OBJECTIVE FOR MICROSCOPE

Abstract

An objective includes, in order from an object side, first, second, and third lens groups. The first lens group includes, in order from the object side, a first lens, a second lens, and a third lens component. When NA represents an objective numerical aperture, f represents an objective focal length, fG1 represents a first lens group focal length, r11 represents a radius of curvature of a lens surface on the object side of the first lens, r12 represents a radius of curvature of a lens surface on an image side of the first lens, and d012 represents a distance on an optical axis from a front-side focal plane of the objective to a lens surface on the image side of the first lens, the objective satisfies: 0.8≦NA<1, 1.6≦fG1/f≦6, −1.6≦r11/f≦−0.2, and −2≦r12/d012≦−0.86.

Description

CROSS REFERENCE TO RELATED APPLICATIONS

This application is a Continuation application of U.S. Ser. No. 14/885,223, filed Oct. 16, 2015, which is based upon and claims the benefit of priority from prior Japanese Patent Application No. 2014-217747, filed Oct. 24, 2014, the entire contents of both of which are incorporated herein by this reference.

BACKGROUND OF THE INVENTION

Field of the Invention

The present invention relates to an objective for a microscope.

Description of the Related Art

In recent years, the number of pixels of an image sensor has increased remarkably, and in the field of a microscope, expectations for a microscope device that enables observation and image acquisition while achieving both a wide field of view and high resolving power are increasing. As an example, when such a microscope device is employed for a virtual slide, a scanning speed can be increased.

In order to realize the microscope device above, an objective having a wide field of view (namely, a large field number and a low magnification) and a high numerical aperture is desired. Such an objective is described, for example, in Japanese Laid-Open Patent Publication No. 2010-186162 and Japanese Laid-Open Patent Publication No. 2011-75982.

SUMMARY OF THE INVENTION

An aspect of the present invention is a dry objective for a microscope. The objective includes, in order from an object side, a first lens group with positive refractive power, a second lens group with positive refractive power, the second lens group including a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and a third lens group with negative refractive power. The first lens group includes, in order from the object side, a first lens that is a single lens having a meniscus shape with a concave surface facing the object side, a second lens that is a single lens with positive refractive power, the single lens having a meniscus shape with a concave surface facing the object side, and a third lens component that is a single lens or cemented lens with positive refractive power. When NA represents a numerical aperture of the objective, f represents a focal length of the objective, f_G1 represents a focal length of the first lens group, r₁₁ represents a radius of curvature of a lens surface on the object side of the first lens, r₁₂ represents a radius of curvature of a lens surface on an image side of the first lens, and d₀₁₂ represents a distance on an optical axis from a front-side focal plane of the objective to the lens surface on the image side of the first lens, the objective satisfies the following conditional expressions:

0.8≦NA<1   (4)

1.6≦f_G1/f≦6   (5)

−1.6≦r₁₁/f≦−0.2   (6)

−2≦r₁₂/d₀₁₂≦−0.86.   (7)

Another aspect of the present invention is an immersion type objective for a microscope. The objective includes, in order from an object side, a first lens group with positive refractive power, a second lens group with positive refractive power, the second lens group including a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and a third lens group with negative refractive power. The first lens group includes, in order from the object side, a first lens that is a single lens having a meniscus shape with a concave surface facing the object side, or a first cemented lens that is configured of the first lens and a lens arranged on the object side of the first lens, a second lens that a single lens with positive refractive power, the single lens having a meniscus shape with a concave surface facing the object side, and a third lens component that is a single lens or cemented lens with positive refractive power. The third lens group includes a rear lens group with negative refractive power closest to an image side, and the rear lens group includes a fourth lens component that is a single lens or cemented lens having a meniscus shape with a concave surface facing the object side, and a fifth lens component that is arranged closer to the object side than the fourth lens component and that is a single lens or cemented lens with negative refractive power with a concave surface facing the object side. When NA represents a numerical aperture of the objective, f represents a focal length of the objective, f_G1 represents a focal length of the first lens group, r12 represents a radius of curvature of a lens surface on the image side of the first lens, and d₀₁₂ represents a distance on an optical axis from a front-side focal plane of the objective to the lens surface on the image side of the first lens, the objective satisfies the following conditional expressions:

0.8≦NA≦1.5   (8)

2.3≦f_G1/f≦8   (9)

−1.5≦r₁₂/d₀₁₂≦−0.75.   (10)

Yet another aspect of the present invention is an objective for a microscope. The objective includes, in order from an object side, a first lens group with positive refractive power, a second lens group with positive refractive power, and a third lens group with negative refractive power. When NA represents a numerical aperture of the objective, FN represents a field number of the objective, β represents a magnification of the objective, ε represents an Airy disk diameter on an axis to a d-line of the objective, φ_max represents a maximum value of an effective diameter of a lens included in the objective, and h_exp represents a radius of an exit pupil of the objective, the objective satisfies the following conditional expressions:

0.8≦NA≦1.5   (1)

1000≦FN/|β|/ε≦10000   (2)

1.7≦Φ_max/2/h_exp/NA≦4.   (3)

BRIEF DESCRIPTION OF THE DRAWINGS

The present invention will be more apparent from the following detailed description when the accompanying drawings are referenced.

FIG. 1 illustrates a configuration of a microscope device according to an embodiment of the present invention.

FIG. 2 is a sectional view of an objective in Example 1 of the present invention.

FIG. 3 is a sectional view of a tube lens used in combination with an objective.

FIG. 4A to FIG. 4D are aberration diagrams in a case in which a combination of an objective illustrated in FIG. 2 and a tube lens illustrated in FIG. 3 is used, and respectively illustrate spherical aberration, a sine condition violation amount, astigmatism, and comatic aberration.

FIG. 5 is a sectional view of an objective in Example 2 of the present invention.

FIG. 6A to FIG. 6D are aberration diagrams in a case in which a combination of an objective illustrated in FIG. 5 and a tube lens illustrated in FIG. 3 is used, and respectively illustrate spherical aberration, a sine condition violation amount, astigmatism, and comatic aberration.

FIG. 7 is a sectional view of an objective in Example 3 of the present invention.

FIG. 8A to FIG. 8D are aberration diagrams in a case in which a combination of an objective illustrated in FIG. 7 and a tube lens illustrated in FIG. 3 is used, and respectively illustrate spherical aberration, a sine condition violation amount, astigmatism, and comatic aberration.

FIG. 9 is a sectional view of an objective in Example 4 of the present invention.

FIG. 10A and FIG. 10D are aberration diagrams in a case in which a combination of an objective illustrated in FIG. 9 and a tube lens illustrated in FIG. 3 is used, and respectively illustrate spherical aberration, a sine condition violation amount, astigmatism, and comatic aberration.

FIG. 11 is a sectional view of an objective in Example 5 of the present invention.

FIG. 12A to FIG. 12D are aberration diagrams in a case in which a combination of an objective illustrated in FIG. 11 and a tube lens illustrated in FIG. 3 is used, and respectively illustrate spherical aberration, a sine condition violation amount, astigmatism, and comatic aberration.

FIG. 13 is a sectional view of an objective in Example 6 of the present invention.

FIG. 14A to FIG. 14D are aberration diagrams in a case in which a combination of an objective illustrated in FIG. 13 and a tube lens illustrated in FIG. 3 is used, and respectively illustrate spherical aberration, a sine condition violation amount, astigmatism, and comatic aberration.

FIG. 15 is a sectional view of an objective in Example 7 of the present invention.

FIG. 16A to FIG. 16D are aberration diagrams in a case in which a combination of an objective illustrated in FIG. 15 and a tube lens illustrated in FIG. 3 is used, and respectively illustrate spherical aberration, a sine condition violation amount, astigmatism, and comatic aberration.

FIG. 17 is a sectional view of an objective in Example 8 of the present invention.

FIG. 18A to FIG. 18D are aberration diagrams in a case in which a combination of an objective illustrated in FIG. 17 and a tube lens illustrated in FIG. 3 is used, and respectively illustrate spherical aberration, a sine condition violation amount, astigmatism, and comatic aberration.

FIG. 19 is a sectional view of an objective in Example 9 of the present invention.

FIG. 20A to FIG. 20D are aberration diagrams in a case in which a combination of an objective illustrated in FIG. 19 and a tube lens illustrated in FIG. 3 is used, and respectively illustrate spherical aberration, a sine condition violation amount, astigmatism, and comatic aberration.

FIG. 21 is a sectional view of an objective in Example 10 of the present invention.

FIG. 22A to FIG. 22D are aberration diagrams in a case in which a combination of an objective illustrated in FIG. 21 and a tube lens illustrated in FIG. 3 is used, and respectively illustrate spherical aberration, a sine condition violation amount, astigmatism, and comatic aberration.

FIG. 23 is a sectional view of an objective in Example 11 of the present invention.

FIG. 24A to FIG. 24D are aberration diagrams in a case in which a combination of an objective illustrated in FIG. 23 and a tube lens illustrated in FIG. 3 is used, and respectively illustrate spherical aberration, a sine condition violation amount, astigmatism, and comatic aberration.

DESCRIPTION OF THE EMBODIMENTS

Objectives described in Japanese Laid-Open Patent Publication No. 2010-186162 and Japanese Laid-Open Patent Publication No. 2011-75982 insufficiently correct comatic aberration. Therefore, when both a wider field of view and a high numerical aperture are achieved, or when vignetting is reduced and an off-axis numerical aperture is enlarged, circumference performance remarkably deteriorates due to comatic aberration. Accordingly, it is difficult to achieve both a wide field of view and high resolving power at a higher level.

In view of the foregoing, embodiments of the present invention are described below.

FIG. 1 is a schematic diagram illustrating a configuration of a microscope device 100 according to an embodiment of the present invention. The microscope device 100 illustrated in FIG. 1 includes a microscope body 2, a light source device 3 connected to the microscope body 2 via an optical fiber 4, an imaging optical system including an objective 8 and a tube lens 1, and a digital camera incorporating an image sensor 9. The microscope device 100 further includes an XY handle 6 that moves a stage 5 in a direction orthogonal to an optical axis of the objective 8, and a Z handle 7 that moves the stage 5 in a direction parallel to the optical axis of the objective 8. In addition, the microscope device 100 may include an eyepiece (not illustrated).

The objective 8 is an infinity correction type objective (a microscope objective) for a microscope. The objective 8 may be a dry objective or an immersion type objective. The objective 8 is configured to realize a wide field of view (namely, a low magnification and a large field number) and a high numerical aperture. Specifically, the objective 8 is configured so as to satisfy the following conditional expressions, although the other details are described later.

0.8≦NA1.5   (1)

1000≦FN/|β|/ε≦10000   (2)

1.7≦φ_max/2/h_exp/NA≦4   (3)

In these conditional expressions, NA represents a numerical aperture on an object side of the objective 8. FN represents a field number of the objective 8. β represents a magnification of the objective 8. ε represents an Airy disk diameter on an axis to the d-line (588 nm) of the objective 8. φ_max represents a maximum value of an effective diameter of a lens included in the objective 8. h_exp represents the radius of an exit pupil of the objective 8. The magnification of an objective corresponds to a projection magnification of a microscope optical system formed by combining a tube lens having a focal length between 160 mm and 200 mm and the objective, which is usually used for a microscope device. The field number of an objective corresponds to twice the maximum image height of the microscope optical system above formed by combining the tube lens and the objective. It can be said that, when digital observation is performed on a sample image formed by this microscope optical system by using an image sensor, the objective can deal with an image sensor having a diagonal length that is the same as a field number at the maximum.

Conditional expression (1) represents a condition for obtaining sufficient resolving power. By NA not being less than a lower limit value of conditional expression (1), an Airy disk diameter can be sufficiently reduced, and therefore sufficient resolving power can be obtained. By NA not being greater than an upper limit value of conditional expression (1), a spread angle of a marginal ray incident on the objective 8 does not excessively increase, and deterioration in performance primarily due to comatic aberration can be suppressed. Accordingly, sufficient resolving power can be obtained.

Conditional expression (2) represents a condition for obtaining sufficient resolving power and a wide field of view. By FN/|β|/ε not being less than a lower limit value of conditional expression (2), sample observation and image acquisition can be performed with a wide field of view and high resolving power while making the best use of performance of the image sensor 9 having high definition and a large size (namely, a large number of pixels) that is described later. By FN/|β|/ε not being greater than an upper limit value of conditional expression (2), an Airy disk diameter does not become small enough to exceed resolving power of the image sensor 9, and there is no need to correct aberration due to an excessively high NA. Therefore, deterioration in performance primarily due to comatic aberration can be suppressed. A value obtained by dividing a field number of an objective by a magnification of the objective is equal to twice the object height of the objective. Accordingly, when the object height of the objective is Y_ob, conditional expression (2) is synonymous with the following expression.

1000≦2×Y_ob/ε≦10000   (2A)

Conditional expression (3) represents a condition for satisfactorily correcting primarily comatic aberration so as to attain a wide field of view and high resolving power. By φ_max/2/h_exp/NA not being less than a lower limit value of conditional expression (3), there is no need to converge an off-axis pencil of light with high refractive power in an optical system in a portion located on a side of a sample S within the objective 8. Therefore, an incident angle and a refraction angle of an off-axis marginal ray to a lens surface does not excessively increase, and this allows the generation of comatic aberration to be reduced. By φ_{max /}2/h_exp/NA not being greater than an upper limit value of conditional expression (3), an outer diameter of a lens configuring the objective 8 does not excessively increase, and this prevents the objective 8 from having a large diameter. The pencil of light is a bundle of rays emitted from one point of an object (an object point).

It is preferable that the objective 8 satisfy conditional expression (2-1) and conditional expression (3-1) described below, instead of conditional expression (2) and conditional expression (3) described above, respectively, and it is further preferable that the objective 8 satisfy conditional expression (2-2) and conditional expression (3-2).

1200≦FN/|β|/ε≦8000   (2-1)

1400≦FN/|β|/ε≦6000   (2-2)

1.9≦φ_max/2/h_exp/NA≦3.5   (3-1)

2.1≦φ_max/2/h_exp/NA≦3   (3-2)

The tube lens 1 is a tube lens for a microscope that forms a magnified image of an object (sample S) by being used in combination with the objective 8. The tube lens 1 is configured so as to satisfactorily correct aberration and realize a large field number and a high numerical aperture.

The image sensor 9 is, for example, a CCD (Charge Coupled Device), a CMOS (Complementary Metal Oxide Semiconductor), or the like, and is arranged on an image plane on which a magnified image is formed by the objective 8 and the tube lens 1.

It is preferable that the image sensor 9 have a large size in order to sufficiently utilize a large field number realized by the objective 8 and the tube lens 1. It is also preferable that the image sensor 9 have high definition in order to sufficiently exhibit high imaging performance realized by the objective 8 and the tube lens 1. It is preferable that the image sensor 9 have, for example, a pixel size L (namely, a length of one side of each pixel) between 1 μm and 17 μm. This is because, when the pixel size L is greater than 17 μm, a Nyquist frequency is lower than a cut-off frequency of an imaging optical system and this prevents resolution performance of the imaging optical system from being sufficiently exhibited. This is also because, when the pixel size L is less than 1 μm, a Nyquist frequency greatly exceeds a cut-off frequency of the imaging optical system and excessively increases, and resolution performance of an image sensor is not sufficiently exhibited.

In the microscope device 100, the sample S arranged on the stage 5 is illuminated with light that is emitted from the light source device 3 and is made incident via the optical fiber 4. The illuminated sample S is magnified and projected to the image sensor 9 by the objective 8 and the tube lens 1, and a magnified image of the sample S that has been formed by the objective 8 and the tube lens 1 is captured by the image sensor 9. When the microscope device 100 includes an eyepiece, the magnified image of the sample S is observed via the eyepiece.

The microscope device 100 having the above configuration enables observation and image acquisition while achieving both a wide field of view and a high resolution.

