成不容 易0 39 M364878 綜合上述,-種鍍膜基板成像置,適麟攝健視,包含有 一不透光容器的殼體2 ’殼體2的-側放置有_鍍膜基板t與殼體2 的内部收納有一取像單元(攝影機3)。其中摘要如下; (1) 為了阻止或衰減反射光L2c與紅外反射光L3a等進入攝影鏡 頭31 ,如在鍍膜基板丨上僅鍍有一多層介電質膜化時,則在攝影鏡 頭31外圍套入一不透光的黑色軟套32或是在殼體2的内部表面21 I形成有黑色或深色的粗糖表面。 (2) 為了阻止或衰減反射光L2c與紅外反射光L3a等進入攝影鏡 頭31,如鍍有一多層介電質膜lb與一金屬膜層lc時,可利用金屬膜 層1c對反射光L2c與紅外反射光L3a進行吸收與衰減。其中多層介 電質膜lb與一金屬膜層lc兩者可共同锻在鍍膜基板j的同一面上或 分別锻在鍍膜基板1的不同兩個面上。 (3) 為了阻止或衰減反射光L2c與紅外反射光L3a等進入攝影鏡 U頭31,可以加上一黑色軟套32、或是在殼體2的内部表面21形成有 黑色或深色的粗糙表面、或是鍍上一金屬膜層lc等三者之一或三者之 二、或三者全部。 (4) 為了阻止反射光L2c與紅外反射光L3a同時進入攝影鏡頭 31,就在攝影機3的影像感測器前增添一自動雙濾光片切換裴置,其 中包含有一紅外截止濾光片ICF (Infraredcutfiltter)與一紅外通過渡 光片丨PF (Infrared Passfiltter)兩濾光片的切換裝置。 M364878 (5)為了達到具有更高的反射率(例如反射光Lla)在鍍膜基板 1鍍上多層介電質膜lb用以取代先前技術的鍍金屬鋁。 以上的具體實施例說明本創作之實施方式,熟習此技藝之人士可 由本說明書所揭示之内容輕易地瞭解本創作之其他優點與功效。本創 作亦可藉由其他不同的具體實施例加以施行或應用,本說明書中的各 項細節亦可基於不同觀點與應用,在不悖離本創作之精神下進行各種 修飾與變更。 41 M364878 【圖式簡單說明】’ 圖一為本實施例裝置設計示意圖。 圖二為薄膜反射率與光學厚度的變化關係圖。 圖三為設計本實施例樣品A的光譜圖。 -_ 圖四為樣品A鍍膜完成後的實際光譜圖。 圖五為樣品A1的反射光譜圖。 *圖六為樣品A2的反射光譜圖。 圖七為本實施例裝置應用示意圖。 圖八為本實施例裝置實驗示意圖。 圖九為内建紅外光源的裝置應用示意圖。 42 M364878 【主要元件符號說明】 L1入射光 -Lla反射光 …Lib透射光 Lie透射光 φ Lid透射光 Lie透射光 L2入射光 L2a透射光 L2b反射光 U L2c反射光 L3入射光 L3a紅外反射光 L3b紅外透射光 N膜的折射率 Ns基板的折射率 M364878About 18%). Simply put, the physical properties of light are determined by both amplitude and wavelength. The amplitude determines the intensity of the light, and the wavelength distinguishes the characteristics and types of the color, that is, the difference in amplitude, giving the difference between light and dark; and the difference in wavelength gives the difference in hue. The industry always selects those metals having a large extinction coefficient and a relatively stable optical property as a metallized film material. For example, the metal film material commonly used in the ultraviolet region is aluminum, which is commonly used in the visible region and silver, and gold, silver and copper are commonly used in the infrared region. In addition, chromium Cr and platinum are also commonly used as special coating materials. Since materials such as aluminum, silver, and copper are easily oxidized in the air to lower the performance, they must be protected by a dielectric film. The commonly used protective film materials are cerium oxide, magnesium fluoride, MgF2, and the like. Since the function of the metal film layer lc is to "all the light energy in the absorbing casing 2", the film of the metal film layer lc is not limited to chrome-plated Cr. Please refer to FIG. 3 for the spectrum of the sample A of this embodiment. As shown in FIG. 3, the requirements for the sample design of this embodiment are as follows: (1) In the visible light (400 nm to 700 nm) portion, it is desirable to control the average at 18 〇/〇. (2) The penetration rate in the infrared (780 nm to 1,000 nm) portion is %, and it is desirable to control the average value at 70% or more. 24 M364878 Preparation - A transparent cyan plate with a thickness of 3 mm is cleaned and reinforced and placed in a coater for Mg. There are three or more sheets in the coating machine, which are equipped with membranes such as leakage 5, Si〇2, and Cr. In Figure 3, the ordinate is the percentage of penetration T% (Transmjttance 0/〇). The abscissa is the spectral wavelength (in nm). Other parameters are (丨) white light environment, (2) frontal incident angle (twist) (3) reference wavelength is 450 nm., (4) is designed in a qUarter-wave-stack multi-layered mode. The film of the multi-layer dielectric film lb is selected as much as possible by selecting the least two combinations. It is not easy to find one or more when adding an appropriate combination. In the present embodiment, the dielectric film lb is formed by alternately vapor-depositing two kinds of film materials having different refractive indexes in a coater. Generally, two kinds of refractive index materials are selected, and there are often oxide films, such as Ti〇2 having a high refractive index and si〇2 having a low refractive index. Since Τι〇2 is prone to oxygen loss, and there are different structures (such as anatase coffee core, etc.). At present, electron retort or sputtering Ti2〇5 or Ti3〇5 is more stable than Ti〇2. The Ti3〇5 film is easier to absorb and scatter than the Ti〇2 film. Therefore, in this embodiment, a film having a different refractive index of Ti3〇5 (substituting Ti〇2) and Si〇2 is alternately vapor-deposited in the coating machine by 18 layers. The first layer: Ti3〇5. Optical film thickness = 〇. 5075 Second layer: Si〇2. Optical film thickness = 0.4615 Third layer: Ti3〇5. Optical film thickness = 2. 0697 Fourth layer: Si〇2. Optical film thickness = 〇. 3996 25 M364878 Fifth layer: Ti3〇5. Optical film thickness = 1. 2309 Sixth layer: Si〇2 plating. Optical film thickness = 0.921 The seventh layer: Ti3〇5. Optical film thickness = 0.656 '8th layer: Si〇2 plating. Optical film thickness = 1.2178 Ninth layer: Ti3〇5. Optical film thickness = 1.4742 Tenth layer: Si〇2 plating. Optical film thickness = 0.3776 11th layer: Ti3〇5. Optical film thickness = 4.1621 I Twelfth layer: Si镀2 plating. Optical film thickness = 0.8100 The thirteenth layer: Ti3〇5. Optical film thickness = 1. 