WO2011021271A1 - 撮像レンズ、撮像装置及び携帯端末 - Google Patents
撮像レンズ、撮像装置及び携帯端末 Download PDFInfo
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- WO2011021271A1 WO2011021271A1 PCT/JP2009/064435 JP2009064435W WO2011021271A1 WO 2011021271 A1 WO2011021271 A1 WO 2011021271A1 JP 2009064435 W JP2009064435 W JP 2009064435W WO 2011021271 A1 WO2011021271 A1 WO 2011021271A1
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- lens
- imaging
- imaging lens
- refractive power
- image side
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/001—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
- G02B13/0015—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design
- G02B13/002—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface
- G02B13/0045—Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design having at least one aspherical surface having five or more lenses
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/18—Optical objectives specially designed for the purposes specified below with lenses having one or more non-spherical faces, e.g. for reducing geometrical aberration
Definitions
- the present invention relates to a small imaging lens, an imaging apparatus, and a portable terminal using a solid-state imaging device such as a CCD image sensor or a CMOS image sensor.
- a first lens having a positive refractive power in order from the object side, a first lens having a positive refractive power, a second lens having a negative refractive power, a third lens having a positive refractive power, and a first lens having a negative refractive power.
- An imaging lens including four lenses and a fifth lens having a negative refractive power is disclosed (for example, see Patent Document 1).
- An imaging lens composed of a fifth lens having power is disclosed (for example, see Patent Document 2).
- an imaging lens having a five-lens structure is difficult to reduce in size because the number of lenses is larger than that of a lens having three or four lenses.
- the imaging lens described in Patent Document 1 bears most of the refractive power of the entire system from the first lens to the third lens, and the fourth lens and the fifth lens serve as an image plane correction lens having a weak refractive power. Only effective. Therefore, if the aberration correction is insufficient and the total lens length is further shortened, there is a problem that it becomes difficult to cope with the increase in the number of pixels of the image pickup device due to performance deterioration.
- the imaging lens described in Patent Document 2 has an excellent performance with insufficient correction of spherical aberration and coma aberration because the front group including the first lens and the second lens is configured by a spherical system. It cannot be secured.
- the front group and the rear group after the third lens have positive refractive power, the principal point position of the optical system is an image as compared with the configuration of the telephoto type in which the rear group has negative refractive power. This is a disadvantageous type for downsizing because the back focus becomes longer.
- the present invention has been made in view of such a problem, and is a five-lens imaging lens in which various aberrations are favorably corrected while being smaller than the conventional type, an imaging device including the imaging lens, and the imaging An object is to provide a portable terminal including the device.
- the present invention aims at downsizing that satisfies the following formula. By satisfying this range, the entire imaging apparatus can be reduced in size and weight.
- L Distance on the optical axis from the lens surface closest to the object side to the image-side focal point of the entire imaging lens system 2Y: Diagonal length of the imaging surface of the solid-state imaging device (diagonal length of the rectangular effective pixel region of the solid-state imaging device)
- the image-side focal point refers to an image point when a parallel light beam parallel to the optical axis is incident on the imaging lens.
- the imaging lens is parallel.
- the flat plate portion is calculated as the above L value after the air conversion distance. Moreover, the range of the following formula is more desirable.
- an imaging lens for forming a subject image on a photoelectric conversion unit of a solid-state imaging device
- a first lens having a positive refractive power and a convex surface facing the object side
- a second lens having a negative refractive power and a concave surface facing the image side
- positive refraction A third lens having a power and a convex surface facing the image side
- a fourth lens having a positive refractive power and a convex surface facing the image side and having a meniscus shape, and a concave surface having a negative refractive power and the image side
- an imaging lens characterized by satisfying the following conditional expression:
- the basic configuration of the present invention for obtaining a well-corrected imaging lens includes an aperture stop, a first lens having a positive refractive power and a convex surface facing the object side, and an image side having a negative refractive power.
- This so-called telephoto type lens configuration in which a positive lens group including a first lens, a second lens, a third lens, and a fourth lens and a negative fifth lens are arranged in this order from the object side shortens the overall length of the imaging lens.
- This is an advantageous configuration.
- Conditional expression (1) defines the shaping factor of the fourth lens.
- the refractive power of the positive lens such as the first lens and the third lens is increased to move the principal point position to the object side, and the focal length of the entire system tends to be shortened. is there.
- exceeding the lower limit value of the conditional expression (1) makes the fourth lens a strong meniscus shape, and suppresses the difference between the incident angles of the upper marginal ray and the lower marginal ray of the ray passing off the axis, and coma aberration. Since the principal point position of the fourth lens having positive refractive power can be moved to the image side, the focal length of the entire system can be increased.
- by lowering the upper limit value of conditional expression (1) it is possible to suppress the occurrence of higher-order aberrations such as field curvature due to an increase in the radius of curvature of the image side surface.
- Conditional expression (2) defines the ratio of the distance on the optical axis from the aperture stop to the image side focal point and the focal length.
- the image-side focal point refers to an image point when a parallel light beam parallel to the optical axis is incident on the imaging lens.
- the imaging lens When a parallel plate such as an optical low-pass filter, an infrared cut filter, or a seal glass of a solid-state imaging device package is disposed between the image-side surface of the imaging lens and the image-side focal position, the imaging lens is parallel.
- the flat plate portion is calculated as the SL value after the air conversion distance.
- the exit pupil position can be arranged farther from the imaging surface even in the imaging lens with a shortened total length,
- the chief ray incident angle (the angle formed between the chief ray and the optical axis) of the light beam that forms an image on the periphery of the imaging surface of the solid-state imaging device can be kept small, and so-called telecentric characteristics can be secured.
- an increase in the total length can be suppressed by falling below the upper limit value of conditional expression (2). Even when a mechanical shutter is required, since it can be arranged closest to the object side, an imaging lens with a short overall length can be obtained.
- f4 Focal length of the fourth lens
- f Focal length of the entire imaging lens
- Conditional expression (3) defines a ratio between the focal length of the fourth lens and the focal length of the entire system.
- the back focus is shortened in the same manner as the focal length of the entire system, and an optical low-pass filter, an infrared cut filter, or a solid object between the image side surface of the imaging lens and the image side focal position.
- the back focus can be secured by satisfying the range of the conditional expression (1), but the focal length of the entire system may become too long.
- the refractive power of the fourth lens becomes strong by satisfying the range of conditional expression (1) and falling below the upper limit value of conditional expression (3), the focal length of the entire system is ensured while ensuring the back focus. Can be kept.
- the positive refractive power of the fourth lens can be appropriately maintained by exceeding the lower limit value of the conditional expression (3), the overall length of the lens is shortened and off-axis such as field curvature and distortion is off-axis. Correction of various aberrations can be suppressed satisfactorily.
- conditional expression (4) defines the ratio of the focal lengths of the third lens and the fourth lens.
- the refractive power of the third lens can be maintained moderately, the composite principal point of the first lens to the fourth lens can be arranged closer to the object side, and imaging is performed.
- the total lens length can be shortened.
- by exceeding the lower limit value it is possible to secure the focal length of the entire system by sharing the refractive power of the third lens with the fourth lens on the image side.
- Conditional expression (5) is a conditional expression for favorably correcting chromatic aberration of the entire imaging lens system.
- chromatic aberrations such as axial chromatic aberration and lateral chromatic aberration in a well-balanced manner.
- it can comprise with the easily available glass material by being less than an upper limit.
- Conditional expression (6) is a conditional expression for satisfactorily correcting chromatic aberration and curvature of field of the entire imaging lens system.
- conditional expression (6) exceeds the lower limit, the refractive power of the second lens having relatively large dispersion can be maintained appropriately, and chromatic aberration and curvature of field can be corrected well.
- it can comprise with the easily available glass material by being less than an upper limit.
- the partial group When the partial group is extended, depending on the optical system, it is possible to reduce the performance degradation at the time of focusing at a short distance, and the moving group may be a part rather than the whole lens, so that the drive mechanism can be simplified, and the imaging device There is an advantage that the overall size and weight can be reduced.
- conditional expression (7) When the value of conditional expression (7) exceeds the lower limit, it is possible to secure a sufficient stroke when the partial group is extended from the first lens to the third lens.
- the positive refractive power around the fourth lens can be appropriately maintained, the lateral chromatic aberration can be corrected well, and the telecentric characteristics at the peripheral portion can be easily secured.
- the air gap on the optical axis of the third lens and the fourth lens does not become excessively large, and the entire length of the imaging lens can be shortened.
- the image side surface of the second lens By making the image side surface of the second lens an aspherical shape in which the negative refractive power decreases as going from the center to the periphery, light rays are not excessively bounced around the periphery, and off-axis aberrations are good It is possible to secure a good telecentric characteristic in the peripheral portion after correcting to.
