Taking lens system

Abstract

A taking lens system has, from the object side, a front lens unit including a first lens element and a second lens element, an aperture stop, and a rear lens unit including a third positive lens element, a fourth negative lens element, and a fifth positive lens element. In the taking lens system, the following condition is fulfilled:0.3

Description

This disclosure is based on application No. H10-373630 filed in Japan on Dec. 28, 1998, the entire contents of which are hereby incorporated by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a taking lens system, and more particularly to a compact taking lens system suitable for use in a digital input apparatus such as a digital still camera or digital video camera.

2. Description of the Prior Art

In recent years, as personal computers become prevalent, digital still cameras, digital video cameras, and the like (hereafter referred to simply as digital cameras) that allow easy storage of image data in a digital format have become more popular for personal use. Such digital cameras are expected to become more widespread as an apparatus for inputting image data.

On the other hand, such digital cameras have come to employ smaller and smaller solid-state imaging devices, for example, CCDs (charge-coupled devices), and therefore digital cameras themselves are quite naturally expected to be made more compact. Consequently, further miniaturization is eagerly sought in taking lens systems, because they occupy the largest space within digital input devices.

To cope with such requirements, for example, Japanese Laid-open Patent Application No. H9-166748 proposes a compact taking lens system suitable for use in a camera having a CCD that is composed of as few constituent lens elements as possible. In this proposed arrangement, however, the taking lens system has a negative-positive-positive lens arrangement on the rear (image) side of its aperture stop. In a taking lens system of this type, convex lens elements are located in a rear portion thereof, and therefore it is difficult to secure a sufficient edge margin in the convex lens elements. This makes it difficult to achieve further miniaturization of the entire taking lens system. In this context, the edge margin of a lens element refers to the portion of the lens element that falls outside its effective diameter.

SUMMARY OF THE INVENTION

An object of the present invention is to provide a compact taking lens system that offers sufficiently high optical performance. To achieve this object, according to one aspect of the present invention, a taking lens system is provided with, from the object side, a first negative lens element, a second biconvex lens element, an aperture stop, a third positive lens element, a fourth negative lens element, and a fifth positive lens element. In the taking lens system, the following condition is fulfilled:

−0.99<(r 21 +r 22 )/(r 21 −r 22 )<0.56

where

r 21 represents the radius of curvature of the object-side surface of the second lens element; and

r 22 represents the radius of curvature of the image-side surface of the second lens element.

According to another aspect of the present invention, a taking lens system is provided with, from the object side, a first biconcave lens element, a second positive lens element, an aperture stop, a third positive lens element, a fourth negative lens element, and a fifth positive lens element. In the taking lens system, the following condition is fulfilled:

0.12<n 2 −n 1 <0.39

where

n 1 represents the refractive index of the first lens element for the d line; and

n 2 represents the refractive index of the second lens element for the d line.

According to another aspect of the present invention, a taking lens system is provided with, from the object side, a first negative lens element, a second positive lens element, an aperture stop, a third positive lens element, a fourth negative lens element, and a fifth positive lens element. The third and fourth lens elements are cemented together. In the taking lens system, the following condition is fulfilled:

−0.02<F/F 34 <0.18

where

F represents the focal length of the entire taking lens system; and

F 34 represents the focal length of the doublet lens element formed by cementing together the third and fourth lens elements.

According to another aspect of the present invention, a taking lens system is provided with, from the object side, a first negative lens element, a second biconvex lens element, an aperture stop, a third positive lens element, a fourth negative lens element, and a fifth positive lens element. The third and fourth lens elements are cemented together. In the taking lens system, the following condition is fulfilled:

0.3<F/F 345 <0.9

where

F represents the focal length of the entire taking lens system; and

F 345 represents the composite focal length of the third to fifth lens elements.

According to still another aspect of the present invention, a taking lens system is provided with, from the object side, a first negative lens element, a second biconvex lens element, an aperture stop, a third positive meniscus lens element convex to the image side, a fourth negative lens element, and a fifth positive lens element. The fourth and fifth lens elements are cemented together. In the taking lens system, the following condition is fulfilled:

0.3<F/F 345 <0.9

where

F represents the focal length of the entire taking lens system; and

F 345 represents the composite focal length of the third to fifth lens elements.

BRIEF DESCRIPTION OF THE DRAWINGS

The objects and features of this invention will become clear from the following description, taken in conjunction with the preferred embodiments with reference to the accompanied drawings in which:

FIG. 1 is a lens arrangement diagram of the taking lens system of a first embodiment (Example 1) of the present invention;

FIG. 2 is a lens arrangement diagram of the taking lens system of a second embodiment (Example 2) of the present invention;

FIG. 3 is a lens arrangement diagram of the taking lens system of a third embodiment (Example 3) of the present invention;

FIG. 4 is a lens arrangement diagram of the taking lens system of a fourth embodiment (Example 4) of the present invention;

FIG. 5 is a lens arrangement diagram of the taking lens system of a fifth embodiment (Example 5) of the present invention;

FIG. 6 is a lens arrangement diagram of the taking lens system of a sixth embodiment (Example 6) of the present invention;

FIG. 7 is a lens arrangement diagram of the taking lens system of a seventh embodiment (Example 7) of the present invention;

FIG. 8 is a lens arrangement diagram of the taking lens system of an eighth embodiment (Example 8) of the present invention;

FIGS. 9A to 9 C are graphic representations of the aberrations observed in the taking lens system of Example 1;

FIGS. 10A to 10 C are graphic representations of the aberrations observed in the taking lens system of Example 2;

FIGS. 11A to 11 C are graphic representations of the aberrations observed in the taking lens system of Example 3;

FIGS. 12A to 12 C are graphic representations of the aberrations observed in the taking lens system of Example 4 ;

FIGS. 13A to 13 C are graphic representations of the aberrations observed in the taking lens system of Example 5;

FIGS. 14A to 14 C are graphic representations of the aberrations observed in the taking lens system of Example 6;

FIGS. 15A to 15 C are graphic representations of the aberrations observed in the taking lens system of Example 7;

FIGS. 16A to 16 C are graphic representations of the aberrations observed in the taking lens system of Example 8; and

FIG. 17 is a block diagram illustrating the arrangement of optical components in a digital camera.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

Hereinafter, fixed focal length taking lens systems embodying the present invention will be described with reference to the drawings. FIGS. 1 to 8 are lens arrangement diagrams of the lens systems of a first, a second, a third, a fourth, a fifth, a sixth, a seventh, and an eighth embodiment, respectively. In each diagram, the left-hand side corresponds to the object side, and the right-hand side corresponds to the image side. Aspherical surfaces are identified with an asterisk (*). In a digital camera, these components are arranged as shown in FIG. 17 , where light from an object passes through the taking lens system (TLS) and the low pass filter (LPF) to be directed onto an image sensor (IS), such as a CCD.

