TWM355391U - Photographing lens and the photographing device thereof - Google Patents

Photographing lens and the photographing device thereof Download PDF

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Publication number
TWM355391U
TWM355391U TW97219419U TW97219419U TWM355391U TW M355391 U TWM355391 U TW M355391U TW 97219419 U TW97219419 U TW 97219419U TW 97219419 U TW97219419 U TW 97219419U TW M355391 U TWM355391 U TW M355391U
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Taiwan
Prior art keywords
lens
photographic
central portion
refracting power
effective diameter
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TW97219419U
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Chinese (zh)
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Taro Asami
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Fujinon Corp
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Publication of TWM355391U publication Critical patent/TWM355391U/en

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M355391 五、新型說明: ’ 【新型所屬之技術領域】 本創作關於一種使被攝體之像成像的攝影透鏡及使用 該攝影透鏡的攝影裝置。 5 k 【先前技術】 習知用於車載用、手機用、監視用等的攝影裝置的小 型化、輕量化的廣角的攝影透鏡。這種攝影透鏡將作爲被 • 攝體的物體的像成像在咖元件或c刪元件等的攝影 -10 元件的受光面上。 作爲謀求小型化、輕量化的廣角的攝影透鏡,已知由 六片透鏡構成且第三透鏡由玻璃材料形成的攝影透鏡(參 照專利前案1)、和由包含塑膠接合透鏡的五至六片透鏡構 成的攝影透鏡(參照專利前案2)。申請人申請了專利前案3 I5記載的攝影透鏡的發明專利。 ’、M355391 V. New description: ‘New technical field to which it belongs. This creation relates to a photographic lens that images an image of a subject and a photographic apparatus using the photographic lens. 5 k [Prior Art] A wide-angle photographic lens that is small and lightweight for use in an imaging device such as a vehicle, a mobile phone, or a monitor. This photographic lens images an image of an object to be photographed on a light receiving surface of a photographic element 10 such as a coffee element or a c-cut component. As a wide-angle photographic lens that is miniaturized and lightweight, a photographic lens composed of six lenses and a third lens made of a glass material (see Patent Document 1), and five to six sheets including a plastic cemented lens are known. A photographic lens composed of a lens (refer to Patent Prep. 2). The applicant applied for the invention patent of the photographic lens described in Patent No. 3 I5. ’,

專利前案1 專利前案2 專利前案 曰本特開2007— 249073號公報; 曰本特開2006— 284620號公報; 20 日本特願2007— 261626號。 仁疋如專利刚案1至3,若第三透鏡由破璃材料形 成,則成本升高。此外,透過在第三透鏡中使用非球 鏡,可以很好地補正像面彎曲。 咬 用塑膠非球面透鏡的接合 則製造成本升高。 專利前案2記載的技術是使 透鏡。若接合透鏡使用非球面, 4 M355391 然而近年來CCD元件和CMOS元件等的攝影元件的 小型化、高像素化急速發展。隨之,要求將用於車載用、 手機用、監視用等的攝影裝置的攝影透鏡進一步廣角化、 小型化的同時使其像差減小。 【新型内容】 本創作是鑒於上述情況做出的’其目的在於,提供— 種在能夠廣角化及小型化的同時提高光學性能之攝影透鏡 及使用該攝影透鏡的攝影裝置。 ' 1〇 纟創作#第一攝影透鏡的特徵在於,從物體側起順次 包括具有.負的屈光度的第一透鏡、具有負的屈光度的第 二透鏡、第三透鏡、具有正的屈光度的第四透鏡、具有正 的屈光度的第五透鏡、及具有負的屈光度的第六透鏡;從 第二透鏡到第六透鏡中的各透鏡的至少一個透鏡面呈非球 Μ面;第三透鏡及第六透鏡由對d線的阿貝數爲45以下的材 料形成。 本創作的第二攝影透鏡的特徵在於,從物體側起依序 包::第-透鏡’具有負的屈光度’{凹面朝向成成像側 的透鏡’第二透鏡’至少成成像側的透鏡面呈非球面, 該透鏡面的中心部呈凹面且有效直徑周邊部的負的屈光度 小於上述中心部;第三透鏡,至少_ 又 ^ V個透鏡面呈非球面; 弟四透鏡’具有正的屈光度,至少一個 ^ 夕個透鏡面呈非球面; 弟五透鏡’具有正的屈光度,至少一 個透鏡面呈非球面; 及第六透鏡,具有負的屈光度,至少—彻 個透鏡面呈非球面。 5 M355391 和第攝影透鏡較佳為在第三透鏡 物體側的透鏡 上述第三透鏡較佳為具有正的屈光度 面的中心部呈凸面。 第六透 上述第一透鏡較佳為玻璃透鏡,從第二透 鏡的各透鏡較佳為塑膠透鏡。 上述第-攝影透鏡及第二攝影透鏡較佳為滿足 (1):2.〇<f56/f<5.5。其中’,是上述攝影透鏡整個系統的 焦距’ f56是上述第五透鏡和第六透鏡的合成焦距。 上述第-攝影透鏡及第二攝影透鏡較佳為滿足條件式 叩W<”/f<5’5Q其中’ f是上述攝影透鏡整個 糸統的焦距,D4是上述第二透鏡和第三透鏡之間的空氣間 隔,D5是上述第三透鏡的中心厚度。 15 上述第一攝影透鏡及第二攝影透鏡較佳為滿足條件式 (3): 4.0<f3/f<9.G。其巾,f是上述攝影透鏡整個系統的 焦距,f3是上述第三透鏡的焦距。 • 就上述第二透鏡的成成像側的透鏡面而言,較佳為透 鏡面的中心部呈凹面,有效直徑周邊部的負的屈光度小於 上述中心部。 上述第二透鏡的物體側的透鏡面,較佳為透鏡面的中 心部呈凸面且有效直徑周邊部的正的屈光度小於該中心 ’或者a玄透鏡面的中心部呈凸面且有效直徑周邊部耳有 負的屈光度。 6 M355391 上述第三透鏡的物體側的透鏡面,較佳為透鏡面的中 心部呈凸面,在有效直㈣具有正的以度大於上 部的區域。 上述第五透鏡的成像側的透鏡面,較佳為透鏡面的中 5心部呈凸面,有效直徑周邊部的正的屈光度小於該中心部。 上述第六透鏡的物體側的透鏡面,較佳為透鏡面的中 心部呈凹面且有效直徑周邊部的負的屈光度小於該中心 部。 上述第六透鏡的成成像側的透鏡面,較佳為透鏡面的 10中心部呈凸面且有效直徑周邊部的正的屈光度小於中心 部。 上述第一攝影透鏡及第二攝影透鏡較佳為滿足條件式 (4) 11 < L/f < 1 8。其中’ f是上述攝影透鏡整個系統的焦 距,L是從上述第一透鏡的物體側的透鏡面到成像面的距 15離。 本創作的攝影裝置的特徵在於,具備第一攝影透鏡或 第二攝影透鏡、和將該攝影透鏡所形成的光學像變換成電 信號的攝影元件。 「透鏡面的有效光線直徑」是表示通過透鏡面的有效 2〇光線中的通過最外側(從光軸最遠的位置)的光線與該透鏡 面的父點所描晝的圓的直徑,通過上述透鏡面的有效光線 疋用於被攝體的像的成像的光線《此處透鏡面的有效光線 直徑與透鏡面的有效直徑一致。 7 M355391 透鏡面的有效直徑周邊部」表示通過透鏡面的有效 直徑内的所有光線中的、通過最外側(從透鏡的光軸最遠的 位置)的光線與透鏡面相交的該透鏡面上的部位。 「具有正的屈光度的透鏡」表示該透鏡是在近軸量區 _ 5具有正的屈光度的透鏡。 「具有負的屈光度的透鏡」表示該透鏡是在近軸量區 具有負的屈光度的透鏡。 「透鏡面的中心部呈凸面、且有效直徑周邊部的正的 鲁 @光度小於上述中心部」表示有效直徑周邊部和中心部均 10呈凸面、且有效直徑周邊部的曲率半徑的值的絕對值大於 該中心部的曲率半徑的值的絕對值的情況。 「透鏡面的中心部呈凸面、且有效直徑周邊部的正的 屈光度大於上述中心、部」表料效直徑周邊部和中心部均 呈凸面、且有效直徑周邊部的曲率半徑的值的絕對值小於 15該中心部的曲率半徑的值的絕對值的情況。 透兄面的中〜邛呈凸面且在有效直徑周邊部具有負 • ㈣光度」表示透鏡面的中心部呈凸面且有效直徑周邊部 呈凹面的情況。 透鏡面的中…[5呈凹面、且有效直徑周邊部的負的 2〇屈光度小於上述中心部」表示有效直徑周邊部和中心部均 呈凹面、且有效直徑周邊部的曲率半徑的值的絕對值大於 該中心部的曲率半徑的值的絕對值的情況。 M355391 透鏡面的中心部呈凹面且在有效直徑周邊部具有正 的屈光度」表示透鏡面的中^部呈凹面且有效直徑周邊部 呈凸面的情況。Pre-patent case 1 Pre-patent case 2 Pre-patent case 曰本特开2007-249073号; 曰本特开2006- 284620号; 20 Japan's special wish 2007-261626. Ren Yan, such as the patents 1 to 3, if the third lens is formed of a broken glass material, the cost increases. Further, by using an aspherical lens in the third lens, the curvature of field can be corrected. Bonding with a plastic aspheric lens increases the manufacturing cost. The technique described in Patent Document 2 is a lens. In the case of the aspherical surface of the spliced lens, 4 M355391. In recent years, the size and high pixelation of photographic elements such as CCD elements and CMOS elements have been rapidly increasing. In response to this, it is required to further reduce the size of the imaging lens for an imaging device such as a vehicle, a mobile phone, or a monitor, while reducing the size thereof. [New content] The present invention has been made in view of the above circumstances, and an object thereof is to provide an image pickup lens that can improve the optical performance while being wide-angled and downsized, and an image pickup apparatus using the same. The first photographic lens is characterized by including, in order from the object side, a first lens having a negative refracting power, a second lens having a negative refracting power, a third lens, and a fourth having a positive refracting power. a lens, a fifth lens having a positive refracting power, and a sixth lens having a negative refracting power; at least one lens surface of each of the second lens to the sixth lens having an aspherical surface; a third lens and a sixth lens The lens is formed of a material having an Abbe number of 45 or less for the d line. The second photographic lens of the present invention is characterized in that, from the object side, the package is sequentially: the first lens 'has a negative refracting power' {the concave surface faces the lens on the imaging side, and the second lens ′ is at least the lens side of the imaging side. The aspherical surface, the central portion of the lens surface is concave and the negative diopter of the effective diameter peripheral portion is smaller than the central portion; the third lens has at least _ and the V lens surfaces are aspherical; the fourth lens has a positive refracting power. At least one of the lens faces is aspherical; the fifth lens has a positive refracting power, at least one lens surface is aspherical; and the sixth lens has a negative refracting power, at least - the entire lens surface is aspherical. 5 M355391 and the first photographic lens are preferably the lens on the third lens object side. The third lens preferably has a convex portion at a central portion having a positive refracting surface. Preferably, the first lens is a glass lens, and the lenses from the second lens are preferably plastic lenses. Preferably, the first photographic lens and the second photographic lens satisfy (1): 2. 〇 < f56/f < 5.5. Wherein, the focal length 'f56 of the entire system of the above photographic lens is the combined focal length of the fifth lens and the sixth lens. Preferably, the first photographic lens and the second photographic lens satisfy a conditional formula &W<"/f<5'5Q, where 'f is the focal length of the entire photographic lens, and D4 is the second lens and the third lens The air gap between the D5 is the center thickness of the third lens. The first photographic lens and the second photographic lens preferably satisfy the conditional expression (3): 4.0 <f3/f<9.G. f is the focal length of the entire system of the photographic lens, and f3 is the focal length of the third lens. • For the lens surface on the imaging side of the second lens, it is preferable that the central portion of the lens surface is concave, and the effective diameter peripheral portion The negative diopter is smaller than the center portion. The lens surface on the object side of the second lens preferably has a convex portion at a central portion of the lens surface and a positive refracting power of the peripheral portion of the effective diameter is smaller than a center portion of the center or a central lens surface The convex portion has a negative diopter in the peripheral portion of the effective diameter. 6 M355391 The lens surface on the object side of the third lens is preferably convex at the center of the lens surface, and has a positive direct (4) area with a greater degree than the upper portion. Preferably, the lens surface on the imaging side of the fifth lens has a convex surface in the middle of the lens surface, and the positive refractive power of the peripheral portion of the effective diameter is smaller than the central portion. Preferably, the central portion of the lens surface is concave and the negative diopter of the effective diameter peripheral portion is smaller than the central portion. The lens surface on the imaging side of the sixth lens is preferably convex at the center portion of the lens surface and has an effective diameter periphery. The positive diopter of the portion is smaller than the central portion. The first photographic lens and the second photographic lens preferably satisfy the conditional expression (4) 11 < L/f < 18 . wherein ' f is the focal length of the entire system of the photographic lens L is a distance from the lens surface on the object side of the first lens to the imaging surface. The photographing apparatus of the present invention is characterized in that it is provided with a first photographing lens or a second photographing lens, and a photoreceptor lens The photographic element that converts the optical image into an electrical signal. The "effective ray diameter of the lens surface" is the ray that passes through the outermost side (the farthest position from the optical axis) among the effective two rays passing through the lens surface. The diameter of the circle depicted by the parent point of the lens surface, the effective light ray passing through the lens surface, and the imaged light used for the image of the subject. "The effective ray diameter of the lens surface is consistent with the effective diameter of the lens surface. . 7 M355391 The effective diameter peripheral portion of the lens surface" means that the light passing through the outermost side (the position farthest from the optical axis of the lens) passing through the outermost surface (the position farthest from the optical axis of the lens) intersects the lens surface among all the rays in the effective diameter of the lens surface Part. "Lens having a positive refracting power" means that the lens is a lens having a positive refracting power in the paraxial region _5. "Lens having a negative refracting power" means that the lens is a lens having a negative refracting power in the paraxial region. "The central portion of the lens surface is convex, and the positive Lu @光度 of the effective diameter peripheral portion is smaller than the center portion", indicating that the effective diameter peripheral portion and the central portion are both convex, and the absolute radius of the effective diameter is the absolute value of the radius of curvature. The case where the value is larger than the absolute value of the value of the radius of curvature of the center portion. "The central portion of the lens surface has a convex surface, and the positive refractive power of the peripheral portion of the effective diameter is larger than the center and the portion." The peripheral portion of the material effective diameter and the central portion are convex, and the absolute value of the radius of curvature of the peripheral portion of the effective diameter is The case where the absolute value of the radius of curvature of the center portion is less than 15. The center of the through-face is convex and has a negative at the peripheral portion of the effective diameter. (4) The luminosity indicates that the central portion of the lens surface is convex and the peripheral portion of the effective diameter is concave. In the middle of the lens surface, [5 is concave and the negative 2〇 diopter of the effective diameter peripheral portion is smaller than the center portion", indicating that the effective diameter peripheral portion and the central portion are both concave and the absolute value of the radius of curvature of the effective diameter peripheral portion is absolute. The case where the value is larger than the absolute value of the value of the radius of curvature of the center portion. M355391 The central portion of the lens surface is concave and has a positive refracting power at the peripheral portion of the effective diameter, which means that the middle portion of the lens surface is concave and the peripheral portion of the effective diameter is convex.

