Title:

Zoom lens and image pickup apparatus equipped with same

Document Type and Number:

United States Patent 7417802

Abstract:

A zoom lens comprises, in the following order from the object side to the image side, a positive first lens unit, a negative second lens unit, which moves during zooming, a positive third lens unit, and a positive fourth lens unit, which moves during zooming. The first lens unit includes a negative lens subunit and a positive lens subunit. The negative lens subunit includes at least two negative lenses each having a concave surface facing the image side and at least one positive lens arranged from the object side. The positive lens subunit includes at least one biconvex positive lens, a negative lens and at least two positive lenses arranged from the object side, or at least one biconvex positive lens, a cemented lens composed of a negative lens and a positive lens and at least one positive lens arranged from the object side.

Inventors:

Horiuchi, Akihisa (Utsunomiya, JP)

Plaque It!

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a zoom lens and an image pickup apparatus equipped with the same. The present invention can be suitably applied to an electronic camera such as a video camera or a digital still camera, a film camera, and a broadcast camera etc.

2. Description of the Related Art

In recent years, image pickup apparatuses (or cameras) such as video cameras, digital still cameras and surveillance cameras using a solid state image pickup element are required to have many functions and to be small in their entire size.

In accordance with such requirements, optical systems (image pickup optical systems) used in such cameras are required to be constructed as zoom lenses that are small in size, have a wide angle of view while having excellent optical performance.

When a color separating optical system such as a prism or filter is used in an image pickup apparatus, the color separating optical system is provided in its image side end portion. Accordingly, zoom lenses used in such image pickup apparatuses are required to have back focus equal to the optical path length of the color separating optical system.

As a zoom lens that meets the above requirements, a four-unit zoom lens having a positive first lens unit, a negative second lens unit, a positive third lens unit and a positive fourth lens unit arranged in the mentioned order from the object side to the image side is known. Note that a lens unit or element having a positive optical power or positive refractive power is referred to as a positive lens unit or element in this specification, and a lens unit or element having a negative optical power or refractive power is referred to as a negative lens unit or element.

One known type of such a four-unit zoom lens is what is called a rear-focus four-unit zoom lens in which the second lens unit is moved to effect zooming and the fourth lens unit is moved to correct image plane variations caused during zooming and to effect focusing.

There have been disclosed various rear-focus four-unit zoom lenses that have the first lens unit including a negative front subunit and a positive rear subunit arranged in the mentioned order from the object side to the image side to achieve a wide angle of view (see Japanese Patent Application Laid-Open Nos. H11-287952 and H11-287954).

A five-unit zoom lens having a positive first lens unit, a negative second lens unit, a positive third lens unit, a positive fourth lens unit and a positive fifth lens unit arranged in the mentioned order from the object side to the image side is also known as a zoom lens that meets the above described requirements.

In a known type of such a five-unit zoom lens that has a relatively wide angle of view, the second lens unit and the fourth lens unit are moved for zooming, and the fourth lens unit is moved for focusing (see U.S. Pat. No. 5,694,252 and Japanese Patent Application Laid-Open No. 2002-365539).

When a zoom lens is constructed as a rear focus system, the size of the entire lens system can be made smaller, focusing can be made faster and short distance shooting can be made easier as compared to zoom lenses in which focusing is effected by the first lens unit.

On the other hand, however, the rear focus zoom lens suffers from larger aberration variations during focusing.

It is difficult to achieve a wide angle of view and a high zoom ratio while achieving excellent optical performance throughout the entire zoom range.

To achieve a wide angle of view and a high zoom ratio in a rear-focus zoom lens while achieving excellent optical performance throughout the entire zoom range, it is necessary to design the configuration of each lens unit, especially the configuration of the first lens unit appropriately.

In addition, to provide back focus long enough to allow to provide a color separating optical system on the image side of the zoom lens, it is necessary to design the refractive power arrangement and the lens configuration in each lens unit appropriately.

In particular, in the case of the above described types of four-unit zoom lenses and five-unit zoom lenses, it is very difficult to enlarge the angle of view and increase the zoom ratio while achieving excellent optical performance throughout the zoom range unless the lens configuration of the first lens unit is appropriately designed.

SUMMARY OF THE INVENTION

An object of the present invention is to provide a zoom lens having a wide angle of view and a high zoom ratio in which excellent optical performance is easily achieved throughout the entire zoom range and to provide an image pickup apparatus equipped with such a zoom lens.

A zoom lens according to one aspect of the present invention comprises, in the following order from the object side to the image side, a positive first lens unit, a negative second lens unit, which moves during zooming, a positive third lens unit, and a positive fourth lens unit, which moves during zooming, wherein the first lens unit includes a negative lens subunit and a positive lens subunit, the negative lens subunit includes at least two negative lenses each having a concave surface facing the image side and at least one positive lens arranged in the mentioned order from the object side, and the positive lens subunit includes at least one biconvex positive lens, a negative lens and at least two positive lenses arranged in the mentioned order from the object side, or at least one biconvex positive lens, a cemented lens composed of a negative lens and a positive lens and at least one positive lens arranged in the mentioned order from the object side.

A zoom lens according to another aspect of the present invention comprises, in the following order from the object side to the image side, a positive first lens unit, a negative second lens unit, which moves during zooming, a positive third lens unit, and a positive fourth lens unit, which moves during zooming, wherein the first lens unit includes a negative lens subunit and a positive lens subunit, the negative lens subunit includes at least two negative lenses each having a concave surface facing the image side and at least one positive lens, and said positive lens subunit includes at least three positive lenses and at least one negative lens, or at least two positive lenses and a cemented lens composed of a negative lens and a positive lens.

A zoom lens according to still another aspect of the present invention comprises, in the following order from the object side to the image side, a positive first lens unit, a negative second lens unit, which moves during zooming, a positive third lens unit, and a positive fourth lens unit, which moves during zooming, wherein the first lens unit includes a negative lens subunit and a positive lens subunit, the negative lens subunit includes two negative lenses each having a concave surface facing the image side and a biconvex positive lens, the absolute value of the refractive power of the image side surface of the biconvex positive lens being larger than the absolute value of the refractive power of the object side surface of the same biconvex positive lens, and the positive lens subunit includes a biconvex positive lens, a negative lens or a cemented lens composed of a negative lens and a positive lens, and a positive lens having a convex surface facing the object side, the absolute value of the refractive power of the object side surface of the last mentioned positive lens being larger than the absolute value of the refractive power of the image side surface of the same positive lens.

A zoom lens according to a further aspect of the present invention comprises, in the following order from the object side to the image side, a positive first lens unit, a negative second lens unit, which moves during zooming, a positive third lens unit, and a positive fourth lens unit, which moves during zooming, wherein the first lens unit includes a negative lens subunit and a positive lens subunit, the negative lens subunit includes two negative lenses each having a concave surface facing the image side and a biconvex positive lens, the absolute value of the refractive power of the image side surface of the biconvex positive lens being larger than the absolute value of the refractive power of the object side surface of the same biconvex positive lens, and the positive lens subunit includes a biconvex positive lens, a negative lens having a concave surface facing the image side or a cemented lens composed of a negative lens having a concave surface facing the image side and a positive lens, and two positive lenses each having a convex surface facing the object side.

Further features of the present invention will become apparent from the following description of exemplary embodiments with reference to the attached drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a cross sectional view of a zoom lens according to a first embodiment.

