1235845 (1) 玖、發明說明 【發明所屬之技術領域】 本發明主要是有關一種高性能攝像鏡頭與攝像裝置， 適用於使用CCD與CMOS類型的固體攝像元件之極爲精 密的行動電話或行動模組相機等。 【先前技術】 具有C C D等固體攝像元件的相機模組，攝像鏡頭 (或攝影鏡頭）與攝像元件之間，爲確保配置低通濾光鏡 或覆蓋玻璃等光學元件的空間，要求保留有一定的後焦距 (透鏡最後面與成像面的距離）。 再者’內建於行動電話等的相機模組，需將攝像鏡頭 的光學長度縮到極短，設計成小型化。更且，伴隨固體攝 像元件的高像素化，亦要求攝像鏡頭有更高的解析度。 爲」滿足如此的需求’開發有經由複數的透鏡構成攝 像鏡頭，雖然爲小型仍有修正諸像差，之高解析度攝像鏡 頭。例如，專利文件1中則揭示有此種攝像鏡頭。 〔專利文件1〕 日本特開2003 — 7^7]9號 【發明內容】 但是，專利文件】中記載的攝像鏡頭，自女，、.丁 ^ 錢有以下的問 題。專利文件]中記載的攝像鏡頭，係自％ ^ u β物體方向開 - 4 - (2) 1235845 始，依序裝配雙面非球面之雙凸面凸透鏡、和以凸面面向 成像側的彎月形狀凸透鏡；此種構造的後焦距（自彎月形 狀正透鏡之像側之面至成像處之距離）過短，而透鏡光學 長度（自鏡頭開口光圈面至彎月形狀正透鏡之像側之面之 距離+後焦距）卻過長，並不適合內建於行動電話等薄型 製品之中。 因此’本發明之目的，即爲解決上述傳統攝像鏡頭之 問題’提供具有足夠之後焦距與更短之光學長度，精密且 局性能的攝像鏡頭。 更甚者’本發明並同時以提供裝配此種攝像鏡頭之小 型化攝像裝置爲目的。 本發明之中所提到的攝像鏡頭，其特徵係具有雙凸面 鏡之正能量（聚光），雙凸面爲非球面之第1透鏡，和具 有向物體側爲凹面之彎月形狀具有負能量（散射）、雙面 爲非球面之第2透鏡，前述第1、第2透鏡自物體側依序 配置’並滿足下記之計算式（1 )與計算式（2 )。1235845 (1) 发明 Description of the invention [Technical field to which the invention belongs] The present invention is mainly related to a high-performance camera lens and camera device, which is suitable for extremely precise mobile phones or mobile modules using CCD and CMOS type solid-state image sensors. Camera, etc. [Previous technology] For a camera module with a solid-state imaging element such as a CCD, between the imaging lens (or photographic lens) and the imaging element, in order to ensure the space for disposing a low-pass filter or covering optical elements such as glass, a certain amount of space must be reserved. Back focal length (distance between the rearmost surface of the lens and the imaging surface). Furthermore, a camera module built in a mobile phone or the like needs to reduce the optical length of the camera lens to an extremely short length and design it to be compact. Furthermore, with the increase in pixelation of solid-state imaging devices, higher resolutions are required for imaging lenses. In order to "meet such needs", a high-resolution camera lens has been developed that uses a plurality of lenses to form a camera lens. Although it is small, it corrects various aberrations. For example, Patent Document 1 discloses such a camera lens. [Patent Document 1] Japanese Patent Laid-Open No. 2003-7 ^ 7] No. 9 [Summary of the Invention] However, the camera lens described in the patent document has the following problems. [Patent Document] The camera lens described in the document is from% ^ u β object direction-4-(2) 1235845, sequentially assembled double-sided aspherical lenticular convex lens, and meniscus convex lens with convex surface facing imaging side ; The back focal length of this structure (the distance from the image-side surface of the meniscus-shaped positive lens to the imaging location) is too short, and the optical length of the lens (from the aperture surface of the lens opening to the image-side surface of the meniscus-shaped positive lens) Distance + back focus) is too long, not suitable for built-in thin products such as mobile phones. Therefore, 'the object of the present invention is to solve the above-mentioned problems of the conventional camera lens' and to provide a camera lens with sufficient rear focal length and shorter optical length, precise and local performance. What is more, the present