TWM356934U - Photographic lens and the photographic device using the same - Google Patents
Photographic lens and the photographic device using the same Download PDFInfo
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- TWM356934U TWM356934U TW97218489U TW97218489U TWM356934U TW M356934 U TWM356934 U TW M356934U TW 97218489 U TW97218489 U TW 97218489U TW 97218489 U TW97218489 U TW 97218489U TW M356934 U TWM356934 U TW M356934U
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Description
M356934 五、新型說明: 【新型所屬之技術領域】 本創作係關於一種攝影透鏡及使用該攝影透鏡的攝 景夕裝置’尤指一種使被攝體像成像的攝影透鏡及使用此攝 5 影透鏡的攝影裝置。 【先前技術】M356934 V. New description: [New technical field] This creation is about a photographic lens and a photographic device using the photographic lens, especially a photographic lens for imaging a subject image and using the photographic lens Photographic device. [Prior Art]
10 1510 15
以往’公知的有在車載用、手機用、監視用等的攝影 裝置中所使用的小型化、輕量化的且具有高耐候性的廣角 攝衫透鏡。這種攝影透鏡使成為被攝體的物體的像成像在 CCD元件或CMOS元件等攝影元件的受光面上(參照專利前 案1)。而且,還公知有由4片透鏡結構的且實現了小型化及 輕里化的廣角攝影透鏡(參照專利前案2、3)。 …一 J Μ 4、付网 /υ4號公報; 【專利前案2】日本特開2〇〇7_264676號公報,· 【專利前案3】日本特開2〇〇5_227426號公報。 然而’近幾年’ CCD元件或CM〇s元件等攝影元件的 視Γ二::素化迅速發展。隨此,車載用、手機用、監 〜、置所使用的攝影透鏡要進-步廣角化、小型 像差要減少,存在這樣的要求。 【新型内容】 20 M356934 一本創作是蓉於上述内容而被提出的,其目的在於提供 二種廣角化及小型化且光學性能提高的攝影透鏡及使 用此攝影透鏡的攝影裝置。 本創作的第一攝影透鏡,其中,從物體側依次具備·· 5具有負光焦度的第一透鏡、具有負光焦度的第二透鏡、具 有正,焦度的第三透鏡、光攔、及具有正光焦度的第四透 鏡’第二透鏡、第三透鏡、及第四透鏡是各透鏡的至少工 個透鏡面呈非球面的透鏡,滿足以下條件式⑴: 2-4<(D4+D5)/f<5.5 ......(1); 10 式中, D4 .第二透鏡和第三透鏡之間的空氣間隔;Conventionally, there are known wide-angle lens lenses that are small, lightweight, and have high weather resistance, which are used in imaging devices such as vehicles, mobile phones, and monitors. Such an illuminating lens images an image of an object to be a subject on a light receiving surface of an photographic element such as a CCD element or a CMOS element (see Patent P. 1). Further, a wide-angle photographic lens having a four-lens structure and achieving miniaturization and lightening is also known (see Patent Documents 2 and 3). 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。. However, in recent years, photographic elements such as CCD elements or CM 〇s elements have seen the rapid development of priming. Accordingly, there is a demand for the photographic lens used for the vehicle, the mobile phone, the monitor, and the camera to be wide-angled and the small aberration is reduced. [New Content] 20 M356934 A creation was proposed in the above-mentioned contents, and its object is to provide two kinds of photographic lenses which are wide-angled and miniaturized and have improved optical performance, and a photographic apparatus using the same. The first photographic lens of the present invention, wherein a first lens having a negative refractive power, a second lens having a negative refractive power, a third lens having a positive power, and a light barrier are provided in order from the object side. And the fourth lens, the third lens, and the fourth lens having positive refractive power are lenses in which at least one lens surface of each lens is aspherical, and the following conditional expression (1) is satisfied: 2-4 < (D4) +D5)/f<5.5 (1); 10 where D4 is the air gap between the second lens and the third lens;
05 ·第三透鏡的中心壁厚; f :攝影透鏡整個系統的焦距Q 第二透鏡的物體側透鏡面,較佳地在此透鏡面的有效 15徑内至少具有1個拐點,此透鏡面的中心部呈凸面,有效徑 周緣。P的正光焦度比中心部弱,或者此透鏡面的中心部呈 凸面’有效徑周緣部呈凹面。 本創作的第二攝影透鏡,其中,從物體側起依次包 括具有負光焦度,且將凹面朝向像側的彎月形透鏡的第 2〇 透鏡,物體側透鏡面呈非球面,此透鏡面的中心部呈凸 面,有效徑周緣部的正光焦度比中心部弱,或者此透鏡面 的中心部呈凸面,在有效徑周緣部具有負光焦度的第二透 鏡’具有正光焦度,物體側透鏡面呈非球面的第三透鏡; 光攔,和具有正光焦度,像側透鏡面呈非球面的第四透鏡。 4 M356934 第二攝影透鏡,較佳地滿足下述條 2.4<(D4+D5)/f<5.5 ......⑴; ;* 式中, D4j二透鏡和第三透鏡之間的空氣間隔 D5 .第三透鏡的中心壁厚 f :攝影透鏡整個系統的焦距。 第二透鏡,較佳地由此第 ,, ^ 乐—透鏡的對d線的阿貝數^ 们滿足以下條件式(2)的材料形成: "d3<45 ......⑺。 式⑺第三透鏡’較佳地此第三透鏡的焦距π滿足以下條件 LO<f3/f<3.〇 (3)。 15 ❿ 第二透鏡的像側透鏡面較佳為:此透鏡面的中心部呈 凹面,且有效徑周緣部的負光焦度比中心部弱。 。第三透鏡的物體側透鏡面較佳為:此透鏡面的中心部 王凸面’且有效徑周緣部的正光焦度比中心部弱。 第三透鏡的像側透鏡面較佳為:有效徑周緣部的光焦 度比此透鏡面的中心部弱。 第四透鏡的物體側透鏡面較佳為:此透鏡面的中心部 呈凹面’且有效徑周緣部的負光焦度比中心部強。 第四透鏡的像側透鏡面較佳為:此透鏡面的中心部呈 凸面,且有效徑周緣部的正光焦度比中心部弱。 第一透鏡和第二透鏡的合成焦距m、及第三透鏡和第 四透鏡的合成焦距f34,較佳地滿足以下條件式(句: 20 M356934 0.01<|fl2/f34|<0.5 ......(4)。 從第一透鏡的物體側透鏡面到攝影透鏡的成像面的 距離L ’較佳地滿足以下條件式(5): 7<L/f< 16 ......(5)。 5 本創作的攝影裝置,其中,包括:第一攝影透鏡或第 二攝影透鏡、和將該攝影透鏡所形成的光學像轉換成電氣 信號的攝影元件。 另外,「具有正光焦度的透鏡」及「具有負光焦度的 透鏡」,是至少對在近軸上的光焦度進行規定的透鏡。 1〇 「透鏡面的有效光線徑」意味著在通過透鏡面的有效 光線之中通過最外側(從光轴離得最遠的位置)的光線與該 透鏡面的交點所描繪的圓的直徑。而且’通過上述透鏡面 的有效光線為使用於成像被攝體像的光線。 此處,透鏡面的有效光線徑和透鏡面的有效徑一致。 15 ^而且,有效徑周緣部是由在通過各透鏡有效徑内的全 光線之中,通過最外側的光線與各透鏡面相交的點而成的 部位。 “而且,「透鏡面的中心部呈凸面,有效徑周緣部的正 光焦度比中心部弱」是意味著有效徑周緣部也如同中心部 2〇呈凸面,有效徑周緣部的曲率半徑值的絕對值比此中心部 的曲率半徑值的絕對值大的情況。 而且,「透鏡面的中心部呈凸面,在有效徑周緣部具 有負光焦度」是意味著透鏡面的中心部呈凸面,有效徑周 緣部呈凹面的情況。 M356934 進-步,「透鏡面的中心部呈凹面’有效徑周緣部的 立光焦度比中心、部弱」{意味著有效徑周緣部也如同中心 部呈凹面’有效徑周緣部的曲率半徑值的絕對 部的曲率半徑值的絕對值大的情況。 心 而且’ 「透鏡面的中心部呈凹面,在有效徑周緣部且 有正光焦度」i意味著透鏡面的中心部呈凹面 ; 緣部呈凸面的情況。 们文仫周05 · the center wall thickness of the third lens; f: the focal length of the entire lens of the photographic lens Q, the object side lens surface of the second lens, preferably having at least one inflection point in the effective 15 diameter of the lens surface, the lens surface The central part is convex and has a effective circumference. The positive refractive power of P is weaker than the central portion, or the central portion of the lens surface is convex. The effective diameter peripheral portion is concave. The second photographic lens of the present invention includes a second 〇 lens having a negative refractive power and a meniscus lens having a concave surface facing the image side in order from the object side, and the object side lens surface is aspherical, the lens surface The central portion has a convex surface, the positive refractive power of the peripheral portion of the effective diameter is weaker than the central portion, or the central portion of the lens surface is convex, and the second lens having negative optical power at the periphery of the effective diameter has positive refractive power, the object a third lens having an aspherical surface on the side lens surface; a light barrier; and a fourth lens having a positive refractive power and an aspherical surface of the image side lens surface. 4 M356934 The second photographic lens preferably satisfies the following section 2.4<(D4+D5)/f<5.5 (1); ;* where the air between the D4j two lens and the third lens Interval D5. Center wall thickness f of the third lens: focal length of the entire system of the photographic lens. The second lens, preferably the abbe number of the d-line of the music lens, satisfies the following conditional formula (2): "d3<45 (7). The third lens of the formula (7) is preferably such that the focal length π of the third lens satisfies the following condition LO<f3/f<3.〇 (3). 15 ❿ The image side lens surface of the second lens preferably has a concave portion at a central portion of the lens surface, and a negative refractive power at a peripheral portion of the effective diameter is weaker than a central portion. . The object side lens surface of the third lens is preferably such that the central portion of the lens surface is convex and the positive refractive power of the peripheral portion of the effective diameter is weaker than the central portion. The image side lens surface of the third lens preferably has a refractive power at a peripheral portion of the effective diameter which is weaker than a central portion of the lens surface. The object side lens surface of the fourth lens preferably has a concave portion at the center portion of the lens surface and a negative refractive power at the peripheral portion of the effective diameter is stronger than the central portion. The image side lens surface of the fourth lens preferably has a convex portion at a central portion of the lens surface, and a positive refractive power at a peripheral portion of the effective diameter is weaker than a central portion. The combined focal length m of the first lens and the second lens, and the combined focal length f34 of the third lens and the fourth lens preferably satisfy the following conditional expression (sentence: 20 M356934 0.01<|fl2/f34|<0.5.. The distance L ' from the object side lens surface of the first lens to the imaging surface of the photographic lens preferably satisfies the following conditional expression (5): 7 < L / f < 16 ..... (5) The photographic apparatus of the present invention includes: a first photographic lens or a second photographic lens, and a photographic element that converts the optical image formed by the photographic lens into an electrical signal. A lens having a degree of light and a lens having a negative power are lenses that define at least the power on the paraxial axis. 1 "The effective light path of the lens surface" means effective light passing through the lens surface. The diameter of a circle drawn by the intersection of the outermost light (the position farthest from the optical axis) and the lens surface, and the 'effective light passing through the lens surface is the light used for imaging the image of the subject Here, the effective ray diameter of the lens surface and the effective diameter of the lens surface are 15 ^ Further, the effective diameter peripheral portion is a portion which is formed by a point at which the outermost light rays intersect the respective lens faces among the total rays passing through the effective diameter of each lens. "And, "the center portion of the lens surface" The convex surface is such that the positive refractive power of the peripheral portion of the effective diameter is weaker than the central portion. This means that the effective diameter peripheral portion is also convex like the central portion 2〇, and the absolute value of the radius of curvature of the effective diameter peripheral portion is larger than the radius of curvature of the central portion. In the case where the absolute value of the value of the lens surface is convex, the central portion of the lens surface has a negative refractive power, which means that the central portion of the lens surface has a convex surface, and the effective diameter peripheral portion has a concave surface. M356934 progresses, "the central portion of the lens surface is concave". The effective power of the peripheral portion of the effective diameter is weaker than the center and the portion." This means that the peripheral portion of the effective diameter is also concave like the central portion. The radius of curvature of the peripheral portion of the effective diameter. When the absolute value of the radius of curvature value of the absolute portion of the value is large, the center of the lens surface is concave, and the positive refractive power is present at the periphery of the effective diameter. i means the center of the lens surface. It is concave; is convex edge portion of the case are text Mu weeks.
