JP2005352021A - Objective lens for microscope - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide an objective lens for microscope which exhibits an excellent imaging performance and has satisfactory operability of a correction ring. <P>SOLUTION: The objective lens is provided with a first lens group G1 which comprises a positive meniscus lens component of directing a concave face to the object side and has a positive refractive power of converting luminous flux from an object to weak divergent luminous flux, a second lens group G2 which has a positive refractive power and is movable along a light axis and a third lens group G3 having a negative refractive power in order from the object side. The objective lens satisfies the following conditional relations; 1<f<SB>1</SB>/f<3, 3<f<SB>2</SB>/f<12, -0.9<f<SB>2</SB>/f<SB>3</SB><-0.6, wherein f<SB>1</SB>is a focal distance of the first lens group, f<SB>2</SB>is a focal distance of the second lens group, f<SB>3</SB>is a focal distance of the third lens group and f is a focal distance of a whole system. <P>COPYRIGHT: (C)2006,JPO&NCIPI

Description

  The present invention relates to an objective lens for a microscope, and in particular, with a correction ring that can maintain good imaging performance even when the thickness of a plane parallel plate such as a cover glass arranged on the object side changes. The present invention relates to a microscope objective lens.

In general, when the thickness of a plane parallel plate such as a cover glass changes more than a design value, the objective lens for a microscope deteriorates its imaging performance, and this tendency is caused by the numerical aperture (NA) of the objective lens. The larger it becomes, the more noticeable it becomes. In view of this, a so-called objective lens with a correction ring is known that corrects aberration fluctuations by changing the lens interval in the objective lens in accordance with the change in the thickness of the cover glass (for example, Patent Documents 1 and 2). reference).
JP-A-10-133118 JP-A-8-114747

The objective lens with a correction ring described in Patent Document 1 includes, in order from the object side, a first lens group having a positive refractive power for converging a light beam from the object, and positive, negative, and positive 3 arranged in order from the object side. A second lens group that is composed of a cemented lens and has a small refractive power, and a third lens group that has a negative refractive power, and the second lens group is moved along the optical axis. Aberration correction is performed by changing the glass thickness.
Moreover, the objective lens with a correction ring described in Patent Document 2 has a positive meniscus lens component having a concave surface directed toward the object side in order from the object side, and has a positive refractive power for converting the light beam from the object into a substantially parallel light beam. A first lens group, a second lens group including a divergent cementing surface and having a positive refractive power in combination, a third lens group having a negative refractive surface having a strong diverging action, and a fourth lens group having a negative refractive power By moving the second lens group along the optical axis, aberration correction is performed by changing the thickness of the cover glass.

  In recent years, in the field of biology, the main focus is shifting from the conventional observation of cell morphology to examining the information transmission mechanism between cells. Along with this, the need for higher performance of microscopes and objective lenses has also been expanded. Therefore, there is a need for a microscope objective lens with good operability that has a high resolution, high contrast corresponding to these thicknesses, and a correction ring mechanism with a small focus position shift when adjusting the correction ring. It is increasing.

  However, the objective lens described in Patent Document 1 suppresses fluctuations in the overall focal length by reducing the refractive power of the moving lens group, thereby reducing the deviation of the image at the paraxial position. Therefore, the amount of movement of the lens group that corrects the occurrence of spherical aberration due to the change in the cover glass thickness must be secured, and the focus position is shifted due to the change in the best image plane due to the movement of the lens group. As a result, it takes time to operate the correction ring. The objective lens described in Patent Document 2 has a large NA and chromatic aberration is corrected by a cemented lens, resulting in high resolution and high contrast. However, when the moving group is moved, the focus position is shifted, and the correction ring is operated. Takes time.

  The present invention has been made in view of the problems of the prior art as described above, and an object of the present invention is to provide a microscope objective lens that exhibits good imaging performance and good operability of the correction ring. It is to provide.

