OPTICAL SYSTEM, OPTICAL APPARATUS AND METHOD FOR MANUFACTURING THE OPTICAL SYSTEM

Information

  • Patent Application
  • 20220291489
  • Publication Number
    20220291489
  • Date Filed
    August 26, 2020
    3 years ago
  • Date Published
    September 15, 2022
    a year ago
Abstract
An optical system (LS) has an aperture stop (S), and a negative lens (L73) disposed closer to the image side than the aperture stop (S) and satisfying the following conditional expressions.
Description
TECHNICAL FIELD

The present invention relates to an optical system, an optical apparatus and a method for manufacturing the optical system.


TECHNICAL BACKGROUND

In recent years, the image resolutions of imaging elements included in imaging apparatuses, such as digital cameras and video cameras, have been improved. It is desired that a photographing lens provided in an imaging apparatus including such an imaging element be a lens of which not only the reference aberrations (aberrations for single-wavelength aberrations), such as the spherical aberration and the coma aberration, be favorably corrected, but also chromatic aberrations be favorably corrected so as not to cause color bleeding for a white light source, and which have a high resolution. In particular, for correction of the chromatic aberrations, it is desirable that not only primary achromatism be achieved but also secondary spectrum be favorably corrected. As means for correcting the chromatic aberrations, for example, a method of using a resin material having anomalous dispersion characteristics (for example, see Patent literature 1) has been known. As described above, accompanied by the recent improvement in imaging element resolution, a photographing lens with various aberrations being favorably corrected has been desired.


PRIOR ARTS LIST
Patent Document



  • Patent literature 1: Japanese Laid-Open Patent Publication No. 2016-194609(A)



SUMMARY OF THE INVENTION

A first optical system according to the present invention comprises: an aperture stop; and a negative lens that is disposed closer to an image than the aperture stop, wherein the negative lens satisfies the following conditional expressions:





−0.010<ndN2−(2.015−0.0068×νdN2),





50.00<νdN2<65.00,





0.545<θgFN2,





−0.010<θgFN2−(0.6418−0.00168×νdN2)


where ndN2: a refractive index of the negative lens for d-line,


νdN2: an Abbe number of the negative lens with reference to d-line,


θgFN2: a partial dispersion ratio of the negative lens, defined by a following expression when a refractive index of the negative lens for g-line is ngN2, a refractive index of the negative lens for F-line is nFN2, and a refractive index of the negative lens for C-line is nCN2:





θgFN2=(ngN2−nFN2)/(nFN2−nCN2).


A second optical system according to the present invention comprises: a plurality of lens groups that include lens groups having negative refractive powers, wherein upon zooming or focusing, a distance between the lens groups adjacent to each other changes, and an image-side negative lens group disposed closest to an image among the lens groups having the negative refractive powers includes a negative lens that satisfies the following conditional expressions:





−0.010<ndN4−(2.015−0.0068×νdN4),





50.00<νdN4<65.00,





0.545<θgFN4,





−0.010<θgFN4−(0.6418−0.00168×νdN4)


where ndN4: a refractive index of the negative lens for d-line,


νdN4: an Abbe number of the negative lens with reference to d-line, and


θgFN4: a partial dispersion ratio of the negative lens, defined by a following expression when a refractive index of the negative lens for g-line is ngN4, a refractive index of the negative lens for F-line is nFN4, and a refractive index of the negative lens for C-line is nCN4:





θgFN4=(ngN4−nFN4)/(nFN4−nCN4).


An optical apparatus according to the present invention comprises the optical system described above.


A first method for manufacturing an optical system according to the present invention arranges each lens in a lens barrel so that the optical system comprises: an aperture stop; and a negative lens that is disposed closer to an image than the aperture stop, the negative lens satisfying the following conditional expressions:





−0.010<ndN2−(2.015−0.0068×νdN2),





50.00<νdN2<65.00,





0.545<θgFN2,





−0.010<θgFN2−(0.6418−0.00168×νdN2)


where ndN2: a refractive index of the negative lens for d-line,


νdN2: an Abbe number of the negative lens with reference to d-line, and


θgFN2: a partial dispersion ratio of the negative lens, defined by a following expression when a refractive index of the negative lens for g-line is ngN2, a refractive index of the negative lens for F-line is nFN2, and a refractive index of the negative lens for C-line is nCN2:





θgFN2=(ngN2−nFN2)/(nFN2−nCN2).


A second method for manufacturing an optical system according to the present invention that includes a plurality of lens groups including lens groups having negative refractive powers, the method arranging each lens in a lens barrel so that upon zooming or focusing, a distance between the lens groups adjacent to each other changes, and an image-side negative lens group disposed closest to an image among the lens groups having the negative refractive powers includes a negative lens that satisfies the following conditional expressions:





−0.010<ndN4−(2.015−0.0068×νdN4),





50.00<νdN4<65.00,





0.545<θgFN4,





−0.010<θgFN4−(0.6418−0.00168×νdN4)


where ndN4: a refractive index of the negative lens for d-line,


νdN4: an Abbe number of the negative lens with reference to d-line, and


θgFN4: a partial dispersion ratio of the negative lens, defined by a following expression when a refractive index of the negative lens for g-line is ngN4, a refractive index of the negative lens for F-line is nFN4, and a refractive index of the negative lens for C-line is nCN4:





θgFN4=(ngN4−nFN4)/(nFN4−nCN4).





BRIEF DESCRIPTION OF THE DRAWINGS


FIG. 1 is a lens configuration diagram of an optical system in a state upon focusing on infinity according to First Example;



FIGS. 2A, 2B and 2C are graphs respectively showing various aberrations of the optical system according to First Example upon focusing on infinity in the wide-angle end state, the intermediate focal length state and the telephoto end state;



FIG. 3 is a lens configuration diagram of an optical system in a state upon focusing on infinity according to Second Example;



FIGS. 4A, 4B and 4C are graphs respectively showing various aberrations of the optical system according to Second Example upon focusing on infinity in the wide-angle end state, the intermediate focal length state and the telephoto end state;



FIG. 5 is a lens configuration diagram of an optical system in a state upon focusing on infinity according to Third Example;



FIGS. 6A, 6B and 6C are graphs respectively showing various aberrations of the optical system according to Third Example upon focusing on infinity in the wide-angle end state, the intermediate focal length state and the telephoto end state;



FIG. 7 is a lens configuration diagram of an optical system in a state upon focusing on infinity according to Fourth Example;



FIGS. 8A, 8B and 8C are graphs respectively showing various aberrations of the optical system according to Fourth Example upon focusing on infinity in the wide-angle end state, the intermediate focal length state and the telephoto end state;



FIG. 9 is a lens configuration diagram of an optical system in a state upon focusing on infinity according to Fifth Example;



FIGS. 10A, 10B, 10C and 10D are graphs respectively showing various aberrations of the optical system according to Fifth Example upon focusing on infinity in the wide-angle end state, a first intermediate focal length state, a second intermediate focal length state and the telephoto end state;



FIG. 11 is a lens configuration diagram of an optical system in a state upon focusing on infinity according to Sixth Example;



FIGS. 12A, 12B and 12C are graphs respectively showing various aberrations of the optical system according to Sixth Example upon focusing on infinity, upon focusing on an intermediate distant object and upon focusing on a short distant object;



FIG. 13 is a lens configuration diagram of an optical system in a state upon focusing on infinity according to Seventh Example;



FIGS. 14A, 14B and 14C are graphs respectively showing various aberrations of the optical system according to Seventh Example upon focusing on infinity in the wide-angle end state, the intermediate focal length state and the telephoto end state;



FIG. 15 shows a configuration of a camera that includes the optical system according to each embodiment;



FIG. 16 is a flowchart showing a method of manufacturing the optical system according to a first embodiment; and



FIG. 17 is a flowchart showing a method of manufacturing the optical system according to a second embodiment.





DESCRIPTION OF THE EMBODIMENTS

Hereinafter, preferable embodiments according to the present invention are described. First, a camera (optical apparatus) that includes an optical system according to each embodiment is described with reference to FIG. 15. As shown in FIG. 15, the camera 1 is a digital camera that includes the optical system according to each embodiment, as a photographing lens 2. In the camera 1, light from an object (photographic subject), not shown, is collected by the photographing lens 2, and reaches an imaging element 3. Accordingly, the light from the photographic subject is captured by the imaging element 3, and is recorded as a photographic subject image in a memory, not shown. As described above, a photographer can take the image of the photographic subject through the camera 1. Note that this camera may be a mirrorless camera, or a single-lens reflex camera that includes a quick return mirror.


Next, the optical system according to a first embodiment is described. As shown in FIG. 1, an optical system LS(1) as an example of an optical system (photographing lens) LS according to the first embodiment comprises: an aperture stop S; and a negative lens (L73) that is disposed closer to an image than the aperture stop S, the negative lens (L73) satisfying following conditional expressions (1) to (4).





−0.010<ndN2−(2.015−0.0068×νdN2),  (1),





50.00<νdN2<65.00  (2),





0.545<θgFN2  (3),





−0.010<θgFN2−(0.6418−0.00168×νdN2)  (4)


where ndN2: a refractive index of the negative lens for d-line,


νdN2: an Abbe number of the negative lens with reference to d-line, and


θgFN2: a partial dispersion ratio of the negative lens, defined by a following expression when a refractive index of the negative lens for g-line is ngN2, a refractive index of the negative lens for F-line is nFN2, and a refractive index of the negative lens for C-line is nCN2:





θgFN2=(ngN2−nFN2)/(nFN2−nCN2).


Note that the Abbe number νdN2 of the negative lens with reference to d-line is defined by the following expression:





νdN2=(ndN2−1)/(nFN2−nCN2).


According to this embodiment, the optical system where for correction of chromatic aberrations, in addition to primary achromatization, the secondary spectrum is favorably corrected, and the optical apparatus that includes this optical system can be achieved. The optical system LS according to the first embodiment may be an optical system LS(2) shown in FIG. 3, an optical system LS(3) shown in FIG. 5, an optical system LS(4) shown in FIG. 7, an optical system LS(5) shown in FIG. 9, an optical system LS(6) shown in FIG. 11, or an optical system LS(7) shown in FIG. 13.


The conditional expression (1) defines an appropriate relationship between the refractive index of the negative lens for d-line and the Abbe number with reference to d-line. By satisfying the conditional expression (1), correction of the reference aberrations, such as the spherical aberration and the coma aberration, and correction of the primary chromatic aberration can be favorably performed.


If the corresponding value of the conditional expression (1) falls outside of the range, the correction of the chromatic aberrations becomes difficult. By setting the lower limit value of the conditional expression (1) to −0.005, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (1) may be set to −0.001, 0.000, 0.003, 0.005 or 0.007, or further to 0.008.


Note that the upper limit value of the conditional expression (1) may be set to less than 0.150. Accordingly, correction of the reference aberrations, such as the spherical aberration and the coma aberration, and correction of the primary chromatic aberration (achromatization) can be favorably performed. In this case, by setting the upper limit value of the conditional expression (1) to 0.100, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (1) may be set to 0.080, 0.060 or 0.050, or further to 0.045.


The conditional expression (2) defines an appropriate range of the Abbe number of the negative lens with reference to d-line. By satisfying the conditional expression (2), correction of the reference aberrations, such as the spherical aberration and the coma aberration, and correction of the primary chromatic aberration (achromatization) can be favorably performed.


If the corresponding value of the conditional expression (2) falls outside of the range, the correction of the chromatic aberrations becomes difficult. By setting the lower limit value of the conditional expression (2) to 50.50, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (2) may be set to 51.00, 51.50 or 52.00, or further to 52.40.


By setting the upper limit value of the conditional expression (2) to 64.00, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (2) may be set to 63.00, 62.50, 62.00, 61.50, 61.00 or 60.00, or further to 59.50.


The conditional expression (3) appropriately defines the anomalous dispersion characteristics of the negative lens. By satisfying the conditional expression (3), for correction of chromatic aberrations, in addition to primary achromatization, the secondary spectrum can be favorably corrected.


If the corresponding value of the conditional expression (3) falls outside of the range, the correction of the chromatic aberrations becomes difficult. By setting the lower limit value of the conditional expression (3) to 0.547, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (3) may be set to 0.548 or 0.549, or further to 0.550.


The conditional expression (4) appropriately defines the anomalous dispersion characteristics of the negative lens. By satisfying the conditional expression (4), for correction of chromatic aberrations, in addition to primary achromatization, the secondary spectrum can be favorably corrected.


If the corresponding value of the conditional expression (4) falls outside of the range, the correction of the chromatic aberrations becomes difficult. By setting the lower limit value of the conditional expression (4) to −0.005, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (4) may be set to −0.001.


