Optical system, lens device and imaging apparatus

Abstract

To provide favorable optical performance, while reducing the weight of the whole system in an optical system having a variable-power optical system to be inserted into / extracted from a main optical system.SOLUTION: An optical system L0 comprises a main optical system LM including an aperture stop SP, and a variable-power optical system EXT to be inserted into / extracted from between the aperture stop SP of the main optical system LM and an image surface IP. A distance from a lens surface closest to an object side, of the main optical system LM to the image surface IP before / after insertion / extraction of the variable-power optical system EXT is constant. The main optical system LM includes a plurality of positive lenses and a plurality of negative lenses. A distance from the lens surface closest to the object side, of the main optical system LM to a lens surface in the object side, of a negative lens G1N located closest to the object side, out of the plurality of negative lenses included in the main optical system LM, and the whole length of the main optical system LM satisfy a prescribed relation.SELECTED DRAWING: Figure 3

Description

[Technical Field]

[0001] The present invention relates to an optical system and is suitable for imaging devices such as digital video cameras, digital still cameras, broadcast cameras, and cameras for silver halide film. [Background technology]

[0002] A converter method is known as a method for changing the focal length of an optical system used in an imaging device, in which the focal length of the entire system is changed by inserting a variable magnification optical system (extender) into the optical path.

[0003] Patent Document 1 discloses an optical system having a variable magnification optical system that can be inserted and removed at a predetermined position on the image side of the aperture stop of the main optical system. [Prior art documents] [Patent documents]

[0004] [Patent Document 1] Japanese Patent Application Laid-Open No. 2013-238827 Summary of the Invention [Problem to be solved by the invention]

[0005] When adopting a system in which a variable magnification optical system is built in, in order to obtain good optical performance while reducing the weight of the entire system including the variable magnification optical system, it is important not only to appropriately select the insertion position of the variable magnification optical system, but also to appropriately configure the main optical system. The invention disclosed in Patent Document 1 left room for improvement in terms of achieving both weight reduction and optical performance.

[0006] The present invention aims to achieve good optical performance while reducing the weight of the entire optical system in an optical system having a variable magnification optical system that can be inserted into and removed from the main optical system. [Means for solving the problem]

[0007] The optical system of the present invention includes a main optical system having an aperture stop, and a variable magnification optical system that is inserted or removed between the aperture stop and an image plane, wherein a distance from a lens surface of the main optical system closest to the object side to an image plane is constant before and after the insertion or removal of the variable magnification optical system, and the main optical system includes, in order from the closest to the object side to the image side, a positive lens G1P, a positive lens G2P, and a cemented lens, the cemented lens consisting of a positive lens A and a negative lens G1N, and the main optical system includes a negative lens B, Let D1N be the distance from the lens surface closest to the object in the main optical system to the lens surface closest to the object of the negative lens G1N located closest to the object among the plurality of negative lenses, and LD be the distance from the lens surface closest to the object in the main optical system to the image plane. 0.20 <D1N / LD<0.50 The present invention is characterized in that the following conditional expression is satisfied: [Effects of the Invention]

[0008] According to the present invention, in an optical system having a variable magnification optical system that can be inserted into and removed from a main optical system, it is possible to achieve good optical performance while reducing the weight of the entire system. [Brief explanation of the drawings]

[0009] [Figure 1] FIG. 2 is a cross-sectional view of the main optical system of the first embodiment. [Figure 2] 4A to 4C are aberration diagrams of the main optical system of Example 1. [Figure 3] FIG. 2 is a cross-sectional view of the optical system of Example 1 in a state where a variable magnification optical system is inserted. [Figure 4] 4A to 4C are aberration diagrams of the optical system of Example 1 in a state where a variable magnification optical system is inserted. [Figure 5] FIG. 10 is a cross-sectional view of the main optical system of Example 2. [Figure 6] 10A to 10C are aberration diagrams of the main optical system of Example 2. [Figure 7] FIG. 10 is a cross-sectional view of the optical system of Example 2 in a state where a variable magnification optical system is inserted. [Figure 8] 10A and 10B are aberration diagrams of the optical system of Example 2 in a state where the variable magnification optical system is inserted. [Figure 9]FIG. 10 is a cross-sectional view of the main optical system of Example 3. [Figure 10] 10A to 10C are aberration diagrams of the main optical system of Example 3. [Figure 11] FIG. 10 is a cross-sectional view of the optical system of Example 3 in a state where a variable magnification optical system is inserted. [Figure 12] 10A and 10B are aberration diagrams of the optical system of Example 3 in a state where the variable magnification optical system is inserted. [Figure 13] FIG. 1 is a schematic diagram showing a lens device. [Figure 14] FIG. 1 is a schematic diagram showing an imaging device. DETAILED DESCRIPTION OF THE INVENTION

[0010] Hereinafter, embodiments of the optical system of the present invention, and a lens device and an imaging device having the same will be described with reference to the accompanying drawings.

[0011] Figures 1, 3, 5, 7, 9, and 11 are cross-sectional views of the optical systems L0 of Examples 1 to 3, respectively, when focused at infinity. The optical system L0 of each Example has a main optical system LM and a variable magnification optical system EXT. Figures 1, 5, and 9 show cross-sectional views of the main optical system LM of the optical system L0 of each Example. Also, Figures 3, 7, and 11 show cross-sectional views of the optical system L0 of each Example, with the variable magnification optical system EXT inserted in the optical path of the main optical system LM. The optical system L0 of each Example can be used in imaging devices such as digital video cameras, digital still cameras, broadcast cameras, silver halide film cameras, and surveillance cameras.

[0012] In each cross-sectional view, the left side is the object side and the right side is the image side. SP is an aperture stop. IP is an image plane, and when the optical system L0 of each embodiment is used as an imaging optical system for a digital video camera or digital still camera, the imaging surface of a solid-state imaging element (photoelectric conversion element) such as a CCD sensor or CMOS sensor is arranged on the image plane IP. When the optical system L0 of each embodiment is used as an imaging optical system for a silver halide film camera, the photosensitive surface of the film is arranged on the image plane IP.

[0013] The main optical system LM is an optical system that can be used alone for photography and includes multiple positive lenses and multiple negative lenses. The variable magnification optical system EXT is configured to be insertable into and removable from the optical path of the main optical system LM. In each embodiment, the variable magnification optical system EXT has negative refractive power, and the conversion magnification (focal length expansion ratio) M is 1.4. In other words, when the variable magnification optical system EXT is inserted into the optical path of the main optical system LM, the overall focal length of the optical system L0 is extended. In each embodiment, the variable magnification optical system EXT is inserted or removed between the aperture stop SP and the image plane IP. Furthermore, in each embodiment, the overall lens length (the distance from the lens surface closest to the object to the image plane IP) remains constant before and after the variable magnification optical system EXT is inserted or removed.