7303 Fourteenth layer: Si〇2 plating. Optical film thickness = 1.5163 The fifteenth layer: Ti3〇5. Optical film thickness = 1.1209 Sixteenth layer: Si〇2 plating. Optical film thickness = 1.7299 The seventeenth layer: Ti3〇5. Optical film thickness = 1.4229 Eighteenth layer: Si〇2 plating. Optical film thickness = 2. 8657 & After plating the dielectric film lb, the metal film lc is plated, and the metal film has Cr. The layer of the Cr layer is 3 nm (Physical thickness). After the shovel film treatment is completed, the Japanese Hitachi spectrometer U-4100 is tested and the error is too large and corrected until the error is within the allowable range. Among them, sample A was made into two samples: sample Αι and sample A2. The sample is plated with a dielectric thin film on a surface of a 3 mm transparent green plate, and a metal film lc is plated on the same surface. Therefore, the sample A1 can be referred to as a face mask film. 26 M364878 When the sample is A2 is a thin film of 3mm transparent slab glass, while the metal film lc is on the other surface of the chain. Therefore, the sample A2 can be referred to as a double-sided forged film. • Finally, the spectrometer U-4100 test computer draws the curve 4A2 of the sample curve 4A1 and sample A2 as shown in Fig. 4. Fig. 4 is the actual spectrum of the sample A. In Figure 4, the ordinate is the percentage of penetration T% (Transmjttance %). The horizontal position is marked as the wavelength of the spectrum (in nm). As shown in Figure 4, the sample A after the coating is completed is tested by the spectrometer U-4100. The actual spectral curve of the sample is shown. (4) Three solid samples A were originally used. The simulated spectral curve of the design has a drop. The originally designed spectral curve (Fig. 3) is the penetration T of the desired lesion in the visible light range of 4〇〇nm~7〇〇nm. /. The average control is 18% » while the penetration rate T% of the infrared 780nm to 1,000nm part ® is controlled above 70%. However, in the actual spectral curve after the completion of the coating; the transmittance τ of the curve 4A1 in the visible light portion of 400 nm to 700 nm. /. The average (automated by the spectrometer) has a downward trend after 27.1%' to the long wavelength direction of 580 nm and rises until 75 〇 nm. In the infrared 780 nm to 1,000 nm portion, the transmittance τ% average (manual visual estimation) is about 75%. Curve 4A2 has a transmittance in the visible light range of 400 nm to 700 nm. The /0 average (spectrum meter 27 M364878 is automatically calculated) is 23%, and there is an upward trend in the long-wave direction. The average (% (manual visual estimation) of the transmittance in the infrared 780 nm to 1,000 nm portion is about 7〇% or more. From the curve 4Α1 and the curve 4Α2, the effect of plating double-sided and single-sided plating is not very different, but the working time of plating double-sided is relatively large (the flipping of the double-sided plating in this embodiment and the other side is required) Relatively high. Moreover, it is often necessary to add a protective film to the outer surface of the substrate which is easily stained and scratched. Moreover, when a single mask is applied, as shown in Fig. 4, there is a curve that is obviously convex in the visible light portion (such as at 570 nm). This is in addition to the refractive index of different colors in the visible light portion. In addition to the normal dispersion, the dielectric film layer lb is too close to the bond metal film (Cr) lc, which affects the interference of the dielectric film ratio, but it can be known from the actual situation. In the common ring thief, the non-professional high-resolution type has little effect on photographic imaging (the color shift phenomenon at 57 〇nm is not seen). _ If the difference between the high-bump point of the visible light portion curve and the low-pitched point of the curve is too large, it is possible to generate a color shift corresponding to the wavelength at the wavelength corresponding to the difference. To put it simply, if most of the difference checks correspond to the red silk circumference of the New York, the visible light image captured by the camera will produce a "red" color. If necessary, the design of increasing the number of layers can make the difference between the high-bump and the gamma of Figure 4 in the visible part of the hip, which will increase the manufacturing cost. In another example of the present embodiment, if the transparent substrate la is pMMA, the pMMA may be deformed due to the increase in the number of layers, and the initial solution of the 28 M364878 type is a slightly longer time interval when the layer is further plated. One point, so that there is