invention also aims to provide a compact imaging device equipped with such an imaging lens. The camera lens mentioned in the present invention is characterized by having positive energy (condensing) of a biconvex mirror, a first lens having an aspheric surface, and a meniscus shape having a concave surface toward the object side having negative energy ( Scattering), a second lens with an aspherical surface on both sides, the aforementioned first and second lenses are sequentially arranged from the object side, and satisfy the following formulae (1) and (2).
V ^3 < ^ < 0 惟’ f爲透鏡全系之焦距，bf爲後焦距（從第2透 鏡之像側之面到成像點之距離)，r3爲第2透鏡之物體 側之面之近軸曲率半徑，^爲第2透鏡之像側之面之近軸 ®半半徑’心爲第2透鏡光軸上之芯厚度，以爲第2透 (3) 1235845 鏡之d線折射率。 在計算式（1 )中，即訂定了第2透鏡爲凹透鏡（負 透鏡）之事實。而計算式（2 )，則是將後焦距（b f )與 鏡頭全系之焦距（f )之比率訂在0.6到0.8的範圍之間； 藉此既可得到足夠的後焦距，同時也能縮短透鏡光學長 度。也就是說，當此比率小於 〇. 6時，後焦距將變得過 短，造成於第2透鏡與成像面之間配置光學濾鏡等元件的 困難。另一方面，若是比率大於0.8，透鏡光學長度將會 過長，相對於行動電話或超薄相機等的使用將產生困難。 本發明的攝像鏡頭，其特徵係爲了達到最佳效果，於 上述第1透鏡之物體側加裝開口光圈，並滿足下記之計算 式（3 )與計算式.（4 )。V ^ 3 < ^ < 0 except that f is the focal length of the entire lens system, bf is the back focal length (the distance from the image-side surface of the second lens to the imaging point), and r3 is the object-side surface of the second lens The paraxial radius of curvature, ^ is the paraxial® half-radius' center of the image-side surface of the second lens is the thickness of the core on the optical axis of the second lens, which is the d-line refractive index of the second lens (3) 1235845. In the formula (1), the fact that the second lens is a concave lens (negative lens) is specified. The calculation formula (2) is to set the ratio of the back focal length (bf) to the focal length (f) of the entire lens system in the range of 0.6 to 0.8. This can not only obtain a sufficient back focal length, but also shorten it. Lens optical length. In other words, when this ratio is less than 0.6, the back focal length becomes too short, which makes it difficult to arrange elements such as an optical filter between the second lens and the imaging surface. On the other hand, if the ratio is greater than 0.8, the optical length of the lens will be too long, which will make it difficult to use compared to mobile phones or ultra-thin cameras. The imaging lens of the present invention is characterized in that, in order to achieve the best effect, an aperture stop is installed on the object side of the first lens, and satisfies the following formulas (3) and (4).
1.9 < ^ < 2. 1.2 <M< 1 / 惟，Φ爲透鏡全系之合成折射力，Φι·2爲第1透鏡之 像側面之折射力，Τ爲從開口光圈之物體側之面至第2透 鏡之像側之面之距離。 計算式（3 )將透鏡全系折射力Φ與第1透鏡之像側 之面之折射力Φι·2之比率，訂在1 .9到2.5的範圍之間。 當該比率小於].9時，第1透鏡之像側之面之折射力將變 得過弱；這將會造成焦距拉長，而不適合小型化程序。另 一方面，若該比率大於2.5，第1透鏡之像側鏡之面之弧 -6- (4) 1235845 度需求將變的相當嚴格，使得透鏡的製作困難度提高。 計算式（4)將透鏡光學長度（T + bf)，與透鏡全系 焦距（f )之比率，訂在1 · 2到1 · 8的範圍之間。當該比率 小於1 · 2時，第1透鏡的聚光力將變的過小，造成像差修 正上的困難。另一方面，當該比率大於1 . 8時，總長度將 變的過長，而不適合小型化程序。依此做法，將透鏡光學 長度（T + bf)製成透鏡全系焦距（f)的到u倍，即 可獲得精密且能對應攝像元件之高解析度趨勢之高性能攝 像鏡頭。 本發明中記載之攝像鏡頭，係包含具備上述特徵之攝 像鏡頭，與攝取由上述攝像鏡頭所形成之影像之攝像元 件。攝像元件則是使用例如CCD等固體攝像元件。此種 攝像裝置，因爲係極爲精密之結構，故可用於小型化相機 或簿型相機之上。並且更可爲追求更佳表現，加裝過濾紅 外線（IR )之濾鏡或是低通濾光鏡等光學濾鏡，以求達到 更高的攝像性能。 【實施方式】 接下來說明本發明的實施行方式。本實施方式中所記 載之攝像透鏡1，如第丨圖所示，係以圖面之左側爲物體 側時’開口光圈S、雙凸面並有正能量（聚光）之第1透 鏡L1、對物體方向爲凹面之彎月形狀具有負能量（散 射）之第2透鏡L2等配件，自物體側開始沿光軸〇依序 配置組裝而成。