- the aperture stop is located closer to the image side than the position on the optical axis of the object side surface of the first lens, and is disposed closer to the object side than the most peripheral portion of the object side surface of the first lens.
- the imaging lens according to any one of 1 to 7.
- the aperture stop By disposing the aperture stop on the image side from the position on the optical axis of the object side surface of the first lens and on the object side from the most peripheral part of the object side surface of the first lens, the refraction angle on the object side surface of the first lens Therefore, it is possible to suppress the occurrence of higher-order spherical aberration and coma generated in the first lens.
- the height of the light beam passing through the first lens can be reduced, the edge thickness of the first lens can be easily ensured, and the moldability can be improved.
- the image side surface of the fifth lens is formed in an aspherical shape, and has a negative refractive power at the center thereof, the negative refractive power becomes weaker toward the periphery, and has an inflection point.
- the imaging lens according to any one of 1 to 8 above.
- the negative refracting power becomes weaker as the image side surface of the fifth lens goes from the optical axis to the periphery, and it becomes easy to ensure the telecentric characteristics of the image side light flux by making the aspherical shape having an inflection point. Further, the image side surface of the second lens need not excessively weaken the negative refracting power at the periphery of the lens, and can correct off-axis aberrations satisfactorily.
- the “inflection point” is a point on the aspheric surface where the tangent plane of the aspherical vertex is a plane perpendicular to the optical axis in the curve of the lens cross-sectional shape within the effective radius.
- An imaging apparatus comprising: a solid-state imaging device that photoelectrically converts a subject image; and the imaging lens described in any one of 1 to 10 above.
- a portable terminal comprising the imaging device according to 11 above.
- the imaging lens, the imaging device, and the portable terminal of the present invention it is possible to obtain high-performance optical performance by satisfactorily correcting various aberrations while being smaller than the conventional type.
- FIG. 6 is a schematic sectional drawing of an imaging device. It is an external view of a mobile phone. 2 is a cross-sectional view of the lens of Example 1.
- FIG. 3 is an aberration diagram of the lens according to Example 1.
- 6 is a cross-sectional view of a lens of Example 2.
- FIG. 6 is an aberration diagram of the lens of Example 2.
- FIG. 6 is a cross-sectional view of a lens of Example 3.
- FIG. 6 is an aberration diagram for the lens of Example 3.
- 6 is a sectional view of a lens of Example 4.
- FIG. 6 is an aberration diagram for the lens of Example 4.
- 6 is a cross-sectional view of a lens of Example 5.
- FIG. 6 is an aberration diagram for the lens of Example 5.
- FIG. 6 is a sectional view of a lens of Example 6.
- FIG. FIG. 10 is an aberration diagram for the lens of Example 6.
- 10 is a cross-sectional view of a lens according to Example 7.
- FIG. 10 is an aberration diagram for the lens of Example 7.
- 10 is a cross-sectional view of a lens of Example 8.
- FIG. 10 is an aberration diagram of the lens of Example 8.
- FIG. 10 is a sectional view of the lens of Example 9.
- FIG. 10 is an aberration diagram of the lens of Example 9. FIG.
- the imaging lens L includes a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, and a fifth lens L5 in order from the object side.
- the first lens L1, the second lens L2, and the third lens L3 are held by the lens frame 11, and a diaphragm S is formed on the object side of the first lens L1 in the lens frame 11.
- the fourth lens L4 and the fifth lens L5 are held by the lens frame 12.
- an optical low-pass filter, an IR cut filter, or a parallel plate F that is a seal glass of the solid-state imaging device I is held by the lens frame 12.
- the subject image is focused by the diaphragm S, and passes through the imaging lens L and the parallel plate F to form an image on the imaging surface I of the solid-state imaging device C, which is photoelectrically converted.
- the solid-state imaging device C is mounted on the printed wiring board P, and the printed wiring board P is fixed to the lens frame 12, and the image signal of the subject image subjected to photoelectric conversion is transmitted to the outside through the printed wiring board P.
- the lens frame 11 holding the first lens L1, the second lens L2, and the third lens L3 is moved in the optical axis direction with respect to the lens frame 12, and the focal position is adjusted by an autofocus or macro switching function. .
- FIG. 2A is a view of the folded mobile phone as viewed from the inside
- FIG. 2B is a view of the folded mobile phone as viewed from the outside.
- an upper housing 101 as a case having display screens D ⁇ b> 1 and D ⁇ b> 2 and a lower housing 102 having operation buttons B are connected via a hinge 103.
- the imaging device is built under the display screen D2 in the upper casing 101, and the imaging lens L is exposed on the outer surface of the upper casing 101.
- the position of the imaging device may be arranged above or on the side of the display screen D2 in the upper housing 101.
- the mobile phone T is not limited to a folding type.
- f Focal length of the entire imaging lens system fB: Back focus
- F F number 2Y: Diagonal length of the imaging surface of the solid-state imaging device
- ENTP Entrance pupil position (distance from the first surface to the entrance pupil position)
- EXTP exit pupil position (distance from imaging surface to exit pupil position)
- H1 Front principal point position (distance from the first surface to the front principal point position)
- H2 Rear principal point position (distance from the final surface to the rear principal point position)
- R radius of curvature
- D axial distance between axes
- Nd refractive index of lens material with respect to d-line
- ⁇ d Abbe number of lens material In the surface data, units of R, D, and effective radius are mm.
- the surface described with “*” after each surface number is a surface having an aspherical shape, and the aspherical shape has the vertex of the surface as the origin and the X axis in the optical axis direction.
- the height in the direction perpendicular to the optical axis is represented by the following “Equation 1”.
- FIG. 3 is a sectional view of the imaging lens.
- L1 is a first lens
- L2 is a second lens
- L3 is a third lens
- L4 is a fourth lens
- L5 is a fifth lens
- S is an aperture stop
- I is an imaging surface.
- F is a parallel plate assuming an optical low-pass filter, an IR cut filter, a seal glass of a solid-state image sensor, or the like.
- FIG. 4 is an aberration diagram (spherical aberration, astigmatism, distortion, meridional coma) of the imaging lens.
- all the lenses are made of a plastic material, and a partial group is formed by moving the first lens L1 to the third lens L3 as a single unit for focus position adjustment in an autofocus or macro switching function. It is supposed to be paid out.
- the eccentric error sensitivity of the first lens L1 increases.
- aligning with the first lens L1 it is possible to reduce asymmetric blur in the screen called single blur that occurs in the entire system. In this embodiment, it is assumed that this alignment is performed.
- the alignment means that the lens is decentered with respect to the optical axis, thereby canceling and reducing the one-sided blur caused by other than the first lens L1.
- the alignment may be performed for the purpose of reducing axial coma rather than reducing one-sided blur.
- FIG. 5 is a cross-sectional view of the imaging lens of the second embodiment.
- L1 is a first lens
- L2 is a second lens
- L3 is a third lens
- L4 is a fourth lens
- L5 is a fifth lens
- S is an aperture stop
- I is an imaging surface.
- F is a parallel plate assuming an optical low-pass filter, an IR cut filter, a seal glass of a solid-state image sensor, or the like.
- FIG. 6 is an aberration diagram (spherical aberration, astigmatism, distortion, meridional coma) of the imaging lens of Example 2.
- all the lenses are made of a plastic material, and the sub-group is formed by moving the first lens L1 to the third lens L3 as a single unit for focus position adjustment in autofocus, macro switching function, and the like. It is assumed to be paid out.
- FIG. 7 is a sectional view of the lens of Example 3.
- L1 is a first lens
- L2 is a second lens
- L3 is a third lens
- L4 is a fourth lens
- L5 is a fifth lens
- S is an aperture stop
- I is an imaging surface.
- F is a parallel plate assuming an optical low-pass filter, an IR cut filter, a seal glass of a solid-state image sensor, or the like.
- FIG. 8 is an aberration diagram of Example 3 (spherical aberration, astigmatism, distortion, and meridional coma).
- the first lens L1 is made of a glass mold lens, and the other lenses are made of a plastic material, and the first lens L1 to the third lens L3 are used for focusing with auto focus, macro switching function, or the like. It is assumed that the partial group feeding is performed by moving up to one.
- Example 4 The overall specifications of the imaging lens are shown below.
- FIG. 9 is a sectional view of the lens of Example 4.
- L1 is a first lens
- L2 is a second lens
- L3 is a third lens
- L4 is a fourth lens
- L5 is a fifth lens
- S is an aperture stop
- I is an imaging surface.
- F is a parallel plate assuming an optical low-pass filter, an IR cut filter, a seal glass of a solid-state image sensor, or the like.
- FIG. 10 is an aberration diagram of Example 4 (spherical aberration, astigmatism, distortion, and meridional coma).