A configuration and an action of the objective 8 are described next in detail. The objective 8 is an objective for a microscope that forms a magnified image of an object (the sample S) by being used in combination with the tube lens 1. The objective 8 is configured of the first lens group with positive refractive power, the second lens group with positive refractive power, and the third lens group with negative refractive power in order from the object side.

The first lens group gradually suppresses divergence (spreading) of a pencil of light from the object with the positive power. The second lens group gradually suppresses spreading of a pencil of divergence light from the first lens group with the positive power while correcting primarily on-axis chromatic aberration, and converts the pencil of divergence light into a pencil of convergence light. The third lens group converts the pencil of convergence light from the second lens group into a pencil of parallel light with the negative power.

In the objective 8, a ray height of an on-axis marginal ray becomes the maximum within the second lens group. More specifically, the ray height of the on-axis marginal ray becomes the maximum on a boundary surface of a lens component closest to the object in the second lens group or within the lens component. This characteristic enables a boundary between the first lens group and the second lens group, both having positive power, to be identified. Further, with regard to a boundary between the second lens group and the third lens group, a lens component with positive refractive power that is closest to the object among lens components of the objective 8 other than lens components included in the first lens group and a lens component which the maximum ray height of an on-axis marginal ray pass through is a lens component closest to the image plane in the second lens group. This characteristic enables a boundary between the second lens group with positive power and the third lens group with negative power to be identified.

In this specification, a lens component is one lens block in which only two surfaces, an object-side surface and an image-side surface, are brought into contact with air (or immersion liquid), regardless of whether this is a single lens or a cemented lens.

When the objective 8 is a dry objective for a microscope, the first lens group includes the first lens, the second lens, and the third lens component, in order from the object side. The first lens is a single lens having a meniscus shape with a concave surface facing the object side. The second lens is a single lens with positive refractive power that has a meniscus shape with a concave surface facing the object side. The third lens component is a single lens or cemented lens with positive refractive power. The first lens and the second lens may be cemented.

By arranging a single lens having a meniscus shape with a concave surface facing the object side (the first lens) closest to the object, the concave surface can be arranged in an area in which a marginal ray height is small. Accordingly, primarily field curvature can be satisfactorily corrected with divergence of a pencil of light from an object suppressed. Further, by arranging the second lens and the third lens each having positive refractive power closer to an image plane than the first lens, divergence (spreading) of a pencil of light can be gradually suppressed with the generation of spherical aberration and comatic aberration reduced.

When the objective 8 is an immersion type objective for a microscope, the first lens group includes the first lens or the first cemented lens, the second lens, and the third lens component, in order from the object side. The first cemented lens is a cemented lens that is configured of the first lens and a lens arranged on the object side of the first lens. The first cemented lens and the second lens may be cemented.

By arranging a single lens having a meniscus shape with a concave surface facing the object side (the first lens) closest to the object, the concave surface can be arranged in an area in which a marginal ray height is small. Therefore, primarily field curvature can be satisfactorily corrected with divergence of a pencil of light from an object suppressed. This point is similar to a case of a dry objective. However, in a case of an immersion type objective, it may be difficult to fill a space (a concave portion) formed by the concave surface of the first lens with immersion liquid. In this case, a lens that is made of a material having a refractive index similar to that of the immersion liquid may be cemented to the concave surface of the first lens. Further, by arranging the second lens and the third lens component each having positive refractive power closer to the image plane than the first lens, divergence (spreading) of a pencil of light can be gradually suppressed with the generation of spherical aberration and comatic aberration reduced. This point is similar to a case of a dry objective.

The second lens group includes a cemented lens that is formed of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material. The low dispersion material is a material that satisfies Abbe number υd≧65. The high dispersion material is a material that satisfies Abbe number υd≦55.

In the second lens group, a ray height of a marginal ray is great. Therefore, by the second lens group including a cemented lens that is formed of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, on-axis chromatic aberration can be effectively corrected.

When the objective 8 is an immersion type objective for a microscope, the third lens group includes a rear lens group with negative refractive power closest to the image plane. The rear lens group includes the fourth lens component, and the fifth component arranged closer to the object than the fourth lens component. The fourth lens component is a single lens or cemented lens having a meniscus shape with a concave surface facing the object side. The fifth lens component is a single lens or cemented lens with negative refractive power with a concave surface facing the object side.

The rear lens group in the third lens group converts a pencil of light into a pencil of parallel light by using the negative refractive power, and guides the pencil of parallel light to the tube lens 1. By including the fourth lens component, the rear lens group can have a concave surface of a lens arranged in an area in which a marginal ray height is small. Therefore, the Petzval sum can be corrected in a positive direction, and field curvature can be satisfactorily corrected. In addition, by including the fourth lens component, the rear lens group can have an area in which a marginal ray height is small closer to the object side than the forth lens component. By arranging the fifth lens component with negative refractive power in the area, the Petzval sum can be corrected in a positive direction, and field curvature can be satisfactorily corrected. Further, because the concave surface faces the object side, field curvature can be effectively corrected with the generation of astigmatism and comatic aberration suppressed.

A preferred configuration of the objective 8 is described below.

It is preferable that the third lens component included in the first lens group have a meniscus shape with a concave surface facing the objest side. This enables divergence of a pencil of light to be suppressed while the generation of spherical aberration and comatic aberration is reduced.

Further, it is preferable that the first lens group include the seventh lens component closer to the image plane than the third lens component. The seventh lens component is a single lens or cemented lens with positive refractive power. By arranging the seventh lens component with positive refractive power closer to the image plane than the third lens component, an optical system from the first lens to the third lens component can refract a pencil of light more gradually (in a direction in which spreading of the pencil of light is suppressed) in a state in which the first lens group has a prescribed refractive power. As a result, the generation of comatic aberration and spherical aberration can be reduced.

It is preferable that the second lens group include three-lens-cemented lenses that is configured by cementing lenses with positive refractive power that each are made of a low dispersion material on both surfaces of a lens with negative refractive power that is made of a high dispersion material. This configuration enables on-axis chromatic aberration to be corrected on both of the surfaces of the lens with negative refractive power. Therefore, in the second group in which a ray height of a merginal ray is great, on-axis chromatic aberration can be effectively corrected. Further, because a lens surface is cemented to another lens surface, the generation of spherical aberration and comatic aberration can be reduced.

Further, it is preferable that the second lens group include an aspherical lens that has a lens surface having an aspherical shape. It is preferable that the aspherical shape be an aspherical shape with positive refractive power on the optical axis, and be an aspherical shape in which positive refractive power decreases towards a peripheral portion of the lens surface. By arranging the aspherical lens described above in the second group in which a ray height of a marginal ray is great, spherical aberration and comatic aberration can be satisfactorily corrected.

It is preferable that the third lens group be configured of a front lens group, an intermediate lens group, and a rear lens group, in order from the object side. The front lens group is a lens group arranged closest to the object in the third lens group, and has a focal length that satisfies conditional expression (12) described later. This characteristic enables a boundary between the front lens group and the intermediate lens group to be identified. The front lens group plays a role in correcting on-axis chromatic aberration while gradually reducing a ray height of a marginal ray that has been converted in a convergence direction by the second lens group.

The intermediate lens group is a lens group arranged between the front lens group and the rear lens group. The intermediate lens group plays a different role depending on whether the objective 8 is a dry objective or an immersion type objective. When the objective 8 is a dry objective, the intermediate lens group plays a role in correcting the Petzval sum in a positive direction and further outputting a pencil of light as a pencil of convergence light. This corresponds to actions of an image-side portion of an optical system that is referred to as a so-called gauss group and an object-side portion of an optical system that is referred to as a wide converter. When the objective 8 is an immersion type objective, the intermediate lens group plays a role in correcting the Petzval sum in a positive direction and reducing a marginal ray height of an on-axis pencil of light. This corresponds to an action of an object-side portion of an optical system that is referred to as a so-called gauss group.

The rear lens group is a lens group arranged closest to the image plane in the third lens group. The rear lens group has a different characteristic depending on whether the objective 8 is a dry objective or an immersion type objective. When the objective 8 is a dry objective, the rear lens group has negative refractive power, and has a characteristic whereby an air space between the intermediate lens group and the rear lens group becomes greatest in the objective 8. When the objective 8 is an immersion type objective, the rear lens group has a characteristic whereby an on-axis marginal ray height becomes smallest within a lens component closest to the object in the rear lens group or on a boundary surface of the lens component. These characteristics enable a boundary between the intermediate lens group and the rear lens group to be identified. The rear lens group plays a role in converting an on-axis pencil of light into a pencil of parallel light. This corresponds to actions of an image-side portion of an optical system that is referred to as a so-called gauss group and an image-side portion of an optical system that is referred to as a wide converter. The rear lens group also plays a role in correcting the Petzval sum in a positive direction and converting the on-axis pencil of light into a pencil of parallel light having a prescribed exit pupil diameter. This corresponds to an action of an image-side portion of an optical system that is referred to as a so-called gauss group.

It is preferable that the front lens group include the eighth lens and the ninth lens that are arranged so as to be adjacent to each other. The eighth lens is a lens with positive refractive power that is made of a low dispersion material, and the ninth lens is a lens with negative refractive power that is made of a high dispersion material. A ninth-lens-side lens surface of the eighth lens and an eighth-lens-side lens surface of the ninth lens have a radius of curvature having the same sign. In other words, lens surfaces adjacent to each other are bent in the same direction.

The front lens group has an action of correcting on-axis chromatic aberration while gradually refracting a marginal ray that has been converted in a convergence direction (so as to enter into a convergence state) by the second lens group so as to reduce a ray height of the marginal ray. By the front lens group having the eighth lens and the ninth lens described above, on-axis chromatic aberration can be satisfactorily corrected. By these lenses being arranged so as to be adjacent to each other and by adjacent lens surfaces being bent in the same direction, the generation of comatic aberration and spherical aberration can be reduced. The eighth lens and the ninth lens may be cemented.

When the objective 8 is a dry objective for a microscope, it is preferable that the intermediate lens group include the tenth lens component. The tenth lens component is configured of a single lens or cemented lens having a meniscus shape with a concave surface facing the object side. By arranging the tenth lens component described above in a prescribed position between the front lens group and the rear lens group, a ray height of a marginal ray on a concave surface (on the object side) of the tenth lens component can be smaller than the ray height of the marginal ray on a convex surface (on the image side). As a result, the Petzval sum can be corrected in a positive direction, and field curvature can be satisfactorily corrected. In addition, because the concave surface faces the object side, an incident angle and an exit angle of an off-axis pencil of light do not excessively increase, and the generation of comatic aberration can be reduced.

In this case, it is preferable that the intermediate lens group further include the thirteenth lens with positive refractive power on the image side of the tenth lens component. This enables the thirteenth lens to have a portion of positive refractive power that a convex surface of the tenth lens component originally has, and therefore the generation of spherical aberration and comatic aberration can be suppressed.

When the objective 8 is an immersion type objective for a microscope, it is preferable that the intermediate lens group include the twelfth lens component. The twelfth lens component is configured of a single lens or cemented lens having a meniscus shape with a convex surface facing the object side. It is difficult for an immersion type objective for a microscope to sufficiently correct the Petzval sum on a concave surface closest to the object. Therefore, the third lens group is desired to have an action of correcting a greater Petzval sum, compared with a case in which the objective 8 is a dry objective for a microscope. By arranging the twelfth lens component in the intermediate lens group, a ray height of a marginal ray on a concave surface (on the image side) of the twelfth lens component can be smaller than the ray height of the marginal ray on a convex surface (on the object side). As a result, field curvature can be made satisfactory. Further, because the convex surface of the twelfth lens component faces the object side, a marginal ray height can be reduced in an area on the image side of the intermediate lens group, namely, in an area on the object side of the rear lens group. As a result, the Petzval sum can be corrected more effectively.

When the objective 8 is a dry objective for a microscope, it is preferable that the rear lens group have negative refractive power and that field curvature be satisfactorily corrected by using the negative refractive power. However, when a radius of curvature of a concave surface excessively decreases, at least one of comatic aberration and astigmatism is greatly generated. In view of this, it is preferable that the rear lens group include two or more lens components with negative refractive power. By the two or more lens components sharing negative refractive power, the rear lens group can have a prescribed negative refractive power, and a radius of curvature of each of the lens components can be prevented from excessively decreasing. As a result, the generation of comatic aberration and astigmatism can be reduced.

When the objective 8 is an immersion type objective, it is preferable that the rear lens group include the eleventh lens component that is arranged closer to the object than the fourth lens component. The eleventh lens component is a single lens or cemented lens with negative refractive power. By the rear lens group including the eleventh lens component with negative refractive power separately from the fourth lens component having an action of correcting the Petzval sum, the generation of astigmatism and comatic aberration can be suppressed, and field curvature can be corrected more effectively.

Regardless of whether the objective 8 is a dry objective for a microscope or an immersion type objective for a microscope, it is preferable that the rear lens group include an aspherical lens that has a lens surface having an aspherical shape. It is preferable that the aspherical shape be an aspherical shape with negative refractive power on the optical axis, and be an aspherical shape in which negative refractive power decreases towards a peripheral portion of the lens surface. By arranging the aspherical lens described above in the rear lens group in which an off-axis ray height is great, field curvature and astigmatism can be effectively corrected. It is also preferable that the rear lens group have a diffractive optical element with negative refractive power. This enables chromatic aberration of magnification to be satisfactorily corrected. Even when a lens with positive refractive power that is made of a high dispersion material is arranged in the rear lens group, a similar effect can be attained to some extent. However, by arranging a diffractive optical element, chromatic aberration of magnification of a g-line can be more surely prevented from being excessively corrected.

Regardless of whether the objective 8 is a dry objective for a microscope or an immersion type objective for a microscope, it is preferable that the objective 8 include the sixth lens with positive refractive power that is made of a material having a high partial dispersion. By the objective 8 including the sixth lens, on-axis chromatic aberration of a g-line that is excessively corrected when correcting on-axis chromatic aberration by using a combination of a low-dispersion negative lens and a high-dispersion positive lens can be satisfactorily corrected. The material having a high partial dispersion is a material that satisfies (n_g−n_F)/(n_F−n_C)≧0.58, where n_g, n_F, and n_C respectively represent refractive indices of a material to a g-line, an F-line, and a C-line. As an example, a material such as NBH53, TIH3, or TIH53 of OHARA INC. falls under this material. When the objective 8 is a dry objective for a microscope, it is preferable that the sixth lens be included in the intermediate lens group. In particular, it is preferable that the sixth lens be included in a meniscus lens component included in the intermediate lens group or that the sixth lens be arranged on the image side of the meniscus lens component included in the intermediate lens group. In this case, the sixth lens is arranged in an area in which a marginal ray height is relatively great, and therefore compensation for chromatic aberration of a g-line that has been excessively corrected as described above and correction of field curvature can be performed simultaneously.

Conditions satisfied by the objective 8 are described below.

When the objective 8 is a dry objective, the objective 8 is configured so as to satisfy conditional expression (4) to conditional expression (7) described below.

0.8≦NA<1   (4)

1.6≦f_G1/f≦6   (5)

−1.6≦r₁₁/f≦−0.2   (6)

−2≦r₁₂/d₀₁₂≦−0.86   (7)

When the objective 8 is an immersion type objective, the objective 8 is configured so as to satisfy conditional expression (8) to conditional expression (10) described below.

0.8≦NA≦1.5   (8)

2.3≦f_G1/f≦8   (9)

−1.5≦r₁₂/d₀₁₂≦−0.75   (10)

In these conditional expressions, NA represents a numerical aperture of the objective 8. f represents a focal length of the objective 8. f_G1 represents a focal length of the first lens group. r₁₁ represents a radius of curvature of a lens surface on the object side of the first lens. r₁₂ represents a radius of curvature of a lens surface on the image side of the first lens. d₀₁₂ represents a distance on the optical axis from a front-side focal plane (namely, an object surface) of the objective 8 to a lens surface on the image side of the first lens.

