Image forming optical system and electronic image pickup apparatus using the same

CROSS-REFERENCE TO RELATED APPLICATION

The present application is based upon and claims the benefit of priority from the prior Japanese Patent Application No. 2010-119506 filed on May 25, 2010; the entire contents of which are incorporated herein by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an image forming optical system and an electronic image pickup apparatus using the same.

2. Description of the Related Art

In recent years, with an increase in the number of pixels of an image pickup element and the progress of a digital image processing technology, a digital camera has substituted a silver salt 35 mm film camera. Moreover, since the number of pixels of a small-size liquid crystal panel which is used as a finder has increased, even an interchangeable lens camera is undergoing transition from a so-called single-lens reflex camera to a camera of a new concept in which, a quick-return mirror has been eliminated.

Furthermore, since a capacity of a recording medium such as a flash memory and a bit rate of an image processing system has increased in units of digits, video recording of a high image quality is becoming possible. However, for small-sizing of a camera system while mounting a video function of an improved performance, it is necessary to make a focusing-drive portion light.

Lately, for making the focusing-drive portion in a zooming optical system as light as possible, a lens group of a rear portion of an optical system having a small diameter and a fewer number of lens components has been selected. Particularly, the lens group of the rear portion of the optical system includes only one lens component. However, in a camera in which, an image forming performance beyond a certain degree is sought from infinity to an object-point at a close distance, correction of a chromatic aberration, a coma aberration, and a meridional curvature of field is insufficient.

Therefore, for forming a focusing lens group by a plurality of lens components while maintaining a light weight of the focusing lens group, for a lens group more on an image side than an aperture stop, using a lens group which includes one component in which, a thin resin lens is cemented to a base-material lens as a focusing lens group as proposed in Japanese Patent Application Laid-open Publication Nos. 2007-108707, 2007-108715, 2008-191308, and 2008-191311, is to be taken into consideration.

SUMMARY OF THE INVENTION

An image forming optical system according to the present invention includes in order from an object side

a first lens group G1 having a positive refractive power,

a second lens group G2 having a negative refractive power,

an aperture stop,

a third lens group G3 having a positive refractive power, and

a fourth lens group G4 having a negative refractive power, and

at the time of zooming, air distances between the lens groups are variable, and an air lens nearest to an image side in the third lens group has a shape of a convex lens, and

the fourth lens group G4 includes one lens component, and is movable even at the time of focusing, and satisfies the following conditional expressions

0.5<(R4F+R4R)/(R4F−R4R)<8.0 (1)
−12.0<(R4LAF+R4LAR)/(R4LAF−R4LAR)<−2.0 (2)

where,

R4F denotes a radius of curvature on an optical axis of a surface nearest to an object side, of the fourth lens group G4,

R4R denotes a radius of curvature on an optical axis of a surface nearest to an image side, of the fourth lens group G4,

R4LAF denotes a radius of curvature on an optical axis of a surface on the object side of a positive lens LA which is cemented to the fourth lens group G4, and

R4LAR denotes a radius of curvature on an optical axis of a surface on the image side of the positive lens LA which is cemented to the fourth lens group G4.

Moreover, an electronic image pickup apparatus according to the present invention includes

the abovementioned image forming optical system,

an electronic image pickup element, and

an image processing unit which processes image data which has been obtained by picking up an image formed by the image forming optical system by the electronic image pickup element, and outputs as image data in which, a shape of the image has been changed, and

the image forming optical system is a zoom lens, and the zoom lens, at the time of infinite object point focusing, satisfies the following conditional expression

0.70<y₀₇/(fw·tan ω_07w)<0.96 (13)

where,

y₀₇is expressed as y₀₇=0.7·y₁₀, when a distance (the maximum image height) from a center up to the farthest point on an effective image pickup surface (on a surface on which an image can be picked up) of the electronic image pickup element is let to be y₁₀,

ω_07wis an angle with respect to an optical axis in an object-point direction corresponding to an image point from a center on the image pickup surface up to a position of y₀₇, at a wide angle end, and

fw is a focal length of the overall image forming optical system at the wide angle end.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1A, FIG. 1B, and FIG. 1C are cross-sectional views along an optical axis showing an optical arrangement at the time of infinite object point focusing of a zoom lens according to a first embodiment of the present invention, where, FIG. 1A shows a state at a wide angle end, FIG. 1B shows an intermediate state, and FIG. 1C shows a state at a telephoto end;

FIG. 2A, FIG. 2B, and FIG. 2C are diagrams showing a spherical aberration, an astigmatism, a distortion, and a chromatic aberration of magnification at the time of infinite object point focusing of the zoom lens according to the first embodiment, where, FIG. 2A shows a state at the wide angle end, FIG. 2B shows an intermediate state, and FIG. 2C shows a state at the telephoto end;

FIG. 3A, FIG. 3B, and FIG. 3C are diagrams showing a coma aberration of an off-axis light beam at the time of infinite object point focusing of the zoom lens according to the first embodiment, where, FIG. 3A shows a state at the wide angle end, FIG. 3B shows an intermediate state, and FIG. 3C shows a state at the telephoto end;

FIG. 4A, FIG. 4B, and FIG. 4C are cross-sectional views along an optical axis showing an optical arrangement at the time of infinite object point focusing of a zoom lens according to a second embodiment of the present invention, where, FIG. 4A shows a state at a wide angle end, FIG. 4B shows an intermediate state, and FIG. 4C shows a state at a telephoto end;

FIG. 5A, FIG. 5B, and FIG. 5C are diagrams showing a spherical aberration, an astigmatism, a distortion, and a chromatic aberration of magnification at the time of infinite object point focusing of the zoom lens according to the second embodiment, where, FIG. 5A shows a state at the wide angle end, FIG. 5B shows an intermediate state, and FIG. 5C shows a state at the telephoto end;

FIG. 6A, FIG. 6B, and FIG. 6C are diagrams showing a coma aberration of an off-axis light beam at the time of infinite object point focusing of the zoom lens according to the second embodiment, where, FIG. 6A shows a state at the wide angle end, FIG. 6B shows an intermediate state, and FIG. 6C shows a state at the telephoto end;

FIG. 7A, FIG. 7B, and FIG. 7C are cross-sectional views along an optical axis showing an optical arrangement at the time of infinite object point focusing of a zoom lens according to a third embodiment of the present invention, where, FIG. 7A shows a state at a wide angle end, FIG. 7B shows an intermediate state, and FIG. 7C shows a state at a telephoto end;

FIG. 8A, FIG. 8B, and FIG. 8C are diagrams showing a spherical aberration, an astigmatism, a distortion, and a chromatic aberration of magnification at the time of infinite object point focusing of the zoom lens according to the third embodiment, where, FIG. 8A shows a state at the wide angle end, FIG. 8B shows an intermediate state, and FIG. 8C shows a state at the telephoto end;

FIG. 9A, FIG. 9B, and FIG. 9C are diagrams showing a coma aberration of an off-axis light beam at the time of infinite object point focusing of the zoom lens according to the third embodiment, where, FIG. 9A shows a state at the wide angle end, FIG. 9B shows an intermediate state, and FIG. 9C shows a state at the telephoto end;

FIG. 10A, FIG. 10B, and FIG. 10C are cross-sectional views along an optical axis showing an optical arrangement at the time of infinite object point focusing of a zoom lens according to a fourth embodiment of the present invention, where, FIG. 10A shows a state at a wide angle end, FIG. 10B shows an intermediate state, and FIG. 10C shows a state at a telephoto end;

FIG. 11A, FIG. 11B, and FIG. 11C are diagrams showing a spherical aberration, an astigmatism, a distortion, and a chromatic aberration of magnification at the time of infinite object point focusing of the zoom lens according to the fourth embodiment, where, FIG. 11A shows a state at the wide angle end, FIG. 11B shows an intermediate state, and FIG. 11C shows a state at the telephoto end;

FIG. 12A, FIG. 12B, and FIG. 12C are diagrams showing a coma aberration of a off-axis light beam at the time of infinite object point focusing of the zoom lens according to the fourth embodiment, where, FIG. 12A shows a state at the wide angle end, FIG. 12B shows an intermediate state, and FIG. 12C shows a state at the telephoto end;

FIG. 13 is a front perspective view showing an appearance of a digital camera 40 in which, a zooming optical system according to the present invention is incorporated;

FIG. 14 is a rear perspective view of the digital camera 40;

FIG. 15 is a cross-sectional view showing an optical arrangement of the digital camera 40;

FIG. 16 is a front perspective view of a state in which, a cover of a personal computer 300 which is an example of an information processing apparatus in which, the zooming optical system of the present invention is built-in as an objective optical system, is opened;

FIG. 17 is a cross-sectional view of a photographic optical system 303 of the personal computer 300;

FIG. 18 is a side view of the personal computer 300; and

FIG. 19A, FIG. 19B, and FIG. 19C are diagrams showing a mobile telephone which is an example of the information processing apparatus in which, the zooming optical system of the present invention is built-in as a photographic optical system, where, FIG. 19A is a front view of a mobile telephone 400, FIG. 19B is a side view of the mobile telephone 400, and FIG. 19C is a cross-sectional view of a photographic optical system 405.