第I與第2透鏡L ]、L2之鏡面係皆非球 (5) 1235845 面。故本實施方式之攝像鏡頭1，係由兩群兩片透鏡所構 成之鏡頭。 根據圖示，η係第1透鏡之物體側之面於光軸附近之 曲率半徑，r2係第1透鏡之像側之面於光軸附近之曲率半 徑’ r3係第2透鏡之物體側之面於光軸附近之曲率半徑， r 4係第2透鏡之像側之面於光軸附近之曲率半徑。d 0係 開口光圈與第1透鏡L 1之間隔距離，d 1係第1透鏡於光 軸上之芯厚度，d2係第1透鏡與第2透鏡之間隔距離， d 3係第2透鏡於光軸上之芯厚度，d4係第2透鏡與平行 平面玻璃（光學濾鏡）1 0之間隔距離，d5係平行平面玻 璃之厚度，d 6係平行平面玻璃1 0與覆蓋玻璃2 0之間隔 距離。以上之長度，皆爲光軸0沿線之長度。f係 透鏡全系之焦距，bf係後焦距（自第2透鏡之像側 之面至成像面Μ之距離），T係光軸上自開口光圈§之 物體側之面至第2透鏡之像側之面之距離。 配置於第2透鏡L2之像側與成像面Μ之間的平行平 面玻璃1 〇，係依需求而對固體攝像元件有必要的低通濾 光鏡或紅外線濾鏡等光學濾鏡。另外於平行平面玻璃]Q 與成像面Μ之間配置有覆蓋玻璃2 0。覆蓋坡璃2 〇，係作 爲保護CCD等固體攝像元件表面之用。 又，爲了使射入攝像鏡頭1之攝像元件之光線之人身寸 角更小’並使組裝更爲簡單，故於第1透鏡L1之物體側 配置開口光圈S。此種結構可藉由滿足以下計算式（J ) 與計算式（2 )，提供具有足夠之後焦距與更爿5之光^^ -8- (6) 1235845 度，精密且高顯像性能的攝像鏡頭。 < d3 < ^ < 0.1.9 < ^ < 2. 1.2 < M < 1 / However, Φ is the synthetic refractive power of the entire lens system, Φι · 2 is the refractive power of the image side of the first lens, and Τ is the object side of the aperture from the aperture The distance from the surface to the image-side surface of the second lens. The calculation formula (3) sets the ratio of the entire system refractive power Φ to the refractive power Φ 2 of the surface on the image side of the first lens to be in the range of 1.9 to 2.5. When the ratio is less than] .9, the refractive power of the image-side surface of the first lens becomes too weak; this will cause the focal length to be extended, which is not suitable for miniaturization procedures. On the other hand, if the ratio is greater than 2.5, the arc of the image-side mirror surface of the first lens -6-(4) 1235845 degrees will become quite strict, making it difficult to make the lens. The calculation formula (4) sets the ratio of the optical length (T + bf) of the lens to the focal length (f) of the entire system of the lens in the range of 1 · 2 to 1 · 8. When the ratio is less than 1.2, the condensing power of the first lens will become too small, causing difficulty in correcting aberrations. On the other hand, when the ratio is greater than 1.8, the total length becomes too long, which is not suitable for miniaturization programs. In this way, by making the optical length (T + bf) of the lens to u times the full focal length (f) of the lens, a high-performance camera lens that is precise and can respond to the high-resolution trend of the imaging element can be obtained. The imaging lens described in the present invention includes an imaging lens having the above characteristics, and an imaging element that captures an image formed by the imaging lens. The imaging element is a solid-state imaging element such as a CCD. This kind of imaging device has a very precise structure, so it can be used in miniaturized cameras or book cameras. In addition, for the pursuit of better performance, optical filters such as IR filters or low-pass filters are added to achieve higher imaging performance. [Embodiment] Next, an embodiment of the present invention will be described. As shown in FIG. 