In order to achieve the above object, an objective lens for a microscope according to the present invention includes a positive meniscus lens component having a concave surface facing the object side in order from the object side, and has a positive refractive power for converting a light beam from the object into a weak divergent light beam. The first lens group, the second lens group having positive refractive power and movable along the optical axis, and the third lens group having negative refractive power are arranged, and the following conditional expression is satisfied.
_{1 <f 1 / f <3} (1)
_{3 <f 2 / f <12} (2)
_{-0.9 <f 2 / f 3 <} -0.6 (3)
Here, f ₁ is the focal length of the first lens group, f ₂ is the focal length of the second lens group, f ₃ is the focal length of the third lens group, and f is the focal length of the entire system.

In the microscope objective lens according to the present invention, at least one curvature radius in the third lens group is R ₃ , a refractive index difference between media before and after the surface having the curvature radius R ₃ is Δn, and the second lens. 2. The microscope objective lens according to claim 1, wherein the following conditional expression is satisfied, where the curvature radius R ₂₁ of the surface closest to the object side of the group and the curvature radius R ₂₂ of the surface closest to the image side of the second lens group are satisfied. .
1 <| R ₃ / Δn | / f <12 (4)
−1.3 <R ₂₁ / R ₂₂ <−0.5 (5)

The microscope objective lens of the present invention satisfies the following conditional expression when the Abbe number of the convex lens included in the second lens group is ν ₂ .
ν ₂ <70 (6)

The microscope objective lens of the present invention satisfies the following conditional expression when the magnification of the second lens group is β ₂ .
−1.8 <β ₂ <−1.1 (7)

  According to the present invention, it is possible to provide an objective lens for a microscope that exhibits good imaging performance and that has good operability of the correction ring.

Prior to the description of the embodiments, the reason for the configuration according to the present invention and the operational effects based on the reason will be described.
First, according to the present invention, the first NA lens group having a positive refractive power including a positive lens having a concave surface facing the object side reduces the opening angle of a high NA light beam emitted from the object. Here, the conditional expression (1) defines the refractive power of the first lens group, and is a condition provided for correcting spherical aberration, coma aberration, and chromatic aberration. If the lower limit of this condition is not reached, the refractive power of the first lens group becomes too strong, and spherical aberration, coma aberration, and chromatic aberration are greatly corrected and insufficiently corrected. In addition, high-order spherical aberration that occurs in the short wavelength region is greatly under-corrected and cannot be corrected by the subsequent lens group. On the contrary, if the upper limit of this condition is exceeded, the refractive power of the first lens group becomes too weak, the height of the light beam emitted from the first lens group becomes high, and high-order spherical aberration occurs. In addition, it is difficult to keep the entire length of the objective lens at the same focal length.

The second lens group converts the light beam diameter into a converged light beam by narrowing the light beam diameter. In the second lens group, spherical aberration and chromatic aberration are effectively corrected. Further, the spherical aberration is adjusted by moving this lens group along the optical axis.
Here, the conditional expression (2) defines the refractive power of the second lens group. If the lower limit of this condition is not reached, the converging action becomes too strong and negative spherical aberration occurs, making it difficult to correct the spherical aberration generated in the first lens group. On the contrary, if the upper limit of this condition is exceeded, the amount of spherical aberration generated with respect to the amount of movement when the lens group is moved becomes small. Therefore, to correct spherical aberration, the amount of movement, that is, the first to third lens groups A wide space between each other must be ensured. Furthermore, since the refractive power is weak, in order to balance the Petzval sum, it is necessary to increase the number of lenses in other lens groups, and more space is required, resulting in a longer total length of the lens system. .

  The light beam converged by the second lens group is emitted to the image side by the third lens group. In the objective lens of the present invention, a large positive refractive power is generated by the first lens group and the second lens group. Therefore, in order to correct the curvature of field satisfactorily, it is necessary to control the Petzval sum to an appropriate value, and thus a negative refractive power is required in the third lens group.