Conditional expression (4) and conditional expression (8) are conditional expressions required to obtain sufficient resolving power. By NA being not less than lower limit values of conditional expression (4) and conditional expression (8), an Airy disk diameter can be reduced sufficiently, and therefore sufficient resolving power can be obtained. When the objective 8 is a dry objective, NA does not exceed 1. When the objective 8 is an immersion type objective, a spread angle of a marginal ray incident on the objective 8 does not increase excessively by NA not being greater than an upper limit value of conditional expression (8), and therefore performance deterioration primarily due to comatic aberration can be suppressed. Accordingly, sufficient resolving power can be obtained.

Conditional expression (5) and conditional expression (9) are conditional expressions to satisfactorily correct primarily comatic aberration. By f_m/f not being less than a lower limit value of a conditional expression according to the type of an objective (a dry objective or an immersion type objective) (here, conditional expression (5) or conditional expression (9)), a focal length of the first lens group does not decrease excessively. This can also prevent a focal length of each of the lenses that configures the first lens group from decreasing excessively. As a result, the generation of comatic aberration in the first lens group can be reduced, and comatic aberration of the entirety of the objective 8 can be satisfactorily corrected. By f_G1/f not being greater than an upper limit value of the conditional expression, a focal length of the first lens group does not increase excessively, and therefore an excessive increase in an off-axis marginal ray height in the second lens group can be avoided. Accordingly, the generation of comatic aberration in the second lens group can be reduced, and comatic aberration of the entirety of an objective can be satisfactorily corrected. When conditional expression (5) and conditional expression (9) are compared, upper limit values and lower limit values are different from each other. This results from a smaller convergence (spreading suppression) action of a pencil of light in the first lens group of an immersion type objective, compared with a dry objective, because, in the immersion type objective, a lens surface closest to the object is in contact with immersion liquid.

Conditional expression (6) is a conditional expression to satisfactorily correct primarily field curvature, spherical aberration, and comatic aberration. By r₁₁/f not being less than a lower limit value of conditional expression (6), a radius of curvature of a concave surface that is a lens surface on the objective side of the first lens does not excessively increase. Therefore, a correction amount of the Petzval sum in a positive direction does not excessively decrease, and field curvature can be satisfactorily corrected. In addition, incident angles and refraction angles of on-axis and off-axis marginal rays to a lens surface do not excessively increase, and therefore spherical aberration and comatic aberration can be satisfactorily corrected. By r₁₁/f not being greater than an upper limit value of conditional expression (6), a radius of curvature of a concave surface that is a lens surface on the object side of the first lens does not excessively decrease. Therefore, spreading of on-axis and off-axis pencils of light can be suppressed sufficiently, and the generation of spherical aberration and comatic aberration can be reduced on a lens surface on the image side of the first lens and in an optical system closer to the image plane than the first lens.

Conditional expression (7) and conditional expression (10) are conditional expressions to satisfactorily correct primarily spherical aberration and comatic aberration. By r₁₂/d_o12 not being less than a lower limit value of a conditional expression according to the type of an objective (a dry objective or an immersion type objective) (here, conditional expression (7) or conditional expression (10)), a radius of curvature of a convex surface that is a lens surface on the image side of the first lens does not increase excessively. Therefore, spreading of on-axis and off-axis pencils of light can be suppressed sufficiently, and the generation of spherical aberration and comatic aberration can be reduced in an optical system closer to the image plane than the first lens. By r₁₂/d₀₁₂ not being greater than an upper limit value of the conditional expression, a radius of curvature of a convex surface that is a lens surface on the image side of the first lens does not decrease excessively. Therefore, incident angles and refraction angles of on-axis and off-axis marginal rays to a lens surface do not increase excessively, and as a result, spherical aberration and comatic aberration can be satisfactorily corrected. When conditional expression (7) and conditional expression (10) are compared, upper limit values and lower limit values are different from each other. This results from a smaller convergence (spreading suppression) action of a pencil of light on an object-side surface of the first lens in an immersion type objective than that of a dry objective, because a lens surface closest to the object side in the immersion type objective is in contact with immersion liquid.

When the objective 8 is a dry objective, it is preferable that the objective 8 satisfy conditional expression (5-1) to conditional expression (7-1) described below, instead of conditional expression (5) to conditional expression (7) described above, respectively, and it is further preferable that the objective 8 satisfy conditional expression (5-2) to conditional expression (7-2). When the objective 8 is an immersion type objective, it is preferable that the objective 8 satisfy conditional expression (9-1) and conditional expression (10-1) described below, instead of conditional expression (9) and conditional expression (10) described above, respectively, and it is further preferable that the objective satisfy conditional expression (9-2) and conditional expression (10-2).

1.9≦f_G1/f≦4.5   (5-1)

2.1≦f_G1/f≦3.5   (5-2)

−1.53≦r₁₁/f≦−0.6   (6-1)

−1.46≦r₁₁/f≦−1   (6-2)

−1.75≦r₁₂/d₀₁₂≦−0.95   (7-1)

−1.5≦r₁₂/d₀₁₂≦−1.05   (7-2)

2.55≦f_G1/f≦6   (9-1)

2.8≦f_G1/f≦4   (9-2)

−1.3≦r₁₂/d₀₁₂≦−0.8   (10-1)

−1.1≦r₁₂/d_012≦−0.9   (10-2)

Conditions that the objective 8 preferably satisfies are described below.

It is preferable that the objective 8 satisfy conditional expression (11) to conditional expression (14) described below.

0.2≦D_ogFD_0L≦0.87   (11)

−0.3≦f/f_G30≦0.3   (12)

0.05≦f_G1/f_L2≦0.6   (13)

0.03≦f_G1/f_L3≦0.5   (14)

In these conditional expressions, D_ogF represents a distance on the optical axis from a front-side focal plane (an object surface) of the objective 8 to a lens surface on the image side of the sixth lens. D_oL represents a distance on the optical axis from a front focal plane (an object surface) of the objective 8 to a lens surface closest to the image plane of the objective 8. f_G30 represents a focal length of a front lens group. f_L2 represents a focal length of the second lens. f_L3 represents a focal length of the third lens component.

Conditional expression (11) is a conditional expression relating to a position of the sixth lens in the objective 8. By D_ogF/D_oL satisfying conditional expression (11), the sixth lens can be arranged in an area in which a marginal ray height is great. Therefore, excessive correction of on-axis chromatic aberration of a g-line can be efficiently compensated for. In particular, by D_ogF/D_oL not being greater than an upper limit value of conditional expression (11), the sixth lens can be arranged in an area in which an off-axis principal ray height is small. Therefore, chromatic aberration of magnification of a g-line can be prevented from being excessively corrected.

Conditional expression (12) is a conditional expression relating to a focal length of a rear lens group. By f/f_G30 not being greater than an upper limit value of conditional expression (12), a convergence action of the rear lens group does not excessively increase. Therefore, a marginal ray can gradually pass through the rear lens group without being suddenly refracted. As a result, on-axis chromatic aberration can be effectively corrected while the generation of comatic aberration and spherical aberration is reduced. By f/f_G30 not being less than a lower limit value of condition expression (12), a divergence action in the rear lens group does not excessively increase, and a marginal ray height can be sufficiently reduced within the rear lens group and in an optical system closer to the image plane than the rear lens group.

Conditional expression (13) is a conditional expression to satisfactorily correct primarily comatic aberration and spherical aberration. By f_G1/f_L2 not being greater than an upper limit value of conditional expression (13), a focal length of the second lens does not excessively decrease. Therefore, divergence (spreading) of a pencil of light can be gradually suppressed while the generation of spherical aberration and comatic aberration is reduced. By f_G1/f_L2 not being less than a lower limit value of conditional expression (13), a focal length of the second lens does not excessively increase. Therefore, the first lens group can have prescribed refractive power without an excessive increase in refractive power of other positive lenses that configure the first lens group. Therefore, in the first lens group, divergence (spreading) of a pencil of light can be gradually suppressed while the generation of spherical aberration and comatic aberration is reduced.

Conditional expression (14) is a conditional expression to satisfactorily correct primarily comatic aberration and spherical aberration. By f_G1/f_L3 not being greater than an upper limit value of conditional expression (14), a focal length of the third lens component does not excessively decrease. Therefore, divergence (spreading) of a pencil of light can be gradually reduced while the generation of spherical aberration and comatic aberration is reduced. By f_G1/f_L3 not being less than a lower limit value of conditional expression (14), a focal length of the third lens component does not excessively increase. The first lens group can have prescribed refractive power without an excessive increase in refractive power of other positive lenses that configure the first lens group. Therefore, in the first lens group, divergence (spreading) of a pencil of light can be gradually suppressed while the generation of spherical aberration and comatic aberration is reduced.

It is preferable that the objective 8 satisfy conditional expression (11-1) to conditional expression (14-1) described below, instead of conditional expression (11) to conditional expression (14) described above, respectively, and it is further preferable that the objective 8 satisfy conditional expression (11-2) to conditional expression (14-2).

0.3≦D_ogF/D_oL≦0.83   (11-1)

0.38≦D_ogF/D_oL≦0.75   (11-2)

−0.25≦f/f_G30≦0.2   (12-1)

−0.2≦f/f_G30≦0.11   (12-2)

0.1≦f_G1/f_L2≦0.5   (13-1)

0.15≦f_G1/f_L2≦0.4   (13-2)

0.05≦f_G1/f_L3≦0.4   (14-1)

0.07≦f_G1/f_L3≦0.3   (14-2)

When the objective 8 is a dry objective, it is preferable that the objective 8 satisfy conditional expression (15) and conditional expression (16) described below.

−10≦f_G3I/f≦−1.5   (15)

0.8≦r₂₁/r₁₂≦2   (16)

In these conditional expressions, f_G3I represents a focal length of the rear lens group. r12 represents a radius of curvature of a lens surface on the image side of the first lens. r₂₁ represents a radius of curvature of a lens surface on the object side of the second lens.

Conditional expression (15) is a conditional expression to satisfactorily correct primarily field curvature.

Considering that light from the rear lend group is parallel light, by f_G3I/f not being less than a lower limit value of conditional expression (15), a marginal ray height in the rear lens group can be sufficiently reduced, compared with a lens group closer to the object than the rear lens group. In addition, the rear lens group can have sufficient negative refractive power, and therefore a correction amount of the Petzval sum in a positive direction does not excessively decrease, and field curvature can be satisfactorily corrected. By f_G3I/f not being greater than an upper limit value of conditional expression (15), negative refractive power of the rear lens group does not excessively increase, and a marginal ray height does not excessively increase in a lens group closer to the object than the rear lens group. Therefore, the generation of comatic aberration and spherical aberration can be reduced.

Conditional expression (16) is a conditional expression to satisfactorily correct primarily spherical aberration and comatic aberration. By r₂₁/r₁₂ not being greater than an upper limit value of conditional expression (16), a radius of curvature of a concave surface that is a lens surface on the object side of the second lens does not excessively increase. Therefore, incident angles and refraction angles of on-axis and off-axis marginal rays to the lens surface do not excessively increase, and spherical aberration and comatic aberration can be satisfactorily corrected. By r₂₁/r₁₂ not being less than a lower limit value of conditional expression (16), a radius of curvature of a concave surface that is a lens surface on the object side of the second lens does not excessively decrease. Therefore, divergence (spreading) of on-axis and off-axis pencils of light can be sufficiently suppressed.

It is preferable that the objective 8 satisfy conditional expression (15-1) and conditional expression (16-1) described below, instead of conditional expression (15) and conditional expression (16) described above, respectively, and it is further preferable that the objective 8 satisfy conditional expression (15-2) and conditional expression (16-2).

−7.5≦f_G3I/f≦−2   (15-1)

−5≦f_G3I/f≦−2.5   (15-2)

1≦r₂₁/r₁₂ ≦1.7   (16-1)

1.2≦r₂₁/r₁₂≦1.4   (16-2)

When the objective 8 is a dry objective, an arbitrary combination of conditional expression (11) to conditional expression (16) may be adopted for an objective that satisfies conditional expressions (4) to (7). When the objective 8 is an immersion type objective, an arbitrary combination of conditional expression (11) to conditional expression (14) may be adopted for an objective that satisfies conditional expressions (8) to (10). Respective expressions may be limited merely by one of an upper limit value and a lower limit value.

The objective 8 can realize a microscope objective having a wide field of view and a high numerical aperture with aberration satisfactorily corrected. Examples of the objective 8 above are described below in detail. Example 1 to Example 5 describe a dry objective, and Example 6 and examples that follow describe an immersion type objective.

EXAMPLE 1

FIG. 2 is a sectional view of an objective 11 in this example. The objective 11 illustrated in FIG. 2 is a dry objective for a microscope. The objective 11 is configured of the first lens group G1 with positive refractive power, the second lens group G2 with positive refractive power including a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and the third lens group G3 with negative refractive power, in order from the object side.

The first lens group G1 is configured of a cemented lens CL1 that is configured of a meniscus lens L1 (the first lens) with negative refractive power with a concave surface facing the object side and a meniscus lens L2 (the second lens) with positive refractive power with a concave surface facing the object side, a cemented lens CL2 (the third lens component) that is configured of a meniscus lens L3 with negative refractive power with a concave surface facing the object side and a meniscus lens L4 with positive refractive power with a concave surface facing the object side, and a cemented lens CL3 (the seventh lens component) that is configured of a meniscus lens L5 with negative refractive power with a concave surface facing the object side and a meniscus lens L6 with positive refractive power with a concave surface facing the object side, in order from the object side.

The second lens group G2 is configured of a three-lens-cemented lens CL4 that is configured of a biconvex lens L7, a biconcave lens L8, and a biconvex lens L9, and a cemented lens CL5 that is configured of a meniscus lens L10 with negative refractive power with a concave surface facing the image side and a biconvex lens L11, in order from the object side.

The third lens group G3 is configured of the 3o-th lens group (the front lens group), the 3c-th lens group (the intermediate lens group), and the 3i-th lens group (the rear lens group), in order from the object side. The 3o-th lens group is configured of a meniscus lens L12 with negative refractive power with a concave surface facing the image side, a biconvex lens L13 (the eighth lens), and a meniscus lens L14 (the ninth lens) with negative refractive power with a concave surface facing the object side, in order from the object side. The 3c-th lens group is configured of a cemented lens CL6 (the tenth lens component) that is configured of a meniscus lens L15 with negative refractive power with a concave surface facing the object side and a meniscus lens L16 (the sixth lens; NBH53 of OHARA INC.) with positive refractive power with a concave surface facing the object side, and a biconvex lens L17, in order from the object side. The 3i-th lens group is configured of a meniscus lens L18 with negative refractive power with a concave surface facing the image side, and a cemented lens CL7 that is configured of a meniscus lens L19 with negative refractive power with a concave surface facing the object side and a meniscus lens L20 with positive refractive power with a concave surface facing the object side, in order from the object side.

Various pieces of data of the objective 11 are described below. The d-line (587.56 nm) is used for a reference wavelength. f_G2 represents a focal length of the second lens group G2, and f_L7 represents a focal length of the seventh lens component. E represents a power of 10.

NA=0.85, FN=30 mm, |β|=20, ε=8.43E−04 mm, f=9 mm, f_G1=30.11 mm, r₁₁=−12.2481 mm, r₁₂=−17.8211 mm, d_o12=12.182 mm, Φ_max/2=19.05 mm, h_exp=7.65 mm, f_G30=−196.64 mm, f_G3I=−30.23 mm, r₂₁ =−17.8211 mm, D_oL=133.000 mm, D_ogF=90.312 mm, f_L2=196.11 mm, f_L3=66.55 mm

Lens data of the objective 11 is described below. “INF” in the lens data represents infinity (∞).