DETAILED DESCRIPTION OF THE INVENTION

Exemplary embodiments of an image forming optical system and an electronic image pickup apparatus according to the present invention will be described below in detail by referring to the accompanying diagrams. However, the present invention is not restricted to the embodiments described below.

Prior to the description of the embodiments, an action and an effect of the image forming optical system according to the embodiments will be described below. In the following description, a lens having a positive value of a paraxial focal length is let to be a positive lens and a lens having a negative value of a paraxial focal length is let to be a negative lens.

In the image forming optical system according to the embodiments, an image forming optical system which includes in order from an object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop, a third lens group G3 having a positive refractive power, and a fourth lens group G4 having a negative refractive power, and in which, at the time of zooming, air distances between the lens groups are variable, has been used.

Particularly, the fourth lens group G4 is let to be a lens group which moves for focusing, and furthermore, the fourth lens group G4 includes only one lens component. Accordingly, it is possible to make the lens group which moves for focusing, to be light weight. Moreover, for correcting aberrations which are degraded accordingly, particularly, a coma aberration and a meridional curvature of field, an air lens nearest to an image side in the third lens group G3 is let to have a shape of a convex lens. Moreover, the image forming optical system (the fourth lens group G4) satisfies the following conditional expressions.

0.5<(R4F+R4R)/(R4F−R4R)<8.0 (1)
−12.0<(R4LAF+R4LAR)/(R4LAF−R4LAR)<−2.0 (2)

where,

R4F denotes a radius of curvature on an optical axis of a surface nearest to the object side, of the fourth lens group G4,

R4R denotes a radius of curvature on an optical axis of a surface nearest to an image side, of the fourth lens group G4,

R4LAF denotes a radius of curvature on an optical axis of a surface on the object side of a positive lens LA which is cemented to the fourth lens group G4, and

R4LAR denotes a radius of curvature on an optical axis of a surface on the image side of the positive lens LA which is cemented to the fourth lens group G4.

When a range of any of conditional expressions (1) and (2) is surpassed, even when the air lens nearest to the image side in the third lens group G3 is let to have a shape of a convex lens, correction of the coma aberration and the meridional curvature of field over an entire area which can be focused, becomes difficult.

It is more preferable that the fourth lens group G4 satisfies the following conditional expression (1′) instead of conditional expression (1).

1.5<(R4F+R4R)/(R4F−R4R)<5.0 (1′)

Furthermore, it is all the more preferable that the fourth lens group G4 satisfies the following conditional expression (1″) instead of conditional expression (1).

1.8<(R4F+R4R)/(R4F−R4R)<4.0 (1″)

It is more preferable that the fourth lens group G4 satisfies the following conditional expression (2′) instead of conditional expression (2).

−9.0<(R4LAF+R4LAR)/(R4LAF−R4LAR)<−3.0 (2′)

Furthermore, it is all the more preferable that the fourth lens group G4 satisfies the following conditional expression (2″) instead of conditional expression (2).

−7.0<(R4LAF+R4LAR)/(R4LAF−R4LAR)<−4.0 (2″)

Moreover, it is preferable that a surface on the object side of the air lens nearest to the image side of the third lens group G3 is let to have a convex shape with a large curvature, and furthermore, satisfies the following conditional expression.

−8.0<(R3ALF+R3ALR)/(R3ALF−R3ALR)<−0.3 (3)

where,

R3ALF denotes a radius of curvature on an optical axis of a surface on the object side of the air lens nearest to the image side, of the third lens group G3, and

R3ALR denotes a radius of curvature on an optical axis of a surface on the image side of the air lens nearest to the image side, of the third lens group G3.

When a range of conditional expression (3) is surpassed, even when conditional expressions (1) and (2) are satisfied, correction of the coma aberration and the meridional curvature of field over an entire area which can be focused becomes difficult.

It is more preferable that the third lens group G3 satisfies the following conditional expression (3′) instead of conditional expression (3).

−6.0<(R3ALF+R3ALR)/(R3ALF−R3ALR)<−0.6 (3′)

Furthermore, it is all the more preferable that the third lens group G3 satisfies the following conditional expression (3″) instead of conditional expression (3).

−4.0<(R3ALF+R3ALR)/(R3ALF−R3ALR)<−0.9 (3″)

Moreover, in the image forming optical system according to the present invention, it is preferable that the fourth lens group G4 includes a cemented lens component in which, a plurality of lenses including the positive lens LA are cemented, and

in a rectangular coordinate system in which, a horizontal axis is let to be νd and a vertical axis is let to be nd, when a straight line expressed by

nd=a×νd+b (provided that a=−0.0267)

is set, nd and νd of the positive lens LA are included in an area which is determined by a straight line when it is a lower limit value of a range of the following conditional expression (4) and a straight line when it is an upper limit value of the range of the following conditional expression (4), and an area determined by the following conditional expression (5).

2.00<b<2.40 (provided that nd>1.45) (4)
νd<26.0 (5)

where,

νd denotes Abbe's number (nd−1)/(nF−nC) for the positive lens LA, and

nd, nC, nF denote refractive indices of the positive lens LA for a d-line, a C-line, and an F-line respectively.

When an upper limit value of conditional expression (4) is surpassed, correction of Petzval's sum is susceptible to be difficult, and correction of the meridional curvature of field becomes difficult.

When a lower limit value of conditional expression (4) is surpassed, correction of the coma aberration becomes difficult.

When an upper limit value of conditional expression (5) is surpassed, a fluctuation in a chromatic aberration due to focusing is susceptible to increase.

It is more preferable that the image forming optical system according to the present invention satisfies the following conditional expression (4′) instead of conditional expression (4).

2.10<b<2.33 (4′)

Furthermore, it is all the more preferable that the image forming optical system according to the present invention satisfies the following conditional expression (4″) instead of conditional expression (4).

2.20<b<2.29 (4″)

It is more preferable that the image forming optical system according to the present invention satisfies the following conditional expression (5′) instead of conditional expression (5).

νd<25.0 (5′)

Furthermore, it is all the more preferable that the image forming optical system according to the present invention satisfies the following conditional expression (5″) instead of conditional expression (5).

νd<24.2 (5″)

in a rectangular coordinate system in which, a horizontal axis is let to be νd and a vertical axis is let to be θgF, when a straight line expressed by

θgF=α×νd+β (provided that α=−0.00566)

is set, θgF and νd of the positive lens LA in the fourth group G4 are included in both areas namely, an area determined by a straight line when it is a lower limit value of a range of the following conditional expression (6) and a straight line when it is an upper limit value of the range of the following conditional expression (6), and an area determined by the following conditional expression (5).

0.7200<β<0.8300 (6)
νd<26 (5)

where,

θgF denotes a partial dispersion ratio (ng−nF)/(nF−nC) of the positive lens LA,

νd denotes Abbe's number (nd−1)/(nF−nC) of the positive lens LA, and

nd, nC, nF, and ng denote refractive indices of the positive lens LA for a d-line, a C-line, an F-line, and a g-line respectively.

When a glass material which surpasses an upper limit value of conditional expression (6) is used, correction of chromatic aberration of magnification due to a secondary spectrum, or in other words, the chromatic aberration of magnification for the g-line when achromatized for the F-line and the C-line, is not sufficient. Therefore, in an image which has been picked up, it is difficult to secure sharpness in a similar manner.

When a glass material which surpasses a lower limit value of conditional expression (6) is used, correction of longitudinal chromatic aberration due to the secondary spectrum, or in other words, the longitudinal chromatic aberration for the g-line when achromatized for the F-line and the C-line is not sufficient. Therefore, in an image which has been picked up, it is difficult to secure sharpness in a similar manner.

It is more preferable that the image forming optical system according to the present invention satisfies the following conditional expression (6′) instead of conditional expression (6).

0.7400<β<0.8200 (6′)

Furthermore, it is all the more preferable that the image forming optical system according to the present invention satisfies the following conditional expression (6″) instead of conditional expression (6).