[0014] In the optical system L0 of each embodiment, at least one lens group moves during focusing. LF1, LF2, and LF are focus lens groups that move during focusing. The direction of movement of each focus lens group during focusing from infinity to a close distance is indicated by an arrow in each cross-sectional view. In the optical system L0 of each embodiment, the number of lens groups that move during focusing may be one or more.

[0015] Figures 2, 4, 6, 8, 10, and 12 are longitudinal aberration diagrams of the optical systems of the respective examples when focused at infinity. Of these, Figures 2, 6, and 10 show aberration diagrams of the main optical system LM of the optical system L0 of the respective examples. Also, Figures 4, 8, and 12 show aberration diagrams of the optical system L0 of the respective examples when a variable magnification optical system EXT is inserted in the optical path of the main optical system LM.

[0016] In the spherical aberration diagram, FNo is the F-number. In the spherical aberration diagram, the amount of spherical aberration for the d-line (wavelength 587.6 nm) and g-line (wavelength 435.8 nm) is shown by the solid line and the two-dot chain line, respectively. In the astigmatism diagram, ΔS indicates the amount of astigmatism on the sagittal image plane (solid line), and ΔM indicates the amount of astigmatism on the meridional image plane (dashed line). In the distortion diagram, the amount of distortion for the d-line is shown. In the chromatic aberration diagram, the amount of chromatic aberration for the g-line is shown. Note that ω is the half angle of view (°).

[0017] Next, the characteristic configuration and conditions of the optical system L0 of each embodiment will be described.

[0018] When the main optical system LM is a telephoto lens, the closer the lens is to the object, the larger its effective diameter and outer diameter become. For this reason, if the variable magnification optical system EXT is inserted into a position relatively closer to the object of the main optical system LM, it becomes difficult to reduce the size of the variable magnification optical system EXT. Furthermore, there are cases where the spherical aberration and coma of the optical system L0 fluctuate greatly before and after the insertion of the variable magnification optical system EXT.

[0019] For this reason, in the optical system of each embodiment, the magnification changing aperture EXT is located between the aperture stop SP and the image plane IP at L0. This makes it possible to reduce the diameter of the light beam incident on the magnification changing optical system EXT, thereby achieving a more compact size of the magnification changing optical system EXT. Furthermore, fluctuations in spherical aberration and coma before and after the insertion of the magnification changing optical system EXT are reduced.

[0020] However, when a variable magnification optical system is configured to be insertable into or removable from the optical path of the main optical system, a mechanism for inserting and removing the variable magnification optical system must be provided in the lens device, which tends to increase the weight of the entire lens device, making it important to reduce the weight of the entire optical system, including the main optical system.

[0021] To reduce the weight of an optical system, it is necessary to reduce the weight of each lens that makes up the optical system. To reduce the weight of each lens, it is necessary to reduce the effective diameter of each lens. Furthermore, when comparing a positive lens and a negative lens with the same refractive power, the negative lens tends to be heavier.

[0022] For this reason, in the optical system L0 of each embodiment, the negative lens G1N, which is located closest to the object among the negative lenses in the main optical system LM, is positioned appropriately lower toward the image side. This allows light rays that have been sufficiently converged by one or more positive lenses located on the object side of the negative lens G1N to be incident on the negative lens G1N, making it possible to effectively reduce the diameter of the negative lens G1N. As a result, it is possible to configure the optical system L0 to be lightweight.

[0023] Specifically, the optical system L0 in each embodiment is configured to satisfy the following conditional expressions.

[0024] 0.20 <D1N / LD<0.50 (1) Here, D1N is the distance from the lens surface closest to the object in the optical system L0 to the lens surface closest to the object in the negative lens G1N, and LD is the distance from the lens surface closest to the object in the optical system L0 to the image plane IP (total lens length).

[0025] Conditional formula (1) is a condition for achieving good optical performance while reducing the weight of optical system L0. If the value of D1N / LD is below the lower limit of conditional formula (1), the negative lens G1N will be too close to the object side, and the effective diameter of the negative lens G1N will be too large. This will increase the mass of the negative lens G1N. If the value of D1N / LD is above the upper limit of conditional formula (1), the negative lens G1N will be too close to the image side, and the height of incidence of axial rays incident on the negative lens G1N will be too low. As a result, it will be difficult for the negative lens G1N to correct the spherical aberration of optical system L0.

[0026] With the above configuration, in an optical system having a variable magnification optical system that can be inserted into and removed from the main optical system, it is possible to achieve good optical performance while reducing the weight of the entire system.

[0027] It is more preferable that at least one of the upper limit and lower limit of the numerical range of conditional expression (1) satisfies the following conditional expression (1a), and even more preferable that it satisfies conditional expression (1b).

[0028] 0.23 <D1N / LD<0.47 (1a) 0.25 <D1N / LD<0.45 (1b) Next, conditions that the optical system L0 of each embodiment should preferably satisfy will be described. The optical system L0 of each embodiment should preferably satisfy one or more of the following conditional expressions.

[0029] 0.40 <LD / f<1.20 (2) 0.40 <Le / Lp<0.97 (3) -0.80 <fe / f<-0.20 (4) 1.0 <fa / f<9.0 (5) 0.20 <fb / f<0.90 (6) -18 <fa / fe<-2.0 (7) -3.5 <fb / fe<-0.30 (8) 1.58 <ndG1N<1.89 (9) 22<νdG1N<55 (10) -1.3 <SFG1N<0.50 (11) 1.41 <ndG1P<1.69 (12) 55<νdG1P<95 (13) 1.40 <ndG2P<1.67 (14) 55<νdG2P<99 (15) -0.95 <fG1N / f<-0.08 (16) 0.50 <fG1P / f<3.0 (17) -9.9 <fG1P / fG1N<-1.5 (18) 0.90 <fG1P / fG2P<3.0 (19) Conditional formula (2) defines the conditions related to the total lens length LD and the focal length f of the entire optical system when the variable magnification optical system EXT is not inserted. In other words, f is the focal length of the main optical system LM. If the value of LD / f is below the lower limit of conditional formula (2), the total lens length becomes short, making it difficult to correct axial chromatic aberration and lateral chromatic aberration in a balanced manner. If the value of LD / f is above the upper limit of conditional formula (2), aberration correction becomes easier, but the optical system L0 and the lens barrel that holds it become larger.