丨, the imaging lens 1 described in this embodiment is the first lens L1 having an aperture stop S, a biconvex surface, and positive energy (condensing) when the left side of the figure is the object side. A meniscus with a concave object direction and a second lens L2 with negative energy (scattering) and other accessories are sequentially arranged and assembled along the optical axis 0 from the object side. The mirror surfaces of the first and second lenses L] and L2 are aspherical (5) 1235845 surfaces. Therefore, the imaging lens 1 in this embodiment is a lens composed of two groups of two lenses. According to the figure, η is the radius of curvature of the object-side surface of the first lens near the optical axis, and r2 is the radius of curvature of the image-side surface of the first lens near the optical axis. R3 is the object-side surface of the second lens The radius of curvature near the optical axis, r 4 is the radius of curvature of the image-side surface of the second lens near the optical axis. d 0 is the distance between the aperture stop and the first lens L 1, d 1 is the core thickness of the first lens on the optical axis, d 2 is the distance between the first lens and the second lens, and d 3 is the second lens in the light The thickness of the core on the axis, d4 is the distance between the second lens and the parallel plane glass (optical filter) 10, d5 is the thickness of the parallel plane glass, and d 6 is the distance between the parallel plane glass 10 and the cover glass 20 . The above lengths are the lengths along the optical axis 0. f series lens focal length, bf back focal length (distance from the image-side surface of the second lens to the imaging surface M), T-axis optical axis from the object-side surface of the aperture stop§ to the image of the second lens The distance between the sides. The parallel-planar glass 10 arranged between the image side of the second lens L2 and the imaging surface M is an optical filter such as a low-pass filter or an infrared filter, which is necessary for the solid-state imaging element as required. In addition, a cover glass 20 is disposed between the parallel plane glass] Q and the imaging plane M. Covering glazing 20 is used to protect the surface of solid-state imaging elements such as CCDs. In addition, in order to make the body angle of light incident on the imaging element of the imaging lens 1 smaller 'and to make assembly easier, an aperture stop S is arranged on the object side of the first lens L1. This structure can provide accurate and high-definition imaging by satisfying the following formulas (J) and (2), with sufficient back focal length and more light of 5 ^^ -8- (6) 1235845 degrees Shot. < d3 < ^ < 0.
計算式（1 )制定了第2透鏡L2之合成折射力，而近 軸之合成折射力爲負折射力（散射）。藉由第2透鏡L2 之曲率半徑^及r4，與第2透鏡之芯厚度^2，以及其折 射率η 3之相互關係滿足計算式（1 )之情況，將可保持與 第1透鏡之正折射力（聚光）之平衡，並縮短整體長度。 計算式（2 )制定了透鏡之後焦距（bf )對於透鏡全 系焦距f之比例範圍，若是低於下限値，後焦距將過短， 造成平行平面玻璃10之干涉與透鏡後退之困難，同時造 成周邊光的銳利度不足。反之若高過上限値，全長將過 長，而難以得到所要求的薄型精密攝像鏡頭。 攝像鏡頭1滿足計算式（3 )與計算式（4 )時將有更 佳表現。 1 .9 < Φ；' < 2.5 Φ ...(3) 1.2 < ^T + b^< 1.8 ...(4) 惟，Φ爲透鏡全系之合成折射力，Φι·2爲第1透鏡之 像側之面之折射力。 另外，因計算式（3 )制定了第]透鏡L 1之像側之面 冬 (7) 1235845 另外，因計算式（3 )制定了第〗透鏡L 1之像側之面 r2之折射力，故若該數値低於下限値則全長將變的過長； 而超過上限値則第2透鏡L2之曲率半徑將變的過小，而 造成透鏡難以成形與成像彎曲的修正上之困難。 計算式（4 )，係於滿足計算式（3 )之結構條件下， 制定透鏡光學長度（T + bf)與透鏡全系焦距f之對比。若 低於下限値，則第1透鏡L1之折射力將高過所需，使得 與第2透鏡L2之平衡難以取得，並且無法得到良好畫面 性能。若高過上限値，則與舊式焦距型態相近，全長將變 的過長而無法得到精密之攝像鏡頭。 接下來說明本發明之實施範例。在各實施範例之中， Fno.係Fnumber，ω係半畫角，d爲透鏡間距離，nd係各 透鏡對於d線（5 8 7.6nm )之折射率，v d係各透鏡之阿 貝數。