Objective 11
s	r	d	nd	νd	er
s1(object	INF	0.150	1.52100	56.02	0.75
surface)
s2	INF	1.942			0.85
s3	−12.2481	10.090	1.88300	40.76	3.39
s4	−17.8211	4.612	1.60300	65.44	9.46
s5	−16.9951	0.100			11.64
s6	−23.7081	1.043	1.63779	42.41	12.48
s7	−28.2010	5.361	1.60300	65.44	13.32
s8	−16.3520	0.100			13.94
s9	−40.7739	0.838	1.63779	42.41	15.49
s10	−55.9945	4.018	1.49702	81.54	16.04
s11	−28.6925	0.100			16.46
s12	35.2415	14.308	1.43876	94.93	18.69
s13	−30.8526	1.500	1.63779	42.41	18.54
s14	72.9560	8.018	1.43876	94.93	18.97
s15	−42.3220	0.100			19.05
s16	50.1825	1.300	1.63779	42.41	18.26
s17	20.2794	11.485	1.43876	94.93	16.84
s18	−94.5855	0.200			16.77
s19	101.8945	1.000	1.63779	42.41	16.26
s20	33.4896	0.100			15.67
s21	30.4321	7.731	1.43876	94.93	15.70
s22	−50.4634	0.624			15.62
s23	−42.0010	1.000	1.67305	38.15	15.59
s24	−1706.2591	5.818			15.61
s25	−23.7887	1.891	1.48751	70.23	15.61
s26	−162.4849	6.884	1.73806	32.26	17.41
s27	−31.7625	4.144			17.95
s28	74.7972	5.430	1.63779	42.41	17.18
s29	−199.8224	25.089			16.83
s30	290.9229	1.000	1.49702	81.54	9.57
s31	34.8878	5.025			9.16
s32	−15.6607	1.000	1.49702	81.54	9.02
s33	−663.5991	1.000	1.63779	42.41	9.51
s34	−53.4597	−23.576			9.54

Here, s represents a surface number, r represents a radius of curvature (mm), d represents a surface spacing (mm), nd represents a refractive index to the d-line, υd represents an Abbe number, and er represents an effective radius (mm). These symbols are similar in the following examples. Surfaces represented by surface numbers s1 and s2 are respectively an object surface (a surface on the object side of a cover glass) and a surface on the image side of the cover glass, and surfaces represented by surface numbers s3 and s34 are respectively a lens surface closest to the object and a lens surface closest to the image plane in an objective. As an example, surface spacing d1 represents a distance from a surface represented by surface number s1 to a surface represented by surface number s2. A last value of a surface spacing represents a distance from a lens surface closest to the image plane in an objective to an exit pupil position. A minus value represents that an exit pupil position is located closer to the object than a lens surface closest to the image plane in an objective.

The objective 11 satisfies conditional expressions (1) to (7) and (11) to (16), as described below. A field number FN and a magnification β are values in a case in which the objective 11 is used in combination with the tube lens 10. This point is similar in all of Example 1 to Example 11.

NA=0.85   (1), (4):

FN/|β|/ε=1780   (2):

Φ_max/2/h_exp/NA=−2.93   (3):

f_c1/f=3.35   (5):

r₁₁/f=−1.36   (6):

r₁₂/d₀₁₂=−1.46   (7):

D_ogF/D_oL=0.68   (11):

f/f_G30=−0.05   (12):

f_G1/f_L2=0.15   (13):

f_G1/f_L3=0.45   (14):

f_G3I/f=−3.36   (15):

r₂₁/r₁₂=1.00   (16):

FIG. 3 is a sectional view of the tube lens 10 used in combination with the objective 11. FIG. 4A to FIG. 4D are aberration diagrams in a case in which a combination of the objective 11 and the tube lens 10 illustrated in FIG. 3 is used. FIG. 4A illustrates spherical aberration, FIG. 4B illustrates a sine condition violation amount, FIG. 4C illustrates astigmatism, and FIG. 4D illustrates comatic aberration. In these diagrams, “M” represents a meridional component, and “S” represents a sagittal component. Respective aberration diagrams including diagrams in Example 2 and examples that follow illustrate aberration that is output when the first surface s1 of the tube lens 10 is made to coincide with an exit pupil position of an objective. A configuration of the tube lens 10 illustrated in FIG. 3 is described later.

EXAMPLE 2

FIG. 5 is a sectional view of an objective 12 in this example. The objective 12 illustrated in FIG. 5 is a dry objective for a microscope. The objective 12 is configured of the first lens group G1 with positive refractive power, the second lens group G2 with positive refractive power that includes a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and the third lens group G3 with negative refractive power, in order from the object side.

The first lens group G1 is configured of a meniscus lens L1 (the first lens) with negative refractive power with a concave surface facing the object side, a meniscus lens L2 (the second lens) with positive refractive power with a concave surface facing the object side, a meniscus lens L3 (the third lens component) with positive refractive power with a concave surface facing the object side, and a meniscus lens L4 (the seventh lens component) with positive refractive power with a concave surface facing the object side, in order from the object side.

The second lens group G2 is configured of a three-lens-cemented lens CL1 that is configured of a biconvex lens L5, a biconcave lens L6, and a biconvex lens L7, and a cemented lens CL2 that is configured of a meniscus lens L8 with negative refractive power with a concave surface facing the image side and a biconvex lens L9, in order from the object side.

The third lens group G3 is configured of the 3o-th lens group (the front lens group), the 3c-th lens group (the intermediate lens group), and the 3i-th lens group (the rear lens group), in order from the object side. The 3o-th lens group is configured of a cemented lens CL 3 that is configured of a meniscus lens L10 (the ninth lens) with negative refractive power with a concave surface facing the image side and a meniscus lens L11 (the eighth lens) with positive refractive power with a concave surface facing the image side, and a meniscus lens L12 with negative refractive power with a concave surface facing the image side, in order from the object side. The 3c-th lens group is configured of a cemented lens CL4 (the tenth lens component) that is configured of a meniscus lens L13 with negative refractive power with a concave surface facing the object side and a meniscus lens L14 (the sixth lens; NBH53 of OHARA INC.) with positive refractive power with a concave surface facing the object side, and a biconvex lens L15, in order from the object side. The 3i-th lens group is configured of a biconcave lens L16, and a meniscus lens L17 with negative refractive power with a concave surface facing the object side, in order from the object side.

Various pieces of data of the objective 12 are described below. The d-line (587.56 nm) is used for a reference wavelength.

NA=0.9, FN=30 mm, |β|=20, ε=7.96E−04 mm, f=9 mm, f_G1=19.422 mm, r₁₁=−9.8587 mm, r₁₂=−13.0211 mm, d_o12=11.431 mm, Φ_max/2−16.15 mm, h_exp=8.10 mm, f_G30−−52.9824 mm, f_G3I=−29.147 mm, r₂₁=−16.8701 mm, D_cL=100.382 mm, D_ogF=82.791 mm, f₁₂=57.08 mm, f_L3=238.45 mm

Lens data of the objective 12 is described below.

Objective 12
s	r	d	nd	νd	er
s1(object	INF	0.150	1.52100	56.02	0.75
surface)
s2	INF	1.390			0.86
s3	−9.8587	9.891	1.88300	40.76	2.93
s4	−13.0211	1.258			8.83
s5	−16.8701	3.652	1.67790	55.34	9.99
s6	−12.7760	0.100			10.77
s7	−20.8962	3.754	1.60300	65.44	11.78
s8	−19.4778	0.100			13.02
s9	−55.3230	2.940	1.49700	81.54	14.08
s10	−28.0702	0.100			14.33
s11	24.5700	8.491	1.43875	94.93	16.06
s12	−80.5777	0.800	1.63775	42.41	15.92
s13	19.5830	10.948	1.43875	94.93	14.97
s14	−38.5327	0.100			15.01
s15	27.6315	0.800	1.63775	42.41	14.10
s16	14.3420	10.337	1.43875	94.93	12.71
s17	−46.3046	0.200			12.60
s18	22.3981	0.800	1.63775	42.41	11.38
s19	11.2096	5.812	1.49700	81.54	9.98
s20	45.0258	0.100			9.77
s21	44.9455	0.800	1.63775	42.41	9.74
s22	15.3887	7.272			9.03
s23	−11.7080	0.800	1.48749	70.23	9.03
s24	−45.2675	12.197	1.73800	32.26	10.38
s25	−20.2331	0.100			13.21
s26	82.3763	3.191	1.67790	55.34	13.16
s27	−65.0281	9.354			13.10
s28	−80.8182	0.800	1.49700	81.54	10.35
s29	37.0824	3.163			9.98
s30	−31.4348	0.983	1.49700	81.54	9.96
s31	−254.1359	−25.918			10.13

The objective 12 satisfies conditional expressions (1) to (7) and (11) to (16), as described below.

NA=0.9   (1), (4):

FN/|β|/ε =1885   (2):

Φ_max/2/h_exp/NA=2.22   (3):

f_G1/f=2.16   (5):

r₁₁/f=−1.10   (6):

r₁₂/d₀₁₂=−1.14   (7):

D_ogF/D_oL=0.82   (11):

f/f_G30=−0.17   (12):

f_G1/f_L2=0.34   (13):

f_G1/f_L3=0.08   (14):

f_G3I/f=−3.24   (15):

r₂₁/r₁₂=1.30   (16):

FIG. 6A to FIG. 6D are aberration diagrams in a case in which a combination of the objective 12 and the tube lens 10 is used. FIG. 6A illustrates spherical aberration, FIG. 6B illustrates a sine condition violation amount, FIG. 6C illustrates astigmatism, and FIG. 6D illustrates comatic aberration.

EXAMPLE 3

FIG. 7 is a sectional view of an objective 13 in this example. The objective 13 illustrated in FIG. 7 is a dry objective for a microscope. The objective 13 is configured of the first lens group G1 with positive refractive power, the second lens group G2 with positive refractive power that includes a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and the third lens group G3 with negative refractive power, in order from the object side.

The first lens group G1 is configured of a meniscus lens L1 (the first lens) with negative refractive power with a concave surface facing the object side, a meniscus lens L2 (the second lens) with positive refractive power with a concave surface facing the object side, a meniscus lens L3 (the third lens component) with positive refractive power with a concave surface facing the object side, and a meniscus lens L4 (the seventh lens component) with positive refractive power with a concave surface facing the object side, in order from the object side.

The second lens group G2 is configured of a three-lens-cemented lens CL1 that is configured of a biconvex lens L5, a biconcave lens L6, and a biconvex lens L7, and a cemented lens CL2 that is configured of a meniscus lens L8 with negative refractive power with a concave surface facing the image side and a biconvex lens L9, in order from the object side.

The third lens group G3 is configured of the 3o-th lens group (the front lens group), the 3c-th lens group (the intermediate lens group), and the 3i-th lens group (the rear lens group), in order from the object side. The 3o-th lens group is configured of a cemented lens CL3 that is configured of a meniscus lens L10 (the ninth lens) with negative refractive power with a concave surface facing the image side and a biconvex lens L11 (the eighth lens), and a biconcave lens L12, in order from the object side. The 3c-th lens group is configured of a cemented lens CL 4 (the tenth lens component) that is configured of a meniscus lens L13 with negative refractive power with a concave surface facing the object side and a meniscus lens L14 (the sixth lens; NBH53 of OHARA INC.) with positive refractive power with a concave surface facing the object side, and a biconvex lens L15, in order from the object side. The 3i-th lens group is configured of a biconcave lens L16, and a cemented lens CL5 that is configured of a biconcave lens L17 and a biconvex lens L18, in order from the object side.

Various pieces of data of the objective 13 are described below. The d-line (587.56 nm) is used for a reference wavelength.

NA=0.95, FN=30 mm, |β|=20, ε=7.54E−04 mm, f=9 mm, f_G1=27.3 mm, r₁₁=−13.0828 mm, r₁₂=−18.6447 mm, d_o12=13.101 mm, Φ_max/2=23.948 mm, h_exp=8.55 mm, f_G2=54.7 mm, f_G30=159.94 mm, f_G3C=65.94 mm, f_G3I=−31.75 mm, r₂₁=−25.0446 mm, D_oL=148.679 mm, D_ogF=108.374 mm, f_L2=82.66 mm, f_L3=109.35 mm, f_L7=156.84 mm

Lens data of the objective 13 is described below.

Objective 13
s	r	d	nd	νd	er
s1(object	INF	0.150	1.52100	56.02	0.75
surface)
s2	INF	2.027			0.87
s3	−13.0828	10.924	1.88300	40.76	4.37
s4	−18.6447	1.191			11.63
s5	−25.0446	4.866	1.60300	65.44	13.27
s6	−17.8874	0.110			14.45
s7	−23.8656	5.582	1.60300	65.44	15.60
s8	−19.0650	0.110			16.72
s9	−74.2737	3.752	1.49700	81.54	19.54
s10	−38.6719	0.110			19.84
s11	43.0902	16.297	1.43875	94.93	22.60
s12	−33.2088	1.650	1.63775	42.41	22.55
s13	89.2116	11.130	1.43875	94.93	23.56
s14	−43.0265	0.110			23.66
s15	54.2247	1.430	1.63775	42.41	22.35
s16	22.3467	16.663	1.43875	94.93	20.20
s17	−73.4579	0.220			20.17
s18	49.8507	1.100	1.63775	42.41	19.05
s19	20.7309	11.427	1.43875	94.93	17.33
s20	−180.4116	1.358			17.18
s21	−105.6549	1.100	1.67300	38.15	17.00
s22	111.6317	9.250			16.77
s23	−22.2976	0.880	1.48749	70.23	16.77
s24	−115.6031	6.936	1.73800	32.26	19.07
s25	−28.8606	0.100			19.39
s26	131.0728	3.590	1.63775	42.41	18.58
s27	−126.7311	27.324			18.47
s28	−35.6037	1.100	1.49700	81.54	10.57
s29	349.2902	5.126			10.35
s30	−25.0136	1.100	1.49700	81.54	10.07
s31	59.1028	1.965	1.63775	42.41	10.45
s32	−255.7418	−28.248			10.50

The objective 13 satisfies conditional expressions (1) to (7) and (11) to (16), as described below.

NA=0.95   (1), (4):

FN/|β|/ε =1990   (2):

Φ_max/2/h_exp/NA=2.95   (3):

f_G1/f=3.03   (5):

r₁₁/f=−1.45   (6):

r₁₂/d₀₁₂=−1.42   (7):

D_ogF/D_oL=0.73   (11):

f/f_G30=−0.06   (12):

f_G1/f_L2=0.33   (13):

f_G1/f_L3=0.25   (14):

f_G3I/f=−3.53   (15):

r₂₁/r₁₂=1.34   (16):

FIG. 8A to FIG. 8D are aberration diagrams in a case in which a combination of the objective 13 and the tube lens 10 is used. FIG. 8A illustrates spherical aberration, FIG. 8B illustrates a sine condition violation amount, FIG. 8C illustrates astigmatism, and FIG. 8D illustrates comatic aberration.

EXAMPLE 4

FIG. 9 is a sectional view of an objective 14 in this example. The objective 14 illustrated in FIG. 9 is a dry objective for a microscope. The objective 14 is configured of the first lens group G1 with positive refractive power, the second lens group G2 with positive refractive power that includes a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and the third lens group G3 with negative refractive power, in order from the object side.

The first lens group G1 is configured of a meniscus lens L1 (the first lens) with negative refractive power with a concave surface facing the object side, a meniscus lens L2 (the second lens) with positive refractive power with a concave surface facing the object side, a meniscus lens L3 (the third lens component) with positive refractive power with a concave surface facing the object side, and a meniscus lens L4 (the seventh lens component) with positive refractive power with a concave surface facing the object side, in order from the object side.

The second lens group G2 is configured of a three-lens-cemented lens CL1 that is configured of a biconvex lens L5, a biconcave lens L6, and a biconvex lens L7, and a biconvex lens L8, in order from the object side. The biconvex lens L8 is an aspherical lens for which both surfaces are formed so as to be aspherical.