[0030] Conditional expression (3) defines the conditions for the distance Le from the lens surface closest to the object in variable magnification optical system EXT to the image plane IP, and the distance Lp from the aperture stop SP to the image plane IP. If the value of Le / Lp falls below the lower limit of conditional expression (3), the insertion / removal position of variable magnification optical system EXT becomes too close to the image plane IP, increasing the incidence height of off-axial rays passing through variable magnification optical system EXT. As a result, it becomes difficult to sufficiently compact the variable magnification optical system EXT. If the value of Le / Lp exceeds the upper limit of conditional expression (3), the insertion / removal position of variable magnification optical system EXT becomes too close to the aperture stop SP, increasing the incidence height of on-axial rays passing through variable magnification optical system EXT. In this case, too, it becomes difficult to sufficiently compact the variable magnification optical system EXT.

[0031] Conditional expression (4) defines the condition regarding the focal length fe of the variable magnification optical system EXT and the focal length f of the entire optical system when the variable magnification optical system EXT is not inserted. If the focal length fe of the variable magnification optical system EXT becomes so long that the value of fe / f falls below the lower limit of conditional expression (4), the change in magnification becomes small, which is undesirable. If the focal length fe of the variable magnification optical system EXT becomes so short that the value of fe / f exceeds the upper limit of conditional expression (4), it becomes difficult to sufficiently suppress fluctuations in various aberrations, such as spherical aberration, before and after the variable magnification optical system EXT is inserted and removed.

[0032] Conditional expression (5) defines the condition regarding the combined focal length fa of the partial optical system located closer to the object side than the position of the main optical system LM where the variable magnification optical system EXT is inserted, and the focal length f of the entire optical system when the variable magnification optical system EXT is not inserted. If the value of fa / f is below the lower limit of conditional expression (5), it is advantageous for reducing the size of the variable magnification optical system EXT because it is possible to sufficiently converge the light rays incident on the variable magnification optical system EXT. However, the sensitivity of the image plane position to the insertion position of the variable magnification optical system EXT becomes too high. This results in manufacturing difficulties, which is undesirable. If the value of fa / f exceeds the upper limit of conditional expression (5), the light rays incident on the variable magnification optical system EXT approach afocal, increasing the height of incidence of axial light rays passing through the variable magnification optical system EXT. As a result, it becomes difficult to sufficiently reduce the size of the variable magnification optical system EXT.

[0033] Conditional expression (6) defines the condition regarding the combined focal length fb of the partial optical system located on the image side of the position where the variable magnification optical system EXT of the main optical system LM is inserted, and the focal length f of the entire optical system when the variable magnification optical system EXT is not inserted. If the value of fb / f falls below the lower limit of conditional expression (6), the focal length on the image side of the position where the variable magnification optical system EXT is inserted becomes too short, making it difficult to sufficiently correct various aberrations, such as field curvature, that occur in the lens group on the image side of the position where the variable magnification optical system EXT is inserted. If the value of fb / f exceeds the upper limit of conditional expression (6), the focal length on the image side of the position where the variable magnification optical system EXT is inserted becomes too long, making the distance from the variable magnification optical system EXT to the image plane IP long. As a result, it becomes difficult to sufficiently miniaturize the optical system L0.

[0034] Conditional formula (7) defines the condition regarding the focal length fa of the main optical system LM on the object side of the position where the variable magnification optical system EXT is inserted, and the focal length fe of the variable magnification optical system EXT. If the value of fa / fe falls below the lower limit of conditional formula (7), the light rays entering the variable magnification optical system EXT will approach afocal, and the height of incidence of axial light rays passing through the variable magnification optical system EXT will increase. As a result, it will be difficult to sufficiently reduce the size of the variable magnification optical system EXT. If the value of fa / fe exceeds the upper limit of conditional formula (7), it will be advantageous for reducing the size of the variable magnification optical system EXT in that the light rays entering the variable magnification optical system EXT can be sufficiently converged. However, the sensitivity of the image plane position to the insertion position of the variable magnification optical system EXT will become too high. This will result in manufacturing difficulties, which is undesirable.

[0035] Conditional expression (8) defines the conditions for the focal length fb on the image side of the position of the main optical system LM where the variable magnification optical system EXT is inserted, and the focal length fe of the variable magnification optical system EXT. If the value of fb / fe is below the lower limit of conditional expression (8), the focal length on the image side will be longer than the position where the variable magnification optical system EXT is inserted, and the distance from the variable magnification optical system EXT to the image plane IP will be longer. As a result, it will be difficult to sufficiently compact the optical system L0. If the value of fb / fe is above the upper limit of conditional expression (8), the focal length on the image side will be shorter than the position where the variable magnification optical system EXT is inserted, and it will be difficult to sufficiently correct various aberrations, such as field curvature, that occur in the lens group on the image side of the position where the variable magnification optical system EXT is inserted.

[0036] Conditional expression (9) defines the condition regarding the refractive index ndG1N of the negative lens G1N. Generally, as the refractive index of a lens material increases, the specific gravity of the lens material increases. If the value of ndG1N falls below the lower limit of conditional expression (9), the radius of curvature of the lens surface that must be imparted to give the negative lens G1N the desired refractive power becomes too small, making it more likely that various aberrations, such as spherical aberration, will occur. If the value of ndG1N exceeds the upper limit of conditional expression (9), the specific gravity of the negative lens G1N increases, making it difficult to achieve a sufficient weight reduction.

[0037] Conditional formula (10) defines the condition for the Abbe number νdG1N of the negative lens G1N. Here, the Abbe number νd of a certain material is expressed by the following formula, where Nd, NF, and NC are the refractive indices at the d-line (587.6 nm), F-line (486.1 nm), and C-line (656.3 nm) of the Fraunhofer lines.

[0038] νd=(Nd-1) / (NF-NC) If the value of νdG1N is below the lower limit of conditional expression (10), a glass material with large dispersion will be used for the negative lens G1N. In this case, the variation in spherical aberration for each wavelength is likely to increase. In addition, generally, as the Abbe number of a lens material increases, the refractive index of the lens material decreases. If the value of νdG1N exceeds the upper limit of conditional expression (10), the radius of curvature of the negative lens G1N will become too small to obtain sufficient refractive power for correcting chromatic aberration. As a result, it becomes difficult to sufficiently correct coma aberration.