As shown in FIGS. 1 to 4 , in the first to fourth embodiments, the taking lens system is composed of, from the object side, a front lens unit consisting of a negative biconcave lens element FL 1 (a first lens element) and a positive biconvex lens element FL 2 (a second lens element), an aperture stop A, and a rear lens unit consisting of a positive meniscus lens element RL 1 convex to the image side (a third lens element), and a doublet lens element RL 2 formed by cementing together a biconcave lens element (a fourth lens element) and a biconvex lens element (a fifth lens element). A low-pass filter LPF is arranged on the image side of the rear lens unit.

As shown in FIGS. 5 to 8 , in the fifth to eighth embodiments, the taking lens system is composed of, from the object side, a front lens unit consisting of a negative biconcave lens element FL 1 (a first lens element) and a positive biconvex lens element FL 2 (a second lens element), an aperture stop A, and a rear lens unit consisting of a doublet lens element RL 1 formed by cementing together a biconvex lens element (a third lens element) and a biconcave lens element (a fourth lens element), and a positive biconvex lens element RL 2 (a fifth lens element). A low-pass filter LPF is on the image side of the taking lens unit.

In all of the embodiments, the fixed focal length taking lens system adopts a “total movement” focusing method in which focusing from a condition focused on an infinite distance to a condition focused on a close distance is achieved by moving all of its constituent components toward the object side (not shown). Alternatively, it is also possible to achieve focusing in any other manner, for example, by moving the whole of the taking lens system while varying the distance between the aperture stop and the lens element disposed on the object side of the aperture stop and the distance between the aperture stop and the lens element disposed on the image side of the aperture stop, or by moving the individual lens elements separately, or by moving a plurality of lens elements simultaneously.

Next, the conditions to be preferably fulfilled by the taking lens systems of the embodiments will be described. The individual lens elements constituting the taking lens system are represented as, from the object side, a first, a second, a third, a fourth, and a fifth lens element, respectively. Note that, in any of the taking lens systems of the embodiments, it is not necessary that all of the conditions given below be fulfilled simultaneously; if any of those conditions are fulfilled, it is possible to achieve the corresponding advantages. It is needless to say, however, that more than one condition should preferably be fulfilled to obtain satisfactory results in terms of optical performance, miniaturization, and simplicity of assembly.

In all of the embodiments, it is preferable that the taking lens system fulfill Condition (1) below.

−0.99<(r 21 +r 22 )/(r 21 −r 22 )<0.56  (1)

where

r 21 represents the radius of curvature of the object-side surface of the second lens element; and

r 22 represents the radius of curvature of the image-side surface of the second lens element.

Condition (1) defines the condition to be fulfilled, in particular, to achieve well-balanced correction of coma aberration. If the value of Condition (1) is equal to or less than its lower limit, coma aberration becomes so large as to have unduly adverse effects on high-order lateral chromatic aberration. In contrast, if the value of Condition (1) is equal to or greater than its upper limit, coma aberration becomes so large as to have unduly adverse effects on astigmatism.

In all of the embodiments, it is preferable that the taking lens system fulfill Condition (2) below.

 0.12<n 2 −n 1 <0.39  (2)

where

n 1 represents the refractive index of the first lens element for the d line; and

n 2 represents the refractive index of the second lens element for the d line.

Condition (2) defines the condition to be fulfilled to achieve well-balanced correction of Petzval sum. If the value of Condition (2) is equal to or less than its lower limit, the Petzval sum becomes excessively great in the positive direction. In contrast, if the value of Condition (2) is equal to or greater than its upper limit, the Petzval sum becomes excessively great in the negative direction.

In the embodiments of FIGS. 5-8 , it is preferable that the taking lens system fulfill Condition (3) below.

−0.02<F/F 34 <0.18  (3)

where

F represents the focal length of the entire taking lens system; and

F 34 represents the focal length of the doublet lens element formed by cementing together the third and fourth lens elements.

Condition (3) defines the condition to be fulfilled, in particular, to achieve well-balanced correction of coma aberration. If the value of Condition (3) is equal to or less than its lower limit, coma aberration becomes so large as to have unduly adverse effects on high-order lateral chromatic aberration. In contrast, if the value of Condition (3) is equal to or greater than its upper limit, coma aberration becomes so large as to have unduly adverse effects on astigmatism.

In all of the embodiments, it is preferable that the taking lens system fulfill Condition (4) below.

0.3<F/F 345 <0.9  (4)

where

F represents the focal length of the entire taking lens system; and

F 345 represents the composite focal length of the third to fifth lens elements.

Condition (4) defines the condition to be fulfilled, in particular, to strike a proper balance between the total length and the aberration characteristics. If-the value of Condition (4) is equal to or less than its lower limit, aberrations can be corrected properly, but simultaneously the total length of the taking lens system needs to be made unduly long. An unduly long total length demands an unduly large diameter in the front lens unit, and thus makes the taking lens system as a whole unduly large. In contrast, if the value of Condition (4) is equal to or greater than its upper limit, the total length of the taking lens system is successfully minimized, but simultaneously aberrations (in particular, distortion and curvature of field) become unduly large.

In all of the embodiments, it is preferable that the taking lens system fulfill Condition (5) below.

0.01<(X−X 0 )/N′−N)<2.0  (5)

where

X represents the deviation of the aspherical surface along the optical axis at the height in a direction perpendicular to the optical axis (the direction pointing to the object side is negative);

X 0 represents the deviation of the reference spherical surface of the aspherical surface along the optical axis at the height in a direction perpendicular to the optical axis (the direction pointing to the object side is negative);

N represents the refractive index of the object-side medium of the aspherical surface for the d line; and

N′ represents the refractive index of the image-side medium of the aspherical surface for the d line.

