Camera lens system

A camera lens system consists of first to third lens elements arranged in this order from the object side. The first lens element is a meniscus lens having a weak refractive power and concave toward the object side, the second lens element is a lens having a positive refractive power and the third lens element is a lens having a negative refractive power. A stop or an assumed stop is disposed close to the object side end of the lens system or on the object side of the same formula .nu..sub.3 .ltoreq.40 is satisfied wherein .nu..sub.3 represents the Abbe's number of the third lens element.

BACKGROUND OF THE INVENTION 
1. Field of the Invention 
This invention relates to a lens system consisting of three lens elements, 
and more particularly to a lens system which consists of three lens 
elements and is suitable for use as an image pick up lens system for a 
video camera or a still-video camera for a visual phone, a door phone, 
monitoring or the like. 
2. Description of the Prior Art 
Recently a solid state image pickup device has been in wide use in various 
video cameras or still-video cameras. The solid state image pickup device 
has been made smaller year by year and accordingly there has been a demand 
for miniaturization of the lens system and for reduction in cost of the 
lens system. 
In video cameras and still-video cameras, a low-pass filter for avoiding 
moire patterns, an infrared cut filter for correcting the spectral 
sensitivity of the solid state image pickup device and/or a cover glass 
for protecting the image surface of the image pickup device are generally 
disposed between the lens system and the solid state image pickup device. 
In such a case, the lens system should have a long back focal length in 
order to accommodate such optical elements. 
Recently there has been put into practice a solid state image pickup device 
in which a micro convex lens is disposed in front of each light receiving 
element of the solid state image pickup device in order to accumulate a 
light bundle travelling toward the dead zone of the element to the 
sensitive zone of the element, thereby increasing the sensitivity of the 
solid state image pickup device. When the light bundle entering such a 
solid state image pickup device largely inclines with respect to the 
optical axis of the micro lens, a so-called eclipse occurs at the aperture 
of the micro lens and a part of the incident light cannot reach the light 
receiving element. As a result, the brightness of the image becomes poor 
in the peripheral portion of the image and the peripheral portion of the 
image becomes dark. In order to avoid such a phenomenon, the incident 
angle of the incident light bundle to the solid state image pickup device 
should be as small as possible and it is necessary to position the exit 
pupil of the lens system as far from the image plane as possible. 
In our Japanese Patent Application No. 5(1993)-314649, there is disclosed a 
two-lens image pickup lens system for a video camera or a still-video 
camera. The lens system comprises a meniscus lens element having a 
negative refractive power and a lens element having a positive refractive 
power and satisfies a predetermined condition. This lens system is long in 
the back focal length, clear and relatively wide in the angle of view and 
at the same time is small in size. However in the lens system, the 
incident angle of the incident light bundle to the solid state image 
pickup device is large and an eclipse occurs at the aperture of the micro 
lens when this lens system is used with a solid state image pickup device 
with micro lenses. 
Further when the exit pupil of an image pickup lens system is positioned 
far from the image plane, correction of chromatic aberration becomes 
difficult. 
SUMMARY OF THE INVENTION 
In view of the foregoing observations and description, the primary object 
of the present invention is to provide a three-lens image pickup lens 
system which has a long back focal length, can be relatively large in 
angle of view, is clear, is small in size and at the same time is 
excellent in chromatic aberration. 
The lens system in accordance with the present invention comprises first to 
third lens elements arranged in this order from the object side. The first 
lens element is a meniscus lens having a weak refractive power and concave 
toward the object side, the second lens element is a lens having a 
positive refractive power and the third lens element is a lens having a 
negative refractive power. A stop or an assumed stop is disposed close to 
the object side end of the lens system or on the object side of the same. 
Formula .nu..sub.3 .ltoreq.40 is satisfied wherein .nu..sub.3 represents 
the Abbe's number of the third lens element. 
In the lens system of the present invention, since the stop or the assumed 
stop is disposed close to the object side end of the lens system or on the 
object side of the same, the exit pupil of the lens system can be 
positioned far from the image plane and the incident angle of the incident 
light bundle to the solid state image pickup device can be small, whereby 
any eclipse in a solid state image pickup device with micro lenses can be 
prevented and shortage of the amount of light in the peripheral portion of 
the image can be prevented. 
Further since the first lens is a meniscus lens having a weak refractive 
power and concave toward the object side, the principal point on the image 
plane side is kept far from the object and accordingly the back focal 
length of the lens system can be long. The concave face of the first lens 
facing toward the object erects the image plane which is inclined under by 
the second lens element which is a convex lens. Though the distortion of 
the lens system becomes under due to the concave face of the first lens 
element, it practically gives rise to no problem when the half angle of 
view is about 29.degree.. 
