Zoom lens system

This application is based on application Nos. H10-44812, H10-44816, H10-45097, and H10-45133 filed in Japan, the content of which is hereby incorporated by reference.
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a zoom lens system, and more particularly to a compact and high-zoom-ratio zoom lens system suitable for use in digital still cameras.
2. Description of the Prior Art
In recent years, as personal computers become prevalent, digital still cameras have been coming into wider and wider use that allow easy shooting of images. This trend has created an increasing demand for more compact and more low-cost digital still cameras that offer higher zoom ratios and higher optical performance. This in turn has created an increasing demand for more compact and more low-cost taking optical systems that offer higher zoom ratios and higher optical performance. Moreover, higher and higher image quality has been sought after in digital still cameras. In digital still cameras, image quality depends on the number of pixels that the solid-state imaging device provided therein has. For example, a now typical solid-state imaging device of the so-called VGA class has about 330,000 pixels.
As a taking optical system of the VGA class, it is possible to employ an optical system designed for use in a home-use video camera, because it offers a high zoom ratio at low cost. However, with a VGA class taking optical system, it is impossible to obtain satisfactorily high image quality, because the image quality it offers is far inferior to that obtained with a silver-halide film camera. To obtain satisfactorily high image quality, it is necessary to use at least 1,000,000 pixels, and the greater the number of pixels, the higher optical performance is required in the taking optical system. The problem here is that most taking optical systems that offer image quality as high as would be required to cope with 1,000,000 or more pixels are built as fixed-focal-length lens systems. In other words, to obtain a zoom lens system (in particular, a high-zoom-ratio zoom lens system) satisfying such requirements, there is no alternative but to use an interchangeable lens designed for use with a single-lens reflex camera, or a zoom lens designed for use with a professional-use video camera. However, such zoom lenses are extremely large and expensive. Moreover, in a taking optical system, high optical performance is required not only for an object at infinity but also for an object at a close distance, and therefore the focusing method employed therein greatly affects the overall optical performance.
SUMMARY OF THE INVENTION
An object of the present invention is to provide a compact, low-cost, and high-zoom-ratio zoom lens system that offers high image quality.
To achieve the above object, according to one aspect of the present invention, a zoom lens system is provided with, from the object side, a first lens unit having a positive optical power, a second lens unit having a negative optical power, a third lens unit having a positive optical power, and a fourth lens unit having a positive optical power. The first, second, and fourth lens units are moved during zooming. The third lens unit is kept in a fixed position during zooming. Additionally, this zoom lens system fulfills the conditions below:
-5.0<M1/Ymax<-1.0
-1.0<M4/M2<-0.1
where
M1 represents the displacement amount of the first lens unit from the shortest focal length condition (the wide-angle end) to the longest focal length condition (the telephoto end) (the direction pointing to the object side is negative);
M2 represents the displacement amount of the second lens unit from the shortest focal length condition to the longest focal length condition (the direction pointing to the object side is negative);
M4 represents the displacement amount of the fourth lens unit from the shortest focal length condition to the longest focal length condition (the direction pointing to the object side is negative); and
Ymax represents the maximum image height (the radius of the effective image on the image plane).
According to another aspect of the present invention, a zoom lens system is provided with, from the object side, a first lens unit having a positive optical power, a second lens unit having a negative optical power, a third lens unit having a positive optical power, and a fourth lens unit having a positive optical power. The first, second, and fourth lens units are moved during zooming. The third lens unit is kept in a fixed position during zooming. Additionally, this zoom lens system fulfills the conditions below:
-5.0<M1/Ymax<-1.0
0.2<log(.beta.2T/.beta.2W)/log(Z)<0.9
where
M1 represents the displacement amount of the first lens unit from the shortest focal length condition to the longest focal length condition (the direction pointing to the object side is negative);
Ymax represents the maximum image height (the radius of the effective image on the image plane);
.beta.2W represents the lateral magnification of the second lens unit in the shortest focal length condition;
.beta.2T represents the lateral magnification of the second lens unit in the longest focal length condition; and
Z represents the zoom ratio (which equals fT/fW, where fT represents the focal length of the entire zoom lens system in the longest focal length condition; and fW represents the focal length of the entire zoom lens system in the shortest focal length condition).
According to another aspect of the present invention, a zoom lens system is provided with, from the object side, a first lens unit having a positive optical power, a second lens unit having a negative optical power, a third lens unit having a positive optical power, and a fourth lens unit having a positive optical power. The first lens unit is moved monotonically forward to the object side during zooming from the shortest focal length condition to the longest focal length condition. The second lens unit is moved monotonically backward to the image side during zooming from the shortest focal length condition to the longest focal length condition. The third lens unit is kept in a fixed position during zooming. The fourth lens unit is moved monotonically forward to the object side during zooming from the shortest focal length condition to the longest focal length condition. Additionally, the second lens unit has an aspherical surface that fulfills the condition below:
0<(x-x0)/(N'-N)<0.9
where
x represents the deviation of the aspherical surface in a direction perpendicular to the optical axis direction of the aspherical surface (in millimeters, the direction pointing to the object side is negative);
x0 represents the deviation of the reference spherical surface in a direction perpendicular to the optical axis direction of the reference spherical surface (in millimeters, 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.
According to another aspect of the present invention, a zoom lens system is provided with, from the object side, a first lens unit having a positive optical power, a second lens unit having a negative optical power, a third lens unit having a positive optical power, and a fourth lens unit having a positive optical power. The first and fourth lens units are moved monotonically forward to the object side during zooming from the shortest focal length condition to the longest focal length condition. The second lens unit is moved monotonically backward to the image side during zooming from the shortest focal length condition to the longest focal length condition. The third lens unit is kept in a fixed position during zooming. Additionally, the fourth lens unit has an aspherical surface that fulfills the condition below:
-0.85<(x-x0)/(N'-N)<0
where
x represents the deviation of the aspherical surface in a direction perpendicular to the optical axis direction of the aspherical surface (in millimeters, the direction pointing to the object side is negative);
x0 represents the deviation of the reference spherical surface in a direction perpendicular to the optical axis direction of the reference spherical surface (in millimeters, 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.
According to another aspect of the present invention, a zoom lens system is provided with, from the object side, a first lens unit having a positive optical power, a second lens unit having a negative optical power, a third lens unit having a positive optical power, and a fourth lens unit having a positive optical power. The first and fourth lens units are moved during zooming. The second lens unit is moved during zooming and is moved for focusing. The third lens unit is kept in a fixed position during zooming. Additionally, this zoom lens system fulfills the conditions below:
0.1<.vertline..beta.2T.vertline.<1.0
0.2<.uparw.fW/f2.vertline.<1.5
-5.0<M1/Ymax<-1.0
where
.alpha.2T represents the lateral magnification of the second lens unit in the longest focal length condition;
fW represents the focal length of the entire zoom lens system in the shortest focal length condition;
f2 represents the focal length of the second lens unit;
M1 represents the displacement amount of the first lens unit from the shortest focal length condition to the longest focal length condition (the direction pointing to the object side is negative); and
Ymax represents the maximum image height (the radius of the effective image on the image plane).
According to another aspect of the present invention, a zoom lens system is provided with, from the object side, a first lens unit having a positive optical power, a second lens unit having a negative optical power, a third lens unit having a positive optical power, and a fourth lens unit having a positive optical power. The first and fourth lens units are moved during zooming. The second lens unit is moved during zooming and is moved for focusing. The third lens unit is kept in a fixed position during zooming. Additionally, this zoom lens system fulfills the condition below:
0.1<M4/M1<1.0
where
M1 represents the displacement amount of the first lens unit from the shortest focal length condition to the longest focal length condition (the direction pointing to the object side is negative); and
M4 represents the displacement amount of the fourth lens unit from the shortest focal length condition to the longest focal length condition (the direction pointing to the object side is negative).
According to another aspect of the present invention, a zoom lens system is provided with, from the object side, a first lens unit having a positive optical power, a second lens unit having a negative optical power, a third lens unit having a positive optical power, and a fourth lens unit having a positive optical power. The first and third lens units are kept in fixed positions during zooming. The second lens unit is moved during zooming. The fourth lens unit is moved forward to the object side during zooming. Additionally, this zoom lens system fulfills the conditions below:
2.5<f1/fW<8.0
0.7.times.(.beta.34T/.beta.34W)<.beta.2T/.beta.2W<2.3.times.(.beta.34T/.beta.34W)
where
f1 represents the focal length of the first lens unit;
fW represents the focal length of the entire zoom lens system in the shortest focal length condition;
.beta.34W represents the composite lateral magnification of the third and fourth lens units in the shortest focal length condition;
.beta.34T represents the composite lateral magnification of the third and fourth lens units in the longest focal length condition;
.beta.2W represents the lateral magnification of the second lens unit in the shortest focal length condition; and
.beta.2T represents the lateral magnification of the second lens unit in the longest focal length condition.
According to another aspect of the present invention, a zoom lens system is provided with, from the object side, a first lens unit having a positive optical power, a second lens unit having a negative optical power, a third lens unit having a positive optical power, and a fourth lens unit having a positive optical power. The first and third lens units are kept in fixed positions during zooming. The second lens unit is moved monotonically backward to the image side during zooming from the shortest focal length condition to the longest focal length condition. The fourth lens unit is moved monotonically forward to the object side during zooming from the shortest focal length condition to the longest focal length condition. Additionally, this zoom lens system fulfills the condition below:
2.5<f1/fW<8.0
where
f1 represents the focal length of the first lens unit; and
fW represents the focal length of the entire zoom lens system in the shortest focal length condition.
According to another aspect of the present invention, a zoom lens system is provided with, from the object side, a first lens unit having a positive optical power, a second lens unit having a negative optical power, a third lens unit having a positive optical power, and a fourth lens unit having a positive optical power. The first and third lens units are kept in fixed positions during zooming. The second lens unit is moved during zooming. The fourth lens unit is moved forward to the object side during zooming. Additionally, this zoom lens system fulfills the condition below:
0.4<log(.beta.2T/.beta.2W)/log(Z)<0.75
where
.beta.2W represents the lateral magnification of the second lens unit in the shortest focal length condition;
.beta.2T represents the lateral magnification of the second lens unit in the longest focal length condition; and
Z represents the zoom ratio (which equals fT/fW, where fT represents the focal length of the entire zoom lens system in the longest focal length condition; and fW represents the focal length of the entire zoom lens system in the shortest focal length condition).
According to another aspect of the present invention, a zoom lens system is provided with, from the object side, a first lens unit having a positive optical power, a second lens unit having a negative optical power, a third lens unit having a positive optical power, and a fourth lens unit having a positive optical power. The first and third lens units are kept in fixed positions during zooming. The second lens unit is moved from the object side to the image side during zooming from the shortest focal length condition to the longest focal length condition, and is also moved for focusing. The fourth lens unit is moved forward to the object side during zooming so that the fourth lens unit compensates the movement of the image plane in the optical axis direction caused by moving the second lens unit. Additionally, this zoom lens system fulfills the conditions below:
0.5<.vertline..beta.2T.vertline.<0.98
3.0<f1/fW<9.0
where
.beta.2T represents the lateral magnification of the second lens unit in the longest focal length condition;
fW represents the focal length of the entire zoom lens system in the shortest focal length condition; and
f1 represents the focal length of the first lens unit.
According to still another aspect of the present invention, a zoom lens system is provided with, from the object side, a first lens unit having a positive optical power, a second lens unit having a negative optical power, a third lens unit having a positive optical power, and a fourth lens unit having a positive optical power. The first and third lens units are kept in fixed positions during zooming. The second lens unit is moved monotonically from the object side to the image side during zooming from the shortest focal length condition to the longest focal length condition, and is also moved for focusing. The fourth lens unit is moved monotonically from the image side to the object side during zooming from the shortest focal length condition to the longest focal length condition. Additionally, this zoom lens system fulfills the conditions below:
0.15<M4/M2<0.55
0.4<log(.beta.2T/.beta.2W)log(Z)<0.75
where
M2 represents the displacement amount of the second lens unit from the shortest focal length condition to the longest focal length condition (the direction pointing to the object side is negative);
M4 represents the displacement amount of the fourth lens unit from the shortest focal length condition to the longest focal length condition (the direction pointing to the object side is negative);
.beta.2W represents the lateral magnification of the second lens unit in the shortest focal length condition;
.beta.2T represents the lateral magnification of the second lens unit in the longest focal length condition; and
Z represents the zoom ratio (which equals fT/fW, where fT represents the focal length of the entire zoom lens system in the longest focal length condition; and fW represents the focal length of the entire zoom lens system in the shortest focal length condition).

BRIEF DESCRIPTION OF THE DRAWINGS
This and other 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 zoom lens system of a first embodiment (Example 1) of the present invention;
FIG. 2 is a lens arrangement diagram of the zoom lens system of a second embodiment (Example 2) of the present invention;
FIG. 3 is a lens arrangement diagram of the zoom lens system of a third embodiment (Example 3) of the present invention;
FIGS. 4A to 4I are graphic representations of the aberrations observed in the zoom lens system of Example 1;
FIGS. 5A to 5I are graphic representations of the aberrations observed in the zoom lens system of Example 2;
FIGS. 6A to 6I are graphic representations of the aberrations observed in the zoom lens system of Example 3;
FIG. 7 is a lens arrangement diagram of the zoom lens system of a fourth embodiment (Example 4) of the present invention;
FIG. 8 is a lens arrangement diagram of the zoom lens system of a fifth embodiment (Example 5) of the present invention;
FIG. 9 is a lens arrangement diagram of the zoom lens system of a sixth embodiment (Example 6) of the present invention;
FIG. 10 is a lens arrangement diagram of the zoom lens system of a seventh embodiment (Example 7) of the present invention;
FIGS. 11A to 11I are graphic representations of the aberrations observed in the infinite-distance shooting condition in Example 4;
FIGS. 12A to 12I are graphic representations of the aberrations observed in the close-distance shooting condition (D=1m) in Example 4;
FIGS. 13A to 13I are graphic representations of the aberrations observed in the infinite-distance shooting condition in Example 5;
FIGS. 14A to 14I are graphic representations of the aberrations observed in the close-distance shooting condition (D=1m) in Example 5;
FIGS. 15A to 15I are graphic representations of the aberrations observed in the infinite-distance shooting condition in Example 6;
FIGS. 16A to 16I are graphic representations of the aberrations observed in the close-distance shooting condition (D=1m) in Example 6;
FIGS. 17A to 17I are graphic representations of the aberrations observed in the infinite-distance shooting condition in Example 7;
FIGS. 18A to 18I are graphic representations of the aberrations observed in the close-distance shooting condition (D=1m) in Example 7;
FIG. 19 is a lens arrangement diagram of the zoom lens system of an eighth embodiment (Example 8) of the present invention;
FIG. 20 is a lens arrangement diagram of the zoom lens system of a ninth embodiment (Example 9) of the present invention;
FIG. 21 is a lens arrangement diagram of the zoom lens system of a tenth embodiment (Example 10) of the present invention;
FIGS. 22A to 22I are graphic representations of the aberrations observed in the zoom lens system of Example 8;
FIGS. 23A to 23I are graphic representations of the aberrations observed in the zoom lens system of Example 9;
FIGS. 24A to 24I are graphic representations of the aberrations observed in the zoom lens system of Example 10;
FIG. 25 is a lens arrangement diagram of the zoom lens system of an eleventh embodiment (Example 11) of the present invention;
FIG. 26 is a lens arrangement diagram of the zoom lens system of a twelfth embodiment (Example 12) of the present invention;
FIG. 27 is a lens arrangement diagram of the zoom lens system of a thirteenth embodiment (Example 13) of the present invention;
FIGS. 28A to 28I are graphic representations of the aberrations observed in the infinite-distance shooting condition in Example 11;
FIGS. 29A to 29I are graphic representations of the aberrations observed in the close-distance shooting condition (D=1m) in Example 11;
FIGS. 30A to 30I are graphic representations of the aberrations observed in the infinite-distance shooting condition in Example 12;
FIGS. 31A to 31I are graphic representations of the aberrations observed in the close-distance shooting condition (D=1m) in Example 12;
FIGS. 32A to 32I are graphic representations of the aberrations observed in the infinite-distance shooting condition in Example 13; and
FIGS. 33A to 33I are graphic representations of the aberrations observed in the close-distance shooting condition (D=1m) in Example 13.

