TWI479181B - Optical module - Google Patents

Optical module Download PDF

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TWI479181B
TWI479181B TW101130424A TW101130424A TWI479181B TW I479181 B TWI479181 B TW I479181B TW 101130424 A TW101130424 A TW 101130424A TW 101130424 A TW101130424 A TW 101130424A TW I479181 B TWI479181 B TW I479181B
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lens
optical module
optical
equal
convergence
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TW101130424A
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TW201409065A (en
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Jianhua Wang
Jean-Pierre Lusinchi
Xiaoxiong Qiu
Wanghu Wu
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Ether Precision Inc
Jianhua Wang
Jean-Pierre Lusinchi
Xiaoxiong Qiu
Wanghu Wu
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Description

光學模組Optical module

本發明係有關於一種用於手機以擷取影像之光學模組,特別是有關於一種包括四片透鏡之光學模組。The invention relates to an optical module for capturing images by a mobile phone, in particular to an optical module comprising four lenses.

目前手機的發展趨勢除了厚度愈來愈薄外,對於手機鏡頭解析度的要求也愈來愈高,因此導致手機鏡頭需特別設計才能符合高解析度之要求。鏡頭一般是由一到數片透鏡與光圈經由透鏡固定座固定後組裝而成,對於銷售目標為大量市場之鏡頭,因為每天需生產數以萬計個鏡頭,可以預見的是,其對生產良率之要求幾乎接近百分之一百,所以需特別注意其製造能力。At present, the development trend of mobile phones is getting thinner and thinner, and the requirements for resolution of mobile phone lenses are getting higher and higher. Therefore, mobile phone lenses need to be specially designed to meet the requirements of high resolution. The lens is generally assembled by fixing one to several lenses and apertures through the lens holder. For the lens that sells a large number of markets, because it needs to produce tens of thousands of lenses every day, it is foreseeable that it is good for production. The rate requirement is almost 100%, so special attention must be paid to its manufacturing capabilities.

對於鏡頭設計之限制主要取決於客戶所提出之規格,其中主要的規格包括以下幾種:The restrictions on lens design depend mainly on the specifications proposed by the customer. The main specifications include the following:

有效焦距(Effective Focal Length)Effective Focal Length

有效焦距將決定鏡頭之整體外形尺寸,下文中所提到的有效焦距一詞,將以英文的EFL來代替。The effective focal length will determine the overall dimensions of the lens. The term effective focal length mentioned below will be replaced by the English EFL.

後焦距(Back Focal Length)Back Focal Length

後焦距(BFL)為最靠近影像感測器之透鏡之像側表 面頂點至影像感測器之感測面於光軸上之距離。Back focal length (BFL) is the image side of the lens closest to the image sensor The distance from the vertex to the sensing surface of the image sensor on the optical axis.

收斂(Convergence)Convergence

收斂C等於EFL之倒數,也可以稱為透鏡之屈光力。The convergence C is equal to the reciprocal of the EFL and may also be referred to as the refractive power of the lens.

視角(Field of View)Field of View

EFL值與鏡頭焦平面之影像尺寸大小決定視角之大小,視角一詞,將以英文的FOV來代替。當一直徑等於D之圓形影像,且其影像中心位於光軸與鏡頭焦平面之交點,其FOV值可以下列公式求得:FOV=2.Arctan[D/(2.EFL)]其中Arctan為角度的正切值之反函數。The EFL value and the image size of the focal plane of the lens determine the size of the viewing angle. The term angle of view will be replaced by the English FOV. When a circular image with a diameter equal to D and its image center is at the intersection of the optical axis and the focal plane of the lens, the FOV value can be obtained by the following formula: FOV=2. Arctan[D/(2.EFL)] where Arctan is the inverse of the tangent of the angle.

當影像為矩形且其影像中心點位於光軸與像平面之交叉點時,上述公式中之D值為此矩形影像之對角線長度。When the image is rectangular and its image center point is at the intersection of the optical axis and the image plane, the D value in the above formula is the diagonal length of the rectangular image.

對於影像上任一點位置之定義,一般常見做法不外乎以高度或角度來定義,其中高度指的是影像上任一點至影像中心點之距離,角度指的是影像上任一點與影像中心點所形成之線段所對應之視角角度,兩者都以相對於最大半視角之百分比來表示,記成x% hFOV。For the definition of the position of any point on the image, the common practice is defined by height or angle. The height refers to the distance from any point on the image to the center of the image. The angle refers to any point on the image and the center point of the image. The angle of view corresponding to the line segment, both expressed as a percentage relative to the maximum half angle of view, is recorded as x% hFOV.

在鏡頭設計領域大家都知道,當視角愈大其幾何像差也就愈大,在此條件下,很難設計出一款鏡頭,既具 備高解析度又具備低像散。In the field of lens design, we all know that the larger the angle of view, the larger the geometric aberration. Under this condition, it is difficult to design a lens. High resolution and low astigmatism.

光圈值(Aperture Number)F#Aperture Number F#

鏡頭中的光圈主要用來控制光線進入鏡頭之數量,光圈尺寸與EFL值可決定鏡頭之光圈值,光圈值等於EFL除以光圈直徑,光圈值以F#來表示。The aperture in the lens is mainly used to control the amount of light entering the lens. The aperture size and EFL value determine the aperture value of the lens. The aperture value is equal to EFL divided by the aperture diameter. The aperture value is represented by F#.

當光圈用於控制光線數量進入鏡頭時,光圈通常也被稱做光欄。When the aperture is used to control the amount of light entering the lens, the aperture is often referred to as the diaphragm.

光圈值主要影響到四個重要參數,包括到達影像感測器之光線數量,此光線數量與光圈值平方成反比,景深(DoF),超焦距離(HyF),超焦距離指的是當鏡頭對焦於超焦距離處時,從距離鏡頭二分之一超焦距離處至無窮遠處物體皆能在影像感測器上清晰成像,以及焦深(dof),焦深指的是影像感測器位置相對於鏡頭之誤差值,在誤差值範圍內都不影響影像清晰度。The aperture value mainly affects four important parameters, including the amount of light reaching the image sensor. The amount of light is inversely proportional to the square of the aperture value. Depth of field (DoF), hyperfocal distance (HyF), and hyperfocal distance refer to the lens. When focusing on the hyperfocal distance, the object can be clearly imaged from the image sensor at a distance from the lens to the infinity of the lens, and the depth of focus (dof), the depth of focus refers to the image sensing The error value of the position relative to the lens does not affect the image sharpness within the error value range.

解析度(Resolution)Resolution

解析度是指在某一特定空間頻率所測得的調變轉換函數(MTF),解析度是用來描述鏡頭對於連續交替出現且寬度相同的黑白條狀影像之對比,每一對黑白條狀影像之寬度等於空間頻率之倒數。Resolution is the modulation transfer function (MTF) measured at a particular spatial frequency. The resolution is used to describe the contrast of a lens for consecutive black-and-white strip images of the same width, each pair of black and white strips. The width of the image is equal to the reciprocal of the spatial frequency.