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20 、,有效直徑周邊部的屈光度小於透鏡面的中心部的屈 光度」表不有效直徑周邊部和中心部均呈凸面、且有效直 k周邊。P的正的屈光度小於中心部的情況,或者有效直和 周邊部和中心均呈凹面、且有效直徑周邊部的負的屈光^ 小於中心部的情況。 透鏡面的中〜部呈凹面、且有效直徑周邊部的負的 屈光度大於上述中心部」表示有效直徑周邊部和中心部均 呈凹面、且有效直徑周邊部的曲率半徑的絕對值小於該中 心部的曲率半徑的絕對值的情況。 透兄面的中〜邛呈凸面,在透鏡面的中心部和有效 直徑周邊部之間具有正的屈光度大於上述中心部的區域」 ^不如下結構:從該透鏡面財㈣财效直徑周邊部的 犯Km面呈凸面’在巾^部和有效直㈣邊部之間且有 曲率半徑的值的絕對值比中心部的曲率半徑的值的絕對值 減小的區域°中心部的曲率半徑表示透鏡面與光軸相交的 位置的透鏡面的曲率半徑。而用絕對值表示曲率半徑的值 的理由是爲了明確曲率半徑的A小關係。 ,右採用本創作的第一攝影透鏡及利用該攝影透鏡的攝 影裝置,從物體側起依序配置具有負的屈光度的第—透 鏡、具有負的屈光度的第二透鏡、第三透鏡、具有正的屈 光度的第四透鏡、具有正的屈光度的第五透鏡、及具有負 9 M355391 的屈光度的第六透鏡,·從第二透鏡到第六透鏡中的各透鏡 的至j —個透鏡面呈非球面;第三透鏡及第六透鏡由對d 線的阿貝數爲45以下的材料形成,因此,可以廣角化及小 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 以捕獲以較大的視場角入射的光線,能夠將光學系統廣角 化。透過將第二透鏡的至少單側的面做成非球面,在可以 良好地補正各種像差的同時,將透鏡系統小型化。在第二 透鏡中’軸上光線和軸外光線被分離,因此若將該透鏡面 1〇做成非球面,則有利於像差補正,畸變的補正也比較容易。 第一透鏡也將軸上光線和軸外光線分離,但作爲配置 在透鏡系統的最靠物體側的第一透鏡的材料,如後述較佳 為使用玻璃材料。此外’第一透鏡在透鏡系統中成爲最大 口k的透鏡。因此將適用塑膠材質的第二透鏡做成非球面 B透鏡,在透鏡的製作上及像差補正上是較佳的。 由於上述第二透鏡到第六透鏡中的各透鏡的至少一個 透鏡面呈非球面,因此可在良好地補正球面像差、像面彎 曲、慧形像差的同時,將透鏡系統小型化。 將第二透鏡及第六透鏡由對d線的阿貝數爲45以下的 2〇材料形成,可以良好地補正轴向色像差和倍率色像差。 若採用本創作的第二攝影透鏡及利用該攝影透鏡的攝 影裝置,從物體側起依次配置有:第一透鏡,具有負的屈 光度,是凹面朝向成成像側的彎月透鏡;第二透鏡,至少 成成像側的透鏡面呈非球面’成成像側的透鏡面的中心部 M355391 呈凹面且有效直徑周邊部的負的屈光度小於中心部;第三 透鏡,至少一個透鏡面呈非球面;第四透鏡,具有正的屈 光度,至少一個透鏡面呈非球面;第五透鏡,具有正的屈 光度,至少一個透鏡面呈非球面;及第六透鏡,具有負的 • 5屈光度,至少一個透鏡面呈非球面,所以可廣角化及小型 化的同時提高光學性能。 透過從最靠物體側依次配置負的第一透鏡'第二透 鏡,能夠捕獲以較大的視場角入射的光線,因此能將光學 系統廣角化。透過將第一透鏡做成凹面朝向成成像側的彎 '10月透鏡可以良好地補正像面彎曲。 透過在第二透鏡中至少將成成像側的面做成非球面, 月巨在可良好地補正各種像差的同時,將透鏡系統小型化。 由於第二透鏡將軸上光線和軸外光線分離,因此若將該透 鏡做成非球面,則對像差的補正較有利,對畸變的補正也 15 比較容易。 第一透鏡也將軸上光線和軸外光分離,但作爲配置於 • 透鏡系統的最靠物體側的第一透鏡的材質,如後所述較佳 為使用玻璃材料。而且由於第一透鏡在透鏡系統中爲最大 口徑的透鏡,因此將適用塑膠材質的第二透鏡做成非球面 20透鏡的方案在透鏡的製作上及像差補正上是較佳的。 透過將第二透鏡形成爲:成成像側的面做成非球面、 該透鏡面的中心部呈凹面、且有效直徑周邊部的負的屈光 度小於其中心部的形狀,能使穿過第二透鏡的周邊的光線 不急劇地彎曲就會聚’因此能良好地補正畸變。 11 M355391 將第三透鏡做成至少一個透鏡面呈非球面的透鏡,可 以良好地補正像曲彎曲。 透過將第四透鏡、第五透鏡都做成至少單側的面爲非 球面的且具有正的屈光度的透鏡,將第六透鏡做成至少單 5側的面爲非球面的具有負的屈光度的透鏡,在第三透鏡和 第四透鏡之間配置光攔,可以在良好地補正球面像差、像 面彎曲、慧形像差的同時,將透鏡系統小型化。 【實施方式】 10 下面,參照附圖詳細地說明本創作的攝影透鏡及使用 該攝影透鏡的攝影裝置的實施方式。 圖1是表示利用本創作的攝影透鏡的攝影裝置的簡要 結構的截面圖,圖2是對圖1附加用於說明的輔助線等的 圖。圖示的攝影透鏡20主要是對汽車的前方、側方、後方 15等的狀況進行拍攝的車載用攝影裝置所使用的廣角的攝影 透鏡’將被攝體的像成像在由CCD或CMOS等構成的攝 影元件10的受光面Jk上。該攝影元件1〇將攝影透鏡2〇 所形成的光子像變換成電彳§號,得到表示該光學像的圖像 信號。 20 [關於攝影透鏡的基本結構及其作用、效果] 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從物體側起依次具備:第一透鏡li、第二 透鏡L2、第二透鏡L3、孔彼光棚St、第四透鏡L4、第五 透鏡L5、第六透鏡L6、以及光學部件Cgl。 12 M355391 此處對第— 的情況進行說明 合透鏡。 透鏡L1至第六透鏡L6的各透鏡是單透鏡 ’但這些透鏡不限於單透鏡,也可以是接20, the diopter of the effective diameter peripheral portion is smaller than the refracting power of the central portion of the lens surface." The effective diameter peripheral portion and the central portion are both convex and effective around the k. The positive refractive power of P is smaller than that of the central portion, or the effective straight portion and the peripheral portion and the center are both concave, and the negative refractive power of the peripheral portion of the effective diameter is smaller than that of the central portion. The middle portion of the lens surface has a concave surface, and the negative refractive power of the peripheral portion of the effective diameter is larger than the central portion." The effective diameter peripheral portion and the central portion are both concave, and the absolute value of the radius of curvature of the effective diameter peripheral portion is smaller than the central portion. The case of the absolute value of the radius of curvature. The mid-邛 of the through-face is convex, and has a positive refracting power between the central portion of the lens surface and the peripheral portion of the effective diameter that is larger than the central portion of the center portion. ^Not the following structure: from the lens surface (four) financial effect diameter peripheral portion The Km surface is convexly curved. The area where the absolute value of the radius of curvature between the towel portion and the effective straight (four) edge portion is smaller than the absolute value of the value of the radius of curvature of the central portion. The radius of curvature of the lens surface at the position where the lens surface intersects the optical axis. The reason for using the absolute value to represent the value of the radius of curvature is to clarify the A-small relationship of the radius of curvature. The first photographic lens and the photographic device using the photographic lens are arranged on the right side, and a first lens having a negative refracting power, a second lens having a negative refracting power, and a third lens are positively arranged from the object side. a fourth lens of diopter, a fifth lens having positive refracting power, and a sixth lens having diopter of negative 9 M355391, from the lens to the j-th lens surface of the second lens to the sixth lens Since the third lens and the sixth lens are formed of a material having an Abbe number of 45 or less on the d-line, the optical performance can be improved by widening and miniaturization. 5 By arranging the negative first lens 'second lens on the most object side, it is possible to capture light incident at a large angle of view and widen the optical system. By forming at least one side surface of the second lens as an aspherical surface, the lens system can be miniaturized while various aberrations can be satisfactorily corrected. In the second lens, the on-axis ray and the off-axis ray are separated. Therefore, if the lens surface 1 〇 is made aspherical, the aberration correction is facilitated, and the correction of the distortion is relatively easy. The first lens also separates the on-axis light from the off-axis light. However, as the material of the first lens disposed on the most object side of the lens system, it is preferable to use a glass material as will be described later. Further, the first lens becomes the lens of the largest port k in the lens system. Therefore, the second lens to which the plastic material is applied is made into an aspherical B lens, which is preferable in the fabrication of the lens and the aberration correction. Since at least one lens surface of each of the second lens to the sixth lens has an aspherical surface, the lens system can be miniaturized while satisfactorily correcting spherical aberration, field curvature, and coma aberration. The second lens and the sixth lens are formed of a material having a Abbe number of 45 or less on the d line, and the axial chromatic aberration and the chromatic aberration of magnification can be satisfactorily corrected. According to the second photographic lens of the present invention and the photographic apparatus using the photographic lens, a first lens having a negative refracting power and a meniscus lens having a concave surface toward the imaging side is disposed in order from the object side; At least the lens surface of the imaging side is aspherical. The central portion M355391 of the lens surface on the imaging side is concave and the negative diopter of the effective diameter peripheral portion is smaller than the central portion; the third lens has at least one lens surface aspherical; fourth a lens having a positive refracting power, at least one lens surface being aspherical; a fifth lens having a positive refracting power, at least one lens surface being aspherical; and a sixth lens having a negative • 5 diopter, at least one lens surface being non-spherical The spherical surface makes it possible to increase the optical performance while widening and miniaturizing. By arranging the negative first lens 'second lens in order from the most object side, it is possible to capture light incident at a large angle of view, thereby widening the optical system. The curvature of field can be satisfactorily corrected by making the first lens concave toward the curved side of the imaging side. By forming at least the surface on the imaging side of the second lens as an aspherical surface, Moonlight can reduce the various aberrations while finely correcting the lens system. Since the second lens separates the on-axis ray from the off-axis ray, if the lens is made aspherical, the correction of the aberration is advantageous, and the correction of the distortion is also easy. The first lens also separates the on-axis light from the off-axis light. However, as the material of the first lens disposed on the most object side of the lens system, it is preferable to use a glass material as described later. Further, since the first lens is the lens having the largest aperture in the lens system, it is preferable to apply the second lens of the plastic material to the aspherical lens 20 in the fabrication of the lens and the aberration correction. The second lens is formed such that the surface on the imaging side is an aspherical surface, the central portion of the lens surface is concave, and the negative refractive power of the peripheral portion of the effective diameter is smaller than the shape of the central portion thereof, so that the second lens can be passed through The surrounding light does not sharply bend and gathers, so it can correct the distortion well. 11 M355391 The third lens is made into at least one lens whose aspherical surface is aspherical, which can correct the curvature of the curvature. By making the fourth lens and the fifth lens both at least one side of the surface having a non-spherical surface and having a positive refracting power, the sixth lens is made to have at least a single side having a non-spherical surface having a negative refracting power. In the lens, a light intercept is disposed between the third lens and the fourth lens, and the lens system can be miniaturized while satisfactorily correcting spherical aberration, field curvature, and coma aberration. [Embodiment] Hereinafter, an embodiment of an imaging lens of the present invention and an imaging device using the same will be described in detail with reference to the accompanying drawings. Fig. 1 is a cross-sectional view showing a schematic configuration of an image pickup apparatus using the photographic lens of the present invention, and Fig. 2 is a view showing an auxiliary line and the like which are attached to Fig. 1 for explanation. The photographing lens 20 shown in the drawing is mainly a wide-angle photographic lens used for an in-vehicle photographing device that photographs the front, the side, and the rear of the automobile, etc. The image of the subject is formed by CCD or CMOS. On the light receiving surface Jk of the photographic element 10. The imaging element 1 converts the photon image formed by the photographic lens 2A into an electric signal to obtain an image signal indicating the optical image. 20 [Regarding the basic structure of the photographic lens, its function, and effect] First, the basic structure of the photographic lens 20 will be described. The photographic lens 20 includes, in order from the object side along the optical axis Z1, a first lens li, a second lens L2, a second lens L3, a hole shed St, a fourth lens L4, a fifth lens L5, and a sixth lens L6. And the optical component Cgl. 12 M355391 Here, the case of the - is explained. Each of the lenses of the lenses L1 to L6 is a single lens ‘but these lenses are not limited to a single lens, but may be connected

-10 透過攝衫透鏡20,使表示被攝體的物體的像成像的成 上述配置有攝影元件10的受光面Jk。 在將攝影透鏡應用於攝影裝置時,根據安裝透鏡的照 目機側的結構’較佳為配置蓋玻璃、低通濾光片或紅外線 截=遽光片等’在圖丨中所示將這些設想的平行平板狀的 光學部件Cgl配置在透鏡系統和攝影元件1〇之間的例子。 、取代在透鏡糸統和攝影元件之間配置低通遽光片或要 截止特定的波段的各種濾光片等,可以在第一透鏡L1至 第六透鏡L6中的相鄰的透鏡之間配置這些各種攄光片。 或者,可以在第一透鏡L1至第六透鏡L6的任意的透鏡面 上形成與各種濾光片具有相同作用的塗層。 20 圖1中的符號R1至R16表示如下述的構成因素。R1 和R2表示第一透鏡L1的物體側的透鏡面和成像側的透鏡 面,R3和R4表示第二透鏡L2的物體側的透鏡面和成像 側的透鏡面’ R5和R6表示第三透鏡L3的物體側的透鏡 面和成像側的透鏡面’ R7表示孔徑光攔st的孔徑部,R8 和R9表示第四透鏡L4的物體側的透鏡面和成像側的透鏡 面’ R10和R11表示第五透鏡L5的物體側的透鏡面和成 像側的透鏡面,R12和R13表示第六透鏡L6的物體側的 透鏡面和成像側的透鏡面’ R14和R15表示光學部件Cgl 13 M355391 的物體側的表面和成像側的表面,R16表示如上述與攝影 透鏡20的受光面Jk 一致的成像面。 各透鏡面R1至R6、透鏡面R8至R13分別是由在從 與光軸相交的中心部一直到有效直徑周邊部的範圍的圓滑 5連接的曲面形成的透鏡面,而不是具有階差等的不連續的 區域的透鏡面。 就攝影透鏡20而言,第一透鏡“具有負的屈光度, 第二透鏡L2具有負的屈光度,第四透鏡χ4具有正的屈光 度,第五透鏡L5具有正的屈光度,第六透鏡具有負的 1〇屈光度。 、 該攝影透鏡20的第二透鏡L2、第三透鏡[3、第四透 鏡L4、第五透鏡]^及第六透鏡,各個透鏡的至少一個透 非球面,第二透鏡及第六透鏡由對d線的阿貝數爲 45以下的材料形成。 15-10 The image of the object representing the subject is imaged by the lens 20, and the light receiving surface Jk of the imaging element 10 is placed as described above. When the photographic lens is applied to the photographic device, the structure of the camera side on which the lens is mounted is preferably configured such that a cover glass, a low-pass filter or an infrared ray cut-off light ray sheet, etc. are shown in the figure. An example of a parallel plate-shaped optical component Cg1 is disposed between the lens system and the imaging element 1A. Instead of arranging a low-pass calender between the lens system and the photographic element or various filters to be cut off in a specific wavelength band, it is possible to arrange between adjacent lenses in the first lens L1 to the sixth lens L6. These various enamel films. Alternatively, a coating layer having the same function as the respective filters may be formed on any of the lens faces of the first lens L1 to the sixth lens L6. 20 Symbols R1 to R16 in Fig. 1 indicate constituent elements as described below. R1 and R2 denote the lens side of the object side of the first lens L1 and the lens side of the image side, R3 and R4 denote the lens side of the object side of the second lens L2 and the lens side of the image side 'R5 and R6 denote the third lens L3 The lens side of the object side and the lens surface of the imaging side ' R7 denotes the aperture portion of the aperture stop st, R8 and R9 denote the lens side of the object side of the fourth lens L4 and the lens side of the imaging side ' R10 and R11 denote the fifth The lens side of the object side of the lens L5 and the lens side of the imaging side, R12 and R13 indicate the lens side of the object side of the sixth lens L6 and the lens surface of the image side 'R14 and R15 indicate the surface of the object side of the optical component Cgl 13 M355391 And the surface on the image side, R16 denotes an image plane which coincides with the light receiving surface Jk of the photographing lens 20 as described above. Each of the lens faces R1 to R6 and the lens faces R8 to R13 is a lens face formed by a curved surface connected in a smooth shape 5 from a central portion intersecting the optical axis to a peripheral portion of the effective diameter, instead of having a step or the like. The lens surface of the discontinuous area. In the case of the photographic lens 20, the first lens "has a negative refracting power, the second lens L2 has a negative refracting power, the fourth lens χ4 has a positive refracting power, the fifth lens L5 has a positive refracting power, and the sixth lens has a negative refracting power. 〇 diopter. The second lens L2, the third lens [3, the fourth lens L4, the fifth lens] and the sixth lens of the photographic lens 20, at least one of the lenses is aspherical, the second lens and the sixth The lens is formed of a material having an Abbe number of 45 or less for the d line.