Condition (5) defines the condition to be fulfilled, in particular, to correct distortion and curvature of field. If the value of Condition (5) is equal to or less than its lower limit, positive distortion increases, and simultaneously the inclination of the image plane toward the over side becomes unduly large. In contrast, if the value of Condition (5) is equal to or greater than its upper limit, negative distortion increases, and simultaneously the inclination of the image plane toward the under side becomes unduly large. This makes it impossible to realize a satisfactorily practical taking lens system. Note that, in a taking lens system that includes a plurality of aspherical surfaces, at least one of those aspherical surfaces needs to fulfill Condition (5) above; the other aspherical surfaces do not necessarily have to fulfill Condition (5) above, if that is advantageous for the correction of other aberrations.

In all of the embodiments, it is preferable that the taking lens system fulfill Condition (6) below.

0.47<F/F 2 <1.47  (6)

where

F represents the focal length of the entire taking lens system; and

F 2 represents the focal length of the second lens element.

Condition (6) defines the condition to be fulfilled, in particular, to achieve well-balanced correction of coma aberration. If the value of Condition (6) is equal to or less than its lower limit, coma aberration becomes so large as to have unduly adverse effects on high-order lateral chromatic aberration. In contrast, if the value of Condition (6) is equal to or greater than its upper limit, coma aberration becomes so large as to have unduly adverse effects on astigmatism.

In all of the embodiments, it is preferable that the taking lens system fulfill Condition (7) below.

1<img×R<15  (7)

where

img represents the maximum image height; and

R represents the effective diameter of the image-side-end surface.

Condition (7) defines the condition to be fulfilled to keep appropriate the size and the aberration characteristics of an optical system as well as the conditions expected to be fulfilled thereby when designed for use in a video camera. Usually, a solid-state imaging device (a CCD) has microlenses disposed on the front surfaces of the individual light-sensing elements provided therein so as to enhance its light-sensing efficiency. To make efficient use of the light-condensing ability of those microlenses, it is essential to let rays enter the microlenses substantially parallel to their optical axes. To achieve this, it is preferable to make the entire taking lens system telecentric toward the image side.

If the value of Condition (7) is equal to or greater than its upper limit, the entire taking lens system is too telecentric, and thus negative distortion becomes unduly large, and simultaneously the inclination of the image plane toward the under side becomes unduly large. In contrast, if the value of Condition (7) is equal to or less than its lower limit, it is difficult to make the entire taking lens system substantially telecentric. Even if the entire taking lens system can be made substantially telecentric, the back focal distance is then unduly long and thus the taking lens system as a whole is unduly large.

Hereinafter, taking lens systems embodying the present invention will be presented with reference to their construction data, graphic representations of aberrations, and other data. Tables 1 to 8 list the construction data of Examples 1 to 8, which respectively correspond to the first to eighth embodiments described above and have lens arrangements as shown in FIGS. 1 to 8 .

In the construction data of each example, ri (i =1, 2, 3, . . . ) represents the ith surface counted from the object side and its radius of curvature, di (i=1, 2, 3, . . . ) represents the ith axial distance counted from the object side, and Ni (i=1, 2, 3, . . . ) and vi (i=1, 2, 3, . . . ) respectively represent the refractive index for the d line and the Abbe number of the ith lens element counted from the object side. Moreover, f represents the focal length of the entire taking lens system, and FNO represents the F-number of the entire taking lens system. Furthermore, a surface whose radius of curvature ri is marked with an asterisk (( ) is a refractive optical surface having an aspherical shape, or a surface exerting a refracting effect equivalent to an aspherical surface, whose surface shape is defined by the following formula.

X(H)=(C·H 2 )/{1+ε·C 2·H 2 )}+ΣA i H i

where

X(H) represents the displacement along the optical axis at the height H (relative to the vertex);

H represents the height in a direction perpendicular to the optical axis;

C represents the paraxial curvature;

ε represents the quadric surface parameter; and

A i represents the aspherical coefficient of the ith order.

FIGS. 9A to 9 C, 10 A to 10 C, 11 A to 11 C, 12 A to 12 C, 13 A to 13 C, 14 A to 14 C, 15 A to 15 C, and 16 A to 16 C are graphic representations of the aberrations observed in Examples 1 to 8, respectively. Of these diagrams, FIGS. 9A to 16 A show spherical aberration and sine condition; FIGS. 9B to 16 B show astigmatism; and FIGS. 9C to 16 C show distortion. In the spherical aberration diagrams, the solid line (d) represents the spherical aberration for the d line; the dash-and-dot line g represents the spherical aberration for the g line; and the dash-dot-dot line c represents the spherical aberration for the c line. Moreover, the broken line (SC) represents the amount by which the sine condition remains unfulfilled. In the astigmatism diagrams, the solid line (DS) and the broken line (DM) represent the astigmatism on the sagittal plane and on the meridional plane, respectively. For spherical aberration, the F number is taken along the vertical axis. For astigmatism and distortion, the maximum image height Y′ is taken along the vertical axis. Moreover, Table 9 lists the values corresponding to the parameters defined by Conditions (1) to (4), (6), and (7) in Examples 1 to 8, and Tables 10 to 17 list the values corresponding to Condition (5) to be fulfilled by the aspherical surface in Examples I to 8, respectively. Note that, in Tables 10 to 17, Y represents the maximum height of the optical path on the aspherical surface.