MTF通常以最大可能對比之百分率來表示,對於 一個給定之鏡頭,其MTF介於0%至100%之間,最大的MTF為100%。MTF is usually expressed as a percentage of the maximum possible contrast, for For a given shot, the MTF is between 0% and 100% and the maximum MTF is 100%.

空間頻率被表示成每一毫米中所擁有之線對值,Line Pair Per Millimeters縮寫成lppm。The spatial frequency is expressed as the pair value in each millimeter, and the Line Pair Per Millimeters is abbreviated to lppm.

像差(Aberrations)Aberrations

像差包括幾何像差與色差。Aberrations include geometric aberrations and chromatic aberrations.

幾何像差包括幾何畸變、像散以及影像中不同區域之EFL差值,幾何像差取決於透鏡之曲率和定義透鏡表面凹陷之非球面係數。Geometric aberrations include geometric distortion, astigmatism, and EFL differences in different regions of the image. Geometric aberrations depend on the curvature of the lens and the aspheric coefficients that define the depressions on the lens surface.

色差包括彩色條紋(物體邊緣被與物體邊緣平行的各種不同顏色所圍繞)和色區(例如白色影像於角落處出現粉紅色)。Chromatic aberrations include colored stripes (the edges of the object are surrounded by various colors that are parallel to the edge of the object) and color regions (for example, white images appear pink at the corners).

目標成本(Targeted Costs)Targeted Costs

目標成本主要取決於組成鏡頭的透鏡數量,本發明可經由平衡各透鏡間之收斂來達到降低像差,而不是採用增加透鏡數目來達到降低像差。The target cost mainly depends on the number of lenses constituting the lens, and the present invention can achieve the reduction of the aberration by balancing the convergence between the lenses, instead of increasing the number of lenses to achieve the reduction of the aberration.

更多關於EFL、C、BFL、FOV、MTF以及F#的詳細資料都可以在學術文獻中查到,例如由McGraw Hill公司出版,Warren J Smith所著的Modern Optical Engineer書中即可發現。More details on EFL, C, BFL, FOV, MTF, and F# can be found in the academic literature, such as Modern Optical by Warren J Smith, published by McGraw Hill. It can be found in the Engineer's book.

因為有許多規格的限制,人們可以了解到鏡頭其實是根據一些特別規格而設計,然而,很多時候手機製造商會根據相同的影像感測器,製定出幾款規格稍微不同的鏡頭(EFL、FOV以及MTF等規格略有變化)。有可能設計出一種可多用的鏡頭,使其各種設計參數可在一定的範圍內變動。Because there are many specifications, people can understand that the lens is actually designed according to some special specifications. However, many mobile phone manufacturers will develop several lenses with different specifications (EFL, FOV, etc. according to the same image sensor). Specifications such as MTF have changed slightly). It is possible to design a versatile lens that allows various design parameters to be varied within a certain range.

目前已經有許多專利所描述的鏡頭是由四片透鏡或四組透鏡所組成,例如日本專利JP2003098428、JP2007108770、JP7098430、JP11190820以及美國專利US5367405,其中的限制條件包括使用的透鏡種類、透鏡之焦距以及為了特殊應用而特別設計的非球面表面,皆和本發明不同。There are a number of lenses described in the prior art, which are composed of four lenses or four groups of lenses, such as Japanese Patent No. JP2003098428, JP2007108770, JP7098430, JP11190820, and US Pat. No. 5,367,405, the limitations of which include the type of lens used, the focal length of the lens, and Aspherical surfaces specially designed for special applications are different from the present invention.

本發明提供一種光學模組,從物側至像側包括一第一透鏡、一第二透鏡、一第三透鏡以及一第四透鏡。第一透鏡為一具正屈光力之凹凸透鏡,包括一第一光學表面以及一第二光學表面,第一光學表面為凸面且面向物側。第二透鏡為一具負屈光力之凹凸透鏡,包括一第三光學表面以及一第四光學表面,第三光學表面面向物側。第三透鏡為一具正屈光力之凹凸透鏡,包括一第五 光學表面以及一第六光學表面,第五光學表面為凹面且面向物側,第六光學表面為凸面且面向像側。第四透鏡為一具負屈光力之透鏡,包括一第七光學表面以及一第八光學表面,第七光學表面面向物側。The invention provides an optical module comprising a first lens, a second lens, a third lens and a fourth lens from the object side to the image side. The first lens is a positive refractive power concave-convex lens comprising a first optical surface and a second optical surface, the first optical surface being convex and facing the object side. The second lens is a meniscus lens having a negative refractive power, comprising a third optical surface and a fourth optical surface, the third optical surface facing the object side. The third lens is a positive refractive power convex lens, including a fifth The optical surface and a sixth optical surface, the fifth optical surface being concave and facing the object side, the sixth optical surface being convex and facing the image side. The fourth lens is a lens having a negative refractive power, comprising a seventh optical surface and an eighth optical surface, the seventh optical surface facing the object side.

其中,如果C1為第一透鏡之收斂,C為光學模組之收斂,則1.1 C 1/C 1.35。Wherein, if C1 is the convergence of the first lens and C is the convergence of the optical module, then 1.1 C 1/ C 1.35.

其中,如果C1為第一透鏡之收斂,C2為第二透鏡之收斂,則|C 1/C 2|2。Wherein, if C1 is the convergence of the first lens and C2 is the convergence of the second lens, then | C 1/ C 2| 2.

其中,如果C1為第一透鏡之收斂,C3為第三透鏡之收斂,則0.5 C 1/C 31.1。Wherein, if C1 is the convergence of the first lens and C3 is the convergence of the third lens, then 0.5 C 1/ C 3 1.1.

其中,如果C1為第一透鏡之收斂,Vd1為第一透鏡之阿貝係數,則C1/Vd15.2。Wherein, if C1 is the convergence of the first lens, and Vd1 is the Abbe coefficient of the first lens, then C1/Vd1 5.2.

其中,如果C2為第二透鏡之收斂,Vd2為第二透鏡之阿貝係數,則|C2/Vd2|7。Wherein, if C2 is the convergence of the second lens and Vd2 is the Abbe coefficient of the second lens, then |C2/Vd2| 7.

其中,如果Ci為第i透鏡之收斂,Vdi為第i透鏡之阿貝係數,i=1、2、3、4,則|Σ(Ci/Vdi)|4。Wherein, if Ci is the convergence of the ith lens, Vdi is the Abbe coefficient of the ith lens, i=1, 2, 3, 4, then |Σ(Ci/Vdi)| 4.

其中,當波長為0.555微米、空間頻率為89 lppm時,光學模組中心調變轉換函數(MTF)值大於或等於75%。Wherein, when the wavelength is 0.555 micrometers and the spatial frequency is 89 lppm, the optical modulation center modulation transfer function (MTF) value is greater than or equal to 75%.