DESCRIPTION OF THE PREFERRED EMBODIMENTS
Hereinafter, zoom lens systems embodying the present invention will be described with reference to the corresponding drawings. FIGS. 1 to 3, FIGS. 7 to 10, FIGS. 19 to 21, and FIGS. 25 to 27 show the lens arrangement of the zoom lens systems of the first to thirteenth embodiments, respectively, as observed at the wide-angle end [W]. In each lens arrangement diagram, arrow mj (j=1, 2, 3, and 4) schematically indicates the movement of the jth lens unit (Grj) during zooming from the wide-angle end [W] to the telephoto end [T] (note that arrow mj with a broken line indicates that the jth lens unit (Grj) is kept in a fixed position during zooming). Moreover, in each lens arrangement diagram, a surface marked with ri (i=1, 2, 3, . . ) is the ith surface counted from the object (subject) side, and a surface ri marked with an asterisk (*) is an aspherical surface. Furthermore, di (i=1, 2, 3, . . . ) represents the ith axial distance counted from the object side, though only those axial distances between the lens units that vary with zooming are shown.
Note that, in the zoom lens systems of the first to thirteenth embodiments, the lens units are composed solely of refracting lens elements that deflect incoming rays through refraction. However, the lens units may include, for example, diffracting lens elements that deflect incoming rays through diffraction, refracting-diffracting hybrid-type lens elements that deflect incoming rays through the combined effect of refraction and diffraction, or the like. Note also that applications of the zoom lens systems of the first to thirteenth embodiments, although they are designed originally for use in digital still cameras, are not limited to cameras. These zoom lens systems, with their characteristic optical arrangement, can also be used as a zoom lens system or as a part of a zooming optical system (such as the objective unit of an a focal optical system) for use in optical apparatuses other than cameras.
<Embodiments 1 to 3>
The zoom lens systems of the first to third embodiments are each composed of, from the object side, a first lens unit having a positive optical power (Gr1), a second lens unit having a negative optical power (Gr2), a third lens unit having a positive optical power (Gr3), and a fourth lens unit having a positive optical power (Gr4). During zooming from the wide-angle end [W] to the telephoto end [T], the first and third lens units (Gr1 and Gr3) are kept in fixed positions, the second lens unit (Gr2) is moved monotonically from the object side to the image side, and the fourth lens unit (Gr4) is moved monotonically from the image side to the object side. Note that the fourth lens unit (Gr4) has at its image-side end a low-pass filter (LPF) having the shape of a flat plate.
In the zoom lens system of the first embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gr1) is composed of a doublet lens element formed by cementing together a negative meniscus lens element convex to the object side and a biconvex lens element, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, and a doublet lens element formed by cementing together a biconcave lens element and a biconvex lens element. The third lens unit (Gr3) is composed of an aperture stop (S), and a doublet lens element formed by cementing together a biconvex lens element and a biconcave lens element. The fourth lens unit (Gr4) is composed of a positive meniscus lens element convex to the object side, a biconvex lens element, and a biconcave lens element.
In the zoom lens system of the second embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gri) is composed of a negative meniscus lens element convex to the object side, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of two biconcave lens elements, and a positive meniscus lens element convex to the object side. The third lens unit (Gr3) is composed of an aperture stop (S), and a doublet lens element formed by cementing together a positive meniscus lens element convex to the object side and a negative meniscus lens element convex to the object side. The fourth lens unit (Gr4) is composed of a biconvex lens element, and a negative meniscus lens element convex to the image side.
In the zoom lens system of the third embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gr1) is composed of a doublet lens element formed by cementing together a negative meniscus lens element convex to the object side and a biconvex lens element, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, and a doublet lens element formed by cementing together a biconcave lens element and a biconvex lens element. The third lens unit (Gr3) is composed of an aperture stop (S), and a doublet lens element formed by cementing together a biconvex lens element and a biconcave lens element. The fourth lens unit (Gr4) is composed of a positive meniscus lens element convex to the object side, a biconvex lens element, and a biconcave lens element.
In a zoom lens system, like those of the first to third embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the first and third lens units (Gr1 and Gr3) are kept in fixed positions and the second and fourth lens units (Gr2 and Gr4) are moved (in particular, those of the type in which, during zooming from the wide-angle end [W] to the telephoto end [T], the second lens unit (Gr2) is moved monotonically from the object side to the image side and the fourth lens unit (Gr4) is moved monotonically from the image side to the object side), it is preferable that Condition (1) below be fulfilled.
2.5<f1/fW<8.0 (1)
where
f1 represents the focal length of the first lens unit (Gri); and
fW represents the focal length of the entire zoom lens system at the wide-angle end [W].
Condition (1) defines the ratio of the focal length of the first lens unit (Gr1) to the focal length of the entire zoom lens system to be preferably fulfilled to strike a proper balance between the total length and the aberration characteristics. If the lower limit of Condition (1) is exceeded, the focal length of the first lens unit (Gr1) is so short that the optical power of the first lens unit (Gr1) is too strong. This helps reduce the total length of the zoom lens system, but simultaneously increases aberrations (in particular, the spherical aberration and the longitudinal chromatic aberration on the telephoto side). In contrast, if the upper limit of Condition (1) is exceeded, the focal length of the first lens unit (Gr1) is so long that the optical power of the first lens unit (Gr1) is too weak. This helps reduce aberrations, but simultaneously makes the total length of the zoom lens system unduly long. An unduly long total length demands an unduly large diameter in the front-end lens unit, and thus makes the zoom lens system as a whole unduly large.
In a zoom lens system, like those of the first to third embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the first and third lens units (Gr1 and Gr3) are kept in fixed positions and the second and fourth lens units (Gr2 and Gr4) are moved (in particular, those of the type in which, during zooming from the wide-angle end [W] to the telephoto end [T], the second lens unit (Gr2) is moved monotonically from the object side to the image side and the fourth lens unit (Gr4) is moved monotonically from the image side to the object side), it is preferable that Condition (2) below be fulfilled. Moreover, it is more preferable that Condition (1) noted above be additionally fulfilled.
0.7.times.(.beta.34T/.beta.34W)<.beta.2T/.beta.2W<2.3.times.(.beta.34T/.beta.34W) (2)
where
.beta.2W represents the lateral magnification of the second lens unit (Gr2) at the wide-angle end [W];
.beta.2T represents the lateral magnification of the second lens unit (Gr2) at the telephoto end [T];
.beta.34W represents the composite lateral magnification of the third and fourth lens units (Gr3 and Gr4) at the wide-angle end [W]; and
.beta.34T represents the composite lateral magnification of the third and fourth lens units (Gr3 and Gr4) at the telephoto end [T].
Condition (2) defines the relationship to be preferably fulfilled between the second lens unit (Gr2) and the lens units disposed on the image side thereof in terms of how far they are responsible for zooming. If the lower limit of Condition (2) is exceeded, the responsibility of the second lens unit (Gr2) for zooming is too light (that is, the responsibility of the lens units disposed on the image side of the second lens unit (Gr2) for zooming is too heavy). This increases the variation of aberrations (in particular, the variation of spherical aberration) that accompanies zooming. In contrast, if the upper limit of Condition (2) is exceeded, the responsibility of the second lens unit (Gr2) for zooming is so heavy that the second lens unit (Gr2) needs to be moved for an unduly long distance for zooming. This causes the entrance pupil to be positioned very far at or near the wide-angle end [W], and thus requires that the front-end lens unit have an unduly large diameter.
In a zoom lens system, like those of the first to third embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the first and third lens units (Gr1 and Gr3) are kept in fixed positions and the second and fourth lens units (Gr2 and Gr4) are moved (in particular, those of the type in which, during zooming from the wide-angle end [W] to the telephoto end [T], the second lens unit (Gr2) is moved monotonically from the object side to the image side and the fourth lens unit (Gr4) is moved monotonically from the image side to the object side), it is preferable that Condition (3) below be fulfilled. Moreover, it is more preferable that Condition (1) noted above be additionally fulfilled.
0.9<M2/Z<2.7 (3)
where
M2 represents the displacement amount of the second lens unit (Gr2) during zooming from the wide-angle end [W] to the telephoto end [T]; and
Z represents the zoom ratio (which equals fT/fW, where fT represents the focal length of the entire zoom lens system at the telephoto end [T], and fW represents the focal length of the entire zoom lens system at the wide-angle end [W]).
Condition (3) defines the relationship to be preferably fulfilled between the amount of movement of the second lens unit (Gr2) during zooming from the wide-angle end [W] to the telephoto end [T] and the zoom ratio. Note that, in general, the greater the zoom ratio, the larger the amount of movement. Thus, it can be said that Condition (3) defines the range of the preferable amount of movement of the second lens unit (Gr2) to obtain satisfactory optical performance in a compact optical system. If the upper limit of Condition (3) is exceeded, the amount of movement of the second lens unit (Gr2) is too large relative to the zoom ratio, and thus, at the wide-angle end [W], the gap between the second lens unit (Gr2) and the aperture stop (S) is so large that the entrance pupil is positioned very far. This requires that the front-end lens unit have unduly large diameters. In contrast, if the lower limit of Condition (3) is exceeded, the amount of movement of the second lens unit (Gr2) is too small relative to the zoom ratio. A reduction in the amount of movement of the second lens unit (Gr2) is necessarily accompanied by an increase in the optical power in the second lens unit (Gr2). However, an unduly strong optical power in the second lens unit (Gr2) increases the aberrations that occur in the second lens unit (Gr2) (in particular, the distortion and the curvature of field on the wide-angle side).
In a zoom lens system, like those of the first to third embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the first and third lens units (Gr1 and Gr3) are kept in fixed positions and the second and fourth lens units (Gr2 and Gr4) are moved (in particular, those of the type in which, during zooming from the wide-angle end [W] to the telephoto end [T], the second lens unit (Gr2) is moved monotonically from the object side to the image side and the fourth lens unit (Gr4) is moved monotonically from the image side to the object side), it is preferable that Condition (4) below be fulfilled. Moreover, it is more preferable that Conditions (1), and further, Condition (3) noted above be additionally fulfilled.
0.2<f4/f3<1.0 (4)
where
f3 represents the focal length of the third lens unit (Gr3); and
f4 represents the focal length of the fourth lens unit (Gr4).
Condition (4) defines the preferable ratio of the focal length of the third lens unit (Gr3) to the focal length of the fourth lens unit (Gr4). If the lower limit of Condition (4) is exceeded, the focal length of the fourth lens unit (Gr4) is relatively short, and thus the optical power of the fourth lens unit (Gr4) is relatively strong. Accordingly, if the lower limit of Condition (4) is exceeded, it is difficult to correct off-axial optical performance (in particular, the curvature of field at the wide-angle end [W]) properly. In contrast, if the upper limit of Condition (4) is exceeded, the focal length of the third lens unit (Gr3) is relatively short, and thus the optical power of the third lens unit (Gr3) is relatively strong. Accordingly, if the upper limit of Condition (4) is exceeded, it is difficult to correct the spherical aberration properly over the entire zoom range.
In a zoom lens system, like those of the first to third embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the first and third lens units (Gr1 and Gr3) are kept in fixed positions and the second and fourth lens units (Gr2 and Gr4) are moved (in particular, those of the type in which, during zooming from the wide-angle end [W] to the telephoto end [T], the second lens unit (Gr2) is moved monotonically from the object side to the image side and the fourth lens unit (Gr4) is moved monotonically from the image side to the object side), it is preferable that Condition (5) below be fulfilled.
0.4<log(.beta.2T/.beta.2W)/log(Z)<0.75 (5)
where
.beta.2W represents the lateral magnification of the second lens unit (Gr2) at the wide-angle end [W]; and
.beta.2T represents the lateral magnification of the second lens unit (Gr2) at the telephoto end [T].
In Condition (5), the term "log(.beta.2T/.beta.2W)/log(Z)" defines how far the second lens unit (Gr2) is responsible for the zooming achieved by the entire zoom lens system. Condition (5) assumes that the second lens unit (Gr2) is responsible for zooming substantially to the same extent as the lens units other than the second lens unit (Gr2) are. If the lower limit of Condition (5) is exceeded, the responsibility of the lens units disposed on the image side of the second lens unit (Gr2) for zooming is so heavy that spherical aberration cannot be corrected properly. In contrast, if the upper limit of Condition (5) is exceeded, the responsibility of the second lens unit (Gr2) for zooming is so heavy that distortion and curvature of field cannot be corrected properly.
In a zoom lens system, like those of the first to third embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the first and third lens units (Gr1 and Gr3) are kept in fixed positions and the second and fourth lens units (Gr2 and Gr4) are moved (in particular, those of the type in which, during zooming from the wide-angle end [W] to the telephoto end [T], the second lens unit (Gr2) is moved monotonically from the object side to the image side and the fourth lens unit (Gr4) is moved monotonically from the image side to the object side), the use of an aspherical surface makes it possible to obtain more satisfactory optical performance effectively. For example, it is preferable to use an aspherical surface that fulfills Condition (6) below at least on one surface in the second lens unit (Gr2).
0.45<(.vertline.x.vertline.-.vertline.x0.vertline.)/{C0(N'-N).multidot.f2}<0(6)
where
x represents the deviation (mm) of the aspherical surface in a direction perpendicular to the optical axis (AX) direction of the aspherical surface;
x0 represents the deviation (mm) of the reference spherical surface in a direction perpendicular to the optical axis (AX) direction of the reference spherical surface;
C0 represents the curvature of the reference spherical surface (i.e. the nominal curvature of the aspherical surface (mm.sup.-1 ));
N represents the refractive index of the object-side medium of the aspherical surface for the d-line;
N' represents the refractive index of the image-side medium of the aspherical surface for the d-line; and
f2 represents the focal length (mm) of the second lens unit (Gr2), where x and x0 are defined respectively by Formulae (AS) and (RE) below. Note that x represents the shape of the aspherical surface, and x0 represents the shape of the reference spherical surface. ##EQU1## where y represents the height in a direction perpendicular to the optical axis (AX);
.epsilon. represents the quadric surface parameter; and
Ai represents the aspherical coefficient of the ith order.
Condition (6) defines the aspherical surface as being so shaped as to weaken the negative optical power of the second lens unit (Gr2). Fulfillment of Condition (6) makes it possible to achieve proper correction of aberrations, in particular the distortion and the curvature of field on the wide-angle side. If the lower limit of Condition (6) is exceeded, the positive distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the positive direction becomes unduly large. In contrast, if the upper limit of Condition (6) is exceeded, the negative distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the negative direction becomes unduly large. Note that, in a case where the second lens unit (Gr2) includes a plurality of aspherical surfaces, at least one of those aspherical surfaces needs to fulfill Condition (6) above; that is, the other aspherical surfaces do not necessarily have to fulfill Condition (6) above, if that is advantageous for the correction of other aberrations.
It is preferable that the fourth lens unit (Gr4) include at least one aspherical surface that fulfills Condition (7) below.
0.8<(.vertline.x.vertline.-.vertline.x0.vertline.)/{C0(N'-N).multidot.f4}<0(7)
Condition (7) defines the aspherical surface as being so shaped as to weaken the positive optical power of the fourth lens unit (Gr4). Fulfillment of Condition (7) makes it possible to achieve proper correction of aberrations, in particular the distortion and the curvature of field on the wide-angle side as well as the spherical aberration on the telephoto side. If the lower limit of Condition (7) is exceeded, the positive distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the positive direction becomes unduly large. Moreover, spherical aberration appears notably in the positive direction on the telephoto side. In contrast, if the upper limit of Condition (7) is exceeded, the negative distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the negative direction becomes unduly large. Moreover, spherical aberration appears notably in the negative direction on the telephoto side.
<Embodiments 4 to 7 >
The zoom lens systems of the fourth to seventh embodiments are each composed of, from the object side, a first lens unit having a positive optical power (Gr1), a second lens unit having a negative optical power (Gr2), a third lens unit having a positive optical power (Gr3), and a fourth lens unit having a positive optical power (Gr4). During zooming from the wide-angle end [W] to the telephoto end [T], the first and third lens units (Gr1 and Gr3) are kept in fixed positions, the second lens unit (Gr2) is moved monotonically from the object side to the image side, and the fourth lens unit (Gr4) is moved monotonically from the image side to the object side. Note that the fourth lens unit (Gr4) has at its image-side end a low-pass filter (LPF) having the shape of a flat plate.
In the zoom lens system of the fourth embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gr1) is composed of a doublet lens element formed by cementing together a negative meniscus lens element convex to the object side and a biconvex lens element, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, and a doublet lens element formed by cementing together a biconcave lens element and a biconvex lens element. The third lens unit (Gr3) is composed of an aperture stop (S), and a doublet lens element formed by cementing together a biconvex lens element and a biconcave lens element. The fourth lens unit (Gr4) is composed of a biconvex lens element, and a negative meniscus lens element convex to the object side.
In the zoom lens system of the fifth embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gri) is composed of a doublet lens element formed by cementing together a negative meniscus lens element convex to the object side and a biconvex lens element, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, and a doublet lens element formed by cementing together a biconcave lens element and a biconvex lens element. The third lens unit (Gr3) is composed of an aperture stop (S), and a doublet lens element formed by cementing together a biconvex lens element and a biconcave lens element. The fourth lens unit (Gr4) is composed of a biconvex lens element, a negative meniscus lens element convex to the object side, and a positive meniscus lens element convex to the object side.