0.7580<β<0.8100 (6)

Moreover, in the image forming optical system according to the present invention, it is preferable that in a rectangular coordinate system other than the rectangular coordinate system with νd as a horizontal axis and θgF as a vertical axis, in which, the horizontal axis is let to be νd and the vertical axis is let to be θgh, when a straight line expressed by

θhg=αhg×νd+βhg (provided that αhg=−0.00834)

is set, θhg and νd of the positive lens LA in the fourth lens group G4 are included in both areas namely, an area determined by a straight line when it is a lower limit value of a range of the following conditional expression (7) and a straight line when it is an upper limit value of the range of the following conditional expression (7), and an area determined by the following conditional expression (5).

0.7600<βhg<0.9000 (7)
νd<26 (5)

where,

θhg denotes a partial dispersion ratio (nh−ng)/(nF−nC) of the positive lens LA, and

nh denotes a refractive index of the positive lens LA for an h-line.

When a glass material which surpasses an upper limit value of conditional expression (7) is used, correction of chromatic aberration of magnification due to the secondary spectrum, or in other words, the chromatic aberration of magnification for the h-line when achromatized for the F-line and the C-line, is not sufficient. Therefore, in an image which has been picked up, chromatic spreading and chromatic flare of purple are susceptible to occur in a similar manner.

When a glass material which surpasses a lower limit value of conditional expression (7) is used, correction of longitudinal chromatic aberration due to the secondary spectrum, or in other words, the longitudinal chromatic aberration for the h-line when achromatized for the F-line and the C-line is not sufficient. Therefore, in an image which has been picked up, chromatic spreading and chromatic flare for purple are susceptible to occur in a similar manner.

It is more preferable that the image forming optical system according to the present invention satisfies the following conditional expression (7′) instead of conditional expression (7).

0.7650<βhg<0.8700 (7′)

Furthermore, it is all the more preferable that the image forming optical system according to the present invention satisfies the following conditional expression (7″) instead of conditional expression (7).

0.7680<βhg<0.8620 (7″)

Moreover, in the image forming optical system according to the present invention, it is preferable that the fourth lens group G4 includes a cemented lens component in which, only two lenses namely, the positive lens LA and a negative lens LB are cemented.

Moreover, in the image forming optical system according to the present invention, it is preferable that when a lens having a negative value of a paraxial focal length is let to be a negative lens, a lens LB to which, the positive lens LA is to be cemented is a negative lens,

- and satisfies the following conditional expression.
  
  0.000≦θgF(LA)−θgF(LB)≦0.200 (8)

where,

θgF(LA) denotes a partial dispersion ratio (ng−nF)/(nF−nC) of the positive lens LA, and

θgF(LB) denotes a partial dispersion ratio (ng−nF)/(nF−nC) of the lens LB which is to be cemented.

When a glass material which surpasses an upper limit value of conditional expression (8) is used, correction of chromatic aberration of magnification due to the secondary spectrum, or in other words, the chromatic aberration of magnification for the g-line when achromatized for the F-line and the C-line, is not sufficient. Therefore, in an image which has been picked up, it is difficult to secure sharpness in a similar manner.

When a glass material which surpasses a lower limit value of conditional expression (8) is used, correction of longitudinal chromatic aberration due to the secondary spectrum, or in other words, the longitudinal chromatic aberration for the g-line when achromatized for the F-line and the C-line is not sufficient. Therefore, in an image which has been picked up, it is difficult to secure sharpness in a similar manner.

Moreover, it is more desirable that the negative lens satisfies the following conditional expression (8′) instead of conditional expression (8).

0.050≦θgF(LA)−θgF(LB)≦0.150 (8′)

Furthermore, it is all the more preferable that the negative lens satisfies the following conditional expression (8″) instead of conditional expression (8).

0.065≦θgF(LA)−θgF(LB)≦0.130 (8″)

- and satisfies the following conditional expression.
  
  0.000≦θhg(LA)−θhg(LB)≦0.300 (9)

where,

θhg(LA) denotes a partial dispersion ratio (nh−ng)/(nF−nC) of the positive lens LA, and

θhg(LB) denotes a partial dispersion ratio (nh−ng)/(nF−nC) of the lens LB which is to be cemented.

When a glass material which surpasses an upper limit value of conditional expression (9) is used, correction of chromatic aberration of magnification due to the secondary spectrum, or in other words, the chromatic aberration of magnification for the h-line when achromatized for the F-line and the C-line, is not sufficient. Therefore, in an image which has been picked up, chromatic spreading and chromatic flare of purple are susceptible to occur in a similar manner.

When a glass material which surpasses a lower limit value of conditional expression (9) is used, correction of longitudinal chromatic aberration due to the secondary spectrum, or in other words, the longitudinal chromatic aberration for the h-line when achromatized for the F-line and the C-line is not sufficient. Therefore, in an image which has been picked up, chromatic spreading and chromatic flare for purple are susceptible to occur.

Moreover, it is more desirable that the negative lens satisfies the following conditional expression (9′) instead of conditional expression (9).

0.100≦θhg(LA)−θhg(LB)≦0.250 (9′)

Furthermore, it is all the more preferable that the negative lens satisfies the following conditional expression (9″) instead of conditional expression (9).

0.105≦θhg(LA)−θhg(LB)≦0.210 (9″)

Moreover, in the image forming optical system according to the present invention, it is preferable that when a lens having a negative value of a paraxial focal length is let to be a negative lens, a lens LB to which the positive lens LA is to be cemented is a negative lens,

- and satisfies the following conditional expression.
  
  νd(LA)−νd(LB)≦−15 (10)

where,

νd(LA) denotes Abbe's number (nd−1)/(nF−nC) of the positive lens LA, and

νd(LB) denotes Abbe's number (nd−1)/(nF−nC) of the lens LB which is to be cemented.

When an upper limit value of conditional expression (10) is surpassed, a fluctuation in the chromatic aberration due to focusing is susceptible to increase.

Incidentally, let us assume that an image of an object at infinity has been formed by an optical system having no distortion. In this case, since there is no distortion of the image which has been formed, the following relationship holds true.

f=y/tan ω (11)

where,

y is a height of an image point from an optical axis,

f is a focal length of the image forming system, and

ω is an angle with respect to an optical axis in an object-point direction corresponding to an image point from a center on an image pickup surface up to a position of y.

However, when there is a barrel distortion in the optical system, the following relationship holds true.

f>y/tan ω (12)

In other words, when f and y are let to be constant values, ω assumes a large value.

Therefore, in an electronic image pickup apparatus, it is preferable to use intentionally an optical system having a large barrel distortion for a focal length near a wide angle end in particular. In this case, it is possible to achieve widening of an angle of field of the optical system, as the purpose is served without correcting the distortion.

However, an image of an object is formed on an electronic image pickup element, with a barrel distortion. Therefore, in the electronic image pickup apparatus, an arrangement has been made such that image data acquired by the electronic image pickup element is processed by image processing. In the image processing, the image data (shape of the image) is changed to correct the barrel distortion.

When such an arrangement is made, the image data which has been acquired finally is image data having a shape almost similar to the object. Therefore, based on this image data, the image of the object is to be output to a CRT (cathode ray tube) or a printer.

In this case, for the image forming optical system, it is preferable to use zoom lens which satisfies the following conditional expression (13) at the time of almost infinite object point focusing, namely, at the time of focusing at an object point which is infinite distance.

0.70<y₀₇/(fw·tan ω_07w)<0.96 (13)

where,

fw is a focal length of the overall image forming optical system at the wide angle end.

Conditional expression (13) is an expression in which, an amount of barrel distortion at a zoom wide angle end is regulated. When the zoom lens satisfies conditional expression (13), it is possible to fetch information of a wide angle of field without making the optical system thick. The image distorted to be barrel shaped is subjected to photoelectric conversion by the image pickup element, and becomes image data which is distorted to be barrel shaped.

The image data which is distorted to be barrel shaped is subjected to a process equivalent to a shape-change of an image electrically by the image processing unit which is a signal processing system of the electronic image pickup apparatus. When such an arrangement is made, even when image data which has been output finally from the image processing unit is reproduced by a display apparatus, the distortion is corrected and an image almost similar to a shape of the object is achieved.

Here, when an upper limit value of conditional expression (13) is surpassed, and particularly, a value close to 1 is assumed, an image in which, the distortion has been corrected favorably is achieved. Therefore, a small correction carried out by the image processing unit serves the purpose. However, it is difficult to widen the angle of field of the optical system while maintaining the small size of the optical system.

Whereas, when a lower limit value of conditional expression (13) is surpassed, in a case in which, an image distortion due to distortion of the optical system is corrected by the image processing unit, a rate of drawing in a direction of irradiation in a portion surrounding an angle of field becomes excessively large. As a result, in an image which has been picked up, degradation of sharpness in a portion surrounding the image becomes conspicuous.