Note that the upper limit value of the conditional expression (4) may be set to less than 0.040. Accordingly, correction of the reference aberrations, such as the spherical aberration and the coma aberration, and correction of the primary chromatic aberration (achromatization) can be favorably performed. In this case, by setting the upper limit value of the conditional expression (4) to 0.030, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (4) may be set to 0.025, or further to 0.020.


Preferably, the optical system LS according to the first embodiment consists of: the aperture stop S; a front group GF disposed closer to the object than the aperture stop S; and a rear group GR disposed closer to an image than the aperture stop S, wherein the rear group GR includes the negative lens, and satisfies the following conditional expression (5):





−10.00<(−fN2)/fR<10.00  (5)


where fN2: the focal length of the negative lens, and


fR: a focal length of the rear group GR; in a case where the optical system LS is a zoom optical system, the focal length of the rear group GR in the wide angle end state.


The conditional expression (5) defines an appropriate relationship between the focal length of the negative lens and the focal length of the rear group GR. By satisfying the conditional expression (5), the reference aberrations, such as the spherical aberration and the coma aberration, can be favorably corrected.


If the corresponding value of the conditional expression (5) falls outside of the range, the correction of the reference aberrations, such as the spherical aberration and the coma aberration, becomes difficult. By setting the lower limit value of the conditional expression (5) to −9.50, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (5) may be set to −9.00, −8.50, −8.00, −7.00, −5.00, −3.00, −1.50, −0.05 or 0.05, or further to 0.10.


By setting the upper limit value of the conditional expression (5) to 8.50, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (5) may be set to 7.50, 6.50, 5.00 or 4.00, or further to 3.00.


In the optical system LS according to the first embodiment, preferably, the negative lens satisfies the following conditional expression (6),





0.10<(−fN2)/f<15.00  (6)


where fN2: the focal length of the negative lens, and


f: a focal length of the optical system; the focal length of the optical system LS in the wide angle end state in a case where the optical system LS is a zoom optical system.


The conditional expression (6) defines an appropriate relationship between the focal length of the negative lens and the focal length of the optical system LS. By satisfying the conditional expression (6), the reference aberrations, such as the spherical aberration and the coma aberration, can be favorably corrected.


If the corresponding value of the conditional expression (6) falls outside of the range, the correction of the reference aberrations, such as the spherical aberration and the coma aberration, becomes difficult. By setting the lower limit value of the conditional expression (6) to 0.20, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (6) may be set to 0.30, 0.40 or 0.45, or further to 0.50.


By setting the upper limit value of the conditional expression (6) to 14.20, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (6) may be set to 12.00, 10.00 or 8.50, or further to 7.50.


In the optical system LS according to the first embodiment, the negative lens may satisfy the following conditional expression (3-1),





0.555<θgFN2.  (3-1)


The conditional expression (3-1) is an expression similar to the conditional expression (3), and can exert advantageous effects similar to those of the conditional expression (3). By setting the lower limit value of the conditional expression (3-1) to 0.556, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, it is preferable to set the lower limit value of the conditional expression (3-1) to 0.557.


In the optical system LS according to the first embodiment, the negative lens may satisfy the following conditional expression (4-1),





0.010<θgFN2−(0.6418−0.00168×νdN2).  (4-1)


The conditional expression (4-1) is an expression similar to the conditional expression (4), and can exert advantageous effects similar to those of the conditional expression (4). By setting the lower limit value of the conditional expression (4-1) to 0.011, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, it is preferable to set the lower limit value of the conditional expression (4-1) to 0.012.


Note that the upper limit value of the conditional expression (4-1) may be set to less than 0.030. Accordingly, advantageous effects similar to those of the conditional expression (4) can be achieved. In this case, by setting the upper limit value of the conditional expression (4-1) to 0.028, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (4-1) may be set to 0.025 or 0.023, or further to 0.020.


In the optical system LS according to the first embodiment, preferably, the negative lens satisfies the following conditional expression (7),






DN2>0.400 [mm]  (7)


where DN2: a thickness of the negative lens on an optical axis.


The conditional expression (7) appropriately defines the thickness of the negative lens on the optical axis. By satisfying the conditional expression (7), the various aberrations, such as the coma aberration, the chromatic aberrations (the longitudinal chromatic aberration and the chromatic aberration of magnification), can be favorably corrected.


If the corresponding value of the conditional expression (7) falls outside of the range, the correction of the various aberrations, such as the coma aberration and the chromatic aberrations (the longitudinal chromatic aberration and the chromatic aberration of magnification), becomes difficult. By setting the lower limit value of the conditional expression (7) to 0.450 [mm], the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (7) may be set to 0.490 [mm], 0.550 [mm], 0.580 [mm], 0.650 [mm], 0.680 [mm], 0.750 [mm], 0.800 [mm], 0.850 [mm], 0.880 [mm], 0.950 [mm], 0.980 [mm], 1.050 [mm], 1.100 [mm], 1.140 [mm], 1.250 [mm], or further to 1.350 [mm].


In the optical system LS according to the first embodiment, preferably, the negative lens is a single lens, or one lens of two lenses of a cemented lens consisting of the two lenses cemented to each other. Use of glass as the material of the lens has smaller variation in optical characteristics due to temperature than that of resin. In this embodiment, glass can be used as a material of the negative lens. Accordingly, even in the case where the negative lens has a lens surface in contact with air (i.e., a single lens, or one lens of two lenses of a cemented lens consisting of the two lenses cemented to each other), it is preferable because variation in optical characteristics due to temperature is small.


In the optical system LS according to the first embodiment, it is desirable that at least one lens surface of an object-side lens surface and an image-side lens surface of the negative lens be in contact with air. Use of glass as the material of the lens has smaller variation in optical characteristics due to temperature than that of resin. In this embodiment, glass can be used as a material of the negative lens. Accordingly, even in a case where a lens surface of the negative lens is in contact with air, it is preferable because the variation in optical characteristics due to temperature is small.


In the optical system LS according to the first embodiment, it is desirable that the negative lens be a glass lens. The secular change of the negative lens that is a glass lens is smaller than that of a resin lens. Accordingly, it is preferable because the variation in optical characteristics due to temperature is small.


Subsequently, referring to FIG. 16, a method for manufacturing the optical system LS according to the first embodiment is schematically described. First, an aperture stop S, and a negative lens closer to an image than the aperture stop S are arranged (step ST1). At this time, each lens is arranged in a lens barrel so that at least one of the negative lenses arranged closer to the image than the aperture stop S satisfies the conditional expressions (1) to (4) and the like (step ST2). According to such a manufacturing method, the optical system where for correction of chromatic aberrations, in addition to primary achromatization, the secondary spectrum is favorably corrected can be manufactured.


Next, the optical system according to a second embodiment is described. As shown in FIG. 1, the optical system LS(1) as an example of the optical system (photographing lens) LS according to the second embodiment includes a plurality of lens groups that include lens groups having negative refractive powers. Upon zooming or focusing, a distance between the lens groups adjacent to each other changes. An image-side negative lens group disposed closest to an image among the lens groups having the negative refractive powers includes a negative lens (L73) that satisfies the following conditional expressions (11) to (14).





−0.010<ndN4−(2.015−0.0068×νdN4),  (11)





50.00<νdN4<65.00,  (12)





0.545<θgFN4,  (13)





−0.010<θgFN4−(0.6418−0.00168×νdN4),  (14)


where ndN4: a refractive index of the negative lens for d-line,


νdN4: an Abbe number of the negative lens with reference to d-line, and


θgFN4: a partial dispersion ratio of the negative lens, defined by a following expression when a refractive index of the negative lens for g-line is ngN4, a refractive index of the negative lens for F-line is nFN4, and a refractive index of the negative lens for C-line is nCN4:





θgFN4=(ngN4−nFN4)/(nFN4−nCN4).


Note that the Abbe number νdN4 of the negative lens with reference to d-line is defined by the following expression:





νdN4=(ndN4−1)/(nFN4−nCN4).


According to this embodiment, the optical system where for correction of chromatic aberrations, in addition to primary achromatization, the secondary spectrum is favorably corrected, and the optical apparatus that includes this optical system can be achieved. The optical system LS according to the second embodiment may be an optical system LS(2) shown in FIG. 3, an optical system LS(3) shown in FIG. 5, an optical system LS(4) shown in FIG. 7, an optical system LS(5) shown in FIG. 9, an optical system LS(6) shown in FIG. 11, or an optical system LS(7) shown in FIG. 13.


The conditional expression (11) defines an appropriate relationship between the refractive index of the negative lens for d-line and the Abbe number with reference to d-line. By satisfying the conditional expression (11), correction of the reference aberrations, such as the spherical aberration and the coma aberration, and correction of the primary chromatic aberration (achromatization) can be favorably performed.


If the corresponding value of the conditional expression (11) falls outside of the range, the correction of the chromatic aberrations becomes difficult. By setting the lower limit value of the conditional expression (11) to −0.005, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (11) may be set to −0.001, 0.000, 0.003, 0.005 or 0.007, or further to 0.008.


Note that the upper limit value of the conditional expression (11) may be set to less than 0.150. Accordingly, correction of the reference aberrations, such as the spherical aberration and the coma aberration, and correction of the primary chromatic aberration (achromatization) can be favorably performed. In this case, by setting the upper limit value of the conditional expression (11) to 0.100, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (11) may be set to 0.080, 0.060 or 0.050, or further to 0.045.


The conditional expression (12) defines an appropriate range of the Abbe number of the negative lens with reference to d-line. By satisfying the conditional expression (12), correction of the reference aberrations, such as the spherical aberration and the coma aberration, and correction of the primary chromatic aberration (achromatization) can be favorably performed.


If the corresponding value of the conditional expression (12) falls outside of the range, the correction of the chromatic aberrations becomes difficult. By setting the lower limit value of the conditional expression (12) to 50.50, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (12) may be set to 51.00, 51.50 or 52.00, or further to 52.40.


By setting the upper limit value of the conditional expression (12) to 64.00, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (12) may be set to 63.00, 62.50, 62.00, 61.50, 61.00 or 60.00, or further to 59.50.


The conditional expression (13) appropriately defines the anomalous dispersion characteristics of the negative lens. By satisfying the conditional expression (13), for correction of chromatic aberrations, in addition to primary achromatization, the secondary spectrum can be favorably corrected.


If the corresponding value of the conditional expression (13) falls outside of the range, the correction of the chromatic aberrations becomes difficult. By setting the lower limit value of the conditional expression (13) to 0.547, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (13) may be set to 0.548 or 0.549, or further to 0.550.


The conditional expression (14) appropriately defines the anomalous dispersion characteristics of the negative lens. By satisfying the conditional expression (14), for correction of chromatic aberrations, in addition to primary achromatization, the secondary spectrum can be favorably corrected.


If the corresponding value of the conditional expression (14) falls outside of the range, the correction of the chromatic aberrations becomes difficult. By setting the lower limit value of the conditional expression (14) to −0.005, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (14) may be set to −0.001.


Note that the upper limit value of the conditional expression (14) may be set to less than 0.040. Accordingly, correction of the reference aberrations, such as the spherical aberration and the coma aberration, and correction of the primary chromatic aberration (achromatization) can be favorably performed. In this case, by setting the upper limit value of the conditional expression (14) to 0.030, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (14) may be set to 0.025, or further to 0.020.


In the optical system LS according to the second embodiment, preferably, the negative lens satisfies the following conditional expression (15):





0.02<fN4/fGb<3.00  (15)


where fN4: the focal length of the negative lens, and


fGb: a focal length of the image-side negative lens group.


The conditional expression (15) defines an appropriate relationship between the focal length of the negative lens and the focal length of the image-side negative lens group. By satisfying the conditional expression (15), the reference aberrations, such as the spherical aberration and the coma aberration, can be favorably corrected.


If the corresponding value of the conditional expression (15) falls outside of the range, the correction of the reference aberrations, such as the spherical aberration and the coma aberration, becomes difficult. By setting the lower limit value of the conditional expression (15) to 0.03, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (15) may be set to 0.04, 0.10, 0.15, 0.20, 0.25, 0.30, 0.35 or 0.40, or further to 0.42.


By setting the upper limit value of the conditional expression (15) to 2.80, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (15) may be set to 2.50, 2.30, 2.20, 2.00, 1.75 or 1.50, or further to 1.30.


In the optical system LS according to the second embodiment, preferably, the image-side negative lens group satisfies the following conditional expression (16):





0.50<(−fGb)/f<100.00  (16)


where fGb: a focal length of the image-side negative lens group, and


f: a focal length of the optical system; in a case where the optical system LS is a zoom optical system, the focal length of the optical system LS in the wide angle end state.


The conditional expression (16) defines an appropriate relationship between the focal length of the image-side negative lens group and the focal length of the optical system LS. By satisfying the conditional expression (16), the reference aberrations, such as the spherical aberration and the coma aberration, can be favorably corrected.