TABLE 1
Construction Data of Example 1
f = 5.5 mm (Focal Length of Entire Taking Lens System)
FNO = 2.87 (F-number)
Radius of	Axial	Refractive	Abbe
Curvature	Distance	Index (Nd)	Number(d)
r1* = −14.466	d1 = 1.000	N1 = 1.52510	ν1 = 56.38
r2* = 2.869	d2 = 2.022
r3 = 8.079	d3 = 1.951	N2 = 1.77250	ν2 = 49.77
r4 = −9.790	d4 = 2.694
r5 = (Aperture Stop)	d5 = 1.703
r6* = 27.830	d6 = 1.990	N3 = 1.52510	ν3 = 56.38
r7* = −4.334	d7 = 0.167
r8 = −7.673	d8 = 0.750	N4 = 1.75000	ν4 = 25.14
r9 = 9.263	d9 = 3.916	N5 = 1.77250	ν5 = 49.77
r10 = −7.281	d10 = 1.720
r11 = ∞	d11 = 3.400	N6 = 1.51680	ν6 = 64.20
r12 = ∞
[Aspherical Coefficients of First Surface (r1)]
ε = 0.10000 × 10
A4 = 0.32598 × 10 −2
A6 = −0.53772 × 10 −3
A8 = 0.40558 × 10 −4
A10 = −0.11829 × 10 −5
[Aspherical Coefficients of Second Surface (r2)]
ε = 0.10000 × 10
A4 = 0.23068 × 10 −3
A6 = −0.87711 × 10 −3
A8 = −0.32225 × 10 −4
[Aspherical Coefficients of Sixth Surface (r6)]
ε = 0.10000 × 10
A4 = 0.18957 × 10 −3
A6 = 0.7572510 × 10 −4
A8 = 0.15634 × 10 −4
[Aspherical Coefficients of Seventh Surface (r7)]
ε= 0.10000 × 10
A4 = 0.33291 × 10 −2
A6 = 0.91104 × 10 −4
A8 = 0.19074 × 1010 −4

TABLE 2
Construction Data of Example 2
f = 5.08 mm (Focal Length of Entire Taking Lens System)
FNO = 2.87 (F-number)
Radius of	Axial	Refractive	Abbe
Curvature	Distance	Index (Nd)	Number(d)
r1* = #18.815	d1= 1.174	N1 = 1.52510	ν1 = 56.38
r2* = 2.944	d2 = 2.962
r3 = 8.046	d3 = 1.902	N2 = 1.77250	ν2 = 49.77
r4 = −12.815	d4 = 2.535
r5 = (Aperture Stop)	d5 = 1.795
r6* = 186.397	d6 = 1.978	N3 = 1.52510	ν3 = 56.38
r7* = 4.671	d7 = 0.201
r8 = −7.286	d8 = 0.750	N4 = 1.75000	ν4 = 25.14
r9 = 8.268	d9 = 3.802	N5 = 1.77250	ν5 = 49.77
r10 = −7.072	d10 = 2.002
r11 = ∞	d11 = 3.400	N6 = 1.51680	ν6 = 64.20
r12 = ∞
[Aspherical Coefficients of First Surface (r1)]
ε = 0.10000 × 10
A4 = 0.38568 × 10 −2
A6 = −0.47407 × 10 −3
A8 = 0.29044 × 10 −4
A10 = −0.70508 × 10 −6
[Aspherical Coefficients of Second Surface (r2)]
ε = 0.10000 × 10
A4 = 0.18848 × 10 −2
A6 = −0.69884 × 10 −3
A8 = −0.37034 × 10 −4
[Aspherical Coefficients of Sixth Surface (r6)]
ε = 0.10000 × 10
A4 = −0.55229 × 10 −4
A6 = 0.41120 × 10 −4
A8 = 0.11917 × 10 −4
[Aspherical Coefficients of Seventh Surface (r7)]
ε = 0.10000 × 10
A4 = 0.33291 × 10 −2
A6 = 0.83984 × 10 −4
A8 = 0.15080 × 10 −4

TABLE 3
Construction Data of Example 3
f = 4.75 mm (Focal Length of Entire Taking Lens System)
FNO = 2.87 (F-number)
Radius of	Axial	Refractive	Abbe
Curvature	Distance	Index (Nd)	Number(d)
r1* = −20.753	d1 = 1.684	N1 = 1.52510	ν1 = 56.38
r2* = 3.061	d2 = 3.764
r3 = 8.337	d3 = 2.028	N2 = 1.77250	ν2 = 49.77
r4 = −14.877	d4 = 2.368
r5 = (Aperture Stop)	d5 = 1.524
r6* = −51.018	d6 = 1.858	N3 = 1.52510	ν3 = 56.38
r7* = −5.136	d7 = 0.672
r8 = −8.525	d8 = 0.750	N4 = 1.79850	ν4 = 22.60
r9 = 9.772	d9 = 3.775	N5 = 1.77250	ν5 = 49.77
r10 = −6.594	d10 = 1.336
r11 = ∞	d11 = 3.400	N6 = 1.51680	ν6 = 64.20
r12 = ∞
[Aspherical Coefficients of First Surface (r1)]
ε = 0.10000 × 10
A4 = 0.34597 × 10 −2
A6 = −0.29030 × 10 −3
A8 = 0.13266 × 10 −4
A10 = −0.24941 × 10 −6
[Aspherical Coefficients of Second Surface (r2)]
ε = 0.10000 × 10
A4 = 0.26461 × 10 −2
A6 = −0.39182 × 10 −2
A8 = −0.38071 × 10 −4
[Aspherical Coefficients of Sixth Surface (r6)]
ε = 0.10000 × 10
A4 = 0.55997 × 10 −3
A6 = 0.41246 × 10 −4
A8 = 0.22329 × 10 −4
[Aspherical Coefficients of Seventh Surface (r7)]
ε = 0.10000 × 10
A4 = 0.38136 × 10 −2
A6 = 0.14206 × 10 −3
A8 = 0.17258 × 10 −4