20 透過將开> 成第二透鏡L3的材料對d線的阿貝數設爲 45 >以下,因此良好地補正倍率色像差變得容易。但若是形 成第三透鏡L3的材料對d線的阿貝數超過45,則倍率色 像差的補正變得困難。 透過將形成第六透鏡L6的材料對d線的阿貝數設爲 =下,因此良好地補正轴向色像差變得容易。但若是形 成第六透鏡L6的材料對厂線的阿貝數超 二 像差補正變得困難。 …5’則軸向色 作爲用帝人 形成第三透鏡L3或第六透鏡L6 化成株式會社制的聚碳 的材料,可以使酸酯樹脂、 14 M355391By setting the Abbe number of the material of the second lens L3 to the d line to 45 > or less, it is easy to correct the chromatic aberration of magnification. However, if the Abbe number of the material forming the third lens L3 to the d line exceeds 45, the correction of the chromatic aberration of magnification becomes difficult. By setting the Abbe number of the material forming the sixth lens L6 to the d line to be lower, it is easy to satisfactorily correct the axial chromatic aberration. However, if the material forming the sixth lens L6 is corrected for the Abbe number super-two aberration of the factory line, it becomes difficult. (5', axial color) As a material for forming a third lens L3 or a sixth lens L6 into a polycarbon produced by Teijin Co., Ltd., an acid ester resin, 14 M355391

PanliteSP-15i6(該公司產品名稱、“panme,,是該公司註 冊商標)。該材料具有1.6以上的折射率、阿貝數小到25.5、 且光學變形小的特徵。 透過將第三透鏡L3或第六透鏡L6使用該材料,在可 5以良好地補正倍率色像差和軸向色像差的同時,能將因成 里時所生成的變形而造成的影響抑制爲最小限,例如使用 於超過-百萬像素那樣的高像素的攝影元件用的透鏡,也 能夠得到良好的圖像。 將第二透鏡到第六透鏡做成各個透鏡的至少一個透鏡 1〇 ^呈非球面’可以在為廣角的同時良好地補正球面像差(也 稱球差)、像面彎曲(也稱場曲)、慧形像差(也稱慧差)及崎 15 20 上述攝衫透鏡2G可以構成如下:攝影透鏡2()沿著光 物體側起依次配置有:第—透鏡^,具有負的屈 度’是凹面朝向成像側的彎月透鏡;第二透鏡L2,至少 成像側的透鏡面呈非球面’成像側的透鏡面的中心部呈凹 面且有效直徑周邊部的負的屈光度小於巾心、部;第三透鏡 至少—㈣鏡面呈非球面;第四透鏡L4,具有正的屈 至/自透鏡面呈非球面;第五透鏡L5,具有正的 ,光度’至個透鏡面呈非球面;及第六透鏡L6,具有 負的屈光度,至少—個透鏡面呈非球面。 將第二透鏡L2的成像側的透鏡面如上述構成,可以 良好地補正畸變。 15 M355391 第六透鏡L6具右鱼止& 轴向色像差。有負的屈先度’因此可以更好地補正 構成透鏡的透鏡面的中心部是與通過該透鏡的光轴 父的透鏡面上的部位(光軸和透鏡面的交點)。 本創作的攝影透鏡可以滿足上述兩種基本結構中的任 ,也可以同時滿足上述兩種基本結構。 透鏡述攝影透鏡具備的基本結構,能夠在將攝影 兄 小型化的同時’提高該攝影透鏡的光學性能。 作用:果糊嫩⑽本結構進—步限定的結構及其 接著說明對該攝影透鏡20具備的 步限定的構成因素及其作用、效果。進一步;構 的構成因料相作的攝料鏡㈣以必^=:構 15 20 效果][關於用條件式限定上述基本結構的結構和其作用與 步限定攝料鏡的基本__下條件式 與效果進行說明。本創作的攝影透鏡可以 二=式0漸 ιτ的兩個以上的組合。 納如式⑴至(9)中用記號表示的各參數據的意思歸 二:攝影透鏡整個系統的焦距’即,第—透鏡li至第 透鏡L6的合成焦距; f 1:第一透鏡的焦距; 16 M355391 f2 : 第二透鏡的焦距; f3 : 第三透鏡的焦距; f4 : 第四透鏡的焦距; f5 : 第五透鏡的焦距; f6 : 第六透鏡的焦距; fl2:第一透鏡、及第二透鏡的合成焦距; f5 6 :第五透鏡、及第六透鏡的合成焦距’ fl23 :第一透鏡、第二透鏡、及第三透鏡的合成焦距; f45 6:第四透鏡、第五透鏡、及第六透鏡的合成焦距; 10 D1 :第一透鏡的中心厚度; 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; vd3 :第三透鏡對d線的阿貝數; vd5 :第五透鏡對d線的阿貝數;Panlite SP-15i6 (the company's product name, "panme," is a registered trademark of the company). This material has a refractive index of 1.6 or more, an Abbe number as small as 25.5, and a small optical distortion. Through the third lens L3 or The sixth lens L6 uses this material, and can correct the chromatic aberration of magnification and the axial chromatic aberration well, and can minimize the influence caused by the deformation generated during the formation, for example, A lens for a high-pixel imaging element such as a megapixel can also obtain a good image. At least one lens 1 of the second lens to the sixth lens is formed as an aspheric surface. Wide-angle correction of spherical aberration (also called spherical aberration), image curvature (also called field curvature), coma aberration (also called coma) and Saki 15 20 can be made as follows: photography The lens 2 () is disposed in order from the side of the light object: a first lens ^ having a negative flexion 'is a meniscus lens having a concave surface toward the imaging side; and a second lens L2 having at least an aspheric surface on the imaging side' Lens surface on the imaging side The central portion is concave and the negative diopter of the effective diameter peripheral portion is smaller than the center of the towel; the third lens is at least—(4) the mirror surface is aspherical; and the fourth lens L4 has a positive flexion/aspheric surface from the lens surface; The lens L5 has a positive, luminosity 'to the lens surface is aspherical; and the sixth lens L6 has a negative refracting power, at least one lens surface is aspherical. The lens surface of the imaging side of the second lens L2 is as described above The composition can correct the distortion well. 15 M355391 The sixth lens L6 has a right fish stop & axial chromatic aberration. It has a negative yaw degree 'so it can better correct the center of the lens surface constituting the lens. The position of the optical axis of the lens on the lens surface of the parent (the intersection of the optical axis and the lens surface). The photographic lens of the present invention can satisfy either of the above two basic structures, and can simultaneously satisfy the above two basic structures. The basic structure of the photographic lens can improve the optical performance of the photographic lens while miniaturizing the photographic lens. Function: Fruity and tender (10) The structure defined by the structure and its subsequent description The constituent elements of the step lens 20 and the functions and effects thereof are further defined. Further, the configuration of the photographing mirror (4) of the constituents of the structure is required to be a function of the above-mentioned basic structure. The structure and its function are described in the basic __lower conditional expressions and effects of the step-limited photographic mirror. The photographic lens of the present invention can be a combination of two or more of two = 0 ι ι τ. The meaning of each parameter data indicated by the symbol is two: the focal length of the entire system of the photographic lens 'that is, the composite focal length of the first lens li to the lens L6; f 1: the focal length of the first lens; 16 M355391 f2: the second lens Focal length; f3: focal length of the third lens; f4: focal length of the fourth lens; f5: focal length of the fifth lens; f6: focal length of the sixth lens; fl2: composite focal length of the first lens and the second lens; f5 6 a composite focal length of the fifth lens and the sixth lens ' fl23 : a combined focal length of the first lens, the second lens, and the third lens; f45 6: a combined focal length of the fourth lens, the fifth lens, and the sixth lens; 10 D1 : center thickness of the first lens D4: air separation of the second lens and the third lens; D5: center thickness of the third lens; vd3: Abbe number of the third lens to the d line; vd5: Abbe number of the fifth lens to the d line;

vd6 :第六透鏡對d線的阿貝數; L .從第一透鏡的物體側的透鏡面到成像面的距離。 上述距離L的值是後截距距離量按空氣換算長度表示 的值、及上述距離L值令的除後截距距離量以外的值按實 際長度表示的值相加後的值。後截距距離Bf是從第六透鏡 20 L6的成像側的透鏡面R13到成像面R16的空氣換算長度。 條件式(1)·· 2.0<f56/f<5,5是有關像差補正的式子开。又 若透鏡系統構成爲滿足條件式⑴,則能夠容易地 差及像面f曲的補正。若將透鏡系統構成爲⑽ 過條件式(1)的上限,即滿足f56/f^5 5 ,超 町條件式,則難以 17 M355391 良好地補正色像差。若將透鏡系統構成爲f56/f的值小於 條件式(1)的下限,即滿足2.〇2£56纤的條件式,則難以良 好地補正像面彎曲。 、條件式(2): 2·5 < (D4+D5)/f< 5.5是有關像差的補正或 透鏡系統的大小的式子。Vd6: Abbe number of the sixth lens to the d line; L. Distance from the lens side of the object side of the first lens to the image plane. The value of the distance L is a value obtained by dividing the value of the back-intercept distance by the air-converted length and the value of the actual length by the value of the distance-L value. The back intercept distance Bf is an air-converted length from the lens surface R13 on the imaging side of the sixth lens 20 L6 to the imaging plane R16. The conditional expression (1)·· 2.0 <f56/f<5,5 is a formula relating to aberration correction. Further, when the lens system is configured to satisfy the conditional expression (1), it is possible to easily correct the correction of the image plane f. When the lens system is configured to (10) the upper limit of conditional expression (1), that is, satisfying f56/f^5 5 and the super-conditional formula, it is difficult for 17 M355391 to correct the chromatic aberration well. When the lens system is constructed such that the value of f56/f is smaller than the lower limit of the conditional expression (1), that is, the conditional expression of 2.22£56 fiber is satisfied, it is difficult to correct the curvature of field. Conditional Formula (2): 2·5 <(D4+D5)/f<5.5 is a formula relating to correction of aberration or size of a lens system.