  The objective lens of the present invention is characterized in that the shift of the focus position of the image is small when the second lens group is moved. In order to reduce the shift of the focus position, it is not sufficient to reduce the fluctuation of the paraxial image position when the lens group is moved. This is because the focus position, that is, the best image plane is shifted from the paraxial position due to generation of spherical aberration due to the movement of the lens group. Therefore, in order to reduce the shift of the focus position, the paraxial image position must be changed so as to cancel in the direction opposite to the direction in which the best surface changes. Therefore, if the angle of the paraxial ray incident on the second lens group is larger than the angle of the paraxial ray emitted from the second lens group with respect to the optical axis, spherical aberration occurs when the moving group is moved. The paraxial image position fluctuates in the direction opposite to the direction in which it is performed. Conditional expression (3) must be satisfied with respect to the ratio of the refractive power of the second lens group and the refractive power of the third lens group so as to satisfy such a light ray relationship.

  Conditional expression (3) determines the ratio of the refractive power converged by the second lens group and the divergent refractive power of the third lens group so that the ray angle is slightly tighter on the incident side than on the outgoing side. It has established. If the lower limit of this condition is not reached, the refractive power that the second lens group converges is smaller than the refractive power that the third lens group diverges, and the light angle on the incident side becomes smaller and the lens group is moved. In addition, the paraxial image position greatly fluctuates in the same direction as the spherical aberration occurs, and the focus position shift increases. On the contrary, if the upper limit of this condition is exceeded, the refractive power that the second lens group converges is larger than the refractive power that the third lens group diverges, and the light ray angle on the incident side increases, and the lens group When the is moved, the paraxial image position largely fluctuates in the direction opposite to the direction in which spherical aberration occurs, and the focus position shift increases.

  It is desirable that the microscope objective lens of the present invention described above further satisfies the conditional expression (4). Conditional expression (4) defines the divergent power of the negative refracting power surface of the third lens group. This negative refracting power surface generates a positive spherical aberration and is generated in the first lens group and the second lens group. This is a condition provided for effectively canceling the amount of negative spherical aberration generated. If the lower limit of this condition is not reached, the negative refracting power surface becomes tight, and the amount of positive spherical aberration that occurs increases too much, and high-order spherical aberration also occurs, thereby canceling the change in the cover glass thickness. Even when the second lens group is moved to the positive, positive spherical aberration and higher-order spherical aberration remain. On the other hand, if the upper limit of this condition is exceeded, the positive spherical aberration generated on the negative refractive power surface is reduced, and the axial chromatic aberration is insufficiently corrected. Even if the group is moved, negative spherical aberration and axial chromatic aberration cannot be corrected and remain.

  In the microscope objective lens of the present invention, it is further desirable if conditional expression (5) is satisfied. Conditional expression (5) determines that the ray angle of the paraxial ray with respect to the optical axis is slightly larger on the incident side than on the emission side. Below the lower limit of this condition, the radius of curvature of the exit-side surface becomes too smaller than the radius of curvature of the entrance-side surface, and the ray angle on the exit side becomes large. The position greatly fluctuates in the direction opposite to the direction in which spherical aberration occurs, and the focus position shift increases. Conversely, if the upper limit of this condition is exceeded, the radius of curvature of the exit-side surface becomes too larger than the radius of curvature of the entrance-side surface, the ray angle on the exit side becomes smaller, and when the lens group is moved, The paraxial image position greatly fluctuates in the same direction as the spherical aberration occurs, and the focus position shift increases.

  Furthermore, in the microscope objective lens of the present invention, it is further desirable if conditional expression (6) is satisfied. Conditional expression (6) defines the Abbe number of the convex lens included in the second lens group, and is a condition provided for correcting chromatic aberration. If the range of the conditional expression is not satisfied, the chromatic aberration is insufficiently corrected.