The third lens group G3 is configured of the 3o-th lens group (the front lens group), the 3c-th lens group (the intermediate lens group), and the 3i-th lens group (the rear lens group), in order from the object side. The 3o-th lens group is configured of a cemented lens CL2 that is configured of a meniscus lens L9 (the ninth lens) with negative refractive power with a concave surface facing the image side and a biconvex lens L10 (the eighth lens), and a cemented lens CL3 that is configured of a meniscus lens L11 with negative refractive power with a concave surface facing the image side and a biconvex lens L12, in order from the object side. The 3c-th lens group is configured of a cemented lens CL4 that is configured of a biconvex lens L13 (the sixth lens; NBH53 of OHARA INC.) and a meniscus lens L14 with negative refractive power with a concave surface facing the object side, a meniscus lens L15 with a concave surface facing the image side, and a meniscus lens L16 with a concave surface facing the image side, in order from the object side. The 3i-th lens group is configured of a biconcave lens L17, and a meniscus lens L18 with positive refractive power with a concave surface facing the image side, in order from the object side. The meniscus lens L15, the meniscus lens L16, and the biconcave lens L17 are aspherical lenses for which both surfaces are formed so as to be aspherical.

Various pieces of data of the objective 14 are described below. The d-line (587.56 nm) is used for a reference wavelength.

NA=0.95, FN=30 mm, |β|=20, ε=7.54E−04 mm, f=9 mm, f_G1=23.6 mm, r₁₁=−10.2441 mm, r₁₂=−13.3175 mm, d_o12=10.314 mm, Φ_max/2=21.728 mm, h_exp=8.55 mm, f_G30=909.357 mm, f_G3I=−81.92 mm, r₂₁=−17.6973 mm, D_oL=149.641 mm, D_ogF=107.876 mm, f_L2=65.24 mm, f_L3=175.06 mm

Lens data of the objective 14 is described below. The mark “*” put on a surface number represents that a surface is aspherical.

Objective 14
s	r	d	nd	νd	er
s1(object	INF	0.150	1.52100	56.02	0.75
surface)
s2	INF	2.214			0.87
s3	−10.2441	7.950	1.88300	40.76	4.33
s4	−13.3175	0.121			9.56
s5	−17.6973	5.166	1.67790	55.34	10.43
s6	−14.1306	0.121			12.08
s7	−21.3714	5.186	1.56907	71.30	13.44
s8	−19.1452	0.396			15.16
s9	−44.1327	5.129	1.49700	81.54	17.10
s10	−25.6809	0.121			17.75
s11	35.9327	14.463	1.49700	81.54	21.12
s12	−54.0221	0.968	1.63775	42.41	20.79
s13	30.9878	11.469	1.43875	94.93	20.15
s14	−57.0147	0.121			20.17
s15*	762.8936	2.743	1.43875	94.93	19.93
s16*	−95.8052	0.121			19.95
s17	107.5081	0.968	1.67300	38.15	19.20
s18	20.6405	22.188	1.43875	94.93	17.71
s19	−72.7389	0.242			18.35
s20	124.0168	0.968	1.67300	38.15	18.27
s21	24.4575	9.958	1.43875	94.93	17.76
s22	−117.0784	0.121			17.84
s23	2449.3135	16.993	1.73800	32.26	17.93
s24	−24.6714	5.354	1.48749	70.23	18.29
s25	−53.1343	2.770			16.63
s26*	683.9611	8.787	1.49700	81.54	14.40
s27*	31.7810	2.371			12.29
s28*	22.1813	8.754	1.49700	81.54	11.98
s29*	13.6459	5.257			9.41
s30*	−33.9011	6.266	1.49700	81.54	9.76
s31*	135.5589	1.000			10.28
s32	60.0363	1.206	1.73800	32.26	10.50
s33	115.3925	−29.031			10.50

Aspherical data of the objective 14 is described below. Here, an aspherical shape is represented by the expression below. In this expression, z represents a coordinate in an optical axis direction of an aspherical surface, Y represents a coordinate in a direction orthogonal to an optical axis of the aspherical surface, K represents a conical coefficient, r represents a paraxial radius of curvature of the aspherical surface, and A4, A6, A8, and A10 respectively represent the fourth, sixth, eighth, and tenth aspherical coefficients. E represents a power of 10.

$Z=\frac{Y^2}{r+r\sqrt{1-\left(K+1\right){\left(Y/r\right)}^2}}+A4Y^4+A6Y^6+A8Y^8+A10Y^{10}$

Fifteenth Surface s15

• K=−130.5839 A4=−3.374E−06 A6=−2.550E−09 A8=−4.653E−12 A10=−1.689E−14

Sixteenth Surface s16

• K=0.9776 A4=−1.333E−06 A6=−2.475E−09 A8=−9.516E−12 A10=−6.753E−15

Twenty-Sixth Surface s26

• K=−115.0934 A4=9.081E−07 A6=−5.191E−08 A8=−1.147E−10 A10=1.250E−13

Twenty-Seventh Surface s27

• K=−0.5111 A4=1.769E−05 A6=−2.561E−08 A8=−7.502E−10 A10=1.643E−12

Twenty-Eighth Surface s28

• K=−2.9135 A4=6.461E−07 A6=−2.152E−08 A8=4.242E−10 A10=2.141E−12

Twenty-Ninth Surface s29

• K=−1.5929 A4=2.967E−05 A6=4.115E−07 A8=3.764E−09 A10=2.546E−11

Thirtieth Surface s30

• K=−3.3854 A4=1.580E−05 A6=4.658E−07 A8=1.813E−09 A10=−1.025E−11

Thirty-First Surface s31

• K=−79.1359 A4=-5.487E−06 A6=4.016E−08 A8=4.241E−10 A10=-1.231E−11

The objective 14 satisfies conditional expressions (1) to (7) and (11) to (16), as described below.

NA=0.95   (1), (4):

FN/|β|/ε =1990   (2):

Φ_max/2/h_exp/NA=2.68   (3):

f_G1/f=2.62   (5):

r₁₁/f=−1.14   (6):

r₁₂/d₀₁₂=−1.29   (7):

D_ogF/D_oL=0.72   (11):

f/f_G30=−0.01   (12):

f_G1/f_L2=0.36   (13):

f_G1/f_L3=0.13   (14):

f_G3I/f=−9.10   (15):

r₂₁/r₁₂=1.33   (16):

FIG. 10A and FIG. 10D are aberration diagrams in a case in which a combination of the objective 14 and the tube lens 10 is used. FIG. 10A illustrates spherical aberration, FIG. 10B illustrates a sine condition violation amount, FIG. 10C illustrates astigmatism, and FIG. 10D illustrates comatic aberration.

EXAMPLE 5

FIG. 11 is a sectional view of an objective 15 in this example. The objective 15 illustrated in FIG. 11 is a dry objective for a microscope. The objective 15 is configured of the first lens group G1 with positive refractive power, the second lens group G2 with positive refractive power that includes a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and the third lens group G3 with negative refractive power, in order from the object side.

The first lens group G1 is configured of a meniscus lens L1 (the first lens) with negative refractive power with a concave surface facing the object side, a meniscus lens L2 (the second lens) with positive refractive power with a concave surface facing the object side, a meniscus lens L3 (the third lens component) with positive refractive power with a concave surface facing the object side, and a meniscus lens L4 (the seventh lens component) with positive refractive power with a concave surface facing the object side, in order from the object side.

The second lens group G2 is configured of a three-lens-cemented lens CL1 that is configured of a biconvex lens L5, a biconcave lens L6, and a biconvex lens L7, and a cemented lens CL2 that is configured of a meniscus lens L8 with negative refractive power with a concave surface facing the image side and a biconvex lens L9, in order from the object side.

The third lens group G3 is configured of the 3o-th lens group (the front lens group), the 3c-th lens group (the intermediate lens group), and the 3i-th lens group (the rear lens group), in order from the object side. The 3o-th lens group is configured of a cemented lens CL3 that is configured of a meniscus lens L10 (the ninth lens) with negative refractive power with a concave surface facing the image side and a biconvex lens L11 (the eighth lens), and a biconcave lens L12, in order from the object side. The 3c-th lens group is configured of a cemented lens CL4 (the tenth lens component) that is configured of a meniscus lens L13 with negative refractive power with a concave surface facing the object side and a meniscus lens L14 (the sixth lens; NBH53 of OHARA INC.) with positive refractive power with a concave surface facing the object side, and a biconvex lens L15, in order from the object side. The 3i-th lens group is configured of a biconcave lens L16, a meniscus lens L17 with negative refractive power with a concave surface facing the object side, and a diffractive optical element (DOE) L18, in order from the object side. The diffractive optical element L18 is an optical element in which at least two layers that are made of optical materials different from each other are laminated, and is a diffractive optical element, as described in Japanese Patent No. 3717555, in which a relief pattern is formed on a boundary surface and diffraction efficiency is enhanced in a wide wavelength region. However, a diffractive optical element used for the objective 15 in this example is not limited to the diffractive optical element above. The diffractive optical element may be a diffractive optical element as described, for example, in Japanese Laid-Open Patent Publication No. 2003-215457 or Japanese Laid-Open Patent Publication No. 11-133305.

The diffractive optical element L18 has been designed with an ultra-high index method, as described, for example, in Japanese Laid-Open Patent Publication No. 8-286113. A surface shape (a radius of curvature and an aspherical coefficient) of the diffractive optical element L18 is a lens surface shape in a case in which the diffractive optical element L18 is replaced with a virtual lens (an ultra-high index lens) having extremely great refractive power.

Various pieces of data of the objective 15 is described below. The d-line (587.56 nm) is used for a reference wavelength.

NA=0.95, FN=30 mm, |β|=20, ε=7.54E−04 mm, f=9 mm, f_G1=25.9 mm, r₁₁=−11.7553 mm, r₁₂=−16.9884 mm, d_o12=14.223 mm, Φ_max/2=21.938 mm, h_exp=8.55 mm, f_G30=−102.2878 mm, f_G31=−38.562 mm, r₂₁=−23.2686 mm, D_oL=151.183 mm, D_ogF=102.274 mm, f_L2=139.125 mm, f_L3=104.96 mm

Lens data of the objective 15 is described below. The mark “*” put on a surface number represents that a surface is aspherical. A surface number s34 indicates a lens surface shape in a case in which a diffractive optical element is replaced with a virtual lens (an ultra-high index lens) having extremely great refractive power.

Objective 15
s	r	d	nd	νd	er
s1(object	INF	0.165	1.52103	56.02	0.75
surface)
s2	INF	1.760			0.88
s3	−11.7553	12.298	1.88306	40.76	3.84
s4	−16.9884	0.088			11.65
s5	−23.2686	4.402	1.5691	71.30	12.60
s6	−19.2175	0.110			14.17
s7	−22.4059	4.840	1.5691	71.30	14.80
s8	−17.5706	0.110			15.53
s9	−58.7666	4.091	1.49702	81.54	18.10
s10	−31.1809	0.110			18.44
s11	39.7049	15.367	1.43876	94.93	21.02
s12	−30.5156	1.650	1.63779	42.41	20.96
s13	123.7205	9.396	1.43876	94.93	21.75
s14	−40.5802	0.110			21.86
s15	53.0777	1.430	1.63779	42.41	20.40
s16	20.1928	15.788	1.43876	94.93	18.30
s17	−62.8184	0.220			18.26
s18	91.8568	1.100	1.63779	42.41	17.44
s19	20.0113	11.538	1.43876	94.93	16.06
s20	−67.1527	0.508			16.00
s21	−56.6330	1.100	1.63779	42.41	15.97
s22	322.2650	8.580			16.01
s23	−20.5345	0.823	1.48751	70.23	16.04
s24	−74.6275	6.688	1.73806	32.26	18.44
s25	−26.5166	0.194			18.85
s26	136.8083	3.519	1.67305	38.15	18.47
s27	−149.8267	33.112			18.38
s28	−60.0182	1.100	1.49702	81.54	11.00
s29	192.7648	6.268			10.82
s30	−27.1426	1.100	1.49702	81.54	10.51
s31	−105.6533	1.116			10.74
s32	INF	0.500	1.61006	27.48	10.87
s33	INF	0	1000	−3.45	10.90
s34*	2075000	2.000	1.63768	34.21	10.90
s35	INF	−32.826			11.00

Aspherical data of the objective 15 is described below.

Thirty-Fourth Surface s34

• K=0 A4=4.591E−11 A6=3.073E−13 A8=0 A10=0

The objective 15 satisfies conditional expressions (1) to (7) and (11) to (16), as described below.

NA=0.95   (1), (4):

FN/|β|/ε =1990   (2):

Φ_max/2/h_exp/NA=2.70   (3):

f_G1/f=2.88   (5):

r₁₁/f=−1.31   (6):

r₁₂/d₀₁₂=−1.19   (7):

D_ogF/D_oL=0.68   (11):

f/f_G30=−0.09   (12):

f_G1/f_L2=0.19   (13):

f_G1/f_L3=0.25   (14):

f_G3I/f=−4.28   (15):

r₂₁/r₁₂=1.37   (16):

FIG. 12A to FIG. 12D are aberration diagrams in a case in which a combination of the objective 15 and the tube lens 10 is used. FIG. 12A illustrates spherical aberration, FIG. 12B illustrates a sine condition violation amount, FIG. 12C illustrates astigmatism, and FIG. 12D illustrates comatic aberration.

EXAMPLE 6

FIG. 13 is a sectional view of an objective 16 in this example. The objective 16 illustrated in FIG. 13 is an immersion type objective for a microscope. The objective 16 is configured of the first lens group G1 with positive refractive power, the second lens group G2 with positive refractive power that includes a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and the third lens group G3 with negative refractive power, in order from the object side.

The first lens group G1 is configured of a cemented lens CL1 (the first cemented lens) that is configured of a plano-convex lens L0 with a plane surface facing the object side and a meniscus lens L1 (the first lens) with negative refractive power with a concave surface facing the object side, a meniscus lens L2 (the second lens) with positive refractive power with a concave surface facing the object side, a cemented lens CL2 (the third lens component) that is configured of a biconcave lens L3 and a biconvex lens L4, and a cemented lens CL3 (the seventh lens component) that is configured of a biconcave lens L5 and a biconvex lens L6, in order from the object side.

The second lens group G2 is configured of a three-lens-cemented lens CL4 that is configured of a meniscus lens L7 with positive refractive power with a concave surface facing the image side, a meniscus lens L8 with negative refractive power with a concave surface facing the image side, and a biconvex lens L9, and a three-lens-cemented lens CL5 that is configured of a meniscus lens L10 (the sixth lens; TIH53 of OHARA INC.) with positive refractive power with a concave surface facing the image side, a meniscus lens L11 with negative refractive power with a concave surface facing the image side, and a biconvex lens L12, in order from the object side.

The third lens group G3 is configured of the 3f-th lens group (the front lens group), the 3m-th lens group (the intermediate lens group), and the 3e-th lens group (the rear lens group), in order from the object side. The 3f-th lens group is configured of a meniscus lens L13 (the ninth lens) with negative refractive power with a concave surface facing the image side, a biconvex lens L14 (the eighth lens), and a cemented lens CL6 that is configured of a meniscus lens L15 with negative refractive power with a concave surface facing the image side and a meniscus lens L16 with positive refractive power with a concave surface facing the image side, in order from the object side. The 3m-th lens group is configured of a cemented lens CL7 (the twelfth lens component) that is configured of a biconvex lens L17 and a biconcave lens L18, and a meniscus lens L19 with negative refractive power with a concave surface facing the object side, in order from the object side. The 3e-th lens group is configured of a meniscus lens L20 (the eleventh lens component) with negative refractive power with a concave surface facing the image side, a meniscus lens L21 (the fifth lens component) with negative refractive power with a concave surface facing the object side, a cemented lens CL8 (the fourth lens component) that is configured of a meniscus lens L22 with negative refractive power with a concave surface facing the object side and a meniscus lens L23 with positive refractive power with a concave surface facing the object side, and a biconvex lens L24, in order from the object side.

Various pieces of data of the objective 16 are described below. The d-line (587.56 nm) is used for a reference wavelength. A refractive index N_o of immersion liquid is 1.5148.