10 若將透鏡系統構成爲滿足條件式(2),可以良好地補正 ^面像差、畸變像差、及慧形像差’且由於後截距距離取 T長,所以能夠在增大視場角的同時作爲攝影透鏡得到充 分的光學性能。若將透鏡系統構成爲(D4+D5)/f的值超過 條件式(2)的上限,則第一透鏡的物體側的透鏡面的直徑增 大、且透鏡整體長度也變長而難以小型化。若將透鏡系^ 構成爲(D4+D5)/f的值小於條件式⑺的下限,不能良好地 補正球面像差、及慧形像差,難以構成明亮且F值小的透 鏡。 條件式(3): 4.0<f3/f<9.0是有關倍率色像差和後截 距距離的式子。 若將透鏡系統構成爲滿足條件式(3),則可以不縮短後 截距距離而良好地補正倍率色像差。若將透鏡系統構成爲 f3/f的值超過條件式(3)的上限,則難以良好地補正倍率色 20像差。若將透鏡系統構成爲f3/f的值小於條件式(3)的下 限,則能夠良好地補正倍率的色像差、但後截距距離變短, 難以在攝影元件10和攝影透鏡2〇之間插入各種濾光片。 條件式(4): ll<L/f<l8是有關視場角和裝置尺寸的 式子。 M355391 若將透鏡系統構成爲滿足條件式(4),可以實現小型且 寬視場角的透鏡系統。若將透鏡系統構成爲L/f的值超過 條件式(4)的上限,則容易實現廣角化、但透鏡系統會大型 化。若將透鏡系統構成爲L/f的值小於條件式(4)的下限, 5則旎夠將透鏡系統小型化,但難以實現廣角化。 條件式(5) : 一4.2< f6/f< — 1.0是有關倍率色像差及 軸向色像差的式子。 若將透鏡系統構成爲滿足條件式(5),可以良好地補正 • 料色像差及軸向色像差。若將透鏡系統構成爲f6/f的值 -10超過條件式(5)的上限,則倍率色像差增大。若將透鏡系統 構成爲f6/f的值小於條件式(5)的下限,則第五透鏡具有的 負屈光度減小’不能夠良好地補正軸向色像差。 條件式(6): — 2.0<fl2/f< — l.〇是有關視場角、裝置 尺寸、及像差的式子。 15 若將透鏡系統構成為滿足條件式(6),則可以不增大像 面f曲而Λ現小型且見視場角的透鏡系統。若將透鏡系統 • 構成爲fl2/f的值超過條件式(6)的上限,則能夠容易實現 廣角化,但像面彎曲增大。若將透鏡系統構成爲fl2/f的 值小於條件式(6)的下限,則對於配置在物體側的具有負的 20屈光度的第一透鏡及第二透鏡而言,負的屈光度減小,所 以穿過這些透鏡的光線不能夠較大地彎曲,難以兼顧廣角 化和透鏡系統的小型化。 條件式(7) vd5/vd6> 1.5是有關軸向色像差和倍率色 像差的式子。 19 M355391 若將透鏡系統構成爲滿足條件式(7),則可以同時良好 地補正轴向色像差和倍率色像差。若將透鏡系統構成爲 vd5/vd6的值小於條件式(7)的下限,則難以同時良好地補 正軸向色像差和倍率色像差。 5 條件式(8) ·· — 2.5<fl23/f456< — 0.5是有關視場角、 後截距距離、及像差的式子。 若將透鏡系統構成爲滿足條件式(8),則不用增大像面 彎曲而可以兼顧廣角化和規定長度的後截距距離的讀保。 若將透鏡系統構成爲fl23/f456的值超過條件式(8)的上 10限’則容易實現廣角化、但像面彎曲增大,難以成像良好 的像。若將透鏡系統構成爲H23/f456的值小於條件式 的下限,則難以兼顧廣角化和規定長度的後截距距離的確 保。若後截距距離縮短,難以在成像側的透鏡面和攝影元 件的受光面之間插入蓋玻璃或各種濾光片。 15 條件式(9) : 0.8<Dl/f是有關第一透鏡的耐衝擊性的 式子。 若將透鏡系統構成爲滿足條件式(9 ),可以提高例如於 車载使用時的第一透鏡對各種衝擊的強度。若將透鏡系統 構成爲Dl/f的值小於條件式(9)的下限,則第一透鏡變薄 2〇 且變得易碎。 [關於限定上述基本結構的其他的構成因素、和其作 用、效果] ^ 以下,對限定攝影透鏡的上述條件式以外的構成因 素、及其作用與效果進行說明。 20 M355391 關於有關透鏡的形成材料的進一步限定: 透過將第-透鏡做成破璃透鏡,可以製作耐氣候性高 且,容易碎的攝影透鏡。透過由塑膠材料製作從第二透鏡 到第六透鏡的各透鏡,可以準確地再現非球面形狀,並且 5可以使透鏡系統低價且輕量。 爲了良好地補正倍率色像差,較佳為第三透鏡L3及 第六透鏡L6的材質w線的阿貝數爲3()以下。爲了良好 :補正軸向色像差,更佳為第三透鏡L3及第六透鏡“的 材質對d線的阿貝數爲28以下。 10第-透鏡、第二透鏡、第四透鏡、第五透鏡的材質較 為對d線的阿貝數爲4〇以上。如此抑制色像差的發生, 可以得到良好的分辨性能。 關於有關孔徑光攔的構成因素的限定: 孔徑光欄St較佳為配置在第三透鏡L3和第四透鏡L4 之間。將孔徑光柢 1 st s己置在第三透鏡L3和第四透鏡L4 之間,可使整個透鏡系統小型化。 關於有關第一透鏡的構成因素的限定: 例如在車載照相機或監視照相機的嚴格的環境下使用 2。2攝衫透鏡’作爲第—透鏡較佳為使用高耐水性、高耐醆 性、及高耐藥品性的材質。 作爲用於形成第—透鏡的材料,較佳為使用日本光學 續工#會標準(日本光學石肖子卫業會規格)的粉末法耐水 性爲一級到四級的材料。 22 M355391 作爲用於形成第—透鏡的材料,較佳為使用日本光學 ^會‘準的粉末法耐酸性爲一級到四級的材料。 作爲形成第一透鏡的材料,較佳為使用堅硬的材質。 彳卩爲第—透鏡的形成材料較佳為使用玻璃材料,也可 以使用透明的陶瓷材料。 透過將第-透鏡L1做成玻璃透鏡,可以製作高耐氣 候性且不易碎的攝影透鏡。 第一透鏡L1 +限於做成玻璃$面透鏡,該第一透鏡 L1的單側的透鏡面或兩側的透鏡面可以由非球面構成。透 10過將第一透鏡⑴故成非球面玻璃透鏡,可以形成高耐水 性、高耐酸性、及高耐藥品性等、並且可以更良好地補正 各種像差的攝影透鏡。 15 可以在比第一透鏡更靠物體側配置保護透鏡的蓋玻 璃’或者可以在第一透鏡物體側的透鏡面配置提高耐氣候 性的硬塗層、或例如玻璃質的薄膜的構件。 採用在比第一透鏡更靠物體側配置蓋玻璃等、且第一 透鏡難以受到外部環境的影響的結構時,第一透鏡可以做 成塑膠非球面透鏡。冑第一透鏡冑成塑膠非球面透鏡能夠 更良好地補正像面彎曲、及畸變。 20 關於有關第二透鏡的構成因素的限定: 第二透鏡L2的物體側的透鏡面趵較佳爲非球面。 第二透鏡L2的物體側的透鏡面R3的中心部呈凸面 (具有正的屈光度),有效直徑周邊部的正的屈光度小於中 22 M355391 心部,或者較佳為有效直徑周 度)。 邊部呈凹面(具有負的屈光 510 If the lens system is configured to satisfy the conditional expression (2), the surface aberration, the distortion aberration, and the coma aberration can be well corrected, and since the back intercept distance is T long, the field of view can be increased. At the same time as the photographic lens, sufficient optical performance is obtained. When the lens system is configured such that the value of (D4+D5)/f exceeds the upper limit of the conditional expression (2), the diameter of the lens surface on the object side of the first lens increases, and the overall length of the lens also becomes long, which makes it difficult to miniaturize. . When the lens system is configured such that the value of (D4 + D5) / f is smaller than the lower limit of the conditional expression (7), the spherical aberration and the coma aberration are not satisfactorily corrected, and it is difficult to form a bright lens having a small F value. Conditional Formula (3): 4.0 < f3/f < 9.0 is an expression relating to magnification chromatic aberration and back intercept distance. When the lens system is configured to satisfy the conditional expression (3), the chromatic aberration of magnification can be satisfactorily corrected without shortening the back intercept distance. When the lens system is configured such that the value of f3/f exceeds the upper limit of the conditional expression (3), it is difficult to satisfactorily correct the magnification color 20 aberration. When the lens system is configured such that the value of f3/f is smaller than the lower limit of the conditional expression (3), the chromatic aberration of the magnification can be satisfactorily corrected, but the back intercept distance becomes short, and it is difficult to perform the imaging element 10 and the photographic lens 2. Insert various filters between them. Conditional Formula (4): ll < L/f < l8 is an expression relating to the angle of view and the size of the device. M355391 If the lens system is configured to satisfy conditional expression (4), a lens system with a small and wide angle of view can be realized. When the lens system is configured such that the value of L/f exceeds the upper limit of the conditional expression (4), it is easy to achieve wide angle, but the lens system is enlarged. When the lens system is configured such that the value of L/f is smaller than the lower limit of the conditional expression (4), the lens system is miniaturized, but it is difficult to achieve wide angle. Conditional Formula (5): A 4.2 <f6/f< - 1.0 is an expression relating to chromatic aberration of chromaticity and axial chromatic aberration. When the lens system is configured to satisfy the conditional expression (5), it is possible to satisfactorily correct the chromatic aberration of the material and the axial chromatic aberration. When the lens system is configured such that the value -10 of f6/f exceeds the upper limit of the conditional expression (5), the chromatic aberration of magnification increases. When the lens system is configured such that the value of f6/f is smaller than the lower limit of the conditional expression (5), the negative refractive power of the fifth lens is reduced 'the axial chromatic aberration cannot be satisfactorily corrected. Conditional Formula (6): — 2.0<fl2/f<- l.〇 is an expression relating to the angle of view, the size of the device, and the aberration. 15 If the lens system is configured to satisfy the conditional expression (6), it is possible to realize a lens system that is small and has an angle of view without increasing the image plane. When the lens system is configured such that the value of fl2/f exceeds the upper limit of the conditional expression (6), the wide angle can be easily achieved, but the image plane curvature is increased. When the lens system is configured such that the value of fl2/f is smaller than the lower limit of the conditional expression (6), the negative diopter is reduced for the first lens and the second lens having a negative 20 diopter disposed on the object side. The light passing through these lenses cannot be bent largely, and it is difficult to achieve both wide-angle and miniaturization of the lens system. The conditional expression (7) vd5/vd6> 1.5 is an expression relating to axial chromatic aberration and chromatic aberration of magnification. 19 M355391 If the lens system is configured to satisfy conditional expression (7), axial chromatic aberration and lateral chromatic aberration can be corrected well at the same time. When the lens system is configured such that the value of vd5/vd6 is smaller than the lower limit of the conditional expression (7), it is difficult to satisfactorily correct axial chromatic aberration and lateral chromatic aberration at the same time. 5 Conditional Formula (8) ·· — 2.5<fl23/f456<-0.5 is an expression relating to the angle of view, the back intercept distance, and the aberration. When the lens system is configured to satisfy the conditional expression (8), the read angle of the wide-angle and the back-intercept distance of the predetermined length can be achieved without increasing the curvature of the image plane. When the lens system is configured such that the value of fl23/f456 exceeds the upper limit of the conditional expression (8), it is easy to achieve wide angle, but the curvature of the image is increased, and it is difficult to form a good image. When the lens system is configured such that the value of H23/f456 is smaller than the lower limit of the conditional expression, it is difficult to achieve both the wide angle and the back intercept distance of the predetermined length. If the back intercept distance is shortened, it is difficult to insert a cover glass or various filters between the lens surface on the imaging side and the light receiving surface of the photographic element. 15 Conditional Formula (9): 0.8<Dl/f is an equation relating to the impact resistance of the first lens. When the lens system is configured to satisfy the conditional expression (9), it is possible to improve the strength of various impacts of the first lens, for example, when used in a vehicle. If the lens system is constructed such that the value of D1/f is smaller than the lower limit of the conditional expression (9), the first lens becomes thinner and becomes brittle. [Other constituent factors, effects, and effects of the above-described basic structure] ^ Hereinafter, constituent elements other than the above-described conditional expressions for limiting the photographic lens, and their actions and effects will be described. 20 M355391 Further restrictions on the material for forming the lens: By making the first lens into a glass lens, it is possible to produce a photographic lens that is highly weather-resistant and easily broken. By making each lens from the second lens to the sixth lens from a plastic material, the aspherical shape can be accurately reproduced, and the lens system can make the lens system inexpensive and lightweight. In order to correct the chromatic aberration of magnification, it is preferable that the Abbe number of the material w line of the third lens L3 and the sixth lens L6 is 3 () or less. In order to improve the axial chromatic aberration, it is more preferable that the material of the third lens L3 and the sixth lens "the Abbe number of the d line is 28 or less. 10th lens, second lens, fourth lens, fifth The material of the lens has an Abbe number of 4 Å or more for the d line. Therefore, good resolution can be obtained by suppressing the occurrence of chromatic aberration. About the limitation of the constituent elements of the aperture stop: The aperture stop St is preferably configured. Between the third lens L3 and the fourth lens L4, the aperture stop 1sts is placed between the third lens L3 and the fourth lens L4, so that the entire lens system can be miniaturized. Limitation of factors: For example, the use of a 2. 2 camera lens as a first lens in a strict environment of an in-vehicle camera or a surveillance camera is preferably a material that uses high water resistance, high scratch resistance, and high chemical resistance. The material for forming the first lens is preferably a material having a water resistance of one to four grades using a powder method of the Japan Optics Continuation ## standard (Japan Optical Shikoko Health Industry Co., Ltd.) 22 M355391 Lens The material is preferably a material having a acid resistance of from 1 to 4 using a powder method of the Japanese Optical Society. As a material for forming the first lens, a hard material is preferably used. It is preferable to use a glass material, or a transparent ceramic material can be used. By forming the first lens L1 as a glass lens, it is possible to produce a photographic lens which is highly weather resistant and is not easily broken. The first lens L1 + is limited to a glass $ face In the lens, the lens surface on one side of the first lens L1 or the lens surface on both sides may be formed by an aspherical surface. When the first lens (1) is formed as an aspherical glass lens, high water resistance and high acid resistance can be formed. And a photographic lens that is highly resistant to chemicals and can correct various aberrations better. 15 A cover glass that can be placed on the object side of the first lens or a lens surface that can be placed on the first lens object side A hard coat layer for improving weather resistance or a member such as a vitreous film. The cover glass is disposed on the object side of the first lens, and the first lens is difficult to receive the external environment. In the affected structure, the first lens can be made into a plastic aspherical lens. The first lens is formed into a plastic aspherical lens to better correct the curvature of field and distortion. 20 Regarding the limitation of the constituent elements of the second lens: The lens surface 物体 on the object side of the second lens L2 is preferably aspherical. The central portion of the lens surface R3 on the object side of the second lens L2 has a convex surface (having a positive refracting power), and the positive refracting power of the peripheral portion of the effective diameter is smaller than 22 M355391 heart, or preferably effective diameter circumference.) Concave at the side (with negative refraction 5