[0039] Conditional formula (11) defines the condition for the shape factor SFG1N of the negative lens G1N located closest to the object. Here, the shape factor of a lens is defined by the following formula, where R1 is the radius of curvature of the object-side surface of that lens and R2 is the radius of curvature of the image-side surface. In the case of an aspheric shape, the base R (the radius of the reference quadratic surface) is used as the radius of curvature.

[0040] SF=(R2+R1) / (R2-R1) If the value of SFG1N is below the lower limit of conditional expression (11), the radius of curvature of the negative lens G1N on the object side becomes large, making it difficult to suppress axial chromatic aberration and sufficiently correct coma aberration at the same time.If the value of SFG1N is above the upper limit of conditional expression (11), the radius of curvature of the negative lens G1N on the object side becomes small, making it difficult to sufficiently correct coma aberration.

[0041] Conditional expression (12) defines the condition for the refractive index ndG1P of the positive lens G1P located closest to the object in optical system L0. If the lower limit of conditional expression (12) is not met, the radius of curvature of the surface becomes small in order to obtain the refractive power of the lens, which is undesirable because various aberrations such as spherical aberration occur. If the upper limit of conditional expression (12) is exceeded, the specific gravity of the positive lens G1P becomes large, which makes it difficult to reduce the lens weight, which is undesirable.

[0042] Conditional expression (13) defines the condition related to the Abbe number νdG1P of the positive lens G1P located closest to the object in optical system L0. If the value of νdG1P is below the lower limit of conditional expression (13), it becomes difficult to sufficiently suppress axial chromatic aberration and lateral chromatic aberration. If the value of νdG1P is above the upper limit of conditional expression (13), the refractive index of the positive lens G1P becomes low, making it difficult to sufficiently suppress spherical aberration and coma.

[0043] Conditional expression (14) defines the condition for the refractive index ndG2P of the positive lens G2P, which is located closest to the object among the positive lenses located on the image side of the positive lens G1P. If the value of ndG2P is below the lower limit of conditional expression (14), the radius of curvature that must be imparted to the positive lens G2P to obtain the refractive power required becomes small, making it more likely that various aberrations, such as spherical aberration, will occur. If the value of ndG2P is above the upper limit of conditional expression (14), the specific gravity of the positive lens G2P becomes large, making it difficult to achieve sufficient weight reduction.

[0044] Conditional expression (15) defines the condition related to the Abbe number νdG2P of the positive lens element G2P. If the value of νdG2P falls below the lower limit of conditional expression (15), it becomes difficult to sufficiently suppress axial chromatic aberration and lateral chromatic aberration. If the value of νdG2P exceeds the upper limit of conditional expression (15), the refractive index of the positive lens element G2P becomes too low, making it difficult to sufficiently suppress spherical aberration and coma.

[0045] Conditional expression (16) defines the condition related to the focal length fG1N of the negative lens G1N and the focal length f of the entire optical system when the variable magnification optical system EXT is not inserted. If the value of fG1N / f is below the lower limit of conditional expression (16), the power of the negative lens G1N becomes too weak, making it difficult to effectively correct axial chromatic aberration and lateral chromatic aberration. If the value of fG1N / f is above the upper limit of conditional expression (16), the power of the negative lens G1N becomes too strong, making it difficult to sufficiently suppress various aberrations, such as spherical aberration.

[0046] Conditional expression (17) defines the condition relating to the focal length fG1P of the positive lens G1P located closest to the object and the focal length f of the entire optical system when the variable magnification optical system EXT is not inserted. If the value of fG1P / f is below the lower limit of conditional expression (17), the power of the positive lens G1P becomes too strong, making it difficult to sufficiently suppress various aberrations such as spherical aberration. If the value of fG1P / f is above the upper limit of conditional expression (17), the power of the positive lens G1P becomes too weak, making it difficult to effectively correct axial chromatic aberration and lateral chromatic aberration.

[0047] Conditional expression (18) defines the conditions related to the focal length fG1P of the positive lens G1P located closest to the object and the focal length fG1N of the negative lens G1N. If the value of fG1P / fG1N is below the lower limit of conditional expression (18), the power of the positive lens G1P becomes too weak, making it difficult to effectively correct axial chromatic aberration and lateral chromatic aberration. If the value of fG1P / fG1N is above the upper limit of conditional expression (18), the power of the positive lens G1P becomes too strong, making it difficult to adequately suppress various aberrations such as spherical aberration. Furthermore, if the power of the positive lens G1P becomes too strong, the radius of curvature of the positive lens G1P becomes small, which increases the volume of the positive lens G1P and makes it difficult to achieve a sufficient weight reduction.

[0048] Conditional expression (19) defines the conditions for the focal length fG1P of the positive lens G1P located closest to the object and the focal length fG2P of the positive lens G2P located closest to the object among the positive lenses located on the image side of the positive lens G1P. If the value of fG1P / fG2P is below the lower limit of conditional expression (19), the power of the positive lens G1P becomes too strong, making it difficult to sufficiently suppress various aberrations such as spherical aberration. Furthermore, if the power of the positive lens G1P becomes too strong, the radius of curvature of the positive lens G1P becomes small, resulting in an increase in the volume of the positive lens G1P and making it difficult to achieve sufficient weight reduction. If the value of fG1P / fG2P exceeds the upper limit of conditional expression (19), the power of the positive lens G1P becomes too weak, making it difficult to effectively correct axial chromatic aberration and lateral chromatic aberration.

[0049] It is more preferable that at least one of the upper limit values ​​or lower limit values ​​of the conditional expressions (2) to (19) be set to values ​​defined by the following conditional expressions (2a) to (19a).

[0050] 0.50 <LD / f<1.15 (2a) 0.45 <Le / Lp<0.95 (3a) -0.75 <fe / f<-0.25 (4a) 1.1 <fa / f<8.0 (5a) 0.22 <fb / f<0.85 (6a) -16 <fa / fe<-2.2 (7a) -3.3 <fb / fe<-0.35 (8a) 1.59 <ndG1N<1.87 (9a) 23<νdG1N<53 (10a) -1.2 <SFG1N<0.40 (11a) 1.42 <ndG1P<1.67 (12a) 58<νdG1P<85 (13a) 1.41 <ndG2P<1.65 (14a) 58<νdG2P<97 (15a) -0.95 <fG1N / f<-0.08 (16a) 0.55 <fG1P / f<2.8 (17a) -9.5 <fG1P / fG1N<-1.7 (18a) 0.95 <fG1P / fG2P<2.8 (19a) It is more preferable that at least one of the upper limit and lower limit of the conditional expressions (2) to (19) be a value defined by the following conditional expressions (2b) to (19b).