其中,當半視角為50%、波長為0.555微米、空間頻率為89 lppm時,光學模組弧矢向與子午向之調變轉換函數(MTF)差值小於8%;當半視角為90%、波長為 0.555微米、空間頻率為89 lppm時,光學模組的弧矢向與子午向之調變轉換函數(MTF)差值小於15%。Wherein, when the half angle of view is 50%, the wavelength is 0.555 micrometer, and the spatial frequency is 89 lppm, the difference between the sagittal direction and the meridional modulation transfer function (MTF) of the optical module is less than 8%; when the half angle of view is 90%, Wavelength is At 0.555 micron and a spatial frequency of 89 lppm, the difference between the sagittal direction and the meridional modulation transfer function (MTF) of the optical module is less than 15%.

其中,當半視角為50%、波長為0.555微米、空間頻率為89 lppm時,光學模組的弧矢向MTF值大於或等於70%,子午向MTF值大於或等於65%。Wherein, when the half angle of view is 50%, the wavelength is 0.555 micrometer, and the spatial frequency is 89 lppm, the sagittal MTF value of the optical module is greater than or equal to 70%, and the meridional to MTF value is greater than or equal to 65%.

其中,當半視角為90%、波長為0.555微米、空間頻率為89 lppm時,光學模組的弧矢向MTF值大於或等於58%,子午向MTF值大於或等於51%。Wherein, when the half angle of view is 90%, the wavelength is 0.555 micrometer, and the spatial frequency is 89 lppm, the sagittal MTF value of the optical module is greater than or equal to 58%, and the meridional to MTF value is greater than or equal to 51%.

上述光學模組可更包括一光圈,光圈設置在第一透鏡與第二透鏡之間,或者設置在物側與第一透鏡之間。The optical module may further include an aperture disposed between the first lens and the second lens or between the object side and the first lens.

其中,第一透鏡的材質可為玻璃,第二、三、四透鏡之材質可為塑膠。The material of the first lens may be glass, and the material of the second, third, and fourth lenses may be plastic.

或者,第一、二透鏡的材質為玻璃,第三、四透鏡之材質為塑膠。Alternatively, the first and second lenses are made of glass, and the third and fourth lenses are made of plastic.

或者,第一、三透鏡的材質為玻璃,第二、四透鏡之材質為塑膠。Alternatively, the first and third lenses are made of glass, and the second and fourth lenses are made of plastic.

其中,當波長為0.555微米時,光學模組的有效焦距(EFL)小於4.4 mm。Among them, when the wavelength is 0.555 micron, the effective focal length (EFL) of the optical module is less than 4.4 mm.

其中,當波長為0.555微米時,光學模組的有效焦距(EFL)小於3.6 mm。Among them, when the wavelength is 0.555 micron, the effective focal length (EFL) of the optical module is less than 3.6 mm.

上述光學模組可更包括一紅外濾光片及/或一影像 感測器,設置於第四透鏡與像側之間。The optical module may further include an infrared filter and/or an image The sensor is disposed between the fourth lens and the image side.

其中,光學模組的視角(FOV)在63度到75度之間。The optical module has a viewing angle (FOV) between 63 degrees and 75 degrees.

上述光學模組可更包括一影像感測器,設置於第四透鏡與像側之間,包括五百萬個畫素,每一畫素面積小於或等於1.4微米乘以1.4微米,排列成矩形陣列,矩形陣列的長邊與短邊之比值約為4/3。The optical module may further include an image sensor disposed between the fourth lens and the image side, including five million pixels, each pixel area being less than or equal to 1.4 micrometers and 1.4 micrometers, arranged in a rectangular shape. The ratio of the long side to the short side of the array, rectangular array is about 4/3.

或者,上述影像感測器包括七百九十萬個畫素,每一畫素面積小於或等於1.4微米乘以1.4微米,排列成矩形陣列,矩形陣列的長邊與短邊之比值約為4/3。Alternatively, the image sensor comprises 7.9 million pixels, each pixel area is less than or equal to 1.4 micrometers and 1.4 micrometers, arranged in a rectangular array, and the ratio of the long side to the short side of the rectangular array is about 4 /3.

為使本發明之上述目的、特徵、和優點能更明顯易懂,下文特舉較佳實施例並配合所附圖式做詳細說明。The above described objects, features, and advantages of the invention will be apparent from the description and appended claims

第1圖係依據本發明之一實施例之四片透鏡光學模組10的示意圖。1 is a schematic illustration of a four-lens optical module 10 in accordance with an embodiment of the present invention.

光學模組10有一物側12和一像側14,從物側12到像側14包括一具正屈光力之第一透鏡16,其焦距為F1且其包括一第一光學表面18和一第二光學表面20,第一光學表面18為凸面且面向物側12。The optical module 10 has an object side 12 and an image side 14, and includes a positive lens 16 having a positive refractive power from the object side 12 to the image side 14 having a focal length F1 and including a first optical surface 18 and a second The optical surface 20, the first optical surface 18 is convex and faces the object side 12.

光學模組10還包括一具負屈光力之第二透鏡22,其焦距為F2且其包括一第三光學表面24和一第四光學表面26,第三光學表面24面向物側12。The optical module 10 further includes a second lens 22 having a negative refractive power having a focal length F2 and including a third optical surface 24 and a fourth optical surface 26, the third optical surface 24 facing the object side 12.

光學模組10更包括一具正屈光力之第三透鏡27,其焦距為F3且其包括一第五光學表面28和一第六光學表面29,第五光學表面28面向物側12且為凹面,第六光學表面29面向像側14且為凸面。The optical module 10 further includes a third lens 27 having a positive refractive power having a focal length F3 and including a fifth optical surface 28 and a sixth optical surface 29, the fifth optical surface 28 facing the object side 12 and being concave. The sixth optical surface 29 faces the image side 14 and is convex.

光學模組10尚包括一具負屈光力之第四透鏡30,其焦距為F4且其包括一第七光學表面31和一第八光學表面32,第七光學表面31面向物側12。The optical module 10 further includes a fourth lens 30 having a negative refractive power having a focal length F4 and including a seventh optical surface 31 and an eighth optical surface 32, the seventh optical surface 31 facing the object side 12.

較佳者,光學模組10更包括一光圈33,其不是置於第一透鏡16與第二透鏡22之間,就是置於第一透鏡16之前,最好第一透鏡16是由玻璃材質製成。Preferably, the optical module 10 further includes an aperture 33 disposed between the first lens 16 and the second lens 22, or before the first lens 16, preferably the first lens 16 is made of glass. to make.

較佳者,四個透鏡中的每一個透鏡之兩個光學表面皆為非球面且每一個透鏡是由模造方式製成。Preferably, the two optical surfaces of each of the four lenses are aspherical and each lens is made by molding.

依據本發明,光學模組整體屈光力是分佈於四個透鏡之間,正屈光力透鏡與負屈光力透鏡分別對光學模組整體屈光力產生正的影響與負的影響。According to the present invention, the overall refractive power of the optical module is distributed between the four lenses, and the positive refractive power lens and the negative refractive power lens respectively have a positive influence and a negative influence on the overall refractive power of the optical module.