If the corresponding value of the conditional expression (16) falls outside of the range, the correction of the reference aberrations, such as the spherical aberration and the coma aberration, becomes difficult. By setting the lower limit value of the conditional expression (16) to 0.60, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (16) may be set to 0.70, 0.80 or 0.90, or further to 0.95.


By setting the upper limit value of the conditional expression (16) to 85.00, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (16) may be set to 70.00, 50.00, 35.00, 20.00, 10.00, 5.00, 3.50 or 2.80, or further to 2.20.


In the optical system LS according to the second embodiment, the negative lens may satisfy the following conditional expression (13-1),





0.555<θgFN4.  (13-1)


The conditional expression (13-1) is an expression similar to the conditional expression (13), and can exert advantageous effects similar to those of the conditional expression (13). By setting the lower limit value of the conditional expression (13-1) to 0.556, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, it is preferable to set the lower limit value of the conditional expression (13-1) to 0.557.


In the optical system LS according to the second embodiment, the negative lens may satisfy the following conditional expression (14-1),





0.010<θgFN4−(0.6418−0.00168×νdN4).  (14-1)


The conditional expression (14-1) is an expression similar to the conditional expression (14), and can exert advantageous effects similar to those of the conditional expression (14). By setting the lower limit value of the conditional expression (14-1) to 0.011, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, it is preferable to set the lower limit value of the conditional expression (14-1) to 0.012.


Note that the upper limit value of the conditional expression (14-1) may be set to less than 0.030. Accordingly, advantageous effects similar to those of the conditional expression (14) can be achieved. In this case, by setting the upper limit value of the conditional expression (14-1) to 0.028, the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the upper limit value of the conditional expression (14-1) may be set to 0.025 or 0.023, or further to 0.020.


In the optical system LS according to the second embodiment, preferably, the negative lens satisfies the following conditional expression (17),






DN4>0.400 [mm]  (17)


where DN4: a thickness of the negative lens on an optical axis.


The conditional expression (17) appropriately defines the thickness of the negative lens on the optical axis. By satisfying the conditional expression (17), the various aberrations, such as the coma aberration, the chromatic aberrations (the longitudinal chromatic aberration and the chromatic aberration of magnification), can be favorably corrected.


If the corresponding value of the conditional expression (17) falls outside of the range, the correction of the various aberrations, such as the coma aberration and the chromatic aberrations (the longitudinal chromatic aberration and the chromatic aberration of magnification), becomes difficult. By setting the lower limit value of the conditional expression (17) to 0.450 [mm], the advantageous effects of this embodiment can be further secured. To further secure the advantageous effects of this embodiment, the lower limit value of the conditional expression (17) may be set to 0.490 [mm], 0.550 [mm], 0.580 [mm], 0.650 [mm], 0.680 [mm], 0.750 [mm], 0.800 [mm], 0.850 [mm], 0.880 [mm], 0.950 [mm], 0.980 [mm], 1.050 [mm], 1.100 [mm], 1.140 [mm] or 1.250 [mm], or further to 1.350 [mm].


In the optical system LS according to the second embodiment, preferably, the negative lens is a single lens, or one lens of two lenses of a cemented lens consisting of the two lenses cemented to each other. Use of glass as the material of the lens has smaller variation in optical characteristics due to temperature than that of resin. In this embodiment, glass can be used as a material of the negative lens. Accordingly, even in the case where the negative lens has a lens surface in contact with air (i.e., a single lens, or one lens of two lenses of a cemented lens consisting of the two lenses cemented to each other), it is preferable because variation in optical characteristics due to temperature is small.


In the optical system LS according to the second embodiment, at least one lens surface of an object-side lens surface and an image-side lens surface of the negative lens is in contact with air. Use of glass as the material of the lens has smaller variation in optical characteristics due to temperature than that of resin. In this embodiment, glass can be used as a material of the negative lens. Accordingly, even in a case where a lens surface of the negative lens is in contact with air, it is preferable because the variation in optical characteristics due to temperature is small.


In the optical system LS according to the second embodiment, it is desirable that the negative lens be a glass lens. The secular change of the negative lens that is a glass lens is smaller than that of a resin lens. Accordingly, it is preferable because the variation in optical characteristics due to temperature is small.


Subsequently, referring to FIG. 17, a method for manufacturing the optical system LS according to the second embodiment is schematically described. First, a plurality of lens groups including lens groups having negative refractive powers are arranged (step ST11). The configuration is made so that the distance between lens groups adjacent to each other changes upon zooming or focusing (step ST12). Each lens is arranged in the lens barrel so that the image-side negative lens group disposed closest to the image among the lens groups having negative refractive powers includes the negative lens satisfying the conditional expressions (11) to (14) and the like (step ST13). According to such a manufacturing method, the optical system where for correction of chromatic aberrations, in addition to primary achromatization, the secondary spectrum is favorably corrected can be manufactured.


EXAMPLES

Optical systems LS according to Examples of each embodiment are described with reference to the drawings. FIGS. 1, 3, 5, 7, 9, 11 and 13 are sectional views showing the configurations and refractive power allocations of optical systems LS {LS(1) to LS(7)} according to First to Seventh Examples. In the sectional views of the optical systems LS(1) to LS(7) according to First to Seventh Examples, the moving direction upon focusing by each focusing lens group from the infinity to a short-distance object is indicated by an arrow accompanied by characters “FOCUSING”. In the sectional views of the optical systems LS(1) to LS(5) according to First to Fifth Examples and the optical system LS(7) according to Seventh Example, the moving direction of each lens group along the optical axis upon zooming from the wide angle end state (W) to the telephoto end state (T) is indicated by an arrow.


In FIGS. 1, 3, 5, 7, 9, 11 and 13, each lens group is represented by a combination of a symbol G and a numeral, and each lens is represented by a combination of a symbol L and a numeral. In this case, to prevent complication due to increase in the types and numbers of symbols and numerals, the lens groups and the like are represented using the combinations of symbols and numerals independently on an Example-by-Example basis. Accordingly, even when the same combination of a symbol and a numeral is used among Examples, such usage does not mean the same configuration.


Tables 1 to 7 are shown below. Among the drawings, Table 1 is a table showing each data item in First Example, Table 2 is that in Second Example, Table 3 is that in Third Example, Table 4 is that in Fourth Example, Table 5 is that in Fifth Example, Table 6 is that in Sixth Example, and Table 7 is that in Seventh Example. In each Example, as targets of calculation of aberration characteristics, d-line (wavelength λ=587.6 nm), g-line (wavelength λ=435.8 nm), C-line (wavelength λ=656.3 nm), and F-line (wavelength λ=486.1 nm) are selected.


In the table of [General Data], f indicates the focal length of the entire lens system, FNO indicates the f-number, 2ω indicates the angle of view (the unit is ° (degrees), and co is the half angle of view), and Y indicates the image height. TL indicates a distance obtained by adding BF to the distance from the lens foremost surface to the lens last surface on the optical axis upon focusing on infinity. BF indicates the distance (back focus) from the lens last surface to the image surface I on the optical axis upon focusing on infinity. fF indicates the focal length of the front group, and fR indicates the focal length of the rear group. Note that in a case where the optical system is a zoom optical system, these values are indicated for each of zoom states at the wide-angle end (W), the intermediate focal length (M) and the telephoto end (T).


In the table of [Lens Data], Surface Number indicates the order of the optical surface from the object side along the direction in which the ray travels, R indicates the radius of curvature (the surface whose center of curvature resides on the image side is regarded to have a positive value) of each optical surface, D indicates the surface distance which is the distance to the next lens surface (or the image surface) from each optical surface on the optical axis, nd is the refractive index of the material of the optical member for d-line, νd indicates the Abbe number of the material of the optical member with respect to d-line, and θgF indicates the partial dispersion ratio of the material of the optical member. The radius of curvature “∞” indicates a plane or an opening. (Aperture Stop S) indicates an aperture stop S. The description of the air refractive index nd=1.00000 is omitted. In a case where the optical surface is an aspherical surface, the surface number is assigned * symbol, and the field of the radius of curvature R indicates the paraxial radius of curvature.


The refractive index of the optical member for g-line (wavelength λ=435.8 nm) is indicated by ng. The refractive index of the optical member for F-line (wavelength λ=486.1 nm) is indicated by nF. The refractive index of the optical member for C-line (wavelength λ=656.3 nm) is indicated by nC. Here, the partial dispersion ratio θgF of the material of the optical member is defined by the following expression (A).





θgF=(ng−nF)/(nF−nC).  (A)


In the table of [Aspherical Surface Data], the shape of the aspherical surface indicated in [Lens Data] is indicated by the following expression (B). X(y) indicates the distance (sag amount) from the tangent plane at the vertex of the aspherical surface to the position on the aspherical surface at the height y along the optical axis direction. R indicates the radius of curvature (paraxial radius of curvature) of the reference spherical surface. κ indicates the conic constant. Ai indicates the i-th aspherical coefficient. “E−n” indicates “×10−n”. For example, 1.234E−05=1.234×10−5. Note that the second-order aspherical coefficient A2 is zero, and the description thereof is omitted.






X(y)=(y2/R)/{1+(1−κ×y2/R2)1/2}+Ay4+Ay6+Ay8+A10×y10+A12×y12.  (B)


In a case where the optical system is not a zoom optical system, f indicates the focal length of the entire lens system, and β indicates the photographing magnification, as [Variable Distance Data on Short-Distance Photographing]. The table of [Variable Distance Data on Short-Distance Photographing] indicates the surface distance at the surface number where the surface distance is “Variable” in [Lens Data] corresponding to each focal length and photographing magnification.


In the case where the optical system is the zoom optical system, the surface distance at the surface number where the surface distance is “Variable” in [Lens Data] corresponding to each of zooming states at the wide angle end (W), the intermediate focal length (M) and the telephoto end (T) are indicated as [Variable Distance Data on Zoom Photographing].


The table of [Lens Group Data] shows the first surface (the surface closest to the object) and the focal length of each lens group.


The table of [Conditional Expression Corresponding Value] shows the value corresponding to each conditional expression.


Hereinafter, at all the data values, the listed focal length f, the radius of curvature R, the surface distance D, other lengths and the like are represented with “mm” if not otherwise specified. However, even after subjected to proportional scaling in or out, the optical system can achieve equivalent optical performance. Accordingly, the representation is not limited thereto.


The descriptions of the tables so far are common to all the Examples. Redundant descriptions are hereinafter omitted.


First Example

First Example is described with reference to FIGS. 1 and 2A, 2B and 2C and Table 1. FIG. 1 is a diagram showing a lens configuration of an optical system in a state upon focusing on infinity according to First Example of each embodiment. The optical system LS(1) according to First Example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a positive refractive power; a fifth lens group G5 having a positive refractive power; a sixth lens group G6 having a positive refractive power; and a seventh lens group G7 having a negative refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the first to seventh lens groups G1 to G7 move in directions indicated by arrows in FIG. 1. The aperture stop S is disposed between the second lens group G2 and the third lens group G3. A sign (+) or (−) assigned to each lens group symbol indicates the refractive power of each lens group. This indication similarly applies to all the following Examples.


The first lens group G1 consists of, in order from the object: a cemented lens consisting of a negative meniscus lens L11 having a convex surface facing the object, and a positive meniscus lens L12 having a convex surface facing the object; and a positive meniscus lens L13 having a convex surface facing the object.


The second lens group G2 consists of, in order from the object: a negative meniscus lens L21 having a convex surface facing the object; a biconcave negative lens L22; a biconvex positive lens L23; and a negative meniscus lens L24 having a concave surface facing the object. The negative meniscus lens L21 has an object-side lens surface that is an aspherical surface.


The third lens group G3 consists of, in order from the object: a positive meniscus lens L31 having a convex surface facing the object; and a biconvex positive lens L32. The aperture stop S is disposed adjacent to the object side of the positive meniscus lens L31, and moves with the third lens group G3 upon zooming. The positive meniscus lens L31 has an object-side lens surface that is an aspherical surface.


The fourth lens group G4 consists of, in order from the object, a cemented lens consisting of a negative meniscus lens L41 having a convex surface facing the object, and a biconvex positive lens L42.


The fifth lens group G5 consists of, in order from the object: a negative meniscus lens L51 having a concave surface facing the object; and a biconvex positive lens L52. Upon focusing from the infinity object to the short-distant (finite distant) object, the fifth lens group G5 and the sixth lens group G6 move toward the object along the optical axis by different amounts of movement.


The sixth lens group G6 consists of a positive meniscus lens L61 having a concave surface facing the object. The positive meniscus lens L61 has an image-side lens surface that is an aspherical surface.