[0051] 0.60 <LD / f<1.10 (2b) 0.50 <Le / Lp<0.90 (3b) -0.70 <fe / f<-0.30 (4b) 1.2 <fa / f<7.0 (5b) 0.25 <fb / f<0.80 (6b) -14 <fa / fe<-2.5 (7b) -3.0 <fb / fe<-0.40 (8b) 1.60 <ndG1N<1.86 (9b) 24<νdG1N<50 (10b) -1.1 <SFG1N<0.30 (11b) 1.43 <ndG1P<1.65 (12b) 60<νdG1P<82 (13b) 1.42 <ndG2P<1.63 (14b) 60<νdG2P<96 (15b) -0.90 <fG1N / f<-0.10 (16b) 0.60 <fG1P / f<2.5 (17b) -9.0 <fG1P / fG1N<-2.0 (18b) 1.0 <fG1P / fG2P<2.5 (19b) Next, the configuration that is preferably satisfied in the optical system L0 of each embodiment will be described.

[0052] It is also preferable that the variable magnification optical system EXT includes two or more negative lenses and one or more positive lenses, which prevents the Petzval sum from becoming an excessively negative value and enables good correction of field curvature.

[0053] Furthermore, in the optical system L0 of each embodiment, some of the lenses in the main optical system LM may be configured as an image stabilization lens group that is driven in a direction perpendicular to the optical axis. In this case, since the effective diameter of the lens closer to the image side than the aperture stop SP tends to be small, it is preferable to position the image stabilization lens group closer to the image side than the aperture stop SP. This simplifies the holding mechanism that holds the image stabilization lens group and the driving mechanism that drives it, and reduces the weight of the lens device including the optical system L0.

[0054] Preferably, the variable magnification optical system EXT is inserted and removed at a position between lenses included in the main optical system LM. In other words, the variable magnification optical system EXT is inserted and removed at a position that is not closest to the image side of the main optical system LM. This allows the diameter of the variable magnification optical system EXT to be made even smaller.

[0055] Furthermore, the lens group that moves during focusing may be moved in conjunction with inserting or removing the variable magnification optical system EXT. Although the in-focus position may change when the variable magnification optical system EXT is inserted or removed, by appropriately moving the focus lens group, it is possible to reduce the change in the in-focus position that occurs when the variable magnification optical system EXT is inserted or removed.

[0056] Preferably, the variable magnification optical system EXT has a positive single lens closest to the object. The variable magnification optical system EXT also has at least one cemented lens. The at least one cemented lens may be at least one of a cemented lens formed by cementing a positive lens and a negative lens, a cemented lens formed by cementing a negative lens, a positive lens and a negative lens, or a cemented lens formed by cementing a positive lens and a negative lens. The variable magnification optical system EXT may have all of these cemented lenses. By providing the variable magnification optical system EXT with at least one cemented lens, chromatic aberration can be reduced while also improving ease of manufacture.

[0057] The variable magnification optical system EXT in the optical system L0 of Example 1 is composed of, arranged in order from the object side to the image side, a positive lens, a cemented lens formed by cementing a positive lens and a negative lens, a cemented lens formed by cementing a negative lens, a positive lens and a negative lens, and a cemented lens formed by cementing a positive lens and a negative lens.

[0058] The variable magnification optical system EXT in the optical system L0 of Example 2 is composed of, arranged in order from the object side to the image side, a positive lens, a cemented lens formed by cementing a positive lens and a negative lens, a cemented lens formed by cementing a negative lens, a positive lens and a negative lens, and a cemented lens formed by cementing a positive lens and a negative lens.

[0059] The variable magnification optical system EXT in the optical system L0 of Example 3 is composed of, arranged in order from the object side to the image side, a positive lens, a cemented lens formed by cementing a positive lens and a negative lens, a cemented lens formed by cementing a negative lens, a positive lens and a negative lens, and a cemented lens formed by cementing a positive lens and a negative lens.

[0060] Next, Numerical Examples 1 to 3 corresponding to Examples 1 to 3, respectively, are shown.

[0061] In each numerical example, each surface of the optical system is assigned a surface number i (i is a natural number) from the object side. r is the radius of curvature of each surface (mm), d is the lens thickness or distance (air gap) (mm) on the optical axis between the surface with surface number i and the surface with surface number (i+1), nd is the refractive index for the d-line of the material of the optical element that makes up each surface, and νd is the Abbe number for the d-line of the material of the optical element that makes up each surface.

[0062] The focal length (mm), F-number, and half angle of view (°) are values ​​when the optical system is focused on an object at infinity. The total lens length is the distance on the optical axis from the front surface of the optical system (the lens surface closest to the object) to the last surface (the lens surface closest to the image) plus the back focal length SK. The back focal length SK is the distance from the last surface of the optical system to the image plane IP.

[0063] Table 1 shows the values ​​corresponding to the above-mentioned conditional expressions (1) to (19) in Numerical Examples 1 to 3.

[0064] In each numerical example, each surface of the optical system is assigned a surface number i (i is a natural number) from the object side. r is the radius of curvature of each surface (mm), d is the lens thickness or distance (air gap) (mm) on the optical axis between the surface with surface number i and the surface with surface number (i+1), nd is the refractive index for the d-line of the material of the optical element that makes up each surface, and νd is the Abbe number for the d-line of the material of the optical element that makes up each surface.

[0065] The focal length (mm), F-number, and half angle of view (°) are values ​​when the optical system is focused on an object at infinity. The total lens length is the distance on the optical axis from the front surface of the optical system (the lens surface closest to the object) to the last surface (the lens surface closest to the image) plus the back focal length SK. The back focal length SK is the air-equivalent distance from the last surface of the optical system to the image plane IP.