依據本發明,其中第一透鏡之屈光力需介於1.1倍至1.35倍的光學模組屈光力,可以下列的數學式來表示兩者之關係: 其中C1為第一透鏡之收斂,C為整個光學模組之收斂。According to the present invention, the refractive power of the first lens needs to be between 1.1 and 1.35 times the optical module refractive power, and the relationship between the two can be expressed by the following mathematical formula: Where C1 is the convergence of the first lens and C is the convergence of the entire optical module.

另外,依據本發明,其中第一透鏡之屈光力與第二透鏡之屈光力的比值之絕對值必需大於或等於2,可 以下列的數學式來表示兩者之關係: Further, according to the present invention, the absolute value of the ratio of the refractive power of the first lens to the refractive power of the second lens must be greater than or equal to 2, and the relationship between the two can be expressed by the following mathematical formula:

另外,依據本發明,其中第一透鏡之屈光力與第三透鏡之屈光力的比值需介於0.5至1.1之間,可以下列的數學式來表示兩者之關係: In addition, according to the present invention, the ratio of the refractive power of the first lens to the refractive power of the third lens needs to be between 0.5 and 1.1, and the relationship between the two can be expressed by the following mathematical formula:

如果將高屈光力特性集中在第一透鏡16與第三透鏡27,而沒有加入額外的限制條件,將導致高色散。If the high refractive power characteristics are concentrated on the first lens 16 and the third lens 27 without adding additional restrictions, high dispersion will result.

因為一個透鏡的EFL取決於其折射率,對於EFL為F之光學模組,其色散△f指的是在可見光譜兩端之氫的紅線c與藍線f所測得的EFL值之差值,即△f=EFL(Nc)-EFL(Nf)。Since the EFL of a lens depends on its refractive index, for an optical module whose EFL is F, the dispersion Δf refers to the difference between the EFL values measured by the red line c and the blue line f of hydrogen at both ends of the visible spectrum. That is, Δf=EFL(Nc)-EFL(Nf).

根據學術文獻,將收斂為Ca、折射率為Nda、阿貝係數為Vda的玻璃透鏡A與收斂為Cb、折射率為Ndb、阿貝係數為Vdb的玻璃透鏡B組合成具有收斂為C的二片透鏡式光學模組,當底下的條件滿足時,此二片透鏡式光學模組將有最小的色散:(Ca/Vda+Cb/Vdb)儘可能接近零(~0)According to the academic literature, a glass lens A that converges to Ca, has a refractive index of Nda, an Abbe's coefficient of Vda, and a glass lens B that converges to Cb, has a refractive index of Ndb, and has an Abbe's coefficient of Vdb is combined to have a convergence of C. A lenticular optical module, the two lenticular optical modules will have minimal dispersion when the underlying conditions are met: (Ca/Vda+Cb/Vdb) as close to zero as possible (~0)

假設Vdi代表第i片透鏡相對於波長位於可見光譜中間的鈉黃線(波長λ等於587.56 nm)之阿貝係數。It is assumed that Vdi represents the Abbe's coefficient of the i-th lens relative to the sodium yellow line (wavelength λ equals 587.56 nm) whose wavelength is in the middle of the visible spectrum.

當擴展為多片透鏡式光學模組時,上述條件將變為如下所述: Σ(Ci/Vdi)~0 (4)When expanded into a multi-lens optical module, the above conditions will become as follows: Σ(Ci/Vdi)~0 (4)

其中Ci與Vdi分別為第i片透鏡之收斂與阿貝係數。Among them, Ci and Vdi are the convergence and Abbe coefficient of the ith lens, respectively.

加入此條件表示光學模組必需由具正收斂之透鏡與具負收斂之透鏡組合而成,再搭配選用不同材質以調整其阿貝係數,使條件(4)滿足。Adding this condition means that the optical module must be composed of a lens with positive convergence and a lens with negative convergence, and then different materials are used to adjust the Abbe's coefficient to satisfy the condition (4).

本發明包括交替出現的正透鏡與負透鏡,另外,依據本發明其中的透鏡需滿足底下條件(C以屈光度表示): The present invention includes alternating positive and negative lenses, and in addition, the lens according to the present invention is required to satisfy the underlying conditions (C is expressed in diopter):

其中i=1、2、3、4且Ci為第i片透鏡之收斂、Vdi為第i片透鏡相對於波長為上述鈉黃線之阿貝係數,阿貝係數Vdi被定義成Vdi=(Ndi-1)/(Nfi-Nci),其中Ndi為第i片透鏡相對於波長位於可見光譜中間的鈉黃線之折射率,Nfi為第i片透鏡相對於波長為氫的藍線之折射率,Nci為第i片透鏡相對於波長為氫的紅線之折射率。Where i=1, 2, 3, 4 and Ci is the convergence of the i-th lens, Vdi is the Abbe coefficient of the i-th lens relative to the wavelength of the above-mentioned sodium yellow line, and the Abbe's coefficient Vdi is defined as Vdi=(Ndi -1) / (Nfi-Nci), where Ndi is the refractive index of the i-th lens relative to the yellow-yellow line whose wavelength is in the middle of the visible spectrum, and Nfi is the refractive index of the i-th lens relative to the blue line of hydrogen. Nci is the refractive index of the i-th lens relative to the red line of hydrogen.

須注意,當第一透鏡16具有相對較大之屈光力C1超過250屈光度時,只要Vd1>65,就很容易滿足條件(5)。It should be noted that when the first lens 16 has a relatively large refractive power C1 exceeding 250 diopters, it is easy to satisfy the condition (5) as long as Vd1>65.

此外,根據本發明之四片透鏡式光學模組,其中的透鏡滿足上述條件(1)至條件(3)以及條件(5)至條件(7),可大幅度的改善像散,達到高光學性能。例如根據本發明之四片透鏡式光學模組,當波長為0.555微米、空間頻率為89 lppm時,其中心(0%度半視角,0% degree hFOV)MTF大於或等於75%。Further, according to the four-lens optical module of the present invention, the lens satisfies the above conditions (1) to (3) and the conditions (5) to (7), which can greatly improve astigmatism and achieve high optical efficiency. performance. For example, according to the four-lens optical module of the present invention, when the wavelength is 0.555 micrometers and the spatial frequency is 89 lppm, the center (0% degree half angle, 0% degree hFOV) MTF is greater than or equal to 75%.

根據本發明之光學模組,更進一步顯示,當半視角為50%、波長為0.555微米、空間頻率為89 lppm時,其弧矢向與子午向之MTF差值小於8%。當半視角為90%、波長為0.555微米、空間頻率為89 lppm時,其弧矢向與子午向之MTF差值小於15%。According to the optical module of the present invention, it is further shown that when the half angle of view is 50%, the wavelength is 0.555 micrometers, and the spatial frequency is 89 lppm, the difference between the sagittal direction and the MTF of the meridional direction is less than 8%. When the half angle of view is 90%, the wavelength is 0.555 micrometers, and the spatial frequency is 89 lppm, the difference between the sagittal direction and the MTF of the meridional direction is less than 15%.