enough time to cool down. In the latter application examples, the image tests of the samples A1 and A2 revealed that these curved curves in the visible light portion did not significantly affect the quality of the image (e.g., color shift phenomenon). In fact, for a design like Round Three, different coating machines will have different results. As described above, the computer can be corrected or the key film can be modified one or two more times. After the correction, the file will be stored and the same coating machine will be used to produce a stable product in the future. In addition, if the 3 nm thickness of the Cr-plated layer is tested by the final spectrometer, if the transmittance of Lie is less than 18% (or not ideal) after the test, the thickness of the Cr-plated layer is reduced (or re-corrected) and plated again. Until Lie's penetration rate is close to 18% (or close to the ideal value). After adjusting the penetration rate of Lie, what is the effect of plating the metal film lc? Lu, please refer to Figure 5 for the reflection spectrum of sample A1. In the reflection spectrum of Figure 5, the ordinate is the reflectance percentage R〇/〇. The abscissa is the spectral wavelength (in nm). In the reflection spectrum circle of sample A1, curve A10 is the front side (no coating surface) reflection spectrum curve of sample A1. The curve All is the reflection spectrum curve of the back side (the metal film ic surface) of the sample A1. It can be seen from the curve A10 and the curve All hyperbola that the lower reflection curve A11, 29 M364878 does have a metal film lc having an anti-reflection effect. That is to say, cr is built into the effect of "absorption", so it is also called a Cr layer as a metal film layer. Please refer to the reflection spectrum of sample A2. In the reflection spectrum of Figure 6, the ordinate is the reflectance percentage R%. The abscissa is the spectral wavelength (in nm). In the reflection spectrum of the sample A2, the curve A20 is a reflection spectrum curve of the front surface (plated dielectric layer lb surface) of the sample A2. The curve A21 is a reflection spectrum curve of the back surface (metal plated film lc plane) of the sample A2. From the curve A20 and the curve A21 hyperbola, it can be seen that the lower reflection curve A21, indeed, the metallized film lc has an anti-reflection effect. In other words, Cr achieves the effect of "absorption." The thickness of the Cr-plated layer is proportional to the effect of "absorption". That is, the thinner the thickness of the Cr-plated layer, the less the amount of absorption. The coated substrate 1 (including a 3 mm thick transparent blue plate glass, a TisOs and Si〇 2 dielectric film and a metal plated Cr film layer) after the above ore film is completed, and the lens 31 of the camera 3 is aligned with the coating base. The metal Cr film layer of the material 1 is used for application. Please refer to the seventh application diagram of the device in this embodiment. Figure 7 is also a schematic diagram of the application of the device shown in Figure 1. Fig. 7 includes a coated substrate 1, a housing 2, a camera 3, and a 30 M364878 image display 4 formed by sample A1. Also included are representative light rays that are conveniently described, such as L1, Lla, Lle, and L2a, L2b, L2c and L3, L3a, L3b, and the like. When the incident light LI (100%) is incident on the front surface of the coated substrate 1, the reflected light Lla is about 56% as shown in the fifth spectrum diagram, and the transmitted light penetrating through the coated substrate 1 as shown in the fourth spectrum. Lie is about 27%. About 56% of the reflected light Lla has a bright mirror surface on the front surface of the coated substrate 1 (see a mirror like a mirror). About 27% of the transmitted light Lie enters the photographic lens 31 for imaging. About 17% (100%-56%-27%) is lost in the coated substrate 1 (mostly absorbed by the Cr-plated layer). When the other incident light L2 (100%) is incident on the front surface of the coated substrate 1, the transmitted light L2a (the same as the transmitted light Lie) penetrating through the coated substrate 1 is about 27%. However, the transmitted light L2a does not directly enter the photographic lens 31 but is reflected in the casing 2 to form another reflected light L2b. When the reflected light L2b is reflected to the back surface of the coated substrate 1, a further reflected light L2c' is generated. The reflected light L2c is reflected into the photographic lens 31 for imaging, and the reflected light L2c and the transmitted light Lie enter the photographic lens 31 to cause overlapping images, which is commonly called ghost image affecting the quality of imaging. When the reflected light L2c is reflected to the back surface of the coated substrate 1 by about 56%, the light energy is about 15.1% (27% * 56%) of the incident light L2. M364878 