10 15 如圖2所不’上述「透鏡面幻的中心部呈凸面沣有 正的屈光度有效直徑周邊部的正的屈光度小於中心部的 結構(以下還稱爲透鏡面R3的結構例)」如下述結 將中心部呈凸面的透鏡面R3的有效直徑周邊部上的 點X3的法線H3和光軸Z1相交的點設爲交點p3,將連接 點X3和交點P3的線段χ3_ρ3的長度作爲透鏡面幻的點 X3的曲率半徑的絕對值。將透鏡面R3和光轴ζι的交點 設爲中心部C3。如此設定時’上述透鏡面R3的結構例為: 透鏡面R3在光軸Z1上(中心部C3)呈凸面(具有正的屈光 度),透鏡面R3的中心部C3的曲率中心£3及上述交點 P3兩者均比中心部C3更位於成像側,且線段χ3 —p3的 長度(透鏡面R3的點X3的曲率半徑R3x的絕對值)大於透 鏡面R3的中心部C3的曲率半徑R3C的絕對值。 20 在圖中表示出以交點P3爲中心、半徑長度爲線段 X3-P3的長度的圓Spl,及以曲率中心E3爲中心、半徑長 度爲曲率半徑R3c的絕對值的圓Sp2。 用絕對值表示曲率半徑的值的理由是爲了明瞭曲率半 徑的大小關係。 在透鏡面R3以外的有關後述的透鏡面的相同的說明 中’省略上述說明中所使用的符號的圖示。 後述δ兑明中’用絕對值表示曲率半徑的大小的理由同 上述。 23 M355391 「第二透鏡的物體側的透鏡面,中心部具有正的屈光 度,有效直徑周邊部具有負的屈光度(呈凹面)」如下述: 透鏡面R3的中心部C3的曲率中心的點E3比作爲透鏡面 R3和光軸Z1的交點的中心部C3更位於成像側,表示作 5爲上述透鏡面R3上的有效直徑周邊部的點X3的曲率中心 的點P3比中心部C3更位於物體側。 如上所述,第二透鏡L2的物體側的透鏡面R3的中心 部呈凸面,使其有效直徑周邊部的正的屈光度比中心部 弱或者使有效直徑周邊部呈凹面,因此在可以維持廣角 10 化的同時良好地補正像面彎曲。 第二透鏡L2的成像側的透鏡面R4較佳為做成非球 面。 第二透鏡L2的成像側的透鏡面R4較佳為中心部呈凹 面(具有負的屈光度)’在有效直徑周邊部其負的屈光度比 15 中心部弱。 上述「透鏡面R4的中心部呈凹面,有效直徑周邊部 # 的負的屈光度比中心部弱的結構(下面,還稱爲透鏡面R4 的結構例)」為如下述的結構。 2〇古^即,將中心部呈凹面(具有負的屈光度)的透鏡面R4的 < t直;L周邊部上的點χ4的法線H4和光軸z 1相交的點 二爲=點P4,將連接點χ4和交點p4的線段χ4_ρ4的長 度作爲透鏡面R4的點χ4的曲率半徑的絕對值。此外,將 透鏡面R4和光軸Z1的交點設爲中心部C4。如此設定時, 上述透鏡面R4的結構例為:透鏡面R4在光軸Z1上(中心 24 M355391 部C4)呈凹面(具有負的屈光度),透鏡面R4的中心部C4 的曲率中心E4及上述交點?4兩者均比中心部Q更位於 成像侧,且線段X4—P4的長度(透鏡面R4的點X4的曲率 半feR4x的絕對值)大於透鏡^4的中心部c4的曲 徑R4c的絕對值。 如上所述,第二透鏡的成像側的透鏡® R4的中心部 呈凹面’在其有效直徑周邊部使其負的屈光度比中心部 弱’因此能夠使穿過第二透鏡的周邊的光線不急劇地彎曲 而會聚,因此可以良好地補正畸變。 將第二透鏡L2的物體側的透鏡面R3的有效直徑周邊 部X3上的曲率半徑設爲R3x時,該曲率半徑咖的絕對 值(1X3 - P3丨)較佳為中心部C3的曲率半徑心的絕對值的 1.5倍以上。 透過將曲率半徑R3x的絕對值設爲曲率半徑R3c 對值i.5倍以上,可以在使廣角化容易的同時良好地補正 像面彎曲。 Φ 將第二透鏡L2的成像側的透鏡面R4的有效直徑周邊 部X4上的曲率半徑設爲R4x時,該曲率半徑R4x的絕對 值(|X4 - P4|)較佳為中心部C4的曲率半徑R4c的絕對值的 20 1.5倍以上。 透過將曲率半徑R4x的絕對值設爲曲率半徑r3c的絕 對值的1.5倍以上,因此可以良好地補正畸變。 關於有關第三透鏡的構成因素的限定: 25 M355391 孝又佳為第二透鏡L3具有正的屈光度,且物體側的透 鏡面R5的中q。卩呈凸面。透過如此設置,可以良好地補 正像面彎曲。 第三透鏡可以具有負的屈光度。 5 第三透鏡L3的物體側的透鏡面R5較佳爲非球面。 此外,較佳為採用以下結構:第三透鏡L3的物體側 的透鏡面R5的中心部呈凸面(具有正的屈光度),在中心部 和有效直徑周邊部之間具有正的屈光度比中心部強的區 域。 1〇 上述「透鏡面R5的中心部呈凸面,在中心部和有效 ^徑周邊部之間具有i的屈光度比中心部強的結構(以下 還稱爲透鏡面R5的結構例)」如下的結構。 即,將中心部呈凸面(具有正的屈光度)的透鏡面R5的 有j直徑上的某點χ5Α的法線H5A和光軸Z1相交的點設 15爲父點P5A,將連接點X5A和交點P5A的線段X5A-P5A 的長度設爲透鏡面R5的點X5A的曲率半徑的絕對值。如 此設定時,為一在中心部和有效直徑周邊部之間具有曲率 半徑的絕對值比中心部小的區域的結構。 第二透鏡L3的物體側的透鏡面R5的中心部呈凸面’ 2〇有效直徑周邊部的正的屈光度比中心部強也可。 上述「透鏡面R5的中心部呈凸面,有效直徑周邊部 的正的屈光度比中心部強的結構」是如下的結構。 即,將中心部呈凸面(具有正的屈光度)的透鏡面R5的 有放直彳二周邊σ卩上的點Χ5的法線H5和光軸Z1相交的點 26 M355391 设爲交點P5 ’將連接點X5和交點P5的線段X5-P5的長 度設爲透鏡面R5的點X5的曲率半徑的絕對值。將透鏡面 R5和光軸Z1的交點設爲中心部C5。如此設定時,上述透 鏡面R5的結構例是透鏡面R5在光軸z 1上(中心部C5)呈 5凸面(具有正的屈光度),透鏡面R5的中心部C5的曲率中 〜E5及上述交點P5兩者均比中心部匚5更位於成像側, 且線段X5 —P5的長度(透鏡面R5的點X5的曲率半徑R5x 的絕對值)比透鏡面R5的中心部C5的曲率半徑R5c的絕 對值小。 10 如上所述’第三透鏡的物體側的透鏡面的中心部呈凸 面,在中心部和有效直徑周邊部具有正的屈光度比中心部 強的區域,或第三透鏡的物體側的透鏡面的中心部呈凸 面,且在該有效直徑周邊部使正的屈光度比中心部強,因 此能在取長的後截距距離的同時良好地補正像面彎曲。 15 第三透鏡L3的物體侧的透鏡面R5可以構成爲:中心 部呈凸面(具有正的屈光度),在中心部和有效直徑周邊部 之間具有正的屈光度比中心部強的區域,在有效直徑周邊 部使正的屈光度比中心部弱。 第三透鏡L3的成像側的透鏡面R6較佳為做成非球 20 面。 第二透鏡L3的成像側的透鏡面R6較佳為中心部呈凹 面’在有效直彳空周邊部使其負的屈光度比中心部強。 27 M355391 即’較佳為該透鏡面R6的有效直徑周邊部的曲率半 佐的絕對值比透鏡面R6的中心部上的曲率半徑的絕對值 小 〇 如此第二透鏡L3的成像側的透鏡面R6的中心部呈凹 5面’在該有效直徑周邊部與中心部相比而使其負的屈光度 增強’因此可以良好地補正像面彎曲和慧形像差。 將弟二透鏡L3的物體側的透鏡面R5的有效直徑周邊 X5的曲率半徑設爲R5x時’該曲率半徑R5x的絕對值 (IX5-P5I)較佳為在中心部C5的曲率半徑R5c的絕對值的 10 0·4倍到1.5倍之間。 透過將曲率半徑R5x的絕對值設爲曲率半徑R5c的絕 對值的0.4倍到1 ‘5倍之間,可以良好地補正倍率色像差。 關於有關第四透鏡的構成因素的限定: 第四透鏡L4的成像側的透鏡面R9較佳爲非球面。 15 較佳為第四透鏡L4的成像側的透鏡面R9的中心部呈 凸面’在有效直徑周邊部的正的屈光度比中心部弱。 上述「透鏡面R9的中心部呈凸面,有效直徑周邊部 的正的屈光度比中心部弱的結構(以下還稱爲透鏡面R9的 結構例)」是如下述的結構。 即’將中心部呈凸面(具有正的屈光度)的透鏡面R9的 有效直徑周邊部上的點X9上的法線H9和光軸zi相交的 點設爲交點P9,將連接點X9和交點P9的線段X9_P9的 長度没爲透鏡面R9的點X9的曲率半徑的絕對值,並將透 鏡面R9和光軸Z1的交點設爲中心部C9 ;如此設定時, 28 M355391 上述透鏡面R9的結構例如下:透鏡面R9在光軸ζι上(中 心部C9)呈凸面(具有正的屈光度),透鏡面R9的中心部 的曲率中心E9及上述交點p9兩者均比中心部C9更位於 成像側,且線段X9 — P9的長度(透鏡面R9的點χ9的曲率 5半徑R9x的絕對值)比透鏡面R9的中心部C9的曲率半徑 R9c的絕對值大。 如上述,將透鏡面R9做成中心部C9呈凸面,在有效 直徑周邊部使正的屈光度比中心部C9弱,因此可以良好 地補正像面彎曲。 10 關於有關第五透鏡的構成因素的限定: 第五透鏡L5的物體側的透鏡面請較佳爲非球面。 第五透鏡L5的物體側的透鏡面R1〇較佳為其中心部 呈凹面(具有負的屈光度),在有效直徑端使負的屈光度比 中心增強。 15 上述「透鏡面R1G的中心部呈凹面,有效直徑周邊部 的負的屈光度比中心部強的結構(以下還稱爲透鏡面ri〇 的結構例)」為如下的結構。 P將中〜邓呈凹面(具有負的屈光度)的透鏡面R1〇 的有效直徑周邊部上的點χι〇的法線H1〇和光軸ζι相交 2〇的點設爲交點PIO,將連接點XI〇和交點ρι〇的線段 X10-P1G的長度作爲透鏡面㈣的點χΐ()的曲率半徑的絕 對值’並將透鏡面R10和光軸Z1的交點設爲中心部ci〇; 如此設定時,上述透鏡面R1〇的結構例是:透鏡面ri〇在 光軸Z1上(中心部cl〇)呈凹面(具有負的屈光度卜透鏡面 29 M35539110 15 as shown in Fig. 2, the center portion of the lens surface is convex and has a positive refractive power. The positive refractive power of the peripheral portion of the effective diameter is smaller than that of the central portion (hereinafter, also referred to as a configuration example of the lens surface R3). The point at which the normal line H3 of the point X3 on the effective diameter peripheral portion of the lens surface R3 having the convex portion on the center portion intersects with the optical axis Z1 is defined as the intersection point p3, and the length of the line segment χ3_ρ3 of the connection point X3 and the intersection point P3 is taken as the lens surface. The absolute value of the radius of curvature of the magic point X3. The intersection of the lens surface R3 and the optical axis 设为 is set as the center portion C3. In the case of setting as described above, the configuration of the lens surface R3 is such that the lens surface R3 has a convex surface (having a positive refracting power) on the optical axis Z1 (the central portion C3), and the center of curvature of the central portion C3 of the lens surface R3 is £3 and the above-mentioned intersection point. Both of P3 are located on the imaging side more than the central portion C3, and the length of the line segment χ3 - p3 (the absolute value of the radius of curvature R3x of the point X3 of the lens surface R3) is larger than the absolute value of the radius of curvature R3C of the central portion C3 of the lens surface R3. . In the figure, a circle Sp1 having a length of a line segment X3-P3 centered on the intersection point P3 and a circle Sp2 having a radius of curvature center radius R3c centered on the curvature center E3 are shown. The reason why the value of the radius of curvature is expressed by an absolute value is to understand the magnitude relationship of the radius of curvature. In the same description of the lens surface to be described later other than the lens surface R3, the illustration of the symbols used in the above description is omitted. The reason why the magnitude of the radius of curvature is expressed by an absolute value in the above-described "delta" is the same as described above. 23 M355391 "The lens surface on the object side of the second lens has a positive refracting power at the center portion and a negative refracting power (concave surface) at the peripheral portion of the effective diameter" as follows: The point E3 ratio of the center of curvature of the center portion C3 of the lens surface R3 The center portion C3 which is the intersection of the lens surface R3 and the optical axis Z1 is located on the image side, and the point P3 indicating that the center of curvature of the point X3 at the peripheral portion of the effective diameter on the lens surface R3 is 5 is located on the object side than the center portion C3. As described above, the central portion of the lens surface R3 on the object side of the second lens L2 has a convex surface such that the positive refractive power of the peripheral portion of the effective diameter is weaker than the central portion or the peripheral portion of the effective diameter is concave, so that the wide angle 10 can be maintained. At the same time, it corrects the curvature of the image surface. The lens surface R4 on the imaging side of the second lens L2 is preferably made aspherical. The lens surface R4 on the imaging side of the second lens L2 preferably has a concave portion (having a negative refracting power) at the center portion. The negative refractive power is weaker than the central portion at the peripheral portion of the effective diameter. The "the center portion of the lens surface R4 has a concave surface, and the negative refractive power of the effective diameter peripheral portion # is weaker than the central portion (hereinafter, also referred to as a configuration example of the lens surface R4)" is as follows. 2〇, that is, the lens surface R4 whose center portion is concave (having a negative refracting power) is < t straight; the point H2 at which the normal line H4 of the point χ4 on the peripheral portion of L intersects with the optical axis z 1 is = point P4 The length of the line segment χ4_ρ4 connecting the point χ4 and the intersection point p4 is taken as the absolute value of the radius of curvature of the point χ4 of the lens surface R4. Further, the intersection of the lens surface R4 and the optical axis Z1 is defined as the center portion C4. In this configuration, the lens surface R4 has a configuration in which the lens surface R4 has a concave surface (having a negative refracting power) on the optical axis Z1 (center 24 M355391 portion C4), a curvature center E4 of the central portion C4 of the lens surface R4, and the above Intersection? 4 both are located on the imaging side more than the central portion Q, and the length of the line segments X4 - P4 (the absolute value of the curvature half feR4x of the point X4 of the lens surface R4) is larger than the absolute value of the meander diameter R4c of the central portion c4 of the lens ^4 . As described above, the central portion of the lens® R4 on the imaging side of the second lens has a concave surface 'having a negative diopter at its effective diameter peripheral portion which is weaker than the central portion', so that the light passing through the periphery of the second lens is not sharply The ground bends and converges, so the distortion can be corrected well. When the radius of curvature of the effective diameter peripheral portion X3 of the lens surface R3 on the object side of the second lens L2 is R3x, the absolute value (1X3 - P3丨) of the curvature radius is preferably the radius of curvature of the center portion C3. The absolute value is 1.5 times or more. By setting the absolute value of the radius of curvature R3x to the radius of curvature R3c to be equal to or greater than the value of i. 5 times or more, it is possible to satisfactorily correct the field curvature while making the wide angle easier. Φ When the radius of curvature of the effective diameter peripheral portion X4 of the imaging surface R4 of the second lens L2 is R4x, the absolute value of the curvature radius R4x (|X4 - P4|) is preferably the curvature of the central portion C4. The absolute value of the radius R4c is more than 150 times 20 times. By setting the absolute value of the radius of curvature R4x to 1.5 times or more of the absolute value of the radius of curvature r3c, the distortion can be satisfactorily corrected. Regarding the limitation of the constituent elements of the third lens: 25 M355391 The second lens L3 has a positive refracting power and a medium q of the transmissive surface R5 on the object side.卩 is convex. With this setting, the curvature of field can be corrected well. The third lens can have a negative refracting power. The lens surface R5 on the object side of the third lens L3 is preferably aspherical. Further, it is preferable to adopt a configuration in which the central portion of the lens surface R5 on the object side of the third lens L3 has a convex surface (having a positive refracting power), and a positive refracting power between the central portion and the effective diameter peripheral portion is stronger than the central portion. Area. In the above-mentioned structure, the center portion of the lens surface R5 is convex, and the refracting power of i is stronger than the center portion (hereinafter, also referred to as a configuration example of the lens surface R5) between the center portion and the effective peripheral portion. . In other words, the point at which the normal line H5A of the lens surface R5 having the convex portion (having a positive refracting power) having a certain point χ5 of the j diameter intersects the optical axis Z1 is 15 as the parent point P5A, and the connection point X5A and the intersection point P5A are formed. The length of the line segment X5A-P5A is set to the absolute value of the radius of curvature of the point X5A of the lens surface R5. When this is set, it is a structure in which the absolute value of the curvature radius is smaller than the central portion between the center portion and the effective diameter peripheral portion. The central portion of the lens surface R5 on the object side of the second lens L3 has a convex surface. 2 The positive refractive power of the peripheral portion of the effective diameter may be stronger than the central portion. The "the center portion of the lens surface R5 is convex, and the positive refractive power of the peripheral portion of the effective diameter is stronger than the central portion" is as follows. That is, the point R M35391 of the lens surface R5 having the convex portion (having a positive refracting power) having the convex surface (having a positive refracting power) having the normal line H5 of the point Χ5 on the 彳2 circumference σ卩 and the optical axis Z1 intersecting is set as the intersection point P5′ The length of the line segment X5-P5 of X5 and the intersection point P5 is set to the absolute value of the radius of curvature of the point X5 of the lens surface R5. The intersection of the lens surface R5 and the optical axis Z1 is defined as the center portion C5. In this configuration, the lens surface R5 has a configuration in which the lens surface R5 has a convex surface (having a positive refractive power) on the optical axis z 1 (center portion C5), and the curvature of the central portion C5 of the lens surface R5 is equal to E5 and the above. Both of the intersection points P5 are located on the imaging side more than the center portion 匚5, and the length of the line segments X5 - P5 (the absolute value of the radius of curvature R5x of the point X5 of the lens surface R5) is larger than the radius of curvature R5c of the central portion C5 of the lens surface R5. The absolute value is small. 10 As described above, the central portion of the lens surface on the object side of the third lens has a convex surface, and the central portion and the effective diameter peripheral portion have a region where the positive refractive power is stronger than the central portion, or the lens surface of the object side of the third lens Since the center portion has a convex surface and the positive refractive power is stronger than the central portion at the peripheral portion of the effective diameter, the curvature of field can be satisfactorily corrected while taking the long back intercept distance. The lens surface R5 on the object side of the third lens L3 may be configured such that the central portion has a convex surface (having a positive refracting power), and a region having a positive refracting power between the central portion and the effective diameter peripheral portion is stronger than the central portion, and is effective The peripheral portion of the diameter makes the positive diopter weaker than the central portion. The lens surface R6 on the imaging side of the third lens L3 is preferably made to be an aspherical surface. The lens surface R6 on the imaging side of the second lens L3 preferably has a concave portion at the center portion. The effective diopter peripheral portion has a negative refracting power stronger than the central portion. 27 M355391 That is, it is preferable that the absolute value of the curvature half of the effective diameter peripheral portion of the lens surface R6 is smaller than the absolute value of the curvature radius at the central portion of the lens surface R6, and thus the lens side of the imaging side of the second lens L3 The center portion of R6 has a concave surface 5, and the negative refractive power of the effective diameter peripheral portion is increased as compared with the central portion. Therefore, the field curvature and the coma aberration can be satisfactorily corrected. When the radius of curvature of the effective diameter periphery X5 of the lens surface R5 on the object side of the second lens L3 is R5x, the absolute value (IX5 - P5I) of the curvature radius R5x is preferably the absolute radius of curvature R5c of the center portion C5. The value is between 10.4 and 1.5 times. By setting the absolute value of the radius of curvature R5x to be 0.4 times to 1 '5 times the absolute value of the radius of curvature R5c, the chromatic aberration of magnification can be satisfactorily corrected. Regarding the limitation of the constituent elements of the fourth lens: The lens surface R9 on the imaging side of the fourth lens L4 is preferably aspherical. It is preferable that the central portion of the lens surface R9 on the imaging side of the fourth lens L4 has a convex surface. The positive refractive power at the peripheral portion of the effective diameter is weaker than the central portion. The above-mentioned "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 a configuration example of the lens surface R9)" is as follows. That is, the point at which the normal line H9 at the point X9 on the effective diameter peripheral portion of the lens surface R9 having the convex portion (having a positive refracting power) intersects with the optical axis zi is defined as the intersection point P9, and the connection point X9 and the intersection point P9 are The length of the line segment X9_P9 is not the absolute value of the radius of curvature of the point X9 of the lens surface R9, and the intersection of the lens surface R9 and the optical axis Z1 is the center portion C9; when so set, the structure of the lens surface R9 of 28 M355391 is as follows: The lens surface R9 has a convex surface (having a positive refracting power) on the optical axis ( (the central portion C9), and both the center of curvature E9 of the central portion of the lens surface R9 and the above-mentioned intersection point p9 are located on the imaging side more than the central portion C9, and the line segment The length of X9 - P9 (the curvature of the point χ 9 of the lens surface R9 5 the absolute value of the radius R9x) is larger than the absolute value of the curvature radius R9c of the center portion C9 of the lens surface R9. As described above, the lens surface R9 has a convex portion at the center portion C9, and the positive refractive power is weaker than the central portion C9 at the effective diameter peripheral portion, so that the field curvature can be satisfactorily corrected. 10 Regarding the limitation of the constituent elements of the fifth lens: The lens surface on the object side of the fifth lens L5 is preferably an aspherical surface. The lens side R1 of the object side of the fifth lens L5 preferably has a concave portion (having a negative refracting power) at its center portion, and a negative refracting power is enhanced at the effective diameter end with respect to the center. In the above-mentioned "the lens portion R1G, the central portion of the lens surface R1G has a concave surface, and the negative refractive power of the peripheral portion of the effective diameter is stronger than the central portion (hereinafter also referred to as a configuration example of the lens surface ri ))" is as follows. P points the intersection of the normal line H1 χ of the point χ 〇 on the effective diameter of the lens surface R1 中 of the concave surface (having a negative refracting power) and the optical axis ζ 〇 at the intersection point PIO, and the connection point XI The length of the line segment X10-P1G of the 〇 and the intersection point ρι〇 is taken as the absolute value of the radius of curvature of the point χΐ() of the lens surface (4) and the intersection of the lens surface R10 and the optical axis Z1 is the center portion ci〇; A configuration example of the lens surface R1〇 is that the lens surface ri〇 is concave on the optical axis Z1 (center portion cl〇) (having a negative refractive power lens surface 29 M355391)