- all the lenses are made of a plastic material, and a partial group is formed by moving the first lens L1 to the third lens L3 as a single unit for focus position adjustment in an autofocus or macro switching function. It is supposed to be paid out.
- FIG. 11 is a sectional view of the lens of Example 5.
- L1 is a first lens
- L2 is a second lens
- L3 is a third lens
- L4 is a fourth lens
- L5 is a fifth lens
- S is an aperture stop
- I is an imaging surface.
- F is a parallel plate assuming an optical low-pass filter, an IR cut filter, a seal glass of a solid-state image sensor, or the like.
- FIG. 12 is an aberration diagram of Example 5 (spherical aberration, astigmatism, distortion, and meridional coma).
- the first lens L1 and the second lens L2 are made of glass mold lenses, and the other lenses are made of a plastic material, and the first lens L1 is used for focusing with auto focus, macro switching function, or the like.
- To the third lens L3 is assumed to be a partial group extension.
- FIG. 13 is a sectional view of the lens of Example 6.
- L1 is a first lens
- L2 is a second lens
- L3 is a third lens
- L4 is a fourth lens
- L5 is a fifth lens
- S is an aperture stop
- I is an imaging surface.
- F is a parallel plate assuming an optical low-pass filter, an IR cut filter, a seal glass of a solid-state image sensor, or the like.
- FIG. 14 is an aberration diagram of Example 6 (spherical aberration, astigmatism, distortion, and meridional coma).
- all the lenses are made of a plastic material, and a partial group is formed by moving the first lens L1 to the third lens L3 as a single unit for focus position adjustment in an autofocus or macro switching function. It is supposed to be paid out.
- FIG. 15 is a sectional view of the lens of Example 7.
- L1 is a first lens
- L2 is a second lens
- L3 is a third lens
- L4 is a fourth lens
- L5 is a fifth lens
- S is an aperture stop
- I is an imaging surface.
- F is a parallel plate assuming an optical low-pass filter, an IR cut filter, a seal glass of a solid-state image sensor, or the like.
- FIG. 16 is an aberration diagram of Example 7 (spherical aberration, astigmatism, distortion, and meridional coma).
- all the lenses are made of a plastic material, and a partial group is formed by moving the first lens L1 to the third lens L3 as a single unit for focus position adjustment in an autofocus or macro switching function. It is supposed to be paid out.
- FIG. 17 is a sectional view of the lens of Example 8.
- L1 is a first lens
- L2 is a second lens
- L3 is a third lens
- L4 is a fourth lens
- L5 is a fifth lens
- S is an aperture stop
- I is an imaging surface.
- F is a parallel plate assuming an optical low-pass filter, an IR cut filter, a seal glass of a solid-state image sensor, or the like.
- FIG. 18 is an aberration diagram of Example 8 (spherical aberration, astigmatism, distortion, and meridional coma).
- all the lenses are made of a plastic material, and a partial group is formed by moving the first lens L1 to the third lens L3 as a single unit for focus position adjustment in an autofocus or macro switching function. It is supposed to be paid out.
- Example 9 The overall specification of the imaging lens of Example 9 is shown below.
- FIG. 19 is a sectional view of the lens of Example 9.
- L1 is a first lens
- L2 is a second lens
- L3 is a third lens
- L4 is a fourth lens
- L5 is a fifth lens
- S is an aperture stop
- I is an imaging surface.
- F is a parallel plate assuming an optical low-pass filter, an IR cut filter, a seal glass of a solid-state image sensor, or the like.
- FIG. 20 is an aberration diagram of Example 9 (spherical aberration, astigmatism, distortion, and meridional coma).
- all the lenses are made of a plastic material, and a partial group is formed by moving the first lens L1 to the third lens L3 as a single unit for focus position adjustment in an autofocus or macro switching function. It is supposed to be paid out.
- the plastic material has a large refractive index change when the temperature changes, if all of the first lens L1 to the fifth lens L5 are made of plastic lenses, the image point of the entire imaging lens system when the ambient temperature changes. The problem is that the position will fluctuate.
- inorganic fine particles can be mixed in a plastic material to reduce the temperature change of the plastic material. More specifically, mixing fine particles with a transparent plastic material generally causes light scattering and lowers the transmittance, so it was difficult to use as an optical material. By making it smaller than the wavelength, it is possible to substantially prevent scattering.
- the refractive index of the plastic material decreases with increasing temperature, but the refractive index of inorganic particles increases with increasing temperature. Therefore, it is possible to make almost no change in the refractive index by using these temperature dependencies so as to cancel each other.