In the zoom lens system of the sixth embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gr1) is composed of a negative meniscus lens element convex to the object side, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, a biconcave lens element, and a plano-convex lens element convex to the object side. The third lens unit (Gr3) is composed of an aperture stop (S), and a doublet lens element formed by cementing together a positive meniscus lens element convex to the object side and a negative meniscus lens element convex to the object side. The fourth lens unit (Gr4) is composed of a biconvex lens element, and a biconcave lens element.
In the zoom lens system of the seventh embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gri) is composed of a doublet lens element formed by cementing together a negative meniscus lens element convex to the object side and a biconvex lens element, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, and a doublet lens element formed by cementing together a biconcave lens element and a biconvex lens element. The third lens unit (Gr3) is composed of an aperture stop (S), and a doublet lens element formed by cementing together a biconvex lens element and a biconcave lens element. The fourth lens unit (Gr4) is composed of a biconvex lens element, a biconcave lens element, and a positive meniscus lens element convex to the object side.
Two examples of focusing methods that are considered fit for a zoom lens system like those of the fourth to seventh embodiments are: a front-end-unit-focusing method in which focusing is achieved by moving the first lens unit (Gr1), and an inner-unit-focusing method in which focusing is achieved by moving the fourth lens unit (Gr4). According to the former focusing method, the first lens unit (Gr1) is moved out toward the object side for focusing on a close-distance object, and therefore the front-end lens unit needs to be given a comparatively large diameter in order to secure sufficient amount of peripheral light. Moreover, the lens unit that is moved for focusing is kept in a fixed position during zooming. This is inefficient. On the other hand, according to the latter focusing method, although the third and fourth lens units (Gr3 and Gr4) come closest to each other in the range from the middle-focal-length position [M] to the telephoto end [T], where a relatively large amount of movement is required for focusing, it is necessary to secure a sufficient space between the third and fourth lens units (Gr3 and Gr4) to achieve focusing. This is also inefficient.
For these reasons, the zoom lens systems of the fourth to seventh embodiments adopt the inner-unit-focusing method, and thus perform focusing by moving the second lens unit (Gr2); more precisely, for focusing on a close-distance object, it moves the second lens unit (Gr2) toward the object side. Where focusing is performed by moving the second lens unit (Gr2) in this way, the first and second lens units (Gr1 and Gr2) come closest to each other at the wide-angle end [W], where a minimum amount of movement of the second lens unit (Gr2) is required for focusing. This makes it possible to secure a space for focusing very efficiently.
In a zoom lens system, like those of the fourth to seventh embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming from the wide-angle end [W] to the telephoto end [T], the first and third lens units (Gr1 and Gr3) are kept in fixed positions, the second lens unit (Gr2) is moved from the object side to the image side, and simultaneously the fourth lens unit (Gr4) is so moved as to compensate the movement of the image plane properly, and in which the second lens unit (Gr2) is moved for focusing, it is preferable that Condition (8) below be fulfilled.
0.5<.vertline..beta.2T<0.98 (8)
where
.beta.2T represents the lateral magnification of the second lens unit (Gr2) at the telephoto end [T].
Condition (8) defines the lateral magnification of the second lens unit (Gr2) at the telephoto end [T] to be preferably fulfilled. If the lower limit of Condition (8) is exceeded, the total length is too long and the diameter of the front-end lens unit is too large, and simultaneously, spherical aberration appears notably toward the positive side. In contrast, if the upper limit of Condition (8) is exceeded, spherical aberration appears notably toward the negative side.
In a zoom lens system, like those of the fourth to seventh embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming from the wide-angle end [W] to the telephoto end [T], the first and third lens units (Gr1 and Gr3) are kept in fixed positions, the second lens unit (Gr2) is moved from the object side to the image side, and simultaneously the fourth lens unit (Gr4) is so moved as to compensate the movement of the image plane properly, and in which the second lens unit (Gr2) is moved for focusing, it is preferable that Condition (9) below be fulfilled. Moreover, it is more preferable that Condition (8) noted above be additionally fulfilled.
3.0<f1/fW<9.0 (9)
where
f1 represents the focal length of the first lens unit (Gr1); and
fW represents the focal length of the entire zoom lens system at the wide-angle end [W].
Condition (9) defines the ratio of the focal length of the first lens unit (Gr1) to the focal length of the entire zoom lens system to be preferably fulfilled to strike a proper balance between the total length and the aberration characteristics. If the lower limit of Condition (9) is exceeded, the focal length of the first lens unit (Gr1) is so short that the optical power of the first lens unit (Gr1) is too strong. This helps reduce the total length of the zoom lens system, but simultaneously increases aberrations (in particular, the spherical aberration and the longitudinal chromatic aberration on the telephoto side). In contrast, if the upper limit of Condition (9) is exceeded, the focal length of the first lens unit (Gr1) is so long that the optical power of the first lens unit (Gr1) is too weak. This helps reduce aberrations, but simultaneously makes the total length of the zoom lens system unduly long. An unduly long total length demands an unduly large diameter in the front-end lens unit, and thus makes the zoom lens system as a whole unduly large.
In a zoom lens system, like those of the fourth to seventh embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming from the wide-angle end [W] to the telephoto end [T], the first and third lens units (Gr1 and Gr3) are kept in fixed positions, the second lens unit (Gr2) is moved monotonically from the object side to the image side, and simultaneously the fourth lens unit (Gr4) is moved monotonically from the image side to the object side, and in which the second lens unit (Gr2) is moved for focusing, it is preferable that Condition (10) below be fulfilled.
0.15<M4/M2<0.55 (10)
where
M2 represents the displacement amount of the second lens unit (Gr2) during zooming from the wide-angle end [W] to the telephoto end [T]; and
M4 represents the displacement amount of the fourth lens unit (Gr4) during zooming from the wide-angle end [W] to the telephoto end [T].
Condition (10) defines the ratio of the amount of movement of the fourth lens unit (Gr4) to that of the second lens unit (Gr2) during zooming from the wide-angle end [W] to the telephoto end [T]. Fulfillment of Condition (10) makes it possible to keep the ratio of the responsibility of the second lens unit (Gr2) for zooming to the responsibility of the lens units other than the second lens unit (Gr2) for zooming in an appropriate range, and thereby strike a proper balance between the size of the zoom lens system and the aberration characteristics. If the lower limit of Condition (10) is exceeded, the amount of movement of the second lens unit (Gr2) is too large, and thus the entrance pupil is positioned too far. This requires that the front-end lens unit have an unduly large diameter. Moreover, the responsibility of the second lens unit (Gr2) for zooming is so heavy that distortion and curvature of field cannot be corrected properly. In contrast, if the upper limit of Condition (10) is exceeded, the amount of movement of the second lens unit (Gr2) is too small, and thus the responsibility of the lens units disposed on the image side of the second lens unit (Gr2) for zooming is so heavy that spherical aberration cannot be corrected properly.
In a zoom lens system, like those of the fourth to seventh embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming from the wide-angle end [W] to the telephoto end [T], the first and third lens units (Gr1 and Gr3) are kept in fixed positions, the second lens unit (Gr2) is moved monotonically from the object side to the image side, and simultaneously the fourth lens unit (Gr4) is moved monotonically from the image side to the object side, and in which the second lens unit (Gr2) is moved for focusing, it is preferable that Condition (11) below be fulfilled. Moreover, it is more preferable that Condition (10) noted above be additionally fulfilled.
0.4<log(.beta.2T/.beta.2W)/log(Z)<0.75 (11)
where
.beta.2W represents the lateral magnification of the second lens unit (Gr2) at the wide-angle end [W]; and
Z represents the zoom ratio (which equals fT/fW, where fW represents the focal length of the entire zoom lens system at the wide-angle end [W]; and fT represents the focal length of the entire zoom lens system at the telephoto end [T].
In Condition (11), the term "log(.beta.2T/.beta.2W)/log(Z)" defines how far the second lens unit (Gr2) is responsible for the zooming achieved by the entire zoom lens system. Condition (11) assumes that the second lens unit (Gr2) is responsible for zooming substantially to the same extent as the lens units other than the second lens unit (Gr2) are. If the lower limit of Condition (11) is exceeded, the responsibility of the lens units disposed on the image side of the second lens unit (Gr2) for zooming is so heavy that spherical aberration cannot be corrected properly. In contrast, if the upper limit of Condition (11) is exceeded, the responsibility of the second lens unit (Gr2) for zooming is so heavy that distortion and curvature of field cannot be corrected properly.
In a zoom lens system, like those of the fourth to seventh embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming from the wide-angle end [W] to the telephoto end [T], the first and third lens units (Gr1 and Gr3) are kept in fixed positions, the second lens unit (Gr2) is moved from the object side to the image side, and simultaneously the fourth lens unit (Gr4) is so moved as to compensate the movement of the image plane properly, and in which the second lens unit (Gr2) is moved for focusing, the use of an aspherical surface makes it possible to obtain more satisfactory optical performance. For example, it is preferable to use an aspherical surface that fulfills Condition (12) below at least on one surface in the second lens unit (Gr2).
-0.45<(.vertline.x.vertline.-.vertline.x0.vertline.)/{C0(N'-N).multidot.f2}<0 (12)
where
x represents the deviation (mm) of the aspherical surface in a direction perpendicular to the optical axis (AX) direction of the aspherical surface;
x0 represents the deviation (mm) of the reference spherical surface in a direction perpendicular to the optical axis (AX) direction of the reference spherical surface;
C0 represents the curvature of the reference spherical surface (i.e. the nominal curvature of the aspherical surface (mm.sup.-1));
N represents the refractive index of the object-side medium of the aspherical surface for the d-line;
N' represents the refractive index of the image-side medium of the aspherical surface for the d-line; and
f2 represents the focal length (mm) of the second lens unit (Gr2), where x and x0 are defined respectively by Formulae (AS) and (RE) noted previously. Note that x represents the shape of the aspherical surface, and x0 represents the shape of the reference spherical surface.
Condition (12) defines the aspherical surface as being so shaped as to weaken the negative optical power of the second lens unit (Gr2). Fulfillment of Condition (12) makes it possible to achieve proper correction of aberrations, in particular the distortion and the curvature of field on the wide-angle side in a close-distance shooting condition. If the lower limit of Condition (12) is exceeded, the positive distortion increases on the wide-angle side, in particular in the close-distance shooting condition, and simultaneously the inclination of the image plane in the positive direction becomes unduly large. In contrast, if the upper limit of Condition (12) is exceeded, the negative distortion increases on the wide-angle side, in particular in the close-distance shooting condition, and simultaneously the inclination of the image plane in the negative direction becomes unduly large. Note that, in a case where the second lens unit (Gr2) includes a plurality of aspherical surfaces, at least one of those aspherical surfaces needs to fulfill Condition (12) above; that is, the other aspherical surfaces do not necessarily have to fulfill Condition (12) above, if that is advantageous for the correction of other aberrations.
It is preferable that the fourth lens unit (Gr4) include at least one aspherical surface that fulfills Condition (13) below.
-0.8<(.vertline.x.vertline.-.vertline.x0.vertline.)/{C0(N'-N).multidot.f4}<0(13)
where
f4 represents the focal length (mm) of the fourth lens unit (Gr4).
Condition (13) defines the aspherical surface as being so shaped as to weaken the positive optical power of the fourth lens unit (Gr4). Fulfillment of Condition (13) makes it possible to achieve proper correction of aberrations, in particular the distortion and the curvature of field on the wide-angle side as well as the spherical aberration on the telephoto side. If the lower limit of Condition (13) is exceeded, the positive distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the positive direction becomes unduly large. Moreover, spherical aberration appears notably in the positive direction on the telephoto side. In contrast, if the upper limit of Condition (13) is exceeded, the negative distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the negative direction becomes unduly large. Moreover, spherical aberration appears notably in the negative direction on the telephoto side.
<Embodiments 8 to 10>
The zoom lens systems of the eighth to tenth embodiments are each composed of, from the object side, a first lens unit having a positive optical power (Gr1), a second lens unit having a negative optical power (Gr2), a third lens unit having a positive optical power (Gr3), and a fourth lens unit having a positive optical power (Gr4). During zooming from the wide-angle end [W] to the telephoto end [T], the third lens unit (Gr3) is kept in a fixed position, the first and fourth lens units (Gr1 and Gr4) are moved monotonically toward the object side, and the second lens unit (Gr2) is moved monotonically toward the image side. Note that the fourth lens unit (Gr4) has at its image-side end a low-pass filter (LPF) having the shape of a flat plate.
In the zoom lens system of the eighth embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gr1) is composed of a doublet lens element formed by cementing together a negative meniscus lens element convex to the object side and a biconvex lens element, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, and a doublet lens element formed by cementing together a biconcave lens element and a biconvex lens element. The third lens unit (Gr3) is composed of an aperture stop (S), a biconvex lens element, and a negative meniscus lens element convex to the object side. The fourth lens unit (Gr4) is composed of a biconvex lens element, a negative meniscus lens element convex to the object side, and a positive meniscus lens element convex to the object side.
In the zoom lens system of the ninth embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gr1) is composed of a doublet lens element formed by cementing together a negative meniscus lens element convex to the object side and a biconvex lens element, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, a biconcave lens element, and a biconvex lens element. The third lens unit (Gr3) is composed of an aperture stop (S), a biconvex lens element, and a negative meniscus lens element convex to the object side. The fourth lens unit (Gr4) is composed of a biconvex lens element, a negative meniscus lens element convex to the object side, and a positive meniscus lens element convex to the object side.
In the zoom lens system of the tenth embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gr1) is composed of a doublet lens element formed by cementing together a negative meniscus lens element convex to the object side and a biconvex lens element, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, and a doublet lens element formed by cementing together a biconcave lens element and a biconvex lens element. The third lens unit (Gr3) is composed of an aperture stop (S), and a doublet lens element formed by cementing together a biconvex lens element and a biconcave lens element. The fourth lens unit (Gr4) is composed of a positive meniscus lens element convex to the object side, a biconvex lens element, and a biconcave lens element.
In a zoom lens system, like those of the eighth to tenth embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the third lens unit (Gr3) is kept in a fixed position and the first, second, and fourth lens units (Gr1, Gr2, and Gr4) are moved, it is preferable that Condition (14) below be fulfilled.
-5.0<M1/Ymax<-1.0 (14)
where
M1 represents the displacement amount of the first lens unit (Gr1) from the wide-angle end [W] to the telephoto end [T] (assuming that the direction pointing to the object side is negative); and
Ymax represents the maximum image height.
Condition (14) defines the amount of movement of the first lens unit (Gr1) during zooming to be preferably fulfilled to strike a proper balance between the total length and the diameter of the front-end lens unit. If the lower limit of Condition (14) is exceeded, the amount of movement of the first lens unit (Gr1) during zooming is so large that the total length of the zoom lens system becomes unduly long at the telephoto end [T], and simultaneously the diameter of the front-end lens unit needs to be unduly large in order to secure sufficient amount of peripheral light at the telephoto end [T]. In contrast, if the upper limit of Condition (14) is exceeded, the amount of movement of the first lens unit (Gr1) during zooming is so small that the total length of the zoom lens system becomes unduly long at the wide-angle end [W], and simultaneously the diameter of the front-end lens unit needs to be unduly large in order to secure sufficient amount of peripheral light at the wide-angle end [W].
In a zoom lens system, like those of the eighth to tenth embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the third lens unit (Gr3) is kept in a fixed position and the first, second, and fourth lens units (Gr1, Gr2, and Gr4) are moved, it is preferable that Condition (15) below be fulfilled. Moreover, it is more preferable that Condition (14) noted above be additionally fulfilled.
1.0<M4/M2<-0.1 (15)
where
M2 represents the displacement amount of the second lens unit (Gr2) from the wide-angle end [W] to the telephoto end [T] (assuming that the direction pointing to the object side is negative); and
M4 represents the displacement amount of the fourth lens unit (Gr4) from the wide-angle end [W] to the telephoto end [T] (assuming that the direction pointing to the object side is negative).
Condition (15) defines the ratio of the amount of movement of the fourth lens unit (Gr4) to that of the second lens unit (Gr2) during zooming to be preferably fulfilled. If the lower limit of Condition (15) is exceeded, the amount of movement of the fourth lens unit (Gr4) is too large. As a result, the responsibility of the fourth lens unit (Gr4) for zooming is so heavy that spherical aberration cannot be corrected properly. In contrast, if the upper limit of Condition (15) is exceeded, the amount of movement of the second lens unit (Gr2) is too large. This increases the distance between the second lens unit (Gr2) and the aperture stop (S) at the wide-angle end [W]. As a result, the entrance pupil is positioned too far, and thus the front-end lens unit needs to be given an unduly large diameter. Moreover, the responsibility of the second lens unit (Gr2) for zooming is so heavy that distortion and curvature of field cannot be corrected properly.