In the test of this embodiment, if the incident light L2 is too small (for example, 5〇j_ux), the reflected light L2c is about 7.5Lux, and the reflected light L2c enters the photographic lens 31 together with the transmitted light Lie' on the image display 4 No image of L2c is displayed. If the incident light L2 is too large (for example, 300 Lux), the reflected light L2c is about 45 Lux, and the reflected light L2c enters the photographic lens 31 together with the transmitted light Lie to cause an overlapping image, and the image of the L2c is clearly displayed on the image display 4. In order to prevent or reduce the reflected light L2c from entering the photographic lens 31, there are three methods: First, an opaque black soft cover 32 is placed around the photographic lens 31 to block the reflected light L2c. The black soft cover 32 must be close to the back surface of the coated substrate without a light-transmissive gap, and the stray light other than the light directly entering the front of the photographic lens 31 (e.g., Ue) is blocked by the black soft cover 32. The black soft cover 32 is preferably black or dark. If white is used, the white reflection causes the eye to see a white trap image from the front surface of the coated substrate. The first method above, if applied to the currently popular High Speed Dome Camera, has a certain degree of difficulty. Because the mirror chatter of this type of high-speed dome camera is often used as an idle button, the black soft cover 32 on which it is placed will be hit to cause damage to the back surface of the coated substrate 1. Second, a black or dark thick wheel surface is formed on the inner surface 21 of the shell 2 . The purpose is to absorb and scatter L2a, making L2b difficult to form. That is to say, L2c is indirectly made indirectly. 32 M364878 In the second method above, if the coated substrate 1 is not a flat plate, but the new patent number M326646 "aluminized hemispherical cover photographic device" is generally hemispherical, the incident light L2 is transmitted to a hemispherical shape. When the substrate 1 is coated, it may be re-transmitted from the other side of the coated substrate 1 and is not transmitted to the inner surface 21 of the casing 2 at all. At this time, if someone looks at the incident direction of L2, it is easy to see the camera 3 behind the coated substrate. Second, a metal film layer is added in front of the photographic lens 31 to absorb or reduce the light energy. The third method above is one of the design priorities of this embodiment. Therefore, the third method as above is more suitable, but if the three methods can be combined, the application can exert a better effect. Please refer to FIG. 8 for the experimental example of the device in this embodiment. The difference between Figure 8 and Figure 7 is that the housing 2 of Figure 7 is removed in Figure 8. As shown in FIG. 8, when the incident light L2 is incident on the coated substrate 1 and the transmitted light L2a does not touch the object (for example, the casing 2), L2a continues straight ahead until the light energy is exhausted, and there is no occurrence. Reflect the problem of L2b. At this time, if the human eye sees the coated substrate 1 from the direction of L2, it will be found that the coated substrate 1 is in a transparent state, and the human eye can easily see the object behind the coated substrate 1, especially the illuminance behind the coated substrate 1 is greater than the coated substrate. The illuminance of the front of the material 1 (in the same direction as the human eye) is more obvious. 33 M364878 When the background environment of the coated substrate 1 is dark (for example, dark blue) or black (for example, in the casing 2), in the general environment (for example, an illumination environment of about 2 〇〇 Lux), the human eye is coated from the coating base. The front side of the material 1 can exhibit the effect of specular reflection when it has 50% or more of reflected light. More than 60% of the reflected light is more like a mirror surface, and more than 7〇% of the reflected light is more like a side ~ mirror. Figure 8 is one of the test work when the coated substrate 1 is completed, mainly testing the imaging of the coated back surface of the coated substrate 1 effect. This work is to align the lens 31 of the camera 3 with the back surface of the coated substrate 1, and then connect the image display 4 to test the imaging effect of the transmitted light Lie. The imaging effect displayed on the image display 4 depends mainly on the light energy of the transmitted light Lie and the imaging quality of the camera 3 under a certain ambient illumination. The larger the light energy ratio (percentage of incident light L1) of the transmitted light Lie, the better the imaging effect displayed on the image display 4. # However, the larger the light energy ratio of the transmitted