FIG. 2 shows aberration diagrams for a numerical embodiment corresponding to the first embodiment at the wide angle end.

FIG. 3 shows aberration diagrams for the numerical embodiment according to the first embodiment at an intermediate zoom position.

FIG. 4 shows aberration diagrams for the numerical embodiment according to the first embodiment at the telephoto end.

FIG. 5 is a cross sectional view of a zoom lens according to a second embodiment.

FIG. 6 shows aberration diagrams for a numerical embodiment corresponding to the second embodiment at the wide angle end.

FIG. 7 shows aberration diagrams for the numerical embodiment according to the second embodiment at an intermediate zoom position.

FIG. 8 shows aberration diagrams for the numerical embodiment according to the second embodiment at the telephoto end.

FIG. 9 is a cross sectional view of a zoom lens according to a third embodiment.

FIG. 10 shows aberration diagrams for a numerical embodiment corresponding to the third embodiment at the wide angle end.

FIG. 11 shows aberration diagrams for the numerical embodiment according to the third embodiment at an intermediate zoom position.

FIG. 12 shows aberration diagrams for the numerical embodiment according to the third embodiment at the telephoto end.

FIG. 13 is a cross sectional view of a zoom lens according to a fourth embodiment.

FIG. 14 shows aberration diagrams for a numerical embodiment corresponding to the fourth embodiment at the wide angle end.

FIG. 15 shows aberration diagrams for the numerical embodiment according to the fourth embodiment at an intermediate zoom position.

FIG. 16 shows aberration diagrams for the numerical embodiment according to the fourth embodiment at the telephoto end.

FIG. 17 is a cross sectional view of a zoom lens according to a fifth embodiment.

FIG. 18 shows aberration diagrams for a numerical embodiment corresponding to the fifth embodiment at the wide angle end.

FIG. 19 shows aberration diagrams for the numerical embodiment according to the fifth embodiment at an intermediate zoom position.

FIG. 20 shows aberration diagrams for the numerical embodiment according to the fifth embodiment at the telephoto end.

FIG. 21 is a cross sectional view of a zoom lens according to a sixth embodiment.

FIG. 22 shows aberration diagrams for a numerical embodiment corresponding to the sixth embodiment at the wide angle end.

FIG. 23 shows aberration diagrams for the numerical embodiment according to the sixth embodiment at an intermediate zoom position.

FIG. 24 shows aberration diagrams for the numerical embodiment according to the sixth embodiment at the telephoto end.

FIG. 25 is a cross sectional view of a zoom lens according to a seventh embodiment.

FIG. 26 shows aberration diagrams for a numerical embodiment corresponding to the seventh embodiment at the wide angle end.

FIG. 27 shows aberration diagrams for the numerical embodiment according to the seventh embodiment at an intermediate zoom position.

FIG. 28 shows aberration diagrams for the numerical embodiment according to the seventh embodiment at the telephoto end.

FIG. 29 is a cross sectional view of a zoom lens according to a eighth embodiment.

FIG. 30 shows aberration diagrams for a numerical embodiment corresponding to the eighth embodiment at the wide angle end.

FIG. 31 shows aberration diagrams for the numerical embodiment according to the eighth embodiment at an intermediate zoom position.

FIG. 32 shows aberration diagrams for the numerical embodiment according to the eighth embodiment at the telephoto end.

FIG. 33 is a perspective view schematically illustrating the relevant portions of an image pickup apparatus according to the present invention.

DESCRIPTION OF THE EMBODIMENTS

In the following, a zoom lens and an image pickup apparatus equipped with the zoom lens according to an embodiment of the present invention will be described.

FIG. 1 is a cross sectional view showing the lens configuration of a zoom lens according to the first embodiment of the present invention at the wide angle end (i.e. at the shortest focal length zoom position). FIGS. 2, 3 and 4 show aberrations of the zoom lens according to the first embodiment respectively at the wide angle end, at an intermediate zoom position and at the telephoto end (i.e. at the longest focal length zoom position).

FIG. 5 is a cross sectional view showing the lens configuration of a zoom lens according to the second embodiment of the present invention at the wide angle end. FIGS. 6, 7 and 8 show aberrations of the zoom lens according to the second embodiment respectively at the wide angle end, at an intermediate zoom position and at the telephoto end.

FIG. 9 is a cross sectional view showing the lens configuration of a zoom lens according to the third embodiment of the present invention at the wide angle end. FIGS. 10, 11 and 12 show aberrations of the zoom lens according to the third embodiment respectively at the wide angle end, at an intermediate zoom position and at the telephoto end.

FIG. 13 is a cross sectional view showing the lens configuration of a zoom lens according to the fourth embodiment of the present invention at the wide angle end. FIGS. 14, 15 and 16 show aberrations of the zoom lens according to the fourth embodiment respectively at the wide angle end, at an intermediate zoom position and at the telephoto end.

FIG. 17 is a cross sectional view showing the lens configuration of a zoom lens according to the fifth embodiment of the present invention at the wide angle end. FIGS. 18, 19 and 20 show aberrations of the zoom lens according to the fifth embodiment respectively at the wide angle end, at an intermediate zoom position and at the telephoto end.

FIG. 21 is a cross sectional view showing the lens configuration of a zoom lens according to the sixth embodiment of the present invention at the wide angle end. FIGS. 22, 23 and 24 show aberrations of the zoom lens according to the sixth embodiment respectively at the wide angle end, at an intermediate zoom position and at the telephoto end.

FIG. 25 is a cross sectional view showing the lens configuration of a zoom lens according to the seventh embodiment of the present invention at the wide angle end. FIGS. 26, 27 and 28 show aberrations of the zoom lens according to the seventh embodiment respectively at the wide angle end, at an intermediate zoom position and at the telephoto end.

FIG. 29 is a cross sectional view showing the lens configuration of a zoom lens according to the eighth embodiment of the present invention at the wide angle end. FIGS. 30, 31 and 32 show aberrations of the zoom lens according to the eighth embodiment respectively at the wide angle end, at an intermediate zoom position and at the telephoto end.

FIG. 33 is a schematic illustration of a video camera (image pickup apparatus) equipped with a zoom lens according to the present invention.

The zoom lens according to each embodiment is a taking optical system used in an image pickup apparatus, and the zoom lens ZL and the camera body CB are illustrated in each of the cross sectional views.

Each zoom lens has a positive first lens unit L 1 , namely a first lens unit L 1 having a positive refractive power (i.e. optical power represented by the inverse of the focal length), a negative second lens unit L 2 , a positive third lens unit L 3 , a positive fourth lens unit L 4 and a positive fifth lens unit L 5 . The zoom lens also has an aperture stop SP for adjusting the light quantity, which is disposed on the object side of the third lens unit L 3 .

In the seventh and eighth embodiments shown in FIGS. 25 and 29, there is provided a protection glass plate GA, which is sometimes provided additionally to protect the zoom lens ZL, if need be. Such a protection glass plate GA may also be provided in the first to sixth embodiment.

In the cross sectional views is also illustrated an optical block GB. The optical block GB may be a color separating prism, an optical filter, a face plate and/or a low pass filter. In the case where the zoom lens is used as a taking optical system of a video camera or a digital still camera, the image plane IP of the zoom lens corresponds to the image pickup surface of a solid state image pickup element (photoelectric conversion element) such as a CCD sensor or a CMOS sensor. In the case where the zoom lens is used as a taking optical system of a film camera, the image plane IP corresponds to the film surface.

