CN100541258C - Imaging optics - Google Patents
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- CN100541258C CN100541258C CNB200610104300XA CN200610104300A CN100541258C CN 100541258 C CN100541258 C CN 100541258C CN B200610104300X A CNB200610104300X A CN B200610104300XA CN 200610104300 A CN200610104300 A CN 200610104300A CN 100541258 C CN100541258 C CN 100541258C
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Abstract
Description
技术领域 technical field
本发明涉及一种光学镜组,特别是指一种应用于照相手机的小型化成像用光学镜组。The invention relates to an optical mirror group, in particular to a miniaturized imaging optical mirror group applied to a camera phone.
背景技术 Background technique
最近几年来,随着照相手机的兴起,摄影镜头的厚度逐渐缩小,而一般数字相机的感光组件不外乎是CMOS或CCD两种,由于半导体制程技术的进步,感光组件的画素大小由早期的7.4um减少至目前的1.75um,这使得小型化摄影镜头的需求更为殷切。In recent years, with the rise of camera phones, the thickness of photographic lenses has gradually shrunk, and the photosensitive components of general digital cameras are nothing more than CMOS or CCD. Due to the advancement of semiconductor process technology, the pixel size of photosensitive components has changed from the early 7.4um has been reduced to the current 1.75um, which makes the demand for miniaturized photographic lenses more ardent.
目前的手机镜头,为考虑像差的补正,多采用三枚式镜片结构,其中最普遍的为正负正Triplet型式,但是,当镜头的高度由5mm缩小至3mm时,成像系统体积缩小,使得三枚镜片欲置入此空间变得困难,而镜片厚度也必须缩小,使得以塑料射出成型制作的镜片其材质的均匀度不良。The current mobile phone lens, in order to consider the correction of aberration, mostly adopts three lens structures, the most common of which is the positive and negative triplet type. However, when the height of the lens is reduced from 5mm to 3mm, the volume of the imaging system is reduced, making the It becomes difficult to place the three lenses in this space, and the thickness of the lenses must also be reduced, so that the material uniformity of the lenses produced by plastic injection molding is poor.
有鉴于此,特提出本发明。In view of this, the present invention is proposed.
发明内容 Contents of the invention
为解决光学系小型化的问题,本发明提供一种由二枚透镜构成的光学镜组,其要旨如下:In order to solve the problem of miniaturization of the optical system, the present invention provides an optical mirror group composed of two lenses, the gist of which is as follows:
一成像用光学镜组,由二片具屈折力的塑料镜片构成,由物侧至像侧,首先为一具正屈折力的第一透镜,其前、后表面都为凸面,且其前表面、后表面皆为非球面,再者为一具负屈折力的第二透镜,其前表面为凹面,后表面为凸面,且其前表面、后表面皆为非球面。成像用光学镜组中并设置有一光圈,位于第一透镜之前,用于控制光学系的亮度,并且可使光线在感光组件上的入射角有效减少。An optical lens group for imaging, consisting of two plastic lenses with refractive power, from the object side to the image side, firstly a first lens with positive refractive power, its front and rear surfaces are convex, and its front surface , the rear surface are all aspherical, and the second lens with negative refractive power, the front surface is concave, the rear surface is convex, and both the front surface and the rear surface are aspheric. An aperture is arranged in the optical lens group for imaging, which is located in front of the first lens, and is used to control the brightness of the optical system, and can effectively reduce the incident angle of light on the photosensitive component.
成像用光学镜组中,具正屈折力的第一透镜,其折射率为N1,具负屈折力的第二透镜,其折射率为N2,两者满足下记关系:In the optical lens group for imaging, the first lens with positive refractive power has a refractive index of N1, and the second lens with negative refractive power has a refractive index of N2, and the two satisfy the following relationship:
1.6>N1>1.51.6>N1>1.5
N2>1.55N2>1.55
则可使成像用光学镜组获得有效的屈折力,更进一步来看,第一透镜折射率N1及第二透镜折射率N2,需满足下记关系:Then the optical lens group for imaging can obtain effective refractive power. Further, the refractive index N1 of the first lens and the refractive index N2 of the second lens need to satisfy the following relationship:
N1>1.54N1>1.54
N2<1.65N2<1.65
在成像用光学镜组中,系统的屈折力主要由第一透镜提供,而具负屈折力的第二透镜其功能为平衡及修正系统所产生的各项像差,但若其折射率超过此上限值,将使得系统的高度增加,因此透过上述各镜片折射率的适当配置,将使得成像用光学镜组在屈折力与像差的修正中取得平衡。In the optical lens group for imaging, the refractive power of the system is mainly provided by the first lens, and the function of the second lens with negative refractive power is to balance and correct various aberrations generated by the system, but if its refractive index exceeds this The upper limit value will increase the height of the system. Therefore, through the proper configuration of the refractive index of the above-mentioned lenses, the imaging optical lens group will achieve a balance in the correction of refractive power and aberration.