light L1e, the smaller the relative reflected light L1a. The smaller the reflected light Lla, the less visible the mirror surface. Without the bright mirror surface, it is not easy to hide the object behind the decorative coating substrate 1 (such as the camera 3), which also loses the hidden decoration of this embodiment. The purpose of imaging. It is economical and reasonable to choose the light energy ratio of the transmitted light L1e from 10% to 30%. As for the imaging quality of the camera 3, it mainly refers to the sensitivity quality of the image sensor of the camera 3. There are many types of products commonly used in domestic and foreign markets, including Japanese s〇ny, Sharp and South Korea's Samsung, which have different types of high-end (end) and low-order (L〇w 34 M364878 end) models. For example, the camera 3 of the present embodiment has tested more than ten models of CCD and Cmos, and has achieved different imaging effects in different illumination environments. In order to save on the purchase of high-end, low-light cameras, it is an alternative to only purchase low-end cameras and properly pair the auxiliary light sources. Figure 8 shows the test work when the forged film substrate 1 is completed. That is to say, when the forged film substrate 1 is mass-produced, the coated substrate 1 can be separately sold to the quality test of the camera manufacturer or the system manufacturer. That is to say 'the separate forged film substrate 1 can be sold as a key component. A housing 2 is often added to the actual application to form a product that can be directly applied and sold. Please refer to Figure 9 for a schematic diagram of the application of the built-in infrared light source. Another application device is shown in FIG. The difference between FIG. 9 and FIG. 7 lies in that an infrared light source 5 and an aluminum casing 2 for facilitating heat dissipation of the infrared light source 5 are added to FIG. In recent years, the International Safety Equipment Exhibition has shown that there are day and night type anti-theft surveillance cameras, most of which combine the auxiliary infrared light source for night vision with the camera lens and then put it into the same aluminum housing 2 for convenient construction. . During the daytime (enough ambient light energy), visible light is taken, and at night (the ambient light energy is insufficient), the auxiliary infrared light source is used for photography. An infrared light-emitting diode called IR-LED is commonly used for night vision auxiliary light sources, and is the cheapest and convenient night vision auxiliary light source on the market. The center wavelength is usually 850nm, and the single power is about 100mW. In the finished products of day and night anti-theft cameras, 12, 24, 36 or even more than one hundred R-LEDs are often surrounded by a circuit board. And a circular cavity in the center of the circuit 35 M364878 is placed directly around the camera lens 31. An infrared light source 5 added in FIG. 9 is the same as a small-sized anti-theft surveillance photographing device (commonly known as a gun in Taiwan and China), which is also a combination of the infrared light source 5 and the camera lens 31. Placed in the same cabinet 2. The infrared light source 5 can also be disposed outside the casing 2 or independently of the casing 2. In recent years, most of the newly-produced rushing machines have adopted protective covers of single or double-layer transparent glass. _ Figure 9 is a protective cover for replacing the transparent glass with the coated substrate 1. The light emitted by the LED light source is 850 nm in the infrared range, which is within the range recognizable by the human eye. Therefore, the red glow is often referred to as the "red burst" in the industry, and is exposed at night. main reason. As shown in FIG. 9, the infrared ray radiated by the newly added infrared light source 5 in the case 为 2 is infrared L3 (the infrared radiation energy is assumed to be 100%), and when the infrared L3 is incident on the chain film substrate 1, 豢 infrared L3 is about 75% of the coated substrate 1 is infrared transmitted light L3b (as shown in Figure 4) and about 15% is infrared reflected light L3a (Figure 5), and most of the others are absorbed by the metal film lc of the mineral film substrate i. Drop it. When the infrared transmitted light L3b penetrates the coated substrate 1 and is incident on the object a, the object a is absorbed and then radiated out through the coated substrate 1, and the L3C enters the photographic lens 31 to be imaged (infrared image). In addition, if the infrared reflected light L3a is not blocked by the black soft cover 32, it may enter the 36 M364878 into the camera lens 31 for imaging, and the white exposed block is displayed on the image display 4. 