- a plastic material with extremely low temperature dependency of the refractive index is obtained.
- a plastic material with extremely low temperature dependency of the refractive index is obtained.
- the refractive index change due to temperature change can be reduced.
- the temperature change of the entire imaging lens system is achieved. It is possible to suppress the image point position fluctuation at the time.
- an energy curable resin as the material of the imaging lens, since the optical performance degradation when exposed to high temperatures is small compared to a lens using a thermoplastic resin such as polycarbonate or polyolefin, It is effective for the reflow process, is easier to manufacture than a glass mold lens, is inexpensive, and can achieve both low cost and mass productivity of an imaging apparatus incorporating an imaging lens.
- the energy curable resin refers to both a thermosetting resin and an ultraviolet curable resin.
- the plastic lens of the present invention may be formed using the aforementioned energy curable resin.
- the principal ray incident angle of the light beam incident on the imaging surface of the solid-state imaging device is not necessarily designed to be sufficiently small in the periphery of the imaging surface.
- recent techniques have made it possible to reduce shading by reviewing the arrangement of the color filters of the solid-state imaging device and the on-chip microlens array. Specifically, if the pitch of the arrangement of the color filters and the on-chip microlens array is set slightly smaller than the pixel pitch of the imaging surface of the imaging device, the color filter or Since the on-chip microlens array is shifted to the optical axis side of the imaging lens, the obliquely incident light beam can be efficiently guided to the light receiving portion of each pixel. Thereby, the shading which generate
- the present embodiment is a design example aiming at further miniaturization with respect to the portion where the requirement is relaxed.
Abstract
Description
但し、
L:撮像レンズ全系の最も物体側のレンズ面から像側焦点までの光軸上の距離
2Y:固体撮像素子の撮像面対角線長(固体撮像素子の矩形実効画素領域の対角線長)
ここで、像側焦点とは撮像レンズに光軸と平行な平行光線が入射した場合の像点をいう。
物体側より順に、開口絞りと、正の屈折力を有し物体側に凸面を向けた第1レンズと、負の屈折力を有し像側に凹面を向けた第2レンズと、正の屈折力を有し像側に凸面を向けた第3レンズと、正の屈折力を有し像側に凸面を向けてメニスカス形状を有する第4レンズと、負の屈折力を有し像側に凹面を向けた第5レンズと、から成り、以下の条件式を満足することを特徴とする撮像レンズ。
0.8<SL/f<1.5 (2)
但し、
r7:前記第4レンズ物体側面の曲率半径
r8:前記第4レンズ像側面の曲率半径
SL:前記開口絞りから像側焦点までの光軸上の距離
f:撮像レンズ全系の焦点距離
小型で収差の良好に補正された撮像レンズを得るための本発明の基本構成は、開口絞り、正の屈折力を有し物体側に凸面を向けた第1レンズと、負の屈折力を有し像側に凹面を向けた第2レンズと、正の屈折力を有し像側に凸面を向けた第3レンズと、正の屈折力を有し像側に凸面を向けてメニスカス形状の第4レンズと、負の屈折力を有し像側に凹面を向けた第5レンズと、から成る。物体側より順に、第1レンズ、第2レンズ、第3レンズ、第4レンズから成る正レンズ群と、負の第5レンズとを配置する所謂テレフォトタイプのこのレンズ構成は撮像レンズ全長の短縮化には有利な構成である。更に、5枚構成のうち2枚を負レンズとすることで、発散作用を有する面を多くしてペッツバール和の補正を容易とし、画面周辺部まで良好な結像性能を確保した撮像レンズを得ることが可能となる。
但し、
f4:前記第4レンズの焦点距離
f:撮像レンズ全系の焦点距離
条件式(3)は、第4レンズの焦点距離と全系の焦点距離の比を規定している。全長の短縮化に伴い、全系の焦点距離と同様にバックフォーカスも短くなり、撮像レンズの最も像側の面と像側焦点位置との間に、光学的ローパスフィルタ、赤外線カットフィルタ、若しくは固体撮像素子パッケージのシールガラス等の平行平板を配置するスペースの確保が困難となる場合がある。また、条件式(1)の範囲を満たすことによってもバックフォーカスは確保できるが、全系の焦点距離も長くなりすぎてしまう場合がある。それに対し、条件式(1)の範囲を満たしつつ、条件式(3)の上限値を下回ることによって、第4レンズの屈折力が強くなるので、バックフォーカスを確保しつつ、全系の焦点距離を保つことが出来る。一方で、条件式(3)の下限値を上回ることによって、第4レンズの正の屈折力を適度に維持することが出来るので、レンズ全長の短縮化及び像面湾曲や歪曲収差等の軸外諸収差の補正を良好に抑えることが出来る。
但し、
f3:前記第3レンズの焦点距離
f4:前記第4レンズの焦点距離
条件式(4)は、第3レンズと第4レンズの焦点距離の比を規定している。条件式(4)の上限値を下回ることで第3レンズの屈折力を適度に維持することができ、第1レンズから第4レンズの合成主点をより物体側へ配置することができ、撮像レンズ全長を短縮化することができる。一方、下限値を上回ることによって、第3レンズの屈折力をより像側の第4レンズに分担させることによって全系の焦点距離を確保することができる。
但し、
ν1:前記第1レンズのアッベ数
ν2:前記第2レンズのアッベ数
条件式(5)は、撮像レンズ全系の色収差を良好に補正するための条件式である。条件式(5)の下限を上回ることで、軸上色収差や倍率色収差などの色収差をバランス良く補正することができる。一方、上限を下回ることで、入手しやすい硝材で構成することができる。
5.以下の条件式を満足することを特徴とする前記1~4の何れか1項に記載の撮像レンズ。
但し、
n2:前記第2レンズのd線に対する屈折率
条件式(6)は、撮像レンズ全系の色収差、像面湾曲を良好に補正するための条件式である。条件式(6)の値が下限を上回ることで、比較的分散の大きな第2レンズの屈折力を適度に維持することができ、色収差、像面湾曲を良好に補正することができる。一方、上限を下回ることで、入手し易い硝材で構成することができる。
6.第1レンズから第3レンズを移動させて焦点位置合わせを行い、以下の条件式を満足することを特徴とする前記1~5の何れか1項に記載の撮像レンズ。
但し、
d6:前記第3レンズと前記第4レンズの軸上の空気間隔
f:撮像レンズ全系の焦点距離
オートフォーカスやマクロ切り替え機能等で焦点位置合わせをしようとした場合、通常はレンズ群全体を光軸方向に移動させて行う全体繰り出しが一般的であるが、レンズ群の一部分、例えば第1レンズから第3レンズまでを光軸方向に移動させて焦点位置合わせを行う部分群繰り出しも可能である。部分群繰り出しにすると、光学系によっては、近距離への焦点位置合わせ時の性能劣化を低減することができ、移動群がレンズ全体ではなく一部分でよいため、駆動機構を簡略化でき、撮像装置全体の小型軽量化を達成することができるといったメリットが得られる。
fB:バックフォーカス
F:Fナンバー
2Y:固体撮像素子の撮像面対角線長
ENTP:入射瞳位置(第1面から入射瞳位置までの距離)
EXTP:射出瞳位置(撮像面から射出瞳位置までの距離)
H1:前側主点位置(第1面から前側主点位置までの距離)
H2:後側主点位置(最終面から後側主点位置までの距離)
R:曲率半径
D:軸上面間隔
Nd:レンズ材料のd線に対する屈折率
νd:レンズ材料のアッベ数
なお、面データにおいて、R,D及び有効半径の単位はmmである。
Ai:i次の非球面係数
R :曲率半径
K :円錐定数
また、非球面係数において、10のべき乗数(例えば2.5×10-02)をE(例えば2.5E-02)を用いて表す。
(実施例1)
・撮像レンズの全体緒元を以下に示す。
fB=0.48mm
F=2.88
2Y=7.016mm
ENTP=0mm
EXTP=-2.97mm
H1=-1.59mm
H2=-4.15mm
・撮像レンズの面データを以下に示す。
1(絞り) ∞ -0.050 0.80
2(*) 2.033 0.686 1.54470 56.2 0.88
3(*) -12.786 0.050 0.96
4(*) 8.852 0.300 1.63200 23.4 0.98
5(*) 2.389 0.591 1.03
6(*) -8.677 0.642 1.54470 56.2 1.20
7(*) -3.322 0.483 1.42
8(*) -2.286 0.738 1.54470 56.2 1.65