10 有效徑周緣部的光焦度比透鏡面的中心部的光焦 度弱」是意味著有效徑周緣部也如同中心部呈凸面,有: ,周緣部的正光焦度比中心部弱的情況,或者有效徑周緣 =也如同中心部呈凹面,有效徑周緣部的負光焦度比中心 部弱的情況。 透鏡面的中心部呈凹面,有效徑周緣部的負光焦度 比令〜部強」是意味著有效徑周緣部也如同中心部呈凹 15面,有效徑周緣部的曲率半徑值的絕對值比此中心部的曲 率半控值的絕對值小的情況。 _另外中〜部的曲率半徑是意味著在透鏡面與光軸相 交的位置的透鏡面的曲率半徑。 而且,以絕對值表示曲率半徑值的理由是為了明確曲 20率半徑的大小關係。 旦,根據本創作的第一攝影透鏡及使用此攝影透鏡的攝 〜裝置’從物體側起依次包括:具有負光焦度的第-頭鏡、 :有負光焦度的第二透鏡、具有正光焦度的第三透鏡、光 及”有正光焦度第四透鏡,第二透鏡、第三透鏡、及 M356934 第四透鏡是各透鏡的至少1個透鏡面呈非球面的透鏡,且滿 足條件式(1) : 2.4<(D4+D5)/f<5.5,所以,可進行廣角化及 小型化的同時提高光學性能。 透過在最靠物體側配置負的第一透鏡、第二透鏡,可 5以捉住以大視角入射而來的光線,可進行廣角化。透過將 第二透鏡的至少一側面設為非球面,而可良好地校正諸像 差的同時,可使透鏡系統小型化。在第二透鏡中,軸上光 線和軸外光線被分離,因此,若將此透鏡設為非球面,則 、 在权正像差方面是有利的,崎變的校正也比較容易。 1〇 另外,第一透鏡的軸上光線和軸外光線也被分離,但 作為配置在透鏡系統的最靠物體側的第一透鏡U的材 貝,較佳地使用如後述的玻璃材料。而且,第一透鏡在透 鏡系統中成為最大口徑透鏡。從這些情況,將容易適用塑 料材質的第二透鏡設為非球面透鏡,則在透鏡製作上及像 15差校正上是較佳的。 、而且,將第三透鏡、第四透鏡均設為至少—側面為非 球面的具有正光焦度的透鏡,透過將光欄配置在第三透鏡 和第四透鏡之間,而可良好地校正像面彎曲、彗形像差的 同時,使透鏡系統小型化。 2〇旦根據本創作的第二攝影透鏡及使用此攝影透鏡的攝 影裝置,從物體側起依次包括:具有負光焦度,將凹面朝 向像側的彎月形透鏡的第一透鏡;物體側的透鏡面呈非球 面,此透鏡面的中心部呈凸面,且有效徑周緣部的正光焦 度比中〜部弱,或者此透鏡面的中心部呈凸面,且在有效 M356934 徑周緣部具有負光焦度的第二透鏡;具有正光焦度,物體 側透鏡面呈非球面的第三透鏡;光攔;和具有正光焦产, 像側透鏡面呈非球面的第四透鏡,所以,可進行廣角化及 小型化的同時提高光學性能。 5 、透過在最靠物體側配置負的第一透鏡、第二透鏡,可 以捉住以大視角入射而來的光線,可進行廣角化。 . 巾且’將第一透鏡設為在物體側具有負光焦度且凹面 φ 帛向像側的’幫月形透鏡,而可將拍兹伐和設小,可在廣視 、 角全領域範圍校正像面彎曲。 而且透過將第二透鏡的至少一側面設為非球面,而 γ良好地校正諸像差的同時,可使透鏡系統小型化。在第 -透鏡中,軸上光線和轴外光線被分離,因此,若將此透 ^設為非球面,則在校正像差上有利,也比較容易校正時 15 、另外,第一透鏡的軸上光線和軸外光線也被分離,但 #為配置在透鏡系統的最靠物體側的第一透鏡的材質,較 ’ @地使用如後述的玻璃材料。而且’第—透鏡在透鏡系統 中成為最大口徑透鏡。從這些情況,將容易適用塑料材質 的第二透鏡設為非球面透鏡,則在透鏡製作上及像差校正 20 上為較佳。 ^透過將第二透鏡的物體側面設為非球面,容易使透鏡 系統小型化、廣角化。而且,透過將第二透鏡的物體側面 設為透鏡面的中心部呈凸面,有效徑周緣部的正光焦度比 中心部弱’或者此透鏡面的中心部呈凸面,在有效徑周緣 M356934 =㈣光焦度的面,而容易使透鏡系統小型化、廣角化 、同吋,可良好地校正像面彎曲。 、 而且,將第三透鏡、第四透鏡均設為至少-側面為非 球面的具有正井隹序沾、泰# ^ w曲马非 有A焦度的透鏡’透過將光攔配置在第三透鏡 四透鏡之間’而可良好地校正像面彎曲、鞋形像差的 同時’使透鏡系統小型化。 透過將第三透鏡物體側的面設為非球面,可良 正像面彎曲。 透過將第四透鏡像側的面設為非球面,可良好地校正 像面彎曲和彗形像差。 【實施方式】 以下,參照附圖對本倉“乍的攝影透鏡及使用此攝影透 鏡的攝影裝置的實施方式進行詳細說明。 15 是表示使用本創作的攝影透鏡的攝影裝置的概略 t構的剖視圖’圖2是對圖加了用於說明的輔助線等的 圖。 圖示的攝影透鏡20是用於在戶外對周圍狀況進行攝影 的車載用或防盜用攝影裝置所使用的廣角攝影透鏡,其使 2〇被攝體的像成像在由CCD4CM〇s等而成的攝影元件1〇的 受光面Jk上。此攝影元件10將攝影透鏡2〇所形成的光學像 轉換成電氣尨號,而獲得表示此光學像的圖像信號。 首先,對攝影透鏡20的基本結構進行說明。攝影透鏡 20沿著光軸Z1從物體側起依次包括有:第一透鏡u、第二 10 M356934 透鏡L2、第三透鏡⑴孔徑光攔&、第四透鏡 部件Cg 1。 另外,在此處對第一透鏡L1〜第四透鏡L4的各透鏡為 單透鏡的情況進行說明,但這些透鏡不限於單透鏡,也可 5 以為接合透鏡等。 在通過此攝影透鏡20而成像有表示被攝體的物體像的 成像面R12上,配置有攝影元件1〇的受光面Jk。The power of the peripheral portion of the effective diameter is weaker than the refractive power at the central portion of the lens surface. This means that the peripheral portion of the effective diameter is convex like the central portion, and the positive refractive power of the peripheral portion is weaker than the central portion. Or the effective diameter circumference = also as the center portion is concave, and the negative refractive power at the peripheral portion of the effective diameter is weaker than the central portion. The central portion of the lens surface is concave, and the negative refractive power of the effective diameter peripheral portion is stronger than that of the portion. This means that the effective diameter peripheral portion is also concave as the center portion, and the absolute value of the radius of curvature of the effective diameter peripheral portion is The case where the absolute value of the half value of the curvature of the center portion is smaller than this. The radius of curvature of the middle portion is the radius of curvature of the lens surface at the position where the lens surface intersects the optical axis. Further, the reason why the curvature radius value is expressed in absolute value is to clarify the magnitude relationship of the radius of curvature. According to the present invention, the first photographic lens and the photographic device using the photographic lens include, in order from the object side, a first-head mirror having a negative refractive power, a second lens having a negative refractive power, and having The third lens of the positive power, the light and the fourth lens having the positive power, the second lens, the third lens, and the M356934 fourth lens are lenses in which at least one lens surface of each lens is aspherical, and the condition is satisfied. Formula (1): 2.4 < (D4 + D5) / f < 5.5, so that the optical performance can be improved while widening and miniaturization can be achieved. By arranging the negative first lens and second lens on the most object side, The lens 5 can capture a light incident from a large viewing angle, and can be wide-angled. By using at least one side surface of the second lens as an aspherical surface, the aberration can be well corrected, and the lens system can be miniaturized. In the second lens, the on-axis ray and the off-axis ray are separated. Therefore, if the lens is aspherical, it is advantageous in terms of positive aberrations, and correction of the sag is relatively easy. In addition, the on-axis and off-axis rays of the first lens It is separated, but as a material of the first lens U disposed on the most object side of the lens system, a glass material as described later is preferably used. Further, the first lens becomes the largest aperture lens in the lens system. It is preferable to use a second lens which is easy to apply a plastic material as an aspherical lens, and it is preferable to perform lens correction and image aberration correction. Further, the third lens and the fourth lens are all set to at least a side surface. The lens having a positive refractive power of the aspherical surface can accurately correct the field curvature and the coma aberration while minimizing the lens system by arranging the diaphragm between the third lens and the fourth lens. According to the second photographic lens of the present invention and the photographic apparatus using the photographic lens, the first lens having a negative refractive power and a meniscus lens having a concave surface toward the image side is included in order from the object side; The mirror surface is aspherical, the central portion of the lens surface is convex, and the positive power of the effective diameter peripheral portion is weaker than the middle portion, or the central portion of the lens surface is convex, and is effective at the M356934 diameter circumference. a second lens having a negative refractive power; a third lens having a positive refractive power, an aspherical surface of the object side lens surface; a light barrier; and a fourth lens having a positive optical coke and an aspherical surface of the image side lens surface, It is possible to increase the optical performance while wide-angle and miniaturization. 5. By arranging the negative first lens and the second lens on the most object side, it is possible to capture light incident from a large angle of view and wide-angle. . towel and 'the first lens is set to have a negative power on the object side and the concave surface φ 帛 to the image side of the 'moon-shaped lens, and can be set to small and small, can be in the wide view, the full range of angles The range corrects the image plane curvature. Further, by arranging at least one side surface of the second lens as an aspherical surface, γ can well correct the aberrations, and the lens system can be miniaturized. In the first lens, the on-axis ray and the axis The external light is separated. Therefore, if the transparency is set to be aspherical, it is advantageous in correcting the aberration, and it is easier to correct. 15 In addition, the on-axis ray and the off-axis ray of the first lens are also separated, but #为为最最的眼系的系统The material of the first lens on the object side is made of a glass material as described later. Moreover, the 'first lens' becomes the largest aperture lens in the lens system. In these cases, it is preferable to use the second lens which is easy to apply the plastic material as the aspherical lens, and to make the lens and the aberration correction 20. By making the side surface of the second lens aspherical, it is easy to reduce the size and wide angle of the lens system. Further, by forming the object side surface of the second lens as a convex portion at the center of the lens surface, the positive refractive power of the effective diameter peripheral portion is weaker than the central portion or the central portion of the lens surface is convex, at the effective diameter periphery M356934 = (4) The surface of the power is easy to make the lens system compact, wide-angled, and the same, and the field curvature can be corrected well. Further, the third lens and the fourth lens are all disposed at least with a side surface that is aspherical, with a positive well order, and a Thai lens that transmits a light intercept to the third lens. The lens system can be miniaturized while accurately correcting the curvature of field and the shoe-shaped aberration between the four lenses. By making the surface on the side of the third lens object aspherical, the positive image plane can be bent. By making the surface on the fourth lens image side aspherical, it is possible to satisfactorily correct field curvature and coma aberration. [Embodiment] Hereinafter, an embodiment of an image pickup lens of the present magazine and an image pickup apparatus using the same will be described in detail with reference to the drawings. Fig. 15 is a cross-sectional view showing a schematic configuration of an image pickup apparatus using the image pickup lens of the present invention. Fig. 2 is a view in which an auxiliary line or the like for explanation is added to the figure. The illustrated photographing lens 20 is a wide-angle lens used for an in-vehicle or anti-theft photographing apparatus for photographing a surrounding situation outdoors. The image of the subject is imaged on the light-receiving surface Jk of the photographing element 1A made of CCD4CM〇s, etc. The photographing element 10 converts the optical image formed by the photographing lens 2 into an electrical signal to obtain a representation. First, the basic structure of the photographic lens 20. The photographic lens 20 includes, in order from the object side along the optical axis Z1, a first lens u, a second 10 M356934 lens L2, and a third The lens (1) aperture stop & and the fourth lens component Cg 1. Further, in the case where the lenses of the first lens L1 to the fourth lens L4 are single lenses, the lenses are not limited thereto. In the case of the single lens, it is also possible to use a light-receiving surface Jk of the image sensor 1A on the image forming surface R12 on which the object image indicating the object is imaged by the image pickup lens 20.