In a zoom lens system, like those of the eighth to tenth embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the third lens unit (Gr3) is kept in a fixed position and the first, second, and fourth lens units (Gr1, Gr2, and Gr4) are moved, it is preferable that Condition (16) below be fulfilled. Moreover, it is more preferable that Condition (14) noted above be additionally fulfilled.
0.2<log(.beta.2T/.beta.2W)/log(Z)<0.9 (16)
where
.beta.2W represents the lateral magnification of the second lens unit (Gr2) at the wide-angle end [W];
.beta.2T represents the lateral magnification of the second lens unit (Gr2) at the telephoto end [T]; and
Z represents the zoom ratio (which equals fT/fW, where fr represents the focal length of the entire zoom lens system at the telephoto end [T]; and fW represents the focal length of the entire zoom lens system at the wide-angle end [W]).
In Condition (16), the term "log(.beta.2T/.beta.2W)/log(Z)" defines how far the second lens unit (Gr2) is responsible for the zooming achieved by the entire zoom lens system. If the lower limit of Condition (16) is exceeded, the responsibility of the lens units disposed on the image side of the second lens unit (Gr2) for zooming is so heavy that spherical aberration cannot be corrected properly. In contrast, if the upper limit of Condition (16) is exceeded, the responsibility of the second lens unit (Gr2) for zooming is so heavy that distortion and curvature of field cannot be corrected properly.
In a zoom lens system, like those of the eighth to tenth embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the third lens unit (Gr3) is kept in a fixed position and the first, second, and fourth lens units (Gr1, Gr2, and Gr4) are moved (in particular, those of the type in which, during zooming from the wide-angle end [W] to the telephoto end [T], the first and fourth lens units (Gr1 and Gr4) are moved monotonically to the object side and the second lens unit (Gr2) is moved monotonically to the image side), the use of an aspherical surface makes it possible to obtain more satisfactory optical performance. For example, it is preferable to use an aspherical surface that fulfills Condition (17) below in the second lens unit (Gr2). Moreover, it is more preferable that Conditions (14) and (15), or Conditions (14) and (16) noted above be additionally fulfilled.
0<(x-x0)/(N'-N)<0.9 (17)
where
x represents the deviation of the aspherical surface in a direction perpendicular to the optical axis (AX) direction of the aspherical surface (in millimeters, assuming that the direction pointing to the object side is negative);
x0 represents the deviation of the reference spherical surface in a direction perpendicular to the optical axis (AX) direction of the reference spherical surface (in millimeters, assuming that 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,
where x and x0 are defined respectively by Formulae (AS) and (RE) noted previously. Note that x represents the shape of the aspherical surface, and x0 represents the shape of the reference spherical surface.
Condition (17) defines the aspherical surface as being so shaped as to weaken the negative optical power of the second lens unit (Gr2). Fulfillment of Condition (17) makes it possible to achieve proper correction of aberrations, in particular the distortion and the curvature of field on the wide-angle side. If the lower limit of Condition (17) is exceeded, the positive distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the positive direction becomes unduly large. In contrast, if the upper limit of Condition (17) is exceeded, the negative distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the negative direction becomes unduly large. Note that, in a case where the second lens unit (Gr2) includes a plurality of aspherical surfaces, at least one of those aspherical surfaces needs to fulfill Condition (17) above; that is, the other aspherical surfaces do not necessarily have to fulfill Condition (17) above, if that is advantageous for the correction of other aberrations.
It is preferable to use an aspherical surface that fulfills Condition (18) below in the third lens unit (Gr3). Moreover, it is more preferable that Conditions (14) and (15), or Conditions (14) and (16) noted above be additionally fulfilled.
-0.35<(x-x0)/(N'-N)<0 (18)
Condition (18) defines the aspherical surface as being so shaped as to weaken the positive optical power of the third lens unit (Gr3). Fulfillment of Condition (18) makes it possible to achieve proper correction of aberrations, in particular spherical aberration. If the lower limit of Condition (18) is exceeded, in particular, spherical aberration appears notably in the positive direction on the telephoto side. In contrast, if the upper limit of Condition (18) is exceeded, in particular, spherical aberration appears notably in the negative direction on the telephoto side. Note that, in a case where the third lens unit (Gr3) includes a plurality of aspherical surfaces, at least one of those aspherical surfaces needs to fulfill Condition (18) above; that is, the other aspherical surfaces do not necessarily have to fulfill Condition (18) above, if that is advantageous for the correction of other aberrations.
It is preferable to use an aspherical surface that fulfills Condition (19) below in the fourth lens unit (Gr4). Moreover, it is more preferable that Conditions (14) and (15), or Conditions (14) and (16) noted above be additionally fulfilled.
0.85<(x-x0)/(N'-N)<0 (19)
Condition (19) defines the aspherical surface as being so shaped as to weaken the positive optical power of the fourth lens unit (Gr4). Fulfillment of Condition (19) makes it possible to achieve proper correction of aberrations, in particular the distortion and the curvature of field on the wide-angle side as well as the spherical aberration on the telephoto side. If the lower limit of Condition (19) is exceeded, the positive distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the positive direction becomes unduly large. Moreover, spherical aberration appears notably in the positive direction on the telephoto side. In contrast, if the upper limit of Condition (19) is exceeded, the negative distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the positive direction becomes unduly large. Moreover, spherical aberration appears notably in the negative direction on the telephoto side. Note that, in a case where the fourth lens unit (Gr4) includes a plurality of aspherical surfaces, at least one of those aspherical surfaces needs to fulfill Condition (19) above; that is, the other aspherical surfaces do not necessarily have to fulfill Condition (19) above, if that is advantageous for the correction of other aberrations.
<Embodiments 11 to 13>
The zoom lens systems of the eleventh to thirteenth embodiments are each composed of, from the object side, a first lens unit having a positive optical power (Gr1), a second lens unit having a negative optical power (Gr2), a third lens unit having a positive optical power (Gr3), and a fourth lens unit having a positive optical power (Gr4). During zooming from the wide-angle end [W] to the telephoto end [T], the third lens unit (Gr3) is kept in a fixed position, the first and fourth lens units (Gr1 and Gr4) are moved monotonically to the object side, and the second lens unit (Gr2) is moved monotonically to the image side. Note that the fourth lens unit (Gr4) has at its image-side end a low-pass filter (LPF) having the shape of a flat plate. In the zoom lens system of the eleventh embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gr1) is composed of a doublet lens element formed by cementing together a negative meniscus lens element convex to the object side and a biconvex lens element, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, a biconcave lens element, and a biconvex lens element. The third lens unit (Gr3) is composed of an aperture stop (S), a positive meniscus lens element convex to the object side, and a negative meniscus lens element convex to the object side. The fourth lens unit (Gr4) is composed of a positive meniscus lens element convex to the object side, a negative meniscus lens element convex to the object side, and a positive meniscus lens element convex to the object side.
In the zoom lens system of the twelfth embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gr1) is composed of a doublet lens element formed by cementing together a negative meniscus lens element convex to the object side and a biconvex lens element, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, and a doublet lens element formed by cementing together a biconcave lens element and a biconvex lens element. The third lens unit (Gr3) is composed of an aperture stop (S), a biconvex lens element, and a negative meniscus lens element convex to the object side. The fourth lens unit (Gr4) is composed of a biconvex lens element, a negative meniscus lens element convex to the object side, and a positive meniscus lens element convex to the object side.
In the zoom lens system of the thirteenth embodiment, the lens units are each composed, from the object side, as follows. The first lens unit (Gr1) is composed of a doublet lens element formed by cementing together a negative meniscus lens element convex to the object side and a biconvex lens element, and a positive meniscus lens element convex to the object side. The second lens unit (Gr2) is composed of a negative meniscus lens element convex to the object side, and a doublet lens element formed by cementing together a biconcave lens element and a biconvex lens element.
The third lens unit (Gr3) is composed of an aperture stop (S), and a doublet lens element formed by cementing together a biconvex lens element and a negative meniscus lens element concave to the object side. The fourth lens unit (Gr4) is composed of a positive meniscus lens element convex to the object side, a biconvex lens element, and a negative meniscus lens element convex to the object side.
Two examples of focusing methods that are considered fit for a zoom lens system like those of the eleventh to thirteenth embodiments are: a front-end-unit-focusing method in which focusing is achieved by moving the first lens unit (Gr1), and an inner-unit-focusing method in which focusing is achieved by moving the fourth lens unit (Gr4). According to the former focusing method, the first lens unit (Gr1) is moved out toward the object side for focusing on a close-distance object, and therefore the front-end lens unit needs to be given a comparatively large diameter in order to secure sufficient amount of peripheral light. On the other hand, according to the latter focusing method, although the third and fourth lens units (Gr3 and Gr4) come closest to each other in the range from the middle-focal-length position [M] to the telephoto end [T], where a relatively large amount of movement is required for focusing, it is necessary to secure a sufficient space between the third and fourth lens units (Gr3 and Gr4) to achieve focusing. This is inefficient.
For these reasons, the zoom lens systems of the eleventh to thirteenth embodiments adopt the inner-unit-focusing method, and thus perform focusing by moving the second lens unit (Gr2); more precisely, for focusing on a close-distance object, it moves the second lens unit (Gr2) toward the object side. Where focusing is performed by moving the second lens unit (Gr2) in this way, the first and second lens units (Gr1 and Gr2) come closest to each other at the wide-angle end [W], where a minimum amount of movement of the second lens unit (Gr2) is required for focusing. This makes it possible to secure a space for focusing very efficiently.
In a zoom lens system, like those of the eleventh to thirteenth embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the first, second, and fourth lens units (Gr1, Gr2, and Gr4) are moved and the second lens unit (Gr2) is moved for focusing, it is preferable that Condition (20) below be fulfilled.
0.1<.vertline..beta.2T.vertline.<1.0 (20)
where
.beta.2T represents the lateral magnification of the second lens unit (Gr2) at the telephoto end [T].
Condition (20) defines the lateral magnification of the second lens unit (Gr2) at the telephoto end [T] to be preferably fulfilled. If the lower limit of Condition (20) is exceeded, the total length is too long and the diameter of the front-end lens unit is too large, and simultaneously, spherical aberration appears notably toward the positive side. In contrast, if the upper limit of Condition (20) is exceeded, spherical aberration appears notably toward the negative side.
In a zoom lens system, like those of the eleventh to thirteenth embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the first, second, and fourth lens units (Gr1, Gr2, and Gr4) are moved and the second lens unit (Gr2) is moved for focusing, it is preferable that Condition (21) below be fulfilled. Moreover, it is more preferable that Condition (20) noted above be additionally fulfilled.
0.2<fW/f2<1.5 (21)
where
fW represents the focal length of the entire zoom lens system at the wide-angle end [W]; and
f2 represents the focal length of the second lens unit (Gr2).
Condition (21) defines the ratio of the focal length of the second lens unit (Gr2) to the focal length of the entire zoom lens system to be preferably fulfilled to strike a proper balance between the total length and the aberration characteristics. If the lower limit of Condition (21) is exceeded, the focal length of the second lens unit (Gr2) is so long that the optical power of the second lens unit (Gr2) is too weak. This helps reduce aberrations, but simultaneously makes the total length of the zoom lens system unduly long. An unduly long total length demands an unduly large diameter in the front-end lens unit, and thus makes the zoom lens system as a whole unduly large. In contrast, if the upper limit of Condition (21) is exceeded, the focal length of the second lens unit (Gr2) is so short that the optical power of second lens unit (Gr2) is too strong. This helps reduce the total length of the zoom lens system, but simultaneously increases aberrations (in particular, the negative distortion increases on the wide-angle side). Moreover, the inclination of the image plane in the positive direction becomes unduly large.
In a zoom lens system, like those of the eleventh to thirteenth embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the first, second, and fourth lens units (Gr1, Gr2, and Gr4) are moved and the second lens unit (Gr2) is moved for focusing, it is preferable that Condition (22) below be fulfilled. Moreover, it is more preferable that Condition (20), and further, Condition (21) noted above be additionally fulfilled.
-5.0<M1/Ymax<-1.0 (22)
where
M1 represents the displacement amount of the first lens unit (Gr1) from the wide-angle end [W] to the telephoto end [T] (assuming that the direction pointing to the object side is negative).
Ymax represents the maximum image height.
Condition (22) defines the amount of movement of the first lens unit (Gr1) during zooming to be preferably fulfilled to strike a proper balance between, in particular the total length and the diameter of the front-end lens unit. If the lower limit of Condition (22) is exceeded, the amount of movement of the first lens unit (Gr1) during zooming is so large that the total length of the zoom lens system becomes unduly long at the telephoto end [T], and simultaneously the diameter of the front-end lens unit needs to be unduly large in order to secure sufficient amount of peripheral light at the telephoto end [T]. In contrast, if the upper limit of Condition (22) is exceeded, the amount of movement of the first lens unit (Gr1) during zooming is so small that the total length of the zoom lens system becomes unduly long at the wide-angle end [W], and simultaneously the diameter of the front-end lens unit needs to be unduly large in order to secure sufficient amount of peripheral light at the wide-angle end [W].
In a zoom lens system, like those of the eleventh to thirteenth embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the first, second, and fourth lens units (Gr1, Gr2, and Gr4) are moved and the second lens unit (Gr2) is moved for focusing, the use of an aspherical surface makes it possible to obtain more satisfactory optical performance. For example, it is preferable to use an aspherical surface that fulfills Condition (23) below in the second lens unit (Gr2).
0<(x-x0)/(N'-N)<0.9 (23)
where
x represents the deviation of the aspherical surface in a direction perpendicular to the optical axis (AX) direction of the aspherical surface (in millimeters, assuming that the direction pointing to the object side is negative);
x0 represents the deviation of the reference spherical surface in a direction perpendicular to the optical axis (AX) direction of the reference spherical surface (in millimeters, assuming that 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,
where x and x0 are defined respectively by Formulae (AS) and (RE) noted previously. Note that x represents the shape of the aspherical surface, and x0 represents the shape of the reference spherical surface.
Condition (23) defines the aspherical surface as being so shaped as to weaken the negative optical power of the second lens unit (Gr2). Fulfillment of Condition (23) makes it possible to achieve proper correction of aberrations, in particular the distortion and the curvature of field on the wide-angle side. If the lower limit of Condition (23) is exceeded, the positive distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the positive direction becomes unduly large. In contrast, if the upper limit of Condition (23) is exceeded, the negative distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the negative direction becomes unduly large. Note that, in a case where the second lens unit (Gr2) includes a plurality of aspherical surfaces, at least one of those aspherical surfaces needs to fulfill Condition (23) above; that is, the other aspherical surfaces do not necessarily have to fulfill Condition (23) above, if that is advantageous for the correction of other aberrations.
It is preferable to use an aspherical surface that fulfills Condition (24) below in the third lens unit (Gr3).
0.35<(x-x0)/(N'-N)<0 (24)
Condition (24) defines the aspherical surface as being so shaped as to weaken the positive optical power of the third lens unit (Gr3). Fulfillment of Condition (24) makes it possible to achieve proper correction of aberrations, in particular spherical aberration. If the lower limit of Condition (24) is exceeded, in particular, spherical aberration appears notably in the positive direction on the telephoto side. In contrast, if the upper limit of Condition (24) is exceeded, in particular, spherical aberration appears notably in the negative direction on the telephoto side. Note that, in a case where the third lens unit (Gr3) includes a plurality of aspherical surfaces, at least one of those aspherical surfaces needs to fulfill Condition (24) above; that is, the other aspherical surfaces do not necessarily have to fulfill Condition (24) above, if that is advantageous for the correction of other aberrations.
It is preferable to use an aspherical surface that fulfills Condition (25) below in the fourth lens unit (Gr4).
-0.85<(x-x0)/(N'-N)<0 (25)
Condition (25) defines the aspherical surface as being so shaped as to weaken the positive optical power of the fourth lens unit (Gr4). Fulfillment of Condition (25) makes it possible to achieve proper correction of aberrations, in particular the distortion and the curvature of field on the wide-angle side as well as the spherical aberration on the telephoto side. If the lower limit of Condition (25) is exceeded, the positive distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the positive direction becomes unduly large. Moreover, spherical aberration appears notably in the positive direction on the telephoto side. In contrast, if the upper limit of Condition (25) is exceeded, the negative distortion increases on the wide-angle side, and simultaneously the inclination of the image plane in the negative direction becomes unduly large. Moreover, spherical aberration appears notably in the negative direction on the telephoto side. Note that, in a case where the fourth lens unit (Gr4) includes a plurality of aspherical surfaces, at least one of those aspherical surfaces needs to fulfill Condition (25) above; that is, the other aspherical surfaces do not necessarily have to fulfill Condition (25) above, if that is advantageous for the correction of other aberrations.