The first to the fifth lens units L 1 to L 5 (and the protection glass GA in the case of the seventh and eighth embodiments shown in FIGS. 25 and 29) are elements of the zoom lens (or zoom lens portion) ZL. On the other hand, the glass block GB and the image pickup element are housed in the camera body CB. The zoom lens portion ZL is detachably mounted on the camera body CB using a mount portion C.

In the aberration diagrams are shown curves for the d-line and g-line (designated by “d” and “g”) and the meridional image plane ΔM and the sagittal image plane ΔS. The lateral chromatic aberrations are shown for the g-line.

The F-number Fno of the lens and half the angle of view ω are also shown in the aberration diagrams.

In the following description of the embodiments, the wide angle end and the telephoto end refer to the zoom positions at the time when the zooming or variator lens unit (that is, the second lens unit L 2 in the embodiments) is at the respective ends of the range over which that lens unit can move mechanically along the optical axis.

In all the embodiments, during zooming (i.e. during changing the focal length) from the wide angle end to the telephoto end, the second lens unit L 2 is moved toward the image side to change the focal length as illustrated by an arrow in each cross sectional view, and the fourth lens unit L 4 is moved in a way represented by an arrow (in the cross sectional view) that is convex toward the object side to correct image plane variations caused during zooming.

The zoom lenses according to the embodiments are rear focus systems in which focusing is performed by moving a part of the fourth lens unit L 4 or the whole of the fourth lens unit L 4 (the latter being the case in the illustrated embodiments) along the optical axis.

The way of movement of the fourth lens unit L 4 during zooming changes depending on the object distance.

The solid curved arrow 4 a and the broken curved arrow 4 b in each cross sectional view represent how the fourth lens unit L 4 moves to correct image plane variations during zooming respectively when the zoom lens is focused on an object at infinity and when the zoom lens is focused at an object at a short distance. By moving the fourth lens unit L 4 in a manner represented by a curved arrow that is convex toward the object side, the space between the third lens unit L 3 and the fourth lens unit L 4 can be used efficiently, and the entire length of the zoom lens can be reduced advantageously.

In each embodiment, during focusing operation from an object at infinity to an object at a short distance at, for example, the telephoto end zoom position, the fourth lens unit L 4 is moved frontward as represented by arrow 4 c . The first lens unit L 1 and the third lens unit L 3 are not moved along the optical axis during zooming or focusing, but they may be moved, if necessary, to correct aberrations.

In each embodiment, a part or the whole of the third lens unit L 3 (which constitutes the image stabilizing lens unit) is moved in such a way to have a movement component in the direction perpendicular to the optical axis to correct image blur caused by vibration of the entire optical system. In this way, image stabilization is performed.

As per the above, image stabilization is performed without providing additional optical members such as a variable angle prism or an additional image-stabilizing lens unit. Thus, increase in the size of the entire optical system can be prevented.

A video camera according to the present invention illustrated in FIG. 33 has the above described zoom lens, a color separating element, image pickup elements for respective colors resulting from separation by the color separating element and a circuit for processing picked-up image signals.

In the following, the lens configurations of the lens units in the first to sixth embodiments shown in FIGS. 1, 5 , 9 , 13 , 17 and 21 will be described.

Each of the zoom lenses according to the first to sixth embodiments has a positive first lens unit L 1 , a negative second lens unit L 2 , a positive third lens unit L 3 , a positive fourth lens unit L 4 and a positive fifth lens unit L 5 arranged in the mentioned order from the object side to the image side.

As described before, the second and fourth lens units L 2 and L 4 are moved during zooming. The first lens unit L 1 includes a negative lens subunit L 1 a and a positive lens subunit L 1 b . Here, the negative lens subunit is located L 1 a at a position nearer the object side than that of the positive lens subunit L 1 b.

The negative lens subunit L 1 a is defined as the lens unit that is on the object side (i.e. on the magnification conjugate side) of the largest air gap among the air gaps in the first lens unit L 1 except for the air gap between the lens closest to the object (or the frontmost lens) in the first lens unit L 1 and the lens on the image side thereof (or the second-frontmost lens). The positive lens subunit L 1 b is defined as the lens unit on the image side (i.e. on the reduction conjugate side) of the aforementioned largest air gap in the first lens unit L 1 . In the illustrated embodiments, the first lens unit L 1 includes, as lens subunits, only the negative lens subunit L 1 a and the positive lens subunit L 1 b.

The negative lens subunit L 1 a includes two negative lenses each having a concave surface facing the image side and a biconvex positive lens having a refractive power whose absolute value is larger on the image side than on the object side. In other words, the absolute power of the image side surface of this biconvex positive lens is larger than the absolute value of the refractive power of object side surface thereof.

The positive lens subunit L 1 b includes a biconvex positive lens, a negative lens having a concave surface facing the image side or a cemented lens composed of a negative lens having a concave surface facing the image side and a positive lens, and one or two positive lenses each having a convex surface facing the object side.

The negative lens subunit L 1 a may include two or more negative lenses (may include three or four negative lenses) each having a concave surface facing the image side and a biconvex positive lens having a refractive power whose absolute value is larger on the image side than on the object side.

The positive lens subunit L 1 b may includes a biconvex positive lens, a negative lens or a cemented lens composed of a negative lens and a positive lens, and a positive lens that is disposed closest to the image side in that subunit, having a convex surface facing the object side and having a refractive power whose absolute value is larger on the object side than on the image side.

The positive lens subunit L 1 b may include a biconvex positive lens, a negative lens and a positive lens having a convex surface facing the object side. In this case, the lens configuration can be made simple.

Axial chromatic aberration and spherical aberration are excellently corrected by the lens configuration of the positive lens subunit L 1 b including at least one negative lens or a cemented lens and a positive lens disposed closest to the image side and having a convex surface facing the object side.

As per the above, the positive lens subunit L 1 b is composed of three to five lenses to correct aberrations excellently.

Thanks to correction achieved by the above described lens configuration of the first lens unit L 1 , distortion in the zoom lenses according to the embodiments is on a par with zoom lenses having normal angles of view, in spite that the zoom lenses according to the embodiments have ultra-wide angles of view of 75 degrees or more at the wide angle end.

In addition, astigmatism and curvature of field are also corrected excellently.

The second lens unit L 2 includes a negative meniscus lens having the concave surface facing the image side, a cemented lens composed of a positive lens having a convex surface facing the image side and a biconcave negative lens, and a cemented lens composed of a biconvex positive lens and a negative lens or a single positive lens, arranged in the mentioned order from the object side to the image side. In the second lens unit L 2 , one or two negative lens may be provided on the image side of the negative lens that is disposed closest to the object.

With the above described configuration of the second lens unit L 2 that is moved for zooming, aberrations are corrected excellently. To achieve excellent optical performance, the lens configuration of the second lens unit L 2 is designed in such a way as to excellently correct aberration variations caused during zooming.

An aspherical surface is used in the second lens unit L 2 in each embodiment. The use of the aspherical lens in the second lens unit L 2 is advantageous in correcting astigmatism at the wide angle end satisfactorily to achieve excellent optical performance.

The third lens unit L 3 includes a cemented lens composed of a biconcave negative lens and a positive lens, and a cemented lens composed of a positive lens and a negative lens or a single positive lens arranged in the mentioned order from the object side to the image side.