TABLE 4
Construction Data of Example 4
f = 4.45 mm (Focal Length of Entire Taking Lens System)
FNO = 2.87 (F-number)
Radius of	Axial	Refractive	Abbe
Curvature	Distance	Index (Nd)	Number(d)
r1* = −25.047	d1 = 1.835	N1 = 1.52510	ν = 56.38
r2* = 3.236	d2 = 5.109
r3 = 8.334	d3 = 1.991	N2 = 1.77250	ν2 = 49.77
r4 = −18.189	d4 = 2.129
r5 = (Aperture Stop)	d5 = 1.506
r6* = −74.710	d6 = 1.774	N3 = 1.52510	ν3 = 56.38
r7* = #6.086	d7 = 0.727
r8 = −8.960	d8 = 0.750	N4 = 1.79850	ν4 = 22.60
r9 = 8.054	d9 = 3.876	N5 = 1.77250	ν5 = 49.77
r10 = −6.465	d10 = 1.198
r11 = ∞	d11 = 3.400	N6 = 1.51680	ν6 = 64.20
r12 = ∞
[Aspherical Coefficients of First Surface (r1)]
ε = 0.10000 × 10
A4 = 0.29609 × 10 −2
A6 = −0.18008 × 10 −3
A8 = 0.59843 × 10 −5
A10 = −0.81068 × 10 −7
[Aspherical Coefficients of Second Surface (r2)]
ε = 0.10000 × 10
A4 = 0.24791 × 10 −2
A6 = −0.72633 × 10 −3
A8 = −0.38558 × 10 −5
[Aspherical Coefficients of Sixth Surface (r6)]
ε = 0.10000 × 10
A4 = 0.79719 × 10 −3
A6 = 0.25473 × 10 −4
A8 = 0.19582 × 10 −4
[Aspherical Coefficients of Seventh Surface (r7)]
ε = 0.10000 × 10
A4 = 0.41192 × 10 −2
A6 = 0.14598 × 10 −3
A8 = 0.15095 × 10 −4

TABLE 5
Construction Data of Example 5
f = 5.55 mm (Focal Length of Entire Taking Lens System)
FNO = 2.87 (F-number)
Radius of	Axial	Refractive	Abbe
Curvature	Distance	Index (Nd)	Number(d)
r1 = −14.041	d1 = 1.000	N1 = 1.52510	ν1 = 56.38
r2* = 3.248	d2 = 2.191
r3 = 11.415	d3 = 1.798	N2 = 1.85000	ν2 = 40.04
r4 = −13.010	d4 = 2.703
r5 = (Aperture Stop)	d5 = 1.000
r6 = 6.844	d6 = 2.529	N3 = 1.77250	ν3 = 49.77
r7 = −8.719	d7 = 0.750	N4 = 1.75000	ν4 = 25.14
r8 = 5.135	d8 = 1.715
r9* = 6.722	d9 = 2.597	N5 = 1.52510	ν5 = 56.38
r10* = −6.717	d10 = 0.919
r11 = ∞	d11 = 3.400	N6 = 1.51680	ν6 = 64.20
r12 = ∞
[Aspherical Coefficients of Second Surface (r2)]
ε = 0.10000 × 10
A4 = −0.38963 × 10 −2
A6 = −0.98085 × 10 −4
A8 = −0.26318 × 10 −4
[Aspherical Coefficients of Ninth Surface (r9))
ε = 0.10000 × 10
A4 = −0.22552 × 10 −3
A6 = 0.72085 × 10 −4
A8 = 0.68284 × 10 −6
[Aspherical Coefficients of Tenth Surface (r10)]
ε = 0.10000 × 10
A4 = 0.21821 × 10 −2
A6 = 0.10796 × 10 −4
A8 = 0.72248 × 10 −5

TABLE 6
Construction Data of Example 6
f = 5.08 mm (Focal Length of Entire Taking Lens System)
FNO = 2.87 (F-number)
Radius of	Axial	Refractive	Abbe
Curvature	Distance	Index (Nd)	Number(d)
r1 = −19.703	d1 = 1.000	N1 = 1.52510	ν1 = 56.38
r2* = 3.283	d2 = 3.321
r3 = 13.385	d3 = 1.770	N2 = 1.85000	ν2 = 40.04
r4 = −12.871	d4 = 2.615
r5 = (Aperture Stop)	d5 = 1.000
r6 = 7.317	d6 = 2.546	N3 = 1.77250	ν3 = 49.77
r7 = −6.841	d7 = 0.750	N4 = 1.75000	ν4 = 25.14
r8 = 5.573	d8 = 2.042
r9* = 6.103	d9 = 2.502	N5 = 1.52510	ν5 = 56.38
r10* = −8.403	d10 = 0.554
r11 = ∞	d11 = 3.400	N6 = 1.51680	ν6 = 64.20
r12 = ∞
[Aspherical Coefficients of Second Surface (r2)]
ε = 0.10000 × 10
A4 = −0.32151 × 10 −2
A6 = −0.61776 × 10 −4
A8 = −0.26559 × 10 −4
[Aspherical Coefficients of Ninth Surface (r9)]
ε = 0.10000 × 10
A4 = −0.30193 × 10 −3
A6 = 0.70895 × 10 −4
A8 = 0.13241 × 10 −5
[Aspherical Coefficients of Tenth Surface (r10)]
ε = 0.10000 × 10
A4 = 0.25310 × 10 −2
A6 = 0.18889 × 10 −4
A8 = 0.79656 × 10 −5

TABLE 7
Construction Data of Example 7
f = 4.75 mm (Focal Length of Entire Taking Lens System)
FNO = 2.87 (F-number)
Radius of	Axial	Refractive	Abbe
Curvature	Distance	Index (Nd)	Number(d)
r1* = #16.409	d1 = 1.000	N1 = 1.52510	ν1 = 56.38
r2* = 3.090	d2 = 3.427
r3 = 11.537	d3 = 1.826	N2 = 1.85000	ν2 = 40.04
r4 = −13.947	d4 = 2.799
r5 = (Aperture Stop)	d5 = 1.200
r6 = 14.134	d6 = 2.638	N3 = 1.77250	ν3 = 49.77
r7 = A.734	d7 = 0.750	N4 = 1.75000	ν4 = 25.14
r8 = 14.443	d8 = 2.331
r9* = 6.298	d9 = 2.374	N5= 1.52510	ν5 = 56.38
r10* = −12.035	d10 = 0.500
r11 = ∞	d11 = 3.400	N6 = 1.51680	ν6 = 64.20
r12 = ∞
[Aspherical Coefficients of First Surface (r1)]
ε = 0.10000 × 10
A4 = 0.18968 × 10 −2
A6 = −0.17409 × 10 −3
A8 = 0.58303 × 10 −5
[Aspherical Coefficients of Second Surface (r2)]
ε = 0.10000 × 10
A4 = −0.14087 × 10 −2
A6 = −0.26121 × 10 −3
A8 = −0.46363 × 10 −4
[Aspherical Coefficients of Ninth Surface (r9)]
ε = 0.1000 × 10
A4 = 0.41700 × 10 −4
A6 = 0.65832 × 10 −4
A8 = 0.10742 × 10 −5
[Aspherical Coefficients of Tenth Surface (r10)]
ε = 0.10000 × 10
A4 = 0.25448 × 10 −2
A6 = 0.68837 × 10 −4
A8 = 0.44660 × 10 −5