Rio的中心部CIO的曲率中心E10及上述交點pl0兩者均 比中心部C10更位於物體側,且線段χι〇 一 ρι〇的長度(透 鏡面R10的點Χίο上的曲率半徑R1〇x的絕對值)小於透鏡 面R10的中心部C10的曲率半徑R1〇c的絕對值。 5 第五透鏡L5的物體側的透鏡面R1〇的中心部呈凸面 (具有正的屈光度)’在有效直徑端具有負的屈光度。 上述「透鏡面R10的中心部呈凸面,在有效直徑周邊 部具有負的屈光度的結構」是如下結構。 即,將中心部呈凸面(具有正的屈光度)的透鏡面Ri〇 10的有效直徑周邊部上的點Χίο的法線H10和光軸Z1相交 的點設爲交點P10,將連接點X10和交點P10的線段 X10-P10的長度設爲透鏡面R10的點乂10上的曲率半徑的 絕對值,且將透鏡面R10和光軸Z1的交點設爲中心部 C10;如此設定時,「透鏡面R10的中心部呈凸面有效直 徑周邊部具有負的屈光度的結構」是透鏡面Rl〇在光軸幻 上(中心部C10)呈凸面(具有正的屈光度),透鏡面Ri〇的中 心部C10的曲率中心E10比中心部C10更位於物體側,上 述交點P10比中心部C 10更位於成像側。 如上所述’將第五透鏡L5的物體側的透鏡面R1 〇做 20成中心部呈凹面(具有負的屈光度)、有效直徑周邊部的負 的屈光度大於中心部,或者中心部呈凸面且有效直徑周邊 部呈凹面,因此可良好地補正像面彎曲。 第五透鏡L5的成像側的透鏡面R11較佳為做成非球 面。 30 M355391 第五透鏡L5的成像側的透鏡面R11較佳為中心部呈 凸面(具有正的屈光度),有效直徑周邊部的正的屈光度小 於中心部。 上述「透鏡面Rl 1的中心部呈凸面,有效直徑周邊部 的正的屈光度小於中心部的結構(下面’還稱爲透鏡面R J J 的結構例)」為如下的結構。 15 20 即,將中心部呈凸面(具有正的屈光度)的透鏡面 的有效直徑周邊部上的點XU的法線H11和光轴Ζι相交 的點設爲交點P11 ’將連接點X11和交點pil的線段 XII P11的長度作爲透鏡面R11的點XII的曲率半徑的絕 對值。將透鏡面R11和光軸ζι的交點設爲中心部。 如此設定時,上述透鏡面R11的結構例為:透鏡面R11在 光轴21上(中心部C11)呈凸面(具有正的屈光度),透鏡面 im的中心部C11的曲率中心E11及上述交點Pu兩者均 比中心部Cli更位於物體側,且線段xu —PU的長度(透 鏡面R11的點XU的曲率半徑_的絕對值)大於透^面 R11的中心部C11中的曲率半徑RUe的絕對值。 如上所述第五透鏡L5的成像側的透鏡面汉11的 心部呈凸面(具有正的屈光声、,产计士 ^ + J出尤厪)’在其有效直徑周邊部使正 的屈光度小於中心部,因此能夠良好地補正球面像差。 關於有關第六透鏡的構成因素的限定: 第六透鏡L6的物體你丨的、丞 巧體倒的透鏡面R12較佳爲非球面。 31 M355391 /、透鏡L6的物體側的透鏡面R12的中心 4呈凹面(具有倉的 貝的屈光度),在有效直徑周邊部使負的屈 光度比中心減小。 上述透鏡面R12的中心部呈凹面,有效直徑周邊部 5的負的屈光度小於φ、、α / 又】於中、部的結構(以下還稱爲透鏡面R12 的結構例)」是如下的結構。 P將中呈凹面(具有負的屈光度)的透鏡面R12 的有效直徑周邊部上的點X12的法線H12和光軸Z1相交 的點設爲交點P12,將連接,點χΐ2和交點pi2的線段 1〇 X12-P12的長度作爲透鏡面R12的點χΐ2的曲率半徑的絕 對值,並將透鏡面R12和光軸Z1的交點設爲中心部cn 如此設定時,上述透鏡面R12的結構例為:透鏡面心在 光軸U上(中心部C12)呈凹面(具有負的屈光度),透鏡面 R12的中心部Ci2的曲率中心E12及上述交點pi2兩者均 15比中心部C12更位於物體側,且線段χΐ2—pi2的長产(透 鏡面R12的點X12的曲率半徑R12X的絕對值)大於透鏡面 R12的中心部C12的曲率半徑R12C的絕對值。 如此形成第六透鏡的物體側的透鏡面Rl2的中心部呈 凹面(具有負的屈光度)、且有效直徑周邊部的負的屈光产 2〇比中心減小的形狀’因此可以與色像差—同良好地:正^ 面彎'曲。 第六透鏡L6的成像側的透鏡R13較佳爲非〗求@ 32 M355391 且較佳為第六透鏡L6的成像側的透鏡面R13的中心 部呈凸面(具有正的屈光度)’有效直徑周邊部的正的屈光 度比中心部減小。 上述「透鏡面R13的中心部呈凸面’在有效直徑周邊 5部的正的屈光度小於中心部的結構(以下,還稱爲透鏡面 R13的結構例)」為如下述結構。 即’將中心部呈凸面(具有正的屈光度)的透鏡面 的有效直徑周邊部上的點X13的法線H13和光軸zi相交 的點設爲交點P13,將連接點X13和交點pi3的線段 ίο X13_P13的長度設爲透鏡面R13的點Χ13的曲率半徑的絕 對值’並將透鏡面R13和光轴Ζ1的交點設爲中心部c 13 ; 如此設定時’上述透鏡面R13的結構例為:透鏡面R13在 光軸Z1上(中心部C13)呈凸面(具有正的屈光度),透鏡面 R13的中心部C13的曲率中心e13及上述交點p13兩者均 15比中心部C13更位於物體側,且線段Χ13_ρΐ3的長度(透 鏡面R13的點χΐ3的曲率半徑R13x的絕對值)比透鏡面 R13的中心部CI3的曲率半徑R13C的絕對值大。 如此將第六透鏡的成像側的透鏡面R 1 3做成中心部呈 凸面、且在有效直徑周邊部正的屈光度比中心部減小的形 20狀,或者透鏡面R13的中心部呈凸面、且有效直徑周邊部 呈凹面(具有負的屈光度),可以良好地補正球面像差及慧 形像差。 ^ 將第六透鏡L6的物體側的透鏡面R12的有效直徑周 邊部X12的曲率半徑設爲R12x時,該曲率半徑R12x的絕 33 M355391 對值(|X12 — P12|)較佳為中心部C12的曲率半徑幻以的絕 對值的1.5倍以上;將曲率半徑R12x的絕對值設爲曲率半 徑R12c的絕對值的1.5倍以上可以與色像差一同良好地補 正像面彎曲。 5 若將第六透鏡L6的成像側的透鏡面R13的有效直徑 周邊部X13上的曲率半徑設爲R13x時,該曲率半徑Ri3x 的絕對值(|X13 —P13|)較佳為中心部C13的曲率半徑R13c 的絕對值的兩倍以上;將曲率半徑R丨3χ的絕對值設爲曲 率半徑R13c的絕對值的兩倍以上,可以良好地補正球面 10 像差和慧形像差。 關於其他構成因素的限定: 本創作的攝影透鏡若設理想像高爲2fxtan(e/2)時,畸 變較佳為在± 10%以内。 若穿過第一透鏡L1或第二透鏡L2的有效直徑外的光 15束成爲雜散光而到達成像面,則成爲重影,因此在透鏡l 1 和第二透鏡L2上的有效直徑以外的區域設置作爲遮光單 元的遮光板Ski、Sk2來遮斷雜散光。 该遮光單元可以採用將對光進行遮斷的板構件配置在 透鏡上的有效直徑外的區域’或者採用將由遮光塗料構成 20的被膜塗敷在透鏡上的有效直徑以外的區域的結構。 遮光單元可以根據需要配置在第一透鏡L1和第二透 鏡L2之間’遮光單元也可以配置在第二透鏡[2至第六透 鏡L6上的有效直徑外的區域、或這些透鏡之間。 34 M355391 第二透鏡到第六透鏡的各透鏡的材質較佳為塑膠(樹 脂材料)。 作爲從第二透鏡到第六透鏡的透鏡的材質,可以使用 將尺寸小於光的波長的粒子混合在樹脂材料中的奈米複合 5 材料。 第一透鏡至第六透鏡的各透鏡不限於由折射率一定的 材料形成的情況,可在六片透鏡中的任一個以上使用折射 率分佈型透鏡。Both the center of curvature E10 of the central portion CIO of Rio and the above-mentioned intersection point pl0 are located on the object side more than the center portion C10, and the length of the line segment χι〇-ρι〇 (the absolute radius of curvature R1〇x on the point Χίο of the lens surface R10) The value is smaller than the absolute value of the radius of curvature R1〇c of the central portion C10 of the lens surface R10. 5 The central portion of the lens surface R1 of the object side of the fifth lens L5 has a convex surface (having a positive refracting power)' having a negative refracting power at the effective diameter end. The above-mentioned "structure in which the central portion of the lens surface R10 has a convex surface and has a negative refractive power in the peripheral portion of the effective diameter" has the following structure. In other words, a point at which the normal line H10 of the point Χίο on the effective diameter peripheral portion of the lens surface Ri 〇 10 having the convex portion (having a positive refracting power) intersects with the optical axis Z1 is defined as the intersection point P10, and the connection point X10 and the intersection point P10 are formed. The length of the line segment X10-P10 is the absolute value of the radius of curvature at the point 乂10 of the lens surface R10, and the intersection of the lens surface R10 and the optical axis Z1 is the center portion C10; when set, "the center of the lens surface R10" The structure in which the peripheral portion of the convex effective diameter has a negative refracting power" is a convex surface (having a positive refracting power) of the lens surface R1 幻 on the optical axis (the central portion C10), and the center of curvature E10 of the central portion C10 of the lens surface Ri 〇 The intersection point P10 is located on the object side more than the center portion C10, and the intersection point P10 is located on the imaging side more than the center portion C10. As described above, 'the lens surface R1 of the object side of the fifth lens L5 is 20, the center portion is concave (having a negative refracting power), the negative diopter of the effective diameter peripheral portion is larger than the center portion, or the center portion is convex and effective. The peripheral portion of the diameter is concave, so that the curvature of field can be corrected well. The lens surface R11 on the imaging side of the fifth lens L5 is preferably made aspherical. 30 M355391 The lens surface R11 on the imaging side of the fifth lens L5 preferably has a convex portion (having a positive refracting power) at the center portion, and a positive refracting power at the peripheral portion of the effective diameter is smaller than the center portion. The above-mentioned "the central portion of the lens surface R1 1 has a convex surface, and the positive refractive power of the peripheral portion of the effective diameter is smaller than that of the central portion (the configuration of the lower surface is also referred to as the lens surface R J J)" has the following structure. 15 20 That is, the point at which the normal line H11 of the point XU on the peripheral portion of the effective diameter of the lens surface having the convex portion (having a positive refracting power) intersects with the optical axis 设为 is set as the intersection point P11 'to connect the point X11 and the intersection point pil The length of the line segment XII P11 is the absolute value of the radius of curvature of the point XII of the lens surface R11. The intersection of the lens surface R11 and the optical axis 设为 is referred to as a central portion. In this configuration, the lens surface R11 has a configuration in which the lens surface R11 has a convex surface (having a positive refracting power) on the optical axis 21 (the central portion C11), a curvature center E11 of the central portion C11 of the lens surface im, and the above-mentioned intersection point Pu. Both are located on the object side more than the center portion Cli, and the length of the line segment xu - PU (the absolute value of the radius of curvature _ of the point XU of the lens surface R11) is larger than the absolute radius of curvature RUe in the central portion C11 of the transparent surface R11 value. As described above, the core portion of the lens surface 11 of the imaging side of the fifth lens L5 has a convex surface (having a positive refractive power, and the product is made to have a positive refractive power smaller than the center in the peripheral portion of the effective diameter thereof). Therefore, it is possible to correct the spherical aberration well. Regarding the limitation of the constituent elements of the sixth lens: The object of the sixth lens L6 is preferably aspherical, and the lens surface R12 which is inverted is preferably aspherical. 31 M355391 /, the center 4 of the lens surface R12 on the object side of the lens L6 has a concave surface (having the diopter of the chamber), and the negative refractive power is reduced from the center at the peripheral portion of the effective diameter. The central portion of the lens surface R12 has a concave surface, and the negative refractive power of the effective diameter peripheral portion 5 is smaller than φ, and α / is also a structure of the middle portion (hereinafter also referred to as a configuration example of the lens surface R12). . P is a point at which the normal line H12 of the point X12 on the peripheral portion of the effective diameter of the lens surface R12 having a concave surface (having a negative refracting power) intersects with the optical axis Z1 as the intersection point P12, which will be connected, the point χΐ2 and the line segment 1 of the intersection point pi2 When the length of the 〇X12-P12 is the absolute value of the radius of curvature of the point χΐ2 of the lens surface R12, and the intersection of the lens surface R12 and the optical axis Z1 is set as the center portion cn, the configuration of the lens surface R12 is as follows: The core has a concave surface (having a negative refracting power) on the optical axis U (the central portion C12), and both the center of curvature E12 of the central portion Ci2 of the lens surface R12 and the above-described intersection point pi2 are located on the object side more than the central portion C12, and the line segment The long production of χΐ2-pi2 (the absolute value of the radius of curvature R12X of the point X12 of the lens surface R12) is larger than the absolute value of the radius of curvature R12C of the central portion C12 of the lens surface R12. The central portion of the lens surface R12 on the object side of the sixth lens thus formed has a concave surface (having a negative refracting power), and the negative refractive power of the peripheral portion of the effective diameter is reduced to a shape smaller than the center'. Therefore, chromatic aberration can be performed. - Same as good: positive ^ face bend 'curve. The lens R13 on the imaging side of the sixth lens L6 is preferably non-required @32 M355391 and preferably the central portion of the lens surface R13 on the imaging side of the sixth lens L6 is convex (having a positive refracting power)' effective diameter peripheral portion The positive diopter is reduced compared to the central portion. The configuration in which the central portion of the lens surface R13 is convex is a structure in which the positive refractive power of the peripheral portion 5 is smaller than the central portion (hereinafter, also referred to as a configuration of the lens surface R13) is as follows. That is, a point at which the normal line H13 of the point X13 on the effective diameter peripheral portion of the lens surface having the convex portion (having a positive refracting power) intersects with the optical axis zi is defined as the intersection point P13, and the line segment connecting the point X13 and the intersection point pi3 is ίο The length of X13_P13 is set to the absolute value of the radius of curvature of the point Χ13 of the lens surface R13', and the intersection of the lens surface R13 and the optical axis Ζ1 is the center portion c13. When so set, the configuration of the lens surface R13 is as follows: R13 has a convex surface (having a positive refracting power) on the optical axis Z1 (the central portion C13), and both the curvature center e13 of the central portion C13 of the lens surface R13 and the above-described intersection point p13 are located more on the object side than the central portion C13, and the line segment The length of Χ13_ρΐ3 (the absolute value of the radius of curvature R13x of the point χΐ3 of the lens surface R13) is larger than the absolute value of the radius of curvature R13C of the central portion CI3 of the lens surface R13. In this manner, the lens surface R 1 3 on the imaging side of the sixth lens has a convex shape in which the central portion is convex, and the positive refractive power at the peripheral portion of the effective diameter is smaller than the central portion, or the central portion of the lens surface R13 is convex. Moreover, the peripheral portion of the effective diameter has a concave surface (having a negative refracting power), and the spherical aberration and the coma aberration can be satisfactorily corrected. When the radius of curvature of the effective diameter peripheral portion X12 of the lens surface R12 on the object side of the sixth lens L6 is R12x, the absolute value of the radius of curvature R12x is preferably the center portion C12 (|X12 - P12|). The absolute value of the curvature radius R12x is 1.5 times or more of the absolute value of the radius of curvature R1, and the curvature of the curvature radius R12c is 1.5 times or more of the absolute value of the curvature radius R12c. 5 When the radius of curvature of the effective diameter peripheral portion X13 of the imaging surface R13 of the sixth lens L6 is R13x, the absolute value of the curvature radius Ri3x (|X13 - P13|) is preferably the center portion C13. The absolute value of the radius of curvature R13c is twice or more; and the absolute value of the radius of curvature R丨3χ is set to be twice or more the absolute value of the radius of curvature R13c, so that the spherical aberration 10 and the coma aberration can be satisfactorily corrected. Restriction on other constituent factors: When the ideal image height of the photographic lens of this creation is 2fxtan(e/2), the distortion is preferably within ±10%. If the light 15 passing through the effective diameter of the first lens L1 or the second lens L2 becomes stray light and reaches the image plane, it becomes a ghost, and thus an area other than the effective diameter on the lens 11 and the second lens L2 The visors Ski, Sk2, which are the light shielding units, are provided to block stray light. The light-shielding unit may be configured such that a plate member that blocks light is disposed in a region outside the effective diameter of the lens or a region in which the film of the light-shielding paint composition 20 is applied to a region other than the effective diameter of the lens. The light shielding unit may be disposed between the first lens L1 and the second lens L2 as needed. The light shielding unit may be disposed in a region outside the effective diameter of the second lens [2 to the sixth lens L6, or between the lenses. 34 M355391 The material of each lens of the second lens to the sixth lens is preferably plastic (resin material). As the material of the lens from the second lens to the sixth lens, a nanocomposite 5 material in which particles having a size smaller than the wavelength of light are mixed in a resin material can be used. The lenses of the first to sixth lenses are not limited to those formed of a material having a constant refractive index, and a refractive index distribution type lens may be used in any one of the six lenses.