A part or the whole of the third lens unit L 3 is moved in such a way as to have a movement component in the direction perpendicular to the optical axis to thereby shift the image.

The third lens unit L 3 includes a cemented lens composed of a biconcave negative lens and a positive lens, and a cemented lens composed of a positive lens and a negative lens or a single positive lens (alternatively, two or more positive lenses may be provided) arranged in the mentioned order from the object side to the image side.

The third lens unit L 3 has at least one aspherical surface. By the use of the aspherical surface(s), spherical aberration and coma at the wide angle end and lateral chromatic aberration are satisfactorily corrected.

It is desired that the aspherical surface used in the third lens unit L 3 have a refractive power that decreases from the center toward the periphery of the lens.

A part or the whole of the third lens unit L 3 is moved in such a way as to have a movement component in the direction perpendicular to the optical axis to thereby shift the image. In other words, a part or the whole of the third lens unit L 3 is moved in such a way as to have a movement component in the direction perpendicular to the optical axis in order to perform image stabilization, namely to reduce image blur or to reduce positional shift of the image.

The fourth lens unit L 4 includes a positive lens, and a cemented lens composed of a negative lens and a positive lens arranged in the mentioned order from the object side to the image side.

The fifth lens unit L 5 includes a cemented lens composed of a biconvex positive lens and a negative lens arranged in the mentioned order from the object side to the image side.

In the lens system as a whole, the lens configuration of the fifth lens unit L 5 is relevant to the fourth lens unit. The fifth lens unit L 5 takes over a portion of the role of correcting spherical aberration and chromatic aberration that the moving fourth lens unit L 4 is required to play. Thus, the number of lenses in the fourth lens unit L 4 can be reduced. Thus, the fourth lens unit L 4 can have a configuration that is most suitable for quick focusing.

The fifth lens unit L 5 correct aberrations, especially spherical aberration and chromatic aberration remaining uncorrected by the first to fourth lens units L 1 to L 4 , thereby achieving aberration correction adequate for high quality image forming.

In the following, the lens configuration of each lens unit in the seventh and eighth embodiments illustrated in FIGS. 25 and 29 will be described.

Each of the zoom lenses according to the seventh and eight embodiments has a positive first lens unit L 1 , a negative second lens unit L 2 , a positive third lens unit L 3 and a positive fourth lens unit L 4 arranged in the mentioned order from the object side to the image side.

During zooming, the second and fourth lens units L 2 and L 4 are moved, as described before.

The first lens unit L 1 includes a negative lens sub unit L 1 a and a positive lens subunit L 1 b.

The lens configurations of the negative lens subunit L 1 a and the positive lens subunit L 1 b and advantages they have are the same as those in the first to sixth embodiments.

The second lens unit L 2 includes a negative meniscus lens having the concave surface facing the image side, a cemented lens composed of a positive lens having a convex surface facing the image side and a biconcave negative lens, and a cemented lens composed of a biconvex positive lens and a negative lens, and the cemented lens composed of the biconvex positive lens and the negative lens can be replaced with a single positive lens, arranged in the mentioned order from the object side to the image side.

The third lens unit L 3 includes a cemented lens composed of a biconcave negative lens and a positive lens, and a cemented lens composed of a positive lens and a negative lens, arranged in the mentioned order from the object side to the image side.

The configuration of the fourth lens unit L 4 is the same as that in the first to sixth embodiments.

In these embodiments, the positive lens subunit may include at least one biconvex positive lens, a negative lens, and at least two positive lenses arranged in the mentioned order from the object side to the image side, or alternatively at least one biconvex positive lens, a cemented lens composed of a negative lens and a positive lens, and at least one positive lens arranged in the mentioned order from the object side to the image side.

The positive lens disposed closest to the image side in the positive lens subunit is a positive lens having a convex surface facing the object side and having a refractive power whose absolute value is larger on the object side than on the image side. To put it differently, the absolute value of the refractive power of the object side surface of the positive lens disposed closest to the image side in the positive lens subunit is larger than the absolute value of the refractive power of the image side surface of the positive lens disposed closest to the image side in the positive lens subunit, and the object side surface of the positive lens disposed closest to the image side in the positive lens subunit is a convex surface.

In the case where the positive lens subunit includes at least one biconvex positive lenses, a negative lens, and at least two positive lenses arranged in the mentioned order from the object side, the aforementioned at least two positive lenses may be two positive lenses each having a convex surface facing the object side. On the other hand, in the case where the positive lens subunit includes at least one biconvex positive lens, a cemented lens composed of a negative lens and a positive lens, and at least one positive lens arranged in the mentioned order from the object side, the aforementioned at least one positive lens may be one or two positive lenses each having a convex surface facing the object side.

The zoom lens according to each of the above described embodiments is designed to satisfy at least one of the conditions presented below and has advantages associated with the corresponding conditions.

In the conditional expressions below, f 1 a is the focal length of the negative lens subunit L 1 a and f 1 is the focal length of the first lens unit L 1 , H 12 w is the principal point interval of the first lens unit L 1 and the second lens unit L 2 at the wide angle end, and fw is the focal length of the entire lens system at the wide angle end. Furthermore, R 1 bf is the radius of curvature of the object side surface of the negative lens in the positive lens subunit L 1 b , f 2 is the focal length of the second lens unit L 2 , Fnow is the F-number of the entire lens system at the wide angle end, and BF is what is called the back focus or the equivalent distance in air (i.e. the distance under the assumption that there is no optical block such as a prism) from the lens surface closest to the image side to the image plane at the wide angle end.

Each zoom lens satisfies at least one of the following conditions.
1.8 <|f 1 a/f 1|<4.0 (1)
−7.7 <H 12 w/fw<− 3.5 (2)
−0.09 <f 1/ R 1 bF< 0.455 (3)
2.8 <|f 2/ fw|< 5.2 (4)
6.4 <BF× √{square root over ( F _no W )}/ fw< 15.0 (5)

In the following, technical meanings of the above conditions will be described.

Conditional expression (1) is intended to limit the refractive power of the negative lens subunit L 1 a in the first lens unit L 1 . This conditional expression (1) relates indirectly to the principal point interval in first and second lens units L 1 , L 2 . If the value of |f 1 a /f 1 | is larger than the upper bound of conditional expression (1), the principal point interval cannot be made short, and the lens system becomes undesirably large. On the other hand, if the negative refractive power of the negative lens subunit L 1 a is so strong that the value of |f 1 a /f 1 | becomes smaller than the lower bound of conditional expression (1), it is difficult to achieve satisfactory correction of astigmatism and lateral chromatic aberration, though such a strong refractive power is advantageous in making the principal point interval short.

Conditional expression (2) expresses a condition to reduce the entire length of the lens system while achieving satisfactory correction of aberrations. If the principal point interval is so large that the value of H 12 w /fw becomes larger than the upper bound of conditional expression (2), the diameter of the frontmost lens is required to be made large, which makes it difficult to make the size of the zoom lens small.

On the other hand, if the principal point interval is so small that the value of H 12 w /fw becomes smaller than the lower bound of conditional expression (2), it is difficult to achieve satisfactory correction of astigmatism and lateral chromatic aberration in the zoom range from the wide angle end to an intermediate zoom position.