而且,在攝影裝置上適用攝影透鏡時,按照裝載透鏡 的相機側結構,較佳地配置玻璃罩、低通遽波器或紅外線 10 截止濾光片等,在圖丨中表示有將對這些進行假設後的平行 平板狀光學部件Cgl配置在透鏡系統和攝影元件1〇之間的 示例。 另外,代替在透鏡系統和攝影元件之間配置低通濾波 器或截止特定的波長域的各種濾光片等,在第一透鏡] I5第四透鏡L4之中的相鄰的透鏡之間配置這些各種濾光片 也可。或者’在第一透鏡L1〜第四透鏡[4中的任意透鏡面 施加與各種濾光片起同樣的作用的塗層也可。 另外’圖1中的符號R1〜R12指以下的結構元件。即, R1和R2表不第—透鏡L1的物體側透鏡面和像側透鏡面,R3 20和R4表示第二透鏡L2的物體側透鏡面和像側透鏡面,R5 和R6表示第三透鏡L3的物體側透鏡面和像側透鏡面,R7 表示孔徑光攔St的位置,r8*R9表示第四透鏡L4的物體側 透鏡面和像側透鏡面,R10和R11表示光學部件Cgl的物體 側表面和像側表面,R12是表示攝影透鏡20的成像面Jk。 11 M356934 父的中心部至有效徑周緣部的範圍光滑地㈣的曲面形成 ㈣鏡面’且是不具有段差等不連續的領域的透鏡面。 就攝影透鏡20而言,第一读错Tia*ir& 弟透鏡L1具有負光焦度,第二透鏡 L2具有負光焦度’第三透鏡L3具有正域度,第四透鏡Μ 具有正光焦度。 進一步,此攝影透鏡2G中,第二透鏡L2'第三透鏡L3、 及第:透鏡L4的各透鏡的至少丨個透鏡面呈非球面。而 且’第二透鏡和第三透鏡之間的空氣間隔〇4、第三透鏡的 10中心厚度D5、攝影透鏡整個系統的焦距f滿足條件式⑴: 2.4<(D4+D5)/f<5.5。 這樣,按㈤滿足條件式⑴等的方式構成的攝影透鏡 2〇’可良好地校正球面像差、歪曲像差、舞像差,且可 將後截距取得較長。進一步,可將視角設大,所以可得到 15 充分的光學性能。 另外,後截距是從第四透鏡£4的像側透鏡面R9到成像 面R12的距離(空氣換算長)。 若(D4+D5)/f值超過條件式(1)的上限,則配置在物體 側的第一透鏡L1的徑變大,並且攝影透鏡的全長也變長, 20 所以難以小型化。 另一面’若(D4+D5)/f值超過條件式(1)的下限,則不 可良好地校正球面像差、彗形像差,且難以形成為明亮(F 值小)的透鏡系統。 而且’攝影透鏡2〇構成如下。 12 M356934 即’攝影透鏡20沿著光轴Z1從物體側起依次包括:第 一透鏡L1、第二透鏡L2、第三透鏡L3、孔徑光欄St、第 四透鏡L4,並且,第一透鏡L1具有負光焦度,且是凹面朝 向像側(圖中箭頭+Z方向側)的彎月形透鏡。 5 就第二透鏡L2而言,其物體側(圖中箭頭一z方向側) 透鏡面R3呈非球面’且此透鏡面R3的中心部呈凸面,有效 仅周、’彖。p的正光焦度比中心部弱,或者此透鏡面的中心 部呈凸面’在有效徑周緣部具有負光焦度。第三透鏡面L3 具有正光焦度,且物體側透鏡面R5呈非球面。第四頭鏡面 10 L4具有正光焦度,且像側透鏡面R9呈非球面。 另外’透鏡面的中心部是透鏡面和光軸相交的透鏡面 上的部位。 以下’對「透鏡面尺3的中心部呈凸面,有效徑周緣部 的正光焦度比中心部弱」的意思進行說明,詳細而言,對 15後述的透鏡面R5進行同樣的說明時,參照圖2進行解說。 另外,對透鏡面R5以外的透鏡面,省略在說明中使用的符 號圖示。 上述「透鏡面R3的中心部呈凸面,有效徑周緣部的正 光焦度比中心部弱的結構(以後,稱為透鏡面R3)」為如下 20 的結構。 即,將中心部呈凸面(具有正光焦度)的透鏡面们在其 有效徑周緣部上的點X3的法線H3與光軸Z1相交的點設為 交點P3,將連結點χ3和交點p3的線段χ3_ρ3的長度設為點 X3的透鏡面R3的曲率半徑絕對值。而且,將透鏡面R3和光 13 M356934 軸Z1的交點設為中心部C3。在如此規定的情況下,透鏡面 R3的實施例為:透鏡面R3在光軸Z1上(中心部C3)呈凸面, 且具有正光焦度,透鏡面R3的中心部C3的曲率中心E3及交 點P3兩方皆比中心部C3更靠像側,並且,線段χ3_ρ3的長 5 度(在透鏡面R3的點X3的曲率半徑R3X的絕對值)比在透鏡 面R3的中心部C3的曲率半徑R3c的絕對值更大。 而且’透鏡面R3的中心部呈凸面且在有效徑周緣部具 有負光焦度,意味著透鏡面R3上的中心部C3的曲率中心E3 比中心部C3更靠像側,交點p3比中心部。更靠物體側。 10 透過將第二透鏡物體側面R3設為非球面,且此透鏡面 的中心部呈凸面,有效徑周緣部的正光焦度比中心部弱, 或者此透鏡面R3的中心部呈凸面,在有效徑周緣部具有負 的光焦度’從而容易將透鏡系統小型化、廣角化的同時, 可良好地校正像面彎曲。 15 20 本創作的攝影透鏡滿足上述2種基本結構的任意上個也 可,滿足上述2種基本結構的雙方也可。 根據上述攝影透鏡具備的基本結構,可將攝影 角化及小型化的同時’可將此攝影透鏡的光學性能提^ 接著,關於對此攝影透鏡2〇具備的上述基本 進一步限定的結構元件及其仙、效果 =仃 Γ基本結構進行進―步限定的這些結構元件在本創^摄 衫透鏡中不是必需的結構。 '攝 以下於對攝影透鏡的基本結構進行進—步限定的 以下條件式⑺〜⑽及其作用、效果進行說明。另外限= 14 M356934 δ月創作的攝影透鏡僅滿足條件式(2)〜(丨2)中的1個也可,或 者滿足條件式(2)〜(12)中的2個以上的組合也可。 而且’對在(2)〜(12)中由記號表示的各參數的意思歸納 表示如下: 5 f:攝影透鏡整個系統的焦距,即,第一透鏡L1〜第四 透鏡L4的合成焦距; f2 :第二透鏡的焦距; ^ f 3 :第三透鏡的焦距; 、 f12 :第一透鏡、第二透鏡的合成焦距; 10 f34.第二透鏡、第四透鏡的合成焦距; D1 :第一透鏡的中心厚度; D3 :第二透鏡的中心厚度; D4 :第二透鏡和第三透鏡的空氣間隔; D5 :第三透鏡的中心厚度; 15 D7 .孔徑光攔和第四透鏡的空氣間隔; R4c ·第二透鏡的像側透鏡面中心部的曲率半徑; _ ^d3:第三透鏡的對d線的阿貝數; L:從第一透鏡的物體側透鏡面到成像面的距離。 此處,上述距離L值是後截距量由空氣換算長表示的 20值與上述距離L值中的除後截距量以外由實長表示的值相 加後的值。 另外,後截距Bf為從第四透鏡L4的像側透鏡面R9到成 像面R12的距離(空氣換算長)。 N1 :第一透鏡的對d線的折射率; 15 M356934 ED :第一透鏡l 1的像側透鏡面R2的有效光線徑,即, 在通過第一透鏡L1的像側透鏡面R2的光線之中通過最外 側的光線VI與該透鏡面R2的交點所描繪的圓的直徑(參照 圖2)。 另外,「透鏡面的有效光線徑」是意味著在通過透鏡 面的有效光線之中通過最外側(距光軸最遠的位置)的光線 與該透鏡面的交點所描繪的圓的直徑。而且,通過上述透 鏡面的有效光線是被攝體的像的成像所使用的光線。 此處,透鏡面的有效光線徑和透鏡面的有效徑一致。 而且,上述的「透鏡面的有效徑周緣部」是由在通過 透鏡面的有效光線之中與通過最外側的光線相《的透鏡面 上的各點而成的部位,意味著有效徑的圓周上。 ◊ 條件式(2) : ^ d3<45是有關倍率色像差的校正等 的式子。 若滿足條件式(2),則容易良好地校正倍率色像差。 、然而,若脫離條件式(2)的範圍,則難以校正倍率色像 斜了進一步良好地校正倍率色像差,只要第三透鏡的 .線的阿貝數u d3滿足以下條件式(2_2)即可: 20 P 们<32 ......(2-2)。 只要第三透鏡 可: 另外,為了將倍率色像差抑制為最小, 的對d線的阿貝數^ 3滿足以下條件式(2-3)即 v d3<28 ......(2-3)。 16 M356934 較佳地將形成第一透鏡、第二透鏡 學材料的對d線的阿貝數設為伽上,由此,就可抑制色像 i的發生,亚得到良好的解像性能。 5 在後述的實施例3、5、6中’作為_三透鏡⑽ 先子材料使用帝人化成株式會社制聚碳酸醋樹脂, panhte(登陸商標)sp,i 5丨6(同社制產品名,另外㈣叫登 陸商標)為同社登陸商標)。此材料的中,對d線的折射率為 1.60以上’對4線的阿貝數小至25 5,而且,光學歪曲小。 透過在第三透鏡L3使用此材料,可良好地校正倍率色 象差的同化,在成型樹脂材料時產生的歪曲發生也被抑制 為f小。透過將本創作的攝影透鏡作為例如超過ι〇〇萬像素 的间像素攝影元件用攝影透|而使帛,可肖到表示物體的 良好的圖像。 ◊條件式(3) : 1.0<f3/f<3.0是有關像差的校正或組裝性 15 等的式子。 若滿足條件式(3)而構成透鏡系統,就可容易進行倍率 色像差的校正、及透鏡組裝。 以而’若f3/f值超過條件式(3)的上限而構成透鏡系 統’則第三透鏡的光焦度變弱,難以校正倍率色像差。 另外’若f3/f值超過條件式(3)的下限而構成透鏡系 1 ’則第三透鏡的光焦度變得過強,對於偏心的敏感度變 南’難以組裝透鏡。 ◊條件式(4) : 0.01<|fl2/f34|<0.5是有關像差的校正等 的式子。 17 M356934 若滿足條件式(4)而構成透鏡李 彎曲或_像差的校正。則可^進行像面 列難以卢角::|fl2/f34i的值設為超過條件式(4)的上限, 若i=化的同時,像面彎曲變大,難以得到良好的像。 成产角化 設為超過條件式(4)的下限,則可容易達 彗形像差增大,在周邊難以得到良好的像。 子。件式(5):7<L/f<16是有關小型化和廣角化等的式 10廣角Γ足條件式(5)而構成透鏡系統,則可達成小型化和 、然而,若將L/f值設為超過條件式(5)的上限,則 達成廣角化,但攝影透鏡的尺寸大型化。 而且,右將L/f值設為超過條件式(5)的下限,則可將 攝影透鏡的尺寸小型化,但難以達成廣角化。 15 ◊條件式⑹:口㈣1々.列是有關像差的校正等的式 子。另外,N1如上述是第一透鏡的對4線的折射率。" 右滿足條件式(6)而構成透鏡系統,則可容易進行 畸變的校正。 I及 然而,若將N1值設為超過條件式(6)的上限,則透鏡 2〇統的阿貝數變小,色像差變大。而且,透鏡部件的成2也 變南’成為攝影透鏡的成本上升的原因。 若將N1值設為超過條件式(6)的下限,則為了達成产 化,必須將物體側面的曲率設大,難以良好地校正畸二。 18 M356934 ◊條件式⑺:wwuo是有關加工 校正等的式子。 丨王和像差 若滿足條件式⑺而構成透鏡系統,則可使良好的加工 性和良好的畸變的校正並存。 5 然而,若將ED/R4c值設為超過條件式⑺的上限 一透鏡的像側透鏡面R4近於半球而難以加工, 攝影透鏡的製造成本。 大 容易力另二’若:r_c值設為超過條件式⑺的下 易加工苐二透鏡,但不能良好地校正畸變。 1等的2件式⑻:心〈陳是有關像差校正和廣角化 ^滿^條件式⑻而構成透鏡系統’則可使廣肖化和良 好的球面像差的校正並存。 15 20 ,若將崎設為超過條件式⑻的上限,則難以 艮好地校正球面像差。 另外,箱f2/m設為超過條件式 透鏡的負光焦度變弱,難以廣角化。 則弟一 ◊條件式(9). 〇.5〇<D3/f<I.5* 有關攝Further, when an imaging lens is applied to the imaging device, a glass cover, a low-pass chopper, an infrared ray 10 cut filter, or the like is preferably disposed in accordance with the camera-side structure of the loading lens, and it is shown in the figure that these will be performed. The example in which the rear parallel flat optical member Cgl is disposed between the lens system and the photographing element 1A is assumed. Further, instead of arranging a low-pass filter between the lens system and the imaging element, or cutting off various filters of a specific wavelength range, etc., these are disposed between adjacent lenses among the first lens I5 and the fourth lens L4. Various filters are also available. Alternatively, a coating layer having the same function as that of the various filters may be applied to any of the first lens L1 to the fourth lens [4]. Further, the symbols R1 to R12 in Fig. 1 refer to the following structural elements. That is, R1 and R2 represent the object side lens surface and the image side lens surface of the first lens L1, R3 20 and R4 represent the object side lens surface and the image side lens surface of the second lens L2, and R5 and R6 represent the third lens L3. The object side lens surface and the image side lens surface, R7 represents the position of the aperture stop Bar St, r8*R9 represents the object side lens surface and the image side lens surface of the fourth lens L4, and R10 and R11 represent the object side surface of the optical component Cgl. And the image side surface, R12 is an image plane Jk indicating the photographic lens 20. 11 M356934 The range from the center of the parent to the periphery of the effective diameter is smooth (4). The curved surface is formed by (4) mirror surface and is a lens surface that does not have a discontinuous field such as a step. In the case of the photographic lens 20, the first read error Tia*ir& L lens has a negative power, the second lens L2 has a negative power. The third lens L3 has a positive power, and the fourth lens Μ has a positive focus. degree. Further, in the photographic lens 2G, at least one lens surface of each of the second lens L2' of the third lens L3 and the first lens L4 is aspherical. Further, 'the air gap 〇4 between the second lens and the third lens, the center thickness D5 of the third lens, and the focal length f of the entire system of the photographic lens satisfy the conditional expression (1): 2.4 < (D4 + D5) / f < 5.5 . As described above, the photographic lens 2 〇 ' configured to satisfy the conditional expression (1) or the like can satisfactorily correct spherical aberration, distortion, and aberration, and can obtain a longer rear intercept. Further, the viewing angle can be set large, so that sufficient optical performance can be obtained. Further, the back intercept is the distance from the image side lens surface R9 of the fourth lens £4 to the image plane R12 (air conversion length). When the value of (D4 + D5) / f exceeds the upper limit of the conditional expression (1), the diameter of the first lens L1 disposed on the object side becomes large, and the total length of the imaging lens also becomes long, so that it is difficult to downsize. On the other hand, if the value of (D4 + D5) / f exceeds the lower limit of the conditional expression (1), spherical aberration and coma aberration are not satisfactorily corrected, and it is difficult to form a lens system which is bright (f value is small). Further, the 'photographic lens 2' is constructed as follows. 12 M356934 That is, the photographic lens 20 includes, in order from the object side along the optical axis Z1, a first lens L1, a second lens L2, a third lens L3, an aperture stop St, a fourth lens L4, and the first lens L1. It has a negative power and is a meniscus lens whose concave surface faces the image side (the arrow + Z direction side in the figure). 5 The second lens L2 has an aspherical surface on the object side (the arrow-z direction side in the drawing), and the central portion of the lens surface R3 has a convex surface, which is effective only for the circumference. The positive power of p is weaker than the central portion, or the central portion of the lens surface has a convex surface 'having a negative refractive power at the peripheral portion of the effective diameter. The third lens surface L3 has positive refractive power, and the object side lens surface R5 has an aspherical surface. The fourth mirror 10 L4 has a positive power and the image side lens surface R9 is aspherical. Further, the central portion of the lens surface is a portion on the lens surface where the lens surface and the optical axis intersect. In the following description, the description will be given of the case where the center of the lens face 3 is convex, and the positive refractive power of the peripheral portion of the effective diameter is weaker than the central portion. Specifically, when the lens surface R5 described later is described in the same manner, reference is made to Figure 2 illustrates. In addition, the symbol planes used in the description of the lens surface other than the lens surface R5 are omitted. The above-mentioned "the center of the lens surface R3 is convex, and the positive refractive power of the peripheral portion of the effective diameter is weaker than the central portion (hereinafter referred to as the lens surface R3)" is as follows. In other words, a point at which the normal surface of the lens surface having the convex portion (having a positive refractive power) at the center of the effective diameter is intersected with the optical axis Z1 at the point where the normal line H3 intersects the optical axis Z1, and the point χ3 and the intersection point p3 are connected. The length of the line segment _3_ρ3 is set to the absolute value of the radius of curvature of the lens surface R3 of the point X3. Further, the intersection of the lens surface R3 and the light 13 M356934 axis Z1 is defined as the center portion C3. In such a case, the lens surface R3 is an embodiment in which the lens surface R3 is convex on the optical axis Z1 (center portion C3) and has positive refractive power, and the center of curvature E3 and the intersection of the central portion C3 of the lens surface R3 Both sides of P3 are closer to the image side than the center portion C3, and the length of the line segment _3_ρ3 is 5 degrees (the absolute value of the radius of curvature R3X at the point X3 of the lens surface R3) is larger than the radius of curvature R3c at the center portion C3 of the lens surface R3. The absolute value is greater. Further, the central portion of the lens surface R3 has a convex surface and has a negative refractive power at the peripheral portion of the effective diameter, which means that the center of curvature E3 of the central portion C3 on the lens surface R3 is closer to the image side than the central portion C3, and the intersection point p3 is larger than the center portion. . More on the side of the object. 