9(*) -1.192 0.464 1.87
10(*) -18.636 0.540 1.54470 56.2 2.41
11(*) 1.450 0.600 2.97
12 ∞ 0.145 1.51630 64.1 3.28
13 ∞ 3.32
・撮像レンズの非球面係数を以下に示す。
K=0.12198E+00,A4=-0.71072E-03,A6=-0.86790E-03,
A8=-0.80391E-02,A10=0.97290E-03,A12=0.57532E-02,
A14=-0.32178E-02
第3面
K=0.30000E+02,A4=0.74126E-02,A6=-0.13036E-01,
A8=0.61402E-02,A10=0.18251E-02,A12=-0.36657E-02,
A14=0.36286E-02
第4面
K=0.19169E+00,A4=-0.40663E-01,A6=0.25243E-01,
A8=-0.30394E-02,A10=0.38707E-02,A12=0.10939E-02,
A14=-0.13121E-02
第5面
K=-0.59793E+01,A4=0.11737E-01,A6=0.26830E-01,
A8=-0.45536E-02,A10=0.49326E-02,A12=0.30501E-03,
A14=-0.79395E-03
第6面
K=0.28708E+02,A4=-0.35476E-01,A6=-0.81047E-02,
A8=0.41706E-02,A10=0.13542E-02,A12=0.97322E-03,
A14=0.10377E-02
第7面
K=0.15874E+01,A4=-0.18118E-01,A6=-0.29331E-02,
A8=-0.84815E-03,A10=0.40327E-03,A12=0.47645E-03,
A14=0.21365E-03
第8面
K=-0.49021E-01,A4=0.17792E-01,A6=0.53331E-03,
A8=0.59862E-03,A10=-0.14526E-04,A12=-0.10324E-04,
A14=0.86216E-05
第9面
K=-0.31540E+01,A4=-0.39857E-01,A6=0.16012E-01,
A8=-0.20775E-02,A10=0.20495E-03,A12=-0.81553E-05,
A14=0.30220E-06
第10面
K=0.27379E+02,A4=-0.44134E-01,A6=0.75013E-02,
A8=-0.22670E-03,A10=-0.11611E-03,A12=0.24952E-04,
A14=-0.15619E-05
第11面
K=-0.73425E+01,A4=-0.33704E-01,A6=0.64660E-02,
A8=-0.91521E-03,A10=0.65512E-04,A12=-0.24773E-05,
A14=0.56535E-07
・撮像レンズの単レンズデータを以下に示す。
1 2 3.273
2 4 -5.272
3 6 9.480
4 8 3.692
5 10 -2.447
・撮像レンズの条件式(1)~(8)に対応する値を以下に示す。
(1)(r7+r8)/(r7-r8)=3.178
(2)SL/f=1.214
(3)f4/f=0.798
(4)f3/f4=2.568
(5)ν1-ν2=32.6
(6)n2=1.632
(7)d6/f=0.104
(8)L/2Y=0.79
図3は撮像レンズの断面図である。L1は第1レンズ、L2は第2レンズ、L3は第3レンズ、L4は第4レンズ、L5は第5レンズ、Sは開口絞り、Iは撮像面を示す。また、Fは光学的ローパスフィルタやIRカットフィルタ、固体撮像素子のシールガラス等を想定した平行平板である。図4は撮像レンズの収差図(球面収差、非点収差、歪曲収差、メリディオナルコマ収差)である。
(実施例2)
・撮像レンズの全体緒元を以下に示す。
fB=0.5mm
F=2.88
2Y=7.016mm
ENTP=0mm
EXTP=-2.75mm
H1=-4.21mm
H2=-5.17mm
・撮像レンズの面データを以下に示す。
1(絞り) ∞ -0.210 0.98
2(*) 1.789 0.762 1.54470 56.2 1.04
3(*) 32.773 0.050 1.03
4(*) 8.946 0.300 1.63200 23.4 1.03
5(*) 2.457 0.787 1.03
6(*) -7.885 0.863 1.54470 56.2 1.30
7(*) -3.100 0.600 1.57
8(*) -2.496 0.544 1.54470 56.2 1.79
9(*) -1.854 0.910 1.96
10(*) -3.401 0.450 1.54470 56.2 2.29
11(*) 3.725 0.300 2.82
12 ∞ 0.145 1.51630 64.1 3.26
13 ∞ 3.30
・撮像レンズの非球面係数を以下に示す。
K=0.25491E+00,A4=0.16645E-02,A6=0.23998E-02,
A8=-0.65481E-03,A10=0.17917E-03,A12=0.33827E-02,
A14=-0.76817E-03
第3面
K=-0.30000E+02,A4=0.91582E-02,A6=0.92103E-02,
A8=0.11014E-01,A10=0.27918E-02,A12=-0.57226E-02,
A14=0.82212E-03
第4面
K=0.25687E+02,A4=-0.21604E-01,A6=0.22333E-01,
A8=-0.13785E-02,A10=0.25428E-02,A12=-0.19960E-02,
A14=-0.55690E-02
第5面
K=-0.25703E+01,A4=0.25673E-01,A6=0.30181E-01,
A8=-0.18004E-02,A10=0.62950E-02,A12=-0.14319E-02,
A14=-0.27246E-03
第6面
K=0.29426E+02,A4=-0.28196E-01,A6=-0.23682E-02,
A8=0.72490E-03,A10=-0.15095E-02,A12=0.39723E-03,
A14=0.10607E-02
第7面
K=0.13046E+01,A4=-0.20555E-01,A6=0.14491E-02,
A8=-0.22122E-02,A10=-0.58787E-04,A12=0.63240E-04,
A14=0.45587E-04
第8面
K=0.55833E+00,A4=0.54873E-02,A6=-0.18708E-02,
A8=0.10416E-02,A10=-0.99807E-04,A12=0.57013E-05,
A14=0.30343E-04
第9面
K=-0.44160E+01,A4=-0.44178E-01,A6=0.10161E-01,
A8=-0.21360E-02,A10=0.34269E-03,A12=0.99841E-05,
A14=0.36643E-06
第10面
K=0.45260E+00,A4=-0.51468E-01,A6=0.93903E-02,
A8=-0.98822E-04,A10=-0.10497E-03,A12=0.25662E-04,
A14=-0.18668E-05
第11面
K=-0.35812E+02,A4=-0.40083E-01,A6=0.56390E-02,
A8=-0.71357E-03,A10=0.73512E-04,A12=-0.44111E-05,
A14=0.10307E-06
・撮像レンズの単レンズデータを以下に示す。
1 2 3.445
2 4 -5.457
3 6 8.818
4 8 10.193
5 10 -3.193
・撮像レンズの条件式(1)~(8)に対応する値を以下に示す。
(1)(r7+r8)/(r7-r8)=6.776
(2)SL/f=1.050
(3)f4/f=1.799
(4)f3/f4=0.865
(5)ν1-ν2=32.6
(6)n2=1.632
(7)d6/f=0.106
(8)L/2Y=0.86
図5は実施例2の撮像レンズの断面図である。L1は第1レンズ、L2は第2レンズ、L3は第3レンズ、L4は第4レンズ、L5は第5レンズ、Sは開口絞り、Iは撮像面を示す。また、Fは光学的ローパスフィルタやIRカットフィルタ、固体撮像素子のシールガラス等を想定した平行平板である。図6は実施例2の撮像レンズの収差図(球面収差、非点収差、歪曲収差、メリディオナルコマ収差)である。
(実施例3)
・撮像レンズの全体緒元を以下に示す。
fB=0.49mm
F=2.88
2Y=7.016mm
ENTP=0mm
EXTP=-2.91mm
H1=-1.88mm
H2=-4.25mm
・撮像レンズの面データを以下に示す。
1(絞り) ∞ -0.073 0.84
2(*) 1.934 0.667 1.49700 81.6 0.92
3(*) -47.809 0.073 0.98
4(*) 4.766 0.300 1.63200 23.4 1.03
5(*) 2.342 0.589 1.05
6(*) -9.253 0.632 1.54470 56.2 1.20
7(*) -4.123 0.493 1.40
8(*) -2.489 0.734 1.54470 56.2 1.59
9(*) -1.198 0.446 1.87
10(*) -14.235 0.539 1.54470 56.2 2.43
11(*) 1.443 0.600 2.95
12 ∞ 0.145 1.51630 64.1 3.28
13 ∞ 3.32
・撮像レンズの非球面係数を以下に示す。
K=0.13772E+00,A4=-0.87773E-03,A6=0.18123E-02,
A8=-0.60787E-02,A10=0.21615E-02,A12=0.58622E-02,
A14=-0.28350E-02
第3面
K=0.30000E+02,A4=0.79602E-02,A6=-0.38490E-03,
A8=0.10461E-01,A10=0.12913E-02,A12=-0.44337E-02,
A14=0.43425E-02
第4面
K=0.35590E+01,A4=-0.36662E-01,A6=0.26138E-01,
A8=-0.16470E-02,A10=0.43560E-02,A12=0.63515E-03,
A14=-0.13734E-02
第5面
K=-0.49965E+01,A4=0.11670E-01,A6=0.23574E-01,
A8=-0.49020E-02,A10=0.63906E-02,A12=0.16798E-02,
A14=-0.72456E-03
第6面
K=0.27405E+02,A4=-0.37115E-01,A6=-0.68643E-02,
A8=0.44963E-02,A10=0.98719E-03,A12=0.80935E-03,
A14=0.14102E-02
第7面
K=0.24832E+01,A4=-0.24318E-01,A6=-0.36567E-02,
A8=-0.10321E-02,A10=0.53577E-03,A12=0.60029E-03,
A14=0.25186E-03
第8面