'This white exposed block is the infrared light source 5 radiates infrared Block image. For example, if there is only one circular 5 mm infrared light emitting diode (|R-LED), the white exposed block is a circular white exposed block. If an object A is in front of the coated substrate 1, the transmitted light Lie enters the camera lens 31 under the incident of visible light L1, and finally the visible image of the object A is displayed on the image display 4. If the camera 3 is a color camera, the visible light image is a color image. If the camera 3 is a black and white camera, the visible light image is a black and white image. However, if an object A is in front of the coated substrate 1, when the infrared light source 5 emits light, the transmitted infrared light L3c enters the camera lens 31 for imaging, and finally an infrared image of the object A is displayed on the image display 4. This infrared image is a monochrome image that is similar to but different from the black and white image for the human eye. _ If an object A is in front of the coated substrate 1, when the incident of the visible light L1 and the infrared light source 5 are emitted, an overlapping image of the visible light image and the infrared image of the object A is displayed on the image display 4. At this time, if the visible light image is larger than the infrared image, the visible light image "over" the infrared image causes the visible light image of the object A to be displayed on the image display 4. At this time, if the visible light image is smaller than the infrared image, the infrared image "over" the visible light image causes the image display 4 to display an infrared image of the object A. At this time, if the visible image is close to the infrared image, both the visible light image and the infrared 37 M364878 image exist at the same time, so that the visible light image of the object A is displayed on the image display 4 but has a block similar to overexposure, resulting in poor image quality. . In order to avoid the display of an image of the visible light of the object A visible on the image display 4, the image is usually detected by a photoresistor (CDS) element. When the ambient illumination is insufficient (for example, about 1〇 Lux), the CDS component startup control circuit turns on the infrared light source 5 to generate infrared light. In this case, the infrared image is larger than the visible light image, so that the infrared image of the object A is displayed on the image display 4. . Figure 9 omits the CDS component because the CDS is a conventional component. The only thing to note is that the CDS component does not pass through the coated substrate 1 in the direction of incident visible light, because the transmittance of the coated substrate 1 is only 15% of the incident visible light, and is placed in the transparent glass with the usual CDS components (almost incident) 90% of visible light is different. If it must be placed in the position of the coated substrate 1, the sensitivity of the CDS element must be adjusted. That is to say, if the CDS element placed in the transparent glass is adjusted to be activated at 10 Lux, the CDS element placed after the coated substrate 1 should be adjusted between 60 and 70 Lux. At present, the high-end products are added to the space between the lens 31 of the camera 3 and the front of the image sensor, plus an automatic dual filter switching device. The automatic dual filter switching device currently on the market is simply a device that automatically switches two filters such as an infrared cut filter 丨CF (Infraredcutfiltter) and a common transparent glass filter. When the infrared cut filter is cut into the front of the image sensor, the entrance of the infrared L3c is blocked, and the image sensor only senses the visible light Lie. When the infrared cut-off filter is removed from the front of the image sensor, the image-sensing 38 M364878 sensor can sense both the visible light Lie and the infrared L3c due to the cut-in relationship of the ordinary transparent glass filter. In this embodiment, the camera 3 is further modified into a camera 3 with an automatic dual filter switching device according to FIG. 9 , wherein the CDS element is placed on the casing 2 (without passing through the film substrate 1), and the original The setting of the CDS component (starting at i〇Lux) remains unchanged. - The result is found that the visible light Lie and the infrared L3c can be sensed when the image sensor of the camera 3 cuts into the ordinary transparent glass filter. The main reason is that when the ambient illuminance is about 10 Lux, the CDS component starts to move the ordinary transparent glass filter into the image sensor of the camera 3, so that the visible light L1 e and the infrared L3c both enter the image sense of the camera 3. Detector imaging. Among them, the camera 3 of the high-order product has an ambient illumination of about 〇Lux, and the CDS element activates the infrared light source 