10, by making the second lens object side surface R3 aspherical, and the central portion of the lens surface is convex, the positive power of the effective diameter peripheral portion is weaker than the central portion, or the central portion of the lens surface R3 is convex, effective The peripheral edge portion of the diameter has a negative refractive power ′, and the lens system can be easily miniaturized and widened, and the field curvature can be satisfactorily corrected. 15 20 The photographic lens of this creation satisfies any of the above two basic structures, and both of the above two basic structures may be satisfied. According to the basic configuration of the photographic lens, the optical performance of the photographic lens can be improved while the photographic angle and the size of the photographic lens are improved, and the substantially further defined structural elements provided for the photographic lens 2 及其These structural elements, which are defined by the basic structure for further steps, are not essential structures in the present invention. The following conditional expressions (7) to (10) which define the basic structure of the photographic lens, and their actions and effects will be described below. In addition, the photographic lens created by the δ month may satisfy only one of the conditional expressions (2) to (丨2), or may satisfy two or more combinations of the conditional expressions (2) to (12). . Further, 'the meanings of the parameters indicated by the symbols in (2) to (12) are summarized as follows: 5 f: the focal length of the entire system of the photographing lens, that is, the combined focal length of the first lens L1 to the fourth lens L4; f2 : focal length of the second lens; ^ f 3 : focal length of the third lens; f12: composite focal length of the first lens and the second lens; 10 f34. composite focal length of the second lens and the fourth lens; D1: first lens Center thickness; D3: center thickness of the second lens; D4: air gap of the second lens and the third lens; D5: center thickness of the third lens; 15 D7. air gap of the aperture stop and the fourth lens; R4c The radius of curvature of the central portion of the image side lens surface of the second lens; _ ^d3: the Abbe number of the d-line of the third lens; L: the distance from the object-side lens surface of the first lens to the imaging surface. Here, the distance L value is a value obtained by adding a value indicated by a real length other than the post-intercept amount of the back-intercept amount by the air-converted length. Further, the back intercept Bf is a distance (length in air conversion) from the image side lens surface R9 of the fourth lens L4 to the image plane R12. N1 : refractive index of the first lens to the d line; 15 M356934 ED : effective light path of the image side lens surface R2 of the first lens l 1 , that is, light passing through the image side lens surface R2 of the first lens L1 The diameter of a circle drawn by the intersection of the outermost light ray VI and the lens surface R2 (see FIG. 2). Further, the "effective ray path of the lens surface" means the diameter of a circle drawn by the intersection of the light rays passing through the outermost side (the position farthest from the optical axis) and the lens surface among the effective rays passing through the lens surface. Moreover, the effective light passing through the above-mentioned lens surface is the light used for imaging the image of the subject. Here, the effective ray diameter of the lens surface coincides with the effective diameter of the lens surface. Further, the above-mentioned "effective diameter peripheral portion of the lens surface" is a portion which is formed by each point on the lens surface which passes through the outermost light among the effective rays passing through the lens surface, and means the circumference of the effective diameter. on. ◊ Conditional expression (2): ^ d3 < 45 is an expression relating to correction of magnification chromatic aberration and the like. When the conditional expression (2) is satisfied, the chromatic aberration of magnification is easily corrected satisfactorily. However, if it is out of the range of the conditional expression (2), it is difficult to correct the magnification color image and the magnification chromatic aberration is further corrected. As long as the Abbe number u d3 of the line of the third lens satisfies the following conditional expression (2_2) Then: 20 P <32 ......(2-2). As long as the third lens can be: In addition, in order to suppress the chromatic aberration of magnification to the minimum, the Abbe number of the d line ^ 3 satisfies the following conditional expression (2-3), that is, v d3 < 28 (2) -3). 16 M356934 Preferably, the Abbe number of the d-line forming the first lens and the second lens material is set to gamma, whereby the occurrence of the color image i can be suppressed, and good resolution performance is obtained. 5 In the third, fifth, and sixth examples to be described later, 'the _ three-lens (10) precursor material is a polycarbonate resin manufactured by Teijin Chemical Co., Ltd., panhte (registered trademark) sp, i 5丨6 (product name of the company, and (4) Calling the landing mark) is the landing mark of the company. In this material, the refractive index for the d-line is 1.60 or more', and the Abbe number for the 4-line is as small as 25 5, and the optical distortion is small. By using this material in the third lens L3, the assimilation of the chromatic aberration of magnification can be satisfactorily corrected, and the occurrence of distortion in the molding of the resin material is also suppressed to be small f. By using the photographic lens of the present invention as a photographic image of an inter-pixel photographic element of more than 10,000 megapixels, it is possible to display a good image of an object. ◊Conditional expression (3): 1.0<f3/f<3.0 is an expression regarding aberration correction or assemblability 15 or the like. When the lens system is formed by satisfying the conditional expression (3), the correction of the chromatic aberration of magnification and the lens assembly can be easily performed. When the lens system is formed by the f3/f value exceeding the upper limit of the conditional expression (3), the power of the third lens is weak, and it is difficult to correct the chromatic aberration of magnification. Further, when the f3/f value exceeds the lower limit of the conditional expression (3) to form the lens system 1', the power of the third lens becomes too strong, and the sensitivity to eccentricity becomes difficult to assemble the lens. ◊Conditional expression (4): 0.01<|fl2/f34|<0.5 is an expression regarding aberration correction or the like. 17 M356934 Correction of lens Lee bending or _ aberration if the conditional expression (4) is satisfied. Then, the value of the image surface difficulty angle::|fl2/f34i is set to exceed the upper limit of the conditional expression (4), and if the i=ization, the image plane curvature becomes large, and it is difficult to obtain a good image. When the keratinization is set to exceed the lower limit of the conditional expression (4), the coma aberration can be easily increased, and it is difficult to obtain a good image at the periphery. child. (5): 7<L/f<16 is a wide-angled conditional expression (5) of the formula 10 for miniaturization and wide-angle, etc., and the lens system is configured to achieve miniaturization. However, if L/ is When the f value is set to exceed the upper limit of the conditional expression (5), the wide angle is achieved, but the size of the photographic lens is increased. Further, when the L/f value is set to the lower limit of the conditional expression (5), the size of the photographic lens can be reduced, but it is difficult to achieve wide angle. 15 ◊Conditional expression (6): Port (4) 1々. The column is a formula for correction of aberrations. Further, N1 is a refractive index of the first lens which is four lines as described above. " When the lens system is formed by satisfying the conditional expression (6) to the right, the distortion correction can be easily performed. I and However, when the value of N1 is set to exceed the upper limit of the conditional expression (6), the Abbe number of the lens 2 system becomes small, and the chromatic aberration becomes large. Further, the formation 2 of the lens member also becomes a cause of an increase in the cost of the photographic lens. When the value of N1 is set to exceed the lower limit of the conditional expression (6), in order to achieve production, the curvature of the side surface of the object must be made large, and it is difficult to correct the distortion. 18 M356934 ◊Conditional formula (7): wwuo is a formula for machining correction, etc.丨王 and aberrations If the lens system is formed by satisfying conditional expression (7), good workability and good distortion correction can be coexisted. 5 However, if the ED/R4c value is set to exceed the upper limit of the conditional expression (7), the image side lens surface R4 of the lens is close to the hemisphere and is difficult to process, and the manufacturing cost of the photographic lens is high. It is easy to force the other two. If the r_c value is set to be lower than the conditional (7), the second lens is easily processed, but the distortion cannot be corrected well. The two-piece (8) of 1st class: the heart is about the aberration correction and the wide-angled conditional condition (8) constitutes the lens system', and the correction of the spherical aberration and the good spherical aberration can be coexisted. 15 20 . If the saki is set to exceed the upper limit of the conditional expression (8), it is difficult to correct the spherical aberration. Further, the case f2/m is set to be lower than the negative power of the conditional lens, and it is difficult to widen the angle. The younger brother has a conditional formula (9). 〇.5〇<D3/f<I.5*