又，透鏡之各鏡面（r】，r2，1*3，i*4 )爲非球面之結 構；當以光軸方向爲Z軸，與光軸垂直之方向爲X軸’ 光之行進方向爲正向，圓錐定數爲k，非球面係數爲a、 b、c、d時，非球面之形狀可用計算式（5 )表示之。 Z =_^=L==_.+ ax4-fbx6 + cx8 + dx10 1、丨1 一 (k + l)> (實施範例1 ) 實施範例1之攝像鏡頭1 ’其剖面結構係如第一圖所 示。攝像鏡頭1之透鏡資料係如第六圖所示，而第]表之 -10- (8) 1235845 表面編號，係由物體側開始，沿光軸〇依序編成之。表 面編號0 ( S Τ 0 )相當於開口光圈s。表面編號1、2相當 於第1透鏡L】之r】、r2，表面編號3、4相當於第2透鏡 L2之r3、r4。表面編號5相當於平行平面玻璃之物體側之 面r5，表面編號6相當於平行平面玻璃之像側之面r6。間 ， 隔d係表示上述各表面間之光軸上間隔距離（d 1，d2， ^ d3，d4，d5，d6 )。第二表之數値係以科學記號表示，例 如「1.049 89E-01」即「1·04989χ1(Γ】」。覆蓋玻璃 20之 _ 厚度係0.4 m m。 從第7圖到第9圖，表示了實行範例的各種像差；第 7圖係球面像差，第8圖係非點像差，第9圖係彎曲像 差。根據第7圖，破折線係d線之球面像差，實線係F線 之球面像差，虛線係C線之球面像差。根據第8圖，實線 係切線方向成像面之像差，虛線係矢狀成像面之像差。第 九圖係對應d線之彎曲像差。另外，以上圖面所用之像差 記號適用於下記之實行範例2到5。 · (實行範例2-5 ) * 實行範例2到5的攝像鏡頭，其橫剖面圖如第2圖到 · 第5圖所示。又，實行範例2到5的透鏡資訊各自紀錄於 第10圖、第14圖、第18圖，以及第22圖之中；而實行 範例2到5之球面像差則各自紀錄於第n圖、第I 5圖、 第1 9圖，以及第2 3圖之中；實行範例2到5之非點像差 各自紀錄於第]2圖、第]6圖、第2 0圖，以及第2 4圖之 -11 - (9)1235845 中；實行範例2到5之彎由 17圖、第21圖，以及第25 第2 6圖的第1表係依; 透鏡資料，紀錄以計算式（ 第2 6圖的第2表，係依_ 料，紀錄以計算式（1 )到 的表可以明顯得知，據本發 頭，與專利文件 1相較之 (bf)，其透鏡光學長度（ 第二透鏡L2與成像面Μ之 濾鏡）1 0，除了能達到高解 ί象鏡頭與包含其攝像鏡頭之 ^照相機與超薄照相機。 以上雖說明了本發明之 特定之實行型式，並可依專 旨範圍，做多種變形與變更 係如以上說明所述，本 係由第1之雙凸面鏡與第2 (1 )與計算式（2 )的狀況 焦跑與極短光學長度所帶來 能’又有良好成本表現的攝 3像差各自紀錄於第1 3圖、第 圖之中。 據本發明之實行範例1到5之 1 )到（4 )所計算出之數値。 _專利文件1所記載之透鏡資 (4 )所計算出之數値。從以上 明之實行範例1到5之攝像鏡 下，不只是有充分的後焦距 T + bf )也相當的短。因此，在 間能加入平行平面玻璃（光學 析度的攝像之外，還能將該攝 攝像裝置小型化，以適用於小 最佳實行狀態，但本發明並無 利申請範圍內記載之本發明主 〇 發明之攝像鏡頭與攝像裝置， 之彎月形狀透鏡在滿足計算式 下所構成；可提供既有充分後 的之極精密而高性能之攝像功 像鏡頭與攝像裝置。 【圖式簡單說明】 〔第]圖〕 -12- (10) 1235845 本圖係表示關於本發明之實行形態之攝像鏡頭之結 構，也就是實行範例1之攝像鏡頭之結構。 〔第2圖〕 實行範例2之結構示意圖 〔第3圖〕 實行範例3之結構示意圖 〔第4圖〕 實行範例4之結構示意圖 〔第5圖〕 實行範例5之結構示意圖 〔第6圖〕 實行範例1之透鏡資料示意圖 〔第7圖〕 實行範例1之球面像差示意圖 〔第8圖〕 實行範例1之非點像差示意圖 -13- (11) 1235845 〔第9圖〕 實行範例]之彎曲像差示意圖 〔第10圖〕 實行範例2之透鏡資料示意圖 . 〔第1 1圖〕 實行範例2之球面像差示意圖 φ 〔第12圖〕 實行範例2之非點像差示意圖 〔第13圖〕 實行範例2之彎曲像差示意圖 〔第14圖〕 # 實行範例3之透鏡資料示意圖 〔第15圖〕 ~ 實行範例3之球面像差示意圖 〔第]6圖〕 實行範例3之非點像差示意圖 -14 - (12) 1235845 〔第]7圖〕 實行範例3之彎曲像差示意圖 〔第1 8圖〕 實行範例4之透鏡資料示意圖 〔第19圖〕The formula (1) specifies the combined refractive power of the second lens L2, and the combined refractive power of the paraxial axis is a negative refractive power (scattering). When the relationship between the curvature radius ^ and r4 of the second lens L2, the core thickness ^ 2 of the second lens, and its refractive index η 3 satisfies the calculation formula (1), the positive relationship with the first lens will be maintained. Refraction (focusing) balance and shorten overall length. Calculation formula (2) specifies the ratio of the focal length (bf) of the lens to the focal length f of the entire system of the lens. If it is lower than the lower limit 値, the back focal length will be too short, causing interference between the parallel plane glass 10 and the difficulty of the lens to recede. The peripheral light is not sharp enough. Conversely, if it exceeds the upper limit, the total length will be too long, making it difficult to obtain the required thin precision camera lens. Camera lens 1 will perform better when it satisfies calculation formula (3) and calculation formula (4). 