5 in addition to the automatic dual filter. This gives the opportunity to have both an image of visible light Lie and infrared L3c (causing an image with a similar exposure, unless it is a professional artistic photography, it is not suitable for anti-theft photography surveillance purposes). In order to make both the visible light Lie and the infrared L3c images, there is no chance to simultaneously display them on the image display 4. In this embodiment, the ordinary transparent glass optical passage of the automatic double filter switching device is removed, and a type of IPF (Infrared Pass filtter) is used, which is opposite to the ICF. The 丨PF only allows infrared Pass through the visible light Lie through. With such an automatic dual filter (IPF and ICF) switching device, the chance of an image appearing in which the visible light Lie and the infrared L3c are mixed on the image display becomes not easy. 39 M364878 In summary, the above-mentioned coated substrate is imaged, Suitable for the camera, the housing 2 including an opaque container is placed on the side of the housing 2 with the _coated substrate t and the inside of the housing 2 housing an image taking unit (camera 3). The summary is as follows: (1) In order to prevent or attenuate the reflected light L2c and the infrared reflected light L3a from entering the photographic lens 31, if only one layer of dielectric film is plated on the coated substrate ,, the periphery of the photographic lens 31 is nested. An opaque black soft cover 32 or a black or dark raw sugar surface is formed on the inner surface 21 of the casing 2. (2) In order to prevent or attenuate the reflected light L2c and the infrared reflected light L3a from entering the photographic lens 31, such as a multilayer dielectric film lb and a metal film layer lc, the metal film layer 1c can be used to reflect the light L2c and the infrared The reflected light L3a absorbs and attenuates. The multilayer dielectric film lb and a metal film layer lc may be forged together on the same side of the coated substrate j or separately on the different faces of the coated substrate 1. (3) In order to prevent or attenuate the reflected light L2c and the infrared reflected light L3a from entering the photographic lens U head 31, a black soft cover 32 may be added, or a black or dark roughness may be formed on the inner surface 21 of the casing 2. One of the three or three or three of the surface or a metal film layer lc is plated. (4) In order to prevent the reflected light L2c and the infrared reflected light L3a from entering the photographic lens 31 at the same time, an automatic double filter switching device is added in front of the image sensor of the camera 3, which includes an infrared cut filter ICF ( Infraredcutfiltter) and a switching device for infrared through the two filters of the PF (Infrared Passfiltter). M364878 (5) In order to achieve higher reflectance (e.g., reflected light Lla), a multi-layer dielectric film lb is plated on the coated substrate 1 to replace the prior art metal-plated aluminum. The above specific embodiments are illustrative of the embodiments of the present invention, and those skilled in the art can readily appreciate the other advantages and functions of the present invention from the disclosure herein. The present invention can also be implemented or applied by various other specific embodiments. The details of the present specification can also be modified and changed without departing from the spirit of the present invention. 41 M364878 [Simplified description of the drawings] FIG. 1 is a schematic diagram of the device design of the embodiment. Figure 2 is a graph showing the relationship between the reflectance of the film and the optical thickness. Figure 3 is a spectrum diagram of the sample A of this example. -_ Figure 4 shows the actual spectrum after the coating of Sample A is completed. Figure 5 is a reflection spectrum of sample A1. * Figure 6 is a reflection spectrum of sample A2. FIG. 7 is a schematic diagram of the application of the device in the embodiment. Figure 8 is a schematic view of the apparatus of the present embodiment. Figure 9 is a schematic diagram of the application of the built-in infrared light source. 42 M364878 [Description of main components] L1 incident light-Lla reflected light... Lib transmitted light Lie transmitted light φ Lid transmitted light Lie transmitted light L2 incident light L2a transmitted light L2b reflected light U L2c reflected light L3 incident light L3a infrared reflected light L3b Infrared transmission light N film refractive index Ns substrate refractive index M364878

Nd光學厚度 R%反射率百分比 • T%穿透率百分比 ^ 1鍍膜基板 la透明基材 # lb多層介電質膜 lc金屬膜層 2殼體 21殼體内表面 3攝影機 U 31鏡頭 32黑色軟套 4影像顯示器 5紅外光源 44Nd optical thickness R% reflectance percentage • T% transmittance percentage ^ 1 coated substrate la transparent substrate # lb multilayer dielectric film lc metal film layer 2 housing 21 housing inner surface 3 camera U 31 lens 32 black soft Set of 4 image display 5 infrared light source 44