根據本發明較佳實施例之光學模組,當半視角為50%、波長為0.555微米、空間頻率為89 lppm時,其弧矢向MTF值大於或等於70%,其子午向MTF值大於或等於65%。According to the optical module of the preferred embodiment of the present invention, when the half angle of view is 50%, the wavelength is 0.555 micrometers, and the spatial frequency is 89 lppm, the sagittal MTF value is greater than or equal to 70%, and the meridional MTF value is greater than or equal to 65%.

根據本發明較佳實施例之光學模組,當半視角為90%、波長為0.555微米、空間頻率為89 lppm時,其弧矢向MTF值大於或等於58%,其子午向MTF值大於或等於51%。According to the optical module of the preferred embodiment of the present invention, when the half angle of view is 90%, the wavelength is 0.555 micrometers, and the spatial frequency is 89 lppm, the sagittal MTF value is greater than or equal to 58%, and the meridional MTF value is greater than or equal to 51%.

根據本發明較佳實施例之光學模組,其視角可達63度到75度之間。發明者指出,根據本發明之四片透鏡式光學模組,其視角介於63度到75度之間,其全視 角範圍內之弧矢向MTF值與子午向MTF值可以達到良好平衡,當搭配對角線長與焦距比值介於1.27到1.55之間之影像感測器,其影像解析度可達到五百萬畫素以上到八百萬畫素之間,光圈值小於2.5。An optical module according to a preferred embodiment of the present invention has a viewing angle of between 63 and 75 degrees. The inventors pointed out that the four-lens optical module according to the present invention has a viewing angle between 63 degrees and 75 degrees, and its full view. The angular MTF value and the meridional MTF value in the angular range can be well balanced. When using an image sensor with a diagonal length to focal length ratio between 1.27 and 1.55, the image resolution can reach 5 million paintings. Between the above and eight million pixels, the aperture value is less than 2.5.

現在將詳細描述本發明之各實施例。Embodiments of the present invention will now be described in detail.

第一實施例:光學模組之EFL=4.22 mm(C=237)First Embodiment: EFL=4.22 mm (C=237) of optical module

第2圖係依據本發明之光學模組210的示意圖。Figure 2 is a schematic illustration of an optical module 210 in accordance with the present invention.

光學模組210有一物側212和一像側214,這光學模組從物側212到像側214包括一具正屈光力之第一透鏡216,其焦距為F1且其包括一第一光學表面218和一第二光學表面220,第一光學表面218為凸面且面向物側212。The optical module 210 has an object side 212 and an image side 214. The optical module includes a first lens 216 having a positive refractive power from the object side 212 to the image side 214, and has a focal length F1 and includes a first optical surface 218. And a second optical surface 220, the first optical surface 218 is convex and faces the object side 212.

光學模組210然後包括一具負屈光力之第二透鏡222,其焦距為F2且其包括一第三光學表面224和一第四光學表面226,第三光學表面224面向物側212。The optical module 210 then includes a second lens 222 having a negative refractive power having a focal length F2 and including a third optical surface 224 and a fourth optical surface 226, the third optical surface 224 facing the object side 212.

光學模組210還包括一具正屈光力之第三透鏡227,其焦距為F3且其包括一第五光學表面228和一第六光學表面229,第五光學表面228面向物側212且為凹面,第六光學表面229面向像側214且為凸面。The optical module 210 further includes a third lens 227 having a positive refractive power having a focal length F3 and including a fifth optical surface 228 and a sixth optical surface 229, the fifth optical surface 228 facing the object side 212 and being concave. The sixth optical surface 229 faces the image side 214 and is convex.

光學模組210更包括一具負屈光力之第四透鏡230,其焦距為F4且其包括一第七光學表面231和一第 八光學表面232,第七光學表面231面向物側212。The optical module 210 further includes a fourth lens 230 having a negative refractive power, the focal length is F4 and includes a seventh optical surface 231 and a first The eight optical surface 232, the seventh optical surface 231 faces the object side 212.

光學模組210尚包括一光欄或光圈233,其置於第一透鏡216與第二透鏡222之間。The optical module 210 further includes a diaphragm or aperture 233 disposed between the first lens 216 and the second lens 222.

光學模組210可選擇性更包括一紅外濾光片240,其置於第四透鏡230與像側214之間。The optical module 210 can optionally include an infrared filter 240 disposed between the fourth lens 230 and the image side 214.

光學模組210還可選擇性更包括一影像感測器250,其置於第四透鏡230與像側214之間(在紅外濾光片240之後)。或者,光學模組210可以和影像感測器250一起使用,但是影像感測器250不屬於光學模組的一部份。The optical module 210 can also optionally include an image sensor 250 disposed between the fourth lens 230 and the image side 214 (after the infrared filter 240). Alternatively, the optical module 210 can be used with the image sensor 250, but the image sensor 250 does not belong to a portion of the optical module.

依據本發明之一實施例,影像感測器250至少包括七百九十萬個畫素(排列成矩形陣列),其長邊與短邊之比值趨近於4/3,每一畫素面積小於或等於1.4微米乘以1.4微米。According to an embodiment of the invention, the image sensor 250 includes at least 7.9 million pixels (arranged in a rectangular array), and the ratio of the long side to the short side approaches 4/3, and each pixel area Less than or equal to 1.4 microns multiplied by 1.4 microns.

依據本發明之另一個實施例,影像感測器250至少包括五百萬個畫素(排列成矩形陣列),其長邊與短邊之比值趨近於4/3,每一畫素面積小於或等於1.4微米乘以1.4微米。According to another embodiment of the present invention, the image sensor 250 includes at least five million pixels (arranged in a rectangular array), and the ratio of the long side to the short side approaches 4/3, and each pixel area is smaller than Or equal to 1.4 microns multiplied by 1.4 microns.

光學模組210之光圈值F#等於2.5。The aperture value F# of the optical module 210 is equal to 2.5.

其全視角等於67度。Its full viewing angle is equal to 67 degrees.

透鏡所使用之材質具有下表特性: The material used in the lens has the following characteristics:

第2圖中的光學模組具有下表之特性: The optical module in Figure 2 has the following characteristics:

光學模組210完全滿足條件(1)、條件(2)、條件(3)、條件(5)、條件(6)以及條件(7)。The optical module 210 completely satisfies the condition (1), the condition (2), the condition (3), the condition (5), the condition (6), and the condition (7).