In such manner, by the zoom lens satisfying conditional expression (13), small sizing and widening of angle (making an angle of field in a perpendicular direction with distortion to be 38° or more) become possible.

In the image forming optical system according to the present invention, it is preferable that the zoom lens satisfies the following conditional expression (13′) instead of conditional expression (13).

0.80<y₀₇/(fw·tan ω_07w)<0.95 (13′)

Furthermore, it is all the more preferable that the zoom lens satisfies the following conditional expression (13″) instead of conditional expression (13).

0.84<y₀₇/(fw·tan ω_07w)<0.94 (13″)

Here, a glass material means a lens material such as glass and a resin. Moreover, for a cemented lens, a lens which has been selected appropriately from these glass materials is to be used.

Moreover, in the image forming optical system according to the present invention, it is preferable that the cemented lens includes a first lens and a second lens which are thin at a center of an optical axis, and that the first lens satisfies conditional expressions (1) and (2), or conditional expressions (3) and (2). When such an arrangement is made, a further improvement in a correction effect of various aberrations and a further slimming of lens groups can be anticipated.

Moreover, it is desirable that the cemented lens is a composite lens. It is possible to realize a composite lens by curing upon adhering closely a resin as a first lens to a surface of a second lens. By letting the cemented lens to be a composite lens, it is possible to improve a manufacturing accuracy. As a method of manufacturing a composite lens, molding is available. In molding, there is a method in which, a material of the first lens (such as an energy curable transparent resin) is brought in contact with the second lens, and the first lens material is adhered closely to the second lens material directly. This method is extremely effective for thinning a lens element.

Moreover, in a case of letting the cemented lens to be a composite lens, a glass, as the first lens, may be adhered closely to a surface of the second lens, and hardened. Glass, as compared to a resin, is advantageous from a point of resistance such as a light resistance and a chemical resistance. In this case, as properties of the first lens material, it is necessary that, a melting point and a transition point of the first lens material are lower than a melting point and a transition point of the material of the second lens. As a method of manufacturing a composite lens, molding is available. In molding, there is a method in which, the first lens material is brought in contact with the second lens, and the first lens material is adhered closely to the second lens directly. This method is extremely effective for thinning a lens element.

As an example of the energy curable resin, an ultraviolet-curing resin is available. In both the cases namely, a case in which the first lens is made of a resin and a case in which the first lens is made of glass, a surface treatment such as coating may be carried out in advance on a lens which becomes a base material. Moreover, when the second lens is thin, the second lens may be adhered closely to the first lens.

Moreover, it is preferable to dispose a prism in the image forming optical system. The prism is to be used for bending (reflecting) an optical path of the optical system. Particularly, when the image forming optical system is a zoom lens, it is possible to make a dimension of depth thin (to shorten an overall length). It is preferable to dispose the prism in a positive lens group which is first from the object side, or in a negative lens group.

Moreover, in the image forming optical system according to the present invention, it is preferable that the lens LA satisfies the following conditional expression (14).

1.58<nd<1.76 (14)

where,

nd denotes a refractive index of a medium of the lens LA.

When the lens LA satisfies conditional expression (14), correction of a spherical aberration and a correction of astigmatism can be carried out favorably.

It is more preferable that the lens LA satisfies the following conditional expression (14′) instead of conditional expression (14).

1.62<nd<1.72 (14′)

Furthermore, it is all the more preferable that the lens LA satisfies the following conditional expression (14″) instead of conditional expression (14).

1.63<nd<1.68 (14″)

Moreover, it is preferable that the image forming optical system according to the present invention is a zoom lens, and that relative distances on an optical axis between lens groups vary at the time of zooming. It is preferable to use the cemented lens in such image forming optical system (zoom lens).

Moreover, in a case of using the lens LA in the cemented lens, the lens LA is to be cemented to a lens LB. In this case, it is preferable to make a thickness of the lens LA at a center of the optical axis to be thinner than a thickness of the lens LB at the center of the optical axis. Moreover, it is preferable that a thickness t1 of the lens LA at the center of the optical axis satisfies the following conditional expression (15).

0.3<t1<1.5 (15)

By the thickness t1 of the lens LA satisfying conditional expression (15), it is possible to realize a small-size optical system. Moreover, in a case of making the lens LA by molding, it is possible to carry out stable molding.

It is more preferable that the thickness t1 of the lens LA satisfies the following conditional expression (15′) instead of conditional expression (15).

0.4<t1<1.2 (15′)

Furthermore, it is all the more preferable that the thickness t1 of the lens LA satisfies the following conditional expression (15″) instead of conditional expression (15).

0.5<t1<1.0 (15″)

It is preferable that at least one surface of the lens LA is an aspheric surface.

By an image forming optical system for an interchangeable lens still camera having a video function satisfying conditional expressions of the present invention mentioned above, and being provided with the abovementioned structural characteristics, it is possible to make a focusing lens group of the image forming optical system light-weight. Furthermore, it is possible to correct favorably the chromatic aberration, the coma aberration, and the meridional curvature of field. Moreover, in the electronic image pickup apparatus, by using the abovementioned image forming optical system, it is possible to realize a high-speed focusing, a reduction of consumption of electric power, and sharpening of image.

Embodiments

Four exemplary embodiments of the zoom lens will be described below.

To start with, a zoom lens according to a first embodiment of the present invention will be described below. FIG. 1A, FIG. 1B, and FIG. 1C are cross-sectional views along an optical axis showing an optical arrangement at the time of infinite object point focusing of the zoom lens according to the first embodiment of the present invention, where, FIG. 1A shows a state at a wide angle end, FIG. 1B shows an intermediate focal length state, and FIG. 1C shows a state at a telephoto end.

FIG. 2A, FIG. 2B, and FIG. 2C are diagrams showing a spherical aberration (SA), an astigmatism (AS), a distortion (DT), and a chromatic aberration of magnification (CC) at the time of infinite object point focusing of the zoom lens according to the first embodiment, where, FIG. 2A shows a state at the wide angle end, FIG. 2B shows an intermediate state, and FIG. 2C shows a state at the telephoto end.

FIG. 3A, FIG. 3B, and FIG. 3C are diagrams showing a coma aberration (longitudinal aberration) DZY of an off-axis beam at the time of infinite object point focusing of the zoom lens according to the first embodiment, where, FIG. 3A shows a state at the wide angle end, FIG. 3B shows an intermediate focal length state, and FIG. 3C shows a state at the telephoto end.

The zoom lens according to the first embodiment, as shown in FIG. 1A, FIG. 1B, and FIG. 1C, includes in order from an object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, a third lens group G3 having a positive refractive power, and a fourth lens group G4 having a negative refractive power. In all the embodiments which will be described below, in the lens cross-sectional views, CG denotes a cover glass which may have a low pass filter function, and I denotes an image pickup surface of an electronic image pickup element.

The first lens group G1 includes a cemented lens of a negative meniscus lens L1 having a convex surface directed toward the object side and a positive meniscus lens L2 having a convex surface directed toward the object side, in order from the object side, and has a positive refractive power as a whole.

The second lens group G2 includes in order from the object side, a negative meniscus lens L3 having a convex surface directed toward the object side, a biconcave negative lens L4, and a biconvex positive lens L5, and has a negative refractive power as a whole.

The third lens group G3 includes a positive meniscus lens L6 having a convex surface directed toward the object side, a cemented lens of a negative meniscus lens L7 having a convex surface directed toward the object side and a biconvex positive lens L8, a negative meniscus lens L9 having a convex surface directed toward the object side, and a biconvex positive lens L10, and has a positive refractive power as a whole.

The fourth lens group G4 includes a cemented lens of a negative meniscus lens L11 having a convex surface directed toward the object side and a positive meniscus lens L12 having a convex surface directed toward the object side, and has a negative refractive power as a whole.

The negative meniscus lens L11 corresponds to the lens LB according to the present invention, and the positive meniscus lens L12 corresponds to the lens LA according to the present invention.

At the time of zooming from the wide angle end to the telephoto end, the first lens group G1 is fixed. The second lens group G2 moves toward an image side. The third lens group G3 moves toward the object side. The fourth lens group G4 moves toward the object side.

An aspheric surface is provided to four surfaces namely, a surface on the object side of the biconcave negative lens L4 in the second lens group G2, and both surfaces of the positive meniscus lens L6 and a surface on the image side of the biconvex positive lens L8 in the third lens group G3.