Conditional expression (3) expresses a condition to achieve satisfactory correction of aberrations, in particular distortion and lateral chromatic aberration, at the wide angle end. If the curvature of the object side surface of the negative lens in the positive lens subunit L 1 b is so large that the value of f 1 /R 1 b F becomes larger than the upper bound of conditional expression (3), positive lateral chromatic aberration becomes undesirably large. On the other hand, if the curvature of that surface is so small that the value of f 1 /R 1 b F becomes smaller than the lower bound of conditional expression (3), negative distortion becomes undesirably large.

Conditional expressions (4) and (5) express conditions to make the size of the entire lens system small, to achieve a wide angle of view and to ensure a long back focus. By designing a zoom lens in such a way as to satisfy at least one of these conditional expressions (4) and (5), the zoom lens system can be made well-balanced.

Conditional expression (4) relates to the negative refractive power of the second lens unit L 2 and is intended to limit the refractive power of the variator lens unit in order to achieve an ultra wide angle of view.

In addition, conditional expression (4) expresses a condition to achieve a high zoom ratio while making aberration variations during zooming small.

If the negative refractive power of the second lens unit L 2 is so weak that the value of |f 2 /fw| becomes larger than the upper bound of conditional expression (4), the afocal magnification in the variator portion cannot be made sufficiently high, and it becomes difficult to provide a desired back focus. In addition, movement amount of the second lens unit L 2 required to achieve a desired zoom ratio becomes large, which leads to an increase in the distance between the stop SP and the first lens unit L 1 . This invites an undesirable increase in the diameter of the frontmost lens.

On the other hand, if the negative refractive power of the second lens unit L 2 is so strong that the value of |f 2 /fw| becomes smaller than the lower bound of conditional expression (4), the negative Petzval sum becomes large, so does the curvature of field, and aberration variations during zooming also become large.

Conditional expression (5) relates to relationship between the back focus BF and the F-number of the zoom lens. Conditional expression (5) expresses a condition to obtain a high quality image by separating light into three color components using a color separating prism and picking up images of the respective colors. Such an image pickup system is used in a high performance camera.

If the F-number is so small that the value of BF×√{square root over (F _noW)}/fw becomes smaller than the lower bound of conditional expression (5), a significant amount of high order spherical aberration and coma occur, and it is difficult to correct these aberrations. On the other hand, when the F-number is so large that the value of BF×√{square root over (F _noW)}/fw becomes larger than the upper bound of conditional expression (5), the diameter of the on-axis light flux becomes small, and the size of the color separating prism provided on the image side of the zoom lens can be made small. This results in unnecessary enlargement of the back focus and undesirable increase in the length of the entire lens system.

In the zoom lens according to each embodiment, the third lens unit L 3 includes a plurality of lenses arranged with at least one air gap therebetween. The length D 3 a of the at least one air gap along the optical axis and the focal length f 3 of the third lens unit L 3 satisfy the following condition.
0.01 <D 3 a/f 3<0.1 (6)

The air gap in the third lens unit L 3 is provided to allow to insert, in a removable manner, a light quantity adjusting filter such as one or more ND filters besides the stop for adjusting the light quantity.

In the zoom lenses according to the embodiments, one or plurality of light quantity adjusting filters is inserted into the optical path in a removable manner to control the quantity of light incident on the image pickup element.

If the air gap is so large that the value of D 3 a /f 3 becomes larger than the upper bound of conditional expression (6), the size of the entire lens system becomes large, and it becomes difficult to correct spherical aberration at the wide angle end. On the other hand, if the air gap is so small that the value of D 3 a /f 3 becomes smaller than the lower bound of conditional expression (6), it becomes difficult to insert a light quantity adjusting filter into the optical path in a removable manner.

The focal length f 1 FF of the composite system composed of a negative lens subunit L 1 a and the biconvex positive lens in the positive lens sub unit L 1 b and the focal length f 1 of the first lens unit satisfy the following condition.
0.02 <f 1/ f 1 FF< 0.83 (7)

A wide conversion lens to be provided, in a removable manner, on the object side of the first lens unit is generally an afocal system having substantially zero refractive power.

In the zoom lenses according to the embodiments, if a part of the lenses in the first lens unit L 1 constituted an afocal system, they should be the negative lens subunit L 1 a and the object side positive lens in the positive lens subunit L 1 b.

However in the zoom lenses according to the embodiments, an afocal system is not added in, and the composite system composed of the negative lens subunit L 1 a and the object side positive lens in the positive lens subunit L 1 b has a certain refractive power.

Conditional expression (7) appropriately limits the refractive power (as the reciprocal of the focal length) of the composite system.

Conditional expression (7) expresses a condition to make the size of the entire system small. If the focal length of the composite system is so large that the value of f 1 /f 1 FF becomes smaller than the lower bound of conditional expression (7), the size of the entire lens system becomes large. On the other hand, if the focal length of the composite system is so small that the value of f 1 /f 1 FF becomes larger than the upper bound of conditional expression (7), it becomes difficult to correct spherical aberration.

The zoom lenses according to the first to sixth embodiments satisfy the following condition in terms of the focal length f 3 of the third lens unit L 3 and the focal length f 5 of the fifth lens unit L 5 .
1.2 <f 3/ f 5<3.6 (8)

Conditional expression (8) relates to the ratio of the focal length f 3 of the third lens unit L 3 and the focal length f 5 of the fifth lens unit L 5 . More specifically, conditional expression (8) expresses a condition to achieve a high zoom ratio and a long back focus. If the focal length f 3 of the third lens unit L 3 is so large that the value of f 3 /f 5 becomes larger than the upper bound of conditional expression (8), the light flux emergent from the third lens unit L 3 diverges greatly. Then, it is required to make the effective diameter of the fourth lens unit L 4 large, which leads to an increase in the weight of the entire lens system, though a long back focus is achieved.

On the other hand, if the focal length f 3 of the third lens unit L 3 is so short that the value of f 3 /f 5 becomes smaller than the lower bound of conditional expression (8), it becomes difficult to achieve a sufficiently long back focus. Furthermore, if the focal length f 5 of the fifth lens unit L 5 is too long, spherical aberration cannot be corrected sufficiently.

It is more desirable in achieving excellent optical performance more easily that the lower and upper bounds in conditional expressions (1) to (8) be modified as follows.
2.0 <|f 1 a/f 1|<3.5 (1a)
−7.0 <H 12 w/fw<− 4.0 (2a)
−0.07 <f 1 /R 1 bF< 0.417 (3a)
3.1 <|f 2/ fw|< 4.8 (4a)
7.0 <BF× √{square root over ( F _no W )}/ fw< 13.0 (5a)
0.015 <D 3 a/f 3<0.09 (6a)
0.1 <f 1/ f 1 FF< 0.75 (7a)
1.4 <f 3/ f 5<3.2 (8a)

More preferably, the upper bound of conditional expression (1a) may be changed to 3.3, and the lower bound of conditional expression (7a) may be changed to 0.3.

In the zoom lenses according to the embodiments, the specifications of the elements are determined so that distortion in the state that the zoom lens is focused on an object at infinity at the wide angle end falls within the range of −6% to 0% throughout the image frame.

With enlargement of the angle of view to ultra-wide angles, distortion increases more and more, and large minus distortion or barrel distortion occurs. In recent years, the surface of the display panel of TV monitors has been made flat, which makes barrel distortion more conspicuous. Therefore, it is necessary to correct distortion excellently.

Conventionally, in order to correct distortion, a positive lens is disposed closest to the object side or an aspherical surface is used as the surface closest to the object side.

In the zoom lenses according to the embodiments, distortion is corrected excellently by the above described configuration of the first lens unit L 1 .