  Furthermore, in the microscope objective lens of the present invention, it is further desirable if conditional expression (7) is satisfied. Conditional expression (7) defines the magnification of the second lens group, and the light beam angle with respect to the optical axis of the paraxial light beam is determined to be slightly larger on the incident side than on the output side. If the lower limit of this condition is not reached, the ray angle on the incident side will increase, and when the lens group is moved, the paraxial image position will fluctuate greatly in the direction opposite to the direction in which spherical aberration occurs, resulting in a shift in focus position. Becomes larger. On the other hand, if the upper limit of this condition is exceeded, the ray angle on the incident side decreases, and the paraxial image position when the lens group is moved fluctuates greatly in the same direction as the spherical aberration occurs. Misalignment increases.

Embodiments of the objective lens for a microscope according to the present invention will be described below with reference to the drawings.
Example 1
1 is a cross-sectional view along the optical axis showing the optical configuration of Example 1, FIG. 2 is an aberration diagram when the cover glass thickness of Example 1 is 0 mm, (a) is spherical aberration, and (b) is distortion aberration. , (C) is astigmatism, (d) is coma, FIG. 3 is an aberration diagram when the cover glass thickness of Example 1 is 1 mm, (a) spherical aberration, (b) distortion, (C) is astigmatism, (d) is coma, FIG. 4 is an aberration diagram when the cover glass thickness of Example 1 is 2 mm, (a) is spherical aberration, (b) is distortion, ( c) shows astigmatism, and (d) shows coma.

As shown in FIG. 1, the first lens group G1 includes a positive meniscus lens having a concave surface facing the object side, and a cemented lens of a negative meniscus lens having a concave surface facing the image side and a biconvex lens. The second lens group G2 is composed of one biconvex lens. The third lens group G3 includes a cemented meniscus lens including a negative meniscus lens having a concave surface facing the image side, a biconvex lens, a negative meniscus lens having a concave surface facing the object side, a cemented meniscus lens having a biconvex lens and a biconcave lens, It consists of a cemented meniscus lens having a negative meniscus lens with a concave surface facing the side and a positive meniscus lens with a concave surface facing the object side.
Example 1 is an objective lens that has a magnification of 40 × and NA of 0.6, and can be corrected within a range of high resolution and a cover glass thickness of 0 to 2.

The lens data of Example 1 is shown below.
In this lens data, NA is the numerical aperture, and W.I. D. Is a working distance, β is a magnification, r1, r2,... Are curvature radii of the lens surfaces shown in order from the object side, d1, d2,... Are intervals between the lens surfaces shown in order from the object side, n1, n2, ... Is the refractive index of each lens shown in order from the object side, and .nu.1, .nu.2,... Are Abbe numbers of the lenses shown in order from the object side. These codes are also used in common in the lens data of the second embodiment.
Further, the material of the cover glass is a glass petri dish, and the refractive index of the d line and the Abbe number are designed as nd = 1.52287 and νd = 59.89, respectively.

NA = 0.6, WD = 3.92, β = −40, f = 4.5
rl = −12.9703 dl = 2.4988 nl = 1.77250 νl = 49.60
r2 = −6.0227 d2 = 0.3057
r3 = 21.1823 d3 = 1.17 n3 = 1.51823 ν3 = 58.90
r4 = 6.7708 d4 = 3.8916 n4 = 1.49700 ν4 = 81.54
r5 = −41.9148 d5 = 1.3295
r6 = 15.3948 d6 = 2.6371 n6 = 1.43875 ν6 = 94.93
r7 = -18.0885 d7 = 2.6663
r8 = 34.638 d8 = 1.1 n8 = 1.74100 ν8 = 52.64
r9 = 6.1365 d9 = 5.4929 n9 = 1.43875 ν9 = 94.93
rl0 = −6.1365 dl0 = 1.1 nl0 = 1.61340 ν10 = 44.27
rll = -17.9516 dll = 0.3
r12 = 6.165 d12 = 4.6295 n12 = 1.43875 ν12 = 94.93
r13 = −11.9356 d13 = 5.4028 n13 = 1.61340 ν13 = 44.27
r14 = 7.2511 d14 = 6.3314
r15 = -2.8819 d15 = 1.0602 n15 = 1.667790 ν15 = 55.34
r16 = −37.0589 d16 = 3.5724 n16 = 1.67300 ν16 = 38.15
r17 = −5.4988