TABLE 8
Construction Data of Example 8
f = 4.45 mm (Focal Length of Entire Taking Lens System)
FNO = 2.87 (F-number)
Radius of	Axial	Refractive	Abbe
Curvature	Distance	Index (Nd)	Number(d)
r1* =	−14.669
		d1 = 1.000	N1 = 1.52510	ν1 = 56.38
r2* =	3.184
		d2 = 4.546
r3 =	11.731
		d3 = 1.859	N2 = 1.85000	ν2 = 40.04
r4 =	−13.911
		d4 = 2.535
r5 =	(Aperture Stop)
		d5 = 1.200
r6 =	18.535
		d6 = 2.599	N3 = 1.77250	ν3 = 49.77
r7 =	−4.578
		d7 = 0.750	N4 = 1.84666	ν4 = 23.82
r8 =	38.938
		d8 = 2.807
r9* =	6.681
		d9 = 2.305	N5 = 1.52510	ν5 = 56.38
r10* =	−12.665
		d10 = 0.500
r11 =	∞
		d11 = 3.400	N6 = 1.51680	ν6 = 64.20
r12 =	∞
[Aspherical Coefficients of First Surface (r1)]
ε =	0.10000 × 10
A4 =	0.26468 × 10 −2
A6 =	−0.17738 × 10 −3
A8 =	0.46293 × 10 −5
[Aspherical Coefficients of Second Surface (r2)]
ε =	0.10000 × 10
A4 =	−0.10075 × 10 −3
A6 =	−0.58352 × 10 −4
A8 =	−0.54769 × 10 −4
[Aspherical Coefficients of Ninth Surface (r9)]
ε =	0.10000 × 10
A4 =	−0.53743 × 10 −3
A6 =	0.11163 × 10 −3
A8 =	0.43934 × 10 −6
[Aspherical Coefficients of Tenth Surface (r10)]
ε =	0.10000 × 10
A4 =	0.15771 × 10 −2
A6 =	0.11216 × 10 −3
A8 =	0.52257 × 10 −5

TABLE 9
Values Corresponding to Parameters defined by Conditions (1) to (4),
(6), and (7)
	(r21 + r22)/
	(r21 − r22)	n2 − n1	F/F34	F/F345	F/F2	img × r
Example 1	−0.10	0.25		0.63	0.92	11.09
Example 2	−0.23	0.25		0.58	0.76	11.09
Example 3	−0.28	0.25		0.53	0.66	11.26
Example 4	−0.37	0.25		0.48	0.58	11.26
Example 5	−0.07	0.32	−0.002	0.64	0.75	10.95
Example 6	0.02	0.32	0.002	0.57	0.64	10.89
Example 7	−0.09	0.32	0.060	0.55	0.62	11.05
Example 8	−0.09	0.32	0.028	0.49	0.57	11.05

TABLE 10
Values Corresponding to Condition (5) in Example 1
Height (X-X0)/(N′-N)
[1st Surface(r1)]
0.00 Y 0.00000
0.20 Y 0.00056
0.40 Y 0.00763
0.60 Y 0.02992
0.80 Y 0.06692
1.00 Y 0.11070
[2nd Surface(r2)]
0.00 Y 0.00000
0.20 Y −0.00000
0.40 Y 0.00044
0.60 Y 0.00675
0.80 Y 0.04281
1.00 Y 0.17821
[6th Surface(r6)]
0.00 Y 0.00000
0.20 Y 0.00001
0.40 Y 0.00019
0.60 Y 0.00131
0.80 Y 0.00606
1.00 Y 0.02263
[7th Surface(r7)]
0.00 Y 0.00000
0.20 Y −0.00030
0.40 Y −0.00492
0.60 Y −0.02604
0.80 Y −0.08911
1.00 Y −0.24617

TABLE 11
Values Corresponding to Condition (5) in Example 2
Height (X-X0)/(N′-N)
[1st Surface(r1)]
0.00 Y 0.00000
0.20 Y 0.00109
0.40 Y 0.01506
0.60 Y 0.06019
0.80 Y 0.13988
1.00 Y 0.24627
[2nd Surface(r2)]
0.00 Y 0.00000
0.20 Y −0.00014
0.40 Y −0.00171
0.60 Y −0.00294
0.80 Y 0.01883
1.00 Y 0.14656
[6th Surface(r6)]
0.00 Y 0.00000
0.20 Y −0.00000
0.40 Y −0.00002
0.60 Y 0.00011
0.80 Y 0.00160
1.00 Y 0.00914
[7th Surface(r7)]
0.00 Y 0.00000
0.20 Y −0.00030
0.40 Y −0.00495
0.60 Y −0.02606
0.80 Y −0.08825
1.00 Y −0.23977

TABLE 12
Values Corresponding to Condition (5) in Example 3
Height (X-X0)/(N′-N)
[1st Surface(r1)]
0.00 Y 0.00000
0.20 Y 0.00162
0.40 Y 0.02289
0.60 Y 0.09465
0.80 Y 0.23112
1.00 Y 0.42933
[2nd Surface(r2)]
0.00 Y 0.00000
0.20 Y −0.00024
0.40 Y −0.00343
0.60 Y −0.01307
0.80 Y −0.01853
1.00 Y 0.04236
[6th Surface(r6)]
0.00 Y 0.00000
0.20 Y 0.00002
0.40 Y 0.00039
0.60 Y 0.00219
0.80 Y 0.00828
1.00 Y 0.02628
[7th Surface(r7)]
0.00 Y 0.00000
0.20 Y −0.00029
0.40 Y −0.00475
0.60 Y −0.02517
0.80 Y −0.08566
1.00 Y −0.23297