Next, a zoom lens according to a second embodiment of the present invention will be described below. FIG. 4A, FIG. 4B, and FIG. 4C are cross-sectional views along an optical axis showing an optical arrangement at the time of infinite object point focusing of the zoom lens according to the second embodiment of the present invention, where, FIG. 4A shows a state at a wide angle end, FIG. 4B shows an intermediate focal length state, and FIG. 4C shows a state at a telephoto end.

FIG. 5A, FIG. 5B, and FIG. 5C are diagrams showing a spherical aberration (SA), an astigmatism (AS), a distortion (DT), and a chromatic aberration of magnification (CC) at the time of infinite object point focusing of the zoom lens according to the second embodiment, where, FIG. 5A shows a state at the wide angle end, FIG. 5B shows an intermediate focal length state, and FIG. 5C shows a state at the telephoto end.

FIG. 6A, FIG. 6B, and FIG. 6C are diagrams showing a coma aberration (longitudinal aberration) DZY of an off-axis beam at the time of infinite object point focusing of the zoom lens according to the second embodiment, where, FIG. 6A shows a state at the wide angle end, FIG. 6B shows an intermediate focal length state, and FIG. 6C shows a state at the telephoto end.

The zoom lens according to the second embodiment, as shown in FIG. 4A, FIG. 4B, and FIG. 4C, includes in order from an object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, a third lens group G3 having a positive refractive power, and a fourth lens group G4 having a negative refractive power.

The first lens group G1 includes a cemented lens of a negative meniscus lens L1 having a convex surface directed toward the object side and a biconvex positive lens L2, in order from the object side, and has a positive refractive power as a whole.

The second lens group G2 includes in order from the object side, a negative meniscus lens L3 having a convex surface directed toward the object side, a biconcave negative lens L4, and a positive meniscus lens L5 having a convex surface directed toward the object side, and has a negative refractive power as a whole.

The third lens group G3 includes a cemented lens of a biconvex positive lens L6 and a biconcave negative lens L7, a biconvex positive lens L8, a biconcave negative lens L9, and a positive meniscus lens L10 having a convex surface directed toward the object side, and has a positive refractive power as a whole.

The negative meniscus lens L11 corresponds to the lens LB according to the present invention, and the positive meniscus lens L12 corresponds to the lens LA according to the present invention.

An aspheric surface is provided to five surfaces namely, a surface on the object side of the biconcave negative lens L4 in the second lens group G2, a surface on the object side of the biconvex positive lens L6 on the object side and both surfaces of the biconvex positive lens L8 in the third lens group G3, and a surface on the image side of the positive meniscus lens L12 in the fourth lens group G4.

Next, a zoom lens according to a third embodiment of the present invention will be described below. FIG. 7A, FIG. 7B, and FIG. 7C are cross-sectional views along an optical axis showing an optical arrangement at the time of infinite object point focusing of the zoom lens according to the third embodiment of the present invention, where, FIG. 7A shows a state at a wide angle end, FIG. 7B shows an intermediate focal length state, and FIG. 7C shows a state at a telephoto end.

FIG. 8A, FIG. 8B, and FIG. 8C are diagrams showing a spherical aberration (SA), an astigmatism (AS), a distortion (DT), and a chromatic aberration of magnification (CC) at the time of infinite object point focusing of the zoom lens according to the third embodiment, where, FIG. 8A shows a state at the wide angle end, FIG. 8B shows an intermediate focal length state, and FIG. 8C shows a state at the telephoto end.

FIG. 9A, FIG. 9B, and FIG. 9C are diagrams showing a coma aberration (longitudinal aberration) DZY of an off-axis beam at the time of infinite object point focusing of the zoom lens according to the third embodiment, where, FIG. 9A shows a state at the wide angle end, FIG. 9B shows an intermediate focal length state, and FIG. 9C shows a state at the telephoto end.

The zoom lens according to the third embodiment, as shown in FIG. 7A, FIG. 7B, and FIG. 7C, includes in order from an object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, a third lens group G3 having a positive refractive power, and a fourth lens group G4 having a negative refractive power.

The second lens group G2 includes in order from the object side, a biconcave negative lens L3, a negative meniscus lens L4 having a convex surface directed toward the object side, and a positive meniscus lens L5 having a convex surface directed toward the object side, and has a negative refractive power as a whole.

The third lens group G3 includes a positive meniscus lens L6 having a convex surface directed toward the object side, a biconvex positive lens L7, a biconcave negative lens L8, and a biconvex positive lens L9, and has a positive refractive power as a whole.

The fourth lens group G4 includes a cemented lens of a negative meniscus lens L10 having a convex surface directed toward the object side and a positive meniscus lens L11 having a convex surface directed toward the object side, and has a negative refractive power as a whole.

The negative meniscus lens L10 corresponds to the lens LB according to the present invention, and the positive meniscus lens L11 corresponds to the lens LA according to the present invention.

An aspheric surface is provided to five surfaces namely, a surface on the object side of the negative meniscus lens L4 in the second lens group G2, a surface on the object side of the positive meniscus lens L6 and both surfaces of the biconvex positive lens L7 on the object side in the third lens group G3, and a surface on the image side of the positive meniscus lens L11 in the fourth lens group G4.

Next, a zoom lens according to a fourth embodiment of the present invention will be described below. FIG. 10A, FIG. 10B, and FIG. 10C are cross-sectional views along an optical axis showing an optical arrangement at the time of infinite object point focusing of the zoom lens according to the fourth embodiment of the present invention, where, FIG. 10A shows a state at a wide angle end, FIG. 10B shows an intermediate focal length state, and FIG. 10C shows a state at a telephoto end.

FIG. 11A, FIG. 11B, and FIG. 11C are diagrams showing a spherical aberration (SA), an astigmatism (AS), a distortion (DT), and a chromatic aberration of magnification (CC) at the time of infinite object point focusing of the zoom lens according to the fourth embodiment, where, FIG. 11A shows a state at the wide angle end, FIG. 11B shows an intermediate focal length state, and FIG. 11C shows a state at the telephoto end.

FIG. 12A, FIG. 12B, and FIG. 12C are diagrams showing a coma aberration (longitudinal aberration) DZY of an off-axis beam at the time of infinite object point focusing of the zoom lens according to the fourth embodiment, where, FIG. 12A shows a state at the wide angle end, FIG. 12B shows an intermediate focal length state, and FIG. 12C shows a state at the telephoto end.

The zoom lens according to the fourth embodiment, as shown in FIG. 10A, FIG. 10B, and FIG. 10C, includes in order from an object side, a first lens group G1 having a positive refractive power, a second lens group G2 having a negative refractive power, an aperture stop S, a third lens group G3 having a positive refractive power, and a fourth lens group G4 having a negative refractive power.

The third lens group G3 includes a positive meniscus lens L6 having a convex surface directed toward the object side, a biconvex positive lens L7, a negative meniscus lens L8 having a convex surface directed toward the object side, and a positive meniscus lens L9 having a convex surface directed toward an image side, and has a positive refractive power as a whole.

The negative meniscus lens L10 corresponds to the lens LB according to the present invention, and the positive meniscus lens L11 corresponds to the lens LA according to the present invention.

At the time of zooming from the wide angle end to the telephoto end, the first lens group G1 is fixed. The second lens group G2 moves toward the image side. The third lens group G3 moves toward the object side. The fourth lens group G4 moves toward the object side.

An aspheric surface is provided to five surfaces namely, a surface on the object side of the negative meniscus lens L4 in the second lens group G2, a surface on the object side of the positive meniscus lens L6, and both surfaces of the biconvex positive lens L7 in the third lens group G3, and a surface on the image side of the positive meniscus lens L11 in the fourth lens group G4.

Numerical data of each embodiment described above is shown below. Each of r1, r2, . . . denotes radius of curvature of each lens surface, each of d1, d2, . . . denotes a distance between two lenses, each of nd1, nd2, . . . denotes a refractive index of each lens for a d-line, and each of νd1, νd2, . . . denotes an Abbe constant for each lens. F_NOdenotes an F number, f denotes a focal length of the entire zoom lens system, Further, * denotes an aspheric data, S denotes a stop.

When z is let to be an optical axis with a direction of traveling of light as a positive (direction), and y is let to be in a direction orthogonal to the optical axis, a shape of the aspheric surface is described by the following expression.

z=(y²/r)/[1+{1−(K+1)(y/r)²}^1/2]+A₄y⁴+A₆y⁶+A₈y⁸+A₁₀y¹⁰+A₁₂y¹²

where, r denotes a paraxial radius of curvature, K denotes a conical coefficient, A4, A6, A8, A10, and A₁₂denote aspherical surface coefficients of a fourth order, a sixth order, an eight order, a tenth order, and a twelfth order respectively. Moreover, in the aspherical surface coefficients, ‘e−n’ (where, n is an integral number) indicates ‘10⁻ⁿ’.