(1) fl / f = 2.01
(2) f2 / f = 4.33
(3) f2 / f3 = −0.81
(4) | R3 / △ n | /f=4.52
(5) R21 / R22 = −0.85
(6) ν2 = 94.93
(7) β2 = -1.21

Example 2
FIG. 5 is a sectional view along the optical axis showing the optical configuration of Example 2, FIG. 6 is an aberration diagram when the cover glass thickness of Example 2 is 0.11 mm, (a) is spherical aberration, and (b) is Distortion aberration, (c) astigmatism, (d) coma aberration, FIG. 7 is an aberration diagram when the cover glass thickness of Example 2 is 0.17 mm, (a) spherical aberration, (b) Is a distortion aberration, (c) is an astigmatism, (d) is a coma aberration, FIG. 8 is an aberration diagram when the cover glass thickness of Example 2 is 0.23 mm, (a) is a spherical aberration, (b ) Shows distortion, (c) shows astigmatism, and (d) shows coma.

As shown in FIG. 5, the first lens group G1 is composed of two positive meniscus lenses having a concave surface facing the image side. The second lens group G2 is composed of a three-piece cemented lens including a biconvex lens, a biconcave lens, and a biconvex lens. The third lens group G3 includes a biconvex lens, a cemented lens of a negative meniscus lens having a concave surface directed toward the object side, a cemented meniscus lens of a biconvex lens and a biconcave lens, and a cemented meniscus lens of a biconcave lens and a biconvex lens.
Example 2 is an objective lens that has a magnification of 60 × and NA of 0.9, can be corrected within the range of high resolution and cover glass thickness of 0.11 to 0.23.

The lens data of Example 2 is shown below.
In Example 2, a normal cover glass is used, and the refractive index and Abbe number of the d line are designed as nd = 1.52100 and νd = 56.02, respectively.
NA = 0.9, WD = 0.33, β = −60, f = 3
rl = -3.8 dl = 4.682 nl = 1.77250 νl = 49.60
r2 = -4.106 d2 = 0.15
r3 = −35.9576 d3 = 2.7 n3 = 1.56907 ν3 = 71.30
r4 = −6.3898 d4 = 0.7
r5 = 7.849 d5 = 4.4379 n5 = 1.43875 ν5 = 94.93
r6 = −6.5489 d6 = 1.3 n6 = 1.77250 ν6 = 49.60
r7 = 11.8473 d7 = 4.8129 n7 = 1.43875 ν7 = 94.93
r8 = −7.1839 d8 = 1.451
r9 = 23.0308 d9 = 4.9104 n9 = 1.43875 ν9 = 94.93
rl0 = −5.3583 dl0 = 1.35 nl0 = 1.77250 νl0 = 49.60
rll = -18.757 dll = 7.3064
r12 = 5.2936 d12 = 3.4324 n12 = 1.49700 ν12 = 81.54
r13 = −12.1962 d13 = 3 n13 = 1.77250 ν13 = 49.60
r14 = 4.0802 d14 = 1.8814
r15 = -4.0492 d15 = 3.3341 n15 = 1.51633 ν15 = 64.14
r16 = 20.2444 d16 = 2.5 n16 = 1.67300 ν16 = 38.15
r17 = -8.0051

(1) fl / f = 1.78
(2) f2 / f = 7.52
(3) f2 / f3 = −0.65
(4) | R3 / △ n | / f = 5.36
(5) R21 / R22 = -1.09
(6) ν2 = 94.99
(7) β2 = -1.7