In a zoom lens system, like those of the eleventh to thirteenth embodiments, that consists of a positive, a negative, a positive, and a positive lens unit and in which, during zooming, the first, second, and fourth lens units (Gr1, Gr2, and Gr4) are moved and the second lens unit (Gr2) is moved for focusing, it is preferable that Condition (26) below be fulfilled,
0.1<M4/M<1.0 (26)
where
M1 represents the displacement amount of the first lens unit (Gr1) from the wide-angle end [W] to the telephoto end [T] (assuming that the direction pointing to the object side is negative); and
M4 represents the displacement amount of the fourth lens unit (Gr4) from the wide-angle end [W] to the telephoto end [T] (assuming that the direction pointing to the object side is negative).
Condition (26) defines the ratio of the amount of movement of the fourth lens unit (Gr4) to that of the first lens unit (Gr1) during zooming to be preferably fulfilled.
If the upper limit of Condition (26) is exceeded, the amount of movement of the fourth lens unit (Gr4) is too large, and thus the responsibility of the fourth lens unit (Gr4) for zooming is too heavy. This makes it difficult to correct spherical aberration properly. In contrast, if the lower limit of Condition (26) is exceeded, the amount of movement of the first lens unit (Gr1) is too large, and thus the entrance pupil is positioned too far away from the image plane in the longest focal length condition. As a result, the front-end lens unit needs to have an unduly large diameter.
<EXAMPLES>
Hereinafter, examples of the zoom lens systems of the first to thirteenth embodiments described above will be presented with reference to their construction data, graphic representations of aberrations, and other data. Tables 1 to 13 list the construction data of Examples 1 to 13, which respectively correspond to the first to thirteenth embodiments described above and have lens arrangements as shown in FIGS. 1 to 3, FIGS. 7 to 10, FIGS. 19 to 21, and FIGS. 25 to 27.
In the construction data of each example, ri (i=1, 2, 3, . . . ) represents the radius of curvature of the ith surface counted from the object side, 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, . . . ) represent the refractive index (Nd) and the Abbe number (vd), respectively, for the d-line of the ith optical element counted from the object side. Moreover, in the construction data, for each of the axial distances that vary with zooming (i.e. the variable axial distances), three values are listed that represent, from left, the actual surface-to-surface distance between the relevant lens units at the wide-angle end [W] (i.e. in the shortest focal length condition), the same distance at the middle-focal-length position [M], and the same distance at the telephoto end [T] (i.e. in the longest focal length condition). Also listed are the focal lengths f and the F-numbers FNO of the entire zoom lens system in those three focal-length conditions [W], [M], and [T]. Table 15 lists the distances that vary with focusing as observed in a close-distance shooting condition in Examples 4 to 7 (when the object distance D=equals 1m). Table 18 lists the same values as observed in Examples 11 to 13.
Furthermore, a surface whose radius of curvature ri is marked with an asterisk (*) is an aspherical surface, whose surface shape is defined by Formula (AS) noted earlier. Also listed for each Example together with the construction data are the data of the aspherical surfaces, and the values corresponding to Condition (6), (7), (12), (13), (17) to (19), and (23) to (25) that define conditions to be fulfilled by the aspherical surface (note that, there, ymax represents the maximum height of an aspherical surface in a direction perpendicular to its optical axis (AX) (i.e. the maximum effective radius)). Table 14 lists the values corresponding to Conditions (1) to (5) noted above as observed in Examples 1 to 3; Table 16 lists the values corresponding to Conditions (8) to (11) noted above as observed in Examples 4 to 7; Table 17 lists the values corresponding to Conditions (14) to (16) noted above as observed in Examples 8 to 10; and Table 19 lists the values corresponding to Conditions (20) to (22) and (26) noted above as observed in Examples 11 to 13.
FIGS. 4A to 4I, 5A to 5I, and 6A to 6I are graphic representations of the aberrations observed in Examples 1 to 3, respectively; FIGS. 11A to 11I and 12A to 12I, 13A to 13I and 14A to 14I, 15A to 15I and 16A to 16I, and 17A to 17I and 18A to 18I are graphic representations of the aberrations observed in Examples 4 to 7, respectively; FIGS. 22A to 22I, 23A to 23I, and 24A to 24I are graphic representations of the aberrations observed in Examples 8 to 10, respectively; and FIGS. 28A to 28I and 29A to 29I, 30A to 30I and 31A to 31I, and 32A to 32I and 33A to 33I are graphic representations of the aberrations observed in Examples 11 to 13, respectively. Of these diagrams, FIGS. 11A to 11I, 13A to 13I, 15A to 15I, and 17A to 17I show the aberrations observed in the infinite-distance shooting condition in Examples 4 to 7; FIGS. 12A to 12I, 14A to 14I, 16A to 16I, and 18A to 18I show the aberrations observed in the close-distance shooting condition (the object distance D equals 1m) in Examples 4 to 7; FIGS. 28A to 28I, 30A to 30I, and 32A to 32I show the aberrations observed in the infinite-distance shooting condition in Examples 11 to 13; and FIGS. 29A to 29I, 31A to 31I, and 33A to 33I show the aberrations observed in the close-distance shooting condition (the object distance D equals 1m) in Examples 11 to 13.
Of these diagrams, FIGS. 4A to 4C, 5A to 5C, 6A to 6C, 11A to 11C, 12A to 12C, 13A to 13C, 14A to 14C, 15A to 15C, 16A to 16C, 17A to 17C, 18A to 18C, 22A to 22C, 23A to 23C, 24A to 24C, 28A to 28C, 29A to 29C, 30A to 30C, 31A to 31C, 32A to 32C, and 33A to 33C show the aberrations observed at the wide-angle end [W]; FIGS. 4D to 4F, 5D to 5F, 6D to 6F, 11D to 11F, 12D to 12F, 13D to 13F, 14D to 14F, 15D to 15F, 16D to 16F, 17D to 17F, 18D to 18F, 22D to 22F, 23D to 23F, 24D to 24F, 28D to 28F, 29D to 29F, 30D to 30F, 31D to 31F, 32D to 32F, and 33D to 33F show the aberrations observed at the middle focal length [M]; and FIGS. 4G to 4I, 5G to 5I, 6G to 6I, 11G to 11I, 12G to 12I, 13G to 13I, 14G to 14I, 15G to 15I, 16G to 16I, 17G to 17I, 18G to 18I, 22G to 22I, 23G to 23I, 24G to 24I, 28G to 28I, 29G to 29I, 30G to 30I, 31G to 31I, 32G to 32I, and 33G to 33I show the aberrations observed at the telephoto end [T].
Of these diagrams, FIGS. 4A, 4D, 4G, 5A, 5D, 5G, 6A, 6D, 6G, 11A, 11D, 11G, 12A, 12D, 12G, 13A, 13D, 13G, 14A, 14D, 14G, 15A, 15D, 15G, 16A, 16D, 16G, 17A, 17D, 17G, 18A, 18D, 18G, 22A, 22D, 22G, 23A, 23D, 23G, 24A, 24D, 24G, 28A, 28D, 28G, 29A, 29D, 29G, 30A, 30D, 30G, 31A, 31D, 31G, 32A, 32D, 32G, 33A, 33D, and 33G show spherical aberration and sine condition. In these diagrams, the solid line (d) represents the spherical aberration for the d-line and the broken line (SC) represents the sine condition. FIGS. 4B, 4E, 4H, 5B, 5E, 5H, 6B, 6E, 6H, 11B, 11E, 11H, 12B, 12E, 12H, 13B, 13E, 13H, 14B, 14E, 14H, 15B, 15E, 15H, 16B, 16E, 16H, 17B, 17E, 17H, 18B, 18E, 18H, 22B, 22E, 22H, 23B, 23E, 23H, 24B, 24E, 24H, 28B, 28E, 28H, 29B, 29E, 29H, 30B, 30E, 30H, 31B, 31E, 31H, 32B, 32E, 32H, 33B, 33E, and 33H show astigmatism (Y' represents the image height). In these diagrams, the broken line (DM) and the solid line (DS) represent the astigmatism for the d-line on the meridional plane and on the sagittal plane, respectively. FIGS. 4C, 4F, 4I, 5C, 5F, 5I, 6C, 6F, 6I, 11C, 11F, 11I, 12C, 12F, 12I, 13C, 13F, 13I, 14C, 14F, 14I, 15C, 15F, 15I, 16C, 16F, 16I, 17C, 17F, 17I, 18C, 18F, 18I, 22C, 22F, 22I, 23C, 23F, 23I, 24C, 24F, 24I, 28C, 28F, 28I, 29C, 29F, 29I, 30C, 30F, 30I, 31C, 31F, 31I, 32C, 32F, 32I, 33C, 33F, and 33I show distortion (Y' represents the image height).
TABLE 1______________________________________Construction Data of Example 1 f = 5.1.about.12.0.about.29.5 FNO = 2.47.about.2.88.about.3.5______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 43.996 d1 = 0.800 N1 = 1.83350 .nu.1 = 21.00 r2 = 21.914 d2 = 3.302 N2 = 1.60311 .nu.2 = 60.74 r3 = -73.535 d3 = 0.100 r4 = 13.657 d4 = 1.660 N3 = 1.71300 .nu.3 = 53.93 r5 = 22.983 d5 = 0.500.about.6.229.about.10.540 r6 = 23.565 d6 = 0.650 N4 = 1.77250 .nu.4 = 49.77 r7 = 5.746 d7 = 3.043 r8* = -7.343 d8 = 0.700 N5 = 1.77250 .nu.5 = 49.77 r9 = 8.300 d9 = 1.434 N6 = 1.84666 .nu.6 = 23.82 r10* = -31.736 d10 = 10.540.about.4.811.about.0.500 r11 = .infin. d11 = 0.500 (Aperture Stop S) r12* = 10.624 d12 = 1.643 N7 = 1.69680 .nu.7 = 56.47 r13 = -28.755 d13 = 0.600 N8 = 1.84666 .nu.8 = 23.82 r14* = 45.584 d14 = 5.020.about.2.671.about.0.200 r15 = 6.982 d15 = 2.727 N9 = 1.68828 .nu.9 = 52.89 r16 = 118.458 d16 = 0.100 r17 = 10.853 d17 = 1.772 N10 = 1.48749 .nu.10 = 70.44 r18 = -61.268 d18 = 0.100 r19* = -611.273 d19 = 1.000 N11 = 1.84666 .nu.11 = 23.82 r20* = 10.062 d20 = 1.000.about.3.349.about.5.820 r21 = .infin. d21 = 3.400 N12 = 1.51680 .nu.12 = 64.20 r22 = .infin.[Aspherical Data of Eighth Surface (r8)] .epsilon. = 1.0000 A4 = 0.58736 .times. 10.sup.-3 A6 = -0.37613 .times. 10.sup.-4 A8 = 0.15455 .times. 10.sup.-5 [Aspherical Data of Tenth Surface (r10)] .epsilon. = 1.0000 A4 = 0.27038 .times. 10.sup.-3 A6 = -0.12672 .times. 10.sup.-4 A8 = -0.52313 .times. 10.sup.-6 A10 = 0.83144 .times. 10.sup.-7 [Aspherical Data of Twelfth Surface (r12)] .epsilon. = 1.0000 A4 = -0.10024 .times. 10.sup.-3 A6 = 0.22829 .times. 10.sup.-4 A8 = -0.38887 .times. 10.sup.-5 A10 = 0.24924 .times. 10.sup.-6 [Aspherical Data of Fourteenth Surface (r14)] .epsilon. = 1.0000 A4 = 0.79577 .times. 10.sup.-4 A6 = 0.83193 .times. 10.sup.-5 A8 = -0.12804 .times. 10.sup.-5 A10 = 0.89044 .times. 10.sup.-7 [Aspherical Data of Nineteenth Surface (r19)] .epsilon. = 1.0000 A4 = 0.10674 .times. 10.sup.-2 A6 = -0.83586 .times. 10.sup.-4 A8 = 0.11200 .times. 10.sup.-5 [Aspherical Data of Twentieth Surface (r20)] .epsilon. = 1.0000 A4 = 0.29367 .times. 10.sup.-2 A6 = -0.32238 .times. 10.sup.-4 A8 = 0.24911 .times. 10.sup.-5 [Values of Condition (6) on Eighth Surface (r8)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00015 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00218 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00985 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.02713 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.05890 [Values of Condition (6) on Tenth Surface (r10)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00018 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00273 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.01263 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.03506 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.07505 [Values of Condition (7) on Nineteenth Surface (r19)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.01309 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00325 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.35412 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.96012 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.95819 [Values of Condition (7) on Twentieth Surface (r20)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00037 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00580 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.02900 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.09082 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.22259______________________________________
TABLE 2______________________________________Construction Data of Example 2 f = 5.3.about.9.2.about.15.3 FNO = 3.8.about.3.95.about.4.1______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 15.662 d1 = 0.750 N1 = 1.84666 .nu.1 = 23.82 r2 = 9.499 d2 = 0.176 r3 = 9.726 d3 = 2.869 N2 = 1.77250 .nu.2 = 49.77 r4 = 1208.226 d4 = 0.600.about.4.439.about.7.518 r5 = -173.591 d5 = 0.550 N3 = 1.77250 .nu.3 = 49.77 r6 = 6.399 d6 = 1.275 r7* = -40.319 d7 = 0.600 N4 = 1.77250 .nu.4 = 49.77 r8* = 6.348 d8 = 0.116 r9 = 7.236 d9 = 1.313 N5 = 1.84666 .nu.5 = 23.82 r10 = 70.504 d10 = 7.418.about.3.578.about.0.500 r11 = .infin. d11 = 0.500 (Aperture Stop S) r12* = 2.954 d12 = 1.299 N6 = 1.77250 .nu.6 = 49.77 r13 = 6.854 d13 = 0.500 N7 = 1.84666 .nu.7 = 23.82 r14* = 3.296 d14 = 3.142.about.2.287.about.1.757 r15* = 5.968 d15 = 2.100 N8 = 1.51728 .nu.8 = 69.43 r16* = -5.999 d16 = 0.138 r17 = -5.519 d17 = 0.600 N9 = 1.80518 .nu.9 = 25.43 r18 = -8.350 d18 = 1.206.about.2.061.about.2.591 r19 = .infin. d19 = 3.400 N10 = 1.51680 .nu.10 = 64.20 r20 = .infin.[Aspherical Data of Seventh Surface (r7)] .epsilon. = 1.0000 A4 = -0.13314 .times. 10.sup.-2 A6 = 0.12578 .times. 10.sup.-3 A8 = -0.29071 .times. 10.sup.-5 [Aspherical Data of Eighth Surface (r8)] .epsilon. = 1.0000 A4 = -0.19343 .times. 10.sup.-2 A6 = 0.11548 .times. 10.sup.-3 A8 = -0.18660 .times. 10.sup.-5 [Aspherical Data of Twelfth Surface (r12)] .epsilon. = 1.0000 A4 = -0.87387 .times. 10.sup.-3 A6 = -0.76491 .times. 10.sup.-3 A8 = 0.44346 .times. 10.sup.-3 A10 = -0.83383 .times. 10.sup.-4 [Aspherical Data of Fourteenth Surface (r14)] .epsilon. = 1.0000 A4 = 0.29659 .times. 10.sup.-2 A6 = -0.86284 .times. 10.sup.-4 A8 = 0.62922 .times. 10.sup.-3 A10 = -0.91345 .times. 10.sup.-4 [Aspherical Data of Fifteenth Surface (r15)] .epsilon. = 1.0000 A4 = -0.17705 .times. 10.sup.-2 A6 = -0.10599 .times. 10.sup.-3 A8 = -0.16088 .times. 10.sup.-4 A10 = 0.23640 .times. 10.sup.-5 A12 = -0.28239 .times. 10.sup.-6 [Aspherical Data of Sixteenth Surface (r16)] .epsilon. = 1.0000 A4 = 0.69986 .times. 10.sup.-3 A6 = -0.68554 .times. 10 .sup.-4 A8 = -0.16895 .times. 10 .sup.-4 [Values of Condition (6) on Seventh Surface (r7)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00115 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.01671 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.07146 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.17348 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.28312 [Values of Condition (6) on Eighth Surface (r8)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.00019 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.00294 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.01365 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.03805 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.07816 [Values of Condition (7) on Fifteenth Surface (r15)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00016 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00272 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.01511 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.05492 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.16599 [Values of Condition (7) on Sixteenth Surface (r16)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00017 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00233 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00813 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00220 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.09842______________________________________