K=0.30214E+00,A4=0.11961E-01,A6=-0.30818E-02,
A8=0.36932E-04,A10=-0.32668E-04,A12=0.12716E-04,
A14=0.68304E-05
第9面
K=-0.33156E+01,A4=-0.39887E-01,A6=0.16135E-01,
A8=-0.23062E-02,A10=0.13288E-03,A12=-0.15866E-04,
A14=0.38298E-05
第10面
K=0.20282E+02,A4=-0.40585E-01,A6=0.76051E-02,
A8=-0.24424E-03,A10=-0.12022E-03,A12=0.24613E-04,
A14=-0.14874E-05
第11面
K=-0.78153E+01,A4=-0.33411E-01,A6=0.64388E-02,
A8=-0.94677E-03,A10=0.70562E-04,A12=-0.26550E-05,
A14=0.54331E-07
・撮像レンズの単レンズデータを以下に示す。
レンズ 始面 焦点距離(mm)
1 2 3.756
2 4 -7.651
3 6 13.085
4 8 3.530
5 10 -2.376
・撮像レンズの条件式(1)~(8)に対応する値を以下に示す。
(1)(r7+r8)/(r7-r8)=2.855
(2)SL/f=1.177
(3)f4/f=0.743
(4)f3/f4=3.707
(5)ν1-ν2=58.2
(6)n2=1.632
(7)d6/f=0.104
(8)L/2Y=0.79
図7は実施例3のレンズの断面図である。L1は第1レンズ、L2は第2レンズ、L3は第3レンズ、L4は第4レンズ、L5は第5レンズ、Sは開口絞り、Iは撮像面を示す。また、Fは光学的ローパスフィルタやIRカットフィルタ、固体撮像素子のシールガラス等を想定した平行平板である。図8は実施例3の収差図(球面収差、非点収差、歪曲収差、メリディオナルコマ収差)である。
(実施例4)
・撮像レンズの全体緒元を以下に示す。
fB=0.47mm
F=2.88
2Y=7.016mm
ENTP=0mm
EXTP=-2.95mm
H1=-1.8mm
H2=-4.26mm
・撮像レンズの面データを以下に示す。
1(絞り) ∞ -0.034 0.82
2(*) 2.013 0.808 1.54470 56.2 0.91
3(*) -5.260 0.050 1.00
4(*) -15.895 0.300 1.58300 30.0 1.00
5(*) 2.591 0.572 1.07
6(*) -19.256 0.674 1.54470 56.2 1.25
7(*) -3.813 0.455 1.48
8(*) -2.126 0.699 1.54470 56.2 1.66
9(*) -1.180 0.496 1.89
10(*) -13.874 0.450 1.54470 56.2 2.42
11(*) 1.492 0.600 2.93
12 ∞ 0.145 1.51630 64.1 3.28
13 ∞ 3.32
・撮像レンズの非球面係数を以下に示す。
K=0.10080E-01,A4=-0.28888E-02,A6=-0.39224E-02,
A8=-0.10095E-01,A10=-0.64321E-03,A12=0.33368E-02,
A14=-0.83855E-02
第3面
K=0.17593E+02,A4=0.68989E-02,A6=-0.24476E-01,
A8=-0.51515E-04,A10=-0.66266E-03,A12=-0.60012E-02,
A14=-0.13841E-02
第4面
K=0.30000E+02,A4=-0.50797E-01,A6=0.19979E-01,
A8=-0.86800E-02,A10=-0.17009E-02,A12=-0.22618E-02,
A14=-0.17768E-02
第5面
K=-0.78722E+01,A4=0.15937E-01,A6=0.31316E-01,
A8=-0.61323E-02,A10=0.44388E-02,A12=0.45833E-03,
A14=-0.16503E-02
第6面
K=0.30000E+02,A4=-0.35955E-01,A6=-0.76287E-02,
A8=0.37009E-02,A10=-0.80047E-04,A12=-0.58720E-05,
A14=0.76127E-03
第7面
K=0.15645E+01,A4=-0.17291E-01,A6=-0.25578E-02,
A8=-0.95646E-03,A10=0.34055E-03,A12=0.34349E-03,
A14=0.45210E-04
第8面
K=-0.13631E+00,A4=0.18926E-01,A6=0.12474E-02,
A8=0.88858E-03,A10=-0.19331E-04,A12=-0.29333E-04,
A14=0.49655E-05
第9面
K=-0.31788E+01,A4=-0.40092E-01,A6=0.16751E-01,
A8=-0.20937E-02,A10=0.19050E-03,A12=-0.10806E-04,
A14=-0.10048E-05
第10面
K=0.12332E+02,A4=-0.44348E-01,A6=0.76586E-02,
A8=-0.21917E-03,A10=-0.11885E-03,A12=0.24712E-04,
A14=-0.15356E-05
第11面
K=-0.80799E+01,A4=-0.35226E-01,A6=0.66057E-02,
A8=-0.91396E-03,A10=0.65503E-04,A12=-0.26811E-05,
A14=0.73417E-07
・撮像レンズの単レンズデータを以下に示す。
1 2 2.782
2 4 -3.799
3 6 8.595
4 8 3.865
5 10 -2.448
・撮像レンズの条件式(1)~(8)に対応する値を以下に示す。
(1)(r7+r8)/(r7-r8)=3.497
(2)SL/f=1.192
(3)f4/f=0.818
(4)f3/f4=2.224
(5)ν1-ν2=26.0
(6)n2=1.583
(7)d6/f=0.096
(8)L/2Y=0.79
図9は実施例4のレンズの断面図である。L1は第1レンズ、L2は第2レンズ、L3は第3レンズ、L4は第4レンズ、L5は第5レンズ、Sは開口絞り、Iは撮像面を示す。また、Fは光学的ローパスフィルタやIRカットフィルタ、固体撮像素子のシールガラス等を想定した平行平板である。図10は実施例4の収差図(球面収差、非点収差、歪曲収差、メリディオナルコマ収差)である。
(実施例5)
・撮像レンズの全体緒元を以下に示す。
fB=0.51mm
F=2.88
2Y=7.016mm
ENTP=0mm
EXTP=-2.88mm
H1=-1.94mm
H2=-4.25mm
・撮像レンズの面データを以下に示す。
1(絞り) ∞ -0.077 0.84
2(*) 1.919 0.657 1.49700 81.6 0.93
3(*) 411.614 0.052 0.99
4(*) 3.420 0.321 2.00020 19.3 1.04
5(*) 2.290 0.596 1.02
6(*) -7.380 0.590 1.54470 56.2 1.17
7(*) -4.183 0.457 1.37
8(*) -2.723 0.791 1.54470 56.2 1.56
9(*) -1.204 0.471 1.85
10(*) -14.440 0.520 1.54470 56.2 2.43
11(*) 1.429 0.600 2.94
12 ∞ 0.145 1.51630 64.1 3.26
13 ∞ 3.30
・撮像レンズの非球面係数を以下に示す。
K=0.14541E+00,A4=-0.77607E-03,A6=0.24189E-02,
A8=-0.58371E-02,A10=0.19501E-02,A12=0.56443E-02,
A14=-0.24883E-02
第3面
K=-0.30000E+02,A4=0.65178E-02,A6=0.79156E-02,
A8=0.11430E-01,A10=-0.99688E-03,A12=-0.63741E-02,
A14=0.27807E-02
第4面
K=0.35535E+01,A4=-0.35136E-01,A6=0.23600E-01,
A8=-0.35482E-02,A10=0.29306E-02,A12=-0.27257E-03,
A14=-0.19308E-02
第5面
K=-0.41861E+01,A4=0.14176E-01,A6=0.23207E-01,
A8=-0.40956E-02,A10=0.74584E-02,A12=0.16841E-02,
A14=-0.17571E-02
第6面
K=0.28776E+02,A4=-0.43642E-01,A6=-0.75156E-02,
A8=0.62048E-02,A10=0.23665E-02,A12=0.19778E-02,
A14=0.23745E-02
第7面
K=0.33134E+01,A4=-0.30011E-01,A6=-0.44610E-02,
A8=-0.13122E-02,A10=0.78615E-03,A12=0.85884E-03,
A14=0.42316E-03
第8面
K=0.45439E+00,A4=0.10788E-01,A6=-0.47480E-02,
A8=0.99177E-05,A10=-0.10193E-03,A12=-0.15417E-04,
A14=0.15175E-04
第9面
K=-0.33457E+01,A4=-0.40916E-01,A6=0.16615E-01,
A8=-0.24657E-02,A10=0.75700E-04,A12=-0.18737E-04,
A14=0.77174E-05
第10面
K=0.17625E+02,A4=-0.42342E-01,A6=0.79897E-02,
A8=-0.23043E-03,A10=-0.12757E-03,A12=0.24049E-04,
A14=-0.13779E-05
第11面
K=-0.76520E+01,A4=-0.34264E-01,A6=0.65689E-02,
A8=-0.97420E-03,A10=0.75519E-04,A12=-0.30450E-05,
A14=0.64750E-07
・撮像レンズの単レンズデータを以下に示す。
1 2 3.877
2 4 -8.083
3 6 16.644
4 8 3.349
5 10 -2.361
・撮像レンズの条件式(1)~(8)に対応する値を以下に示す。
(1)(r7+r8)/(r7-r8)=2.585
(2)SL/f=1.173
(3)f4/f=0.703
(4)f3/f4=4.970
(5)ν1-ν2=62.3
(6)n2=2.000
(7)d6/f=0.099
(8)L/2Y=0.79
図11は実施例5のレンズの断面図である。L1は第1レンズ、L2は第2レンズ、L3は第3レンズ、L4は第4レンズ、L5は第5レンズ、Sは開口絞り、Iは撮像面を示す。また、Fは光学的ローパスフィルタやIRカットフィルタ、固体撮像素子のシールガラス等を想定した平行平板である。図12は実施例5の収差図(球面収差、非点収差、歪曲収差、メリディオナルコマ収差)である。