1 .9 <Φ; '< 2.5 Φ ... (3) 1.2 < ^ T + b ^ < 1.8 ... (4) However, Φ is the synthetic refractive power of the entire lens system, Φι · 2 Is the refractive power of the image-side surface of the first lens. In addition, the refractive power of the image-side surface r2 of the first lens L 1 is established by the formula (3), and the refractive power of the surface r2 of the image-side lens L 1 is established by the formula (3). Therefore, if the number is lower than the lower limit, the total length will become too long; if it exceeds the upper limit, the curvature radius of the second lens L2 will become too small, which will cause difficulties in shaping the lens and correction of the imaging curvature. The calculation formula (4) is a comparison between the optical length (T + bf) of the lens and the focal length f of the entire lens system under the structural conditions that satisfy the calculation formula (3). If it is lower than the lower limit 値, the refractive power of the first lens L1 will be higher than necessary, making it difficult to achieve a balance with the second lens L2, and good picture performance cannot be obtained. If it exceeds the upper limit 値, it will be similar to the old type of focal length, and the total length will become too long to obtain a precise camera lens. Next, examples of the present invention will be described. In each implementation example, Fno. Is Fnumber, ω is the half-angle, d is the distance between lenses, nd is the refractive index of each lens with respect to the d-line (5 8 7.6nm), and v d is the Abbe number of each lens. In addition, each mirror surface of the lens (r), r2, 1 * 3, i * 4 is an aspherical structure; when the optical axis direction is the Z axis, the direction perpendicular to the optical axis is the X axis, and the traveling direction of the light is In the forward direction, when the conic constant is k and the aspheric coefficients are a, b, c, and d, the shape of the aspheric surface can be expressed by calculation formula (5). Z = _ ^ = L == _. + Ax4-fbx6 + cx8 + dx10 1, 1, 1 (k + l) > (Embodiment Example 1) The camera lens 1 of Embodiment 1 'its cross-sectional structure is like the first As shown. The lens data of the camera lens 1 is shown in the sixth figure, and the surface numbers of Table -10- (8) 1235845 are sequentially compiled from the object side along the optical axis 0. The surface number 0 (ST0) corresponds to the aperture stop s. The surface numbers 1 and 2 correspond to r] and r2 of the first lens L], and the surface numbers 3 and 4 correspond to r3 and r4 of the second lens L2. The surface number 5 corresponds to the object-side surface r5 of the parallel-plane glass, and the surface number 6 corresponds to the image-side surface r6 of the parallel-plane glass. The interval d indicates the distance (d 1, d2, ^ d3, d4, d5, d6) on the optical axis between the surfaces. The numbers in the second table are represented by scientific symbols, for example, "1.049 89E-01", that is, "1 · 04989χ1 (Γ]". The thickness of the cover glass 20 is 0.4 mm. From Figures 7 to 9, Various aberrations of the implementation example; Fig. 7 is a spherical aberration, Fig. 8 is an astigmatic aberration, and Fig. 9 is a curved aberration. According to Fig. 7, a broken line is a spherical aberration of line d and a solid line is F-line spherical aberration, dashed line is spherical aberration