Example 1

Unit mm

Surface data

effective

Surface no.
r
d
nd
νd
radius

Object plane
∞
∞

1
55.9710
1.5000
1.92286
18.90
20.000

2
49.4676
3.7352
1.80400
46.57
16.883

3
143.9824
Variable

15.869

4
90.1274
1.5053
1.84666
23.78
14.000

5
13.8963
7.4674

10.710

6*
−40.0282
1.1523
1.69350
53.20
10.478

7
26.4226
0.4177

10.428

8
24.4014
4.8612
1.84666
23.78
10.688

9
−79.3088
Variable

10.591

10(stop)
∞
Variable

4.670

11*
18.0936
2.7323
1.82080
42.71
7.000

12*
165.5978
4.2202

7.022

13
22.9053
1.3929
1.84666
23.78
7.204

14
10.6875
4.1457
1.49700
81.54
6.847

15*
−83.1506
0.1000

6.886

16
92.4799
0.5700
1.80000
29.84
6.910

17
20.7081
2.1302

6.904

18
39.8829
3.9655
1.78590
44.20
7.402

19
−62.6006
Variable

7.614

20
97.2996
1.0000
1.83481
42.71
7.692

21
21.3586
1.0000
1.63547
22.84
7.661

22
31.8237
Variable

7.676

23
∞
4.2000
1.51633
64.14
12.000

*filter

24
∞
1.9766

12.000

Image plane(Light
∞

receiving surface)

Aspherical surface data

6th surface

K = 1.0000

A2 = 0.0000E+00, A4 = 2.7466E−06, A6 = 3.4652E−09, A8 = −1.1234E−10,

A10 = 0.0000E+00

11th surface

K = 0.

A2 = 0.0000E+00, A4 = −2.0116E−05, A6 = −1.6004E−07, A8 = 0.0000E+00,

A10 = 0.0000E+00

12th surface

K = 0.

A2 = 0.0000E+00, A4 = −1.3060E−05, A6 = −1.8591E−07, A8 = 4.2386E−10,

A10 = 0.0000E+00

15th surface

K = 0.

A2 = 0.0000E+00, A4 = 7.3875E−05, A6 = 2.5574E−07, A8 = −1.2551E−09,

A10 = 0.0000E+00

Various data

Wide angle
Intermediate
Telephoto

Focal length
14.28058
24.22973
40.65127

Fno.
3.4824
3.8174
5.7579

Angle of field 2ω
81.7°
48.4°
29.4°

Image height
10.8
10.8
10.8

Lens total length
99.2172
99.2111
99.2092

d3
0.99972
12.80797
16.15066

d9
25.10689
6.78556
3.41673

d10
10.33688
11.54172
1.50036

d19
1.19364
1.18790
1.18619

d22
13.50750
18.80782
28.88126

Lens
Initial surface
Focal length

1
1
114.05985

2
4
−22.84630

3
11
21.20477

4
20
−48.55991

Table of index
List of index per wavelength of medium

of glass material
used in the present embodiment

GLA
587.56
656.27
486.13
435.84
404.66

L12
1.635473
1.627801
1.655618
1.673790
1.690480

L4
1.693500
1.689550
1.702580
1.709705
1.715640

L6
1.820800
1.815070
1.834290
1.845133
1.854335

L13
1.516330
1.513855
1.521905
1.526213
1.529768

L8
1.496999
1.495136
1.501231
1.504506
1.507205

L10
1.785896
1.780584
1.798364
1.808375
1.816868

L11
1.834807
1.828975
1.848520
1.859547
1.868911

L2
1.804000
1.798815
1.816080
1.825698
1.833800

L9
1.800000
1.792237
1.819043
1.835170
1.849510

L1
1.922860
1.909158
1.957996
1.989713
2.019763

L3, L5, L7
1.846660
1.836488
1.872096
1.894186
1.914294

Example 2

Unit mm

Surface data

effective

Surface no.
r
d
nd
νd
radius

Object plane
∞
∞

1
89.3405
1.5000
1.94595
17.98
20.000

2
70.7392
4.5000
1.69680
55.53
17.371

3
−941.2812
Variable

16.110

4
2092.0128
1.2000
1.83481
42.71
14.000

5
15.9497
6.3742

11.139

6*
−304.5423
1.1000
1.69350
53.20
10.840

7
37.4086
0.8222

10.639

8
26.1684
3.5000
1.84666
23.78
10.779

9
151.1493
Variable

10.536

10(stop)
∞
Variable

4.531

11*
21.4719
3.0000
1.76802
49.24
6.700

12
−86.6030
1.0000
1.84666
23.78
6.796

13
126.7776
5.8273

6.881

14*
17.9813
5.0000
1.49700
81.54
8.023

15*
−19.2416
0.2000

7.974

16
−156.6800
1.0000
1.80000
29.84
7.650

17
16.7907
2.3000

7.368

18
31.1241
2.0000
1.80610
40.92
7.731

19
910.8764
Variable

7.737

20
63.7665
1.0000
1.80610
40.92
7.771

21
16.1697
1.0000
1.67412
20.10
7.661

22*
25.6730
Variable

7.659

23
∞
4.2000
1.51633
64.14
12.000

*filter

24
∞
1.9845

12.000

Image plane(Light
∞

receiving surface)

Aspherical surface data

6th surface

K = 0.

A2 = 0.0000E+00, A4 = −2.5976E−07, A6 = −1.7971E−08, A8 = 8.0384E−11,

A10 = 0.0000E+00

11th surface

K = 0.

A2 = 0.0000E+00, A4 = −5.9689E−06, A6 = −4.7338E−08, A8 = −1.5467E−10,

A10 = 1.1302E−12

14th surface

K = 0.

A2 = 0.0000E+00, A4 = −4.8253E−05, A6 = −5.6030E−08, A8 = −4.4899E−10,

A10 = 0.0000E+00

15th surface

K = 0.

A2 = 0.0000E+00, A4 = 8.5204E−05, A6 = −3.5979E−07, A8 = 8.8359E−10,

A10 = 0.0000E+00

22nd surface

K = 0.

A2 = 0.0000E+00, A4 = −2.1364E−06, A6 = 1.0987E−07, A8 = 4.0071E−10,

A10 = 0.0000E+00

Various data

Wide angle
Intermediate
Telephoto

Focal length
14.27926
24.22818
40.64942

Fno.
3.5210
3.6928
5.7579

Angle of field 2ω
84.1
47.8
29.1

Image height
10.8
10.8
10.8

Lens total length
99.0949
99.1710
99.0925

d3
1.05836
12.42282
16.86721

d9
26.03096
4.86906
3.51074

d10
9.89578
13.84712
1.52108

d19
1.41294
1.11656
2.23423

d22
13.18859
19.38467
27.44140

Lens
Initial surface
Focal length

1
1
127.95824

2
4
−23.62532

3
11
21.02515

4
20
−46.58408

Table of index
List of index per wavelength of medium

of glass material
used in the present embodiment

GLA
587.56
656.27
486.13
435.84
404.66

L12
1.674117
1.665099
1.698643
1.721956
1.745200

L1
1.945950
1.931230
1.983830
2.018254
2.051063

L4
1.693500
1.689550
1.702580
1.709705
1.715640

L6
1.768020
1.763310
1.778910
1.787509
1.794710

L13
1.516330
1.513855
1.521905
1.526213
1.529768

L8
1.496999
1.495136
1.501231
1.504506
1.507205

L10, L11
1.806098
1.800248
1.819945
1.831173
1.840781

L3
1.834807
1.828975
1.848520
1.859547
1.868911

L2
1.696797
1.692974
1.705522
1.712339
1.718005

L9
1.800000
1.792237
1.819043
1.835170
1.849510

L5, L7
1.846660
1.836488
1.872096
1.894186
1.914294

Example 3

Unit mm

Surface data

effective

Surface no.
r
d
nd
νd
radius

Object plane
∞
∞

1
83.1725
1.5000
1.94595
17.98
20.000

2
64.2611
4.5000
1.69680
55.53
16.207

3
−3.540E+04
Variable

14.885

4
−1705.6554
1.2000
1.79952
42.22
14.000

5
14.8599
5.3066

11.070

6*
46.5893
1.1000
1.69350
53.20
10.992

7
21.5202
2.2170

10.591

8
24.7470
3.5000
1.84666
23.78
10.732

9
92.1471
Variable

10.442

10(stop)
∞
Variable

4.623

11*
17.8917
2.4000
1.76802
49.24
7.100

12
29.4476
4.1144

7.078

13*
10.4931
6.0000
1.49700
81.54
8.188

14*
−16.5180
0.0826

7.966

15
−52.0740
1.0000
1.80000
29.84
7.564

16
13.8317
3.5271

7.077

17
83.9594
2.2000
1.77250
49.60
7.541

18
−45.3905
Variable

7.653

19
42.5129
1.0000
1.77250
49.60
7.756(LB)

20
14.4299
1.0000
1.63387
23.38
7.603(LA)

21*
21.7322
Variable

7.599

22
∞
4.2000
1.51633
64.14
12.000

*filter

23
∞
1.9140

12.000

Image plane(Light
∞

receiving surface)

Aspherical surface data

6th surface

K = 0.