The seventh lens group G7 consists of, in order from the object: a positive meniscus lens L71 having a concave surface facing the object; a biconcave negative lens L72; and a negative meniscus lens L73 having a concave surface facing the object. An image surface I is disposed on the image side of the seventh lens group G7. In this Example, the negative meniscus lens L73 of the seventh lens group G7 corresponds to a negative lens that satisfies the conditional expressions (1) to (4) and the like. In this Example, the seventh lens group G7 corresponds to an image-side negative lens group, and the negative meniscus lens L73 of the seventh lens group G7 corresponds to a negative lens that satisfies the conditional expressions (11) to (14) and the like. The negative lens L72 has an object-side lens surface that is an aspherical surface.


In this Example, the cemented lens consisting of the negative meniscus lens L11 and the positive meniscus lens L12, the positive meniscus lens L13, the negative meniscus lens L21, the negative lens L22, the positive lens L23, and the negative meniscus lens L24 constitute the front group GF disposed closer to the object than the aperture stop S. The positive meniscus lens L31, the positive lens L32, the cemented lens consisting of the negative meniscus lens L41 and the biconvex positive lens L42, the negative meniscus lens L51, the biconvex positive lens L52, the positive meniscus lens L61, the positive meniscus lens L71, the negative lens L72, and the negative meniscus lens L73 constitute the rear group GR disposed closer to the image than the aperture stop S.


The following Table 1 lists values of data on the optical system according to First Example.









TABLE 1







[General Data]


Zooming ratio = 2.743













W
M
T







f
24.750
35.000
67.880



FNO
2.918
2.919
2.919




85.363
62.867
33.986



Y
21.600
21.600
21.600



TL
139.342
144.390
169.148



BF
11.701
15.449
28.388



fF
−30.791
−34.682
−46.133



fR
28.627
28.934
30.359











[Lens Data]












Surface







Number
R
D
nd
νd
θgF





 1
234.38730
2.500
1.84666
23.80
0.6215


 2
109.51800
5.200
1.75500
52.34
0.5476


 3
389.68520
0.200


 4
59.06270
5.700
1.77250
49.62
0.5518


 5
135.36490
 D5(Variable)


 6*
218.44200
2.000
1.74389
49.53
0.5533


 7
18.69570
9.658


 8
−59.68560
1.300
1.77250
49.62
0.5518


 9
59.68560
0.442


10
39.20990
6.400
1.72825
28.38
0.6069


11
−48.67310
1.933


12
−26.40650
1.300
1.61800
63.34
0.5411


13
−71.76120
D13(Variable)


14

1.712

(Aperture






Stop S)


 15*
71.88760
2.500
1.69370
53.32
0.5475


16
127.64110
0.716


17
38.74920
5.900
1.59319
67.90
0.5440


18
−105.42740
D18(Variable)


19
67.02760
1.300
1.73800
32.33
0.5900


20
19.51260
9.700
1.49782
82.57
0.5386


21
−50.56090
D21(Variable)


22
−23.92370
1.200
1.72047
34.71
0.5834


23
−56.20810
0.200


24
103.17490
5.900
1.59349
67.00
0.5358


25
−33.01970
D25(Variable)


26
−70.62880
3.500
1.79189
45.04
0.5596


 27*
−38.21530
D27(Variable)


28
−44.77940
3.000
1.94595
17.98
0.6544


29
−32.36650
0.200


 30*
−90.76890
1.500
1.85207
40.15
0.5685


31
89.91740
7.847


32
−24.20670
1.400
1.65240
55.27
0.5607


33
−38.83480
BF










[Aspherical Surface Data]












6th Surface



κ = 1.000, A4 = 5.28E−06, A6 = −5.42E−09



A8 = 1.33E−11, A10 = −2.05E−14, A12 = 2.05E−17



15th Surface



κ = 1.000, A4 = −4.56E−06, A6 = −1.40E−10



A8 = −8.81E−13, A10 = −8.43E−15, A12 = 0.00E+00



27th Surface



κ = 1.000, A4 = 1.10E−05, A6 = −2.36E−08



A8 = 1.43E−10, A10 = −5.03E−13, A12 = 7.52E−16



30th Surface



κ = 1.000, A4 = −2.11E−06, A6 = −2.12E−08



A8 = 3.23E−11, A10 = −8.72E−14, A12 = 0.00E+00











[Variable Distance Data on Zoom Photographing]













W
M
T







D5
1.780
11.383
30.246



D13
19.285
9.934
2.013



D18
9.167
6.537
1.493



D21
5.179
7.338
19.018



D25
2.679
3.818
2.616



D27
6.344
6.725
2.168











[Lens Group Data]











Group
First surface
Focal length







G1
1
119.124



G2
6
−22.126



G3
15
40.880



G4
19
115.687



G5
22
124.717



G6
26
100.365



G7
28
−47.354











[Conditional Expression Corresponding Value]












<Negative meniscus lens L73(fN2 = −102.373)>



Conditional Expression (1)



ndN2 − (2.015 − 0.0068 × νdN2) = 0.013



Conditional Expression (2)νdN2 = 55.27



Conditional Expression (3), (3-1)θgFN2 = 0.5607



Conditional Expression (4), (4-1)



θgFN2 − (0.6418 − 0.00168 × νdN2) = 0.0118



Conditional Expression (5)(−fN2)/fR = 3.576



Conditional Expression (7)(−fN2)/f = 4.136



Conditional Expression (8)DN2 = 1.400



<Negative meniscus lens L73(fN4 = −102.373)>



Conditional Expression (11)



ndN4 − (2.015 − 0.0068 × νdN4) = 0.013



Conditional Expression (12)νdN4 = 55.27



Conditional Expression (13), (13-1)θgFN4 = 0.5607



Conditional Expression (14), (14-1)



θgFN4 − (0.6418 − 0.00168 × νdN4) = 0.0118



Conditional Expression (15)fN4/fGb = 2.162



Conditional Expression (16)(−fGb)/f = 1.913



Conditional Expression (17)DN4 = 1.400











FIG. 2A shows various aberration graphs of the optical system according to First Example upon focusing on infinity in the wide angle end state. FIG. 2B shows various aberration graphs of the optical system according to First Example upon focusing on infinity in the intermediate focal length state. FIG. 2C shows various aberration graphs of the optical system according to First Example upon focusing on infinity in the telephoto end state. In each graph upon focusing on infinity, FNO indicates the f-number, and Y indicates the image height. In each aberration graph upon focusing on the intermediate distant object or focusing on the short distant object, NA indicates the numerical aperture, and Y indicates the image height. The spherical aberration graph indicates the value of the f-number or the numerical aperture that corresponds to the maximum diameter. The astigmatism graph and the distortion graph each indicate the maximum value of the image height. The coma aberration graph indicates the value of the corresponding image height. d indicates d-line (wavelength λ=587.6 nm), g indicates g-line (wavelength λ=435.8 nm), C indicates C-line (wavelength λ=656.3 nm), and F indicates F-line (wavelength λ=486.1 nm). In the astigmatism graph, a solid line indicates a sagittal image surface, and a broken line indicates a meridional image surface. Note that also in the following aberration graphs in each Example, symbols similar to those in this Example are used. Redundant description is omitted.


The various aberration graphs show that the optical system according to First Example has favorably corrected various aberrations, and exerts excellent imaging performance.


Second Example

Second Example is described with reference to FIGS. 3 and 4A, 4B and 4C and Table 2. FIG. 3 is a diagram showing a lens configuration of an optical system in a state upon focusing on infinity according to Second Example of each embodiment. The optical system LS(2) according to Second Example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the first to fifth lens groups G1 to G5 move in directions indicated by arrows in FIG. 3. The aperture stop S is disposed in the third lens group G3.


The first lens group G1 consists of, in order from the object: a cemented lens consisting of a negative meniscus lens L11 having a convex surface facing the object, and a biconvex positive lens L12; and a positive meniscus lens L13 having a convex surface facing the object.


The second lens group G2 consists of, in order from the object: a negative meniscus lens L21 having a convex surface facing the object; biconcave negative lens L22; a biconvex positive lens L23; and a negative meniscus lens L24 having a concave surface facing the object. Upon focusing from the infinity object to the short-distant (finite distant) object, the second lens group G2 moves toward the object along the optical axis. The negative meniscus lens L21 has an object-side lens surface that is an aspherical surface. The negative meniscus lens L24 has an image-side lens surface that is an aspherical surface.


The third lens group G3 consists of, in order from the object: a biconvex positive lens L31; a cemented lens consisting of a negative meniscus lens L32 having a convex surface facing the object, and a biconvex positive lens L33; and a biconvex positive lens L34. An aperture stop S is disposed between the positive lens L31 and the negative meniscus lens L32 (of the cemented lens) of the third lens group G3.


The fourth lens group G4 consists of, in order from the object: a cemented lens consisting of a positive meniscus lens L41 having a concave surface facing the object, and a negative meniscus lens L42 having a concave surface facing the object; and a biconcave negative lens L43. In this Example, the negative lens L43 of the fourth lens group G4 corresponds to a negative lens that satisfies the conditional expressions (1) to (4) and the like. In this Example, the fourth lens group G4 corresponds to an image-side negative lens group, and the negative lens L43 of the fourth lens group G4 corresponds to a negative lens that satisfies the conditional expressions (11) to (14) and the like.


The fifth lens group G5 consists of, in order from the object: a biconvex positive lens L51; and a cemented lens consisting of a biconvex positive lens L52, and a biconcave negative lens L53. An image surface I is disposed on the image side of the fifth lens group G5. The positive lens L51 has an object-side lens surface that is an aspherical surface.


In this Example, the cemented lens consisting of the negative meniscus lens L11 and the positive lens L12, the positive meniscus lens L13, the negative meniscus lens L21, the negative lens L22, the positive lens L23, the negative meniscus lens L24, and the positive lens L31 constitute the front group GF disposed closer to the object than the aperture stop S. The cemented lens consisting of the negative meniscus lens L32 and the positive lens L33, the positive lens L34, the cemented lens consisting of the positive meniscus lens L41 and the negative meniscus lens L42, the negative lens L43, the positive lens L51, and the cemented lens consisting of the positive lens L52 and the negative lens L53 constitute the rear group GR disposed closer to the image than the aperture stop S.


The following Table 2 lists values of data on the optical system according to Second Example.









TABLE 2







[General Data]


Zooming ratio = 4.708













W
M
T







f
24.720
49.985
116.383



FNO
4.070
4.067
4.075




86.259
43.985
19.680



Y
21.600
21.600
21.600



TL
147.198
161.190
192.200



BF
32.884
42.859
55.059



fF
110.031
−646.229
−317.953



fR
67.056
67.484
65.974











[Lens Data]












Surface







Number
R
D
nd
νd
θgF





 1
200.00000
1.200
1.84944
22.29
0.6222


 2
112.14330
7.349
1.49782
82.57
0.5138


 3
−312.82020
0.100


 4
58.25030
5.717
1.59159
54.50
0.5508


 5
133.86910
 D5(Variable)


 6*
68.14700
1.050
1.95375
32.33
0.5916


 7
17.41650
6.493


 8
−50.35820
1.200
1.66903
45.08
0.5674


 9
35.82750
0.100


10
36.58470
6.379
1.84706
22.34
0.6220


11
−41.51350
0.788


12
−27.90490
1.200
1.61571
50.69
0.5574


 13*
−1318.72980
D13(Variable)


14
42.13090
3.781
1.62079
50.23
0.5583


15
−94.85060
0.100


16

0.100

(Aperture






Stop S)


17
39.33600
1.200
1.93546
24.49
0.6135


18
18.65160
5.400
1.49996
81.44
0.5151


19
−167.55480
0.100


20
47.06670
2.967
1.59687
53.64
0.5523


21
−353.88140
D21(Variable)


22
−35.39840
3.883
1.92286
20.88
0.6286


23
−18.10590
1.200
1.68303
40.83
0.5750


24
−151.76460
2.275


25
−61.36760
1.200
1.67769
52.63
0.5546


26
323.52730
D26(Variable)


 27*
128.28980
5.951
1.50114
80.83
0.5161


28
−24.91200
0.100


29
72.70400
7.368
1.69764
43.43
0.5703


30
−24.43980
4.083
1.89451
29.27
0.5989


31
82.68200
BF










[Aspherical Surface Data]












6th Surface



κ = 1.000, A4 = −3.63E−06, A6 = −9.23E−09



A8 = 2.66E−11, A10 = −7.08E−14, A12 = 0.00E+00



13th Surface



κ = 1.000, A4 = −1.30E−05, A6 = −9.67E−09



A8 = −4.06E−11, A10 = 0.00E+00, A12 = 0.00E+00



27th Surface



κ = 1.000, A4 = −1.50E−05, A6 = 9.99E−09



A8 = −2.45E−11, A10 = 3.21E−14, A12 = 0.00E+00











[Variable Distance Data on Zoom Photographing]













W
M
T







D5
1.500
19.687
47.442



D13
24.608
10.433
1.500



D21
2.869
10.044
14.916



D26
14.054
6.884
2.000











[Lens Group Data]











Group
First surface
Focal length







G1
1
116.400



G2
6
−18.800



G3
14
27.200



G4
22
−46.400



G5
27
55.800











[Conditional Expression Corresponding Value]












<Negative lens L43(fN2 = −76.021)>



Conditional Expression (1)



ndN2 − (2.015 − 0.0068 × νdN2) = 0.021



Conditional Expression (2)νdN2 = 52.63



Conditional Expression (3), (3-1)θgFN2 = 0.5546



Conditional Expression (4), (4-1)



θgFN2 − (0.6418 − 0.00168 × νdN2) = 0.0012



Conditional Expression (6)(−fN2)/fR = 1.134



Conditional Expression (7)(−fN2)/f = 3.075



Conditional Expression (8)DN2 = 1.200



<Negative lens L43(fN4 = −76.021)>



Conditional Expression (11)



ndN4 − (2.015 − 0.0068 × νdN4) = 0.021



Conditional Expression (12)νdN4 = 52.63



Conditional Expression (13), (13-1)θgFN4 = 0.5546



Conditional Expression (14), (14-1)



θgFN4 − (0.6418 − 0.00168 × νdN4) = 0.0012



Conditional Expression (15)fN4/fGb = 1.638



Conditional Expression (16)(−fGb)/f = 1.877



Conditional Expression (17)DN4 = 1.200











FIG. 4A shows various aberration graphs of the optical system according to Second Example upon focusing on infinity in the wide angle end state. FIG. 4B shows various aberration graphs of the optical system according to Second Example upon focusing on infinity in the intermediate focal length state. FIG. 4C shows various aberration graphs of the optical system according to Second Example upon focusing on infinity in the telephoto end state. The various aberration graphs show that the optical system according to Second Example has favorably corrected various aberrations, and exerts excellent imaging performance.