[0066] [Numerical Example 1] <Optical system (main optical system) without variable magnification optical system inserted> Unit: mm Surface Data Surface number rd nd νd 1 443.570 8.20 1.48749 70.2 2 -1502.142 0.10 3 227.620 12.00 1.43387 95.1 4 1755.996 97.18 5 173.310 11.00 1.43387 95.1 6 -251.525 0.11 7 -260.995 2.90 1.67300 38.3 8 261.833 59.16 9 79.404 6.60 1.92286 20.9 10 737.207 0.14 11 585.117 1.70 2.00069 25.5 12 52.050 8.90 1.49700 81.5 13 325.993 (variable) 14 73.892 6.20 1.49700 81.5 15 -10892.169 (variable) 16 742.447 1.80 1.75500 52.3 17 63.613 (variable) 18 (Aperture) ∞ 7.09 19 250.640 1.80 1.51742 52.4 20 51.522 3.81 21 -330.459 4.07 1.75211 25.0 22 -59.091 1.80 1.49700 81.5 23 55.745 4.60 24 87.576 3.80 1.49700 81.5 25 -198.126 40.26 26 528.989 5.50 1.51742 52.4 27 -57.284 5.00 28 ∞ 1.50 1.51633 64.1 29∞5.42 30 -351.519 1.50 1.49700 81.5 31 43.426 8.80 1.72916 54.7 32 -141.620 5.35 33 -97.918 1.50 1.96300 24.1 34 212.566 53.83 Image plane ∞ Various data Focal length 389.00 F-number 2.91 Half angle of view (°) 3.18 Image height 21.64 Lens total length 406.00 BF 53.83 d13 12.82 d15 2.00 d17 19.58 <Optical system with variable magnification optical system inserted> Unit: mm Surface Data Surface number rd nd νd 1 443.570 8.20 1.48749 70.2 2 -1502.142 0.10 3 227.620 12.00 1.43387 95.1 4 1755.996 97.18 5 173.310 11.00 1.43387 95.1 6 -251.525 0.11 7 -260.995 2.90 1.67300 38.3 8 261.833 59.16 9 79.404 6.60 1.92286 20.9 10 737.207 0.14 11 585.117 1.70 2.00069 25.5 12 52.050 8.90 1.49700 81.5 13 325.993 (variable) 14 73.892 6.20 1.49700 81.5 15 -10892.169 (variable) 16 742.447 1.80 1.75500 52.3 17 63.613 (variable) 18 (Aperture) ∞ 7.09 19 250.640 1.80 1.51742 52.4 20 51.522 3.81 21 -330.459 4.07 1.75211 25.0 22 -59.091 1.80 1.49700 81.5 23 55.745 4.60 24 87.576 3.80 1.49700 81.5 25 -198.126 2.00 26 30.159 5.00 1.49700 81.5 27 -605.295 0.30 28 120.765 1.82 1.59282 68.6 29 206.372 1.15 1.83400 37.2 30 34.364 9.75 31 -446.680 0.95 1.83481 42.7 32 23.747 8.90 1.71736 29.5 33 -28.370 0.95 1.75500 52.3 34 82.953 1.03 35 63.608 5.36 1.85451 25.2 36 -40.564 1.05 1.95906 17.5 37 1592.914 2.00 38 528.989 5.50 1.51742 52.4 39 -57.284 5.00 40 ∞ 1.50 1.51633 64.1 41∞5.42 42 -351.519 1.50 1.49700 81.5 43 43.426 8.80 1.72916 54.7 44 -141.620 5.35 45 -97.918 1.50 1.96300 24.1 46 212.566 53.83 Image plane ∞ Various data Focal length 544.00 F-number 4.19 Angle of view (°) 2.28 Image height 21.64 Lens total length 406.01 BF 53.83 d13 11.54 d15 8.40 d17 14.46 Lens group data Group starting plane focal length 1 1 290.40 2 14 147.70 3 16 -92.26 4 18 -169.51 5 26 -199.87 6 38 135.82

[0067] [Numerical Example 2] <Optical system (main optical system) without variable magnification optical system inserted> Unit: mm Surface Data Surface number rd nd νd 1 471.114 6.00 1.48749 70.2 2 1760.840 0.10 3 322.972 8.00 1.49700 81.5 4 1400.852 0.10 5 245.037 11.00 1.43387 95.1 6 989.532 89.45 7 174.097 11.00 1.43387 95.1 8 -331.734 0.11 9 -356.387 2.90 1.61340 44.3 10 134.086 71.24 11 130.092 5.40 1.86966 20.0 12 317.855 0.14 13 214.727 1.70 2.00069 25.5 14 79.631 8.90 1.49700 81.5 15 631.283 (variable) 16 95.682 6.20 1.49700 81.5 17 -5591.123 (variable) 18 -1600.590 1.80 1.72916 54.7 19 96.670 (variable) 20 (Aperture) ∞ 7.09 21 111.583 1.80 1.75500 52.3 22 46.851 3.81 23 -213.812 4.06 1.77047 29.7 24 -49.407 1.80 1.49700 81.5 25 75.645 4.60 26 55.135 3.80 1.80810 22.8 27 108.917 40.26 28 58.249 5.50 1.51633 64.1 29 -95.700 5.00 30 ∞ 1.50 1.51633 64.1 31∞2.65 32 -2507.527 1.50 1.59522 67.7 33 29.558 8.80 1.51633 64.1 34 -57.500 1.51 35 -45.670 1.50 1.77830 23.9 36 996.155 81.91 Image plane ∞ Various data Focal length 582.00 F-number 4.12 Angle of view (°) 2.13 Image height 21.64 Lens total length 486.10 BF 81.91 d15 19.60 d17 2.00 d19 63.39 <Optical system with variable magnification optical system inserted> Unit: mm Surface Data Surface number rd nd νd 1 471.114 6.00 1.48749 70.2 2 1760.840 0.10 3 322.972 8.00 1.49700 81.5 4 1400.852 0.10 5 245.037 11.00 1.43387 95.1 6 989.532 89.45 7 174.097 11.00 1.43387 95.1 8 -331.734 0.11 9 -356.387 2.90 1.61340 44.3 10 134.086 71.24 11 130.092 5.40 1.86966 20.0 12 317.855 0.14 13 214.727 1.70 2.00069 25.5 14 79.631 8.90 1.49700 81.5 15 631.283 (variable) 16 95.682 6.20 1.49700 81.5 17 -5591.123 (variable) 18 -1600.590 1.80 1.72916 54.7 19 96.670 (variable) 20 (Aperture) ∞ 7.09 21 111.583 1.80 1.75500 52.3 22 46.851 3.81 23 -213.812 4.06 1.77047 29.7 24 -49.407 1.80 1.49700 81.5 25 75.645 4.60 26 55.135 3.80 1.80810 22.8 27 108.917 2.00 28 28.202 8.05 1.49700 81.5 29 -218.478 0.30 30 224.895 4.82 1.63930 44.9 31 -44.418 1.15 1.72916 54.7 32 28.436 7.01 33 -558.701 0.95 1.83481 42.7 34 23.736 6.71 1.63980 34.5 35 -37.643 0.95 1.59522 67.7 36 108.150 1.24 37 53.148 4.03 1.72825 28.5 38 -47.560 1.05 1.95906 17.5 39 -731.126 2.00 40 58.249 5.50 1.51633 64.1 41 -95.700 5.00 42 ∞ 1.50 1.51633 64.1 43∞2.65 44 -2507.527 1.50 1.59522 67.7 45 29.558 8.80 1.51633 64.1 46 -57.500 1.51 47 -45.670 1.50 1.77830 23.9 48 996.155 81.91 Image plane ∞ Various data Focal length 814.80 F-number 5.88 Angle of view (°) 1.52 Image height 21.64 Lens total length 486.10 BF 81.91 d15 17.65 d17 6.73 d19 60.60