A2 = 0.0000E+00, A4 = 1.9265E−05, A6 = −6.2937E−09, A8 = 4.6374E−10,

A10 = 0.0000E+00

11th surface

K = 0.

A2 = 0.0000E+00, A4 = 3.2099E−05, A6 = −1.3503E−07, A8 = −3.0828E−09,

A10 = 3.2740E−11

13th surface

K = 0.

A2 = 0.0000E+00, A4 = −1.4389E−04, A6 = −3.7673E−07, A8 = −1.0129E−09,

A10 = 0.0000E+00

14th surface

K = 0.

A2 = 0.0000E+00, A4 = 1.7473E−04, A6 = −1.1789E−06, A8 = 1.0866E−08,

A10 = 0.0000E+00

21st surface

K = 0.

A2 = 0.0000E+00, A4 = 1.1147E−07, A6 = 1.2507E−07, A8 = −6.9935E−10,

A10 = 0.0000E+00

Various data

Wide angle
Intermediate
Telephoto

Focal length
14.28613
24.22181
40.64610

Fno.
3.4631
3.7093
5.7579

Angle of field 2ω
80.2
47.1
28.9

Image height
10.8
10.8
10.8

Lens total length
98.8873
99.3953
99.0035

d3
0.68512
12.40038
17.47148

d9
25.88780
4.96713
3.51471

d10
10.85526
14.37143
1.41718

d18
1.77452
0.88219
2.12217

d21
12.92301
20.02770
27.66855

Lens
Initial surface
Focal length

1
1
132.46329

2
4
−24.55536

3
11
21.63266

4
19
−49.87196

Table of index
List of index per wavelength of medium

of glass material
used in the present embodiment

GLA
587.56
656.27
486.13
435.84
404.66

L1
1.945950
1.931230
1.983830
2.018254
2.051063

L4
1.693500
1.689550
1.702580
1.709705
1.715640

L6
1.768020
1.763310
1.778910
1.787509
1.794710

L11
1.633870
1.626381
1.653490
1.671610
1.688826

L12
1.516330
1.513855
1.521905
1.526213
1.529768

L7
1.496999
1.495136
1.501231
1.504506
1.507205

L3
1.799516
1.793879
1.812814
1.823553
1.832706

L9, L10
1.772499
1.767798
1.783374
1.791971
1.799174

L2
1.696797
1.692974
1.705522
1.712339
1.718005

L8
1.800000
1.792237
1.819043
1.835170
1.849510

L5
1.846660
1.836488
1.872096
1.894186
1.914294

Example 4

Unit mm

Surface data

effective

Surface no.
r
d
nd
νd
radius

Object plane
∞
∞

1
87.9659
1.5000
1.94595
17.98
20.000

2
66.4601
4.5000
1.69680
55.53
16.200

3
−428.6745
Variable

14.981

4
−364.1506
1.2000
1.78590
44.20
14.000

5
14.9636
5.0888

11.012

6*
78.2509
1.1000
1.69350
53.20
10.938

7
25.3889
1.9268

10.607

8
24.5062
3.5000
1.84666
23.78
10.787

9
98.7596
Variable

10.514

10(stop)
∞
Variable

4.420

11*
19.8482
3.2676
1.49700
81.54
6.700

12
259.8129
3.9935

6.942

13*
18.9961
5.1811
1.76802
49.24
7.977

14*
−78.3736
0.4461

7.559

15
99.0960
1.0701
1.92286
20.88
7.423

16
16.4313
3.9836

7.127

17
−1887.2477
2.2000
1.71999
50.23
7.644

18
−29.1973
Variable

7.792

19
33.6509
1.0000
1.77250
49.60
7.881

20
13.4328
1.0000
1.63296
24.01
7.656

21*
18.8235
Variable

7.646

22
∞
4.2000
1.51633
64.14
12.000

*filter

23
∞
1.9417

12.000

Image plane(Light
∞

receiving surface)

Aspherical surface data

6th surface

K = 0.

A2 = 0.0000E+00, A4 = 1.2138E−05, A6 = −2.0543E−08, A8 = 4.2477E−10,

A10 = 0.0000E+00

11th surface

K = 0.

A2 = 0.0000E+00, A4 = −5.6167E−06, A6 = 2.7152E−07, A8 = −6.8425E−09,

A10 = 4.1818E−11

13th surface

K = 0.

A2 = 0.0000E+00, A4 = −9.4955E−09, A6 = −1.9916E−07, A8 = 5.9709E−09,

A10 = 0.0000E+00

14th surface

K = 0.

A2 = 0.0000E+00, A4 = 7.6263E−05, A6 = −4.0382E−07, A8 = 9.1001E−09,

A10 = 0.0000E+00

21st surface

K = 0.

A2 = 0.0000E+00, A4 = 1.5568E−06, A6 = −2.3766E−08, A8 = 4.9965E−10,

A10 = 0.0000E+00

Various data

Wide angle
Intermediate
Telephoto

Focal length
14.27990
24.23676
40.64780

Fno.
3.6168
3.7115
5.7579

Angle of field 2ω
81.3
46.6
28.7

Image height
10.8
10.8
10.8

Lens total length
98.8106
99.5647
99.0221

d3
0.62682
12.15692
17.77090

d9
26.61258
4.23361
3.50320

d10
9.53901
15.13554
1.38514

d18
1.87659
0.78920
1.96342

d21
13.05636
20.08762
27.28711

Lens
Initial surface
Focal length

1
1
116.04389

2
4
−24.00002

3
11
21.61328

4
19
−49.44081

Table of index
List of index per wavelength of medium

of glass material
used in the present embodiment

GLA
587.56
656.27
486.13
435.84
404.66

L11
1.632960
1.625570
1.651930
1.668330
1.683330

L8
1.922860
1.910380
1.954570
1.982810
2.009196

L1
1.945950
1.931230
1.983830
2.018254
2.051063

L4
1.693500
1.689550
1.702580
1.709705
1.715640

L7
1.768020
1.763310
1.778910
1.787509
1.794710

L12
1.516330
1.513855
1.521905
1.526213
1.529768

L6
1.496999
1.495136
1.501231
1.504506
1.507205

L3
1.785896
1.780584
1.798364
1.808375
1.816868

L10
1.772499
1.767798
1.783374
1.791971
1.799174

L9
1.719995
1.715670
1.730004
1.737917
1.744546

L2
1.696797
1.692974
1.705522
1.712339
1.718005

L5
1.846660
1.836488
1.872096
1.894186
1.914294

Values of conditional expressions of each embodiment are shown below:

Example 1
Example 2
Example 3
Example 4

fw (Wide angle)
14.281
14.279
14.286
14.280

fs (Intermediate)
24.230
24.228
24.222
24.237

ft (Telephoto)
40.651
40.649
40.646
40.648

Half angle of field
40.9
42.1
40.1
41.7

ωw (Wide angle end)

Half angle of field
24.2
23.9
23.6
23.3

ωs (Intermediate)

Half angle of field
14.7
14.6
14.5
14.4

ωt (Telephoto end)

y10
10.8
10.8
10.8
10.8

(R4F + R4R)/
1.972
2.348
3.092
3.539

(R4F − R4R)

(R4LAF + R4LAR)/
−5.082
−4.403
−4.952
−5.984

(R4LAF − R4LAR)

(R3ALF + R3ALR)/
−3.160
−3.343
−1.394
−0.983

(R3ALF − R3ALR)

nd
1.63547
1.67412
1.63387
1.63296

b
2.2453
2.2108
2.2581
2.2740

θgF [= θgF (LA)]
0.6533
0.6950
0.6684
0.6222

β
0.7826
0.8088
0.8007
0.7581

νd [= νd (LA)]
22.84
20.10
23.38
24.01

θhg [= θhg (LA)]
0.6218
0.6927
0.6476
0.5690

βhg
0.8123
0.8603
0.8425
0.7692

θgF [= θgF (LB)]
0.5645
0.5703
0.5523
0.5523

νd [= νd (LB)]
42.71
40.92
49.60
49.60

θhg [= θhg (LB)]
0.4790
0.4881
0.4624
0.4624

θgF (LA) − θgF (LB)
0.0888
0.1247
0.1161
0.0699

θhg (LA) − θhg (LB)
0.1428
0.2046
0.1852
0.1066

νd (LA) − νd (LB)
−19.87
−20.82
26.22
−25.59

y07
7.56
7.56
7.56
7.56

tanω07w
0.56726
0.57875
0.56124
0.56728

y07/(fw * tanω07w)
0.933
0.915
0.943
0.933

Thus, it is possible to use such image forming optical system of the present invention in a photographic apparatus in which an image of an object is photographed by an electronic image pickup element such as a CCD and a CMOS, particularly a digital camera and a video camera, a personal computer, a telephone, and a portable terminal which are examples of an information processing unit, particularly a portable telephone which is easy to carry. Embodiments thereof will be exemplified below.