(実施例6)
・撮像レンズの全体緒元を以下に示す。
fB=0.7mm
F=2.88
2Y=7.016mm
ENTP=0mm
EXTP=-3.36mm
H1=-1.17mm
H2=-4.31mm
・撮像レンズの面データを以下に示す。
1(絞り) ∞ -0.052 0.87
2(*) 1.963 0.740 1.54470 56.2 0.99
3(*) -25.320 0.053 1.03
4(*) 6.156 0.300 1.63200 23.4 1.05
5(*) 2.124 0.706 1.07
6(*) -7.235 0.700 1.54470 56.2 1.26
7(*) -3.210 0.458 1.51
8(*) -2.056 0.813 1.54470 56.2 1.69
9(*) -1.110 0.400 1.92
10(*) -19.798 0.491 1.54470 56.2 2.49
11(*) 1.505 0.600 2.92
12 ∞ 0.145 1.51630 64.1 3.24
13 ∞ 3.27
・撮像レンズの非球面係数を以下に示す。
K=0.22872E+00,A4=0.11258E-02,A6=0.35117E-02,
A8=-0.63204E-02,A10=0.79095E-03,A12=0.54005E-02,
A14=-0.20981E-02
第3面
K=-0.30000E+02,A4=0.14026E-01,A6=-0.80919E-02,
A8=0.71966E-02,A10=0.20250E-02,A12=-0.43477E-02,
A14=0.22859E-02
第4面
K=-0.46024E+01,A4=-0.42217E-01,A6=0.25928E-01,
A8=-0.38047E-02,A10=0.14132E-02,A12=-0.74428E-03,
A14=-0.18697E-02
第5面
K=-0.51139E+01,A4=0.15116E-01,A6=0.27060E-01,
A8=-0.51308E-02,A10=0.53222E-02,A12=0.53802E-03,
A14=-0.16078E-02
第6面
K=0.22607E+02,A4=-0.34517E-01,A6=-0.95045E-02,
A8=0.32882E-02,A10=0.10679E-03,A12=0.41400E-03,
A14=0.12149E-02
第7面
K=0.16520E+01,A4=-0.16488E-01,A6=-0.28195E-02,
A8=-0.12173E-02,A10=0.72136E-04,A12=0.27934E-03,
A14=0.11888E-03
第8面
K=-0.11817E+00,A4=0.98232E-02,A6=0.13191E-02,
A8=0.84171E-03,A10=-0.45299E-04,A12=-0.19156E-04,
A14=0.21201E-04
第9面
K=-0.29968E+01,A4=-0.53098E-01,A6=0.15866E-01,
A8=-0.21642E-02,A10=0.21132E-03,A12=0.34310E-06,
A14=0.16613E-05
第10面
K=-0.33298E+01,A4=-0.43356E-01,A6=0.74354E-02,
A8=-0.25845E-03,A10=-0.12248E-03,A12=0.24598E-04,
A14=-0.13977E-05
第11面
K=-0.84033E+01,A4=-0.37344E-01,A6=0.65139E-02,
A8=-0.88701E-03,A10=0.66015E-04,A12=-0.28215E-05,
A14=0.77371E-07
・撮像レンズの単レンズデータを以下に示す。
1 2 3.376
2 4 -5.282
3 6 9.982
4 8 3.397
5 10 -2.547
・撮像レンズの条件式(1)~(8)に対応する値を以下に示す。
(1)(r7+r8)/(r7-r8)=3.344
(2)SL/f=1.198
(3)f4/f=0.677
(4)f3/f4=2.938
(5)ν1-ν2=32.6
(6)n2=1.632
(7)d6/f=0.091
(8)L/2Y=0.85
図13は実施例6のレンズの断面図である。L1は第1レンズ、L2は第2レンズ、L3は第3レンズ、L4は第4レンズ、L5は第5レンズ、Sは開口絞り、Iは撮像面を示す。また、Fは光学的ローパスフィルタやIRカットフィルタ、固体撮像素子のシールガラス等を想定した平行平板である。図14は実施例6の収差図(球面収差、非点収差、歪曲収差、メリディオナルコマ収差)である。
(実施例7)
・撮像レンズの全体緒元を以下に示す。
fB=0.7mm
F=2.8
2Y=7.016mm
ENTP=0mm
EXTP=-3.89mm
H1=-0.08mm
H2=-3.97mm
・撮像レンズの面データを以下に示す。
1(絞り) ∞ 0.050 0.83
2(*) 7.940 0.800 1.54470 56.2 0.85
3(*) -2.469 0.101 1.07
4(*) 3.895 0.426 1.63200 23.4 1.26
5(*) 1.632 1.001 1.32
6(*) 26.607 1.175 1.54470 56.2 1.82
7(*) -3.200 0.400 2.00
8(*) -1.734 0.486 1.54470 56.2 2.09
9(*) -1.029 0.100 2.16
10(*) 3.454 0.533 1.54470 56.2 2.46
11(*) 0.917 0.600 3.01
12 ∞ 0.300 1.51630 64.1 3.20
13 ∞ 3.27
・撮像レンズの非球面係数を以下に示す。
K=-0.30000E+02,A4=-0.25530E-01,A6=-0.10297E-01,
A8=-0.15329E-01,A10=0.10320E-01,A12=-0.51000E-03,
A14=-0.20491E-02
第3面
K=-0.22044E+01,A4=0.40354E-02,A6=-0.37192E-01,
A8=0.14675E-01,A10=0.47227E-03,A12=-0.65765E-02,
A14=0.31637E-02
第4面
K=-0.10853E+02,A4=-0.32693E-01,A6=0.25188E-01,
A8=-0.10304E-01,A10=0.23617E-02,A12=0.16228E-02,
A14=-0.67773E-03
第5面
K=-0.45099E+01,A4=-0.79349E-02,A6=0.16704E-01,
A8=-0.97214E-02,A10=0.26187E-02,A12=0.39605E-03,
A14=-0.19963E-03
第6面
K=0.90364E+01,A4=0.68755E-02,A6=-0.10416E-01,
A8=0.35310E-02,A10=0.25200E-03,A12=-0.34061E-03,
A14=0.47853E-04
第7面
K=0.59479E+00,A4=0.12962E-01,A6=-0.40194E-02,
A8=-0.11527E-03,A10=0.11669E-03,A12=0.28478E-04,
A14=-0.49433E-05
第8面
K=-0.43179E+00,A4=0.37096E-01,A6=0.98140E-03,
A8=0.92866E-03,A10=-0.30222E-04,A12=-0.28923E-04,
A14=0.62055E-05
第9面
K=-0.37450E+01,A4=-0.55748E-01,A6=0.20347E-01,
A8=-0.20951E-02,A10=0.20454E-03,A12=-0.94418E-05,
A14=-0.12837E-05
第10面
K=-0.56635E+01,A4=-0.80954E-01,A6=0.10365E-01,
A8=-0.31383E-05,A10=-0.13946E-03,A12=0.20848E-04,
A14=-0.10865E-05
第11面
K=-0.43287E+01,A4=-0.39994E-01,A6=0.66722E-02,
A8=-0.91607E-03,A10=0.85074E-04,A12=-0.46694E-05,
A14=0.10462E-06
・撮像レンズの単レンズデータを以下に示す。
1 2 3.554
2 4 -4.796
3 6 5.319
4 8 3.741
5 10 -2.475
・撮像レンズの条件式(1)~(8)に対応する値を以下に示す。
(1)(r7+r8)/(r7-r8)=3.922
(2)SL/f=1.407
(3)f4/f=0.801
(4)f3/f4=1.422
(5)ν1-ν2=32.6
(6)n2=1.632
(7)d6/f=0.086
(8)L/2Y=0.93
図15は実施例7のレンズの断面図である。L1は第1レンズ、L2は第2レンズ、L3は第3レンズ、L4は第4レンズ、L5は第5レンズ、Sは開口絞り、Iは撮像面を示す。また、Fは光学的ローパスフィルタやIRカットフィルタ、固体撮像素子のシールガラス等を想定した平行平板である。図16は実施例7の収差図(球面収差、非点収差、歪曲収差、メリディオナルコマ収差)である。
(実施例8)
・撮像レンズの全体緒元を以下に示す。
fB=0.79mm
F=2.8
2Y=7.016mm
ENTP=0mm
EXTP=-3.82mm
H1=-0.06mm
H2=-3.88mm
・撮像レンズの面データを以下に示す。
1(絞り) ∞ 0.000 0.83
2(*) 4.338 1.060 1.54470 56.2 0.85
3(*) -3.261 0.050 1.13
4(*) 3.777 0.426 1.63200 23.4 1.26
5(*) 1.655 0.730 1.32
6(*) -15.301 0.834 1.54470 56.2 1.56
7(*) -3.268 0.301 1.75
8(*) -2.158 0.680 1.54470 56.2 1.98
9(*) -1.250 0.100 2.11
10(*) 4.019 0.731 1.54470 56.2 2.49
11(*) 1.167 0.600 2.98
12 ∞ 0.300 1.51630 64.1 3.18
13 ∞ 3.24
・撮像レンズの非球面係数を以下に示す。
K=-0.11529E+01,A4=-0.12315E-01,A6=-0.17373E-02,
A8=-0.10136E-01,A10=0.85871E-02,A12=-0.57045E-03,
A14=-0.20491E-02
第3面
K=-0.46540E+01,A4=0.16705E-01,A6=-0.31022E-01,
A8=0.12878E-01,A10=0.17465E-02,A12=-0.52988E-02,
A14=0.19910E-02
第4面
K=-0.56239E+01,A4=-0.30406E-01,A6=0.22674E-01,
A8=-0.11014E-01,A10=0.19630E-02,A12=0.15868E-02,