[0068] [Numerical Example 3] <Optical system (main optical system) without variable magnification optical system inserted> Unit: mm Surface Data Surface number rd nd νd 1 141.008 11.19 1.59349 67.0 2 1282.754 97.18 3 77.593 8.14 1.49700 81.5 4 -987.708 0.67 5 -476.470 1.80 1.85451 25.2 6 70.845 0.15 7 55.636 8.74 1.43387 95.1 8 -4252.064 2.00 9 59.636 5.45 1.92286 20.9 10 209.603 1.04 11 461.866 1.70 1.75500 52.3 12 33.933 8.90 1.43875 94.7 13 323.847 3.31 14 (Aperture) ∞ (Variable) 15 -985.903 1.30 1.59349 67.0 16 58.442 (variable) 17 1420.368 1.20 1.95906 17.5 18 93.617 3.81 19 -90.465 3.00 1.51633 64.1 20 -56.920 1.20 1.51742 52.4 21 1426.553 4.60 22 233.160 3.80 1.77830 23.9 23 -79.655 49.56 24 136.777 5.50 1.53172 48.8 25 -79.822 2.00 26 ∞ 1.50 1.51633 64.1 27∞4.85 28 -113.057 1.50 1.49700 81.5 29 43.851 6.20 1.75500 52.3 30 -1059.672 3.13 31 -137.877 1.50 1.77830 23.9 32 231.852 49.68 Image plane ∞ Various data Focal length 300.00 F-number 2.91 Angle of view (°) 4.12 Image height 21.64 Lens total length 320.00 BF 49.68 d14 2.00 d16 23.40 d23 49.56 <Optical system with magnification conversion optical system inserted> Unit: mm Surface Data Surface number rd nd νd 1 141.008 11.19 1.59349 67.0 2 1282.754 97.18 3 77.593 8.14 1.49700 81.5 4 -987.708 0.67 5 -476.470 1.80 1.85451 25.2 6 70.845 0.15 7 55.636 8.74 1.43387 95.1 8 -4252.064 2.00 9 59.636 5.45 1.92286 20.9 10 209.603 1.04 11 461.866 1.70 1.75500 52.3 12 33.933 8.90 1.43875 94.7 13 323.847 3.31 14 (Aperture) ∞ (Variable) 15 -985.903 1.30 1.59349 67.0 16 58.442 (variable) 17 1420.368 1.20 1.95906 17.5 18 93.617 3.81 19 -90.465 3.00 1.51633 64.1 20 -56.920 1.20 1.51742 52.4 21 1426.553 4.60 22 233.160 3.80 1.77830 23.9 23 -79.655 2.00 24 35.477 5.01 1.49700 81.5 25 1767.349 0.30 26 100.332 2.14 1.51742 52.4 27 228.702 1.15 1.75500 52.3 28 43.892 22.29 29 -331.482 0.95 1.91082 35.3 30 25.138 7.45 1.66565 35.6 31 -24.346 0.95 1.72916 54.7 32 50.780 0.14 33 46.762 4.13 1.85478 24.8 34 -52.455 1.05 1.95906 17.5 35 -524.464 2.00 36 136.777 5.50 1.53172 48.8 37 -79.822 2.00 38 ∞ 1.50 1.51633 64.1 39∞4.85 40 -113.057 1.50 1.49700 81.5 41 43.851 6.20 1.75500 52.3 42 -1059.672 3.13 43 -137.877 1.50 1.77830 23.9 44 231.852 49.68 Image plane ∞ Various data Focal length 420.00 F-number 4.12 Angle of view (°) 2.95 Image height 21.64 Lens total length 320.00 BF 49.68 d14 6.00 d16 19.41 The table below shows the various values ​​for each example.

[0069] [Table 1]

[0070] [Lens device] Next, an embodiment of a lens apparatus 100 using the optical system of the present invention will be described with reference to Fig. 13. The lens apparatus 100 is an interchangeable lens in an interchangeable lens camera system.

[0071] The lens device 100 has a main optical system 102, a variable magnification optical system 103, a lens barrel 101 that holds the main optical system 102 and the variable magnification optical system 103, and a mount unit 105 for coupling to a camera body. The main optical system 102 and the variable magnification optical system 103 have the characteristics described in Examples 1 to 3, and satisfy at least conditional expression (1).

[0072] The main optical system 102 and the variable magnification optical system 103 included in the lens device 100 of this embodiment have the same characteristics as any of the above-mentioned embodiments 1 to 3, and therefore it is possible to obtain good optical performance while reducing the weight of the entire system.

[0073] The lens barrel 101 has a retraction section 104 that forms a retraction space for retracting the variable magnification optical system 103 from the optical path of the main optical system 102. The lens barrel 101 may also include a plurality of lens holding members, a focus lens movement mechanism, various operation buttons, an operation ring, and the like, all of which are not shown. The retraction section 104 may be configured to be raised higher than the surrounding areas. In this case, the lens device 100 can be configured to be more compact.

[0074] The lens barrel 101 also has an operation unit 106 for inserting and removing the variable magnification optical system 103 into and from the optical path of the main optical system 102. The user can insert and remove the variable magnification optical system 103 into and from the optical path of the main optical system 102 by operating the operation unit 106. The operation unit 106 is configured, for example, with a lever-shaped member. It is preferable that the operation unit 106 be located closer to the mount unit 105 in the optical axis direction than the retraction unit 104. This improves the operability of the lens device 100 for the user.