Third Example

Third Example is described with reference to FIGS. 5 and 6A, 6B and 6C and Table 3. FIG. 5 is a diagram showing a lens configuration of an optical system in a state upon focusing on infinity according to Third Example of each embodiment. The optical system LS(3) according to Third Example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a positive refractive power; and a fifth lens group G5 having a negative refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the second lens group G2 and the fourth lens group G4 move in directions indicated by arrows in FIG. 5. The aperture stop S is disposed in the fifth lens group G5.


The first lens group G1 consists of, in order from the object: a cemented lens consisting of a negative meniscus lens L11 having a convex surface facing the object, and a biconvex positive lens L12; and a plano-convex positive lens L13 having a convex surface facing the object.


The second lens group G2 consists of, in order from the object: a positive meniscus lens L21 having a convex surface facing the object; a cemented lens consisting of biconvex positive lens L22, and a biconcave negative lens L23; a cemented lens consisting of a biconcave negative lens L24, and a positive meniscus lens L25 having a convex surface facing the object; and a negative meniscus lens L26 having a concave surface facing the object.


The third lens group G3 consists of, in order from the object: a biconvex positive lens L31; a biconvex positive lens L32; a biconcave negative lens L33; and a biconvex positive lens L34.


The fourth lens group G4 consists of, in order from the object: a plano-convex positive lens L41 having a convex surface facing the image; and a cemented lens consisting of the biconvex positive lens L42, and a biconcave negative lens L43. Upon focusing from the infinity object to the short-distant (finite distant) object, the fourth lens group G4 moves toward the object along the optical axis.


The fifth lens group G5 consists of, in order from the object: a biconcave negative lens L51; a biconvex positive lens L52; a negative meniscus lens L53 having a convex surface facing the object; a cemented lens consisting of a positive meniscus lens L54 having a concave surface facing the object, and a biconcave negative lens L55; a biconvex positive lens L56; a cemented lens consisting of a negative meniscus lens L57 having a convex surface facing the object, and a biconvex positive lens L58; and a biconcave negative lens L59. An image surface I is disposed on the image side of the fifth lens group G5. An aperture stop S is disposed between the negative lens L51 and the positive lens L52 of the fifth lens group G5. In this Example, the negative lens L55 of the fifth lens group G5 corresponds to a negative lens that satisfies the conditional expressions (1) to (4) and the like. In this Example, the fifth lens group G5 corresponds to an image-side negative lens group, and the negative lens L55 of the fifth lens group G5 corresponds to a negative lens that satisfies the conditional expressions (11) to (14) and the like. Note that a fixed aperture stop (flare cut stop) Sa is disposed between the negative lens L55 (of the cemented lens) and the positive lens L56.


In this Example, the cemented lens consisting of the negative meniscus lens L11 and the positive lens L12, the positive lens L13, the positive meniscus lens L21, the cemented lens consisting of the positive lens L22 and the negative lens L23, the cemented lens consisting of the negative lens L24 and the positive meniscus lens L25, the negative meniscus lens L26, the positive lens L31, the positive lens L32, the negative lens L33, the positive lens L34, the positive lens L41, the cemented lens consisting of the positive lens L42 and the negative lens L43, and the negative lens L51 constitute the front group GF disposed closer to the object than the aperture stop S. The positive lens L52, the negative meniscus lens L53, the cemented lens consisting of the positive meniscus lens L54 and the negative lens L55, the positive lens L56, the cemented lens consisting of the negative meniscus lens L57 and the positive lens L58, and the negative lens L59 constitute the rear group GR disposed closer to the image than the aperture stop S.


The following Table 3 lists values of data on the optical system according to Third Example.









TABLE 3







[General Data]


Zooming ratio = 2.354













W
M
T







f
123.600
200.000
291.000



FNO
2.910
2.910
2.911




19.564
12.076
8.292



Y
21.630
21.630
21.630



TL
341.394
341.394
341.394



BF
54.819
54.819
54.819



fF
1986.248
3213.999
4676.377



fR
102.747
102.747
102.747











[Lens Data]












Surface







Number
R
D
nd
νd
θgF





1
319.23390
5.200
1.90265
35.77
0.5815


2
151.34780
13.400 
1.49782
82.57
0.5386


3
−783.35470
0.100


4
136.11850
13.200 
1.43385
95.23
0.5386


5

 D5(Variable)


6
122.06030
7.600
1.72047
34.71
0.5834


7
1981.86560
13.000 


8
303.62550
4.700
1.71736
29.57
0.6036


9
−303.62550
2.850
1.65240
55.27
0.5607


10
100.55440
3.315


11
−1987.36830
2.650
1.80400
46.60
0.5575


12
51.73610
3.700
1.66382
27.35
0.6319


13
100.83750
6.065


14
−83.24470
2.500
1.87071
40.73
0.5682


15
−665.86980
D15(Variable)


16
601.42740
4.700
1.75500
52.33
0.5475


17
−159.25800
0.100


18
93.67070
6.800
1.43385
95.23
0.5386


19
−253.82990
1.564


20
−113.21580
5.000
1.65412
39.68
0.5738


21
87.15300
0.975


22
116.35500
5.000
1.91082
35.25
0.5822


23
−377.46590
D23(Variable)


24

4.000
1.80400
46.60
0.5575


25
−119.18440
0.100


26
63.25160
6.800
1.59349
67.00
0.5366


27
−196.14820
1.800
1.84666
23.78
0.6192


28
196.14820
D28(Variable)


29
−128.97450
1.900
2.00100
29.13
0.5995


30
94.21930
4.866


31

8.000

(Aperture






Stop S)


32
416.97790
5.000
1.72916
54.61
0.5443


33
−76.00320
4.000


34
163.99730
2.000
1.80611
40.73
0.5672


35
69.61920
3.496


36
−129.19950
3.600
1.90200
25.26
0.6165


37
−52.57870
1.900
1.62731
59.30
0.5583


38
177.27800
5.206


39

9.390


40
78.30600
5.000
2.00100
29.13
0.5995


41
1628.46070
0.100


42
63.86980
3.000
1.80400
46.60
0.5575


43
33.62860
10.000 
1.48749
70.32
0.5291


44
−75.31750
6.047


45
−67.14290
2.000
1.90043
37.37
0.5772


46
216.78070
BF










[Variable distance data on zoom photographing]













W
M
T







D5
5.100
40.193
66.953



D15
63.457
28.364
1.603



D23
21.296
17.639
18.670



D28
6.100
9.757
8.725











[Lens Group Data]











Group
First surface
Focal length







G1
1
252.497



G2
6
−70.230



G3
16
107.659



G4
24
91.176



G5
29
−145.483











[Conditional Expression Corresponding Value]












<Negative lens L55(fN2 = −64.438)>



Conditional Expression (1)



ndN2 − (2.015 − 0.0068 × νdN2) = 0.016



Conditional Expression (2)νdN2 = 59.30



Conditional Expression (3), (3-1)θgFN2 = 0.5584



Conditional Expression (4), (4-1)



θgFN2 − (0.6418 − 0.00168 × νdN2) = 0.0162



Conditional Expression (5)(−fN2)/fR = 0.627



Conditional Expression (6)(−fN2)/f = 0.521



Conditional Expression (7)DN2 = 1.900



<Negative lens L55(fN4 = −64.438)>



Conditional Expression (11)



ndN4 − (2.015 − 0.0068 × νdN4) = 0.016



Conditional Expression (12)νdN4 = 59.30



Conditional Expression (13), (13-1)θgFN4 = 0.5584



Conditional Expression (14), (14-1)



θgFN4 − (0.6418 − 0.00168 × νdN4) = 0.0162



Conditional Expression (15)fN4/fGb = 0.443



Conditional Expression (16)(−fGb)/f = 1.177



Conditional Expression (17)DN4 = 1.900











FIG. 6A shows various aberration graphs of the optical system according to Third Example upon focusing on infinity in the wide angle end state. FIG. 6B shows various aberration graphs of the optical system according to Third Example upon focusing on infinity in the intermediate focal length state. FIG. 6C shows various aberration graphs of the optical system according to Third Example upon focusing on infinity in the telephoto end state. The various aberration graphs show that the optical system according to Third Example has favorably corrected various aberrations, and exerts excellent imaging performance.


Fourth Example

Fourth Example is described with reference to FIGS. 7 and 8A, 8B and 8C and Table 4. FIG. 7 is a diagram showing a lens configuration of an optical system in a state upon focusing on infinity according to Fourth Example of each embodiment. The optical system LS(4) according to Fourth Example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a positive refractive power; a fifth lens group G5 having a negative refractive power; and a sixth lens group G6 having a negative refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the first to sixth lens groups G1 to G6 move in directions indicated by arrows in FIG. 7. The aperture stop S is disposed between the second lens group G2 and the third lens group G3.


The first lens group G1 consists of, in order from the object: a negative meniscus lens L11 having a convex surface facing the object; a biconvex positive lens L12; and a positive meniscus lens L13 having a convex surface facing the object.


The second lens group G2 consists of, in order from the object: a negative meniscus lens L21 having a convex surface facing the object; biconcave negative lens L22; a biconvex positive lens L23; and a negative meniscus lens L24 having a concave surface facing the object.


The third lens group G3 consists of, in order from the object: a biconvex positive lens L31; a cemented lens consisting of a negative meniscus lens L32 having a convex surface facing the object, and a biconvex positive lens L33; and a negative meniscus lens L34 having a concave surface facing the object. The aperture stop S is disposed adjacent to the object side of the positive lens L31, and moves with the third lens group G3 upon zooming. The cemented lens consisting of the negative meniscus lens L32 and the positive lens L33 of the third lens group G3 constitutes a vibration-proof lens group (partial group) that is movable in a direction perpendicular to the optical axis, and corrects variation in imaging position due to a camera shake and the like (image blur on the image surface I).


The fourth lens group G4 consists of, in order from the object: a cemented lens consisting of a biconvex positive lens L41, and a negative meniscus lens L42 having a concave surface facing the object; and a cemented lens consisting of a negative meniscus lens L43 having a convex surface facing the object, and a biconvex positive lens L44. The positive lens L44 has an image-side lens surface that is an aspherical surface.


The fifth lens group G5 consists of, in order from the object: a cemented lens consisting of a biconvex positive lens L51, and a biconcave negative lens L52. Upon focusing from the infinity object to the short-distant (finite distant) object, the fifth lens group G5 moves toward the image along the optical axis. The negative lens L52 has an image-side lens surface that is an aspherical surface.


The sixth lens group G6 consists of, in order from the object: a negative meniscus lens L61 having a concave surface facing the object; and a biconvex positive lens L62. An image surface I is disposed on the image side of the sixth lens group G6. In this Example, the negative meniscus lens L61 of the sixth lens group G6 corresponds to a negative lens that satisfies the conditional expressions (1) to (4) and the like. In this Example, the sixth lens group G6 corresponds to an image-side negative lens group, and the negative meniscus lens L61 of the sixth lens group G6 corresponds to a negative lens that satisfies the conditional expressions (11) to (14) and the like. The negative meniscus lens L61 has an image-side lens surface that is an aspherical surface.