加工性等的式子。 处現扪尺丁A =滿足條件式⑼而構成透鏡系統,則可抑制像差降 炒而、Ϊ使第二透鏡L2的良好的加工性和小型化並存。 右將聰值設為超過條件式⑼的上限,則透鏡系統 ’不能達到小型化的目的。而且,若要防止透鏡系 19 M356934 統的大型化,則第二透鏡L2的像側透鐘面… 的自由心皮限制,且崎變的校正不充分。的非球面形狀 -透鏡L2:.右將^值設*超過條件物的下限,則第 —远鏡L2的中心厚度轡猓 ^ 製造成本增大。㈣小而難以加工’且攝影透鏡的 ◊條件式(1〇) . 〇.5〇<Dl/f是有關耐衝擊性等的式子。 右滿足條件式⑽而構成透鏡系、统,則可使在例如車載等 =途所使用的情況下的第—透鏡的耐衝擊性容易向上。 :將:1/f值設為超過條件式⑽的下限,則第—透鏡變 薄’谷易破碎。 ◊條件式(11) : 0.50<D4/f<2 〇是有關像差校正等的式 子。 若滿足條件式(11)而構成透鏡系統,則可容易進行色 像差的校正。 15 然而,若將D4/f值設為超過條件式(11)的上限,則透 鏡系統的尺寸增大或難以校正色像差。 另外將D4/f值设為超若條件式(11)的下限,則可良 好地校正色像差,但第二透鏡L2的像側透鏡面和第三透鏡 L3的物體側透鏡面過於接近,因此,第二透鏡[2的像側透 2〇鏡面R4及第三透鏡L3的物體側透鏡面R5的非球面形狀被 限制’所以’像差校正不充分。而且,難以組裝的同時, 也發生以在2個透鏡面間的反射為原因的鬼像。 ◊條件式(12): 0.05<D7/f<0.25是有關攝影透鏡的尺寸 或遠心性的式子。 20 M356934 若滿足條件式(12)而構成透鏡系統,則可更加容易使 透鏡系統的小型化和良好的遠心性並存。 然而’若將D7/f值設為超過條件式(丨2)的上限,則透 鏡系統大型化,或為了抑制透鏡系統的大型化而使孔徑光 5攔和第三透鏡的間隔變小。若孔徑光攔和第三透鏡的間隔 憂小,則通過第一透鏡、第二透鏡、第三透鏡的各透鏡的 轴上光線和料外光線就難以分離,在像差校正上為不力, 也難以校正畸變。 另面若將D7/f值设為超過條件式(12)的下限,則 10難以將光學對成像面入射的入射角抑制為小,難以形成所 謂遠心性良好的透鏡系統。 以下,關於對攝影透鏡進行限定的上述條件式以外的 結構元件、及其作用、效果進行說明。 15 20 ◊關於第一透鏡的有關結構元件的限定 ,在車载攝衫鏡頭或監視攝影鏡頭的嚴格環境下使用 的攝影透鏡’作為第-透鏡較佳地使用耐水性、耐酸性、 耐藥品性等良好的材質。 硝+作^於形成第—透鏡的材料,較佳地使用日本光學 規格的粉末法耐水性為從1級到4級的材料。 本作為用於形成第—透鏡的材料,較佳地使用日 料/業會規格的粉末法耐酸性為從m到4級的材 21 M356934 所。而且’作為形成第一透鏡的材料,較佳地使用堅固材 貝。例如’作為第一透鏡的形成材料較佳地使用玻璃材料, 使用透明的陶瓷材料也可。 透過將第一透鏡!^設為玻璃透鏡,而可製作耐候性古 5且難破碎的攝影透鏡。 呵 、另外,不限於將第一透鏡L1設為玻璃球面透鏡的情 況’用非球面結構此第-透鏡L1的一側透鏡面或兩側透鏡 φ 面也可。透過將第一透鏡L1設為非球面玻璃透鏡,而可形 -成对水性、耐酸性、耐藥品性等優異,並且可更加良好地 10校正諸像差的攝影透鏡。 比第一透鏡更靠物體側配置保護透鏡的玻螭罩,或者 在第一透鏡物體側的透鏡面配置使耐候性提高的硬膜: 璃質薄膜也可。 、 在比第一透鏡更靠物體側配置玻璃罩等,將第一透铲 15設為難以受到外部環境影響的結構的情況下,第—透鏡7 設為塑料非球面。將第一透鏡設為塑料非球面時,可 • 步良好地校正像面·彎曲、畸變。 ◊ 關於第二透鏡的有關結構元件的限定 較佳地第二透鏡L2的像側透鏡面R4也設為非球面。 20 此透鏡面R4較佳地其中心部呈凹面,且有效徑周緣部 的負光焦度比中心部弱。 上述「透鏡面R4的中心部呈凹面,有效徑周緣部的負 光焦度比中心部弱的結構」(以後’也稱為透鏡面尺4的實施 例)為如下結構。 22 M356934 即’將中心部呈凹面(具有負光焦度)的透鏡面R4在其 有效徑周緣部上的點X4的法線H4與光軸Z1相交的點設為 交點P4 ’將連結點X4和交點P4的線段X4-P4的長度設為透 鏡面R4的點X4的曲率半徑絕對值。而且,將透鏡面R4和光 5軸Z1的交點設為中心部C4。在如此規定的情況下,透鏡面 R4的實施例為:透鏡面R4在光軸Z1上(中心部C4)呈凹面 (具有負光焦度)’透鏡面R4的中心部C4的曲率中心E4及交 點P4兩方皆比中心部C4更靠像側,並且,線段X4-P4的長 度(在透鏡面R4的點X4的曲率半徑R4X的絕對值)比在透鏡 10 面R4的中心部C4的曲率半徑R4C的絕對值更大。 如上述’透過使透鏡面R4形成為中心部C4呈凹面(具 有負光焦度)、且在有效徑周緣部的負光焦度比中心部C4 弱’就可使周邊光線在不急劇彎曲的狀態下集光,因此, 可良好地校正畸變。 15 而且,將第二透鏡L2的物體側透鏡面R3設為在此透鏡 面R3的有效徑内至少具有i個拐點,且透鏡面R3的中心部 C3呈凸面,有效徑周緣部Χ3的正光焦度比中心部弱,或者 透鏡面R3的中心部C3呈凸面,有效徑周緣部乂3呈凹面也 "5J* 〇 20 透過將第二透鏡物體側面们設為非球面,在此透鏡面 R3的有效徑内至少具有丨個拐點,透鏡面们的中心部〇呈 凸面’有效徑周緣部Χ4的正光焦度比中心部弱;或者透鏡 面R3的中心部C43呈凸φ,有效徑周緣部幻呈凹面,由此, 23 M356934 可容易將透鏡系統小型化、廣角化的同時,良好地校 面彎曲。 另外,將在第二透鏡L2的物體側透鏡面们的有效徑周 緣部上的點X3的曲率半徑設為R3x,將此透鏡面幻與光抽 5 Z1的相交的中心部〇的曲率半徑設為…時,較佳地曲率 半位R3x的絕對值為曲率半徑R3c的絕對值的u倍以上的 值透過將曲率半徑R3X的絕對值設為曲率半徑的絕對 值的1.2七以上的值,而容易廣角化的同時,可良好地校正 像面彎曲。 1〇 而且將第一透鏡1"2的像側透鏡面R4的有效徑周緣部 上=點X4的曲率半徑設為R4x ’將此透鏡面R4與光軸以的 相父的中〜部C4的曲率半徑設為R4C時,較佳地曲率半徑 R4x的絕對值為曲率半徑R4c的絕對值的15倍以上的值。 透過將曲率半徑R4x的絕對值設為曲率半徑R4c的絕對值 15的I.5倍以上的值,而可良好地校正畸變。 ◊ 關於第二透鏡的有關結構元件的限定 較佳地第三透鏡L3的物體側透鏡面R5設為非球面。 此透鏡面R5較佳地中心部呈凸面,有效徑周緣部的正 光焦度比中心部弱。 20 如圖2所示,上述「透鏡面R5的中心部呈凸面,有效 位周緣σ卩的正光焦度比中心部弱的結構(以後,也稱為透鏡 面R5的實施例)」為如下結構。 即,將中心部呈凸面(具有正光焦度)的透鏡面尺5在其 有效控周緣部上的點Χ5的法線Η5與光軸Ζ1相交的點設為 24 M356934 交點P5 ’將連結點χ5和交點p5的線段χ5ρ5的長度設為透 鏡面R5的點X5的曲率半徑絕對值。而且,將透鏡面R5和光 軸Z1的父點設為中心部C5。在如此規定的情況下,透鏡面 R5的貫施例為:透鏡面R5在光軸z 1上(中心部匸5)呈凸面 5 (具有正光焦度),透鏡面R5的中心部C5的曲率中心E5及交 點P5兩方皆比中心部(^更靠像側,並且,線段χ5ρ5的長 度(在透鏡面R5的點Χ5的曲率半徑R5x的絕對值)比在透鏡 ^ 面R5的中心部C5的曲率半徑R5c的絕對值更大。 . 另外,在圖中表示以交點P5為中心,且將半徑長度設 10為線段X5-P5的長度的圓Spl。而且,在圖中表示以曲率中 心E5為中心’且將半徑長度設為曲率半徑R5c的絕對值的 圓 Sp2。 如上述,透過將透鏡面R5形成為其中心部C5呈凸面 (具有正光焦度)、且在有效徑周緣部的正光焦度比中心部 15 弱,而可良好地校正像面彎曲。 較佳地第三透鏡L3的像側透鏡面R6也設為非球面。 β 就此透鏡面R6而言’較佳地,此透鏡面R6的有效徑周 緣部的光焦度比此透鏡面R6的中心部的光焦度更弱。 上述「此透鏡面R6的有效徑周緣部的光焦度比透鏡面 20 R6的中心部的光焦度更弱的結構(以後,也稱為透鏡面R6 的實施例)」為如下結構。 即’將透鏡面R6的有效徑周緣部上的點X6的法線H6 與光軸Z1相交的點設為交點P6 ’將連結點X6和交點P6的線 段X6-P6的長度設為透鏡面R6的點X6的曲率半徑絕對值。 25 M356934 而且,將透鏡面R6和光軸Z丨的交點設為中心部c6。在如此 規定的情況下,透鏡面R6的實施例為:透鏡面R6的中心部 C6的曲率中心E6及交點P6兩方皆相對於中心部C6而位於 物體侧或像側,並且,線段χ6_ρ6的長度(在透鏡面R6的點 5 X6的曲率半徑R6x的絕對值)比在透鏡面R6的中心部C6的 曲率半徑R6c的絕對值更大。 如上述,透過將第三透鏡L3的像側透鏡面R6設為此透 鏡面R6的有效徑周緣部的光焦度比此透鏡面R6的中心部 的光焦度更弱’而可良好地校正球面像差和像面彎曲。 10 而且,將第三透鏡L3的物體側透鏡面R5的有效徑周緣 部上的點X5的曲率半徑設為R5x,將此透鏡面R5與光軸Z1 的相交的中心部C5的曲率半徑設為r5c時,較佳地曲率半 徑R5x的絕對值為曲率半徑R5c的絕對值的^倍以上的 值。透過將曲率半徑R5x的絕對值設為曲率半徑R5c的絕對 值的12倍以上的值,而可良好地校正像面彎曲。 ◊ 關於第四透鏡的有關結構元件的限定 較佳地第四透鏡L4的物體側透鏡面尺8設為非球面。 此透鏡面R8較佳地中心部呈凹面,有效徑周緣部的負 光焦度比中心部弱。 20 上述「透鏡面R8的中心部呈凹面’有效徑周緣部的負 光焦度比中心部弱的結構(以後,也稱為透鏡面尺8的實施 例)」為如下構成。 即’將中心部呈凹面(具有負光焦度)的透鏡面R8的有 效徑周緣部上的點X8的法線H8與光轴Z1相交的點f A六 26 M356934 點P8,將連結點X8和交點P8的線段X8-P8的長度設為透鏡 面R8的點X8的曲率半徑的絕對值。而且,將透鏡面r8和光 轴Z1的交點設為中心部C8。在如此規定的情況下,透鏡面 R8的實施例為:透鏡面Rg在光轴z 1上(中心部c8)呈凹面 5 (具有負光焦度),透鏡面R8的中心部C8點的曲率中心E8及 交點P8兩方皆比中心部C8更靠物體側,並且,線段X8_P8 的長度(在透鏡面R8的點X8的曲率半徑R8X的絕對值)比在 透鏡面R8的中心部C8的曲率半徑R8c的絕對值更小。 如上述’透過將透鏡面R8設為中心部c 8呈凹面(具有 10負光焦度)、且在有效徑周緣部的負光焦度比中心部C8強, 而可良好地校正彗形像差。 較佳地第四透鏡L4的像側透鏡面R9也設為非球面。 此透鏡面R9較佳地中心部呈凸面,且有效徑周緣部的 正光焦度比中心部弱。 15 上述「此透鏡面R9的中心部呈凸面,且有效徑周緣部 的正光焦度比中心部弱的結構(以後,也稱為透鏡面R9的實 施例)」為如下結構。 即’將中心部呈凸面(具有正光焦度)的透鏡面R9的有 效徑周緣部上的點X9的法線H9與光軸21相交的點設為交 2〇點P9,將連結點X9和交點P9的線段χ9_ρ9的長度設為透鏡 面R9的點X9的曲率半徑的絕對值。而且,將透鏡面R9和光 軸Z1的交點設為中心部C9。在如此規定的情況下,透鏡面 R9的實施例為:透鏡面R9在光軸Z1上(中心部C9)呈凸面 (具有正光焦度),透鏡面R9的中心部C9的曲率中心E9及交 27 M356934 點P9兩方皆比中心部C9更靠物體侧,並且,線段χ9_ρΜ々 長度(在透鏡面R9的點χ9的曲率半徑Rx9的絕對值)比在透 鏡面R9的中心部C9的曲率半徑Rc9的絕對值更大。 如上述’透過將透鏡面R9設為中心部C9呈凸面,且在 5有效徑周緣部的正光焦度比中心部C9弱,而可良好地校正 像面彎曲和彗形像差。 進一步,將在第四透鏡[4的像側透鏡面R9的有效徑周 % 緣部上的點X9的曲率半徑設為R9x,將在此透鏡面R9與光 . 軸21的相交的中心部C9的曲率半徑設為R9c時,較佳地曲 1〇率半徑R9x的絕對值為曲率半徑R9c的絕對值的丄2倍以上 的值。透過將曲率半徑R9x的絕對值設為曲率半徑R9c的絕 對值的1_2倍以上的值,而可良好地校正球面像差和像面彎 曲。 這樣,透過將從第二透鏡L2的物體側透鏡面尺3到第四 I5透鏡L4的像側透鏡面R9為止的各透鏡面設為如上述的非 球面形狀,除球面像差、像面彎曲、彗形像差外,也可良 _ 好地校正畸變。 ◊ 關於其他結構元件的限定 孔徑光攔St較佳地配置在第三透鏡匕3和第四透鏡M 20 之間。 透過將孔徑光攔St配置在第三透鏡。和第四透鏡Μ 之間’可將透鏡系統全體小型化。 28 M356934 在此攝影透鏡_,在比第一透鏡更靠物體側未配置玻 璃罩等時,較佳地將第一透鏡LI設為玻璃透鏡,將第二透 鏡L2、第三透鏡£3、第四透鏡以設為塑料透鏡。 透過將第二透鏡L2〜第四透鏡L4的材質設為塑料,可 5正確地再現非球面形狀。而且,可廉價製作透鏡系統。 作為形成從第二透鏡L2到第四透鏡L4的各塑料透鏡 的材料,使用相對於樹脂材料而將比光的波長尺寸小的粒 子混合的、所謂納米複合材料也可。 第透鏡L1〜第四透鏡L4的各透鏡不限於用折射率為 10 疋的材料开》成,在4片透鏡之中的任意1個以上使用折射 率分佈型透鏡也可。 彳疋第一透鏡L2到第四透鏡L4的各透鏡不限於將一面 或者兩面設為非球面的情況,形成為衍射光學面也可。即, 在從第一透鏡L2到第四透鏡L4為止的任意1個以上的透鏡 15 面形成衍射光學元件也可。 透過第一透鏡L1或第二透鏡L2的有效光線徑外的光 束成為雜散光而到達成像面,就存在成為鬼像的現象,但 較佳地在第一透鏡L1或第二透鏡L2上的有效光線徑外的 領域设置遮光手段的遮光板Sk 1、Sk2等(參照圖1、2)而遮 20 斷雜散光。 此遮光手段可採用在透鏡上的有效光線徑外的領域配 置遮斷光的板材,或者在透鏡上的有效光線徑外的領域塗 布由遮光塗料而成的被膜的結構。 29 M356934 而且,根據需要遮光手段配置在第一透鏡匕丨和第二透 鏡L2之間的空間也可。進一步,遮光手段配置在第二透鏡 L2〜第四透鏡];^上的有效光線徑外的領域,或者這些透鏡 之間也可。 5 、透過將從第二透鏡L2到第四透鏡L4設為如上述的非 求面^/狀,在將理想像高設為2fxtan( Θ /2)時,可將畸變形 成為± 10 %以内。 如以上,根據本創作所涉及的攝影透鏡,與以往的廣 角攝影透鏡相比可提高光學性能的_,可進行小型化。、 10 接著,參照圖3〜2卜對根據本創作的實施例1〜實施例 6的各攝影透鏡所涉及的數值數據料行歸納說明。圖3〜 圖8是分別表示實施例!〜實施例6的攝影透鏡的概略結構 的。j視圖。與圖1、2中的符號一致的圖3〜圖8中的符號表 示相互對應的結構。 15 20 圖9〜圖14疋分別表示實施例j〜實施例6的攝影透鏡的 4數據的圖°在各圖中的上左部(圖中用符號⑷表示)表 :透鏡數據,在上中央部(圖中用符號⑻表示)表示攝影透 =概略規格。而且,在下左部(圖巾用符號⑷表示)表示 有表示透鏡面形狀(非球面形狀)的非球面式的各係數。下 =(圖中用符號⑷表示)表示各透鏡面的有效形周緣部的 曲率半徑的絕對值。 在圖9〜圖14的各圖中的F '采 的上左。卩透鏡數據1f7,將透鏡等 件的面號碼以從物體側朝向像側依次增加的第;個 "、2、3、..···.)的面號碼而表示。另外,在這些透鏡數 30 M356934 據中也包括s己載有孔控光搁St的面號碼(i=7)、及平行平面 板的光學部件cgi的物體側面和像側面的面號瑪(i=1〇、 11)、成像面的面號碼(i=12)等。而且,對於透鏡面呈非球 面,在面號碼附有*號。 5 Ri表示第i個(i=l、2、3、……)面的近軸曲率半徑,Formula such as processability. When the lens system is formed by satisfying the conditional expression (9), the aberration reduction can be suppressed, and the good workability and miniaturization of the second lens L2 can be coexisted. When the right value is set to exceed the upper limit of the conditional expression (9), the lens system ' cannot be miniaturized. Further, in order to prevent an increase in size of the lens system 19 M356934, the image side of the second lens L2 is restricted by the free carpel of the clock surface, and the correction of the change is insufficient. Aspherical shape - Lens L2: The right value of * is set to exceed the lower limit of the condition, and the center thickness 第 of the first telescope L2 is increased. (4) It is small and difficult to process, and the ◊ conditional expression of the photographic lens (1〇). 〇.5〇<Dl/f is an expression relating to impact resistance and the like. When the lens system and the system are configured to satisfy the conditional expression (10), the impact resistance of the first lens in the case of use in, for example, a vehicle or the like can be easily made upward. : When the 1/f value is set to exceed the lower limit of the conditional expression (10), the first lens is thinned and the valley is easily broken. ◊Conditional expression (11): 0.50<D4/f<2 〇 is an expression relating to aberration correction or the like. If the lens system is formed by satisfying the conditional expression (11), the chromatic aberration can be easily corrected. However, if the D4/f value is set to exceed the upper limit of the conditional expression (11), the size of the lens system is increased or it is difficult to correct chromatic aberration. Further, when the D4/f value is set to the lower limit of the conditional expression (11), the chromatic aberration can be satisfactorily corrected, but the image side lens surface of the second lens L2 and the object side lens surface of the third lens L3 are too close. Therefore, the aspherical shape of the image side lens surface R4 of the second lens [2] and the object side lens surface R5 of the third lens L3 are restricted, so that the aberration correction is insufficient. Moreover, it is difficult to assemble, and a ghost image due to reflection between the two lens faces also occurs. ◊Conditional expression (12): 0.05 < D7/f < 0.25 is an expression relating to the size or telecentricity of the photographic lens. 20 M356934 If the lens system is formed by satisfying conditional expression (12), it is easier to cope with the miniaturization of the lens system and good telecentricity. However, when the D7/f value is set to exceed the upper limit of the conditional expression (丨2), the size of the lens system is increased, or the interval between the aperture light 5 and the third lens is made small in order to suppress an increase in the size of the lens system. If the interval between the aperture stop and the third lens is small, the on-axis ray and the off-beam light passing through the lenses of the first lens, the second lens, and the third lens are difficult to separate, and the aberration correction is not good, and It is difficult to correct the distortion. On the other hand, when the D7/f value is set to exceed the lower limit of the conditional expression (12), it is difficult to suppress the incidence angle of the incidence of the optical imaging plane to be small, and it is difficult to form a lens system having a good telecentricity. Hereinafter, structural elements other than the above-described conditional expressions that define the photographic lens, and their actions and effects will be described. 15 20 ◊ Regarding the definition of the relevant structural elements of the first lens, the photographic lens used in the strict environment of the car-mounted lens or the surveillance camera lens is preferably used as the first lens for water resistance, acid resistance, and chemical resistance. Good material. The material of the film is formed of a material of the first lens, preferably a material having a water resistance of from 1 to 4 grades using a powder method of the Japanese optical specification. As a material for forming the first lens, it is preferable to use a powder method of the Japanese/Industry specification to have an acid resistance of m to 4 grade 21 M356934. Further, as a material for forming the first lens, a strong material is preferably used. For example, as the material for forming the first lens, a glass material is preferably used, and a transparent ceramic material may be used. By using the first lens !^ as a glass lens, it is possible to produce a photographic lens that is weather-resistant and difficult to break. Further, the present invention is not limited to the case where the first lens L1 is a glass spherical lens. The one lens surface or the side lens φ surface of the first lens L1 may be aspherical. By using the first lens L1 as an aspherical glass lens, it is possible to form an photographic lens which is excellent in water resistance, acid resistance, chemical resistance, and the like, and can more accurately correct aberrations. A glass cover having a protective lens disposed on the object side of the first lens or a hard film having improved weather resistance on the lens surface of the first lens object side may be disposed of a glazed film. When the glass cover or the like is disposed on the object side of the first lens, and the first shovel 15 is configured to be hardly affected by the external environment, the first lens 7 is a plastic aspherical surface. When the first lens is made of a plastic aspherical surface, the image surface, bending, and distortion can be corrected in a good manner. ◊ Definition of the relevant structural element of the second lens Preferably, the image side lens surface R4 of the second lens L2 is also aspherical. Preferably, the lens surface R4 has a concave portion at a central portion thereof, and a negative refractive power at a peripheral portion of the effective diameter is weaker than a central portion. The above-mentioned "the central portion of the lens surface R4 has a concave surface, and the negative refractive power at the peripheral portion of the effective diameter is weaker than the central portion" (hereinafter, also referred to as an embodiment of the lens scale 4) is as follows. 