A14=-0.58687E-03
第5面
K=-0.45094E+01,A4=0.50515E-02,A6=0.16648E-01,
A8=-0.11130E-01,A10=0.27593E-02,A12=0.70672E-03,
A14=-0.34114E-03
第6面
K=0.80000E+02,A4=-0.63214E-02,A6=-0.84416E-02,
A8=0.56682E-02,A10=0.59386E-03,A12=-0.34629E-03,
A14=0.32661E-04
第7面
K=0.19417E+01,A4=0.44144E-02,A6=-0.33790E-02,
A8=0.74821E-03,A10=0.34837E-03,A12=0.78097E-04,
A14=0.46394E-05
第8面
K=-0.21741E+00,A4=0.45377E-01,A6=-0.24638E-03,
A8=0.45745E-03,A10=-0.83017E-05,A12=-0.18840E-04,
A14=0.24646E-05
第9面
K=-0.35183E+01,A4=-0.33241E-01,A6=0.18086E-01,
A8=-0.22745E-02,A10=0.16508E-03,A12=-0.14002E-04,
A14=0.26538E-06
第10面
K=-0.65715E+01,A4=-0.64437E-01,A6=0.96449E-02,
A8=-0.11326E-03,A10=-0.14314E-03,A12=0.21400E-04,
A14=-0.10765E-05
第11面
K=-0.46352E+01,A4=-0.35746E-01,A6=0.61166E-02,
A8=-0.86560E-03,A10=0.73686E-04,A12=-0.36214E-05,
A14=0.86848E-07
・撮像レンズの単レンズデータを以下に示す。
1 2 3.594
2 4 -5.055
3 6 7.446
4 8 4.314
5 10 -3.317
・撮像レンズの条件式(1)~(8)に対応する値を以下に示す。
(1)(r7+r8)/(r7-r8)=3.753
(2)SL/f=1.392
(3)f4/f=0.923
(4)f3/f4=1.726
(5)ν1-ν2=32.6
(6)n2=1.632
(7)d6/f=0.064
(8)L/2Y=0.93
図17は実施例8のレンズの断面図である。L1は第1レンズ、L2は第2レンズ、L3は第3レンズ、L4は第4レンズ、L5は第5レンズ、Sは開口絞り、Iは撮像面を示す。また、Fは光学的ローパスフィルタやIRカットフィルタ、固体撮像素子のシールガラス等を想定した平行平板である。図18は実施例8の収差図(球面収差、非点収差、歪曲収差、メリディオナルコマ収差)である。
(実施例9)
・実施例9の撮像レンズの全体緒元を以下に示す。
fB=0.56mm
F=2.0
2Y=7.016mm
ENTP=0mm
EXTP=-3.41mm
H1=-2.26mm
H2=-5.02mm
・撮像レンズの面データを以下に示す。
1(絞り) ∞ -0.380 1.39
2(*) 2.421 0.920 1.54470 56.2 1.46
3(*) -25.589 0.050 1.43
4(*) 3.179 0.321 1.63200 23.4 1.41
5(*) 1.718 1.008 1.40
6(*) -13.442 0.709 1.54470 56.2 1.60
7(*) -3.644 0.612 1.76
8(*) -2.678 0.770 1.54470 56.2 1.98
9(*) -1.430 0.520 2.16
10(*) -9.920 0.450 1.54470 56.2 2.73
11(*) 1.938 0.600 3.03
12 ∞ 0.145 1.51630 64.1 3.33
13 ∞ 3.35
・撮像レンズの非球面係数を以下に示す。
K=0.36148E+00,A4=0.17371E-02,A6=-0.93252E-04,
A8=-0.30737E-03,A10=0.10423E-02,A12=-0.50599E-03,
A14=0.95554E-04
第3面
K=-0.30000E+02,A4=0.21423E-01,A6=-0.59707E-02,
A8=0.15453E-02,A10=0.51980E-03,A12=-0.83832E-03,
A14=0.17232E-03
第4面
K=-0.43318E+00,A4=-0.57637E-01,A6=0.21407E-01,
A8=-0.96490E-02,A10=0.18300E-02,A12=-0.81816E-03,
A14=0.14616E-03
第5面
K=-0.35304E+01,A4=-0.58482E-02,A6=0.15046E-01,
A8=-0.84000E-02,A10=0.47172E-02,A12=-0.25772E-02,
A14=0.65056E-03
第6面
K=0.23361E+02,A4=-0.19346E-01,A6=0.27182E-04,
A8=0.57107E-03,A10=-0.29448E-03,A12=0.55760E-03,
A14=-0.12701E-03
第7面
K=0.24510E+01,A4=-0.11982E-01,A6=0.47194E-02,
A8=-0.10093E-02,A10=0.31052E-03,A12=0.75567E-04,
A14=0.70094E-05
第8面
K=0.12384E+00,A4=-0.88676E-02,A6=0.43753E-02,
A8=0.34489E-03,A10=0.16651E-04,A12=-0.13926E-05,
A14=-0.24574E-07
第9面
K=-0.35852E+01,A4=-0.46635E-01,A6=0.13524E-01,
A8=-0.26772E-02,A10=0.44420E-03,A12=-0.86058E-05,
A14=-0.28156E-05
第10面
K=0.67292E+01,A4=-0.47747E-01,A6=0.10058E-01,
A8=-0.47748E-03,A10=-0.18904E-03,A12=0.37936E-04,
A14=-0.20468E-05
第11面
K=-0.98800E+01,A4=-0.37219E-01,A6=0.67687E-02,
A8=-0.98376E-03,A10=0.89767E-04,A12=-0.53208E-05,
A14=0.16451E-06
・撮像レンズの単レンズデータを以下に示す。
1 2 4.108
2 4 -6.463
3 6 8.949
4 8 4.628
5 10 -2.937
・撮像レンズの条件式(1)~(8)に対応する値を以下に示す。
(1)(r7+r8)/(r7-r8)=3.292
(2)SL/f=1.117
(3)f4/f=0.829
(4)f3/f4=1.934
(5)ν1-ν2=32.6
(6)n2=1.632
(7)d6/f=0.110
(8)L/2Y=0.94
図19は実施例9のレンズの断面図である。L1は第1レンズ、L2は第2レンズ、L3は第3レンズ、L4は第4レンズ、L5は第5レンズ、Sは開口絞り、Iは撮像面を示す。また、Fは光学的ローパスフィルタやIRカットフィルタ、固体撮像素子のシールガラス等を想定した平行平板である。図20は実施例9の収差図(球面収差、非点収差、歪曲収差、メリディオナルコマ収差)である。
L1 第1レンズ
L2 第2レンズ
L3 第3レンズ
L4 第4レンズ
L5 第5レンズ
S 開口絞り
F 平行平板
I 撮像面
C 固体撮像素子
Claims (12)
- 固体撮像素子の光電変換部に被写体像を結像させるための撮像レンズにおいて、
物体側より順に、開口絞りと、正の屈折力を有し物体側に凸面を向けた第1レンズと、負の屈折力を有し像側に凹面を向けた第2レンズと、正の屈折力を有し像側に凸面を向けた第3レンズと、正の屈折力を有し像側に凸面を向けてメニスカス形状を有する第4レンズと、負の屈折力を有し像側に凹面を向けた第5レンズと、から成り、以下の条件式を満足することを特徴とする撮像レンズ。
2.0<(r7+r8)/(r7-r8)<8.0
0.8<SL/f<1.5
但し、
r7:前記第4レンズ物体側面の曲率半径
r8:前記第4レンズ像側面の曲率半径
SL:前記開口絞りから像側焦点までの光軸上の距離
f:撮像レンズ全系の焦点距離 - 以下の条件式を満足することを特徴とする請求項1に記載の撮像レンズ。
0.6<f4/f<2.0
但し、
f4:前記第4レンズの焦点距離
f:撮像レンズ全系の焦点距離 - 以下の条件式を満足することを特徴とする請求項1又は請求項2に記載の撮像レンズ。
0.5<f3/f4<5.0
但し、
f3:前記第3レンズの焦点距離
f4:前記第4レンズの焦点距離 - 以下の条件式を満足することを特徴とする請求項1~3の何れか1項に記載の撮像レンズ。
20<ν1-ν2<70
但し、
ν1:前記第1レンズのアッベ数
ν2:前記第2レンズのアッベ数 - 以下の条件式を満足することを特徴とする請求項1~4の何れか1項に記載の撮像レンズ。
1.55<n2<2.10
但し、
n2:前記第2レンズのd線に対する屈折率 - 第1レンズから第3レンズを移動させて焦点位置合わせを行い、以下の条件式を満足することを特徴とする請求項1~5の何れか1項に記載の撮像レンズ。
0.05<d6/f<0.15
但し、
d6:前記第3レンズと前記第4レンズの軸上の空気間隔
f:撮像レンズ全系の焦点距離 - 前記第2レンズの像側面は非球面形状を有し、光軸から周辺に離れるに従って負の屈折力が弱くなる形状を有することを特徴とする請求項1~6の何れか1項に記載の撮像レンズ。
- 前記開口絞りは前記第1レンズの物体側面の光軸上の位置より像側に位置し、前記第1レンズの物体側面の最周辺部より物体側に配置されていることを特徴とする請求項1~7の何れか1項に記載の撮像レンズ。
- 前記第5レンズの像側面は非球面形状に形成されており、その中心では負の屈折力を有し、周辺に向かうに従い負の屈折力が弱くなり、変曲点を有することを特徴とする請求項1~8の何れか1項に記載の撮像レンズ。
- 前記第1レンズから第5レンズの全てがプラスチック材料で形成されていることを特徴とする請求項1~9の何れか1項に記載の撮像レンズ。
- 被写体像を光電変換する固体撮像素子と、請求項1~10の何れか1項に記載の撮像レンズを備えたことを特徴とする撮像装置。
- 請求項11に記載の撮像装置を備えたことを特徴とする携帯端末。
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Also Published As
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US20120140104A1 (en) | 2012-06-07 |
US8520124B2 (en) | 2013-08-27 |
JPWO2011021271A1 (ja) | 2013-01-17 |
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