The above formula limits the value of the Abbe's number of the third lens. 
That is, when the Abbe's number of the third lens is not larger than 40, 
longitudinal chromatic aberration, which is apt to become large when the 
exit pupil of the lens system is positioned far from the image plane, can 
be suppressed.

DESCRIPTION OF THE PREFERRED EMBODIMENTS 
As shown in FIG. 1, each of the lens systems in accordance with the first 
and second embodiments of the present invention comprises first third lens 
elements L.sub.1 to L.sub.3 arranged in this order from the object side. A 
low-pass filter 2 is disposed between the third lens element L.sub.3 and a 
solid state image pickup device 1. A stop i is disposed close to the 
object side end of the first lens element L.sub.1 or on the object side of 
the same. Light entering the taking lens system along the optical axis X 
is focused on an imaging position P of the solid state image pickup device 
1. 
The first lens element L.sub.1 is a meniscus lens having a weak refractive 
power and concave toward the object side. The second lens element L.sub.2 
is a double-convex lens having a positive refractive power and is 
positioned so that its face of greater curvature is faced toward the image 
plane. The third lens element L.sub.3 is a meniscus lens having a negative 
refractive power and concave toward the object side. 
In the first and second embodiments, the second and third lens elements 52 
and L.sub.3 are cemented together. 
As shown in FIG. 2, the lens system of the third embodiment is 
substantially the same as those of the first and second embodiments in the 
arrangement of the lens elements except that the second and third lens 
elements L.sub.2 and L.sub.3 are spaced from each other. 
Each of the lens systems satisfies the formula .nu..sub.3 .ltoreq.40 
wherein .nu..sub.3 represents the Abbe's number of the third lens element. 
The radii of curvature R(mm) of the refracting surfaces, the axial surface 
separations d (mm) (the central thicknesses of the lenses or the air 
separations), the refractive indexes n for the e-line of the lenses and 
the Abbe's numbers .nu. of the lenses of the lens systems in accordance 
with the first to third embodiments are as shown in tables 1 to 3, 
respectively. In tables 1 and 2, the radii of curvature of the refracting 
surfaces, the axial surface separations, the refractive indexes for the 
e-line and the Abbe's numbers of the lenses are designated in order from 
the object side at R.sub.1 to R.sub.7, d.sub.1 to d.sub.6, n.sub.1 to 
n.sub.4 and .nu..sub.1 to .nu..sub.4. In table 3, the radii of curvature 
of the refracting surfaces, the axial surface separations, the refractive 
indexes for the e-line and the Abbe's numbers of the lenses are designated 
in order from the object side at R.sub.1 to R.sub.8, d.sub.1 to d.sub.7 , 
n.sub.1 to n.sub.4 and .nu..sub.1 to .nu..sub.4. 
TABLE 1 
______________________________________ 
radius of axial surface 
refracting Abbe's 
curvature R 
separation d index n number .nu. 
______________________________________ 
R.sub.1 = -2.727 
d.sub.1 = 1.25 
n.sub.1 = 1.80831 
.nu..sub.1 = 46.5 
R.sub.2 = -3.295 
d.sub.2 = 0.10 
R.sub.3 = 11.103 
d.sub.3 = 2.83 
n.sub.2 = 1.77621 
.nu..sub.2 = 49.6 
R.sub.4 = -3.200 
d.sub.4 = 0.55 
n.sub.3 = 1.85505 
.nu..sub.3 = 23.8 
R.sub.5 = -8.876 
d.sub.5 = 2.30 
R.sub.6 = .infin. 
d.sub.6 = 4.30 
n.sub.4 = 1.51824 
.nu..sub.4 = 64.0 
R.sub.7 = .infin. 
______________________________________ 
In the first embodiment, the focal length f of the overall lens system is 
6.31 mm, the back focal length is 6.66 mm and d.sub.1 /f is 0.20, d.sub.1 
representing the central thickness of the first lens element L.sub.1. 
Further the F number and the half angle of view .omega. are 2.8 and 
28.2.degree., respectively. The stop i is at a distance of 1.57 mm from 
the object side face of the first lens element L.sub.1 toward the object 
and the exit pupil is at a distance of 17.6 mm from the imaging position P 
toward the object. 
TABLE 2 
______________________________________ 
radius of axial surface 
refracting Abbe's 
curvature R separation d 
index n number .nu. 