In FIG. 13 to FIG. 15 show conceptual diagrams of structures in which the image forming optical system according to the present invention is incorporated in a photographic optical system 41 of a digital camera. FIG. 13 is a frontward perspective view showing an appearance of a digital camera 40, FIG. 14 is a rearward perspective view of the same, and FIG. 15 is a cross-sectional view showing an optical arrangement of the digital camera 40.

The digital camera 40, in a case of this example, includes the photographic optical system 41 (an objective optical system for photography 48) having an optical path for photography 42, a finder optical system 43 having an optical path for finder 44, a shutter 45, a flash 46, and a liquid-crystal display monitor 47. Moreover, when the shutter 45 disposed at an upper portion of the camera 40 is pressed, in conjugation with this, a photograph is taken through the photographic optical system 41 (objective optical system for photography 48) such as the zoom lens in the first embodiment.

An object image formed by the photographic optical system 41 (photographic objective optical system 48) is formed on an image pickup surface 50 of a CCD 49. The object image photoreceived at the CCD 49 is displayed on the liquid-crystal display monitor 47 which is provided on a camera rear surface as an electronic image, via an image processing means 51. Moreover, a memory etc. is disposed in the image processing means 51, and it is possible to record the electronic image photographed. This memory may be provided separately from the image processing means 51, or may be formed by carrying out by writing by recording (recorded writing) electronically by a floppy (registered trademark) disc, memory card, or an MO etc.

Furthermore, an objective optical system for finder 53 is disposed in the optical path for finder 44. This objective optical system for finder 53 includes a cover lens 54, a first prism 10, an aperture stop 2, a second prism 20, and a lens for focusing 66. An object image is formed on an image forming surface 67 by this objective optical system for finder 53. This object image is formed in a field frame of a Porro prism which is an image erecting member equipped with a first reflecting surface 56 and a second reflecting surface 58. On a rear side of this Porro prism, an eyepiece optical system 59 which guides an image formed as an erected normal image is disposed.

By the digital camera 40 structured in such manner, it is possible to realize an optical image pickup apparatus having a zoom lens with a reduced size and thickness, in which the number of structural components is reduced. Further, the present invention could be applied to the above-mentioned collapsible type digital camera as well as a bending type (an optical path reflecting type) digital camera having a bending optical system (optical path reflecting lens).

Next, a personal computer which is an example of an information processing apparatus with a built-in image forming system as an objective optical system is shown in FIG. 16 to FIG. 18. FIG. 16 is a frontward perspective view of a personal computer 300 with its cover opened, FIG. 17 is a cross-sectional view of a photographic optical system 303 of the personal computer 300, and FIG. 18 is a side view of FIG. 16. As it is shown in FIG. 16 to FIG. 18, the personal computer 300 has a keyboard 301, an information processing means and a recording means, a monitor 302, and a photographic optical system 303.

Here, the keyboard 301 is for an operator to input information from an outside. The information processing means and the recording means are omitted in the diagram. The monitor 302 is for displaying the information to the operator. The photographic optical system 303 is for photographing an image of the operator or a surrounding. The monitor 302 may be a display such as a liquid-crystal display or a CRT display. As the liquid-crystal display, a transmission liquid-crystal display device which illuminates from a rear surface by a backlight not shown in the diagram, and a reflection liquid-crystal display device which displays by reflecting light from a front surface are available. Moreover, in the diagram, the photographic optical system 303 is built-in at a right side of the monitor 302, but without restricting to this location, the photographic optical system 303 may be anywhere around the monitor 302 and the keyboard 301.

This photographic optical system 303 has an objective optical system 100 which includes the zoom lens in the first embodiment for example, and an electronic image pickup element chip 162 which receives an image. These are built into the personal computer 300.

At a front end of a mirror frame, a cover glass 102 for protecting the objective optical system 100 is disposed.

An object image received at the electronic image pickup element chip 162 is input to a processing means of the personal computer 300 via a terminal 166. Further, the object image is displayed as an electronic image on the monitor 302. In FIG. 16, an image 305 photographed by the user is displayed as an example of the electronic image. Moreover, it is also possible to display the image 305 on a personal computer of a communication counterpart from a remote location via a processing means. For transmitting the image to the remote location, the Internet and telephone are used.

Next, a telephone which is an example of an information processing apparatus in which the image forming optical system of the present invention is built-in as a photographic optical system, particularly a portable telephone which is easy to carry is shown in FIG. 19A, FIG. 19B, and FIG. 19C. FIG. 19A is a front view of a portable telephone 400, FIG. 19B is a side view of the portable telephone 400, and FIG. 19C is a cross-sectional view of a photographic optical system 405. As shown in FIG. 19A to FIG. 19C, the portable telephone 400 includes a microphone section 401, a speaker section 402, an input dial 403, a monitor 404, the photographic optical system 405, an antenna 406, and a processing means.

Here, the microphone section 401 is for inputting a voice of the operator as information. The speaker section 402 is for outputting a voice of the communication counterpart. The input dial 403 is for the operator to input information. The monitor 404 is for displaying a photographic image of the operator himself and the communication counterpart, and information such as a telephone number. The antenna 406 is for carrying out a transmission and a reception of communication electric waves. The processing means (not shown in the diagram) is for carrying out processing of image information, communication information, and input signal etc.

Here, the monitor 404 is a liquid-crystal display device. Moreover, in the diagram, a position of disposing each structural element is not restricted in particular to a position in the diagram. This photographic optical system 405 has an objective optical system 100 which is disposed in a photographic optical path 407 and an image pickup element chip 162 which receives an object image. As the objective optical system 100, the zoom lens in the first embodiment for example, is used. These are built into the portable telephone 400.

At a front end of a mirror frame, a cover glass 102 for protecting the objective optical system 100 is disposed.

An object image received at the electronic image pickup element chip 162 is input to an image processing means which is not shown in the diagram, via a terminal 166. Further, the object image finally displayed as an electronic image on the monitor 404 or a monitor of the communication counterpart, or both. Moreover, a signal processing function is included in the processing means. In a case of transmitting an image to the communication counterpart, according to this function, information of the object image received at the electronic image pickup element chip 162 is converted to a signal which can be transmitted.

Various modifications can be made to the present invention without departing from its essence.

As it has been described above, the present invention is useful for an image forming optical system in which, the focusing lens group is made light-weight with an improved performance of a video function of an interchangeable lens still camera, and at the same time, the chromatic aberration, the coma aberration, and the meridional curvature of field are corrected favorably. Moreover, the present invention is useful for an electronic image pickup apparatus in which, it is possible to have a high-speed focusing, a reduction of consumption of electric power, and sharpening of image by using the abovementioned image forming optical system.

According to the present invention, it is possible to make the focusing lens group light-weight with an improved performance of the video function of the interchangeable lens still camera. Furthermore, it is possible to achieve an image forming optical system in which, the chromatic aberration, the coma aberration, and the meridional curvature of field are corrected favorably. Moreover, in the electronic image pickup apparatus, by using the abovementioned image forming optical system, it is possible to realize high-speed focusing, reduction of consumption of electric power, and sharpening of image.

Number	Name	Date	Kind
6342972	Yamanashi	Jan 2002	B1
7423813	Kamo	Sep 2008	B2

Number	Date	Country
2007-108707	Apr 2007	JP
2007-108715	Apr 2007	JP
2008-191308	Aug 2008	JP
2008-191311	Aug 2008	JP

Image forming optical system and electronic image pickup apparatus using the same

Information

Patent Number

Date Filed

Date Issued

Inventors

Original Assignees

Examiners

Agents

CPC

US Classifications

Field of Search

US

International Classifications

Term Extension

Abstract

Description

Claims

Priority Claims (1)

US Referenced Citations (2)

Foreign Referenced Citations (4)

Related Publications (1)