TABLE 3______________________________________Construction Data of Example 3 f = 5.1.about.16.0.about.48.9 FNO = 2.2.about.2.7.about.4.1______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 47.735 d1 = 0.800 N1 = 1.84666 .nu.1 = 23.82 r2 = 23.658 d2 = 3.072 N2 = 1.59286 .nu.2 = 59.50 r3 = -113.204 d3 = 0.100 r4 = 16.286 d4 = 2.151 N3 = 1.49310 .nu.3 = 83.58 r5 = 52.129 d5 = 0.500.about.9.086.about.13.505 r6 = 32.852 d6 = 0.650 N4 = 1.77250 .nu.4 = 49.77 r7 = 7.245 d7 = 2.565 r8* = -8.386 d8 = 0.700 N5 = 1.77250 .nu.5 = 49.77 r9 = 6.514 d9 = 1.860 N6 = 1.84666 .nu.6 = 23.82 r10* = -67.944 d10 = 13.505.about.4.919.about.0.500 r11 = .infin. d11 = 0.500 (Aperture Stop S) r12* = 8.994 d12 = 1.803 N7 = 1.70490 .nu.7 = 53.41 r13 = -757.679 d13 = 0.600 N8 = 1.84666 .nu.8 = 23.82 r14* = 16.350 d14 = 9.617.about.5.891.about.0.200 r15 = 6.901 d15 = 2.778 N9 = 1.48749 .nu.9 = 70.44 r16 = 42.197 d16 = 0.100 r17 = 7.060 d17 = 2.808 N10 = 1.48749 .nu.10 = 70.44 r18 = -25.612 d18 = 0.100 r19* = 68.296 d19 = 2.499 N11 = 1.84922 .nu.11 = 34.59 r20* = 6.757 d20 = 1.000.about.4.726.about.10.417 r21 = .infin. d21 = 3.400 N12 = 1.51680 .nu.12 = 64.20 r22 = .infin.[Aspherical Data of Eighth Surface (r8)] .epsilon. = 1.0000 A4 = 0.87732 .times. 10.sup.-3 A6 = -0.13530 .times. 10.sup.-4 A8 = 0.31574 .times. 10.sup.-6 [Aspherical Data of Tenth Surface (r10)] .epsilon. = 1.0000 A4 = 0.58793 .times. 10.sup.-3 A6 = -0.47078 .times. 10.sup.-5 A8 = -0.25169 .times. 10.sup.-6 A10 = 0.18773 .times. 10.sup.-7 [Aspherical Data of Twelfth Surface (r12)] .epsilon. = 1.0000 A4 = -0.17364 .times. 10.sup.-3 A6 = 0.14615 .times. 10.sup.-4 A8 = -0.13173 .times. 10.sup.-5 A10 = 0.54342 .times. 10.sup.-7 [Aspherical Data of Fourteenth Surface (r14)] .epsilon. = 1.0000 A4 = -0.44606 .times. 10.sup.-4 A6 = 0.17082 .times. 10.sup.-4 A8 = -0.15023 .times. 10.sup.-5 A10 = 0.64066 .times. 10.sup.-7 [Aspherical Data of Nineteenth Surface (r19)] .epsilon. = 1.0000 A4 = -0.12211 .times. 10.sup.-2 A6 = 0.11329 .times. 10.sup.-4 A8 = -0.12342 .times. 10.sup.-6 [Aspherical Data of Twentieth Surface (r20)] .epsilon. = 1.0000 A4 = -0.91492 .times. 10.sup.-4 A6 = 0.58137 .times. 10.sup.-4 A8 = 0.11083 .times. 10.sup.-5 [Values of Condition (6) on Eighth Surface (r8)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00050 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00787 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.03833 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.11575 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.27118 [Values of Condition (6) on Tenth Surface (r10)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00171 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.02696 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.13328 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.40716 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.961251 [Values of Condition (7) on Nineteenth Surface (r19)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00298 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.04686 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.23111 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.25716 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.14946 [Values of Condition (7) on Twentieth Surface (r20)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00000 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00000 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00000 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00082 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00665 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.03019______________________________________
TABLE 4______________________________________Construction Data of Example 4 f = 5.1.about.12.0.about.29.5 FNO = 2.9.about.3.38.about.4.1______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 43.378 d1 = 0.800 N1 = 1.83350 .nu.1 = 21.00 r2 = 21.278 d2 = 3.321 N2 = 1.60311 .nu.2 = 60.74 r3 = -69.047 d3 = 0.100 r4 = 13.046 d4 = 1.674 N3 = 1.71300 .nu.3 = 53.93 r5 = 22.328 d5 = 0.500.about.5.897.about.9.983 r6 = 22.712 d6 = 0.650 N4 = 1.77250 .nu.4 = 49.77 r7 = 5.535 d7 = 2.790 r8* = -7.538 d8 = 0.700 N5 = 1.77250 .nu.5 = 49.77 r9 = 7.065 d9 = 1.428 N6 = 1.84666 .nu.6 = 23.82 r10* = -50.971 d10 = 9.983.about.4.586.about.0.500 r11 = .infin. d11 = 0.500 (Aperture Stop S) r12* = 11.185 d12 = 1.630 N7 = 1.69680 .nu.7 = 56.47 r13 = -17.692 d13 = 0.600 N8 = 1.84666 .nu.8 = 23.82 r14* = 325.535 d14 = 5.144.about.2.684.about.0.200 r15 = 5.637 d15 = 3.627 N9 = 1.62280 .nu.9 = 56.88 r16 = -21.578 d16 = 0.509 r17* = 116.000 d17 = 1.000 N10 = 1.84666 .nu.10 = 23.82 r18* = 9.196 d18 = 1.000.about.3.459.about.5.944 r19 = .infin. d19 = 3.400 N11 = 1.51680 .nu.11 = 64.20 r20 = .infin.[Aspherical Data of Eighth Surface (r8)] .epsilon. = 1.0000 A4 = 0.40767 .times. 10.sup.-3 A6 = -0.34613 .times. 10.sup.-4 A8 = 0.14147 .times. 10.sup.-5 [Aspherical Data of Tenth Surface (r10)] .epsilon. = 1.0000 A4 = 0.18081 .times. 10.sup.-3 A6 = -0.94386 .times. 10.sup.-5 A8 = -0.46661 .times. 10.sup.-6 A10 = 0.79702 .times. 10.sup.-7 [Aspherical Data of Twelfth Surface (r12)] .epsilon. = 1.0000 A4 = 0.27751 .times. 10.sup.-4 A6 = -0.29005 .times. 10.sup.-4 A8 = 0.58934 .times. 10.sup.-5 A10 = -0.42363 .times. 10.sup.-6 [Aspherical Data of Fourteenth Surface (r14)] .epsilon. = 1.0000 A4 = 0.11060 .times. 10.sup.-3 A6 = -0.37336 .times. 10.sup.-5 A8 = 0.53196 .times. 10.sup.-7 A10 = 0.36713 .times. 10.sup.-7 [Aspherical Data of Seventeenth Surface (r17)] .epsilon. = 1.0000 A4 = -0.65248 .times. 10.sup.-3 A6 = -0.17220 .times. 10.sup.-4 A8 = -0.18944 .times. 10.sup.-5 [Aspherical Data of Eighteenth Surface (r18)] .epsilon. = 1.0000 A4 = 0.14749 .times. 10.sup.-2 A6 = 0.60592 .times. 10.sup.-4 A8 = 0.94892 .times. 10.sup.-6 [Values of Condition (12) on Eighth Surface (r8)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00001 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00009 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00044 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00133 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00305 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00584 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00987 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.01525 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.02209 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.03074 [Values of Condition (12) on Tenth Surface (r10)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00001 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00018 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00088 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00270 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00633 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.01246 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.02165 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.03437 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.05118 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.07356 [Values of Condition (13) 0n Seventeenth Surface (r17)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00008 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00135 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00695 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.02250 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.05690 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.12379 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.24412 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.20652 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.03851 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.32291 [Values of Condition (13) on Eighteenth Surface (r18)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00001 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00015 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00076 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00247 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00621 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.01337 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.02585 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.04632 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.07838 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.12686______________________________________
TABLE 5______________________________________Construction Data of Example 5 f = 5.1.about.16.0.about.48.8 FNO = 2.4.about.3.0.about.4.1______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 53.056 d1 = 0.800 N1 = 1.84666 .nu.1 = 23.82 r2 = 27.610 d2 = 4.290 N2 = 1.72579 .nu.2 = 52.59 r3 = -748.094 d3 = 0.100 r4 = 20.898 d4 = 2.420 N3 = 1.49310 .nu.3 = 83.58 r5 = 47.005 d5 = 0.500.about.11.370.about.17.892 r6 = 21.952 d6 = 0.650 N4 = 1.77250 .nu.4 = 49.77 r7 = 7.817 d7 = 5.500 r8* = -9.045 d8 = 0.700 N5 = 1.77250 .nu.5 = 49.77 r9 = 9.919 d9 = 1.784 N6 = 1.84666 .nu.6 = 23.82 r10* = -53.111 d10 = 17.892.about.7.023.about.0.500 r11 = .infin. d11 = 0.500 (Aperture Stop S) r12* = 12.961 d12 = 1.642 N7 = 1.75450 .nu.7 = 51.57 r13 = -90.941 d13 = 0.600 N8 = 1.84666 .nu.8 = 23.82 r14* = 30.925 d14 = 7.976.about.4.481.about.0.200 r15 = 6.170 d15 = 4.342 N9 = 1.54762 .nu.9 = 63.26 r16 = -20.156 d16 = 0.100 r17* = 78.855 d17 = 1.154 N10 = 1.84879 .nu.10 = 32.11 r18* = 8.123 d18 = 0.231 r19 = 5.787 d19 = 3.589 N11 = 1.48749 .nu.11 = 70.44 r20 = 6.522 d20 = 1.311.about.4.806.about.9.087 r21 = .infin. d21 = 3.400 N12 = 1.51680 .nu.12 = 64.20 r22 = .infin.[Aspherical Data of Eighth Surface (r8)] .epsilon. = 1.0000 A4 = 0.54279 .times. 10.sup.-3 A6 = -0.15745 .times. 10.sup.-4 A8 = 0.33159 .times. 10.sup.-6 [Aspherical Data of Tenth Surface (r10)] .epsilon. = 1.0000 A4 = 0.30792 .times. 10.sup.-3 A6 = -0.76564 .times. 10.sup.-5 A8 = -0.42745 .times. 10.sup.-7 A10 = 0.76414 .times. 10.sup.-8 [Aspherical Data of Twelfth Surface (r12)] .epsilon. = 1.0000 A4 = -0.96656 .times. 10.sup.-4 A6 = 0.19736 .times. 10.sup.-4 A8 = -0.19467 .times. 10.sup.-5 A10 = 0.74168 .times. 10.sup.-7 [Aspherical Data of Fourteenth Surface (r14)] .epsilon. = 1.0000 A4 = -0.15998 .times. 10.sup.-4 A6 = 0.14448 .times. 10.sup.-4 A8 = -0.12448 .times. 10.sup.-5 A10 = 0.45183 .times. 10.sup.-7 [Aspherical Data of Seventeenth Surface (r17)] .epsilon. = 1.0000 A4 = 0.16025 .times. 10.sup.-3 A6 = -0.26009 .times. 10.sup.-4 A8 = -0.35539 .times. 10.sup.-6 [Aspherical Data of Eighteenth Surface (r18)] .epsilon. = 1.0000 A4 = 0.15014 .times. 10.sup.-2 A6 = 0.57682 .times. 10.sup.-5 A8 = 0.15747 .times. 10.sup.-5 [Values of Condition (12) on Eighth Surface (r8)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00003 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00050 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00247 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00752 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.01753 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.03446 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.06021 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.09678 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.14675 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.21437 [Values of Condition (12) on Tenth Surface (r10)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00007 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00115 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00570 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.01748 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.04099 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.08084 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.14110 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.22524 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.33726 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.48552 [Values of Condition (13) on Seventeenth Surface (r17)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00002 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00032 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00139 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00346 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00537 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00308 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.01269 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.05952 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.16762 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.38533 [Values of Condition (13) on Eighteenth Surface (r18)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00001 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00020 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00099 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00315 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00775 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.01628 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.03072 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.05375 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.08910 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.14192______________________________________
TABLE 6______________________________________Construction Data of Example 6 f = 5.3.about.9.2.about.15.3 FNO = 3.75.about.3.9.about.4.1______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 13.020 d1 = 0.750 N1 = 1.84666 .nu.1 = 23.82 r2 = 7.963 d2 = 0.269 r3 = 8.178 d3 = 3.014 N2 = 1.77250 .nu.2 = 49.77 r4 = 155.044 d4 = 0.600.about.3.950.about.6.618 r5 = 806.822 d5 = 0.550 N3 = 1.77250 .nu.3 = 49.77 r6 = 5.025 d6 = 1.349 r7* = -20.229 d7 = 0.600 N4 = 1.77250 .nu.4 = 49.77 r8* = 6.666 d8 = 0.105 r9 = 7.156 d9 = 1.260 N5 = 1.84666 .nu.5 = 23.82 r10 = .infin. d10 = 6.518.about.3.168.about.0.500 r11 = .infin. d11 = 0.500 (Aperture Stop S) r12* = 3.179 d12 = 1.428 N6 = 1.77250 .nu.6 = 49.77 r13 = 10.090 d13 = 0.519 N7 = 1.84666 .nu.7 = 23.82 r14* = 3.914 d14 = 3.328.about.2.360.about.1.783 r15* = 6.243 d15 = 3.000 N8 = 1.51728 .nu.= 69.43 r16* = -5.478 d16 = 0.100 r17 = -12.214 d17 = 0.600 N9 = 1.70146 .nu.9 = 27.28 r18 = 715.610 d18 = 0.600.about.1.568.about.2.145 r19 = .infin. d19 = 3.400 N10 = 1.51680 .nu.10 = 64.20 r20 = .infin.[Aspherical Data of Seventh Surface (r7)] .epsilon. = 1.0000 A4 = -0.93462 .times. 10.sup.-3 A6 = 0.16333 .times. 10.sup.-3 A8 = -0.62263 .times. 10.sup.-5 [Aspherical Data of Eighth Surface (r8)] .epsilon. = 1.0000 A4 = -0.15378 .times. 10.sup.-2 A6 = 0.15463 .times. 10.sup.-3 A8 = -0.57430 .times. 10.sup.-5 [Aspherical Data of Twelfth Surface (r12)] .epsilon. = 1.0000 A4 = -0.36978 .times. 10.sup.-3 A6 = -0.50889 .times. 10.sup.-3 A8 = 0.31290 .times. 10.sup.-3 A10 = -0.55754 .times. 10.sup.-4 [Aspherical Data of Fourteenth Surface (r14)] .epsilon. = 1.0000 A4 = 0.37389 .times. 10.sup.-2 A6 = -0.10426 .times. 10.sup.-3 A8 = 0.55997 .times. 10.sup.-3 A10 = -0.81568 .times. 10.sup.-4 [Aspherical Data of Fifteenth Surface (r15)] .epsilon. = 1.0000 A4 = -0.27883 .times. 10.sup.-2 A6 = -0.13786 .times. 10.sup.-3 A8 = -0.30248 .times. 10.sup.-4 A10 = 0.54205 .times. 10.sup.-5 A12 = -0.57990 .times. 10.sup.-6 [Aspherical Data of Sixteenth Surface (r16)] .epsilon. = 1.0000 A4 = 0.81443 .times. 10.sup.-3 A6 = -0.14194 .times. 10.sup.-3 A8 = -0.80358 .times. 10.sup.-5 [Values of Condition (12) on Seventh Surface (r7)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00003 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00050 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00234 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00659 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.01371 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.02284 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.03126 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.03425 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.02580 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00051 [Values of Condition (12) on Eighth Surface (r8)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.00001 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.00021 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.00102 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.00307 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.00699 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.01333 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.02231 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.03384 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.04750 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = -0.06281 [Values of Condition (13) on Fifteenth Surface (r15)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00001 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00019 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00097 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00315 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00793 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.01712 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.03330 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.06021 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.10340 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.17192 [Values of Condition (13) on Sixteenth Surface (r16)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00001 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00009 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00043 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00118 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00234 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00336 Y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00268 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00304 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.02000 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.05877______________________________________