第3圖為光學模組210之半視角相對於MTF之示意圖,圖形中顯示當波長為0.555微米、空間頻率為89 lppm時,以百分比標示(從0% -0.0到100% -1.0)之弧矢向MTF(標記S1)與子午向MTF(標記T1)相對於半視角位置(單位為毫米)改變而變化之情形,各不同半視角所對應之MTF如下所述:中心MTF:83%Figure 3 is a schematic diagram of the half angle of view of the optical module 210 relative to the MTF. The graph shows the arc labeled as a percentage (from 0% - 0.0 to 100% - 1.0) when the wavelength is 0.555 microns and the spatial frequency is 89 lppm. The MTF (marker S1) and the meridional MTF (marker T1) change with respect to the half-view position (in millimeters). The MTF corresponding to each different half-view is as follows: Center MTF: 83%

50%半視角MTF:弧矢向MTF=80%,子午向MTF=77%50% half-view MTF: sagittal to MTF=80%, meridional to MTF=77%

90%半視角MTF:弧矢向MTF=71%,子午向MTF=69%90% half-view MTF: sagittal to MTF=71%, meridional to MTF=69%

50%半視角範圍內之弧矢向與子午向MTF相對差值小於4%,90%半視角範圍內之弧矢向與子午向MTF相對差值小於8%。The relative difference between the sagittal direction and the meridional MTF in the range of 50% half angle of view is less than 4%, and the relative difference between the sagittal direction and the meridional MTF in the 90% half angle of view is less than 8%.

於圖示的實施例中,全半視角相當於影像高度為2.856毫米。In the illustrated embodiment, the full half angle of view corresponds to an image height of 2.856 mm.

第二實施例:光學模組之EFL=3.314 mm(C=302)Second embodiment: EFL=3.314 mm (C=302) of the optical module

第4圖係依據本發明之光學模組410的示意圖。Figure 4 is a schematic illustration of an optical module 410 in accordance with the present invention.

光學模組410有一物側412和一像側414,從物側412到像側414包括一具正屈光力之第一透鏡416,其焦距為F1且其包括一第一光學表面418和一第二光學表面420,第一光學表面418為凸面且面向物側412。The optical module 410 has an object side 412 and an image side 414. The object side 412 to the image side 414 includes a first lens 416 having a positive refractive power having a focal length F1 and including a first optical surface 418 and a second surface. Optical surface 420, first optical surface 418 is convex and faces object side 412.

光學模組410還包括一具負屈光力之第二透鏡422,其焦距為F2且其包括一第三光學表面424和一第四光學表面426,第三光學表面424面向物側412。The optical module 410 further includes a second lens 422 having a negative refractive power having a focal length F2 and including a third optical surface 424 and a fourth optical surface 426, the third optical surface 424 facing the object side 412.

光學模組410更包括一具正屈光力之第三透鏡427,其焦距為F3且其包括一第五光學表面428和一第六光學表面429,第五光學表面428面向物側412且為凹面,第六光學表面429面向像側414且為凸面。The optical module 410 further includes a third lens 427 having a positive refractive power having a focal length F3 and including a fifth optical surface 428 and a sixth optical surface 429. The fifth optical surface 428 faces the object side 412 and is concave. The sixth optical surface 429 faces the image side 414 and is convex.

光學模組410尚包括一具負屈光力之第四透鏡430,其焦距為F4且其包括一第七光學表面431和一第八光學表面432,第七光學表面431面向物側412。The optical module 410 further includes a fourth lens 430 having a negative refractive power having a focal length F4 and including a seventh optical surface 431 and an eighth optical surface 432, the seventh optical surface 431 facing the object side 412.

光學模組410包括一光欄或光圈433,其與第一光學表面418互相接觸。The optical module 410 includes a diaphragm or aperture 433 that is in contact with the first optical surface 418.

光學模組410可以像光學模組210一樣包括一紅外濾光片,也可以像光學模組210一樣和影像感測器一起使用。The optical module 410 can include an infrared filter like the optical module 210, or can be used with the image sensor like the optical module 210.

光學模組410適用於大約五百萬個畫素(排列成矩形陣列)之影像感測器450,其長邊與短邊之比值趨近於4/3,每一畫素面積大約等於1.4微米乘以1.4微米。The optical module 410 is applicable to an image sensor 450 of about five million pixels (arranged in a rectangular array), and the ratio of the long side to the short side is close to 4/3, and the area of each pixel is approximately equal to 1.4 micron. Multiply by 1.4 microns.

光學模組410之光圈值F#等於2.4。The aperture value F# of the optical module 410 is equal to 2.4.

其全視角等於67.4度。Its full viewing angle is equal to 67.4 degrees.

透鏡所使用之材質具有下表特性: The material used in the lens has the following characteristics:

此光學模組具有下表之特性: This optical module has the following characteristics:

此光學模組完全滿足條件(1)、條件(2)、條件(3)、條件(5)、條件(6)以及條件(7)。This optical module completely satisfies the condition (1), the condition (2), the condition (3), the condition (5), the condition (6), and the condition (7).

第5圖為光學模組410之半視角相對於MTF之示意圖,圖形中顯示當波長為0.555微米、空間頻率為89 lppm時,以百分比標示(從0% -0.0到100% -1.0)之弧矢向MTF(標記S1)與子午向MTF(標記T1)相對於半視角位置(單位為毫米)改變而變化之情形,各不同半視角所對應之MTF如下所述:中心MTF:81.8%Figure 5 is a schematic diagram of the half angle of view of the optical module 410 relative to the MTF. The graph shows the arc labeled as a percentage (from 0% - 0.0 to 100% - 1.0) when the wavelength is 0.555 microns and the spatial frequency is 89 lppm. The MTF (marker S1) and the meridional MTF (marker T1) change with respect to the half-view position (in millimeters). The MTF corresponding to each different half-view is as follows: Center MTF: 81.8%

50%半視角MTF:弧矢向MTF=80%,子午向MTF=78%50% half-view MTF: sagittal to MTF=80%, meridional to MTF=78%

90%半視角MTF:弧矢向MTF=77%,子午向MTF=70%90% half-view MTF: sagittal to MTF=77%, meridional to MTF=70%

50%半視角範圍內之弧矢向與子午向MTF相對差值小於4%,90%半視角範圍內之弧矢向與子午向MTF相對差值小於8%。The relative difference between the sagittal direction and the meridional MTF in the range of 50% half angle of view is less than 4%, and the relative difference between the sagittal direction and the meridional MTF in the 90% half angle of view is less than 8%.

全半視角相當於影像高度為2.27毫米。The full half angle of view is equivalent to an image height of 2.27 mm.

雖然本發明已以較佳實施例揭露如上,然其並非用以限定本發明,任何熟習此項技藝者,在不脫離本發明之精神和範圍內,仍可作些許的更動與潤飾,因此本發明之保護範圍當視後附之申請專利範圍所界定者為準。Although the present invention has been described above in terms of the preferred embodiments, it is not intended to limit the invention, and the invention may be modified and modified without departing from the spirit and scope of the invention. The scope of the invention is defined by the scope of the appended claims.