In this Example, the negative meniscus lens L11, the positive lens L12, the positive meniscus lens L13, the negative meniscus lens L21, the negative lens L22, the positive lens L23, and the negative meniscus lens L24 constitute the front group GF disposed closer to the object than the aperture stop S. The positive lens L31, the cemented lens consisting of the negative meniscus lens L32 and the positive lens L33, the negative meniscus lens L34, the cemented lens consisting of the positive lens L41 and the negative meniscus lens L42, the cemented lens consisting of the negative meniscus lens L43 and the positive lens L44, the cemented lens consisting of the positive lens L51 and the negative lens L52, the negative meniscus lens L61, and the positive lens L62 constitute the rear group GR disposed closer to the image than the aperture stop S.


The following Table 4 lists values of data on the optical system according to Fourth Example.









TABLE 4







[General Data]


Zooming ratio = 7.848













W
M
T







f
24.720
50.000
194.001



FNO
4.120
5.578
7.747




85.978
44.803
12.176



Y
21.379
21.700
21.700



TL
133.622
151.172
196.635



BF
11.869
21.707
38.749



fF
−22.437
−28.257
−22.437



fR
25.992
24.661
25.992











[Lens Data]












Surface







Number
R
D
nd
νd
θgF





 1
185.39670
1.700
1.90366
31.27
0.5948


 2
76.46580
0.861


 3
79.26480
6.196
1.59319
67.90
0.5440


 4
−565.11920
0.100


 5
63.45420
5.498
1.59319
67.90
0.5440


 6
434.75200
 D6(Variable)


 7
203.01440
1.100
1.90265
35.72
0.5804


 8
19.06950
5.142


 9
−53.01680
1.000
1.75500
52.33
0.5475


10
58.98300
0.511


11
37.16720
3.158
1.92286
20.88
0.6390


12
−70.22260
0.694


13
−33.57890
0.903
1.81600
46.59
0.5567


14
−1345.01350
D14(Variable)


15

2.000

(Aperture






Stop S)


16
40.44850
2.345
1.90265
35.72
0.5804


17
−316.98760
0.605


18
35.70840
1.000
2.00100
29.12
0.5996


19
20.49290
3.549
1.57957
53.74
0.5519


20
−74.86330
1.410


21
−37.16210
1.047
1.95375
32.33
0.5905


22
−418.77410
D22(Variable)


23
37.79500
4.737
1.83481
42.73
0.5648


24
−37.79500
1.004
1.90366
31.27
0.5948


25
−353.80920
0.100


26
31.05870
3.102
1.95375
32.33
0.5905


27
15.35540
8.795
1.49710
81.49
0.5377


 28*
−42.90350
D28(Variable)


29
474.24510
3.208
1.84666
23.80
0.6215


30
−34.68120
1.002
1.85135
40.13
0.5685


 31*
31.38060
D31(Variable)


32
−17.69750
1.400
1.68348
54.80
0.5501


 33*
−23.26090
0.100


34
1014.6406
 2.7385
1.68376
37.57
0.5782


35
−99.7136
BF










[Aspherical Surface Data]












28th Surface



κ = 1.000, A4 = 2.96E−05, A6 = −1.43E−07



A8 = 1.92E−09, A10 = −1.38E−11, A12 = 3.3122E−14



31st Surface



κ = 1.000, A4 = −5.38E−06, A6 = 1.47E−07



A8 = −2.09E−09, A10 = 1.45E−11, A12 = −3.5486E−14



33rd Surface



κ = 1.000, A4 = −2.59E−06, A6 = −1.89E−08



A8 = 8.54E−11, A10 = −2.37E−13, A12 = 0.00E+00











[Variable Distance Data on Zoom Photographing]













W
M
T







D6
1.982
18.089
56.429



D14
19.455
11.059
1.140



D22
13.005
6.692
1.483



D28
4.951
4.074
1.900



D31
9.993
17.182
24.566











[Lens Group Data]











Group
First surface
Focal length







G1
1
103.302



G2
7
−16.985



G3
15
48.485



G4
23
29.299



G5
29
−39.415



G6
32
−2329.811











[Conditional Expression Corresponding Value]












<Negative meniscus lens L61(fN2 = −120.581)>



Conditional Expression (1)



ndN2 − (2.015 − 0.0068 × νdN2) = 0.041



Conditional Expression (2)νdN2 = 54.80



Conditional Expression (3), (3-1)θgFN2 = 0.5501



Conditional Expression (4), (4-1)



θgFN2 − (0.6418 − 0.00168 × νdN2) = 0.0004



Conditional Expression (6)(−fN2)/fR = 4.639



Conditional Expression (7)(−fN2)/f = 4.878



Conditional Expression (8)DN2 = 1.400



<Negative meniscus lens L61(fN4 = −120.581)>



Conditional Expression (11)



ndN4 − (2.015 − 0.0068 × νdN4) = 0.041



Conditional Expression (12)νdN4 = 54.80



Conditional Expression (13), (13-1)θgFN4 = 0.5501



Conditional Expression (14), (14-1)



θgFN4 − (0.6418 − 0.00168 × νdN4) = 0.0004



Conditional Expression (15)fN4/fGb = 0.052



Conditional Expression (16)(−fGb)/f = 94.248



Conditional Expression (17)DN4 = 1.400











FIG. 8A shows various aberration graphs of the optical system according to Fourth Example upon focusing on infinity in the wide angle end state. FIG. 8B shows various aberration graphs of the optical system according to Fourth Example upon focusing on infinity in the intermediate focal length state. FIG. 8C shows various aberration graphs of the optical system according to Fourth Example upon focusing on infinity in the telephoto end state. The various aberration graphs show that the optical system according to Fourth Example has favorably corrected various aberrations, and exerts excellent imaging performance.


Fifth Example

Fifth Example is described with reference to FIGS. 9 and 10A, 10B, 10C and 10D and Table 5. FIG. 9 is a diagram showing a lens configuration of an optical system in a state upon focusing on infinity according to Fifth Example of each embodiment. The optical system LS(5) according to Fifth Example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the first to fifth lens groups G1 to G5 move in directions indicated by arrows in FIG. 9. The aperture stop S is disposed between the second lens group G2 and the third lens group G3.


The first lens group G1 consists of, in order from the object: a cemented lens consisting of a negative meniscus lens L11 having a convex surface facing the object, and a biconvex positive lens L12; and a positive meniscus lens L13 having a convex surface facing the object.


The second lens group G2 consists of, in order from the object: a negative meniscus lens L21 having a convex surface facing the object; a biconcave negative lens L22; a biconvex positive lens L23; and a cemented lens consisting of a biconcave negative lens L24 and a biconvex positive lens L25. Upon focusing from the infinity object to the short-distant (finite distant) object, the second lens group G2 moves toward the object along the optical axis. The negative meniscus lens L21 is a hybrid type lens that includes a lens main body made of glass, and a resin layer provided on the object-side surface of the lens main body. The object-side surface of the resin layer is an aspherical surface. The negative meniscus lens L21 is a composite type aspherical surface lens. In [Lens Data] described later, the surface number 6 indicates the object-side surface of the resin layer, the surface number 7 indicates the image-side surface of the resin layer and the object-side surface of the lens main body (a surface on which both the elements are in contact), and the surface number 8 indicates the image-side surface of the lens main body.


The third lens group G3 consists of, in order from the object: a biconvex positive lens L31; a biconvex positive lens L32; and a cemented lens consisting of a biconvex positive lens L33 and a negative meniscus lens L34 having a concave surface facing the object. The aperture stop S is disposed adjacent to the object side of the positive lens L31, and moves with the third lens group G3 upon zooming.


The fourth lens group G4 consists of, in order from the object: a cemented lens consisting of a biconcave negative lens L41 and a positive meniscus lens L42 having a convex surface facing the object; and a negative meniscus lens L43 having a concave surface facing the object. The cemented lens consisting of the negative lens L41 and the positive meniscus lens L42 of the fourth lens group G4 constitute a vibration-proof lens group (partial group) that is movable in a direction perpendicular to the optical axis, and corrects variation in imaging position due to a camera shake and the like (image blur on the image surface I). In this Example, the negative lens L41 of the fourth lens group G4 corresponds to a negative lens that satisfies the conditional expressions (1) to (4) and the like. In this Example, the fourth lens group G4 corresponds to an image-side negative lens group, and the negative lens L41 of the fourth lens group G4 corresponds to a negative lens that satisfies the conditional expressions (11) to (14) and the like. The negative lens L41 is a hybrid type lens that includes a lens main body made of glass, and a resin layer provided on the object-side surface of the lens main body. The object-side surface of the resin layer is an aspherical surface. The negative lens L41 is a composite type aspherical surface lens. In [Lens Data] described later, the surface number 24 indicates the object-side surface of the resin layer, the surface number 25 indicates the image-side surface of the resin layer and the object-side surface of the lens main body (a surface on which both the elements are in contact), and the surface number 26 indicates the image-side surface of the lens main body and the object-side surface of the positive meniscus lens L42 (a surface on which both the elements are in contact).


The fifth lens group G5 consists of, in order from the object: a positive meniscus lens L51 having a concave surface facing the object; a biconvex positive lens L52; and a cemented lens consisting of a biconcave negative lens L53 and a biconvex positive lens L54. An image surface I is disposed on the image side of the fifth lens group G5. The negative lens L53 has an object-side lens surface that is an aspherical surface.


In this Example, the cemented lens consisting of the negative meniscus lens L11 and the positive lens L12, the positive meniscus lens L13, the negative meniscus lens L21, the negative lens L22, the positive lens L23, the cemented lens consisting of the negative lens L24 and the positive lens L25 constitute the front group GF disposed closer to the object than the aperture stop S. The positive lens L31, the positive lens L32, the cemented lens consisting of the positive lens L33 and the negative meniscus lens L34, the cemented lens consisting of the negative lens L41 and the positive meniscus lens L42, the negative meniscus lens L43, the positive meniscus lens L51, the positive lens L52, and the cemented lens consisting of the negative lens L53 and the positive lens L54 constitute the rear group GR disposed closer to the image than the aperture stop S.


The following Table 5 lists values of data on the optical system according to Fifth Example.









TABLE 5







[General Data]


Zooming ratio = 15.701














W
M1
M2
T







f
18.530
28.008
104.938
290.935



FNO
3.607
4.166
5.692
5.890




79.654
53.877
15.291
5.624



Y
14.750
14.750
14.750
14.750



TL
171.0504
178.6364
231.8494
257.5207



BF
39.2287
46.7036
71.2782
82.7078



fF
−19.991
−22.282
−44.557
−102.163



fR
40.048
38.783
33.819
32.301











[Lens Data]












Surface







Number
R
D
nd
νd
θgF





 1
186.59960
2.200
1.83400
37.17
0.5775


 2
69.08900
8.800
1.49782
82.56
0.5390


 3
−494.44540
0.100


 4
73.40220
6.450
1.59319
67.87
0.5435


 5
2016.71160
 D5(Variable)


 6*
84.85000
0.100
1.55389
38.09
0.5928


 7
74.02190
1.200
1.83481
42.72
0.5640


 8
17.09750
6.950


 9
−37.97970
1.000
1.81600
46.63
0.5571


10
77.67130
0.150


11
36.26560
5.300
1.78472
25.68
0.6158


12
−36.26560
0.800


13
−25.69640
1.000
1.81600
46.63
0.5571


14
66.08300
2.050
1.80809
22.79
0.6289


15
−666.70370
D15(Variable)


16

1.000

(Aperture






Stop S)


17
68.30730
3.400
1.59319
67.87
0.5435


18
−47.99600
0.100


19
68.52370
2.450
1.48749
70.45
0.5289


20
−136.98390
0.100


21
46.52670
4.200
1.48749
70.45
0.5289


22
−36.16400
1.000
1.80809
22.79
0.6289


23
−202.95330
D23(Variable)


 24*
−55.09840
0.200
1.55389
38.09
0.5928


25
−57.24710
0.900
1.66106
56.09
0.5512


26
27.00000
2.150
1.72825
28.46
0.6077


27
70.74880
4.350


28
−26.69880
1.000
1.72916
54.66
0.5442


29
−76.47710
D29(Variable)


30
−333.89500
4.650
1.58913
61.18
0.5389


31
−24.64400
0.100


32
31.19630
5.850
1.48749
70.45
0.5289


33
−43.38890
1.450


 34*
−109.7164
1.000
1.883
40.77


35
20.2992
5.300
1.54814
45.79


36
−808.8132
BF










[Aspherical Surface Data]