An optical member having a weak refractive power may be provided on the image side of the fifth lens unit L 5 in the zoom lenses according to the first to sixth embodiments, and on the image side of the fourth lens unit L 4 in the seventh and eighth embodiments, and/or on the object side of the first lens unit L 1 .

In the following, an embodiment of a video camera (image pickup apparatus) having a zoom lens according to the present invention as a taking optical system will be described with reference to FIG. 33.

In FIG. 33 are illustrated a body 10 or a video camera or a digital still camera and a taking optical system 11 in the form of a zoom lens according to the present invention. An image pickup element 12 such as a CCD receives an object image formed by the taking optical system 11 . Recording means 13 records data of the object image received by the image pickup element 12 . A user can view an object image displayed on a display element of a viewfinder 14 .

The display element may be a liquid crystal panel, on which the object image picked up by the image pickup element 12 is displayed. The video camera also has a liquid crystal display panel 15 having a function similar to the aforementioned view finder.

By using the zoom lens according to the present invention in an image pickup apparatus such as a video camera, an optical apparatus having excellent optical performance can be provided.

As per the above, according to the embodiments of the present invention, there can be provided zoom lenses that are small in the size of the entire lens system and have excellent optical performance in spite of high zoom ratios, and an image pickup apparatus using such a zoom lens.

In addition, according to the embodiments of the present invention, there can be provided zoom lenses having excellent optical performance throughout the zoom range from the wide angle end to the telephoto end and throughout the object distance range from a very short distance to infinity in spite of their high zoom ratios of 6 to 8, having long back focus that allows insertion of an optical element such as a color separating prism while having a large aperture ratio with an F-number about 1.6, and having good performance throughout the zoom range and throughout the object distance range while leaving a space in which a complex stop mechanism can be provided and/or a space in which an ND filter can be provided.

In the following, numerical embodiments 1 to 8 corresponding to the first to eighth embodiments will be presented. The tables presented below show particulars of the numerical embodiments. In the tables, suffix number i represents the surface number counted from the object side. Thus, Ri represents the radius of curvature of the i-th surface, and Di represents the thickness of the member or the air gap between the i-th surface and the (i+1)-th surface. Ni represents the refractive index for the d-line and υi represents the Abbe number. In each numerical embodiment, the three surfaces closest to the image side correspond to a member(s) such as a quartz low pass filter and an infrared cut filter.

The aspherical surface shape is expressed by the following equation in terms of the height h from the optical axis and the displacement (or distance) x in the direction parallel to the optical axis at that height h from the vertex of the aspherical surface as the reference point:

$x = \frac{(1 / R) h^{2}}{1 + \sqrt{{1 - (1 + k) {(h / R)}^{2}}}} + {Bh}^{4} + {Ch}^{6} + {Dh}^{8} + {Eh}^{10} + {Fh}^{12}$

where R is the paraxial radius of curvature, k is the conic constant, and B, C, D, E and F are aspherical coefficients.

In the following, the expression “e-X” stands for “×10 ^−x”. For each numerical embodiment, the focal length f, the F-number Fno and half the angle of field ω will also be presented. Values associated with the above mentioned conditional expressions in the respective numerical embodiments will also be presented in Table 1.


Numerical Embodiment 1
f	1.00-5.84	Fno	1.66-2.66	2ω	82.5-17.1

R1	55.728	D1	0.94	N1	1.712995	ν1	53.9
R2	8.844	D2	4.12
R3	−834.144	D3	0.76	N2	1.719995	ν2	50.2
R4	20.789	D4	1.52
R5	75.948	D5	1.75	N3	1.846660	ν3	23.9
R6	−26.570	D6	3.79
R7	18.490	D7	2.89	N4	1.603112	ν4	60.6
R8	−18.490	D8	0.66
R9	−248.620	D9	0.58	N5	1.846660	ν5	23.9
R10	10.085	D10	0.36
R11	13.077	D11	1.78	N6	1.487490	ν6	70.2
R12	−45.518	D12	0.06
R13	9.697	D13	1.55	N7	1.719995	ν7	50.2
R14	405.903	D14	variable
R15	11.623	D15	0.29	N8	1.882997	ν8	40.8
R16	2.651	D16	0.99
R17	−22.930	D17	1.20	N9	1.808095	ν9	22.8
R18	−3.673	D18	0.50	N10	1.859600	ν10	40.4
R19*	6.115	D19	0.50
R20	5.964	D20	1.13	N11	1.603420	ν11	38.0
R21	−5.964	D21	0.20	N12	1.882997	ν12	40.8
R22	−10.871	D22	variable
R23	stop	D23	1.40
R24	−5.867	D24	0.23	N13	1.638539	ν13	55.4
R25	4.070	D25	1.14	N14	1.683290	ν14	31.4
R26*	−18.373	D26	1.86
R27	30.383	D27	1.61	N15	1.548141	ν15	45.8
R28	−4.309	D28	0.29	N16	2.003300	ν16	28.3
R29	−7.062	D29	variable
R30	137.286	D30	0.73	N17	1.622992	ν17	58.2
R31	−11.175	D31	0.06
R32	11.578	D32	0.29	N18	1.846660	ν18	23.9
R33	5.964	D33	1.49	N19	1.487490	ν19	70.2
R34	−12.755	D34	variable
R35	11.547	D35	0.85	N20	1.487490	ν20	70.2
R36	−8.906	D36	0.26	N21	1.647689	ν21	33.8
R37	−114.307	D37	1.75
R38	∞	D38	5.85	N22	1.589130	ν22	61.2
R39	∞	D39	1.10	N23	1.516330	ν23	64.2
R40	∞

Aspherical surfaces are marked by asterisk *.
Aspherical Coefficient
R19 k = 9.57065e−01, B = −1.80926e−03, C = −4.75705e−05, D = 0.00, E = 0.00, F = 0.00
R26 k = −2.15005e+01, B = 5.86862e−04, C = 2.13598e−05, D = −7.76637e−07, E = 0.00, F = 0.00