of line C. According to Fig. 8, solid line is aberration of imaging surface in tangential direction, and dashed line is aberration of sagittal imaging surface. Ninth image is corresponding to d-line Bending aberration. In addition, the aberration marks used in the above figures are applicable to the following implementation examples 2 to 5. · (exemplification example 2-5) * The camera lens of implementation examples 2 to 5 has a cross-sectional view as shown in FIG. 2 To Figure 5. Also, the lens information of Examples 2 to 5 are recorded in Figures 10, 14, 18, and 22 respectively; and spherical aberrations of Examples 2 to 5 are implemented. Then they are recorded in the nth, I5, 19, and 23; the non-point aberrations of the implementation examples 2 to 5 are recorded in the second], ] Figure 6, Figure 20, and Figure -11 in Figures -11-(9) 1235845; the implementation of the bending of Examples 2 to 5 is shown in Figure 17, Figure 21, and Table 1 in Figures 25 and 26. Depends on; lens data, records are calculated by the formula (Table 2 in Figure 26, according to _ materials, records are calculated by the formula (1) to the table can be clearly known, according to this issue, and patent document 1 phase Compared with (bf), its lens optical length (the second lens L2 and the filter of the imaging surface M) is 10, except that it can achieve a high resolution image lens and a camera and an ultra-thin camera including its imaging lens. In accordance with the specific implementation type of the present invention, various deformations and changes can be made according to the scope of the special purpose. As described above, this is the status of the first biconvex mirror and the second (1) and calculation formula (2). The focal aberration and extremely short optical length can bring about the aberrations with good cost performance. The aberrations of 3 are recorded in Fig. 13 and Fig. 1. According to the implementation examples 1 to 5 of the present invention) to (4 ) Calculated number. _ Calculated number of lens materials (4) described in Patent Document 1. From the above-mentioned implementation of the camera lens of Examples 1 to 5 In addition, not only does it have sufficient back focal length T + bf) but it is also quite short. Therefore, parallel plane glass (in addition to optical resolution imaging) can be added to the camera, and the camera and imaging device can be miniaturized to be suitable for small optimal implementation. However, the invention is not described in the scope of the invention. The camera lens and camera device of the main invention of the invention are composed of a meniscus lens that satisfies the calculation formula; it can provide an extremely precise and high-performance camera lens and camera device with sufficient performance. [Schematic description [Figure] -12- (10) 1235845 This figure shows the structure of the camera lens of the implementation form of the present invention, that is, the structure of the camera lens of Example 1. [Figure 2] The structure of Example 2 Schematic diagram [Fig. 3] Schematic diagram of implementation example 3 [Fig. 4] Schematic diagram of implementation example 4 [Fig. 5] Schematic