[0075] [Imaging device] Next, an embodiment of a digital still camera (image capture device) using the optical system of the present invention will be described with reference to Fig. 14. In Fig. 14, 10 is a camera body, and 11 is a lens device including any of the optical systems L0 described in Examples 1 to 3. The lens 11 is provided with a space for retracting the variable magnification optical system EXT of the optical system L0 from the optical path of the main optical system LM, and with an operating member (such as a lever) for inserting and removing the variable magnification optical system EXT into and from the main optical system LM.

[0076] Reference numeral 12 denotes a solid-state image sensor (photoelectric conversion element) such as a CCD sensor or CMOS sensor that is built into the camera body and receives and photoelectrically converts the optical image formed by the lens device 11. The camera body 10 may be a so-called single-lens reflex camera that has a quick-turn mirror, or a so-called mirrorless camera that does not have a quick-turn mirror.

[0077] In this way, by applying the optical system L0 of the present invention to an imaging device such as a digital still camera, it is possible to obtain good optical performance while reducing the weight of the entire system in a configuration in which a variable magnification optical system can be inserted and removed.

[0078] Although the preferred embodiments and examples of the present invention have been described above, the present invention is not limited to these embodiments and examples, and various combinations, modifications, and changes are possible within the scope of the gist of the present invention. [Explanation of symbols]

[0079] L0 optical system LM main optical system SP aperture stop EXT variable magnification optical system

Claims

1. a main optical system having an aperture stop, and a variable magnification optical system inserted and removed between the aperture stop and an image plane, the distance from the lens surface of the main optical system closest to the object side to the image plane is constant before and after the insertion and removal of the variable magnification optical system; the main optical system includes, in order from the object side to the image side, a positive lens G1P, a positive lens G2P, and a cemented lens; The cemented lens is composed of a positive lens A and a negative lens G1N, the main optical system has a negative lens B, When the distance from the lens surface of the main optical system closest to the object side to the lens surface of the negative lens G1N is D1N and the distance from the lens surface of the main optical system closest to the object side to the image plane is LD, 0.20<D1N / LD<0.50 An optical system characterized by satisfying the following conditional expression:

2. When the focal length of the main optical system is f, 0.40<LD / f<1.20 2. The optical system according to claim 1, wherein the following condition is satisfied:

3. When the distance from the lens surface closest to the object side of the variable magnification optical system to the image plane is Le, and the distance from the aperture stop to the image plane is Lp, 0.40<Le / Lp<0.97 3. The optical system according to claim 1, wherein the following condition is satisfied:

4. When the focal length of the variable magnification optical system is fe and the focal length of the main optical system is f, -0.80<fe / f<-0.20 4. The optical system according to claim 1, wherein the following condition is satisfied:

5. When the focal length of a partial optical system disposed on the object side of the main optical system relative to the position where the variable magnification optical system is inserted is fa and the focal length of the main optical system is f, 1.0<fa / f<9.0 5. The optical system according to claim 1, wherein the following condition is satisfied:

6. When the focal length of a partial optical system arranged closer to the image side than the position where the variable magnification optical system is inserted in the main optical system is defined as fb, and the focal length of the main optical system is defined as f, 0.20<fb / f<0.90 6. The optical system according to claim 1, wherein the following condition is satisfied:

7. When the focal length of a partial optical system arranged on the object side of the main optical system relative to the position where the variable magnification optical system is inserted is fa and the focal length of the variable magnification optical system is fe, -18<fa / fe<-2.0 7. The optical system according to claim 1, wherein the following condition is satisfied:

8. When the focal length of a partial optical system arranged on the image side of the main optical system relative to the position where the variable magnification optical system is inserted is fb and the focal length of the variable magnification optical system is fe, -3.5<fb / fe<-0.30 8. The optical system according to claim 1, wherein the following condition is satisfied:

9. When the refractive index of the negative lens G1N is ndG1N, 1.58<ndG1N<1.89 9. The optical system according to claim 1, wherein the following condition is satisfied:

10. When the Abbe number of the negative lens G1N is νdG1N, 22<νdG1N<55 10. The optical system according to claim 1, wherein the following condition is satisfied:

11. When the shape factor of the negative lens G1N is SFG1N, -1.3<SFG1N<0.50 11. The optical system according to claim 1, wherein the following condition is satisfied:

12. When the refractive index of the positive lens G1P is ndG1P, 1.41<ndG1P<1.69 12. The optical system according to claim 1, wherein the following condition is satisfied:

13. When the Abbe number of the positive lens G1P is νdG1P, 55<νdG1P<95 13. The optical system according to claim 1, wherein the following condition is satisfied:

14. When the refractive index of the positive lens G2P is ndG2P, 1.40<ndG2P<1.67 14. The optical system according to claim 1, wherein the following condition is satisfied:

15. When the Abbe number of the positive lens G2P is νdG2P, 55<νdG2P<99 15. The optical system according to claim 1, wherein the following condition is satisfied:

16. When the focal length of the negative lens G1N is fG1N and the focal length of the main optical system is f, -0.95<fG1N / f<-0.08 16. The optical system according to claim 1, wherein the following condition is satisfied:

17. When the focal length of the positive lens G1P is fG1P and the focal length of the main optical system is f, 0.50<fG1P / f<3.0 17. The optical system according to claim 1, wherein the following condition is satisfied:

18. When the focal length of the positive lens G1P is fG1P and the focal length of the negative lens G1N is fG1N, -9.9<fG1P / fG1N<-1.5 18. The optical system according to claim 1, wherein the following condition is satisfied:

19. When the focal length of the positive lens G1P is fG1P and the focal length of the positive lens G2P is fG2P, 0.90<fG1P / fG2P<3.0 19. The optical system according to claim 1, wherein the following condition is satisfied:

20. 20. The optical system according to claim 1, wherein the variable magnification optical system includes two or more negative lenses and one or more positive lenses.

21. 21. The optical system according to claim 1, wherein the variable magnification optical system is inserted between two lenses included in the main optical system.

22. 22. The optical system according to claim 1, wherein a lens group included in the main optical system that moves during focusing moves in response to insertion or removal of the variable magnification optical system.

23. 23. The optical system according to claim 1, wherein the main optical system includes an image stabilization lens group that is disposed on the image side of the aperture stop and moves in a direction perpendicular to the optical axis.

24. 24. A lens device comprising: an optical system according to claim 1; and a lens barrel that holds the optical system.

25. 25. An imaging device comprising: the optical system according to claim 1; and an imaging element that receives an image formed by the optical system.

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