第二透鏡至第六透鏡的各透鏡不限於單面或雙面爲非 球面的情況,亦可為衍射光學面,即’可以在從第二透鏡 到第六透鏡的任一個以上的透鏡面形成衍射光學元件。 將第二透鏡至第六透鏡做成各透鏡的至少一個透鏡面 爲非球面,可以在維持廣角的同時,良好地補正球面像差 (也稱球差)、像面彎曲(也稱場曲)' 慧形像差(也稱慧差)及 丄、較佳為將第一透鏡做成玻璃透鏡,將從第二透鏡到第 六透鏡做成塑膠透鏡。 20 例如,在車載照相機或監視照相機那樣的嚴格的環境 =時,對第一透鏡的材質要求較高的耐氣候性,因此較 用高耐水性、高财酸性、及高耐藥品性等的材質。 另外’作爲第-透鏡的材質較佳為使用堅硬的材質。 的陶=璃透鏡作爲第一透鏡為佳,亦可以使用由透明 勾瓷構成的透鏡作爲第一透鏡。 35 M355391 透過使第一透鏡的材質爲玻璃,可以做成高耐氣候性 且不易碎的透鏡。 第一透鏡不限於使用玻璃球面透鏡。第一透鏡亦可以 使用單側的透鏡面或兩側的透鏡面做成非球面的玻璃非球 5面透鏡。透過將第一透鏡的透鏡面做成非球面,可以更好 地補正各種像差。 使從第二透鏡到第六透鏡的材質爲塑膠,可以因此準 確地再現非球面的形狀’並可以低價地製作透鏡系統。 從第二透鏡到第六透鏡的各透鏡的兩面是非球面也 10 可。 另外,較佳為上述透鏡系統不使用接合透鏡。透過使 用接合透鏡而可以容易補正色像差,但若使用接合透鏡, 則成爲成本上升的主要原因。透過使用本創作的結構,可 以不使用接合透鏡而製作色像差也被補正的良好性能的透 15 鏡。 <具體的實施例> # 接著,參照圖3至圖15對本創作的實施例1至實施例 4的各攝影透鏡的數值資料等歸納說明。圖3至圖6是實 細例1至實施例4的攝影透鏡的各自的簡要結構的截面 20圖’與圖1、2中的符號一致的圖3至6中的符號示出相互 對應的結構。 圖7至圖10是表示實施例1至實施例4的各攝影透鏡 的基本貝料的圖。在各圖中的左上部(圖中用符號(a)表示) 表不透鏡貝料’上中央部⑽中用符號⑻表示)表示攝影透 36 M355391 透鏡面的形狀(非球面的形狀)的非球面式的各係數。在右The lenses of the second lens to the sixth lens are not limited to the case where the single surface or the double surface is aspherical, and may be a diffractive optical surface, that is, 'may be formed on one or more lens faces from the second lens to the sixth lens. Diffractive optical element. The second lens to the sixth lens are formed such that at least one lens surface of each lens is aspherical, and the spherical aberration (also called spherical aberration) and the curvature of field (also called field curvature) can be satisfactorily corrected while maintaining a wide angle. The coma aberration (also called coma) and 丄, preferably the first lens is made into a glass lens, and the second lens to the sixth lens are made into a plastic lens. 20 For example, in a strict environment such as an in-vehicle camera or a surveillance camera, the material of the first lens is required to have high weather resistance, so that it is made of a material having high water resistance, high acidity, and high chemical resistance. . Further, it is preferable to use a hard material as the material of the first lens. The ceramic lens is preferably used as the first lens, and a lens made of a transparent porcelain may be used as the first lens. 35 M355391 By making the material of the first lens glass, it is possible to make a lens that is highly weather resistant and not fragile. The first lens is not limited to the use of a glass spherical lens. The first lens may also be a non-spherical glass aspherical 5-sided lens using a one-sided lens surface or a lens surface on both sides. By making the lens surface of the first lens aspherical, various aberrations can be better corrected. The material from the second lens to the sixth lens is made of plastic, so that the shape of the aspherical surface can be accurately reproduced, and the lens system can be produced at low cost. Both sides of each of the lenses from the second lens to the sixth lens are aspherical. Further, it is preferable that the above lens system does not use a cemented lens. The chromatic aberration can be easily corrected by using the cemented lens. However, when a cemented lens is used, the cost is increased. By using the structure of the present invention, it is possible to produce a transmissive lens with good performance in which chromatic aberration is corrected without using a cemented lens. <Specific Embodiments># Next, numerical data and the like of the respective photographic lenses of the first to fourth embodiments of the present invention will be collectively described with reference to Figs. 3 to 15 . 3 to 6 are cross-sectional views of the respective schematic structures of the photographic lenses of the first to fourth embodiments, and the symbols in FIGS. 3 to 6 which correspond to the symbols in FIGS. . Fig. 7 to Fig. 10 are views showing basic bead materials of the respective imaging lenses of the first to fourth embodiments. In the upper left part of the figure (indicated by the symbol (a) in the figure), the lens of the upper part (10) is indicated by the symbol (8), and the shape of the lens surface (the shape of the aspherical surface) of the 36 M355391 is shown. The coefficients of the spherical type. On the right

鏡等的光學部件的面號碼以隨著從物體側向成像側依次增 加的第i(i=卜2, 3’ ...)個的面號碼進行表示。在這些透 )個的面號碼進行表示。The face number of the optical member such as the mirror is expressed by the i-th (i = 2, 3' ...) face numbers which are sequentially increased from the object side toward the image side. These face numbers are indicated.

囬現碼U=l4、15)、成像面的面號碼(i=;16)等。透鏡面呈 10非球面’則在面號碼附加*號。The return code U=l4, 15), the face number of the imaging surface (i=; 16), and the like. If the lens surface is 10 aspherical, then the * is appended to the face number.

Ri表不第ι(ι=卜2,3 ’個面的近轴曲率半徑,Di(i -卜2,3,…)表不第i個面和第i+1個面的光軸ζι上的 面間隔。透鏡資料的符號Ri與圖i中的表示透鏡面的符號 Ri(i= 1,2,3,…)對應。 15 各透鏡資料中的Ndj表示隨著從物體側向成像側依次 增加的第j(j= 1’2,3,…)個光學因素對d線(波長587 6nm) 的折射率,vdj表示第j個光學因素對d線的阿貝數。 近軸曲率半徑及面間隔的單位是mm,對近軸曲率半 徑而言’將在物體側凸的情況設爲正,在成像側凸的情況 20設爲負。 各非球面由下述非球面式定義。 [數學式1]The Ri table is not the paraxial radius of curvature of the ι (ι=卜2,3' plane, Di(i - Bu 2,3,...) represents the optical axis of the i-th face and the i+1th face The plane spacing of the lens data corresponds to the symbol Ri (i = 1, 2, 3, ...) representing the lens surface in Fig. i. 15 Ndj in each lens data is sequentially followed from the side of the object toward the imaging side. Increased refractive index of the jth (j=1'2,3,...) optical factor for the d-line (wavelength 587 6nm), vdj represents the Abbe number of the jth optical factor to the d-line. The unit of the surface interval is mm, and for the paraxial radius of curvature, 'the case where the object is convex is set to be positive, and the case where the image is convex is set to be negative. Each aspherical surface is defined by the following aspherical surface. Formula 1]

37 M355391 z :非球面深度(從高度γ的非球面上的點下垂到非球 面頂點相切的且與光軸垂直的平面的垂線的長度); Υ:高度(從光軸的距離 R:近軸曲率半徑(mm);37 M355391 z : aspherical depth (length of the perpendicular from the point on the aspheric surface of height γ to the plane tangential to the aspherical vertex and perpendicular to the optical axis); Υ: height (distance from the optical axis R: near Axis radius of curvature (mm);