diagram of implementation example 5 [Fig. 6] Schematic diagram of lens information for implementation example [Fig. 7] ] Schematic diagram of spherical aberration in Implementation Example 1 [Fig. 8] Schematic diagram of astigmatic aberration in Implementation Example -13- (11) 1235845 [Fig. 9] Implementation example] Curved aberration diagram (Figure 10) Schematic diagram of lens data for implementation example 2. [Figure 11] Schematic diagram of spherical aberration φ for implementation example 2 [Figure 12] Schematic diagram of astigmatic aberration for implementation example 2 [Figure 13] Implementation of curvature for example 2 Schematic diagram of aberrations [Fig. 14] # Schematic diagram of lens data for implementation example 3 [Fig. 15] ~ Schematic diagram of spherical aberration for implementation example 3 [Fig. 6] Schematic of astigmatic aberration for implementation example 14-(12 ) 1235845 [Fig. 7] Schematic diagram of bending aberration in Example 3 [Fig. 18] Schematic diagram of lens data in Example 4 [Fig. 19]
實行範例4之球面像差示意圖 〔第20圖〕 實行範例4之非點像差示意圖 〔第21圖〕Schematic diagram of spherical aberration in Implementation Example 4 [Fig. 20] Schematic diagram of astigmatic aberration in Implementation Example 4 [Fig. 21]
實行範例4之彎曲像差示意圖 〔第22圖〕 實行範例5之透鏡資料示意圖 〔第23圖〕 實行範例5之球面像差示意圖 〔第24圖〕 實行範例5之非點像差示意圖 -15- (13) 1235845 〔第25圖〕 實行範例5之彎曲像差示意圖 〔第26圖〕 本發明所記載之各實行範例之攝像鏡頭，與專利文件 . 1之各實行範例之攝像鏡頭之鏡頭功能對比之圖表。 _ 主要元件符號說明 φ L1第1透鏡 L2第2透鏡 η第1透鏡之物體側之面於光軸附近之曲率半徑 r2第1透鏡之像側之面於光軸附近之曲率半徑 r3第2透鏡之物體側之面於光軸附近之曲率半徑 r4第2透鏡之像側之面於光軸附近之曲率半徑 dl第1透鏡於光軸上之芯厚度 d2第1透鏡與第2透鏡於光軸上的間隔 修 d3第2透鏡於光軸上之芯厚度 d4光學濾鏡之厚度 ‘ d 5覆蓋玻璃之厚度 ' f透鏡全系之焦距 bf後焦距 S開口光圈 T從開口光圈S之物體側之面到第2透鏡之像側之 面之光軸上距離 -16 - (14) (14)1235845 Μ成像面 1攝像鏡頭 1 0平行平面玻璃（光學濾鏡） 2 0覆蓋玻璃Schematic diagram of bending aberration in Implementation Example 4 [Fig. 22] Schematic diagram of lens data in Implementation Example 5 [Fig. 23] Schematic diagram of spherical aberration in Implementation Example 5 [Fig. 24] Schematic of astigmatic aberration in Implementation Example -15- (13) 1235845 [Fig. 25] Schematic diagram of bending aberration of Implementation Example 5 [Fig. 26] The camera functions of the implementation examples described in the present invention are compared with those of the patent document. The chart. _ Explanation of main component symbols φ L1 1st lens L2 2nd lens η 1st lens's curvature radius on the object side near the optical axis r2 1st lens's image side surface on the optical radius r3 near the optical axis 2nd lens Curvature radius r4 near the optical axis of the object-side surface Curvature radius dl near the optical axis of the image-side surface d1 Core thickness of the first lens on the optical axis d2 The first lens and the second lens on the optical axis D3 the thickness of the core on the optical axis of the second lens d4 the thickness of the optical filter 'd 5 the thickness of the cover glass' f the focal length of the entire lens system bf the focal length S opening aperture T from the object side of the opening aperture S Distance from the optical axis to the image-side surface of the second lens -16-(14) (14) 1235845 Μ Imaging surface 1 Camera lens 1 0 Parallel plane glass (optical filter) 2 0 Cover glass
-17--17-