US 20010036022 A1 Abstract A Gaussian lens having no more than six lens elements of refractive power is formed of, in order from the object side: a first lens element which is biconvex, a second lens element which is a positive meniscus lens with its convex surface on the object side, a third lens element which is biconcave, a stop, a joined lens formed of a fourth lens element which is biconcave that is joined to a fifth lens element which is biconvex; and a sixth lens element having positive refractive power. Specified conditions are satisfied in order to provide a compact lens having an f-number F
_{NO }of 1.44 or less, an image angle 2ω of 23.8 degrees or more, and wherein the various aberrations are favorably corrected. The Gaussian lens of the invention is intended for mounting in monitor cameras. Claims(10) 1. A Gaussian lens having no more than six lens elements of refractive power comprising, in order from the object side:
a first lens element which is biconvex; a second lens element which is a positive meniscus lens with its convex surface on the object side; a third lens element which is biconcave; a stop; a joined lens consisting of a fourth lens element which is biconcave and joined to a fifth lens element which is biconvex; and a sixth lens element having positive refractive power. 2. The Gaussian lens of claim 1 4.0
<f _{1} /f _{2}<8.0 1.75<(N _{5} +N _{6})/2 12.0<(ν_{5}−ν^{4}) 1.00<(R _{5} −R _{4})/(R _{5} +R _{4})<6.10 0.37<R _{6} /f<0.50 0.50<|R _{8} |/f<100 where
f
_{1 }is the resultant focal length of the lens elements located on the object-side of the stop, f
_{2 }is the resultant focal length of the lens elements located on the image-side of the stop, N
_{5 }is the index of refraction of the fifth lens element, N
_{6 }is the index of refraction of the sixth lens element, ν
_{5 }is the Abbe number of fifth lens element, ν
_{4 }is the Abbe number of fourth lens element, R
_{5 }is the radius of curvature of the object-side surface of the third lens element, R
_{4 }is the radius of curvature of the image-side surface of the second lens element, R
_{6}is the radius of curvature of the image-side surface of the third lens element, f is the focal length of the Gaussian lens, and
R
_{8 }is the radius of curvature of the image-side surface of the fourth lens element. 3. The Gaussian lens of claim 2 0.11
<f/R _{12 } where
R
_{12 }is the radius of curvature of the image-side surface of the sixth lens element. 4. The Gaussian lens of claim 1 4.0
<f _{1} /f _{2}<8.0 where
f
_{1 }is the resultant focal length of the lens elements located on the object-side of the stop; and f
_{2 }is the resultant focal length of the lens elements located on the image-side of the stop. 5. The Gaussian lens of claim 1 1.75<(
N _{5} +N _{6})/2 where
N
_{5 }is the index of refraction of the fifth lens element, and N
_{6 }is the index of refraction of the sixth lens element. 6. The Gaussian lens of claim 1 12.0<(ν
_{5}−ν_{4}) where
ν
_{5 }is the Abbe number of fifth lens element, and ν
_{4 }is the Abbe number of fourth lens element. 7. The Gaussian lens of claim 1 1.00<(
R _{5} −R _{4})(R _{5} +R _{4})<6.10 where
R
_{5 }is the radius of curvature of the object-side surface of the third lens element, and R
_{4 }is the radius of curvature of the image-side surface of the second lens element. 8. The Gaussian lens of claim 1 0.37
<R _{6} /f<0.50 where
R
_{6 }is the radius of curvature of the image-side surface of the third lens element, and f is the focal length of the Gaussian lens.
9. The Gaussian lens of claim 1 0.50
<|R _{8} |/f<1.00 where
R
_{8 }is the radius of curvature of the image-side surface of the fourth lens element, and f is the focal length of the Gaussian lens.