10‧‧‧光學模組10‧‧‧Optical module

12‧‧‧物側12‧‧‧ object side

14‧‧‧像側14‧‧‧ image side

16‧‧‧第一透鏡16‧‧‧First lens

18‧‧‧第一光學表面18‧‧‧First optical surface

20‧‧‧第二光學表面20‧‧‧Second optical surface

22‧‧‧第二透鏡22‧‧‧second lens

24‧‧‧第三光學表面24‧‧‧ Third optical surface

26‧‧‧第四光學表面26‧‧‧ Fourth optical surface

27‧‧‧第三透鏡27‧‧‧ third lens

28‧‧‧第五光學表面28‧‧‧ Fifth optical surface

29‧‧‧第六光學表面29‧‧‧ Sixth optical surface

30‧‧‧第四透鏡30‧‧‧Fourth lens

31‧‧‧第七光學表面31‧‧‧ seventh optical surface

32‧‧‧第八光學表面32‧‧‧ Eighth optical surface

33‧‧‧光圈33‧‧‧ aperture

210‧‧‧光學模組210‧‧‧Optical module

212‧‧‧物側212‧‧‧ ‧ side

214‧‧‧像側214‧‧‧ image side

216‧‧‧第一透鏡216‧‧‧ first lens

218‧‧‧第一光學表面218‧‧‧First optical surface

220‧‧‧第二光學表面220‧‧‧Second optical surface

222‧‧‧第二透鏡222‧‧‧second lens

224‧‧‧第三光學表面224‧‧‧ Third optical surface

226‧‧‧第四光學表面226‧‧‧ Fourth optical surface

227‧‧‧第三透鏡227‧‧‧ third lens

228‧‧‧第五光學表面228‧‧‧ fifth optical surface

229‧‧‧第六光學表面229‧‧‧ sixth optical surface

230‧‧‧第四透鏡230‧‧‧Fourth lens

231‧‧‧第七光學表面231‧‧‧ seventh optical surface

232‧‧‧第八光學表面232‧‧‧ eighth optical surface

233‧‧‧光欄或光圈233‧‧‧ ray or aperture

240‧‧‧紅外濾光片240‧‧‧Infrared filter

250‧‧‧影像感測器250‧‧‧Image Sensor

410‧‧‧光學模組410‧‧‧Optical module

412‧‧‧物側412‧‧‧ ‧ side

414‧‧‧像側414‧‧‧ image side

416‧‧‧第一透鏡416‧‧‧ first lens

418‧‧‧第一光學表面418‧‧‧First optical surface

420‧‧‧第二光學表面420‧‧‧Second optical surface

422‧‧‧第二透鏡422‧‧‧second lens

424‧‧‧第三光學表面424‧‧‧ Third optical surface

426‧‧‧第四光學表面426‧‧‧Fourth optical surface

427‧‧‧第三透鏡427‧‧‧ third lens

428‧‧‧第五光學表面428‧‧‧ fifth optical surface

429‧‧‧第六光學表面429‧‧‧ sixth optical surface

430‧‧‧第四透鏡430‧‧‧4th lens

431‧‧‧第七光學表面431‧‧‧ seventh optical surface

432‧‧‧第八光學表面432‧‧‧ eighth optical surface

433‧‧‧光欄或光圈433‧‧‧ ray or aperture

450‧‧‧影像感測器450‧‧‧Image sensor

第1圖係依據本發明之一實施例之四片透鏡光學模組示意圖。1 is a schematic view of a four-lens optical module in accordance with an embodiment of the present invention.

第2圖係依據本發明之另一實施例之光學模組示意圖。2 is a schematic view of an optical module according to another embodiment of the present invention.

第3圖係第2圖之光學模組於空間頻率等於89 lppm時之調變轉換函數圖。Figure 3 is a diagram of the modulation transfer function of the optical module of Figure 2 at a spatial frequency equal to 89 lppm.

第4圖係依據本發明之另一實施例之光學模組示意圖。Figure 4 is a schematic diagram of an optical module in accordance with another embodiment of the present invention.

第5圖係第4圖之光學模組於空間頻率等於89 lppm時之調變轉換函數圖。Figure 5 is a diagram of the modulation transfer function of the optical module of Figure 4 at a spatial frequency equal to 89 lppm.

10‧‧‧光學模組10‧‧‧Optical module

12‧‧‧物側12‧‧‧ object side

14‧‧‧像側14‧‧‧ image side

16‧‧‧第一透鏡16‧‧‧First lens

18‧‧‧第一光學表面18‧‧‧First optical surface

20‧‧‧第二光學表面20‧‧‧Second optical surface

22‧‧‧第二透鏡22‧‧‧second lens

24‧‧‧第三光學表面24‧‧‧ Third optical surface

26‧‧‧第四光學表面26‧‧‧ Fourth optical surface

27‧‧‧第三透鏡27‧‧‧ third lens

28‧‧‧第五光學表面28‧‧‧ Fifth optical surface

29‧‧‧第六光學表面29‧‧‧ Sixth optical surface

30‧‧‧第四透鏡30‧‧‧Fourth lens

31‧‧‧第七光學表面31‧‧‧ seventh optical surface

32‧‧‧第八光學表面32‧‧‧ Eighth optical surface

33‧‧‧光圈33‧‧‧ aperture

Claims (18)