6th Surface



κ = 1.000, A4 = 3.13E−06, A6 = 4.73E−10



A8 = −3.41E−11, A10 = 1.17E−13, A12 = 0.00E+00



24th Surface



κ = 1.000, A4 = 5.24E−06, A6 = −2.01E−09



A8 = 0.00E+00, A10 = 0.00E+00, A12 = 0.00E+00



34th Surface



κ = 1.000, A4 = −1.54E−05, A6 = 1.70E−09



A8 = 1.34E−11, A10 = −2.07E−13, A12 = 0.00E+00











[Variable Distance Data on Zoom Photographing]














W
M1
M2
T







D5
2.157
11.716
53.425
76.950



D15
33.801
24.353
11.283
2.000



D23
3.457
5.951
11.607
13.043



D29
10.587
8.092
2.437
1.000











[Lens Group Data]











Group
First surface
Focal length







G1
1
118.969



G2
6
−15.625



G3
16
27.175



G4
24
−25.446



G5
30
34.390











[Conditional Expression Corresponding Value]












<Negative lens L41(fN2 = −27.636)>



Conditional Expression (1)



ndN2 − (2.015 − 0.0068 × νdN2) = 0.027



Conditional Expression (2)νdN2 = 56.09



Conditional Expression (3), (3-1)θgFN2 = 0.5512



Conditional Expression (4), (4-1)



θgFN2 − (0.6418 − 0.00168 × νdN2) = 0.0036



Conditional Expression (5)(−fN2)/fR = 0.690



Conditional Expression (6)(−fN2)/f = 1.491



Conditional Expression (7)DN2 = 0.900



<Negative lens L41(fN4 = −27.636)>



Conditional Expression (11)



ndN4 − (2.015 − 0.0068 × νdN4) = 0.027



Conditional Expression (12)νdN4 = 56.09



Conditional Expression (13), (13-1)θgFN4 = 0.5512



Conditional Expression (14), (14-1)



θgFN4 − (0.6418 − 0.00168 × νdN4) = 0.0036



Conditional Expression (15)fN4/fGb = 1.086



Conditional Expression (16)(−fGb)/f = 1.373



Conditional Expression (17)DN4 = 0.900











FIG. 10A shows various aberration graphs of the optical system according to Fifth Example upon focusing on infinity in the wide angle end state. FIG. 10B shows various aberration graphs of the optical system according to Fifth Example upon focusing on infinity in a first intermediate focal length state. FIG. 10C shows various aberration graphs of the optical system according to Fifth Example upon focusing on infinity in a second intermediate focal length state. FIG. 10D shows various aberration graphs of the optical system according to Fifth Example upon focusing on infinity in the telephoto end state. The various aberration graphs show that the optical system according to Fifth Example has favorably corrected various aberrations, and exerts excellent imaging performances.


Sixth Example

Sixth Example is described with reference to FIGS. 11 and 12A, 12B and 12C and Table 6. FIG. 11 is a diagram showing a lens configuration of an optical system in a state upon focusing on infinity according to Sixth Example of each embodiment. The optical system LS(6) according to Sixth Example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a positive refractive power; and a third lens group G3 having a negative refractive power. Upon focusing from the infinity object to the short-distant (finite distant) object, the first lens group G1 and the second lens group G2 move toward the object along the optical axis by different amounts of movement. The aperture stop S is disposed between the first lens group G1 and the second lens group G2.


The first lens group G1 consists of, in order from the object: a biconcave negative lens L11; a biconvex positive lens L12; a cemented lens consisting of a biconvex positive lens L13 and a biconcave negative lens L14; and a negative meniscus lens L15 having a convex surface facing the object. The aperture stop S is disposed adjacent to the image side of the negative meniscus lens L15, and moves with the first lens group G1 upon focusing. The negative lens L11 has an image-side lens surface that is an aspherical surface.


The second lens group G2 consists of, in order from the object: a biconvex positive lens L21; and a negative meniscus lens L22 having a convex surface facing the object.


The third lens group G3 consists of, in order from the object: a positive meniscus lens L31 having a convex surface facing the object; a negative meniscus lens L32 having a concave surface facing the object; and a biconvex positive lens L33. An image surface I is disposed on the image side of the third lens group G3. In this Example, the negative meniscus lens L32 of the third lens group G3 corresponds to a negative lens that satisfies the conditional expressions (1) to (4) and the like. In this Example, the third lens group G3 corresponds to an image-side negative lens group, and the negative meniscus lens L32 of the third lens group G3 corresponds to a negative lens that satisfies the conditional expressions (11) to (14) and the like. The positive meniscus lens L31 has an image-side lens surface that is an aspherical surface. A cover glass CV is disposed between the third lens group G3 and the image surface I.


In this Example, the negative lens L11, the positive lens L12, the cemented lens consisting of the positive lens L13 and the negative lens L14, and the negative lens L15 constitute the front group GF disposed closer to the object than the aperture stop S. The positive lens L21, the negative meniscus lens L22, the positive meniscus lens L31, the negative meniscus lens L32, and the positive lens L33 constitute the rear group GR disposed closer to the image than the aperture stop S.


The following Table 6 lists values of data on the optical system according to Sixth Example.









TABLE 6







[General Data]













f
58.203



FNO
2.825




40.539



Y
21.700



TL
71.506



BF
0.100



fF
193.264



fR
41.152











[Lens Data]












Surface







Number
R
D
nd
νd
θgF





 1
−63.99090
1.200
1.73077
40.51
0.5727


 2*
71.71180
1.000


 3
42.93270
4.064
1.95375
32.33
0.5905


 4
−51.23440
1.082


 5
49.88300
4.042
1.59319
67.90
0.5440


 6
−30.98750
1.200
1.73800
32.26
0.5899


 7
45.45620
0.200


 8
31.62520
1.200
1.80518
25.45
0.6157


 9
22.75910
6.464


10

D10(Variable)

(Aperture






Stop S)


11
54.06210
3.455
1.59349
67.00
0.5358


12
−32.76480
0.200


13
31.23990
1.200
1.67300
38.15
0.5754


14
22.30120
D14(Variable)


15
43.39570
1.373
1.51680
64.13
0.5357


 16*
43.24690
17.859 


17
−17.25440
1.200
1.68348
54.80
0.5501


18
−176.84520
0.200


19
159.39470
4.819
1.95375
32.33
0.5905


20
83.44720
12.310 


21

1.600
1.51680
64.13
0.5357


22

BF










[Aspherical Surface Data]












2nd Surface



κ = 1.000, A4 = 1.39250E−05, A6 = 3.07014E−09



A8 = −6.46165E−12, A10 = 0.00000E+00, A12 = 0.00000E+00



16th Surface



κ = 1.000, A4 = −1.14801E−05, A6 = −6.50435E−09



A8 = −1.06124E−10, A10 = 0.00000E+00, A12 = 0.00000E+00











[Variable Distance Data on Short-Distance Photographing]













Upon
Upon focusing on
Upon focusing on




focusing
an intermediate
a short-distance




on infinity
distance object
object




f = 58.203
β = −0.500
β = −1.000







D10
5.331
5.445
5.684



D14
1.412
18.266
35.060











[Lens Group Data]











Group
First surface
Focal length







G1
1
193.264



G2
11
46.831



G3
15
−60.650











[Conditional Expression Corresponding Value]












<Negative meniscus lens L32(fN2 = −28.060)>



Conditional Expression (1)



ndN2 − (2.015 − 0.0068 × νdN2) = 0.041



Conditional Expression (2)νdN2 = 54.80



Conditional Expression (3), (3-1)θgFN2 = 0.5501



Conditional Expression (4), (4-1)



θgFN2 − (0.6418 − 0.00168 × νdN2) = 0.0004



Conditional Expression (6)(−fN2)/fR = 0.682



Conditional Expression (7)(−fN2)/f = 0.482



Conditional Expression (8)DN2 = 1.200



<Negative meniscus lens L32(fN4 = −28.060)>



Conditional Expression (11)



ndN4 − (2.015 − 0.0068 × νdN4) = 0.041



Conditional Expression (12)νdN4 = 54.80



Conditional Expression (13), (13-1)θgFN4 = 0.5501



Conditional Expression (14), (14-1)



θgFN4 − (0.6418 − 0.00168 × νdN4) = 0.0004



Conditional Expression (15)fN4/fGb = 0.463



Conditional Expression (16)(−fGb)/f = 1.042



Conditional Expression (17)DN4 = 1.200











FIG. 12A shows various aberration graphs of the optical system according to Sixth Example upon focusing on infinity. FIG. 12B shows various aberration graphs of the optical system according to Sixth Example upon focusing on an intermediate distant object. FIG. 12C shows various aberration graphs of the optical system according to Sixth Example upon focusing on a short-distant (very short distance) object. The various aberration graphs show that the optical system according to Sixth Example has favorably corrected various aberrations, and exerts excellent imaging performance.


Seventh Example

Seventh Example is described with reference to FIGS. 13 and 14A, 14B and 14C and Table 7. FIG. 13 is a diagram showing a lens configuration of an optical system in a state upon focusing on infinity according to Seventh Example of each embodiment. The optical system LS(7) according to Seventh Example consists of, in order from the object: a first lens group G1 having a positive refractive power; a second lens group G2 having a negative refractive power; a third lens group G3 having a positive refractive power; a fourth lens group G4 having a negative refractive power; and a fifth lens group G5 having a positive refractive power. Upon zooming from the wide-angle end state (W) to the telephoto end state (T), the first to fifth lens groups G1 to G5 move in directions indicated by arrows in FIG. 13. The aperture stop S is disposed between the second lens group G2 and the third lens group G3.


The first lens group G1 consists of, in order from the object: a cemented lens consisting of a negative meniscus lens L11 having a convex surface facing the object, and a biconvex positive lens L12; a positive meniscus lens L13 having a convex surface facing the object; and a positive meniscus lens L14 having a convex surface facing the object.


The second lens group G2 consists of, in order from the object: a negative meniscus lens L21 having a convex surface facing the object; a biconcave negative lens L22; and a cemented lens consisting of a biconvex positive lens L23, and a biconcave negative lens L24.


The third lens group G3 consists of, in order from the object: a biconvex positive lens L31; a cemented lens consisting of a positive meniscus lens L32 having a convex surface facing the object, and a negative meniscus lens L33 having a convex surface facing the object; and a biconvex positive lens L34. The aperture stop S is disposed adjacent to the object side of the positive lens L31, and moves with the third lens group G3 upon zooming. The third lens group G3 constitutes a vibration-proof lens group (partial group) that is movable in a direction perpendicular to the optical axis, and corrects variation in imaging position due to a camera shake and the like (image blur on the image surface I). The positive lens L31 has opposite lens surfaces that are aspherical surfaces.


The fourth lens group G4 consists of, in order from the object: a cemented lens consisting of a biconvex positive lens L41, and a biconcave negative lens L42. In this Example, the negative lens L42 of the fourth lens group G4 corresponds to a negative lens that satisfies the conditional expressions (1) to (4) and the like. In this Example, the fourth lens group G4 corresponds to an image-side negative lens group, and the negative lens L42 of the fourth lens group G4 corresponds to a negative lens that satisfies the conditional expressions (11) to (14) and the like.


The fifth lens group G5 consists of, in order from the object: a cemented lens consisting of biconvex positive lens L51, and a negative meniscus lens L52 having a concave surface facing the object. An image surface I is disposed on the image side of the fifth lens group G5. Upon focusing from the infinity object to the short-distant (finite distant) object, the fifth lens group G5 moves toward the image along the optical axis. The positive lens L51 has an object-side lens surface that is an aspherical surface. An optical filter FL is disposed between the fifth lens group G5 and the image surface I. The optical filter FL may be, for example, an NC filter (neutral color filter), a color filter, a polarizing filter, an ND filter (neutral density filter), an IR filter (infrared cutoff filter) or the like.


In this Example, the cemented lens consisting of the negative meniscus lens L11 and the positive lens L22, the positive meniscus lens L13, the positive meniscus lens L14, the negative meniscus lens L21, the negative lens L22, the cemented lens consisting of the positive lens L23 and the negative lens L24 constitute the front group GF disposed closer to the object than the aperture stop S. The positive lens L31, the cemented lens consisting of the positive meniscus lens L32 and the negative meniscus lens L33, the positive lens L34, the cemented lens consisting of positive lens L41 and the negative lens L42, and the cemented lens consisting of the positive lens L51 and the negative meniscus lens L52 constitute the rear group GR disposed closer to the image than the aperture stop S.


The following Table 7 lists values of data on the optical system according to Seventh Example.