成像用光学镜组中,具正屈折力的第一透镜其焦距为f1,具负屈折力的第二透镜其焦距为f2,系统焦距为f,其满足下记关系:In the optical lens group for imaging, the focal length of the first lens with positive refractive power is f1, the focal length of the second lens with negative refractive power is f2, and the focal length of the system is f, which satisfy the following relationship:
f/f1>2.0f/f1>2.0
|f/f2|<1.0|f/f2|<1.0
加大正第一透镜的屈折力,可以缩短光学镜组的高度,而且可以使光线在感光组件上的入射角有效减少,而具负屈折力的第二透镜,负屈折力来自于前表面,其功用为修正系统所产生的像差,但若其屈折力过大,将造成光线在感光组件上的入射角不易压缩,同时,后表面的非球面也将过强而使得制造上较为困难。若考量高阶像差的压制,以及欲使成像用光学镜组产生足够的后焦,则第一透镜的焦距f1与系统焦距f,需满足下记关系:Increasing the refractive power of the positive first lens can shorten the height of the optical lens group, and can effectively reduce the incident angle of light on the photosensitive component, while the second lens with negative refractive power comes from the front surface, and its The function is to correct the aberration produced by the system, but if the refractive power is too large, the incident angle of the light on the photosensitive element will not be easily compressed. At the same time, the aspheric surface on the rear surface will be too strong, making it difficult to manufacture. Considering the suppression of high-order aberrations and the optical lens group for imaging to produce sufficient back focus, the focal length f1 of the first lens and the focal length f of the system must satisfy the following relationship:
f/f1<2.5f/f1<2.5
为了有效修正系统产生的色差,控制第一透镜的色散系数(Abbe Number)V1及第二透镜的色散系数(Abbe Number)V2,必须满足下记关系式:In order to effectively correct the chromatic aberration generated by the system, to control the Abbe Number V1 of the first lens and the Abbe Number V2 of the second lens, the following relationship must be satisfied:
V1>50V1>50
V2<40V2<40
为了有效缩小光线入射感光组件的角度,第一透镜前表面曲率半径R1,第一透镜后表面曲率半径R2,必须满足以下关系式:In order to effectively reduce the angle of light incident on the photosensitive component, the curvature radius R1 of the front surface of the first lens and the curvature radius R2 of the rear surface of the first lens must satisfy the following relationship:
1.4<(R1+R2)/(R1-R2)<1.551.4<(R1+R2)/(R1-R2)<1.55
藉由前置光圈的配置,以及第一透镜后表面提供强大的正屈折力,将使得成像用光学镜组的出射瞳(Exit Pupil)远离成像面,因此,光线离开第二透镜后表面后,将以接近垂直入射的方式入射在感光组件上,此即为像侧的Telecentric特性,此特性对于时下固态感光组件的感光能力是极为重要的,将使得感光组件的感光敏感度提高,减少系统产生暗角的可能性。上述关系式称为透镜的形状因子,当其数值低于下限值,R2变得相对较小,将使得系统产生过大的像差而难以控制,另一方面,当其数值高于上限值时,R2变得相对较大,第一透镜后表面的屈折力变小,使得光圈必须前移才能缩小光线入射在感光组件上的角度,而这将会和成像用光学镜组小型化的目标相违背。With the configuration of the front aperture and the strong positive refractive power provided by the rear surface of the first lens, the exit pupil (Exit Pupil) of the imaging optical lens group will be far away from the imaging surface. Therefore, after the light leaves the rear surface of the second lens, It will be incident on the photosensitive component in a manner close to vertical incidence, which is the Telecentric characteristic of the image side. This feature is extremely important for the photosensitive ability of the current solid-state photosensitive component, which will increase the photosensitive sensitivity of the photosensitive component and reduce system generation. Possibility of dark corners. The above relationship is called the shape factor of the lens. When its value is lower than the lower limit, R2 becomes relatively small, which will cause excessive aberration in the system and is difficult to control. On the other hand, when its value is higher than the upper limit When the value of R2 becomes relatively large, the refractive power of the rear surface of the first lens becomes smaller, so that the aperture must be moved forward to reduce the angle of light incident on the photosensitive component, and this will be consistent with the miniaturization of the optical lens group for imaging Goals contradicted.