TABLE 13
Values Corresponding to Condition (5) in Example 4
Height (X-X0)/(N′-N)
[1st Surface(r1)]
0.00 Y 0.00000
0.20 Y 0.00257
0.40 Y 0.03627
0.60 Y 0.15045
0.80 Y 0.36893
1.00 Y 0.68939
[2nd Surface(r2)]
0.00 Y 0.00000
0.20 Y −0.00036
0.40 Y −0.00548
0.60 Y −0.02432
0.80 Y −0.05232
1.00 Y −0.01202
[6th Surface(r6)]
0.00 Y 0.00000
0.20 Y 0.00003
0.40 Y 0.00052
0.60 Y 0.00278
0.80 Y 0.00976
1.00 Y 0.02840
[7th Surface(r7)]
0.00 Y 0.00000
0.20 Y −0.00029
0.40 Y −0.00476
0.60 Y −0.02507
0.80 Y −0.08450
1.00 Y −0.22633

TABLE 14
Values Corresponding to Condition (5) in Example 5
Height (X-X0)/(N′-N)
[2nd Surface(r2)]
0.00 Y 0.00000
0.20 Y 0.00023
0.40 Y 0.00377
0.60 Y 0.01977
0.80 Y 0.06649
1.00 Y 0.17928
[9th Surface(r9)]
0.00 Y 0.00000
0.20 Y −0.00006
0.40 Y −0.00055
0.60 Y 0.00154
0.80 Y 0.02489
1.00 Y 0.12727
[10th Surface(r10)]
0.00 Y 0.00000
0.20 Y −0.00075
0.40 Y −0.01223
0.60 Y −0.06493
0.80 Y −0.22816
1.00 Y −0.66954

TABLE 15
Values Corresponding to Condition (5) in Example 6
Height (X-X0)/(N′-N)
[2nd Surface(r2)]
0.00 Y 0.00000
0.20 Y 0.00030
0.40 Y 0.00489
0.60 Y 0.02592
0.80 Y 0.08957
1.00 Y 0.25359
[9th Surface(r9)]
0.00 Y 0.00000
0.20 Y −0.00010
0.40 Y −0.00101
0.60 Y −0.00011
0.80 Y 0.02373
1.00 Y 0.14164
[10th Surface(r10)]
0.00 Y 0.00000
0.20 Y −0.00056
0.40 Y −0.00763
0.60 Y −0.02992
0.80 Y −0.06692
1.00 Y −0.11070

TABLE 16
Values Corresponding to Condition (5) in Example 7
Height (X-X0)/(N′-N)
[1st Surface(r1)]
0.00 Y 0.00000
0.20 Y 0.00060
0.40 Y 0.00851
0.60 Y 0.03524
0.80 Y 0.08372
1.00 Y 0.14712
[2nd Surface(r2)]
0.00 Y 0.00000
0.20 Y 0.00015
0.40 Y 0.00283
0.60 Y 0.01833
0.80 Y 0.08130
1.00 Y 0.29579
[9th Surface(r9)]
0.00 Y 0.00000
0.20 Y 0.00003
0.40 Y 0.00116
0.60 Y 0.01181
0.80 Y 0.06574
1.00 Y 0.25899
[10th Surface(r10)]
0.00 Y 0.00000
0.20 Y −0.00092
0.40 Y −0.01529
0.60 Y −0.08330
0.80 Y −0.29574
1.00 Y −0.85079

TABLE 17
Values Corresponding to Condition (5) in Example 8
Height (X-X0)/(N′-N)
[1st Surface(r1)]
0.00 Y 0.00000
0.20 Y 0.00125
0.40 Y 0.01806
0.60 Y 0.07667
0.80 Y 0.18952
1.00 Y 0.34943
[2nd Surface(r2)]
0.00 Y 0.00000
0.20 Y 0.00002
0.40 Y 0.00051
0.60 Y 0.00640
0.80 Y 0.04913
1.00 Y 0.26096
[9th Surface(r9)]
0.00 Y 0.00000
0.20 Y −0.00020
0.40 Y −0.00220
0.60 Y −0.00194
0.80 Y 0.03541
1.00 Y 0.22053
[10th Surface(r10)]
0.00 Y 0.00000
0.20 Y 0.00058
0.40 Y −0.01021
0.60 Y −0.06054
0.80 Y −0.23806
1.00 Y −0.75937

Claims

1. A fixed focal length taking lens system comprising, in order from an object side:a front lens unit having first and second lens elements in that order from the object side, the second lens element being a biconvex lens element; an aperture stop; and a rear lens unit having a third positive lens element, a fourth negative lens element and a fifth positive lens element in that order from the object side with no intervening lenses therebetween, wherein the following condition is fulfilled: 0.3<F/F345<0.9 whereF represents the focal length of the entire taking lens system; and F345 represents the composite focal length of the third to fifth lens elements.

2. The taking lens system of claim 1 wherein the following condition is fulfilled:−0.99<(r21+r22)/(r21−r22)<0.56 wherer21 represents the radius of curvature of the object-side surface of the second lens element; and r22 represents the radius of curvature of the image-side surface of the second lens element.

3. The taking lens system of claim 1 wherein said first lens element is a biconcave lens element.

4. The taking lens system of claim 3 wherein said first lens element is a negative lens element and the second lens element is a positive lens element.

5. The taking lens system of claim 4 wherein the following condition is fulfilled:0.12<n2−n1<0.39 wheren1 represents the refractive index of the first lens element for the d line; and n2 represents the refractive index of the second lens element for the d line.

6. The taking lens system of claim 1 wherein at least two of the lens elements of said rear lens unit are cemented together to form a lens doublet.

7. The taking lens system of claim 6 wherein the fourth and fifth lens elements are cemented together.

8. The taking lens system of claim 6 wherein the third and fourth lens elements are cemented together.

9. The taking lens system of claim 8 wherein the following condition is fulfilled:−0.02<F/F34<0.18 whereF represents the focal length of the entire taking lens system; and F34 represents the focal length of the lens doublet formed by the third and fourth lens elements.