TABLE 7______________________________________Construction Data of Example 7 f = 5.1.about.12.0.about.29.5 FNO = 2.1.about.2.44.about.2.88______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 58.305 d1 = 0.800 N1 = 1.84666 .nu.1 = 23.82 r2 = 23.626 d2 = 3.907 N2 = 1.70986 .nu.2 = 53.21 r3 = -111.097 d3 = 0.100 r4 = 16.699 d4 = 1.803 N3 = 1.71897 .nu.3 = 52.85 r5 = 26.234 d5 = 0.500.about.7.841.about.13.405 r6 = 23.840 d6 = 0.650 N4 = 1.77250 .nu.4 = 49.77 r7 = 6.746 d7 = 4.365 r8* = -7.561 d8 = 0.700 N5 = 1.77250 .nu.5 = 49.77 r9 = 13.086 d9 = 1.508 N6 = 1.84666 .nu.6 = 23.82 r10* = -23.505 d10 = 13.405.about.6.064.about.0.500 r11 = .infin. d11 = 0.500 (Aperture Stop S) r12* = 14.624 d12 = 1.699 N7 = 1.75450 .nu.7 = 51.57 r13 = -33.093 d13 = 0.600 N8 = 1.84666 .nu.8 = 23.82 r14* = 63.509 d14 = 4.485.about.2.327.about.0.200 r15 = 6.186 d15 = 4.237 N9 = 1.67350 .nu.9 = 48.38 r16 = -20.662 d16 = 0.116 r17* = -55.968 d17 = 1.000 N10 = 1.84666 .nu.10 = 23.82 r18* = 8.991 d18 = 1.261 r19 = 11.736 d19 = 1.326 N11 = 1.48749 .nu.11 = 70.44 r20 = 46.541 d20 = 1.669.about.3.827.about.5.954 r21 = .infin. d21 = 3.400 N12 = 1.51680 .nu.12 = 64.20 r22 = .infin.[Aspherical Data of Eighth Surface (r8)] .epsilon. = 1.0000 A4 = 0.66406 .times. 10.sup.-3 A6 = -0.22116 .times. 10.sup.-4 A8 = 0.63051 .times. 10.sup.-6 [Aspherical Data of Tenth Surface (r10)] .epsilon. = 1.0000 A4 = 0.30803 .times. 10.sup.-3 A6 = -0.87997 .times. 10.sup.-5 A8 = -0.19583 .times. 10.sup.-6 A10 = 0.19600 .times. 10.sup.-7 [Aspherical Data of Twelfth Surface (r12)] .epsilon. = 1.0000 A4 = -0.16926 .times. 10.sup.-3 A6 = 0.12252 .times. 10.sup.-4 A8 = -0.13532 .times. 10.sup.-5 A10 = 0.46314 .times. 10.sup.-7 [Aspherical Data of Fourteenth Surface (r14)] .epsilon. = 1.0000 A4 = -0.11449 .times. 10.sup.-3 A6 = 0.11354 .times. 10.sup.-4 A8 = -0.11571 .times. 10.sup.-5 A10 = 0.37393 .times. 10.sup.-7 [Aspherical Data of Seventeenth Surface (r17)] .epsilon. = 1.0000 A4 = 0.43509 .times. 10.sup.-3 A6 = -0.43010 .times. 10.sup.-4 A8 = 0.22007 .times. 10.sup.-6 [Aspherical Data of Eighteenth Surface (r18)] .epsilon. = 1.0000 A4 = 0.21202 .times. 10.sup.-2 A6 = -0.64354 .times. 10.sup.-6 A8 = 0.31309 .times. 10.sup.-5 [Values of Condition (12) on Eighth Surface (r8)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = 0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00002 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00029 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00144 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00442 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.01039 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.02062 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.03644 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.05926 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.09084 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline .x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.13375 [Values of Condition (12) on Tenth Surface (r10)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0(N' - N) .multidot. f2} = -0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00002 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00031 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00153 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.00471 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.01108 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.02193 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.03839 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.06136 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.09168 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f2} = 0.13106 [Values of Condition (13) on Seventeenth Surface (r17)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00003 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00047 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00226 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.00650 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.01390 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.02392 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.03372 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.03703 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = 0.02289 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.02571 [Values of Condition (13) on Eighteenth Surface (r18)] y = 0.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00000 y = 0.10 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00002 y = 0.20 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00024 y = 0.30 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00123 y = 0.40 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00391 y = 0.50 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.00959 y = 0.60 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.02004 y = 0.70 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.03762 y = 0.80 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.06549 y = 0.90 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.10794 y = 1.00 ymax . . . (.vertline.x.vertline. - .vertline.x0.vertline.)/{C0 (N' - N) .multidot. f4} = -0.17102______________________________________
TABLE 8______________________________________Construction Data of Example 8 f = 5.1.about.16.0.about.48.7 FNO = 2.8.about.3.60.about.4.10______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 33.531 d1 = 0.800 N1 = 1.84666 .nu.1 = 23.82 r2 = 24.327 d2 = 2.746 N2 = 1.49310 .nu.2 = 83.58 r3 = -368.533 d3 = 0.100 r4 = 22.561 d4 = 1.895 N3 = 1.48749 .nu.3 = 70.44 r5 = 55.959 d5 = 0.500.about.13.189.about.22.883 r6* = 58.967 d6 = 0.700 N4 = 1.77250 .nu.4 = 49.77 r7* = 7.392 d7 = 4.083 r8 = -8.182 d8 = 0.600 N5 = 1.77250 .nu.5 = 49.77 r9 = 10.789 d9 = 1.180 N6 = 1.84666 .nu.6 = 23.82 r10 = -29.369 d10 = 12.294.about.5.109.about.0.500 r11 = .infin. d11 = 0.500 (Aperture Stop S) r12* = 5.894 d12 = 1.873 N7 = 1.60647 .nu.7 = 58.56 r13* = -291.584 d13 = 0.100 r14 = 9.110 d14 = 0.500 N8 = 1.84666 .nu.8 = 23.82 r15 = 5.333 d15 = 5.668.about.1.785.about.0.200 r16 = 5.057 d16 = 2.915 N9 = 1.48749 .nu.9 = 70.44 r17 = -20.386 d17 = 0.100 r18* = 7.187 d18 = 0.720 N10 = 1.84722 .nu.10 = 40.27 r19* = 3.624 d19 = 0.500 r20 = 4.906 d20 = 2.360 N11 = 1.48749 .nu.11 = 70.44 r21 = 6.236 d21 = 1.164.about.5.047.about.6.632 r22 = .infin. d22 = 3.400 N12 = 1.51680 .nu.12 = 64.20 r23 = .infin.[Aspherical Data of Sixth Surface (r6)] .epsilon. = 1.0000 A4 = 0.24880 .times. 10.sup.-3 A6 = 0.69912 .times. 10.sup.-5 A8 = -0.12045 .times. 10.sup.-6 [Aspherical Data of Seventh Surface (r7)] .epsilon. = 1.0000 A4 = 0.19486 .times. 10.sup.-3 A6 = 0.16546 .times. 10.sup.-4 A8 = 0.68213 .times. 10.sup.-6 [Aspherical Data of Twelfth Surface (r12)] .epsilon. = 1.0000 A4 = -0.63905 .times. 10.sup.-3 A6 = -0.20691 .times. 10.sup.-4 A8 = 0.38158 .times. 10.sup.-7 A10 = -0.16639 .times. 10.sup.-6 [Aspherical Data of Thirteenth Surface (r13)] .epsilon. = 1.0000 A4 = -0.28812 .times. 10.sup.-3 A6 = -0.69833 .times. 10.sup.-5 A8 = -0.13085 .times. 10.sup.-5 A10 = -0.95789 .times. 10.sup.-7 [Aspherical Data of Eighteenth Surface (r18)] .epsilon. = 1.0000 A4 = -0.47322 .times. 10.sup.-2 A6 = 0.17987 .times. 10 .sup.-3 A8 = -0.10821 .times. 10.sup.-4 A10 = 0.28645 .times. 10.sup.-6 [Aspherical Data of Nineteenth Surface (r19)] .epsilon. = 1.0000 A4 = -0.53795 .times. 10.sup.-2 A6 = 0.20587 .times. 10.sup.-3 A8 = -0.14591 .times. 10.sup.-4 [Values of Condition (17) on Sixth Surface (r6)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00106 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.01900 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.10847 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.36418 [Values of Condition (17) on Seventh Surface (r7)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00032 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00661 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.05024 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.25799 [Values of Condition (18) on Twelfth Surface (r12)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00025 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00414 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.02287 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.08500 [Values of Condition (18) on Thirteenth Surface (r13)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00011 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.00179 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.01032 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.04267 [Values of Condition (19) on Eighteenth Surface (r18)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00222 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.03335 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.15571 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.45732 [Values of Condition (19) on Nineteenth Surface (r19)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00157 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.02395 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.11457 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.35603______________________________________
TABLE 9______________________________________Construction Data of Example 9 f = 5.1.about.16.0.about.48.7 FNO = 2.82.about.3.63.about.4.10______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 33.825 d1 = 0.800 N1 = 1.84666 .nu.1 = 23.82 r2 = 24.649 d2 = 2.772 N2 = 1.49310 .nu.2 = 83.58 r3 = -463.265 d3 = 0.100 r4 = 22.909 d4 = 1.910 N3 = 1.48749 .nu.3 = 70.44 r5 = 55.909 d5 = 0.500.about.13.310.about.23.516 r6* = 69.207 d6 = 0.700 N4 = 1.77250 .nu.4 = 49.77 r7* = 8.157 d7 = 3.891 r8 = -7.863 d8 = 0.600 N5 = 1.77250 .nu.5 = 49.77 r9 = 11.112 d9 = 0.137 r10 = 12.158 d10 = 1.142 N6 = 1.84666 .nu.6 = 23.82 r11 = -26.794 d11 = 12.670.about.5.178.about.0.500 r12 = .infin. d12 = 0.500 (Aperture Stop S) r13* = 5.800 d13 = 1.862 N7 = 1.59148 .nu.7 = 59.60 r14* = 796.451 d14 = 0.100 r15 = 8.439 d15 = 0.500 N8 = 1.84666 .nu.8 = 23.82 r16 = 5.171 d16 = 5.590.about.1.650.about.0.200 r17 = 5.002 d17 = 2.912 N9 = 1.48749 .nu.9 = 70.44 r18 = -19.633 d18 = 0.100 r19* = 7.476 d19 = 0.720 N10 = 1.84963 .nu.10 = 40.07 r20* = 3.658 d20 = 0.500 r21 = 4.899 d21 = 2.295 N11 = 1.49659 .nu.11 = 68.88 r22 = 6.256 d22 = 1.180.about.5.120.about.6.570 r23 = .infin. d23 = 3.400 N12 = 1.51680 .nu.12 = 64.20 r24 = .infin.[Aspherical Data of Sixth Surface (r6)] .epsilon. = 1.0000 A4 = 0.34989 .times. 10.sup.-3 A6 = 0.29550 .times. 10.sup.-5 A8 = -0.39655 .times. 10.sup.-7 [Aspherical Data of Seventh Surface (r7)] .epsilon. = 1.0000 A4 = 0.26226 .times. 10.sup.-3 A6 = 0.12936 .times. 10.sup.-4 A8 = 0.40863 .times. 10.sup.-6 [Aspherical Data of Thirteenth Surface (r13)] .epsilon. = 1.0000 A4 = -0.64004 .times. 10.sup.-3 A6 = -0.20905 .times. 10.sup.-4 A8 = 0.14240 .times. 10.sup.-6 A10 = -0.17189 .times. 10.sup.-6 [Aspherical Data of Fourteenth Surface (r14)] .epsilon. = 1.0000 A4 = -0.30103 .times. 10.sup.-3 A6 = -0.74213 .times. 10.sup.-5 A8 = -0.10894 .times. 10.sup.-5 A10 = -0.10624 .times. 10.sup.-6 [Aspherical Data of Nineteenth Surface (r19)] .epsilon. = 1.0000 A4 = -0.47646 .times. 10.sup.-2 A6 = 0.18766 .times. 10.sup.-3 A8 = -0.10271 .times. 10.sup.-4 A10 = 0.22819 .times. 10.sup.-6 [Aspherical Data of Twentieth Surface (r20)] .epsilon. = 1.0000 A4 = -0.53163 .times. 10.sup.-2 A6 = 0.22027 .times. 10.sup.-3 A8 = -0.13269 .times. 10.sup.-4 [Values of Condition (17) on Sixth Surface (r6)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00153 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.02548 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.13541 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.44412 [Values of Condition (17) on Seventh Surface (r7)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00047 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00894 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.06020 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.27574 [Values of Condition (18) on Thirteenth Surface (r13)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00026 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00432 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.02382 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.08851 [Values of Condition (18) on Fourteenth Surface (r14)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00011 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.00192 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.01094 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.04456 [Values of Condition (19) on Nineteenth Surface (r19)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00224 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.03347 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.15514 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.45265 [Values of Condition (19) on Twentieth Surface (r20)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00156 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.02354 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.11104 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.33662______________________________________
TABLE 10______________________________________Construction Data of Example 10 f = 5.1.about.16.0.about.48.9 FNO = 2.5.about.3.10.about.4.10______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 42.418 d1 = 0.800 N1 = 1.84823 .nu.1 = 29.42 r2 = 23.948 d2 = 3.442 N2 = 1.48749 .nu.2 = 70.44 r3 = -157.257 d3 = 0.100 r4 = 19.745 d4 = 2.460 N3 = 1.49310 .nu.3 = 83.58 r5 = 71.793 d5 = 0.500.about.13.232.about.20.307 r6 = 25.259 d6 = 0.650 N4 = 1.77250 .nu.4 = 49.77 r7 = 6.903 d7 = 3.256 r8* = -8.565 d8 = 0.700 N5 = 1.77250 .nu.5 = 49.77 r9 = 7.817 d9 = 1.712 N6 = 1.84666 .nu.6 = 23.82 r10* = -51.478 d10 = 12.722.about.5.490.about.0.500 r11 = .infin. d11 = 0.500 (Aperture Stop S) r12* = 8.881 d12 = 1.710 N7 = 1.75106 .nu.7 = 51.69 r13 = -447.355 d13 = 0.600 N8 = 1.84666 .nu.8 = 23.82 r14* = 15.336 d14 = 6.807.about.3.687.about.0.200 r15 = 6.974 d15 = 2.615 N9 = 1.48749 .nu.9 = 70.44 r16 = 74.803 d16 = 0.100 r17 = 7.833 d17 = 3.107 N10 = 1.48749 .nu.10 = 70.44 r18 = -16.439 d18 = 0.125 r19* = -89.359 d19 = 2.269 N11 = 1.84951 .nu.11 = 38.38 r20* = 8.210 d20 = 1.000.about.4.120.about.7.607 r21 = .infin. d21 = 3.400 N12 = 1.51680 .nu.12 = 64.20 r22 = .infin.[Aspherical Data of Eighth Surface (r8)] .epsilon. = 1.0000 A4 = 0.70923 .times. 10.sup.-3 A6 = -0.16701 .times. 10.sup.-4 A8 = 0.44246 .times. 10.sup.-6 [Aspherical Data of Tenth Surface (r10)] .epsilon. = 1.0000 A4 = 0.42937 .times. 10.sup.-3 A6 = -0.62961 .times. 10.sup.-5 A8 = -0.22968 .times. 10.sup.-6 A10 = 0.19206 .times. 10.sup.-7 [Aspherical Data of Twelfth Surface (r12)] .epsilon. = 1.0000 A4 = -0.22084 .times. 10.sup.-3 A6 = 0.24082 .times. 10.sup.-4 A8 = -0.30206 .times. 10.sup.-5 A10 = 0.14784 .times. 10.sup.-6 [Aspherical Data of Fourteenth Surface (r14)] .epsilon. = 1.0000 A4 = -0.67988 .times. 10.sup.-4 A6 = 0.23632 .times. 10.sup.-4 A8 = -0.28969 .times. 10.sup.-5 A10 = 0.14902 .times. 10.sup.-6 [Aspherical Data of Nineteenth Surface (r19)] .epsilon. = 1.0000 A4 = -0.13544 .times. 10.sup.-2 A6 = 0.13398 .times. 10.sup.-4 A8 = -0.21612 .times. 10.sup.-6 [Aspherical Data of Twentieth Surface (r20)] .epsilon. = 1.0000 A4 = -0.58348 .times. 10.sup.-4 A6 = 0.59161 .times. 10.sup.-4 A8 = -0.48072 .times. 10.sup.-6 [Values of Condition (17) on Eighth Surface (r8)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00077 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.01161 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.05406 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.15895 [Values of Condition (17) on Tenth Surface (r10)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00028 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00428 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.02026 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.05928 [Values of Condition (18) on Twelfth Surface (r12)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00009 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00120 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.00531 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.01508 [Values of Condition (18) on Fourteenth Surface (r14)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00002 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.00017 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.00010 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.00179 [Values of Condition (19) on Nineteenth Surface (r19)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00101 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.01579 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.07723 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.23431 [Values of Condition (19) on Twentieth Surface (r20)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00001 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00042 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.00673 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.04052______________________________________