此外,成像用光学镜组小型化的趋势,以及系统需涵盖广泛的视角,使得焦距变得很短,在这种情况下,镜片的曲率半径以及镜片的大小都变得很小,以传统玻璃研磨的方法将难以制造出上述的镜片,因此,第一透镜及第二透镜都采用塑料材质,藉由射出成型的方式制作镜片,可以用较低廉的成本生产高精密度的镜片;并于各镜面上设置非球面,非球面可以容易制作成球面以外的形状,获得较多的控制变量,用以消减像差,进而缩减镜片使用的数目。In addition, the trend of miniaturization of optical lens groups for imaging and the need for the system to cover a wide range of viewing angles make the focal length very short. In this case, the radius of curvature of the lens and the size of the lens become very small. The method of grinding will be difficult to manufacture the above-mentioned lenses. Therefore, both the first lens and the second lens are made of plastic materials, and the lenses are made by injection molding, which can produce high-precision lenses at a relatively low cost; and in each An aspherical surface is set on the mirror surface, and the aspheric surface can be easily made into a shape other than a spherical surface, and more control variables are obtained to reduce aberrations, thereby reducing the number of lenses used.
下面结合附图对本发明的具体实施方式作进一步详细的说明。The specific implementation manners of the present invention will be further described in detail below in conjunction with the accompanying drawings.
附图说明 Description of drawings
图1第一实施例光学系统示意图;Fig. 1 schematic diagram of the optical system of the first embodiment;
图2第一实施例的像差曲线图;The aberration curve diagram of the first embodiment of Fig. 2;
图3第二实施例光学系统示意图;The schematic diagram of the optical system of the second embodiment of Fig. 3;
图4第二实施例的像差曲线图;The aberration curve diagram of the second embodiment of Fig. 4;
【表】【surface】
表1第一实施例结构数据;Table 1 first embodiment structural data;
表2第一实施例非球面数据;Table 2 first embodiment aspherical data;
表3第二实施例结构数据;Table 3 second embodiment structural data;
表4第二实施例非球面数据;Table 4 second embodiment aspherical data;
表5本发明相关方程式的数值资料;The numerical data of table 5 correlation equation of the present invention;
【主要组件符号说明】[Description of main component symbols]
光圈10,第一透镜20,前表面21,后表面22,第二透镜30,前表面31,后表面32,红外线滤除滤光片40,感光组件50,第一透镜折射率N1,第二透镜折射率N2,第一透镜焦距f1,第二透镜焦距f2,成像用光学镜组系统焦距f,第一透镜色散系数V1(Abbe number),第二透镜色散系数V2(Abbe number),第一透镜前表面曲率半径R1,第一透镜后表面曲率半径R2
具体实施方式 Detailed ways
本发明第一实施例请参阅图1,第一实施例的像差曲线请参阅图2。第一实施例的主要构造为:一成像用光学镜组,由二片具屈折力的塑料镜片构成,由物侧至像侧依序配置一具正屈折力的第一透镜20,其前表面21及后表面22皆为凸面,且其前表面20、后表面21皆为非球面,一具负屈折力的第二透镜31,其前表面31为凹面,后表面32为凸面,且其前表面20、后表面21皆为非球面,另在第二透镜30与感光组件50中间设置有一红外线滤除滤光片(IR Cut Filter)40,其不影响系统的焦距。成像用光学镜组中并设置有一光圈10,位于第一透镜20之前,用于控制光学系的亮度;Please refer to FIG. 1 for the first embodiment of the present invention, and please refer to FIG. 2 for the aberration curve of the first embodiment. The main structure of the first embodiment is: an optical lens group for imaging, which is composed of two plastic lenses with refractive power, and a
成像用光学镜组中,具正屈折力的第一透镜20,其折射率N1=1.543,具负屈折力的第二透镜30,其折射率N2=1.583;In the optical lens group for imaging, the
具正屈折力的第一透镜20其焦距为f1,具负屈折力的第二透镜30其焦距为f2,系统焦距为f,其关系为:f/f1=2.21、|f/f2|=0.81;The focal length of the
第一透镜20的色散系数(Abbe Number)V1=60.3,第二透镜30的色散系数(AbbeNumber)V2=30.2;The dispersion coefficient (Abbe Number) V1=60.3 of the
第一透镜20前表面21曲率半径R1,第一透镜20后表面22曲率半径R2,其关系为:The radius of curvature R1 of the
(R1+R2)/(R1-R2)=1.451;(R1+R2)/(R1-R2)=1.451;
第一透镜20前表面21曲率半径R1=2.18647mm;The radius of curvature R1 of the
第一透镜20及第二透镜30都采用塑料材质,藉由射出成型的方式制作镜片,并于各镜面上设置非球面,非球面曲线的方程式表示如下:Both the
X(Y)=(Y2/R)/(1+sqrt(1-(1+k)*(Y/R)2))+A4*Y4+A6*Y6+…X(Y)=(Y 2 /R)/(1+sqrt(1-(1+k)*(Y/R) 2 ))+A 4 *Y 4 +A 6 *Y 6 +…
其中:in:
X:镜片的截面距离X: the cross-sectional distance of the lens
Y:非球面曲线上的点距离光轴的高度Y: the height of the point on the aspheric curve from the optical axis
k:锥面系数k: cone coefficient
A4、A6、……:4阶、6阶、……的非球面系数。A 4 , A 6 , ...: 4th order, 6th order, ... aspheric coefficients.