Examples 1 and 2 are infinity correction type objective lenses in which light emitted from the objective lens becomes a parallel light beam, and do not form an image by itself. Therefore, for example, it has the following numerical data and is used in combination with an imaging lens whose lens cross section is shown in FIG.
rl = 68.754 dl = 7.732 nl = 1.487 ν1 = 70.2
r2 = -37.567 d2 = 3.474 n2 = 1.806 ν2 = 40.9
r3 = -102.847 d3 = 0.697
r4 = 84.309 d4 = 6.023 n4 = 1.834 ν4 = 37.1
r5 = −50.710 d5 = 3.029 n5 = 1.644 ν5 = 40.8
r6 = 40.661

  In this case, the distance between the objective lens of Examples 1 and 2 and the imaging lens shown in FIG. 9 may be any position between 50 mm and 170 mm. FIGS. 2 to 4 and FIGS. 6 to 8 show aberration diagrams when the distance is 119 mm. In these aberration diagrams, IM. H represents the image height. It should be noted that substantially the same aberration situation is shown at positions other than 119 mm between the above-mentioned intervals of 50 mm to 170 mm.

1 is a cross-sectional view along an optical axis showing an optical configuration of Example 1. FIG. FIG. 6 is an aberration diagram when the cover glass thickness of Example 1 is 0 mm, where (a) shows spherical aberration, (b) shows distortion, (c) shows astigmatism, and (d) shows coma. FIG. 6 is an aberration diagram when the cover glass thickness of Example 1 is 1 mm, where (a) shows spherical aberration, (b) shows distortion, (c) shows astigmatism, and (d) shows coma. FIG. 4 is an aberration diagram when the cover glass thickness of Example 1 is 2 mm, where (a) shows spherical aberration, (b) shows distortion, (c) shows astigmatism, and (d) shows coma. 6 is a cross-sectional view along an optical axis showing an optical configuration of Example 2. FIG. FIG. 6 is an aberration diagram when the cover glass thickness of Example 2 is 0 mm, where (a) shows spherical aberration, (b) shows distortion, (c) shows astigmatism, and (d) shows coma. FIG. 6 is an aberration diagram when the cover glass thickness of Example 2 is 1 mm, where (a) shows spherical aberration, (b) shows distortion, (c) shows astigmatism, and (d) shows coma. FIG. 6 is an aberration diagram when the cover glass thickness of Example 2 is 2 mm, where (a) shows spherical aberration, (b) shows distortion, (c) shows astigmatism, and (d) shows coma. It is sectional drawing which follows the optical axis which shows the optical structure of the imaging lens used in combination with the objective lens of Example 1,2.

Explanation of symbols

G1 First lens group G2 Second lens group G3 Third lens group

Claims (4)

In order from the object side, a first lens unit having a positive refracting power including a positive meniscus lens component having a concave surface facing the object side and converting a light beam from the object into a weak divergent light beam and having a positive refractive power along the optical axis An objective lens for a microscope that includes a movable second lens group and a third lens group having a negative refractive power and satisfies the following conditional expression.
₁ <f 1 / f <3
3 <f ₂ / f <12
−0.9 <f ₂ / f ₃ <−0.6
Here, f ₁ is the focal length of the first lens group, f ₂ is the focal length of the second lens group, f ₃ is the focal length of the third lens group, and f is the focal length of the entire system. R _{3 is} the radius of curvature of at least one of the third lens group, Δn is the refractive index difference of the medium before and after the surface having the radius of curvature R _3, and the radius of curvature R of the surface closest to the object of the second lens group is _21. The microscope objective lens according to claim 1, wherein the following conditional expression is satisfied, where ₂₁ is the radius of curvature R ₂₂ of the surface closest to the image side of the second lens group.
1 <| R ₃ / Δn | / f <12
−1.3 <R ₂₁ / R ₂₂ <−0.5 3. The microscope objective lens according to claim 1, wherein the following conditional expression is satisfied when an Abbe number of a convex lens included in the second lens group is ν ₂ .
ν ₂ <70 4. The microscope objective lens according to claim 1, wherein the following conditional expression is satisfied, where β ₂ is a magnification of the second lens group. 5.
-1.8 <β ₂ <-1.1