22 M356934, that is, the point at which the normal line H4 of the point X4 of the lens surface R4 having the concave portion (having a negative refractive power) at the central portion of the effective diameter intersects the optical axis Z1 is defined as the intersection point P4'. The length of the line segment X4-P4 with the intersection point P4 is set to the absolute value of the radius of curvature of the point X4 of the lens surface R4. Further, the intersection of the lens surface R4 and the light 5 axis Z1 is defined as the center portion C4. In such a case, the lens surface R4 is an embodiment in which the lens surface R4 has a concave surface (having a negative refractive power) on the optical axis Z1 (the central portion C4), and a curvature center E4 of the central portion C4 of the lens surface R4 and Both sides of the intersection point P4 are closer to the image side than the center portion C4, and the length of the line segment X4-P4 (the absolute value of the radius of curvature R4X at the point X4 of the lens surface R4) is larger than the curvature of the center portion C4 of the lens surface R4. The absolute value of the radius R4C is larger. As described above, "the lens surface R4 is formed such that the central portion C4 has a concave surface (having a negative refractive power), and the negative refractive power at the peripheral portion of the effective diameter is weaker than the central portion C4", so that the peripheral light is not sharply curved. The light is collected in the state, so that the distortion can be corrected well. Further, the object side lens surface R3 of the second lens L2 has at least i inflection points in the effective diameter of the lens surface R3, and the central portion C3 of the lens surface R3 is convex, and the positive optical focus of the effective diameter peripheral portion Χ3 The degree is weaker than the center portion, or the center portion C3 of the lens surface R3 is convex, and the effective diameter peripheral portion 乂3 is concave. Also, "5J* 〇20 transmits the second lens object side surface to be aspherical, and the lens surface R3 The effective diameter has at least one inflection point, and the central portion of the lens surface is convex. The positive refractive power of the effective diameter peripheral portion Χ4 is weaker than the central portion; or the central portion C43 of the lens surface R3 is convex φ, and the effective diameter peripheral portion The illusion is concave, and thus, the 23 M356934 can easily reduce the lens system and widen the angle, and bend the surface well. Further, the radius of curvature of the point X3 on the effective diameter peripheral edge portion of the object-side lens surface of the second lens L2 is set to R3x, and the radius of curvature of the central portion 〇 where the lens surface is intersected with the light extraction 5Z1 is set. In the case of ..., the absolute value of the curvature half position R3x is preferably a value greater than or equal to u of the absolute value of the curvature radius R3c, and the absolute value of the curvature radius R3X is set to a value of 1.2 or more of the absolute value of the curvature radius. It is easy to widen the angle of view, and the curvature of field can be corrected well. 1〇 and the radius of curvature of the effective diameter peripheral portion of the image side lens surface R4 of the first lens 1" 2 = point X4 is R4x 'the middle of the phase of the lens surface R4 and the optical axis When the radius of curvature is R4C, the absolute value of the radius of curvature R4x is preferably 15 times or more the absolute value of the radius of curvature R4c. The distortion can be satisfactorily corrected by setting the absolute value of the radius of curvature R4x to a value of 1.5 times or more of the absolute value 15 of the radius of curvature R4c. ◊ Definition of the relevant structural element of the second lens Preferably, the object side lens surface R5 of the third lens L3 is aspherical. Preferably, the lens surface R5 has a convex portion at the center portion, and the positive refractive power of the peripheral portion of the effective diameter is weaker than the central portion. As shown in FIG. 2, the center portion of the lens surface R5 has a convex surface, and the positive refractive power of the effective edge circumference σ卩 is weaker than the central portion (hereinafter, also referred to as an embodiment of the lens surface R5). . That is, the point where the normal line 55 of the point surface 5 of the lens surface 5 having the convex portion (having a positive refractive power) at the central portion of the effective control periphery intersects the optical axis 设为1 is set to 24 M356934, and the intersection point P5' will be connected to the point χ5. The length of the line segment ρ5ρ5 of the intersection point p5 is set to the absolute value of the radius of curvature of the point X5 of the lens surface R5. Further, the parent point of the lens surface R5 and the optical axis Z1 is referred to as a central portion C5. In such a case, the lens surface R5 is a lens surface R5 having a convex surface 5 (having positive refractive power) on the optical axis z 1 (center portion 匸 5), and a curvature of the central portion C5 of the lens surface R5. Both the center E5 and the intersection point P5 are closer to the image side than the center portion (^, and the length of the line segment ρ5ρ5 (the absolute value of the radius of curvature R5x at the point Χ5 of the lens surface R5) is larger than the center portion C5 of the lens surface R5. The absolute value of the radius of curvature R5c is larger. In addition, a circle Spl centering on the intersection point P5 and having a radius length of 10 as the length of the line segment X5-P5 is shown in the figure. Moreover, the center of curvature E5 is shown in the figure. The circle Sp2 whose center length is the absolute value of the radius of curvature R5c. As described above, the lens surface R5 is formed such that the central portion C5 has a convex surface (having a positive refractive power) and a positive light at the peripheral portion of the effective diameter. The power is weaker than the center portion 15, and the field curvature can be corrected well. Preferably, the image side lens surface R6 of the third lens L3 is also aspherical. β For the lens surface R6, preferably, The power of the peripheral portion of the effective diameter of the mirror surface R6 is larger than the central portion of the lens surface R6. The above-mentioned "the refractive power of the peripheral portion of the effective surface of the lens surface R6 is weaker than the refractive power of the central portion of the lens surface 20 R6 (hereinafter, also referred to as an embodiment of the lens surface R6)" The configuration is such that the point at which the normal line H6 of the point X6 on the effective diameter peripheral edge portion of the lens surface R6 intersects the optical axis Z1 is defined as the intersection point P6', and the length of the line segment X6-P6 of the joint point X6 and the intersection point P6 is set. The absolute value of the radius of curvature of the point X6 of the lens surface R6 is 25 M356934. The intersection of the lens surface R6 and the optical axis Z丨 is defined as the center portion c6. In the case of the above, the lens surface R6 is an embodiment of the lens surface. Both the center of curvature E6 and the intersection point P6 of the center portion C6 of R6 are located on the object side or the image side with respect to the center portion C6, and the length of the line segment χ6_ρ6 (the absolute value of the radius of curvature R6x at the point 5 X6 of the lens surface R6) The absolute value of the radius of curvature R6c is larger than the central portion C6 of the lens surface R6. As described above, the image side lens surface R6 of the third lens L3 is set as the power of the effective diameter peripheral portion of the lens surface R6. Better than the power of the central portion of the lens surface R6' Spherical aberration and field curvature. 10 Further, the curvature radius of the point X5 on the effective diameter peripheral edge portion of the object side lens surface R5 of the third lens L3 is R5x, and the lens surface R5 intersects with the optical axis Z1. When the radius of curvature of the center portion C5 is r5c, the absolute value of the radius of curvature R5x is preferably a value equal to or greater than twice the absolute value of the radius of curvature R5c. The absolute value of the radius of curvature R5x is set to the absolute value of the radius of curvature R5c. The image-side curvature can be well corrected by a value of 12 times or more. ◊ Regarding the definition of the structural element of the fourth lens, the object-side lens scale 8 of the fourth lens L4 is preferably aspherical. Preferably, the lens surface R8 has a concave portion at the center portion, and the negative refractive power of the peripheral portion of the effective diameter is weaker than the central portion. In the above-mentioned "the central portion of the lens surface R8 is concave", the structure in which the negative refractive power of the effective diameter peripheral portion is weaker than the central portion (hereinafter, also referred to as an embodiment of the lens scale 8) is as follows. That is, the point F A at which the normal line H8 of the point X8 on the effective diameter peripheral edge portion of the lens surface R8 having the concave portion (having a negative refractive power) intersects the optical axis Z1 is 26 M356934 point P8, and the joint point X8 is connected. The length of the line segment X8-P8 of the intersection point P8 is set to the absolute value of the radius of curvature of the point X8 of the lens surface R8. Further, the intersection of the lens surface r8 and the optical axis Z1 is referred to as a central portion C8. In such a case, the embodiment of the lens surface R8 is such that the lens surface Rg has a concave surface 5 (having a negative refractive power) on the optical axis z 1 (the central portion c8), and a curvature of the central portion C8 of the lens surface R8. Both the center E8 and the intersection point P8 are closer to the object side than the center portion C8, and the length of the line segment X8_P8 (the absolute value of the radius of curvature R8X at the point X8 of the lens surface R8) is larger than the curvature at the center portion C8 of the lens