______________________________________ 
R.sub.1 = -4.277 
d.sub.1 = 5.00 
n.sub.1 = 1.80831 
.nu..sub.1 = 46.5 
R.sub.2 = -6.550 
d.sub.2 = 0.10 
R.sub.3 = 9.236 
d.sub.3 = 2.83 
n.sub.2 = 1.77621 
.nu..sub.2 = 49.6 
R.sub.4 = -4.001 
d.sub.4 = 0.55 
n.sub.3 = 1.85505 
.nu..sub.3 = 23.8 
R.sub.5 = -18.805 
d.sub.5 = 3.80 
R.sub.6 = .infin. 
d.sub.6 = 4.30 
n.sub.4 = 1.51824 
.nu..sub.4 = 64.0 
R.sub.7 = .infin. 
______________________________________ 
In the second embodiment, the focal length f of the overall lens system is 
6.27 mm, the back focal length is 8.17 mm and d.sub.1 /f is 0.8, d.sub.1 
representing the central thickness of the first lens element L.sub.1. 
Further the F number and the half angle of view .omega. are 2.8 and 
29.5.degree., respectively. The stop i is at a distance of 0.1 mm from the 
object side face of the first lens element L.sub.1 toward the image plane 
and the exit pupil is at a distance of 18.4 mm from the imaging position P 
toward the object. 
TABLE 3 
______________________________________ 
radius of axial surface 
refracting Abbe's 
curvature R separation d 
index n number .nu. 
______________________________________ 
R.sub.1 = -6.490 
d.sub.1 = 9.7 
n.sub.1 = 1.80831 
.nu..sub.1 = 46.5 
R.sub.2 = -11.109 
d.sub.2 = 0.1 
R.sub.3 = 9.024 
d.sub.3 = 3.6 
n.sub.2 = 1.77621 
.nu..sub.2 = 49.6 
R.sub.4 = -4.491 
d.sub.4 = 0.005 
R.sub.5 = -4.489 
d.sub.5 = 0.55 
n.sub.3 = 1.85505 
.nu..sub.3 = 23.8 
R.sub.6 = -15.944 
d.sub.6 = 4.30 
R.sub.7 = .infin. 
d.sub.7 = 4.30 
n.sub.4 = 1.51824 
.nu..sub.4 = 64.0 
R.sub.8 = .infin. 
______________________________________ 
In the third embodiment, the focal length f of the overall lens system is 
6.26 mm, the back focal length is 8.66 mm and d.sub.1 /f is 1.55, d.sub.1 
representing the central thickness of the first lens element L.sub.1. 
Further the F number and the half angle of view .omega. are 2.8.degree. 
and 30.5.degree., respectively. The stop i is at a distance of 1.48 mm 
from the object side face of the first lens element L.sub.1 toward the 
image plane and the exit pupil is at a distance of 22.5 mm from the 
imaging position P toward the object. 
FIGS. 3A to 3G, FIGS. 4A to 4G and FIGS. 5A to 5G respectively show various 
aberrations of the lens systems of the first to third embodiments. 
As can be understood from FIGS. 3A to 3G, FIGS. 4A to 4G and FIGS. 5A to 
5G, the lens system of each embodiment is excellent in aberrations. 
In the lens system of each embodiment, the exit pupil is relatively far 
from the image plane and since the Abbe's number of the third lens element 
L.sub.3 is not larger than 40, the longitudinal chromatic aberration can 
be made small. Further, the lens system of each embodiment has a long back 
focal length and a wide half angle of view .omega. (as wide as about 
29.degree.) and is clear (F number is 2.8). At the same time, the lens 
system of each embodiment is small in size and can be manufactured at low 
cost. 
The arrangement of the lens system in accordance with the present invention 
need not be limited to those described above in conjunction with the first 
to third embodiments, but the radius of curvature of each lens element, 
the axial surface separations (including the thickness of the lens 
elements) and the like may be variously modified without departing from 
the spirit and scope of the invention. 
For example, the second lens element L.sub.2 may be a meniscus lens having 
a positive refractive power and the third lens element L.sub.3 may be a 
double-concave lens (see FIG. 6). 
Instead of the low-pass filter employed in the embodiments described above 
or in addition to the low-pass filter, an infrared cut filter and/or a 
cover glass may be inserted between the lens system and the solid state 
image pickup device. 
As can be understood from the description above, in the lens system of the 
present invention, the incident angle of the incident light bundle to the 
solid state image pickup device can be small and the longitudinal 
chromatic aberration can be excellent. Further the lens system of the 
present invention is long in the back focal length, relatively wide in the 
half angle of view, clear and small in size and can be manufactured at low 
cost. Accordingly, the lens system of the present invention is suitable as 
the image pick up lens for various video cameras and still-video cameras.