focal length
variable distance	1.00	3.93	5.84

D14	0.29	6.37	7.53
D22	8.30	2.22	1.06
D29	1.82	1.32	1.83
D34	1.15	1.65	1.14


Numerical Embodiment 2
f	1.00-5.84	Fno	1.68-2.65	2ω	82.5-17.1

R1	48.316	D1	0.94	N1	1.772499	ν1	49.6
R2	9.028	D2	4.20
R3	−101.358	D3	0.76	N2	1.6838539	ν2	55.4
R4	20.481	D4	1.36
R5	71.694	D5	1.75	N3	1.846660	ν3	23.9
R6	−25.772	D6	3.94
R7	18.654	D7	2.69	N4	1.603112	ν4	60.6
R8	−18.654	D8	0.82
R9	−206.775	D9	0.58	N5	1.846660	ν5	23.9
R10	10.347	D10	0.34
R11	13.343	D11	1.76	N6	1.487490	ν6	70.2
R12	−44.086	D12	0.06
R13	9.939	D13	1.44	N7	1.719995	ν7	50.2
R14	447.751	D14	variable
R15	11.953	D15	0.29	N8	1.882997	ν8	40.8
R16	2.713	D16	0.98
R17	−45.759	D17	1.40	N9	1.805181	ν9	25.4
R18	−2.977	D18	0.29	N10	1.848620	ν10	40.0
R19*	6.236	D19	0.48
R20	5.741	D20	1.02	N11	1.603420	ν11	38.0
R21	−28.249	D21	variable
R22	stop	D22	1.77
R23	−4.928	D23	0.23	N12	1.622992	ν12	58.2
R24	4.928	D24	1.14	N13	1.683290	ν13	31.4
R25*	−14.511	D25	1.84
R26	33.785	D26	1.55	N14	1.548141	ν14	45.8
R27	−4.364	D27	0.29	N15	2.003300	ν15	28.3
R28	−6.952	D28	variable
R29	61.240	D29	0.73	N16	1.603112	ν16	60.6
R30	−11.708	D30	0.06
R31	11.643	D31	0.29	N17	1.846660	ν17	23.9
R32	5.931	D32	1.58	N18	1.487490	ν18	70.2
R33	−13.771	D33	variable
R34	11.823	D34	0.85	N19	1.487490	ν19	70.2
R35	−8.558	D35	0.26	N20	1.647689	ν20	33.8
R36	−67.005	D36	1.46
R37	∞	D37	5.85	N21	1.589130	ν21	61.2
R38	∞	D38	1.10	N22	1.516330	ν22	64.2
R39	∞

Aspherical surfaces are marked by asterisk *.
Aspherical Coefficient
R19 k = 2.12088e+00, B = −2.35439e−03, C = −1.22931e−04, D = 0.00, E = 0.00, F = 0.00
R25 k = −1.62372e+00, B = 8.69232e−04, C = 9.25646e−06, D = −9.54787e−07, E = 0.00, F = 0.00


focal length
variable distance	1.00	3.95	5.84

D14	0.29	6.52	7.71
D21	8.73	2.50	1.31
D28	1.29	0.75	1.27
D33	1.46	1.99	1.48


Numerical Embodiment 3
f	1.00-5.84	Fno	1.68-2.65	2ω	82.5-17.1

R1	60.659	D1	0.94	N1	1.712995	ν1	53.9
R2	9.219	D2	4.50
R3	−48.636	D3	0.76	N2	1.638539	ν2	55.4
R4	25.034	D4	1.40
R5	103.195	D5	1.90	N3	1.846660	ν3	23.9
R6	−21.633	D6	4.41
R7	19.247	D7	2.83	N4	1.603112	ν4	60.6
R8	−19.247	D8	0.18
R9	−931.793	D9	0.58	N5	1.846660	ν5	23.9
R10	10.240	D10	0.51
R11	15.325	D11	1.55	N6	1.487490	ν6	70.2
R12	−94.158	D12	0.06
R13	9.951	D13	1.58	N7	1.693501	ν7	53.2
R14	−960.836	D14	variable
R15	12.119	D15	0.29	N8	1.882997	ν8	40.8
R16	2.947	D16	1.00
R17	−40.088	D17	1.40	N9	1.805181	ν9	25.4
R18	−3.447	D18	0.47	N10	1.848620	ν10	40.0
R19*	5.933	D19	0.50
R20	5.803	D20	1.02	N11	1.603420	ν11	38.0
R21	−11.104	D21	0.23	N12	1.882997	ν12	40.8
R22	−16.758	D22	variable
R23	stop	D23	2.01
R24	−5.111	D24	0.23	N13	1.638539	ν13	55.4
R25	5.111	D25	1.14	N14	1.683290	ν14	31.4
R26*	−15.680	D26	1.90
R27	79.346	D27	1.17	N15	1.433870	ν15	95.1
R28	−7.368	D28	variable
R29	23.538	D29	0.73	N16	1.603112	ν16	60.6
R30	−16.898	D30	0.06
R31	15.764	D31	0.29	N17	1.846660	ν17	23.9
R32	6.655	D32	1.58	N18	1.487490	ν18	70.2
R33	−10.971	D33	variable
R34	13.317	D34	0.85	N19	1.487490	ν19	70.2
R35	−8.206	D35	0.26	N20	1.698947	ν20	30.1
R36	−32.545	D36	1.46
R37	∞	D37	5.85	N21	1.589130	ν21	61.2
R38	∞	D38	1.10	N22	1.516330	ν22	64.2
R39	∞

Aspherical surfaces are marked by asterisk *.
Aspherical Coefficient
R19 k = 1.55464e+00, B = −1.88361e−03, C = −6.82493e−05, D = 0.00, E = 0.00, F = 0.00
R26 k = −1.54951e+00, B = 1.33596e−03, C = 2.64342e−05, D = −6.62544e−07, E = 0.00, F = 0.00


focal length
variable distance	1.00	3.94	5.84

D14	0.29	7.25	8.58
D22	9.50	2.54	1.22
D28	1.46	0.94	1.42
D33	1.42	1.94	1.46


Numerical Embodiment 4
f	1.00-5.84	Fno	1.68-2.65	2ω	82.5-17.1

R1	54.227	D1	0.94	N1	1.772499	ν1	49.6
R2	9.750	D2	4.35
R3	−53.303	D3	0.76	N2	1.638539	ν2	55.4
R4	20.328	D4	2.29
R5	211.980	D5	1.90	N3	1.846660	ν3	23.9
R6	−20.320	D6	4.31
R7	19.940	D7	2.83	N4	1.603112	ν4	60.6
R8	−19.940	D8	0.88
R9	−938.652	D9	0.58	N5	1.846660	ν5	23.9
R10	10.223	D10	0.39
R11	14.337	D11	1.45	N6	1.487490	ν6	70.2
R12	−142.318	D12	0.06
R13	9.842	D13	1.45	N7	1.696797	ν7	55.5
R14	590.969	D14	variable
R15	11.796	D15	0.29	N8	1.882997	ν8	40.8
R16	2.928	D16	0.96
R17	−110.824	D17	1.40	N9	1.808095	ν9	22.8
R18	−4.808	D18	0.47	N10	1.848620	ν10	40.0
R19*	6.221	D19	0.42
R20	5.470	D20	1.02	N11	1.603420	ν11	38.0
R21	−7.007	D21	0.23	N12	1.882997	ν12	40.8
R22	−19.590	D22	variable
R23	stop	D23	2.44
R24	−5.647	D24	0.23	N13	1.638539	ν13	55.4
R25	5.647	D25	1.14	N14	1.683290	ν14	31.4
R26*	−18.563	D26	2.14
R27	77.058	D27	1.17	N15	1.496999	ν15	81.5
R28	−8.491	D28	variable
R29	26.207	D29	0.73	N16	1.603112	ν16	60.6
R30	−17.547	D30	0.06
R31	14.490	D31	0.29	N17	1.846660	ν17	23.9
R32	6.816	D32	1.58	N18	1.496999	ν18	81.6
R33	−13.363	D33	variable
R34	15.647	D34	0.85	N19	1.487490	ν19	70.2
R35	−8.463	D35	0.26	N20	1.698947	ν20	30.1
R36	−32.700	D36	1.46
R37	∞	D37	5.84	N21	1.589130	ν21	61.2
R38	∞	D38	1.10	N22	1.516330	ν22	64.2
R39	∞