一種光學模組,具有一物側以及一像側,該光學模組從該物側至該像側包括:一第一透鏡,為一具正屈光力之凹凸透鏡,包括一第一光學表面以及一第二光學表面,該第一光學表面為凸面且面向該物側;一第二透鏡,為一具負屈光力之凹凸透鏡,包括一第三光學表面以及一第四光學表面,該第三光學表面面向該物側;一第三透鏡,為一具正屈光力之凹凸透鏡,包括一第五光學表面以及一第六光學表面,該第五光學表面為凹面且面向該物側,該第六光學表面為凸面且面向該像側;一第四透鏡,為一具負屈光力之透鏡,包括一第七光學表面以及一第八光學表面,該第七光學表面面向該物側;其中,|C1/C2|2、C1/Vd15.2、1.1C1/C1.35,C1為該第一透鏡之收斂等於該第一透鏡之有效焦距的倒數,該第一透鏡之收斂的單位為1/m,C2為該第二透鏡之收斂等於該第二透鏡之有效焦距的倒數,該第二透鏡之收斂的單位為1/m,Vd1為該第一透鏡之阿貝係數,C為該光學模組之收斂等於該光學模組之有效焦距的倒數,該 光學模組之收斂的單位為1/m。An optical module having an object side and an image side, the optical module from the object side to the image side comprising: a first lens, a positive refractive power concave-convex lens, comprising a first optical surface and a a second optical surface having a convex surface facing the object side; a second lens being a concave lens having a negative refractive power, comprising a third optical surface and a fourth optical surface, the third optical surface Facing the object side; a third lens is a positive refractive power concave-convex lens comprising a fifth optical surface and a sixth optical surface, the fifth optical surface being concave and facing the object side, the sixth optical surface a convex surface facing the image side; a fourth lens being a lens having a negative refractive power, comprising a seventh optical surface and an eighth optical surface, the seventh optical surface facing the object side; wherein, |C1/C2 | 2, C1/Vd1 5.2, 1.1 C1/C 1.35, C1 is that the convergence of the first lens is equal to the reciprocal of the effective focal length of the first lens, the unit of convergence of the first lens is 1/m, and C2 is that the convergence of the second lens is equal to the effective focal length of the second lens. Reciprocal, the unit of convergence of the second lens is 1/m, Vd1 is the Abbe coefficient of the first lens, and C is the reciprocal of the convergence of the optical module equal to the effective focal length of the optical module, the optical module The unit of convergence is 1/m. 如申請專利範圍第1項所述之光學模組,其中 C1為該第一透鏡之收斂等於該第一透鏡之有效焦距的倒數,該第一透鏡之收斂的單位為1/m,C3為該第三透鏡之收斂等於該第三透鏡之有效焦距的倒數,該第三透鏡之收斂的單位為1/m。The optical module of claim 1, wherein C1 is that the convergence of the first lens is equal to the reciprocal of the effective focal length of the first lens, the unit of convergence of the first lens is 1/m, and C3 is that the convergence of the third lens is equal to the reciprocal of the effective focal length of the third lens. The unit of convergence of the third lens is 1/m. 如申請專利範圍第1項所述之光學模組,其中 C2為該第二透鏡之收斂等於該第二透鏡之有效焦距的倒數,該第二透鏡之收斂的單位為1/m,Vd2為該第二透鏡之阿貝係數。The optical module of claim 1, wherein C2 is that the convergence of the second lens is equal to the reciprocal of the effective focal length of the second lens, the unit of convergence of the second lens is 1/m, and Vd2 is the Abbe coefficient of the second lens. 如申請專利範圍第1項所述之光學模組,其中 Ci為第i透鏡之收斂等於該第i透鏡之有效焦距的倒數,該第i透鏡之收斂的單位為1/m,Vdi為第i透鏡之阿貝係數,i=1、2、3、4。The optical module of claim 1, wherein Ci is the reciprocal of the ith lens equal to the effective focal length of the ith lens, the unit of convergence of the ith lens is 1/m, and Vdi is the Abbe coefficient of the ith lens, i=1, 2, 3, 4 . 如申請專利範圍第1項所述之光學模組,其中當波長為0.555微米、空間頻率為89lppm時,該光學模組中心調變轉換函數(MTF)值大於或等於75%。 The optical module of claim 1, wherein the optical module central modulation transfer function (MTF) value is greater than or equal to 75% when the wavelength is 0.555 micrometers and the spatial frequency is 89 lppm. 如申請專利範圍第1項所述之光學模組,其中當半視角為50%、波長為0.555微米、空間頻率為89lppm 時,該光學模組弧矢向與子午向之調變轉換函數(MTF)差值小於8%;當半視角為90%、波長為0.555微米、空間頻率為89lppm時,該光學模組的弧矢向與子午向之調變轉換函數(MTF)差值小於15%。 The optical module of claim 1, wherein the half angle of view is 50%, the wavelength is 0.555 micrometers, and the spatial frequency is 89 lppm. The difference between the sagittal direction and the meridional modulation transfer function (MTF) of the optical module is less than 8%; when the half angle of view is 90%, the wavelength is 0.555 micrometers, and the spatial frequency is 89 lppm, the sagittal direction of the optical module The difference from the meridian modulation transfer function (MTF) is less than 15%. 如申請專利範圍第1項所述之光學模組,其中當半視角為50%、波長為0.555微米、空間頻率為89lppm時,該光學模組的弧矢向MTF值大於或等於70%,子午向MTF值大於或等於65%。 The optical module of claim 1, wherein the optical module has a sagittal MTF value greater than or equal to 70% when the half angle of view is 50%, the wavelength is 0.555 micrometers, and the spatial frequency is 89 lppm, and the meridional direction is The MTF value is greater than or equal to 65%. 如申請專利範圍第1項所述之光學模組,其中當半視角為90%、波長為0.555微米、空間頻率為89lppm時,該光學模組的弧矢向MTF值大於或等於58%,子午向MTF值大於或等於51%。 The optical module of claim 1, wherein when the half angle of view is 90%, the wavelength is 0.555 micrometers, and the spatial frequency is 89 lppm, the sagittal MTF value of the optical module is greater than or equal to 58%, and the meridional direction The MTF value is greater than or equal to 51%. 如申請專利範圍第1項所述之光學模組,其更包括一光圈,該光圈設置在該第一透鏡與該第二透鏡之間,或者設置在該物側與該第一透鏡之間。 The optical module of claim 1, further comprising an aperture disposed between the first lens and the second lens or between the object side and the first lens. 如申請專利範圍第1項所述之光學模組,其中該第一透鏡的材質為玻璃,該第二、三、四透鏡之材質為塑膠。 The optical module of claim 1, wherein the first lens is made of glass, and the second, third, and fourth lenses are made of plastic. 如申請專利範圍第1項所述之光學模組,其中該第一、二透鏡的材質為玻璃,該第三、四透鏡之材質為塑膠。 The optical module of claim 1, wherein the first and second lenses are made of glass, and the third and fourth lenses are made of plastic. 如申請專利範圍第1項所述之光學模組,其中 該第一、三透鏡的材質為玻璃,該第二、四透鏡之材質為塑膠。 The optical module of claim 1, wherein The first and third lenses are made of glass, and the second and fourth lenses are made of plastic. 如申請專利範圍第1項所述之光學模組,其中當波長為0.555微米時,該光學模組的有效焦距(EFL)小於4.4mm。 The optical module of claim 1, wherein the optical module has an effective focal length (EFL) of less than 4.4 mm when the wavelength is 0.555 micrometers. 如申請專利範圍第13項所述之光學模組,其中當波長為0.555微米時,該光學模組的有效焦距(EFL)小於3.6mm。 The optical module of claim 13, wherein the optical module has an effective focal length (EFL) of less than 3.6 mm when the wavelength is 0.555 micrometers. 如申請專利範圍第1項所述之光學模組,其更包括一紅外濾光片及/或一影像感測器,設置於該第四透鏡與該像側之間。 The optical module of claim 1, further comprising an infrared filter and/or an image sensor disposed between the fourth lens and the image side. 如申請專利範圍第1項所述之光學模組,其中該光學模組的視角(FOV)在63度到75度之間。 The optical module of claim 1, wherein the optical module has a viewing angle (FOV) of between 63 degrees and 75 degrees. 如申請專利範圍第1項所述之光學模組,其更包括一影像感測器,設置於該第四透鏡與該像側之間,包括五百萬個畫素,每一畫素面積小於或等於1.4微米乘以1.4微米,排列成矩形陣列,該矩形陣列的長邊與短邊之比值約為4/3。 The optical module of claim 1, further comprising an image sensor disposed between the fourth lens and the image side, comprising five million pixels, each pixel area being smaller than Or equal to 1.4 microns by 1.4 microns, arranged in a rectangular array, the ratio of the long side to the short side of the rectangular array is about 4/3. 如申請專利範圍第17項所述之光學模組,其中該影像感測器包括七百九十萬個畫素,每一畫素面積小於或等於1.4微米乘以1.4微米,排列成矩形陣列,該矩形陣列的長邊與短邊之比值約為4/3。The optical module of claim 17, wherein the image sensor comprises 7.9 million pixels, each pixel area being less than or equal to 1.4 micrometers and 1.4 micrometers, arranged in a rectangular array. The ratio of the long side to the short side of the rectangular array is about 4/3.
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