NA=1.3, FN=30 mm, |β|=40, ε=5.51E−04 mm, f=4.5 mm, f_G1=15.83 mm, r₁₂=−6.834 mm, d_o12=7.238 mm, Φ_max/2=21.64 mm, h_exp=5.85 mm, f_G30=67.05 mm, D_oL=145.000 mm, D_ogF=64.477 mm, f_L2=51.90 mm, f_L3=165.57 mm, f_L7=220.49 mm

Lens data of the objective 16 is described below.

Objective 16
s	r	d	nd	νd	er
s1(object	INF	0.170	1.52347	54.41	0.38
surface)
s2	INF	0.362	1.51486	41.00	0.66
s3	INF	0.652	1.51635	64.14	1.29
s4	−3.2441	6.054	1.88306	40.76	1.64
s5	−6.8342	0.144			5.90
s6	−16.1435	11.171	1.5691	71.30	7.68
s7	−13.0577	0.222			12.07
s8	−45.2412	0.891	1.63779	42.41	14.57
s9	164.1406	10.007	1.5691	71.30	16.18
s10	−30.4567	0.122			17.67
s11	−215.6520	0.800	1.63779	42.41	19.01
s12	149.0681	6.993	1.5691	71.30	19.59
s13	−72.7399	0.100			20.19
s14	45.7927	4.715	1.43876	94.93	21.64
s15	112.1092	0.837	1.63779	42.41	21.59
s16	33.3718	14.170	1.43876	94.93	21.26
s17	−61.1831	2.993			21.41
s18	50.0401	4.073	1.84676	23.78	20.46
s19	93.4075	1.331	1.75504	52.32	20.00
s20	23.9768	12.129	1.43876	94.93	18.15
s21	−90.2641	0.100			17.99
s22	109.2684	0.800	1.75504	52.32	17.31
s23	27.2740	0.100			16.40
s24	25.9302	8.731	1.43876	94.93	16.55
s25	−111.0317	0.100			16.40
s26	24.1614	2.386	1.75504	52.32	15.02
s27	20.4571	11.959	1.43876	94.93	13.89
s28	170.5645	2.268			11.48
s29	22.1833	4.491	1.60303	65.44	9.50
s30	−33.1761	2.120	1.73806	32.26	8.95
s31	11.7279	4.969			6.73
s32	−14.2396	0.800	1.49702	81.54	6.45
s33	−43.4343	15.497			6.51
s34	123.5400	0.800	1.60303	65.44	6.15
s35	14.1045	3.245			6.08
s36	−12.7149	0.800	1.75504	52.32	6.15
s37	−41.8941	2.177			6.85
s38	−10.7606	0.800	1.43876	94.93	6.95
s39	−15.4480	2.076	1.73806	32.26	7.77
s40	−12.0682	0.100			8.31
s41	64.1504	2.741	1.88306	40.76	10.19
s42	−53.5056	−53.273			10.32

Surfaces having surface numbers s1 and s2 are respectively an object surface (a surface on the object side of a cover glass) and a surface on the image side of the cover glass. Surfaces having surface numbers s3 and s42 are respectively a lens surface closest to the object and a lens surface closest to the image plane in the objective. A space between the surface having a surface number s2 and the surface having a surface number s3 is filled with immersion liquid.

The objective 16 satisfies conditional expressions (1) to (3) and (8) to (14), as described below.

NA=1.3   (1), (8):

FN/|β|/ε−1361   (2):

Φ_max/2/h_exp/NA=2.85   (3):

f_G1/f=3.52   (9):

r₁₂/d_o12=−0.95   (10):

D_OgF/D_oL=0.44   (11):

f/f_G30=0.07   (12):

f_G1/f_L2=0.31   (13):

f_G1/f_L3=0.10   (14):

FIG. 14A to FIG. 14D are aberration diagrams in a case in which a combination of the objective 16 and the tube lens 10 is used. FIG. 14A illustrates spherical aberration, FIG. 14B illustrates a sine condition violation amount, FIG. 14C illustrates astigmatism, and FIG. 14D illustrates comatic aberration.

EXAMPLE 7

FIG. 15 is a sectional view of an objective 17 in this example. The objective 17 illustrated in FIG. 15 is an immersion type objective for a microscope. The objective 17 is configured of the first lens group G1 with positive refractive power, the second lens group G2 with positive refractive power that includes a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and the third lens group G3 with negative refractive power, in order from the object side.

The first lens group G1 is configured of a cemented lens CL1 (the first cemented lens) that is configured of a plano-convex lens L0 with a plane surface facing the object side and a meniscus lens L1 (the first lens) with negative refractive power with a concave surface facing the object side, a meniscus lens L2 (the second lens) with positive refractive power with a concave surface facing the object side, a cemented lens CL2 (the third lens component) that is configured of a biconcave lens L3 and a biconvex lens L4, and a cemented lens CL3 (the seventh lens component) that is configured of a biconcave lens L5 and a biconvex lens L6, in order from the object side.

The second lens group G2 is configured of a three-lens-cemented lens CL4 that is configured of a meniscus lens L7 with positive refractive power with a concave surface facing the image side, a meniscus lens L8 with negative refractive power with a concave surface facing the image side, and a biconvex lens L9, and a three-lens-cemented lens CL5 that is configured of a meniscus lens L10 (the sixth lens; TIH53 of OHARA, INC.) with positive refractive power with a concave surface facing the image side, a meniscus lens L11 with negative refractive power with a concave surface facing the image side, and a biconvex lens L12, in order from the object side.

The third lens group G3 is configured of the 3f-th lens group (the front lens group), the 3m-th lens group (the intermediate lens group), and the 3e-th lens group (the rear lens group), in order from the object side. The 3f-th lens group is configured of a cemented lens CL6 that is configured of a meniscus lens L13 (the ninth lens) with negative refractive power with a concave surface facing the image side and a biconvex lens L14 (the eighth lens), and a cemented lens CL7 that is configured of a meniscus lens L15 with negative refractive power with a concave surface facing the image side and a meniscus lens L16 with positive refractive power with a concave surface facing the image side, in order from the object side. The 3m-th lens group is configured of a cemented lens CL8 that is configured of a meniscus lens L17 with positive refractive power with a concave surface facing the image side and a meniscus lens L18 with negative refractive power with a concave surface facing the image side, and a cemented lens CL9 that is configured of a meniscus lens L19 with negative refractive power with a concave surface facing the object side and a meniscus lens L20 with positive refractive power with a concave surface facing the object side, in order from the object side. The 3e-th lens group is configured of a biconcave lens L21 (the eleventh lens component), a meniscus lens L22 (the fifth lens component) with negative refractive power with a concave surface facing the object side, a cemented lens CL10 (the fourth lens component) that is configured of a meniscus lens L23 with negative refractive power with a concave surface facing the object side and a meniscus lens L24 with positive refractive power with a concave surface facing the object side, a plano-convex lens L25 with a plane surface facing the object side, and a biconvex lens L26, in order from the object side.

Various pieces of data of the objective 17 are described below. The d-line (587.56 nm) is used for a reference wavelength. A refractive index N_o of immersion liquid is 1.5148.

NA=1.4, FN=30 mm, |β|=40, ε=5.12E−04 mm, f=4.5 mm, f_G1=14.27 mm, r₁₂=−7.0457 mm, d_o12=7.091 mm, Φ_max/2=24.721 mm, h_exp=6.30 mm, f_G30=75.727 mm, D_oL=151.261 mm, D_ogF=66.140 mm, f_L2=47.8 mm, f_L3=146.08 mm

Lens data of the objective 17 is described below.

Objective 17
s	r	d	nd	νd	er
s1(object	INF	0.170	1.52347	54.41	0.38
surface)
s2	INF	0.250	1.51486	41.00	0.74
s3	INF	0.541	1.51635	64.14	1.30
s4	−3.2573	6.130	1.88306	40.76	1.58
s5	−7.0457	0.101			6.17
s6	−18.2608	11.223	1.5691	71.30	8.50
s7	−13.3647	0.100			12.69
s8	−47.9736	0.811	1.63779	42.41	16.07
s9	156.9755	9.957	1.5691	71.30	18.18
s10	−30.2445	0.100			19.18
s11	−199.1341	0.800	1.63779	42.41	21.08
s12	143.4114	6.879	1.5691	71.30	21.93
s13	−70.9607	0.100			22.34
s14	47.7991	5.342	1.43876	94.93	24.60
s15	115.7137	0.801	1.63779	42.41	24.55
s16	34.7896	16.963	1.43876	94.93	24.08
s17	−61.7960	2.077			24.23
s18	57.6791	3.796	1.84676	23.78	23.09
s19	108.1782	0.918	1.75504	52.32	22.75
s20	26.3280	14.393	1.43876	94.93	20.64
s21	−65.8296	0.100			20.57
s22	74.3029	0.810	1.75504	52.32	19.11
s23	22.9020	10.684	1.43876	94.93	17.47
s24	−185.2953	0.324			17.32
s25	23.7108	2.654	1.75504	52.32	16.10
s26	20.7355	12.324	1.43876	94.93	14.89
s27	110.2738	2.752			12.51
s28	19.2575	4.184	1.60303	65.44	10.18
s29	1332.6436	2.153	1.73806	32.26	9.49
s30	10.2792	4.211			7.11
s31	−21.6113	0.800	1.49702	81.54	7.08
s32	−310.2945	1.098	1.73806	32.26	7.07
s33	−94.8995	14.625			7.07
s34	−36.3192	0.800	1.60303	65.44	6.24
s35	20.0000	2.657			6.31
s36	−14.2645	0.800	1.75504	52.32	6.35
s37	−44.8729	2.263			6.99
s38	−10.8850	0.800	1.43876	94.93	7.09
s39	−16.2941	2.006	1.73806	32.26	7.94
s40	−12.8173	0.100			8.48
s41	INF	1.594	1.88306	40.76	9.98
s42	−66.6667	0.100			10.16
s43	84.2007	1.975	1.88306	40.76	10.61
s44	−119.1973	−50.823			10.69

The objective 17 satisfies conditional expressions (1) to (3) and (8) to (14), as described below.

NA=1.4   (1), (8):

FN/|β|/ε−1466   (2):

Φ_max/2/h_exp/NA=2.80   (3):

f_G1/f=3.17   (9):

r₁₂/d_o12=−0.99   (10):

D_OgF/D_oL=0.44   (11):

f/f_G30=0.06   (12):

f_G1/f_L2=0.30   (13):

f_G1/f_L3=0.10   (14):

FIG. 16A to FIG. 16D are aberration diagrams in a case in which a combination of the objective 17 and the tube lens 10 is used. FIG. 16A illustrates spherical aberration, FIG. 16B illustrates a sine condition violation amount, FIG. 16C illustrates astigmatism, and FIG. 16D illustrates comatic aberration.

EXAMPLE 8

FIG. 17 is a sectional view of an objective 18 in this example. The objective 18 illustrated in FIG. 17 is an immersion type objective for a microscope. The objective 18 is configured of the first lens group G1 with positive refractive power, the second lens group G2 with positive refractive power that includes a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and the third lens group G3 with negative refractive power, in order from the object side.

The first lens group G1 is configured of a cemented lens CL1 (the first cemented lens) that is configured of a plano-convex lens L0 with a plane surface facing the object side and a meniscus lens L1 (the first lens) with negative refractive power with a concave surface facing the object side, a meniscus lens L2 (the second lens) with positive refractive power with a concave surface facing the object side, and a meniscus lens L3 (the third lens component) with positive refractive power with a concave surface facing the object side, in order from the object side.

The second lens group G2 is configured of a three-lens-cemented lens CL2 that is configured of a biconvex lens L4, a biconcave lens L5, and a biconvex lens L6, and a three-lens-cemented lens CL3 that is configured of a meniscus lens L7 (the sixth lens; TIH53 of OHARA INC.) with positive refractive power with a concave surface facing the image side, a meniscus lens L8 with negative refractive power with a concave surface facing the image side, and a biconvex lens L9, in order from the object side.

The third lens group G3 is configured of the 3f-th lens group (the front lens group), the 3m-th lens group (the intermediate lens group), and the 3e-th lens group (the rear lens group), in order from the object side. The 3f-th lens group is configured of a cemented lens CL4 that is configured of a meniscus lens L10 (the ninth lens) with negative refractive power with a concave surface facing the image side and a meniscus lens L11 (the eighth lens) with positive refractive power with a concave surface facing the image side, and a cemented lens CL5 that is configured of a meniscus lens L12 with negative refractive power with a concave surface facing the image side and a meniscus lens L13 with positive refractive power with a concave surface facing the image side, in order from the object side. The 3m-th lens group is configured of a cemented lens CL6 (the twelfth lens component) that is configured of a meniscus lens L14 with positive refractive power with a concave surface facing the image side and a meniscus lens L15 with negative refractive power with a concave surface facing the image side, and a cemented lens CL7 that is configured of a meniscus lens L16 with negative refractive power with a concave surface facing the object side and a meniscus lens L17 with positive refractive power with a concave surface facing the object side, in order from the object side. The 3e-th lens group is configured of a biconcave lens L18 (the eleventh lens component), a meniscus lens L19 (the fifth lens component) with negative refractive power with a concave surface facing the object side, a meniscus lens L20 (the fourth lens component) with negative refractive power with a concave surface facing the object side, and a meniscus lens L21 with positive refractive power with a concave surface facing the object side, in order from the object side.

Various pieces of data of the objective 18 are described below. The d-line (587.56 nm) is used for a reference wavelength. A refractive index N_o of immersion liquid is 1.5148.

NA=1.3, FN=30 mm, |β|=20, ε=5.51E−04 mm, f=9 mm, f_G1=25.5 mm, r₁₂=−15.884 mm, d_o12=15.892 mm, Φ_max/2=37.6 mm, h_exp=11.70 mm, f_G30=117 mm, D_oL=240.000 mm, D_ogF=95.874 mm, f _L2=105.04 mm, f_L3=121.71 mm

Lens data of the objective 18 is described below.

Objective 18
s	r	d	nd	νd	er
s1(object	INF	0.170	1.52347	54.41	0.75
surface)
s2	INF	0.471	1.51486	41.00	1.03
s3	INF	1.365	1.51635	64.14	1.82
s4	−7.1989	13.886	1.88306	40.76	3.00
s5	−15.8839	0.376			12.95
s6	−43.6099	24.634	1.5691	71.30	17.08
s7	−30.3807	0.142			26.86
s8	−280.6407	10.229	1.5691	71.30	33.43
s9	−56.2880	0.195			33.75
s10	122.3257	18.520	1.43876	94.93	35.67
s11	−58.5812	1.528	1.63779	42.41	35.65
s12	96.9456	20.013	1.43876	94.93	37.30
s13	−68.2221	0.100			37.50
s14	92.5363	4.245	1.84676	23.78	36.98
s15	161.2978	0.802	1.75504	52.32	36.81
s16	48.4035	18.570	1.43876	94.93	34.52
s17	−179.2671	0.100			34.48
s18	91.9859	0.800	1.75504	52.32	32.93
s19	43.7277	13.061	1.43876	94.93	30.99
s20	787.6851	0.100			30.90
s21	38.5369	4.195	1.63779	42.41	29.04
s22	29.3182	21.077	1.43876	94.93	25.91
s23	187.4254	0.717			23.46
s24	38.5544	9.316	1.49702	81.54	20.94
s25	68.6319	5.690	1.73806	32.26	18.05
s26	18.1926	9.271			13.54
s27	−30.8961	0.800	1.49702	81.54	13.53
s28	−129.8157	6.381	1.73806	32.26	13.80
s29	−48.9189	32.834			14.23
s30	−38.7296	0.800	1.61803	63.33	11.78
s31	109.7621	4.288			12.03
s32	−22.5743	0.800	1.75504	52.32	12.06
s33	−81.3258	4.884			13.25
s34	−19.1249	4.983	1.73806	32.26	13.48
s35	−20.5477	0.100			15.77
s36	−7763.5563	4.558	1.88306	40.76	19.18
s37	−52.0532	−94.014			19.38

The objective 18 satisfies conditional expressions (1) to (3) and (8) to (14), as described below.