surface R8. The absolute value of the radius R8c is smaller. As described above, "the lens surface R8 has a concave portion (having a 10-negative power) as the central portion c 8 and the negative refractive power at the peripheral portion of the effective diameter is stronger than the central portion C8, so that the 彗 image can be satisfactorily corrected. difference. Preferably, the image side lens surface R9 of the fourth lens L4 is also aspherical. Preferably, the lens surface R9 has a convex portion at the center portion, and the positive refractive power of the peripheral portion of the effective diameter is weaker than the central portion. In the above-mentioned structure, the center portion of the lens surface R9 is convex, and the positive refractive power of the peripheral portion of the effective diameter is weaker than the central portion (hereinafter, also referred to as the lens surface R9). That is, the point at which the normal line H9 of the point X9 on the effective diameter peripheral edge portion of the lens surface R9 having the convex portion (having the positive refractive power) intersects the optical axis 21 is referred to as the intersection point P9, and the joint point X9 and The length of the line segment _9_ρ9 of the intersection point P9 is set to the absolute value of the radius of curvature of the point X9 of the lens surface R9. Further, the intersection of the lens surface R9 and the optical axis Z1 is defined as the center portion C9. In such a case, the lens surface R9 is an embodiment in which the lens surface R9 has a convex surface (having a positive refractive power) on the optical axis Z1 (the central portion C9), and a curvature center E9 of the central portion C9 of the lens surface R9 and the intersection 27 M356934 Both points P9 are closer to the object side than the center portion C9, and the length of the line segment _9_ρΜ々 (the absolute value of the radius of curvature Rx9 at the point χ9 of the lens surface R9) is larger than the radius of curvature of the center portion C9 of the lens surface R9. The absolute value of Rc9 is larger. As described above, "the lens surface R9 has a convex portion as the center portion C9, and the positive refractive power at the peripheral portion of the effective axis is weaker than the central portion C9, so that the field curvature and the coma aberration can be satisfactorily corrected. Further, the radius of curvature of the point X9 on the edge portion of the effective-diameter circumference of the image-side lens surface R9 of the fourth lens [4] is set to R9x, and the center portion C9 where the lens surface R9 and the light-axis 21 intersect When the radius of curvature is set to R9c, the absolute value of the curvature radius R9x is preferably 丄2 times or more of the absolute value of the curvature radius R9c. By setting the absolute value of the curvature radius R9x to a value of 1_2 times or more of the absolute value of the curvature radius R9c, the spherical aberration and the image plane curvature can be satisfactorily corrected. In this way, each lens surface from the object side lens surface 3 of the second lens L2 to the image side lens surface R9 of the fourth I5 lens L4 is set to have the aspherical shape as described above, and the spherical aberration and the image plane curvature are removed. In addition to 彗 像 aberration, it can also be good _ to correct distortion. ◊ Definition of other structural elements The aperture stop St is preferably disposed between the third lens 匕3 and the fourth lens M20. The aperture stop St is arranged in the third lens. The entire lens system can be miniaturized with the fourth lens ’. 28 M356934 In the photographic lens _, when the glass cover or the like is not disposed on the object side of the first lens, the first lens L1 is preferably set as a glass lens, and the second lens L2 and the third lens are £3, The four lenses are set as plastic lenses. By setting the material of the second lens L2 to the fourth lens L4 to plastic, the aspherical shape can be accurately reproduced. Moreover, the lens system can be produced at low cost. As a material for forming each of the plastic lenses from the second lens L2 to the fourth lens L4, a so-called nanocomposite in which particles smaller than the wavelength of light are mixed with respect to the resin material may be used. Each of the lenses of the first lens L1 to the fourth lens L4 is not limited to being made of a material having a refractive index of 10 Å, and any one or more of the four lenses may be a refractive index distribution type lens. The respective lenses of the first lens L2 to the fourth lens L4 are not limited to the case where one or both surfaces are aspherical, and may be formed as a diffractive optical surface. In other words, the diffractive optical element may be formed on any one or more lenses 15 from the first lens L2 to the fourth lens L4. When the light beam passing through the effective light path of the first lens L1 or the second lens L2 becomes stray light and reaches the imaging surface, there is a phenomenon of ghost image, but it is preferably effective on the first lens L1 or the second lens L2. The light-shielding plates Sk 1 and Sk 2 (see FIGS. 1 and 2 ) of the light-shielding means are provided in the field outside the light-diameter, and the stray light is blocked. The shading means may be configured by disposing a sheet which blocks light in an area outside the effective light path of the lens, or a structure of a film made of a light-shielding paint on an area outside the effective light path of the lens. 29 M356934 Further, a space between the first lens 匕丨 and the second lens L2 may be disposed depending on the need for the light shielding means. Further, the light shielding means may be disposed in the field outside the effective light path on the second lens L2 to the fourth lens, or between these lenses. 5, the transmission from the second lens L2 to the fourth lens L4 is as described above, and when the ideal image height is 2fxtan ( Θ /2), the distortion can be made within ± 10%. . As described above, according to the photographic lens of the present invention, the optical performance can be improved as compared with the conventional wide-angle lens, and the size can be reduced. Next, the numerical data relating to each of the imaging lenses according to the first to sixth embodiments of the present invention will be described with reference to Figs. 3 to 2. 3 to 8 are diagrams respectively showing an embodiment! ~ The schematic structure of the photographic lens of the sixth embodiment. j view. The symbols in Figs. 3 to 8 which coincide with the symbols in Figs. 1 and 2 indicate mutually corresponding structures. 15 to FIG. 14 to FIG. 14A are diagrams showing four data of the imaging lenses of the first to sixth embodiments, respectively. The upper left portion (indicated by the symbol (4) in the drawing) in each of the figures: lens data, in the upper center The part (indicated by the symbol (8) in the figure) indicates the photography penetration = the outline specification. Further, in the lower left portion (the figure is indicated by symbol (4)), each coefficient of the aspherical shape indicating the lens surface shape (aspherical shape) is shown. Lower = (indicated by symbol (4) in the figure) indicates the absolute value of the radius of curvature of the effective peripheral portion of each lens surface. In the respective diagrams of Figs. 9 to 14, the upper left side of F' is taken. The 卩 lens data 1f7 is expressed by the face number of the first ", 2, 3, . . . . . . . . in which the face number of the lens and the like are sequentially increased from the object side toward the image side. In addition, the number of these lenses 30 M356934 also includes the surface number (i=7) on which the aperture control light rest St is loaded, and the surface of the object and the side surface of the image side of the optical component cgi of the parallel plane plate (i) =1〇, 11), the face number of the imaging surface (i=12), etc. Further, the lens surface is aspherical, and the surface number is accompanied by an *. 5 Ri represents the paraxial radius of curvature of the i-th (i=l, 2, 3, ...) plane,
Di(i-1、2、3、......)表示第i個面和第i+1個面的光軸zi上 的面間隔。而且’透鏡數據的符號Ri對應於表示圖i中的透 鏡面的符號Ri(i=l、2、3、......) 〇 而且,各透鏡數據中的Ndj表示按照從物體側朝向像侧 10依次增加的第j個(j = l、2、3、......)的光學元件的對d線(波 長587.6nm)的折射率,Vdj表示第j個光學元件的對d線的阿 貝數。 而且近轴曲率半徑及面間隔的皁位為mm ,近轴曲率 半徑在將凸面朝物體側的情況下為正,將凸面朝像側的情 15 況下為負。 另外,各非球面通過下述非球面式而定義。 【數學式1】Di(i-1, 2, 3, ...) represents the interplanar spacing on the optical axis zi of the i-th face and the i+1th face. Further, the symbol Ri of the lens data corresponds to the symbol Ri (i = 1, 2, 3, ...) representing the lens surface in Fig. i, and Ndj in each lens data is oriented from the object side. The refractive index of the jth (j = 1, 2, 3, ...) optical element of the image side 10 which is sequentially increased by the side 10 (wavelength 587.6 nm), and Vdj represents the pair of the jth optical element. Abbe number of the d line. Further, the paraxial radius of curvature and the surface spacing of the soap are mm, and the paraxial radius of curvature is positive when the convex surface is toward the object side, and negative when the convex surface is toward the image side. In addition, each aspherical surface is defined by the following aspherical type. [Math 1]
7- Y2/R ϊΐ(Γ^.72/^2)ι/2 +Σ^ζΓ Ζ :非球面深度(從高度γ的非球面上的點下垂於與非 2〇球面頂點接觸的光軸垂直的平面的垂線長度; γ :高度(從光軸的距離)(mm); R :近轴曲率半徑(mm);7- Y2/R ϊΐ(Γ^.72/^2)ι/2 +Σ^ζΓ Ζ : aspherical depth (the point on the aspheric surface from the height γ is perpendicular to the optical axis that is in contact with the vertex of the non-2-spherical surface The vertical length of the plane; γ: height (distance from the optical axis) (mm); R: paraxial radius of curvature (mm);
Ai :非球面係數(i=3〜2〇); 31 M356934 κ:圓錐定數。 在圖9〜圖14的各圖中的上中央部的概略規格中,表示 以下各值。 分別表不F值:Fno.,半視角:ω,像高:m,後截距:Ai : aspherical coefficient (i = 3 to 2 〇); 31 M356934 κ: conical number. In the outline specifications of the upper center portion in each of Figs. 9 to 14, the following values are shown. Table F values are respectively: Fno., half angle of view: ω, image height: m, back intercept:
Bf(二氣換算長/m Air),從第一透鏡的物體側透鏡面到成 像面的距離:L,第一透鏡像側面的有效光線徑:ED,透 鏡整個系統的焦距(第一透鏡〜第四透鏡的合成焦距):f, 第一透鏡的焦距:fl ,第二透鏡的焦距:f2,第三透鏡的 焦距:f3,第四透鏡的焦距:f4,第一透鏡、第二透鏡的 合成焦距:fl2,第三透鏡、第四透鏡的合成焦距:f34的 值。 上述距離L值是後截距量由空氣換算長表示的值與上 述距離L值中的除後截距量以外由實長表示的值相加後的 值0 ° 15 20 進一步,圖9〜圖14的各圖中的下左部表示有,將表示 各非球面Ri(i=3、4)的非球面式的各係數κ、A3、A4、 A 5......以有效數字3位數歸納後的值。 而且,在圖9〜圖14的各圖中的下右部表示在記載的 「記號」欄的IX3-P3丨、|Χ4-Ρ4|、......是對應於說明書中所 記載的「連結點X3和點p3的線段Χ3_ρ3的長度」、「連結 點X4和交點P4的線段X4-P4的長度」的記號。 圖15疋按1〜6的每個實施例表示條件式(丨)〜(丨2)的各 參數值的圖。 32 M356934 圖16〜圖21是分別表示實施例丨〜實施例6的攝影透鏡 的諸像差的圖。圖16〜圖21分別表示有每個實施例的攝影 透鏡的對d線(波長587.6nm)、厂線(波長486 lnm)、c線(波 長65 6.3 nm)的像差。 另外,就畸變的圖而言,使用透鏡整個系統的 視角Θ (使用變數,〇$ 0 $ ω),且將理想像高設為2f>< tan( (9 /2),表示距其的偏移量。 而且,結構呈旋轉對象的形狀的透鏡的透鏡面有效徑 周緣部,通常為距此透鏡光軸的距離為一定的圓形狀。此 圓形狀的領域成為透鏡面上的有效領域的緣部。 15 20 從表示實施例i〜6的基本數據及諸像差的圖等可知, 根據本創作的廣角攝影透鏡,透過實現4片透鏡各自的形狀 或材質的最適化,可提高光學性能的同時實現小型化。 另外γ本創作不限於上述實施方式及各實施例,可進行種 種變°例如’各透鏡成分的曲率半徑、面間隔及折 射率值等不限於表示在上述各圖中的數值,可取其他值。 本創作的攝影透鏡,透過在第二透鏡以後多用非球 面上而可小型化透鏡系統的同時廉價製作,可進—步良好 地校正像面纟考曲、畸變等像差。 7圖22是表*具備本創作的攝影透鏡、和將此攝影透鏡 所形成的光學像韓拖# φ P & __ 、成電虱t唬的攝影元件的裝載攝影裝 置幻的車载攝影鏡頭的汽車的圖。 5〇2〜Γ= ’❹賴料攝料鏡的車麵影鏡頭 疋衣載於汽車501而被使用。此汽車501包括有: 33 M356934 影助手席側的側方死角範圍的車外用攝影鏡頭的車 鏡頭502、用於攝影汽車W後方死角範圍的車外 用攝衫鏡頭的車_影鏡頭跡和衫錢視鏡背面且用 =與駕駛員相同的前方視野範圍的車内用攝影鏡頭的 皁載攝影鏡頭504。 【圖式簡單說明】 圖1是表示本創作的攝影透鏡的概略結構的圖。 圖2是對圖1施加了用於說明的輔助線等的圖。 10圖3疋表不實施例1的攝影透鏡的概略結構的剖視圖。 圖4是表示實施例2的攝影透鏡的概略結構的剖視圖。 圖5是表示實施例3的攝影透鏡的概略結構的剖視圖。 圖6是表示實施例4的攝影透鏡的概略結構的剖視圖。 圖7是表示實施例5的攝影透鏡的概略結構的剖視圖。 15圖8是表示實施例6的攝影透鏡的概略結構的剖視圖。 圖9是表示實施例1的攝影透鏡的基本數據的圖。 圖1〇是表示實施例2的攝影透鏡的基本數據的圖。 圖11是表示實施例3的攝影透鏡的基本數據的圖。 圖12是表示實施例4的攝影透鏡的基本數據的圖。 20圖13是表示實施例5的攝影透鏡的基本數據的圖。 圖14是表示實施例6的攝影透鏡的基本數據的圖。 圖15是按每個實施例表示對應於條件式(1)〜(12)中各參數 值的圖。 圖16是表示實施例1的攝影透鏡的諸像差的圖。 34 M356934 圖17疋表示實施例2的攝影透鏡的諸像差的圖。 圖18是表示實施例3的攝影透鏡的諸像差的圖。 圖19是表示實施例4的攝影透鏡的諸像差的圖。 圖20是表示實施例5的攝影透鏡的諸像差的圖。 5圖21是表示實施例6的攝影透鏡的諸像差的圖。 圖22是表示裝載車載攝影鏡頭的汽車的圖。Bf (two gas conversion length / m Air), the distance from the object side lens surface of the first lens to the imaging surface: L, the effective ray diameter of the first lens image side: ED, the focal length of the entire lens of the lens (first lens ~ The combined focal length of the fourth lens: f, the focal length of the first lens: fl, the focal length of the second lens: f2, the focal length of the third lens: f3, the focal length of the fourth lens: f4, the first lens, the second lens Synthetic focal length: fl2, composite focal length of the third lens and the fourth lens: the value of f34. The distance L value is a value represented by the air-converted length of the back-intercept amount and a value added by the real length other than the post-intercept amount in the distance L value. 0° 15 20 Further, FIG. 9 to FIG. The lower left portion of each of the graphs 14 indicates that each of the coefficients κ, A3, A4, A 5 ... of the aspherical surface representing each aspherical surface Ri (i = 3, 4) is represented by a significant number of 3 The value after the number of digits is summarized. In the lower right part of each of FIGS. 9 to 14 , IX3-P3 丨, |Χ4-Ρ4|, ... in the "mark" column of the description are corresponding to those described in the specification. The symbol "the length of the line segment Χ3_ρ3 connecting the point X3 and the point p3" and the "length of the line segment X4-P4 of the joint point X4 and the intersection point P4". Fig. 15 is a diagram showing the values of the respective conditional values (丨) to (丨2) in each of the embodiments 1 to 6. 32 M356934 Figs. 16 to 21 are diagrams showing aberrations of the imaging lenses of the embodiment ~ to the sixth embodiment, respectively. Fig. 16 to Fig. 21 show aberrations of the photographic lens of each example for the d line (wavelength 587.6 nm), the plant line (wavelength 486 lnm), and the c line (wavelength 65 6.3 nm), respectively. In addition, in terms of the distortion map, the angle of view of the entire system of the lens is used (using the variable 〇$ 0 $ ω), and the ideal image height is set to 2f>< tan((9 /2), indicating the distance from it Further, the peripheral surface of the effective surface of the lens surface of the lens having the shape of the rotating object is usually a circular shape having a constant distance from the optical axis of the lens. The field of the circular shape becomes an effective field on the lens surface. From the basic data and the aberrations of the examples i to 6, it is understood that the wide-angle imaging lens of the present invention can improve the optical performance by optimizing the shape or material of each of the four lenses. In addition, the gamma creation is not limited to the above-described embodiments and the respective embodiments, and various changes can be made. For example, the curvature radius, the surface interval, and the refractive index value of each lens component are not limited to those shown in the above figures. The value of the photographic lens of the present invention can be made inexpensively by miniaturizing the lens system by using the aspherical surface after the second lens, and the image surface can be corrected step by step. Distortion aberrations, etc. 7 Fig. 22 is a photographing device with the photographic lens of the present invention and the photographic element of the photographic element formed by the photographic lens formed by the photographic lens, φ P & __ The car's picture of the car photographic lens. 5〇2~Γ= 'The car's face lens for the photographic camera is used in the car 501. This car 501 includes: 33 M356934 shadow assistant side The car lens 502 of the exterior photographic lens of the side dead angle range, the car photographic lens of the exterior lens for the rear corner of the car W, and the back of the shirt and the same front as the driver Fig. 1 is a view showing a schematic configuration of an imaging lens of the present invention. Fig. 2 is a view showing an auxiliary line for explaining the same as that of Fig. 1. Fig. 3 is a cross-sectional view showing a schematic configuration of an imaging lens of the first embodiment. Fig. 4 is a cross-sectional view showing a schematic configuration of an imaging lens of the second embodiment. Fig. 5 is a view showing a schematic configuration of an imaging lens of the third embodiment. Sectional view of Figure 6. Figure 6 is a representation Fig. 7 is a cross-sectional view showing a schematic configuration of an imaging lens of Example 5. Fig. 8 is a cross-sectional view showing a schematic configuration of an imaging lens of Example 6. Fig. 9 is a view showing an embodiment of the imaging lens of the embodiment. Fig. 1A is a view showing basic data of the imaging lens of the embodiment 2. Fig. 11 is a view showing basic data of the imaging lens of the embodiment 3. Fig. 12 is a view showing an embodiment. Fig. 13 is a view showing basic data of the imaging lens of the embodiment 5. Fig. 14 is a view showing basic data of the imaging lens of the sixth embodiment. Fig. 15 is a diagram showing the basic data of the imaging lens of the sixth embodiment. The example shows a map corresponding to each parameter value in the conditional expressions (1) to (12). Fig. 16 is a view showing aberrations of the imaging lens of the first embodiment. 34 M356934 FIG. 17A is a view showing aberrations of the imaging lens of Example 2. Fig. 18 is a view showing aberrations of the imaging lens of the third embodiment. Fig. 19 is a view showing aberrations of the imaging lens of Example 4; Fig. 20 is a view showing aberrations of the imaging lens of Example 5; Fig. 21 is a view showing aberrations of the imaging lens of the sixth embodiment. Fig. 22 is a view showing a car on which an in-vehicle photographing lens is mounted.
20攝影透鏡 L3第三透鏡 S t孔徑光搁 Cgl光學部件 C3,C5中心部 Spl,Sp2 圓 5〇1汽車 H5法線 X3,X4,X5,X6 點 502,5〇3,504車載攝影鏡頭 【主要元件符號說明】 1 〇攝影元件 L2第二透鏡 Z1光轴20 photographic lens L3 third lens S t aperture light shelf Cgl optical component C3, C5 center Spl, Sp2 circle 5 〇 1 car H5 normal X3, X4, X5, X6 point 502, 5 〇 3, 504 car photographic lens [main components Explanation of symbols] 1 〇 photographic element L2 second lens Z1 optical axis
Ski, Sk2遮光板 P5交點 L1第一透鏡 L4第四透鏡 Jk受光面 R5c,R5x曲率半徑 E5曲率中心 VI光線Ski, Sk2 visor P5 intersection L1 first lens L4 fourth lens Jk light receiving surface R5c, R5x radius of curvature E5 center of curvature VI light
ED第一透鏡L1的像側透鏡面R2的有效光線徑 R1第一透鏡L1的物體側透鏡面 R2第一透鏡L1的像側透鏡面 R3第二透鏡L2的物體側透鏡面 R4第二透鏡L2的像側透鏡面 R5第三透鏡L3的物體側透鏡面 R6第三透鏡L3的像側透鏡面 R7孔徑光欄St的位置 35 M356934 R8第四透鏡L4的物體側透鏡面 R9第四透鏡L4的像側透鏡面 R10光學部件Cgl的物體側表面 R11光學部件Cgl的像側表面 R12成像面JkThe effective ray diameter R1 of the image side lens surface R2 of the ED first lens L1, the object side lens surface R2 of the first lens L1, the image side lens surface R3 of the first lens L1, the object side lens surface R4 of the second lens L2, the second lens L2 Image side lens surface R5 Object side lens surface R6 of third lens L3 Image side lens surface R7 of third lens L3 Position 35 of aperture stop St. M356934 R8 Object side lens surface R9 of fourth lens L4 Fourth lens L4 Image side surface R11 of the side lens surface R10 optical part Cgl Image side surface R12 of the optical part Cgl of the image side Jk
3636
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| JP2008114823A JP5102096B2 (en) | 2008-04-25 | 2008-04-25 | Imaging lens and imaging apparatus using the imaging lens |
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| CN112904531A (en) * | 2014-12-17 | 2021-06-04 | Lg伊诺特有限公司 | Image pickup lens, camera module and digital device including the same |
| TWI832219B (en) * | 2021-04-22 | 2024-02-11 | 美商貓頭鷹實驗室股份有限公司 | Wide angle lens and camera system for peripheral field of view imaging |
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| JP5270425B2 (en) | 2009-03-31 | 2013-08-21 | 富士フイルム株式会社 | Imaging lens and imaging apparatus |
| JP5778260B2 (en) * | 2011-04-28 | 2015-09-16 | 富士フイルム株式会社 | Imaging lens and imaging apparatus |
| JP5889880B2 (en) | 2011-04-28 | 2016-03-22 | 富士フイルム株式会社 | Imaging lens and imaging apparatus |
| CN203519913U (en) * | 2011-04-28 | 2014-04-02 | 富士胶片株式会社 | Imaging lens and imaging apparatus |
| JP5814351B2 (en) | 2011-04-28 | 2015-11-17 | 富士フイルム株式会社 | Imaging lens and imaging apparatus |
| JP5825845B2 (en) * | 2011-05-19 | 2015-12-02 | 京セラ株式会社 | Imaging lens |
| JP5893997B2 (en) * | 2012-04-24 | 2016-03-23 | 京セラ株式会社 | Imaging lens and imaging apparatus |
| CN104981723B (en) * | 2013-02-08 | 2017-07-04 | 柯尼卡美能达株式会社 | Photographic optical system, photo-optics device and digital device |
| US20160139362A1 (en) * | 2013-06-20 | 2016-05-19 | Konica Minolta Inc. | Imaging Lens And Imaging Device |
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| JP4700821B2 (en) * | 2001-02-21 | 2011-06-15 | マクセルファインテック株式会社 | Wide angle lens |
| JP2005227426A (en) * | 2004-02-12 | 2005-08-25 | Nagano Kogaku Kenkyusho:Kk | Wide angle lens |
| JP4847150B2 (en) * | 2005-02-21 | 2011-12-28 | 富士フイルム株式会社 | Wide-angle imaging lens |
| JP4747645B2 (en) * | 2005-04-11 | 2011-08-17 | コニカミノルタオプト株式会社 | Wide angle lens and imaging device |
| JP4744184B2 (en) * | 2005-04-20 | 2011-08-10 | 日本電産コパル株式会社 | Super wide angle lens |
| JP4864403B2 (en) * | 2005-09-29 | 2012-02-01 | 富士フイルム株式会社 | Wide-angle lens system and imaging device |
| JP5084335B2 (en) * | 2007-04-16 | 2012-11-28 | 京セラ株式会社 | Imaging lens |
| JP2008275666A (en) * | 2007-04-25 | 2008-11-13 | Kyocera Corp | Imaging optical device and surveillance camera |
| JP2008281859A (en) * | 2007-05-11 | 2008-11-20 | Largan Precision Co Ltd | Wide angle lens |
| JP5252842B2 (en) * | 2007-06-27 | 2013-07-31 | 京セラ株式会社 | Imaging lens |
| WO2009041382A1 (en) * | 2007-09-28 | 2009-04-02 | Konica Minolta Opto, Inc. | Wide-angle optical system, imaging lens device, monitor camera, and digital apparatus |
| CN101861541B (en) * | 2007-11-22 | 2012-08-01 | 柯尼卡美能达精密光学株式会社 | Wide angle optical system, imaging lens device, monitor camera, and digital apparatus |
| JP2009265338A (en) * | 2008-04-24 | 2009-11-12 | Kyocera Corp | Wide-angle imaging lens |
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| CN112904531A (en) * | 2014-12-17 | 2021-06-04 | Lg伊诺特有限公司 | Image pickup lens, camera module and digital device including the same |
| CN112904531B (en) * | 2014-12-17 | 2023-01-24 | Lg伊诺特有限公司 | Image pickup lens, camera module and digital device including the same |
| TWI832219B (en) * | 2021-04-22 | 2024-02-11 | 美商貓頭鷹實驗室股份有限公司 | Wide angle lens and camera system for peripheral field of view imaging |
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