Ai :非球面深度(i=3至20); K :圓錐常數。 圖7至圖1〇的各圖中的上中央部的簡要規格中表示以 下的各值。 表不如下各值:F值:Fno,半視場角:ω,像高:m, 後截距距離:Bf(空氣換算),第一透鏡的物體側的透鏡面 到成像面的距離:L,透鏡整個系統的焦距(第一透鏡至第 八透鏡的合成焦距):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:以, 15 20 第五透鏡的焦距:f5’帛六透鏡的焦距:f6。並表示如下 各值.第一透鏡、第二透鏡的合成焦距:fl2,第五透鏡、 第六透鏡的合成焦距:f56 ’第一透鏡、第二透鏡、第三透 鏡的合成焦距:f123’第四透鏡、第五透鏡、第六透鏡的 合成焦距:f456。 上述距離L的值如上述,後截距距離量按空氣換算長 度表示的值,與上述距離L值中的除後截距距離量以外的 按實際長度表示的值相加後的值。 圖7至圖10的各圖中的左下 __ 町左下邛不出表示各非球面Ri(i 4···)的非球面式的各係數 K、A3、A4、A5...的值。 38 M355391 圖11是實施例1至4中所表示的條件式(丨)至(9)的各 參數的值的圖。 圖12至15是表示實施例1至4的各攝影透鏡的各種 像差的圖。圖12至圖15分別表示各實施例的每個攝影透 5鏡對d線(波長587.6腿)、F線(波長486.lnm)、c線(波長 656.3nm)的像差。 就畸變的圖而言,利用透鏡整個系統的焦距f、及視 場角Θ(變數處理,〇$θ$ω),將理想像高設爲2fxtan(e/2), 表示距其的偏移量。 10 構成爲旋轉對稱的形狀的透鏡的透鏡面的有效直徑周 邊部,通常成爲距該透鏡的光軸的距離爲一定的呈圓形狀 的區域。呈该形狀的區域成爲透鏡面上的有效區域的邊緣 部。 根據表示實施例1至4的基本的資料及各種像差的圖 15等可知,若採用本創作的廣角的攝影透鏡,則實現六片透 鏡的每一個形狀或材質的最佳化,因此可以在提高光學性 能的同時實現小型化。 本創作不限於上述實施方式及各實施例,可以進行各 種變形實施。例如,各透鏡成分的曲率半徑、面間隔及折 20射率的值等不限於上述各圖中所示的數值,亦可取其他值。 本創作的攝影透鏡在第二透鏡以後大多使用非球面, 可以在將透鏡系統小型化的同時以低價進行製作,而且可 以更好地補正像面彎曲、畸變等的像差。 39 M355391 【圖式簡單說明】 圖1是表示本創作攝影透鏡的示意圖。 圖對圖1附加用於說明的輔助線等的圖。 5 施例1的攝影透鏡的簡要結構的截面圖。 ==不:施例2的攝影透鏡的簡要結構的截面圖。 不貝施例3的攝影透鏡的簡要結構的載面圖。 =疋表不貫施例4的攝影透鏡的簡要結構的截面圖。 圖7是表示實施例1的攝影透鏡的基本資料的圖。 圖8是表示實施例2的攝影透鏡的基本資料的圖。 1。圖9'表示實施例3的攝影透鏡的基本資料的圖。 圖10是表不實施例4的攝影透鏡的基本資料的圖。 圖11是按每個實施例表示與條件式⑴至(9)中的各參數對 應的值的圖》 圖疋表示實施例1的攝影透鏡的各種像差的圖。 15圖13是表示實施例2的攝影透鏡的各種像差的圖。 圖14疋表示實施例3的攝影透鏡的各種像差的圖。 圖15疋表不實施例4的攝影透鏡的各種像差的圖。 【主要元件符號說明】 2 0攝影透鏡 C3透鏡面R3和光軸的交點 E3透鏡面R3的曲率中心 Jk受光面 1 〇攝影元件 2 ω全視角 Cgl光學部件 H3點X3上的法線 M355391 L1第一透鏡 L3第三透鏡 L5第五透鏡 R3c點C3上的曲率半徑 S k 1遮光板Ai : aspheric depth (i = 3 to 20); K: conic constant. The following values are shown in the brief specifications of the upper center portion in each of Figs. 7 to 1B. The values are not as follows: F value: Fno, half angle of view: ω, image height: m, back intercept distance: Bf (air conversion), distance from the lens side of the object side of the first lens to the imaging surface: L The focal length of the entire system of the lens (combined focal length of the first lens to the eighth lens): f' focal length of the first lens: fl, focal length of the second lens: f2 'focal length of the third lens: f3, focal length of the fourth lens :Yes, 15 20 The focal length of the fifth lens: the focal length of the f5'帛6 lens: f6. And the following values are expressed. The combined focal length of the first lens and the second lens: fl2, the combined focal length of the fifth lens and the sixth lens: f56 'The combined focal length of the first lens, the second lens, and the third lens: f123' The combined focal length of the four lens, the fifth lens, and the sixth lens: f456. The value of the distance L is as described above, and the value of the back-intercept distance is expressed by the air-converted length, and the value obtained by adding the value of the actual length other than the post-intercept distance amount of the distance L value. In the lower left __ of each of Figs. 7 to 10, the values of the coefficients K, A3, A4, A5, ... of the aspherical surface of each aspherical surface Ri(i 4 ···) are not shown. 38 M355391 Fig. 11 is a view showing values of respective parameters of the conditional expressions (丨) to (9) shown in the first to fourth embodiments. Figs. 12 to 15 are views showing various aberrations of the respective imaging lenses of the first to fourth embodiments. Fig. 12 through Fig. 15 show aberrations of each of the imaging mirrors of the respective embodiments for the d line (wavelength 587.6 legs), the F line (wavelength 486.1 nm), and the c line (wavelength 656.3 nm). In the case of the distortion map, the focal length f of the entire system of the lens and the angle of view Θ (variable processing, 〇$θ$ω) are used to set the ideal image height to 2fxtan(e/2), indicating the offset from it. the amount. The effective diameter peripheral portion of the lens surface of the lens having a rotationally symmetrical shape is generally a circularly shaped region having a constant distance from the optical axis of the lens. The region having this shape becomes the edge portion of the effective region on the lens surface. According to the basic data showing the first to fourth embodiments and the various aberrations, FIG. 15 and the like, it is possible to optimize each shape or material of the six lenses by using the wide-angle imaging lens of the present invention. Miniaturize while improving optical performance. The present invention is not limited to the above embodiments and the respective embodiments, and various modifications can be made. For example, the values of the radius of curvature, the interplanar spacing, and the refractive index of each lens component are not limited to the numerical values shown in the above figures, and other values may be employed. The photographic lens of the present invention uses an aspherical surface mostly after the second lens, and can be manufactured at a low cost while miniaturizing the lens system, and can better correct aberrations such as curvature of field and distortion. 39 M355391 [Simple description of the drawing] Fig. 1 is a schematic view showing the photographic lens of the present invention. FIG. 1 is a view in which an auxiliary line or the like for explanation is added. 5 is a cross-sectional view showing a schematic configuration of a photographic lens of Embodiment 1. == No: A cross-sectional view of a schematic structure of the photographic lens of Example 2. A plan view of a schematic structure of a photographic lens of Example 3. = A cross-sectional view showing a schematic structure of the photographic lens of Example 4. Fig. 7 is a view showing the basic information of the imaging lens of the first embodiment. Fig. 8 is a view showing the basic information of the imaging lens of the second embodiment. 1. Fig. 9' is a view showing the basic information of the photographing lens of the third embodiment. Fig. 10 is a view showing the basic information of the photographing lens of the fourth embodiment. Fig. 11 is a view showing values corresponding to respective parameters in the conditional expressions (1) to (9) for each of the embodiments. Fig. 11 is a view showing various aberrations of the imaging lens of the first embodiment. Fig. 13 is a view showing various aberrations of the imaging lens of the second embodiment. Fig. 14A is a view showing various aberrations of the imaging lens of the third embodiment. Fig. 15 is a view showing various aberrations of the photographic lens of the fourth embodiment. [Description of main component symbols] 20 Photographic lens C3 Lens surface R3 and intersection of optical axis E3 Curvature center of lens surface R3 Jk light receiving surface 1 〇 Photographic element 2 ω Full viewing angle Cgl Optical component H3 Normal line on point X3 M355391 L1 first Lens L3 third lens L5 fifth lens R3c radius of curvature at point C3 S k 1 mask

St孔徑光攔 L2第二透鏡 L4第四透鏡 L6第六透鏡 R3 z點X3上的曲率半徑St aperture stop L2 second lens L4 fourth lens L6 sixth lens R3 radius of curvature on point x3

Sk2遮光板 VI入射光線Sk2 visor VI incident light

|X3-P3|線段X3-P3的長度 Z1光軸 P3點X3上的法線與光轴相交的點 R1第一透鏡物體側的透鏡面 R2第一透鏡成像侧的透鏡面 R3第二透鏡物體側的透鏡面 R4第二透鏡成像側的透鏡面 R5第三透鏡物體側的透鏡面 R6第三透鏡成像側的透鏡面 R7孔徑光欄的孔徑部 R8第四透鏡物體側的透鏡面 R9第四透鏡成像側的透鏡面 R10第五透鏡物體側的透鏡面 R11第五透鏡成像側的透鏡面 R12第六透鏡物體側的透鏡面 R13第六透鏡成像側的透鏡面 R14光學部件的物體側的表面 41 M355391 R15光學部件的成像側的表面 R16被攝體的物體的像成像的成像面|X3-P3|The length of the line segment X3-P3 Z1 The optical axis P3 The point at which the normal on the X3 intersects the optical axis R1 The lens surface R1 on the first lens object side The lens surface R3 on the imaging side of the first lens The second lens object Side lens surface R4 Second lens imaging side lens surface R5 Third lens object side lens surface R6 Third lens imaging side lens surface R7 Aperture diaphragm aperture portion R8 Fourth lens object side lens surface R9 fourth Lens surface R11 on the lens imaging side L1 on the fifth lens object side L1 on the imaging side of the fifth lens L12 on the imaging side of the sixth lens R13 on the side of the sixth lens image side Surface on the image side of the sixth lens on the image side R14 Surface on the object side of the optical component 41 M355391 R15 optical component imaging side surface R16 object image of the object imaged imaging surface

Spl以P3爲圓心、以線段X3-P3的長度為半徑的圓Spl is a circle with a radius of P3 as the center and a length of the line segment X3-P3.

Sp2以E3爲圓心、以R3c的絕對值為半徑值的圓。 X3透鏡面R3的有效直徑周邊部上的點Sp2 is a circle with E3 as the center and a radius of R3c as the radius. a point on the peripheral portion of the effective diameter of the X3 lens surface R3

4242

Claims (1)

M355391 六、申請專利範圍: 1. 一種攝影透鏡,其從物體側起依序包括:具有負的 屈光度的第一透鏡、具有負的屈光度的第二透鏡、第二透 鏡、具有正的屈光度的第四透鏡、具有正的屈光度的第五 透鏡、及具有負的屈光度的第六透鏡;上述第二透鏡到第 六透鏡中,其中各透鏡的至少一個透鏡面呈非球面;上述 第三透鏡、及第六透鏡由對d線的阿貝數爲45以下的材料 形成。 2· —種攝影透鏡,其從物體側起依序包括: 第-透鏡,其具有負的屈光度,是凹面朝向成像 彎月透鏡; 第二透鏡’其至少成像側的透鏡面呈非球面,該透鏡 面的中心部呈凹面且有效直徑周邊部的負的屈光度比上: 中心部弱; 15 第三透鏡 第四透鏡 球面; 第五透鏡 球面;以及 2〇 第六透鏡 其至少一個透鏡面呈非球面; 其具有正的屈光度,至少__個透鏡面呈非 其具有正的屈光度,至少一個透鏡面呈非 其具有負的屈光度’至少-個透鏡面呈非 球面。 3.如申請專利範圍第U 2項所述的 中,光欄配置在上述第三透鏡和第四透鏡之間。 - 43 M355391 項所述的攝影透鏡,其 ,物體側的透鏡面的中 4.如申请專利範圍第1或2 中’上述第三透鏡具有正的屈光度 心部呈凸面。 5·如申請專利範圍第1或2項所述的攝影透鏡,| 5中,滿足以下的條件式(1) : ^ 2.〇<f56/f<5.5……⑴; 式中, f ’上述攝影透鏡整個系統的焦距; f56.上述第五透鏡和第六透鏡的合成焦距。 1〇 6.如申請專利範圍第1或2項所述的攝影透鏡,其 中,更滿足以下的條件式(2): 2.5< (D4+D5)/f< 5.5......(2); 式中, f:上述攝影透鏡整個系統的焦距; 15 D4 :上述第二透鏡和第三透鏡之間的空氣間隔; D5:上述第三透鏡的中心厚度。 7.如申請專利範圍第丨或2項所述的攝影透鏡,其 中’更滿足以下的條件式(3): 4.0< f3/f< 9.0......(3); 20 〇 ’ f:上述攝影透鏡整個系統的焦距; f3 :上述第三透鏡的焦距。 44 M355391 8. 如申請專利範圍第1 4 2項所迷的攝影透鐘,其 中,上述第二透鏡的成像側的透鏡面,該透鏡面的中心部 呈凹面且有效直徑周邊部的倉 、的出光度比上述中心部弱。 9. 如申請專利範圍第!或 .,.+, ^ 飞2項所述的攝影透鏡,其 中’上述苐一透鏡的物體侧的读於; W边鏡面,該透鏡面的中心部 呈凸面且有效直徑周邊部的正 < I J止的屈先度比上述中心部弱、 或該透鏡面的中心部呈凸面Η亡 1凸面且有效直徑周邊部具有負的屈 光度。 、 10. 如申請專利範圍第1 兄2項所述的攝影透鏡,其 中,上述第三透鏡的物體側的透鏡面,該透鏡面的中心部 呈凸面’在有效直㈣具有正的屈光度比上述中心部強的 區域。 士 U.如申請專利範圍第1或2項所述的攝影透鏡,其 中’上述第五透鏡的成像側的透鏡面,該透鏡面的中心部 15呈凸面且有效直徑周邊部的正的屈光度比上述中心部弱。 12·如申請專利範圍第i或2項所述的攝影透鏡,其 中’上迷第六透鏡的物體側的透鏡面,該透鏡面的中心部 呈凹面且有效直徑周邊部的負的屈光度比上述中心部弱。 13·如申請專利範圍第!或2項所述的攝影透鏡,其 20中,上述第六透鏡的成像側的透鏡面,該透鏡面的中心部 呈凸面且有效直徑周邊部的正的屈光度比上述中心部弱。 A如申請專利範圍第1或2項所述的攝影透鏡,其 中’更滿足以下的條件式(4): 11 < L/f< 18......(4); 45 M355391 式中, f:上述攝影透鏡整個系統的焦距; L :從上述第一透鏡的物體側的透鏡面到成像面的距 離。 15_—種攝影裝置,其具有如申請專利範圍第1至14 項中中任一項所述的攝影透鏡、以及將該攝影透鏡所形成 的光學像變換成電信號的攝影元件。M355391 VI. Patent Application Range: 1. A photographic lens comprising, in order from the object side, a first lens having a negative refracting power, a second lens having a negative refracting power, a second lens, and a first diopter having a positive diopter. a four lens, a fifth lens having a positive refracting power, and a sixth lens having a negative refracting power; wherein the at least one lens surface of each of the second lens to the sixth lens is aspherical; the third lens, and The sixth lens is formed of a material having an Abbe number of 45 or less for the d line. 2) a photographic lens, which includes, in order from the object side, a first lens having a negative refracting power, a concave surface facing the imaging meniscus lens, and a second lens 'having at least the lens side of the imaging side being aspherical, The central portion of the lens surface is concave and the negative diopter ratio of the effective diameter peripheral portion is: the central portion is weak; 15 the third lens fourth lens spherical surface; the fifth lens spherical surface; and the 2〇 sixth lens having at least one lens surface thereof Spherical surface; it has a positive refracting power, at least __ lens surfaces are not positively refracting, and at least one lens surface is non-having a negative refracting power 'at least one lens surface is aspherical. 3. As described in the U.S. Patent Application Serial No. 2, the light barrier is disposed between the third lens and the fourth lens. The photographic lens of item M355391, wherein the lens surface of the object side is 4. In the first or second aspect of the patent application, the third lens has a positive refracting power and the core portion is convex. 5. In the photographic lens described in claim 1 or 2, in the case of 5, the following conditional expression (1) is satisfied: ^ 2. 〇 <f56/f < 5.5 (1); where f ' The focal length of the entire system of the above photographic lens; f56. The combined focal length of the fifth lens and the sixth lens. The photographic lens according to claim 1 or 2, wherein the following conditional expression (2) is more satisfied: 2.5 < (D4 + D5) / f < 5.5 ... ( 2); where f is the focal length of the entire system of the above photographic lens; 15 D4: the air gap between the second lens and the third lens; D5: the center thickness of the third lens. 7. The photographic lens of claim 2 or 2, wherein 'more satisfies the following conditional expression (3): 4.0<f3/f< 9.0 (3); 20 〇' f: the focal length of the entire system of the above photographic lens; f3: the focal length of the above third lens. 44 M355391. The photographic lens disclosed in claim 1, wherein the lens surface on the imaging side of the second lens has a concave portion and a peripheral portion of the effective diameter peripheral portion. The light output is weaker than the above center portion. 9. If you apply for a patent scope! Or .., ^, the photographic lens according to item 2, wherein 'the object side of the first lens is read; the W side mirror surface, the central portion of the lens surface is convex and the positive diameter peripheral portion is positive < The yoke of the IJ is weaker than the center portion, or the center portion of the lens surface is convexly convex and has a convex surface, and the effective diameter peripheral portion has a negative refracting power. 10. The photographic lens of claim 1, wherein the lens surface of the third lens has a convex surface at a central portion of the lens surface, and the positive diopter has a positive diopter ratio. A strong area in the center. The photographic lens according to claim 1 or 2, wherein the lens surface of the imaging side of the fifth lens, the central portion 15 of the lens surface has a convex surface and a positive diopter ratio of the peripheral portion of the effective diameter The above center is weak. 12. The photographic lens of claim ii, wherein the lens surface of the object side of the sixth lens is concave, the central portion of the lens surface is concave and the negative diopter of the effective diameter peripheral portion is The center is weak. 13·If you apply for a patent scope! In the photographic lens according to the above aspect, the lens surface on the imaging side of the sixth lens has a convex surface at a central portion of the lens surface, and a positive refractive power of the peripheral portion of the effective diameter is weaker than the central portion. A photographic lens according to claim 1 or 2, wherein 'more satisfies the following conditional expression (4): 11 < L/f < 18 (4); 45 M355391 f: the focal length of the entire system of the above photographic lens; L: the distance from the lens side of the object side of the first lens to the imaging surface. A photographic lens according to any one of claims 1 to 14, and a photographic element for converting an optical image formed by the photographic lens into an electrical signal. 4646
TW97219419U 2008-05-27 2008-10-30 Photographing lens and the photographing device thereof TWM355391U (en)

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