NA=1.3   (1), (8):

FN/|β|/ε−2723   (2):

Φ_max/2/h_exp/NA=2.47   (3):

f_G1/f=2.83   (9):

r₁₂/d_o12=−1.00   (10):

D_OgF/D_oL=0.40   (11):

f/f_G30=0.08   (12):

f_G1/f_L2=0.24   (13):

f_G1/f_L3=0.21   (14):

FIG. 18A to FIG. 18D are aberration diagrams in a case in which a combination of the objective 18 and the tube lens 10 is used. FIG. 18A illustrates spherical aberration, FIG. 18B illustrates a sine condition violation amount, FIG. 18C illustrates astigmatism, and FIG. 18D illustrates comatic aberration.

EXAMPLE 9

FIG. 19 is a sectional view of an objective 19 in this example. The objective 19 illustrated in FIG. 19 is an immersion type objective for a microscope. The objective 19 is configured of the first lens group G1 with positive refractive power, the second lens group G2 with positive refractive power that includes a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and the third lens group G3 with negative refractive power, in order from the object side.

The first lens group G1 is configured of a cemented lens CL1 (the first cemented lens) that is configured of a plano-convex lens L0 with a plane surface facing the object side and a meniscus lens L1 (the first lens) with negative refractive power with a concave surface facing the object side, a meniscus lens L2 (the second lens) with positive refractive power with a concave surface facing the object side, a meniscus lens L3 (the third lens component) with positive refractive power with a concave surface facing the object side, and a biconvex lens L4 (the seventh lens component), in order from the object side.

The second lens group G2 is configured of a three-lens-cemented lens CL2 that is configured of a biconvex lens L5, a biconcave lens L6, and a biconvex lens L7, and a three-lens-cemented lens CL3 that is configured of a meniscus lens L8 (the sixth lens; TIH53 of OHARA, INC.) with positive refractive power with a concave surface facing the image side, a meniscus lens L9 with negative refractive power with a concave surface facing the image side, and a biconvex lens L10, in order from the object side.

The third lens group G3 is configured of the 3f-th lens group (the front lens group), the 3m-th lens group (the intermediate lens group), and the 3e-th lens group (the rear lens group), in order from the object side. The 3f-th lens group is configured of a cemented lens CL4 that is configured of a meniscus lens L11 (the ninth lens) with negative refractive power with a concave surface facing the image side and a meniscus lens L12 (the eighth lens) with positive refractive power with a concave surface facing the image side, and a cemented lens CL5 that is configured of a meniscus lens L13 with negative refractive power with a concave surface facing the image side and a meniscus lens L14 with positive refractive power with a concave surface facing the image side, in order from the object side. The 3m-th lens group is configured of a cemented lens CL6 (the twelfth lens component) that is configured of a meniscus lens L15 with positive refractive power with a concave surface facing the image side and a meniscus lens L16 with negative refractive power with a concave surface facing the image side, and a cemented lens CL7 that is configured of a meniscus lens L17 with negative refractive power with a concave surface facing the object side and a meniscus lens L18 with positive refractive power with a concave surface facing the object side, in order from the object side. The 3e-th lens group is configured of a biconcave lens L19 (the eleventh lens component), a meniscus lens L20 (the fifth lens component) with negative refractive power with a concave surface facing the object side, a cemented lens CL8 (the fourth lens component) that is configured of a meniscus lens L21 with negative refractive power with a concave surface facing the object side and a meniscus lens L22 with positive refractive power with a concave surface facing the object side, a meniscus lens L23 with positive refractive power with a concave surface facing the object side, and a biconvex lens L24, in order from the object side.

Various pieces of data of the objective 19 are described below. The d-line (587.56 nm) is used for a reference wavelength. A refractive index N_o of immersion liquid is 1.5148.

NA=1.35, FN=30 mm, |β|=20, ε=5.30E−04 mm, f=9 mm, f_G1=26.6 mm, r₁₂=−16.1427 mm, d_o12=15.983 mm, Φ_max/2=42 mm, h_exp=12.15 mm, f_G30=128.44 mm, D_oL=270.000 mm, D_ogF=110.373 mm, f_L2=108 mm, f_L3=145 mm

Lens data of the objective 19 is described below.

Objective 19
s	r	d	nd	νd	er
s1(object	INF	0.170	1.52347	54.41	0.75
surface)
s2	INF	0.500	1.51486	41.00	1.06
s3	INF	1.549	1.51635	64.14	2.01
s4	−6.7369	13.764	1.88306	40.76	3.30
s5	−16.1427	0.696			13.61
s6	−40.4034	24.581	1.5691	71.30	18.50
s7	−29.8313	0.100			27.90
s8	−230.6251	10.855	1.5691	71.30	36.23
s9	−61.8679	0.100			36.81
s10	461.9394	3.119	1.5691	71.30	39.38
s11	−1334.3709	0.100			39.45
s12	111.3362	20.692	1.43876	94.93	40.42
s13	−74.6831	5.662	1.63779	42.41	40.37
s14	88.0169	23.795	1.43876	94.93	41.63
s15	−78.5986	0.100			41.80
s16	103.7530	4.590	1.84676	23.78	40.51
s17	184.2894	2.300	1.75504	52.32	40.33
s18	49.4844	22.221	1.43876	94.93	37.07
s19	−150.7597	0.100			37.02
s20	85.8487	2.000	1.75504	52.32	34.72
s21	40.6690	14.643	1.43876	94.93	31.78
s22	334.4963	0.100			31.67
s23	37.3445	4.191	1.63779	42.41	29.82
s24	29.7904	20.983	1.43876	94.93	26.73
s25	138.8114	0.853			24.22
s26	41.3866	8.957	1.49702	81.54	21.79
s27	87.4837	5.226	1.73806	32.26	19.18
s28	19.0760	9.956			14.46
s29	−34.4437	0.900	1.49702	81.54	14.44
s30	−151.4859	2.117	1.73806	32.26	14.74
s31	−55.0586	42.292			14.81
s32	−58.6989	0.800	1.61803	63.33	12.63
s33	81.0144	4.508			12.80
s34	−26.3219	0.900	1.75504	52.32	12.83
s35	−78.6093	4.395			13.85
s36	−20.4267	1.009	1.88306	40.76	13.92
s37	−37.4278	4.143	1.73806	32.26	15.89
s38	−24.2264	0.100			16.63
s39	−29.1246	2.638	1.63779	42.41	17.21
s40	−24.7643	0.100			17.70
s41	422.1492	4.197	1.88306	40.76	20.86
s42	−79.2452	−106.731			21.00

The objective 19 satisfies conditional expressions (1) to (3) and (8) to (14), as described below.

NA=1.35   (1), (8):

FN/|β|/ε−2828   (2):

Φ_max/2/h_exp/NA=2.56   (3):

f_G1/f=2.96   (9):

r₁₂/d_o12=−1.01   (10):

D_OgF/D_oL=0.41   (11):

f/f_G30=0.07   (12):

f_G1/f_L2=0.25   (13):

f_G1/f_L3=0.18   (14):

FIG. 20A to FIG. 20D are aberration diagrams in a case in which a combination of the objective 19 and the tube lens 10 is used. FIG. 20A illustrates spherical aberration, FIG. 20B illustrates a sine condition violation amount, FIG. 20C illustrates astigmatism, and FIG. 20D illustrates comatic aberration.

EXAMPLE 10

FIG. 21 is a sectional view of an objective 20 in this example. The objective 20 illustrated in FIG. 21 is an immersion type objective for a microscope. The objective 20 is configured of the first lens group G1 with positive refractive power, the second lens group G2 with positive refractive power that includes a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and the third lens group G3 with negative refractive power, in order from the object side.

The first lens group G1 is configured of a cemented lens CL1 (the first cemented lens) that is configured of a plano-convex lens L0 with a plane surface facing the object side and a meniscus lens L1 (the first lens) with negative refractive power with a concave surface facing the object side, a meniscus lens L2 (the second lens) with positive refractive power with a concave surface facing the object side, a meniscus lens L3 (the third lens component) with positive refractive power with a concave surface facing the object side, and a biconvex lens L4 (the seventh lens component), in order from the object side. The biconvex lens L4 is an aspherical lens for which both surfaces are formed so as to be aspherical.

The second lens group G2 is configured of a three-lens-cemented lens CL2 that is configured of a biconvex lens L5, a biconcave lens L6, and a biconvex lens L7, and a plano-convex lens L8 with a plane surface facing the object side, in order from the object side. The plane-convex lens L8 is an aspherical lens in which a lens surface of the image side is formed so as to be aspherical.

The third lens group G3 is configured of the 3f-th lens group (the front lens group), the 3m-th lens group (the intermediate lens group), and the 3e-th lens group (the rear lens group), in order from the object side. The 3f-th lens group is configured of a three-lens-cemented lens CL3 that is configured of a meniscus lens L9 (the sixth lens; TIH53 of OHARA, INC.) with positive refractive power with a concave surface facing the image side, a meniscus lens L10 with negative refractive power with a concave surface facing the image side, and a biconvex lens L11, a cemented lens CL4 that is configured of a meniscus lens L12 (the ninth lens) with negative refractive power with a concave surface facing the image side and a meniscus lens L13 (the eighth lens) with positive refractive power with a concave surface facing the image side, and a cemented lens CL5 that is configured of a meniscus lens L14 with negative refractive power with a concave surface facing the image side and a meniscus lens L15 with positive refractive power with a concave surface facing the image side, in order from the object side. The 3m-th lens group is configured of a cemented lens CL6 (the twelfth lens component) that is configured of a meniscus lens L16 with positive refractive power with a concave surface facing the image side and a meniscus lens L17 with negative refractive power with a concave surface facing the image side, and a cemented lens CL7 that is configured of a meniscus lens L18 with negative refractive power with a concave surface facing the object side and a meniscus lens L19 with positive refractive power with a concave surface facing the object side, in order from the object side. The 3e-th lens group is configured of a biconcave lens L20 (the eleventh lens component), a meniscus lens L21 (the fifth lens component) with negative refractive power with a concave surface facing the object side, a cemented lens CL8 (the fourth lens component) that is configured of a meniscus lens L22 with negative refractive power with a concave surface facing the object side and a meniscus lens L23 with positive refractive power with a concave surface facing the object side, a meniscus lens L24 with positive refractive power with a concave surface facing the object side, and a biconvex lens L25, in order from the object side. The biconcave lens L20 is an aspherical lens for which both surfaces are formed so as to be aspherical. The meniscus lens L21 and the biconvex lens L25 are aspherical lenses in which a lens surface on the object side is formed so as to be aspherical.

Various pieces of data of the objective 20 are described below. The d-line (587.56 nm) is used for a reference wavelength. A refractive index N_o of immersion liquid is 1.5148.

NA=1.45, FN=30 mm, |β|=20, ε=4.94E−04 mm, f=9 mm, f_G1=26.9 mm, r₁₂=−14.9778 mm, d_o12=16.116 mm, Φ_max/2=51.9 mm, h_exp=13.05 mm, f_G30=94.24 mm, D_oL=300.000 mm, D_ogF=134.067 mm, f_L2=137.033 mm, f_L3=270.96 mm

Lens data of the objective 20 is described below.

Objective 20
s	r	d	nd	νd	er
s1(object	INF	0.170	1.52347	54.41	0.75
surface)
s2	INF	0.655	1.51486	41.00	1.25
s3	INF	2.192	1.51635	64.14	3.31
s4	−7.9038	13.099	1.88306	40.76	4.88
s5	−14.9779	2.533			14.26
s6	−34.1464	24.266	1.5691	71.30	22.10
s7	−29.8689	0.127			29.68
s8	−211.5322	9.249	1.5691	71.30	42.08
s9	−90.6020	0.100			43.14
s10*	206.0617	8.203	1.5691	71.30	48.83
s11*	−902.4320	0.100			48.96
s12	84.4233	29.394	1.43876	94.93	51.76
s13	−131.1968	2.488	1.63779	42.41	51.60
s14	77.5618	22.136	1.43876	94.93	49.55
s15	−399.1036	2.027			49.60
s16	INF	12.359	1.43876	94.93	49.60
s17*	−99.6579	0.100			49.60
s18	112.6466	4.869	1.84676	23.78	45.58
s19	185.5705	0.800	1.75504	52.32	45.32
s20	44.4911	32.698	1.43876	94.93	39.48
s21	−107.8277	0.100			39.44
s22	83.7721	0.800	1.75504	52.32	35.73
s23	38.1549	15.109	1.43876	94.93	32.22
s24	141.2766	0.100			32.08
s25	32.5170	2.177	1.63779	42.41	30.58
s26	26.0501	24.782	1.43876	94.93	26.04
s27	114.8265	0.100			25.08
s28	37.1811	8.297	1.49702	81.54	22.33
s29	51.6704	3.874	1.73806	32.26	19.42
s30	17.8456	12.898			14.73
s31	−35.4780	0.800	1.49702	81.54	14.41
s32	−150.7254	2.764	1.73806	32.26	14.57
s33	−61.1012	32.508			14.66
s34*	−497.5063	0.800	1.61803	63.33	12.48
s35*	29.8465	6.746			12.29
s36*	−20.0794	0.800	1.75504	52.32	12.31
s37	−52.3966	6.143			13.65
s38	−20.6189	0.800	1.88306	40.76	14.61
s39	−34.5889	3.515	1.73806	32.26	16.51
s40	−24.7079	0.762			17.12
s41	−94.2453	3.952	1.63779	42.41	20.30
s42	−42.7157	0.179			20.66
s43*	112.0266	4.428	1.88306	40.76	23.36
s44	−180.0961	−118.512			23.00

Aspherical data of the objective 20 is described below.

Tenth Surface s10

• K−−0.7052 A4−1.849E−08 A6−−1.547E−11 A8−−1.063E−14 A10−0

Eleventh Surface s11

• K=−92.9161 A4=2.085E−08 A6=−3.402E−11 A8=−1.112E−14 A10=0

Seventeenth Surface s17

• K=−0.4340 A4=2.270E−07 A6=1.494E−11 A8=−4.829E−15 A10=0

Thirty-Fourth Surface s34

• K=−92.9382 A4=−9.240E−06 A6=1.262E−07 A8=−2.565E−10 A10=0

Thirty-Fifth Surface s35

• K=−3.2850 A4=−1.357E−05 A6=9.443E−08 A8=−2.053E−10 A10=0

Thirty-Sixth Surface s36

• K=−0.0104 A4=−1.169E−06 A6=−1.636E−08 A8=−9.606E−11 A10=0

Forth-Third Surface s43

• K=−18.5319 A4=−1.484E−07 A6=0 A8=0 A10=0

The objective 20 satisfies conditional expressions (1) to (3) and (8) to (14), as described below.

NA=1.45   (1), (8):

FN/|β|/ε−3037   (2):

Φ_max/2/h_exp/NA=2.74   (3):

f_G1/f=2.99   (9):

r₁₂/d_o12=−0.93   (10):

D_OgF/D_oL=0.45   (11):

f/f_G30=0.10   (12):

f_G1/f_L2=0.20   (13):

f_G1/f_L3=0.10   (14):

FIG. 22A to FIG. 22D are aberration diagrams in a case in which a combination of the objective 20 and the tube lens 10 is used. FIG. 22A illustrates spherical aberration, FIG. 22B illustrates a sine condition violation amount, FIG. 22C illustrates astigmatism, and FIG. 22D illustrates comatic aberration.

EXAMPLE 11

FIG. 23 is a sectional view of an objective 21 in this example. The objective 21 illustrated in FIG. 23 is an immersion type objective for a microscope. The objective 21 is configured of the first lens group G1 with positive refractive power, the second lens group G2 with positive refractive power that includes a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material, and the third lens group G3 with negative refractive power, in order from the object side.