Aspherical surfaces are marked by asterisk *.
Aspherical Coefficient
R19 k = 1.36203e+00, B = −1.54961e−03, C = −5.12136e−05, D = 0.00, E = 0.00, F = 0.00
R26 k = −4.82085e+00, B = 1.07535e−03, C = 1.96665e−05, D = −6.81464e−07, E = 0.00, F = 0.00


focal length
variable distance	1.00	3.95	5.84

D14	0.29	7.36	8.71
D22	9.49	2.43	1.08
D28	1.46	0.77	1.17
D33	1.87	2.55	2.16


Numerical Embodiment 5
f	1.00-7.64	Fno	1.66-2.95	2ω	82.5-13.1

R1	60.588	D1	0.93	N1	1.712995	ν1	53.9
R2	9.071	D2	4.19
R3	1747.387	D3	0.76	N2	1.719995	ν2	50.2
R4	22.573	D4	1.48
R5	77.437	D5	1.78	N3	1.846660	ν3	23.9
R6	−25.177	D6	3.90
R7	18.577	D7	2.98	N4	1.603112	ν4	60.6
R8	−18.577	D8	0.25
R9	−205.801	D9	0.58	N5	1.846660	ν5	23.9
R10	10.137	D10	0.40
R11	13.449	D11	1.78	N6	1.487490	ν6	70.2
R12	−66.098	D12	0.06
R13	9.857	D13	1.58	N7	1.719995	ν7	50.2
R14	460.450	D14	variable
R15	11.110	D15	0.29	N8	1.882997	ν8	40.8
R16	2.652	D16	1.05
R17	−25.710	D17	1.20	N9	1.808095	ν9	22.8
R18	−3.602	D18	0.50	N10	1.859600	ν10	40.4
R19*	5.810	D19	0.50
R20	5.695	D20	1.14	N11	1.603420	ν11	38.0
R21	−5.695	D21	0.20	N12	1.882997	ν12	40.8
R22	−11.597	D22	variable
R23	stop	D23	1.06
R24	−6.017	D24	0.23	N13	1.638539	ν13	55.4
R25	4.380	D25	1.14	N14	1.683290	ν14	31.4
R26*	−18.056	D26	1.84
R27	27.200	D27	1.61	N15	1.548141	ν15	45.8
R28	−4.307	D28	0.29	N16	2.003300	ν16	28.3
R29	−7.070	D29	variable
R30	140.480	D30	0.73	N17	1.622992	ν17	58.2
R31	−11.298	D31	0.06
R32	11.963	D32	0.29	N18	1.846660	ν18	23.9
R33	6.100	D33	1.49	N19	1.487490	ν19	70.2
R34	−13.286	D34	variable
R35	12.235	D35	0.85	N20	1.487490	ν20	70.2
R36	−8.964	D36	0.26	N21	1.647689	ν21	33.8
R37	−90.929	D37	1.75
R38	∞	D38	5.84	N22	1.589130	ν22	61.2
R39	∞	D39	1.10	N23	1.516330	ν23	64.2
R40	∞

Aspherical surfaces are marked by asterisk *.
Aspherical Coefficient
R19 k = 7.27547e−01, B = −1.74498e−03, C = −4.15999e−05, D = 0.00, E = 0.00, F = 0.00
R26 k = −2.11922e+01, B = 4.97721e−04, C = 2.24620e−05, D = −1.74512e−06, E = 0.00, F = 0.00


focal length
variable distance	1.00	4.73	7.64

D14	0.29	7.11	8.41
D22	9.03	2.20	0.91
D29	1.81	1.18	2.07
D34	1.31	1.93	1.05


Numerical Embodiment 6
f	1.00-5.84	Fno	1.66-2.06	2ω	82.5-17.1

R1	39.180	D1	0.94	N1	1.712995	ν1	53.9
R2	8.296	D2	4.31
R3	−586.941	D3	0.76	N2	1.719995	ν2	50.2
R4	16.889	D4	1.70
R5	42.969	D5	1.87	N3	1.846660	ν3	23.9
R6	−28.993	D6	4.44
R7	20.532	D7	2.78	N4	1.693501	ν4	53.2
R8	−20.532	D8	0.15
R9	2981.244	D9	0.58	N5	1.846660	ν5	23.9
R10	7.932	D10	2.64	N6	1.496999	ν6	81.5
R11	−343.826	D11	0.06
R12	10.456	D12	1.55	N7	1.834000	ν7	37.2
R13	134.579	D13	variable
R14	11.099	D14	0.29	N8	1.882997	ν8	40.8
R15	2.614	D15	1.05
R16	−22.875	D16	1.20	N9	1.808095	ν9	22.8
R17	−3.697	D17	0.50	N10	1.859600	ν10	40.4
R18*	5.828	D18	0.51
R19	5.907	D19	1.13	N11	1.603420	ν11	38.0
R20	−5.907	D20	0.20	N12	1.882997	ν12	40.8
R21	−11.060	D21	variable
R22	stop	D22	0.98
R23	−5.869	D23	0.23	N13	1.638539	ν13	55.4
R24	4.135	D24	1.14	N14	1.683290	ν14	31.4
R25*	−18.230	D25	1.84
R26	29.742	D26	1.61	N15	1.548141	ν15	45.8
R27	−4.311	D27	0.29	N16	2.003300	ν16	28.3
R28	−7.073	D28	variable
R29	149.677	D29	0.73	N17	1.622992	ν17	58.2
R30	−11.179	D30	0.06
R31	11.578	D31	0.29	N18	1.846660	ν18	23.9
R32	5.987	D32	1.54	N19	1.487490	ν19	70.2
R33	−12.771	D33	variable
R34	11.426	D34	0.85	N20	1.487490	ν20	70.2
R35	−9.059	D35	0.26	N21	1.647689	ν21	33.8
R36	−104.038	D36	1.75
R37	∞	D37	5.84	N22	1.589130	ν22	61.2
R38	∞	D38	1.10	N23	1.516330	ν23	64.2
R39	∞

Aspherical surfaces are marked by asterisk *.
Aspherical Coefficient
R18 k = 5.36513e−02, B = −1.49583e−03, C = −3.74820e−05, D = 0.00000e+00, E = 0.00000e+00, F = 0.00000E+00
R25 k = −1.04670e+01, B = 8.10605e−04, C = 9.09617e−06, D = −1.95751e−07, E = 0.00000e+00, F = 0.00000E+00


focal length
variable distance	1.00	3.92	5.84

D13	0.29	6.13	7.24
D21	8.44	2.60	1.49
D28	1.83	1.30	1.82
D33	1.14	1.66	1.14


Numerical Embodiment 7
f	1.00-7.45	Fno	1.66-2.95	2ω	82.4-13.4

R1	44.646	D1	0.93	N1	1.712995	ν1	53.9
R2	9.256	D2	4.79
R3	−38.531	D3	0.85	N2	1.719995	ν2	50.2
R4	22.491	D4	1.68
R5	97.614	D5	2.34	N3	1.846660	ν3	23.9
R6	−19.144	D6	4.61
R7	19.465	D7	2.80	N4	1.603112	ν4	60.6
R8	−19.465	D8	0.35
R9	−186.277	D9	0.58	N5	1.846660	ν5	23.9
R10	10.161	D10	0.40
R11	13.429	D11	1.67	N6	1.487490	ν6	70.2
R12	−1198.396	D12

5694252	Zoom lens	December, 1997	Yahagi
7268955	Zoom lens and imager using the same	September, 2007	Ogata	359/690

JP11287952	October, 1999	REAR FOCUS TYPE ZOOM LENS
JP11287954	October, 1999	REAR FOCUS TYPE ZOOM LENS
JP2002365539	December, 2002	ZOOM LENS AND IMAGING DEVICE USING THE SAME