10. The taking lens system as claimed in claim 1, wherein at least one of the lens elements is provided, at least on one side thereof, with an aspherical surface and wherein the following condition is fulfilled:0.01<|(X−X0)/(N′−N)|<2.0 whereX represents a deviation of the aspherical surface along an optical axis at a height in a direction perpendicular to the optical axis, where a direction pointing to the object side is negative; X0 represents a deviation of a reference spherical surface of the aspherical surface along an optical axis at a height in a direction perpendicular to the optical axis; N represents the refractive index of an object-side medium of the aspherical surface for the d line; and N′ represents the refractive index of an image-side medium of the aspherical surface for the d line.

11. The taking lens system as claimed in claim 1, wherein the following condition is fulfilled:0.47<F/F2<1.47 whereF represents a focal length of the entire taking lens system; and F2 represents a focal length of the second lens element.

12. The taking lens system as claimed in claim 1, wherein the following condition is fulfilled:1<img×R<15 whereimg represents a maximum image height; and R represents an effective diameter of an image-side-end surface.

13. A digital camera comprising a taking lens system, a low-pass filter and an image sensor, wherein said taking lens system includes, in order from an object side:a front lens unit having first and second lens elements in that order from the object side, the second lens element being a biconvex lens element; an aperture stop; and a rear lens unit having a third positive lens element, a fourth negative lens element and a fifth positive lens element in that order from the object side with no intervening lenses therebetween, wherein the following condition is fulfilled: 0.3<F/F345<0.9 whereF represents the focal length of the entire taking lens system; and F345 represents the composite focal length of the third to fifth lens elements.

14. The digital camera of claim 13 wherein the following condition is fulfilled:−0.99<(r21+r22)/(r2−r22)<0.56 wherer21 represents the radius of curvature of the object-side surface of the second lens element; and r22 represents the radius of curvature of the image-side surface of the second lens element.

15. The digital camera of claim 13 wherein said first lens element is a biconcave lens element.

16. The digital camera of claim 15 wherein said first lens element is a negative lens element and the second lens element is a positive lens element.

17. The digital camera of claim 16 wherein the following condition is fulfilled:0.12<n2−n1<0.39 wheren1 represents the refractive index of the first lens element for the d line; and n2 represents the refractive index of the second lens element for the d line.

18. The digital camera of claim 13 wherein at least two of the lens elements of said rear lens unit are cemented together to form a lens doublet.

19. The digital camera of claim 18 wherein the fourth and fifth lens elements are cemented together.

20. The digital camera of claim 18 wherein the third and fourth lens elements are cemented together.

21. The digital camera of claim 20 wherein the following condition is fulfilled:−0.02<F/F34<0.18 whereF represents the focal length of the entire taking lens system; and F34 represents the focal length of the lens doublet formed by the third and fourth lens elements.

22. The digital camera as claimed in claim 13, wherein at least one of the lens elements is provided, at least on one side thereof, with an aspherical surface and wherein the following condition is fulfilled:0.01<|(X−X0)/(N′−N)|<2.0 whereX represents a deviation of the aspherical surface along an optical axis at a height in a direction perpendicular to the optical axis, where a direction pointing to the object side is negative; X0 represents a deviation of a reference spherical surface of the aspherical surface along an optical axis at a height in a direction perpendicular to the optical axis; N represents the refractive index of an object-side medium of the aspherical surface for the d line; and N′ represents the refractive index of an image-side medium of the aspherical surface for the d line.

23. The digital camera as claimed in claim 13, wherein the following condition is fulfilled:0.47<F/F2<1.47 whereF represents a focal length of the entire taking lens system; and F2 represents a focal length of the second lens element.

24. The digital camera as claimed in claim 13, wherein the following condition is fulfilled:1<img×R<15 whereimg represents a maximum image height; and R represents an effective diameter of an image-side-end surface.

25. A fixed focal length taking lens system comprising, in order from an object side:a first negative lens element; a second biconvex lens element; an aperture stop; a third positive lens element; a fourth negative lens element; and and a fifth positive lens element, wherein there are no intervening lenses between the second biconvex lens element and the aperture stop, wherein the first negative lens element is separated from the second biconvex lens element with no intervening lenses therebetween, and wherein the following condition is fulfilled: −0.99<(r21+r22)/(r21−r22)<0.56 wherer21 represents a radius of curvature of an object-side surface of the second biconvex lens element; and r22 represents a radius of curvature of an image-side surface of the second biconvex lens element.

26. A fixed focal length taking lens system comprising, in order from an object side:a first biconcave lens element; a second positive lens element; an aperture stop; a third positive lens element; a fourth negative lens element; and a fifth positive lens element, wherein there are no intervening lenses between the second positive lens element and the aperture stop, and wherein the following condition is fulfilled: 0.12<n2−n1<0.39 wheren1 represents a refractive index of the first lens element for the d line; and n2 represents a refractive index of the second lens element for the d line.

27. A fixed focal length taking lens system comprising, in order from an object side:a first negative lens element; a second positive lens element; an aperture stop; a third positive lens element; a fourth negative lens element; and a fifth positive lens element, wherein the third and fourth lens elements are cemented together to form a doublet lens element and wherein the following condition is fulfilled: −0.02<F/F34<0.18 whereF represents a focal length of the entire taking lens system; and F34 represents a focal length of the doublet lens element formed by cementing together the third and fourth lens elements.

28. A fixed focal length taking lens system comprising, in order from an object side:a first negative lens element; a second biconvex lens element; an aperture stop; a third positive lens element; a fourth negative lens element; and a fifth positive lens element, the third, fourth and fifth lens elements having no intervening lenses therebetween, wherein the third and fourth lens elements are cemented together and wherein the following condition is fulfilled: 0.3<F/F345<0.9 whereF represents a focal length of the entire taking lens system; and F345 represents a composite focal length of the third to fifth lens elements.

29. A fixed focal length taking lens system comprising, in order from an object side:a first negative lens element; a second biconvex lens element; an aperture stop; a third positive meniscus lens element convex to an image side; a fourth negative lens element; and a fifth positive lens element, the third, fourth and fifth lens elements having no intervening lenses therebetween, wherein the fourth and fifth lens elements are cemented together and wherein the following condition is fulfilled: 0.3<F/F345<0.9 whereF represents a focal length of the entire taking lens system; and F345 represents a composite focal length of the third to fifth lens elements.