TABLE 11______________________________________Construction Data of Example 11 f = 5.1.about.16.0.about.48.7 FNO = 2.9.about.3.74.about.4.10______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 34.217 d1 = 0.800 N1 = 1.84666 .nu.1 = 23.82 r2 = 24.902 d2 = 2.968 N2 = 1.49310 .nu.2 = 83.58 r3 = -395.465 d3 = 0.100 r4 = 23.286 d4 = 2.048 N3 = 1.48749 .nu.3 = 70.44 r5 = 58.161 d5 = 0.500.about.12.971.about.23.475 r6* = 83.573 d6 = 0.700 N4 = 1.77250 .nu.4 = 49.77 r7* = 9.371 d7 = 3.909 r8 = -7.275 d8 = 0.600 N5 = 1.77250 .nu.5 = 49.77 r9 = 9.509 d9 = 0.165 r10 = 10.889 d10 = 1.166 N6 = 1.84666 .nu.6 = 23.82 r11 = -29.625 d11 = 12.284.about.4.883.about.0.500 r12 = .infin. d12 = 0.500 (Aperture Stop S) r13* = 5.757 d13 = 1.862 N7 = 1.59897 .nu.7 = 59.07 r14* = 997.208 d14 = 0.100 r15 = 8.468 d15 = 0.500 N8 = 1.84666 .nu.8 = 23.82 r16 = 5.153 d16 = 5.529.about.1.347.about.0.200 r17 = 5.837 d17 = 1.923 N9 = 1.48749 .nu.9 = 70.44 r18 = 36.246 d18 = 0.100 r19 = 5.995 d19 = 0.720 N10 = 1.84778 .nu.10 = 27.58 r20 = 4.073 d20 = 0.500 r21* = 4.261 d21 = 2.463 N11 = 1.49926 .nu.11 = 62.44 r22* = 6.138 d22 = 1.832.about.6.013.about.7.161 r23 = .infin. d23 = 3.400 N12 = 1.51680 .nu.12 = 64.20 r24 = .infin.[Aspherical Data of Sixth Surface (r6)] .epsilon. = 1.0000 A4 = 0.41216 .times. 10.sup.-3 A6 = -0.32215 .times. 10.sup.-5 A8 = 0.90023 .times. 10.sup.-7 [Aspherical Data of Seventh Surface (r7)] .epsilon. = 1.0000 A4 = 0.27744 .times. 10.sup.-3 A6 = 0.24211 .times. 10.sup.-5 A8 = 0.16608 .times. 10.sup.-6 [Aspherical Data of Thirteenth Surface (r13)] .epsilon. = 1.0000 A4 = -0.66034 .times. 10.sup.-3 A6 = -0.21659 .times. 10.sup.-4 A8 = 0.53081 .times. 10.sup.-6 A10 = -0.18714 .times. 10.sup.-6 [Aspherical Data of Fourteenth Surface (r14)] .epsilon. = 1.0000 A4 = -0.29541 .times. 10.sup.-3 A6 = -0.59954 .times. 10.sup.-5 A8 = -0.12127 .times. 10.sup.-5 A10 = -0.77251 .times. 10.sup.-7 [Aspherical Data of Twenty-first Surface (r21)] .epsilon. = 1.0000 A4 = -0.32651 .times. 10.sup.-3 A6 = -0.22504 .times. 10.sup.-4 A8 = -0.20624 .times. 10.sup.-5 A10 = -0.44963 .times. 10.sup.-6 [Aspherical Data of Twenty-second Surface (r22)] .epsilon. = 1.0000 A4 = 0.18461 .times. 10.sup.-2 A6 = 0.55914 .times. 10.sup.-4 A8 = -0.13108 .times. 10.sup.-4 A10 = -0.89500 .times. 10.sup.-7 [Values of Condition (23) on Sixth Surface (r6)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00234 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.03604 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.17875 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.59806 [Values of Condition (23) on Seventh Surface (r7)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00066 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.01114 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.06327 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.24571 [Values of Condition (24) on Thirteenth Surface (r13)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00024 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00405 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.02215 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.08057 [Values of Condition (24) on Fourteenth Surface (r14)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00011 Y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.00178 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.01005 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.04005 [Values of Condition (25) on Twenty-first Surface (r21)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00024 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00447 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.03262 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.19925 [Values of Condition (25) on Twenty-second Surface (r22)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00084 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.01370 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.06700 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.17012______________________________________
TABLE 12______________________________________Construction Data of Example 12 f = 5.1.about.16.0.about.48.7 FNO = 2.81.about.3.62.about.4.10______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 33.573 d1 = 0.800 N1 = 1.84666 .nu.1 = 23.82 r2 = 24.414 d2 = 2.746 N2 = 1.49310 .nu.2 = 83.58 r3 = -381.263 d3 = 0.100 r4 = 22.675 d4 = 1.904 N3 = 1.48749 .nu.3 = 70.44 r5 = 55.836 d5 = 0.500.about.13.356.about.23.059 r6* = 75.409 d6 = 0.700 N4 = 1.77250 .nu.4 = 49.77 r7* = 7.577 d7 = 4.153 r8 = -8.104 d8 = 0.600 N5 = 1.77250 .nu.5 = 49.77 r9 = 11.284 d9 = 1.170 N6 = 1.84666 .nu.6 = 23.82 r10 = -27.352 d10 = 12.417.about.5.161.about.0.500 r11 = .infin. d11 = 0.500 (Aperture Stop S) r12* = 5.838 d12 = 1.882 N7 = 1.60021 .nu.7 = 58.99 r13* = -368.366 d13 = 0.100 r14 = 8.835 d14 = 0.500 N8 = 1.84666 .nu.8 = 23.82 r15 = 5.247 d15 = 5.685.about.1.809.about.0.200 r16 = 5.021 d16 = 2.899 N9 = 1.48749 .nu.9 = 70.44 r17 = -19.996 d17 = 0.100 r18* = 7.465 d18 = 0.720 N10 = 1.84530 .nu.10 = 40.44 r19* = 3.677 d19 = 0.500 r20 = 4.985 d20 = 2.292 N11 = 1.48749 .nu.11 = 70.44 r21 = 6.356 d21 = 1.150.about.5.026.about.6.635 r22 = .infin. d22 = 3.400 N12 = 1.51680 .nu.12 = 64.20 r23 = .infin.[Aspherical Data of Sixth Surface (r6)] .epsilon. = 1.0000 A4 = 0.33469 .times. 10.sup.-3 A6 = 0.39659 .times. 10.sup.-5 A8 = -0.85661 .times. 10.sup.-7 [Aspherical Data of Seventh Surface (r7)] .epsilon. = 1.0000 A4 = 0.28413 .times. 10.sup.-3 A6 = 0.15690 .times. 10.sup.-4 A8 = 0.56334 .times. 10.sup.-6 [Aspherical Data of Twelfth Surface (r12)] .epsilon. = 1.0000 A4 = -0.64367 .times. 10.sup.-3 A6 = -0.20690 .times. 10.sup.-4 A8 = 0.96767 .times. 10.sup.-7 A10 = -0.17214 .times. 10.sup.-6 [Aspherical Data of Thirteenth Surface (r13)] .epsilon. = 1.0000 A4 = -0.28758 .times. 10.sup.-3 A6 = -0.72834 .times. 10.sup.-5 A8 = -0.11256 .times. 10.sup.-5 A10 = -0.10975 .times. 10.sup.-6 [Aspherical Data of Eighteenth Surface (r18)] .epsilon. = 1.0000 A4 = -0.47552 .times. 10.sup.-2 A6 = 0.18708 .times. 10.sup.-3 A8 = -0.10431 .times. 10.sup.-4 A10 = 0.24544 .times. 10.sup.-6 [Aspherical Data of Nineteenth Surface (r19)] .epsilon. = 1.0000 A4 = -0.53185 .times. 10.sup.-2 A6 = 0.21778 .times. 10.sup.-3 A8 = -0.13316 .times. 10.sup.-4 [Values of Condition (23) on Sixth Surface (r6)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00146 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.02452 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.13023 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.41267 [Values of Condition (23) on Seventh Surface (r7)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00048 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00929 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.06401 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.30124 [Values of Condition (24) on Twelfth Surface (r12)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00026 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00429 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.02365 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.08799 [Values of Condition (24) on Thirteenth Surface (r13)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00011 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.00182 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.01043 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.04310 [Values of Condition (25) on Eighteenth Surface (r18)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00226 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.03388 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.15712 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.45821 [Values of Condition (25) on Nineteenth Surface (r19)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00159 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.02405 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.11362 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.34557______________________________________
TABLE 13______________________________________Construction Data of Example 13 f = 5.1.about.16.0.about.48.8 FNO = 2.88.about.3.74.about.4.10______________________________________Radius of Axial Refractive Abbe Curvature Distance Index Number______________________________________ r1 = 44.089 d1 = 0.800 N1 = 1.84947 .nu.1 = 36.15 r2 = 22.689 d2 = 3.368 N2 = 1.48749 .nu.2 = 70.44 r3 = -268.849 d3 = 0.100 r4 = 20.608 d4 = 2.606 N3 = 1.49310 .nu.3 = 83.58 r5 = 103.926 d5 = 0.500.about.13.388.about.23.790 r6 = 18.124 d6 = 0.650 N4 = 1.77250 .nu.4 = 49.77 r7 = 6.084 d7 = 4.870 r8* = -6.916 d8 = 0.700 N5 = 1.77250 .nu.5 = 49.77 r9 = 13.205 d9 = 1.411 N6 = 1.84666 .nu.6 = 23.82 r10* = -21.602 d10 = 12.440.about.4.980.about.0.500 r11 = .infin. d11 = 0.500 (Aperture Stop S) r12* = 15.792 d12 = 1.575 N7 = 1.75450 .nu.7 = 51.57 r13 = -23.111 d13 = 0.600 N8 = 1.84666 .nu.8 = 23.82 r14* = 213.351 d14 = 5.822.about.1.575.about.0.200 r15 = 5.730 d15 = 2.725 N9 = 1.48749 .nu.9 = 70.44 r16 = 141.739 d16 = 0.100 r17 = 14.740 d17 = 1.783 N10 = 1.48749 .nu.10 = 70.44 r18 = -16.220 d18 = 0.100 r19* = 318.459 d19 = 1.000 N11 = 1.84889 .nu.11 = 32.66 r20* = 8.319 d20 = 1.000.about.5.247.about.6.622 r21 = .infin. d21 = 3.400 N12 = 1.51680 .nu.12 = 64.20 r22 = .infin.[Aspherical Data of Eighth Surface (r8)] .epsilon. = 1.0000 A4 = 0.91360 .times. 10.sup.-3 A6 = -0.38654 .times. 10.sup.-4 A8 = 0.13085 .times. 10.sup.-5 [Aspherical Data of Tenth Surface (r10)] .epsilon. = 1.0000 A4 = 0.40438 .times. 10.sup.-3 A6 = -0.16170 .times. 10.sup.-4 A8 = -0.20488 .times. 10.sup.-6 A10 = 0.36662 .times. 10.sup.-7 [Aspherical Data of Twelfth Surface (r12)] .epsilon. = 1.0000 A4 = -0.14855 .times. 10.sup.-3 A6 = 0.27632 .times. 10.sup.-4 A8 = -0.38928 .times. 10.sup.-5 A10 = 0.19997 .times. 10.sup.-6 [Aspherical Data of Fourteenth Surface (r14)] .epsilon. = 1.0000 A4 = -0.53448 .times. 10.sup.-4 A6 = 0.15480 .times. 10.sup.-4 A8 = -0.18236 .times. 10.sup.-5 A10 = 0.80884 .times. 10.sup.-7 [Aspherical Data of Nineteenth Surface (r19)] .epsilon. = 1.0000 A4 = -0.11631 .times. 10.sup.-2 A6 = 0.32367 .times. 10.sup.-5 A8 = -0.10732 .times. 10.sup.-5 [Aspherical Data of Twentieth Surface (r20)] .epsilon. = 1.0000 A4 = 0.26988 .times. 10.sup.-3 A6 = 0.37732 .times. 10.sup.-4 A8 = 0.13560 .times. 10.sup.-5 [Values of Condition (23) on Eighth Surface (r8)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00075 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.01090 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.04825 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.13750 [Values of Condition (23) on Tenth Surface (r10)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00019 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00280 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.01220 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.03179 [Values of Condition (24) on Twelfth Surface (r12)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00003 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00045 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.00180 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.00499 [Values of Condition (24) on Fourteenth Surface (r14)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = 0.00001 y = 0.50 ymax . . . (x - x0)/(N' - N) = 0.00012 y = 0.75 ymax . . . (x - x0)/(N' - N) = 0.00030 y = 1.00 ymax . . . (x - x0)/(N' - N) = 0.00039 [Values of Condition (25) on Nineteenth Surface (r19)] y = 0.00 ymax . . . (x - x0)/(N' - N) = 0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00063 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.01011 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.05213 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.17470 [Values of Condition (25) on Twentieth Surface (r20)] y = 0.00 ymax . . . (x - x0)/(N' - N) = -0.00000 y = 0.25 ymax . . . (x - x0)/(N' - N) = -0.00010 y = 0.50 ymax . . . (x - x0)/(N' - N) = -0.00201 y = 0.75 ymax . . . (x - x0)/(N' - N) = -0.01383 y = 1.00 ymax . . . (x - x0)/(N' - N) = -0.06294______________________________________
TABLE 14__________________________________________________________________________<<Values Corresponding to Conditions (1) to (5)>> Cond. (5) Cond. (1) Cond. (2) Cond. (3) Cond. (4) log(.beta.2T/.beta.Examples f1/fW .beta.2T/.beta.2W .beta.34T/.beta.34W M2/Z f4/f3 2W)/log(Z)__________________________________________________________________________1 5.01 2.735 2.108 1.75 0.51 0.574 2 4.22 2.087 1.374 2.39 0.69 0.698 3 5.92 2.978 3.207 1.36 0.37 0.483__________________________________________________________________________
TABLE 15__________________________________________________________________________<<Distances Varying with Focusing in Close-Distance Condition (D = 1 m)>>focal-length Ex. 4 Ex. 5 Ex. 6 Ex. 7conditions d5 d10 d5 d10 d4 d10 d5 d11__________________________________________________________________________[W] 0.419 10.063 0.362 17.892 0.497 6.621 0.376 13.529 [M] 5.666 4.817 10.889 7.503 3.694 3.424 7.484 6.421 [T] 8.719 1.764 15.527 2.865 5.573 1.545 11.538 2.367__________________________________________________________________________
TABLE 16______________________________________<<Values Corresponding to Conditions (8) to (11)>> Cond. (8) Cond. (9) Cond. (10) Cond. (11) Examples .vertline..beta.2T.vertline. f1/fW M4/M2 log(.beta.2T/.beta.2W) /log(Z)______________________________________4 0.949 4.752 0.522 0.577 5 0.949 7.610 0.448 0.531 6 0.950 3.751 0.272 0.701 7 0.951 6.159 0.334 0.601______________________________________
TABLE 17______________________________________<<Values Corresponding to Conditions (14) to (16)>> Cond. (14) Cond. (15) Cond. (16) M1/Ymax M4/M2 log(.beta.2T/.beta.2W)/log(Z)______________________________________Ex. 8 -3.42 -0.46 0.67 Ex. 9 -3.50 -0.44 0.67 Ex. 10 -2.45 -0.54 0.59______________________________________
TABLE 18______________________________________<<Distances Varying with Focusing in Close-Distance Condition (D = 1 m)>> focal-length Ex. 11 Ex. 12 Ex. 13conditions d5 d11 d5 d10 d5 d10______________________________________[W] 0.424 12.360 0.423 12.494 0.423 12.517 [M] 12.733 5.121 13.097 5.420 13.141 5.227 [T] 21.220 21.220 20.826 2.733 21.517 2.774______________________________________
TABLE 19______________________________________<<Values Corresponding to Conditions (20) to (22), and (26)>> Cond. (20) Cond. (21) Cond. (22) Cond. (26) .vertline..beta.2T.vertline. .vertline.fW/f2.vertline. M1/Ymax M4/M1______________________________________Ex. 11 0.95 0.84 -3.61 0.48 Ex. 12 0.95 0.83 -3.43 0.52 Ex. 13 0.95 0.84 -3.66 0.50______________________________________

Number	Date	Country
10-044812	Feb 1998	JPX
10-044816	Feb 1998	JPX
10-045097	Feb 1998	JPX
10-045133	Feb 1998	JPX

Number	Name	Date
4113355	Tsuji et al.	Sep 1978
4691513	Takahashi	Sep 1987
4818083	Mihara	Apr 1989
4859042	Tanaka	Aug 1989
4952039	Ito	Aug 1990
5100223	Ono et al.	Mar 1992
5528423	Arimoto et al.	Jun 1996
5546231	Sato	Aug 1996

Zoom lens system

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