Claims (1)

M364878 九、申請專利範圍 1. 一種鍍膜基板成像裝置,適用於攝影,包含有: 板與 一殼體,該殼體為一不透光容器,該殼體的一侧玫置有一锻膜基 該殼體的内部收納有一取像單元; 一鍵膜基板,該鏟膜基板為包含有一鍍有多層介電質膜的透^月基^ 一取像單元,該取像單元的取像窗口面對於該鍍膜基板的背面,’ 其中可見光入射到該鍍膜基板的多層介電質膜呈現高反射 : 透’以及;紅外入射到該鍍膜基板的多層介電質膜呈現古反射氐穿 其中,該 2.依據申請專利範圍第丨項所述之一種鍍膜基板成像裝置, 殼體内部表面形成有黑色或深色的粗糙表面。 其中,該 其中,該 3·依據申請專利範圍第丨.述之—種鍍膜基板成像裝置, 殼體内部設置有一紅外光源。 ’ U 4·依射請專利範圍第丨項所述之—種麵基板成像 鍍膜基板上更包含有一鍍金屬膜層。 , 5. 依據申請專利範圍第丨項所述之 鍵多卿職二種高低不同折射率置,其中,該 6. 依據申請專利範圍第5項所述之一種錢膜基板成像裝置 鑛-種高低不同折射率的鍍膜材料是兩種氧化物。 、中,該 7·依據申細細峨跑,其中,該 45 M364878 鍍二種高低不同折射率的鐘膜材科是五氧化三欽與二氧切兩種。 8.依據申請專概群4項所述之—種賴基減雜置,其中,該 鍍金屬膜層的金屬是鉻(cr)e 。9.依據申請專利範圍第i項所述之一種鑛膜基板成像裝置,其中,該 鍵膜基板雜可為平、曲面狀或平面與曲面的混合狀。 10. 依據申請專利範圍第i項所述之一種鍍膜基板成像裝置,其中,該 籲透明基材為玻璃。 Λ 11. 依據申請專利範圍第i項所述之—種鍍膜基板成像裝置,其中,該 透明基材為光學級樹脂。 Λ 12. 依據申請專利範圍帛6項所述之一種鍍膜基板成像裝置,其中,該 光學級樹脂為聚破酸樹脂PC。 S ^ 13·依據申請專利範圍第i項所述之一種鍵媒基板成像裝置,其中,該 取像單元為CMOS。 S 14·依據申料利範圍帛1項所述之-種麵基板成像褒置,其中,該 取像單元為CCD。 15·依據申請專利範圍第15項所述之一種鍍膜基板成像裝置,其中, 該CCD設置有-包含有一紅外通過遽光片與一紅外截止遽光片的雙據 光片切換裝置。 46 M364878 16.依據申請專利範圍第13項與第14項所述之一種鍍膜基板成像裝 置,其中,該取像單元的鏡頭套有一黑色軟套。M364878 IX. Patent Application Range 1. A coated substrate imaging device suitable for photography, comprising: a plate and a casing, the casing being an opaque container, and a side of the casing is provided with a forged film base An image capturing unit is disposed in the interior of the housing; the shovel substrate includes a transparent image substrate coated with a plurality of dielectric films, and the image capturing window of the image capturing unit is The back surface of the coated substrate, 'the multilayer dielectric film in which visible light is incident on the coated substrate exhibits high reflection: through; and the infrared dielectric film incident on the coated substrate exhibits an ancient reflection and penetrates therein. According to a coated substrate image forming apparatus according to the above application, the inner surface of the casing is formed with a black or dark rough surface. Wherein, wherein, according to the scope of the patent application, a coated substrate imaging device is provided, and an infrared light source is disposed inside the casing. </ br> </ RTI> <RTIgt; </ RTI> <RTIgt; </ RTI> <RTIgt; </ RTI> <RTIgt; </ RTI> <RTIgt; 5. According to the application of the scope of the patent application, the two types of high and low refractive index of the key multi-clearing, wherein the 6. according to the scope of claim 5 of the money film substrate imaging device mine-species Coating materials of different refractive indices are two oxides. In the middle, the 7th is run according to the application. Among them, the 45 M364878 is coated with two kinds of high and low refractive index discs. 8. According to the application of the general group 4, the type of the base is reduced, wherein the metal of the metallized layer is chromium (cr)e. 9. The mineral film substrate imaging apparatus according to the invention of claim 1, wherein the key film substrate is a flat, curved surface or a mixture of a plane and a curved surface. 10. A coated substrate image forming apparatus according to the invention of claim 1, wherein the transparent substrate is glass. Λ 11. The coated substrate imaging apparatus of claim i, wherein the transparent substrate is an optical grade resin. Λ 12. A coated substrate image forming apparatus according to claim 6, wherein the optical grade resin is a polybroken acid resin PC. The invention relates to a key media substrate imaging device according to the invention of claim 1, wherein the image capturing unit is a CMOS. S 14· The seed surface substrate imaging device according to the claim 1 , wherein the image capturing unit is a CCD. The coated substrate imaging apparatus according to claim 15, wherein the CCD is provided with a dual-light-switching device including an infrared light-passing sheet and an infrared-cutting light-emitting sheet. A coated substrate imaging apparatus according to any one of claims 13 to 14, wherein the lens unit of the image taking unit has a black soft cover. 4747
TW97215929U 2008-09-04 2008-09-04 Image forming apparatus for coating substrate TWM364878U (en)

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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10261025B2 (en) 2016-11-04 2019-04-16 Industrial Technology Research Institute Workpiece surface detection method and system using the same
CN113064030A (en) * 2021-03-16 2021-07-02 华北电力大学 Optical fiber EFPI sensor, manufacturing method and measuring system

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10261025B2 (en) 2016-11-04 2019-04-16 Industrial Technology Research Institute Workpiece surface detection method and system using the same
CN113064030A (en) * 2021-03-16 2021-07-02 华北电力大学 Optical fiber EFPI sensor, manufacturing method and measuring system

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