The first lens group G1 is configured of a cemented lens CL1 (the first cemented lens) that is configured of a plano-convex lens L0 with a plane surface facing the object side and a meniscus lens L1 (the first lens) with negative refractive power with a concave surface facing the object side, a meniscus lens L2 (the second lens) with positive refractive power with a concave surface facing the object side, a cemented lens CL2 (the third lens component) that is configured of a biconcave lens L3 and a biconvex lens L4, and a cemented lens CL3 (the seventh lens component) that is configured of a biconcave lens L5 and a biconvex lens L6, in order from the object side.

The second lens group G2 is configured of a three-lens-cemented lens CL4 that is configured of a meniscus lens L7 with positive refractive power with a concave surface facing the image side, a meniscus lens L8 with negative refractive power with a concave surface facing the image side, and a biconvex lens L9, and a three-lens-cemented lens CL5 that is configured of a meniscus lens L10 (the sixth lens; TIH53 of OHARA, INC.) with positive refractive power with a concave surface facing the image side, a meniscus lens L11 with negative refractive power with a concave surface facing the image side, and a biconvex lens L12, in order from the object side.

The third lens group G3 is configured of the 3f-th lens group (the front lens group), the 3m-th lens group (the intermediate lens group), and the 3e-th lens group (the rear lens group), in order from the object side. The 3f-th lens group is configured of a cemented lens CL6 that is configured of a meniscus lens L13 (the ninth lens) with negative refractive power with a concave surface facing the image side and a biconvex lens L14 (the eighth lens), and a cemented lens CL7 that is configured of a meniscus lens L15 with negative refractive power with a concave surface facing the image side and a meniscus lens L16 with positive refractive power with a concave surface facing the image side, in order from the object side. The 3m-th lens group is configured of a cemented lens CL8 (the twelfth lens component) that is configured of a biconvex lens L17 and a biconcave lens L18, and a meniscus lens L19 with negative refractive power with a concave surface facing the object side, in order from the object side. The 3e-th lens group is configured of a biconcave lens L20 (the eleventh lens component), a meniscus lens L21 (the fifth lens component) with negative refractive power with a concave surface facing the object side, a cemented lens CL9 (the fourth lens component) that is configured of a meniscus lens L22 with negative refractive power with a concave surface facing the object side and a meniscus lens L23 with positive refractive power with a concave surface facing the object side, a biconvex lens L24, and a diffractive optical element (DOE) L25, in order from the object side.

Various pieces of data of the objective 21 are described below. The d-line (587.56 nm) is used for a reference wavelength. A refractive index N. of immersion liquid is 1.5148.

NA=1.3, FN=30 mm, |β|=40, ε=5.51E−04 mm, f=4.5 mm, f_G1−14.30 mm, r₁₂−−6.990 mm, d_o12−7.199 mm, Φ_max/2−21.32 mm, h_exp=5.85 mm, f_G30=69.74 mm, D_oL=145.000 mm, D_ogF=65.076 mm, f_L2=49.55 mm, f_L3=117.33 mm

Lens data of the objective 21 is described below. A surface number s44 indicates a lens surface shape in a case in which a diffractive optical element is replaced with a virtual lens (an ultra-high index lens) having extremely great refractive power.

Objective 21
s	r	d	nd	νd	er
s1(object	INF	0.170	1.52347	54.41	0.38
surface)
s2	INF	0.333	1.51486	41.00	0.66
s3	INF	0.618	1.51635	64.14	1.24
s4	−3.2999	6.078	1.88306	40.76	1.59
s5	−6.9896	0.121			5.91
s6	−17.4528	11.219	1.5691	71.30	7.74
s7	−13.2943	0.194			12.15
s8	−48.9021	0.980	1.63779	42.41	14.73
s9	146.3471	10.058	1.5691	71.30	16.37
s10	−28.2615	0.100			17.61
s11	−141.0081	0.802	1.63779	42.41	18.79
s12	100.4622	6.354	1.5691	71.30	19.57
s13	−70.7737	0.100			19.90
s14	44.9582	5.106	1.43876	94.93	21.32
s15	106.1692	2.298	1.63779	42.41	21.26
s16	32.5030	13.613	1.43876	94.93	20.84
s17	−63.5018	2.579			20.97
s18	52.2478	4.354	1.84676	23.78	20.20
s19	112.2228	1.743	1.75504	52.32	19.73
s20	24.7453	11.491	1.43876	94.93	17.94
s21	−82.1758	0.100			17.81
s22	81.6786	0.803	1.75504	52.32	16.99
s23	24.9223	8.083	1.43876	94.93	15.97
s24	−136.1825	0.100			15.84
s25	23.8425	2.286	1.75504	52.32	14.71
s26	19.9624	12.027	1.43876	94.93	13.63
s27	162.1933	2.258			11.34
s28	21.5140	4.479	1.60303	65.44	9.49
s29	−43.3478	2.154	1.73806	32.26	8.85
s30	11.2466	3.863			6.73
s31	−18.7530	0.962	1.49702	81.54	6.66
s32	−43.9945	13.831			6.68
s33	−64.0343	0.800	1.60303	65.44	5.86
s34	17.2665	3.000			5.86
s35	−10.9759	0.840	1.75504	52.32	5.91
s36	−32.8559	1.928			6.66
s37	−10.5993	0.879	1.43876	94.93	6.76
s38	−14.9478	2.126	1.73806	32.26	7.56
s39	−11.6319	0.100			8.11
s40	89.1554	2.572	1.88306	40.76	9.75
s41	−43.4106	1.000			9.89
s42	INF	0.500	1.61006	27.48	10.06
s43	INF	0	1000	−3.45	10.09
s44*	6076000	2.000	1.63768	34.21	10.09
s45	INF	−51.001			10.19

Aspherical data of the objective 21 is described below.

Forty-Fourth Surface s44

• K=0 A4=1.645E−10 A6=8.451E−13 A8=0 A10=0

The objective 21 satisfies conditional expressions (1) to (3) and (8) to (14), as described below.

NA=1.3   (1), (8):

FN/|β|/ε−1361   (2):

Φ_max/2/h_exp/NA=2.80   (3):

f_G1/f=3.18   (9):

r₁₂/d_o12=−0.97   (10):

D_OgF/D_oL=0.45   (11):

f/f_G30=0.06   (12):

f_G1/f_L2=0.29   (13):

f_G1/f_L3=0.12   (14):

FIG. 24A to FIG. 24D are aberration diagrams in a case in which a combination of the objective 21 and the tube lens 10 is used. FIG. 24A illustrates spherical aberration, FIG. 24B illustrates a sine condition violation amount, FIG. 24C illustrates astigmatism, and FIG. 24D illustrates comatic aberration.

Lastly, the tube lens 10 illustrated in FIG. 3, which is used in common in Example 1 to Example 11, is described. The tube lens 10 is a tube lens for a microscope that is used in combination with an infinity correction type objective so as to form a magnified image of an object. The tube lens 10 is configured of the first lens group G1 with positive power that includes a cemented lens CL1, the second lens group G2 with negative power, and the third lens group G3 having positive power as a whole that is configured of a plurality of lenses (L6 and L7) that each have positive power, in order from the object side.

The first lens group G1 is configured of a biconvex lens L1, and a cemented lens CL1 that is configured of a biconvex lens L2 and a biconcave lens L3, in order from the object side. The second lens group G2 is configured of a cemented lens CL2 that is configured of a biconcave lens L4 and a biconvex lens L5, in order from the object side. The third lens group G3 is configured of a meniscus lens L6 with positive power with a concave surface facing the object side, and a biconvex lens L7, in order from the object side. Each of the first lens and the second lens has a meniscus shape.

Lens data of the tube lens 10 is described below. “INF” in the lens data represents infinity (∞).

Tube lens 10
s	r	d	nd	νd
s1	INF	162.2
s2	63.8523	9.3326	1.497	81.54
s3	−1485.8995	3.1666
s4	39.1423	13.9864	1.497	81.54
s5	−145.3496	6	1.51633	64.14
s6	26.8639	20.2953
s7	−53.5928	8.0905	1.72047	34.71
s8	110.3106	7.877	1.43875	94.93
s9	−130	14.8023
s10	−288.1082	6	1.59522	67.74
s11	−114.1428	0.4703
s12	176.2945	6	1.85026	32.27
s13	−475.1754

Claims

1. A dry objective for a microscope, the dry objective comprising in order from an object side:

a first lens group with positive refractive power;

a second lens group with positive refractive power, the second lens group including a cemented lens that is configured of a lens with positive refractive power that is made of a low dispersion material and a lens with negative refractive power that is made of a high dispersion material; and

a third lens group with negative refractive power,

wherein:

the first lens group includes in order from the object side: a first lens that is a single lens having a meniscus shape with a concave surface facing the object side; a second lens that is a single lens with positive refractive power, the single lens having a meniscus shape with a concave surface facing the object side; and a third lens component that is a single lens or cemented lens with positive refractive power,

the dry objective is configured in a manner such that a ray height of an on-axis marginal ray becomes maximum on a boundary surface of a lens component closest to an object in the second lens group or within the lens component, and

when NA represents a numerical aperture of the objective, f represents a focal length of the objective, fG1 represents a focal length of the first lens group, r11 represents a radius of curvature of a lens surface on the object side of the first lens, r12 represents a radius of curvature of a lens surface on an image side of the first lens, and do12 represents a distance on an optical axis from a front-side focal plane of the objective to a lens surface on the image side of the first lens, the objective satisfies the following conditional expressions: 0.8≦NA<1   (4) 1.6≦fG1/f≦6   (5) −1.6≦r11/f≦−0.2   (6) −2≦r12/do12≦−0.86   (7).

2. The objective according to claim 1, wherein the third lens component has a meniscus shape with a concave surface facing the object side.

3. The objective according to claim 1, wherein the second lens group includes a three-lens-cemented lens that is formed by respectively cementing lenses with positive refractive power that are made of a low dispersion material to both surfaces of a lens with negative refractive power that is made of a high dispersion material.

4. The objective according to claim 2, wherein the second lens group includes a three-lens-cemented lens that is formed by respectively cementing lenses with positive refractive power that are made of a low dispersion material to both surfaces of a lens with negative refractive power that is made of a high dispersion material.

5. The objective according to claim 1, wherein the first lens group includes a seventh lens component that is a single lens or cemented lens with positive refractive power, closer to the image side than the third lens component.

6. The objective according to claim 2, wherein the first lens group includes a seventh lens component that is a single lens or cemented lens with positive refractive power, closer to the image side than the third lens component.

7. The objective according to claim 3, wherein the first lens group includes a seventh lens component that is a single lens or cemented lens with positive refractive power, closer to the image side than the third lens component.

8. The objective according to claim 4, wherein the first lens group includes a seventh lens component that is a single lens or cemented lens with positive refractive power, closer to the image side than the third lens component.

9. The objective according to claim 1, wherein:

the third lens group includes a front lens group closest to the object side,

the front lens group includes: an eighth lens with positive refractive power that is made of a low dispersion material; and a ninth lens with negative refractive power that is made of a high dispersion material, the eighth lens and the ninth lens being arranged so as to be adjacent to each other,

a lens surface on a ninth-lens side of the eighth lens and a lens surface on an eighth lens-side of the ninth lens have a radius of curvature having the same sign, and

when fG30 represents a focal length of the front lens group, the objective satisfies the following conditional expression: −0.3≦f/fG30≦0.3   (12).

10. The objective according to claim 2, wherein:

the third lens group includes a front lens group closest to the object side,

the front lens group includes: an eighth lens with positive refractive power that is made of a low dispersion material; and a ninth lens with negative refractive power that is made of a high dispersion material, the eighth lens and the ninth lens being arranged so as to be adjacent to each other,

a lens surface on a ninth-lens side of the eighth lens and a lens surface on an eighth lens-side of the ninth lens have a radius of curvature having the same sign, and

when fG30 represents a focal length of the front lens group, the objective satisfies the following conditional expression: −0.3≦f/fG30≦0.3   (12).

11. The objective according to claim 3, wherein:

the third lens group includes a front lens group closest to the object side,

the front lens group includes: an eighth lens with positive refractive power that is made of a low dispersion material; and a ninth lens with negative refractive power that is made of a high dispersion material, the eighth lens and the ninth lens being arranged so as to be adjacent to each other,

a lens surface on a ninth-lens side of the eighth lens and a lens surface on an eighth lens-side of the ninth lens have a radius of curvature having the same sign, and

when fG30 represents a focal length of the front lens group, the objective satisfies the following conditional expression: −0.3≦f/fG30≦0.3   (12).

12. The objective according to claim 4, wherein:

the third lens group includes a front lens group closest to the object side,

the front lens group includes: an eighth lens with positive refractive power that is made of a low dispersion material; and a ninth lens with negative refractive power that is made of a high dispersion material, the eighth lens and the ninth lens being arranged so as to be adjacent to each other,

a lens surface on a ninth-lens side of the eighth lens and a lens surface on an eighth lens-side of the ninth lens have a radius of curvature having the same sign, and

when fG0 represents a focal length of the front lens group, the objective satisfies the following conditional expression: −0.3≦f/fG30≦0.3   (12).

13. The objective according to claim 5, wherein:

the third lens group includes a front lens group closest to the object side,

the front lens group includes: an eighth lens with positive refractive power that is made of a low dispersion material; and a ninth lens with negative refractive power that is made of a high dispersion material, the eighth lens and the ninth lens being arranged so as to be adjacent to each other,

a lens surface on a ninth-lens side of the eighth lens and a lens surface on an eighth lens-side of the ninth lens have a radius of curvature having the same sign, and

when fG30 represents a focal length of the front lens group, the objective satisfies the following conditional expression: −0.3≦f/fG30≦0.3   (12).

14. The objective according to claim 6, wherein:

the third lens group includes a front lens group closest to the object side,

the front lens group includes: an eighth lens with positive refractive power that is made of a low dispersion material; and a ninth lens with negative refractive power that is made of a high dispersion material, the eighth lens and the ninth lens being arranged so as to be adjacent to each other,

a lens surface on a ninth-lens side of the eighth lens and a lens surface on an eighth lens-side of the ninth lens have a radius of curvature having the same sign, and

when fG30 represents a focal length of the front lens group, the objective satisfies the following conditional expression: −0.3≦f/fG30≦0.3   (12).

15. The objective according to claim 7, wherein:

the third lens group includes a front lens group closest to the object side,

the front lens group includes: an eighth lens with positive refractive power that is made of a low dispersion material; and a ninth lens with negative refractive power that is made of a high dispersion material, the eighth lens and the ninth lens being arranged so as to be adjacent to each other,

a lens surface on a ninth-lens side of the eighth lens and a lens surface on an eighth lens-side of the ninth lens have a radius of curvature having the same sign, and

when fG30 represents a focal length of the front lens group, the objective satisfies the following conditional expression: −0.3≦f/fG30≦0.3   (12).

16. The objective according to claim 1, wherein:

the third lens group includes a rear lens group with negative refractive power closest to the image side, and

when fG3I represents a focal length of the rear lens group, the objective satisfies the following conditional expression: −10≦fG3I/f≦−1.5   (15).

17. The objective according to claim 16, wherein the rear lens group includes two or more lens components with negative refractive power.

18. The objective according to claim 16, wherein:

the third lens group includes: a front lens group arranged closest to the object side; and an intermediate lens group arranged between the front lens group and the rear lens group, and

the intermediate lens group includes a tenth lens component that is configured of a single lens or cemented lens having a meniscus shape with a concave surface facing the object side.

19. The objective according to claim 1, wherein when r12 represents the radius of curvature of the lens surface on the image side of the first lens, and r21 represents a radius of curvature of a lens surface on the object side of the second lens, the objective satisfies the following conditional expression:

0.8≦r21/r12≦2   (16).

20. The objective according to claim 1, wherein a lens component closest to an image plane in the second lens group is a lens component with positive refractive power that is closest to the object among lens components other than lens components included in the first lens group and a lens component which the maximum ray height of the on-axis marginal ray passes through.