第一实施例详细的结构数据如同表一所示,其非球面数据如同表二所示。The detailed structural data of the first embodiment are shown in Table 1, and the aspheric data are shown in Table 2.
本发明第二实施例请参阅图3,第二实施例之像差曲线请参阅第4图。第二实施例的主要构造为:一成像用光学镜组,由二片具屈折力的塑料镜片构成,由物侧至像侧依序配置一具正屈折力的第一透镜20,其前表面21及后表面22皆为凸面,且其前表面20、后表面21皆为非球面,一具负屈折力的第二透镜30,其前表面31为凹面,后表面32为凸面,且其前表面20、后表面21皆为非球面,另在第二透镜30与感光组件50中间设置有一红外线滤除滤光片(IR Cut Filter)40,其不影响系统的焦距。成像用光学镜组中并设置有一光圈10,位于第一透镜20之前,用于控制光学系的亮度;Please refer to FIG. 3 for the second embodiment of the present invention, and please refer to FIG. 4 for the aberration curve of the second embodiment. The main structure of the second embodiment is: an optical lens group for imaging, which is composed of two plastic lenses with refractive power, and a
成像用光学镜组中,具正屈折力的第一透镜20,其折射率N1=1.543,具负屈折力的第二透镜30,其折射率N2=1.583;In the optical lens group for imaging, the
具正屈折力的第一透镜20其焦距为f1,具负屈折力的第二透镜30其焦距为f2,系统焦距为f,其关系为:f/f1=2.34、|f/f2|=0.95;The focal length of the
第一透镜20的色散系数(Abbe Number)V1=60.3,第二透镜30的色散系数(AbbeNumber)V2=30.2;The dispersion coefficient (Abbe Number) V1=60.3 of the
第一透镜20前表面21曲率半径R1,第一透镜20后表面22曲率半径R2,其关系为:The radius of curvature R1 of the
(R1+R2)/(R1-R2)=1.466;(R1+R2)/(R1-R2)=1.466;
第一透镜20前表面21曲率半径R1=1.78647mm;The radius of curvature R1 of the
第一透镜20及第二透镜30皆采用塑料材质,藉由射出成型的方式制作镜片,并于各镜面上设置非球面,非球面曲线方程式的表示同第一实施例的型式;Both the
第二实施例详细的结构数据如同表三所示,其非球面数据如同表四所示。The detailed structure data of the second embodiment is shown in Table 3, and the aspheric surface data is shown in Table 4.
在此先行述明,表一至表四所示为成像用光学镜组实施例的不同数值变化表,然本发明各个实施例的数值变化都属实验所得,即使使用不同数值,相同结构的产品仍应属于本发明的保护范畴。表五为各个实施例对应本发明相关方程式的数值资料。It is stated in advance that Tables 1 to 4 show the different numerical changes of the embodiments of the optical lens group for imaging. However, the numerical changes of the various embodiments of the present invention are all experimental results. Even if different numerical values are used, the products of the same structure are still the same. Should belong to the protection category of the present invention. Table 5 is the numerical data corresponding to the relevant equations of the present invention for each embodiment.
综上所述,本发明成像用光学镜组,藉此透镜结构、排列方式与镜片配置可以有效缩小镜组体积,更能同时获得较高的解像力。To sum up, the optical lens group for imaging of the present invention can effectively reduce the volume of the lens group through the lens structure, arrangement and lens configuration, and can obtain higher resolution at the same time.
表1Table 1
表3table 3
表5table 5
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US20040036983A1 (en) * | 2002-05-10 | 2004-02-26 | Noboru Ninomiya | Image pick-up lens |
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