TABLE 7







[General Data]


Zooming ratio = 56.903













W
M
T







f
4.397
12.677
250.201



FNO
3.354
4.256
7.172




87.200
34.963
1.798



Y
3.400
4.000
4.000



TL
102.372
105.195
145.381



BF
0.600
0.600
0.600



fF
−10.163
−14.077
−146.596



fR
19.989
20.803
109.602











[Lens Data]












Surface







Number
R
D
nd
νd
θgF





 1
233.16059
1.800
1.80440
39.61
0.5719


 2
63.31232
5.650
1.43700
95.10
0.5336


 3
−315.75938
0.200


 4
75.70769
3.500
1.49782
82.57
0.5386


 5
509.52120
0.200


 6
54.53234
4.100
1.49782
82.57
0.5386


 7
394.77865
 D7(Variable)


 8
1001.52720
1.000
1.78800
47.35
0.5559


 9
8.03857
4.500


10
−24.83933
0.900
1.83481
42.73
0.5648


11
53.48225
0.200


12
17.37996
3.000
1.92286
20.88
0.6390


13
−72.51614
0.900
1.91082
35.25
0.5822


14
48.65649
D14(Variable)


15

0.750

(Aperture






Stop S)


 16*
10.27226
2.500
1.55332
71.68
0.5404


 17*
−59.97135
0.200


18
10.93597
2.100
1.49782
82.57
0.5386


19
1249.11870
0.800
1.88300
40.66
0.5668


20
8.89183
0.650


21
27.08310
1.900
1.48749
70.32
0.5291


22
−18.25921
D22(Variable)


23
73.43106
1.200
1.79504
28.69
0.6065


24
−179.22763
0.600
1.66501
53.81
0.5539


25
15.48596
D25(Variable)


 26*
17.31291
3.050
1.62299
58.12
0.5438


27
−12.30844
0.800
1.83400
37.18
0.5778


28
−65.03803
D28(Variable)


29

0.210
1.51680
63.88
0.5360


30

1.348


31

0.500
1.51680
63.88
0.5360


32

BF










[Aspherical Surface Data]












16th Surface



κ = 0.468, A4 = −1.37799E−06, A6 = −2.97638E−08



A8 = 0.00000E+00, A10 = 0.00000E+00, A12 = 0.00000E+00



17th Surface



κ = 1.000, A4 = 7.52375E−05, A6 = −3.72394E−07



A8 = 0.00000E+00, A10 = 0.00000E+00, A12 = 0.00000E+00



26th Surface



κ = 1.000, A4 = 2.35970E−05, A6 = 1.60894E−07



A8 = 0.00000E+00, A10 = 0.00000E+00, A12 = 0.00000E+00











[Variable Distance Data on Zoom Photographing]













W
M
T







D7
0.500
18.809
61.777



D14
43.318
19.648
0.833



D22
1.000
4.130
8.170



D25
8.806
8.909
27.759



D28
5.590
10.542
3.684











[Lens Group Data]











Group
First surface
Focal length







G1
1
79.658



G2
8
−8.400



G3
15
16.089



G4
23
−32.356



G5
26
31.403











[Conditional Expression Corresponding Value]












<Negative lens L42(fN2 = −21.409)>



Conditional Expression (1)



ndN2 − (2.015 − 0.0068 × νdN2) = 0.016



Conditional Expression (2)νdN2 = 53.81



Conditional Expression (3), (3-1)θgFN2 = 0.5539



Conditional Expression (4), (4-1)



θgFN2 − (0.6418 − 0.00168 × νdN2) = 0.0025



Conditional Expression (5)(−fN2)/fR = 1.071



Conditional Expression (6)(−fN2)/f = 4.869



Conditional Expression (7)DN2 = 0.600



<Negative lens L42(fN4 = −21.409)>



Conditional Expression (11)



ndN4 − (2.015 − 0.0068 × νdN4) = 0.016



Conditional Expression (12)νdN4 = 53.81



Conditional Expression (13), (13-1)θgFN4 = 0.5539



Conditional Expression (14), (14-1)



θgFN4 − (0.6418 − 0.00168 × νdN4) = 0.0025



Conditional Expression (15)fN4/fGb = 0.662



Conditional Expression (16)(−fGb)/f = 7.359



Conditional Expression (17)DN4 = 0.600











FIG. 14A shows various aberration graphs of the optical system according to Seventh Example upon focusing on infinity in the wide angle end state. FIG. 14B shows various aberration graphs of the optical system according to Seventh Example upon focusing on infinity in the intermediate focal length state. FIG. 14C shows various aberration graphs of the optical system according to Seventh Example upon focusing on infinity in the telephoto end state. The various aberration graphs show that the optical system according to Seventh Example has favorably corrected various aberrations, and exerts excellent imaging performance.


According to each Example, the optical system where for correction of chromatic aberrations, in addition to primary achromatization, the secondary spectrum is favorably corrected can be achieved.


Here, Examples described above show specific examples of the invention of the present application. The invention of the present application is not limited to these Examples.


Note that the following content can be adopted in a range without impairing the optical performance of the optical system of this embodiment.


The focusing lens group is assumed to indicate a portion that includes at least one lens separated by air distances changing upon focusing. That is, a focusing lens group may be adopted that moves a single or multiple lens groups, or a partial lens group in the optical axis direction to achieve focusing from the infinity object to the short-distant object. The focusing lens group is also applicable to autofocusing, and is suitable also for motor drive for autofocusing (using an ultrasonic motor).


In Fourth, Fifth, and Seventh Examples, the configurations having the vibration-proof function are described. However, the present application is not limited thereto, and may adopt a configuration having no vibration-proof function. The other Examples having no vibration-proof function may have a configuration having the vibration-proof function.


The lens surface may be made of a spherical surface or a planar surface, or an aspherical surface. A case where the lens surface is a spherical surface or a planar surface is preferable because lens processing, and assembling and adjustment are facilitated, and the optical performance degradation due to errors caused by processing and assembling and adjustment can be prevented. Furthermore, it is preferable because the degradation in representation performance even with the image surface being misaligned is small.


In a case where the lens surface is an aspherical surface, the aspherical surface may be any of an aspherical surface made by a grinding process, a glass mold aspherical surface made by forming glass into an aspherical shape with a mold, and a composite type aspherical surface made by forming a resin on a surface of glass into an aspherical shape. The lens surface may be a diffractive surface. The lens may be a gradient-index lens (GRIN lens), or a plastic lens.


An antireflection film having a high transmissivity in a wide wavelength region may be applied onto each lens surface in order to reduce flares and ghosts and achieve optical performances having a high contrast. Accordingly, flares and ghosts can be reduced, and high optical performances having a high contrast can be achieved.












EXPLANATION OF NUMERALS AND CHARACTERS


















G1 First lens group
G2 Second lens group



G3 Third lens group
G4 Fourth lens group



G5 Fifth lens group
G6 Sixth lens group



G7 Seventh lens group



I Image surface
S Aperture stop









Claims
  • 1. An optical system, comprising: an aperture stop; and a negative lens that is disposed closer to an image than the aperture stop, wherein the negative lens satisfies the following conditional expressions: −0.010<ndN2−(2.015−0.0068×νdN2),50.00<νdN2<65.00,0.545<θgFN2,−0.010<θgFN2−(0.6418−0.00168×νdN2)where ndN2: a refractive index of the negative lens for d-line,νdN2: an Abbe number of the negative lens with reference to d-line, andθgFN2: a partial dispersion ratio of the negative lens, defined by a following expression when a refractive index of the negative lens for g-line is ngN2, a refractive index of the negative lens for F-line is nFN2, and a refractive index of the negative lens for C-line is nCN2: θgFN2=(ngN2−nFN2)/(nFN2−nCN2).
  • 2. The optical system according to claim 1, consisting of: the aperture stop; a front group disposed closer to an object than the aperture stop; and a rear group disposed closer to the image than the aperture stop,wherein the rear group includes the negative lens and satisfies the following conditional expression: −10.00<(−fN2)/fR<10.00where fN2: a focal length of the negative lens, andfR: a focal length of the rear group; in a case where the optical system is a zoom optical system, the focal length of the rear group in a wide angle end state.
  • 3. The optical system according to claim 1, wherein the negative lens satisfies the following conditional expression: 0.10<(−fN2)/f<15.00where fN2: a focal length of the negative lens, andf: a focal length of the optical system; in a case where the optical system is a zoom optical system, the focal length of the optical system in a wide angle end state.
  • 4. The optical system according to claim 1, wherein the negative lens satisfies the following conditional expression: 0.555<θgFN2.
  • 5. The optical system according to claim 1, wherein the negative lens satisfies the following conditional expression: 0.010<θgFN2−(0.6418−0.00168×νdN2).
  • 6. The optical system according to claim 1, wherein the negative lens satisfies the following conditional expression: DN2>0.400 [mm]where DN2: a thickness of the negative lens on an optical axis.
  • 7. An optical system, comprising a plurality of lens groups that include lens groups having negative refractive powers, upon zooming or focusing, a distance between the lens groups adjacent to each other changes, andan image-side negative lens group disposed closest to an image among the lens groups having the negative refractive powers includes a negative lens that satisfies the following conditional expressions: −0.010<ndN4−(2.015−0.0068×νdN4),50.00<νdN4<65.00,0.545<θgFN4,−0.010<θgFN4−(0.6418−0.00168×νdN4)where ndN4: a refractive index of the negative lens for d-line,νdN4: an Abbe number of the negative lens with reference to d-line, andθgFN4: a partial dispersion ratio of the negative lens, defined by a following expression when a refractive index of the negative lens for g-line is ngN4, a refractive index of the negative lens for F-line is nFN4, and a refractive index of the negative lens for C-line is nCN4: θgFN4=(ngN4−nFN4)/(nFN4−nCN4).
  • 8. The optical system according to claim 7, wherein the negative lens satisfies the following conditional expression: 0.02<fN4/fGb<3.00where fN4: a focal length of the negative lens, andfGb: a focal length of the image-side negative lens group.
  • 9. The optical system according to claim 7, wherein the image-side negative lens group satisfies the following conditional expression: 0.50<(−fGb)/f<100.00where fGb: a focal length of the image-side negative lens group, andf: a focal length of the optical system; in a case where the optical system is a zoom optical system, the focal length of the optical system in a wide angle end state.
  • 10. The optical system according to claim 7, wherein the negative lens satisfies the following conditional expression: 0.555<θgFN4.
  • 11. The optical system according to claim 7, wherein the negative lens satisfies the following conditional expression: 0.010<θgFN4−(0.6418−0.00168×νdN4).
  • 12. The optical system according to claim 7, wherein the negative lens satisfies the following conditional expression: DN4>0.400 [mm]where DN4: a thickness of the negative lens on an optical axis.
  • 13. The optical system according to claim 7, wherein the negative lens is a single lens, or one lens of two lenses of a cemented lens consisting of the two lenses cemented to each other.
  • 14. The optical system according to claim 1, wherein at least one lens surface of an object-side lens surface and an image-side lens surface of the negative lens is in contact with air.
  • 15. The optical system according to claim 7, wherein the negative lens is a glass lens.
  • 16. An optical apparatus comprising the optical system according to claim 1.
  • 17. A method for manufacturing an optical system, the method comprises a step of arranging each lens in a lens barrel so that the optical system comprises an aperture stop; and a negative lens that is disposed closer to an image than the aperture stop, wherein the negative lens satisfies the following conditional expressions: −0.010<ndN2−(2.015−0.0068×νdN2),50.00<νdN2<65.00,0.545<θgFN2,−0.010<θgFN2−(0.6418−0.00168×νdN2)where ndN2: a refractive index of the negative lens for d-line,νdN2: an Abbe number of the negative lens with reference to d-line, andθgFN2: a partial dispersion ratio of the negative lens, defined by a following expression when a refractive index of the negative lens for g-line is ngN2, a refractive index of the negative lens for F-line is nFN2, and a refractive index of the negative lens for C-line is nCN2: θgFN2=(ngN2−nFN2)/(nFN2−nCN2).
  • 18. A method for manufacturing an optical system that includes a plurality of lens groups including lens groups having negative refractive powers, the method comprises a step of arranging each lens in a lens barrel so that upon zooming or focusing, a distance between the lens groups adjacent to each other changes, andan image-side negative lens group disposed closest to an image among the lens groups having the negative refractive powers includes a negative lens that satisfies the following conditional expressions: −0.010<ndN4−(2.015−0.0068×νdN4),50.00<νdN4<65.00,0.545<θgFN4,−0.010<θgFN4−(0.6418−0.00168×νdN4)where ndN4: a refractive index of the negative lens for d-line,νdN4: an Abbe number of the negative lens with reference to d-line, andθgFN4: a partial dispersion ratio of the negative lens, defined by a following expression when a refractive index of the negative lens for g-line is ngN4, a refractive index of the negative lens for F-line is nFN4, and a refractive index of the negative lens for C-line is nCN4: θgFN4=(ngN4−nFN4)/(nFN4−nCN4).
Priority Claims (2)
Number Date Country Kind
2019-157741 Aug 2019 JP national
2019-157744 Aug 2019 JP national
PCT Information
Filing Document Filing Date Country Kind
PCT/JP2020/032106 8/26/2020 WO