10. The Gaussian lens of claim 1 −0.11
<f/R _{12 } where
f is the focal length of the Gaussian lens, and
R
_{12 }is the radius of curvature of the image-side surface of the sixth lens element.Description [0001] Gaussian lenses are known for photographic use, in that they have a sufficiently long back focal length and provide excellent optical performance. Their typical structure is described in Japanese Patent Publication No. S62-87922 and Japanese Laid Open Patent Application No. H8-160293. Recently there has been an increased demand for monitor cameras that have a low F [0002] There have been attempts to use the Gaussian lens systems disclosed in the publications mentioned above in monitor cameras. However, the Gaussian lens system described in Japanese Patent Publication No. S62-87922 does not have its aberrations sufficiently corrected and it does not provide a sufficiently bright image, in that its F [0003] The object of the present invention is to provide a compact Gaussian lens having an F [0004] The present invention will become more fully understood from the detailed description given below and the accompanying drawings, which are given by way of illustration only and thus are not limitative of the present invention, wherein: [0005]FIG. 1 shows the basic lens element configuration of Embodiments 1 and 2 of the present invention, and is also representative of Embodiments 3 and 4 of the invention except for the sign of the radius of curvature of the image side of the sixth lens element, in order from the object side; [0006] FIGS. [0007] FIGS. [0008] FIGS. [0009] FIGS. [0010]FIG. 1 shows the basic lens element configuration of Embodiments 1-2 of the present invention, and is also representative of Embodiments 3 and 4 of the invention except for the sign of the radius of curvature of the image-side of the sixth lens element. The Gaussian lens according to the present invention is formed of, in order from the object side, a first lens element L 4.0 1.75<( 12.0<(ν 1.00<( 0.37 0.50 [0011] where [0012] f [0013] f [0014] N [0015] N [0016] ν [0017] ν [0018] R [0019] R [0020] R [0021] f is the focal length of the Gaussian lens; and [0022] R [0023] In addition, it is preferred that the following Condition (7) also is satisfied: −0.11< [0024] where [0025] f is as defined above, and [0026] R [0027] The Gaussian lens according to the present invention ensures a bright image in that the F [0028] The purposes of the above Conditions will now be discussed. Condition (1) ensures proper power distribution among the lens elements positioned on both sides of the stop in order to realize a large aperture. Exceeding the upper limit results in reducing the refractive power of the front lens group (i.e., the first to third lens elements, in order from the object side). This is advantageous for maintaining a sufficient back focal length. However, the relatively increased negative power of the third lens element excessively corrects spherical aberration. Not satisfying the lower limit makes it difficult to obtain a sufficiently large back focal length. [0029] Condition (2) defines the refractive power of the positive lens elements that form the rear lens group (i.e., the fifth and sixth lens elements of among the fourth through sixth lens elements). Failure to satisfy the lower limit means that each lens element has a small radius of curvature, which causes the Petzval sum to increase. Spherical aberration will be insufficiently corrected, so that a large aperture will not be possible without reduced optical performance. [0030] Condition (3) defines the Abbe numbers of the fourth and fifth lens elements which form a joined lens component. Failure to satisfy the lower limit reduces the corrective effect on chromatic aberration. [0031] Condition (4) defines the refractive power of the air lens located between the second and third lens elements. Exceeding the upper limit enhances the divergent power of the air lens so that spherical aberration will be excessively corrected. On the other hand, not satisfying the lower limit causes coma to increase. [0032] Conditions (5) and (6) determine the profile of the two concave surfaces located on either side of the stop. Exceeding the upper limit leads to insufficiently corrected spherical aberration and an increase in the Petzval sum. On the other hand, not satisfying the lower limit results in increased coma. [0033] Condition (7) determines the refractive power of the convex surface on the image-side of the sixth lens element in order to ensure a proper back focal length. Failure to satisfy Condition (7) makes it difficult to obtain a sufficiently large back focal length. [0034] Several embodiments of the invention will now be described in detail. [0035] The Gaussian lens of Embodiment 1 is formed of a first lens element L [0036] Table 1 below lists the surface number #, in order from the object side, the radius of curvature R (in mm) of the surface, the on-axis spacing D (in mm) between surfaces, as well as the index of refraction N
[0037] As is shown in the middle portion of Table 1, the focal length f of the Gaussian lens is 25.78 mm, the f-number F [0038] FIGS. [0039] The Gaussian lens of Embodiment 2 has the same basic lens element configuration as that of Embodiment 1. [0040] Table 2 below lists the surface number #, in order from the object side, the radius of curvature R (in mm) of the surface, the on-axis spacing D (in mm) between surfaces, as well as the index of refraction N
[0041] As is shown in the middle portion of Table 2, the focal length f of the Gaussian lens is 26.90 mm, the f-number F [0042] FIGS. [0043] The Gaussian lens of this embodiment has nearly the same basic lens element configuration as that of Embodiments 1 and 2 except, in this embodiment, the sixth lens element L [0044] Table 3 below lists the surface number #, in order from the object side, the radius of curvature R (in mm) of the surface, the on-axis spacing D (in mm) between surfaces, as well as the index of refraction N
[0045] As is shown in the middle portion of Table 3, the focal length f of the Gaussian lens is 25.78 mm, the f-number F [0046] FIGS. [0047] The Gaussian lens of Embodiment 4 has the same basic lens element configuration as that of Embodiment 3. [0048] Table 4 below lists the surface number #, in order from the object side, the radius of curvature R (in mm) of the surface, the on-axis spacing D (in mm) between surfaces, as well as the index of refraction N
[0049] As shown in the middle portion of Table 4, the focal length f of the Gaussian lens is 26.62 mm, the f-number F [0050] FIGS. [0051] The invention being thus described, it will be obvious that the same may be varied in many ways. For example, the radii of curvature R and spacings D may be readily scaled so as to provide a Gaussian lens of a desired focal length. A cover glass can be inserted between the Gaussian lens and the image surface (i.e., the location of the solid-state detector array). Also, a a filter member 2, which may include a low pass filter and/or an infrared cut filter, may be inserted between the Gaussian lens and the image surface. Such variations are not to be regarded as a departure from the spirit and scope of the invention. Rather the scope of the invention shall be defined as set forth in the following claims and their legal equivalents. All such modifications as would be obvious to one skilled in the art are intended to be included within the scope of the following claims. Referenced by
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