Information
-
Patent Grant
-
6301056
-
Patent Number
6,301,056
-
Date Filed
Monday, November 8, 199925 years ago
-
Date Issued
Tuesday, October 9, 200123 years ago
-
Inventors
-
Original Assignees
-
Examiners
Agents
-
CPC
-
US Classifications
Field of Search
US
- 359 648
- 359 753
- 359 782
- 359 784
- 359 715
- 359 716
- 348 776
- 348 778
- 348 779
- 348 781
-
International Classifications
-
Abstract
Projection lens systems (13) for use in CRT projection televisions (10) are provided. From the screen side, the systems have three lens units (U1, U2, U3), the first two units (U1, U2) forming a retrofocus lens and the third unit (U3) being associated with the CRT during use and serving to correct field curvature. At its screen end, the first lens unit (U1) has a negative element (E1) which has a screen surface (S1) which is concave to the screen. The second lens unit (U2) has two positive subunits (US1, US2), the first subunit (US1) being a color correcting doublet composed of glass and the second subunit having a positive lens element (E2) at its screen end. The projection lens systems are fully color corrected, have f/#'s of 1.0 for an infinite conjugate, have half fields of view of at least 25°, and are economical to manufacture.
Description
FIELD OF THE INVENTION
This invention relates to projection lens systems for use in projection televisions.
BACKGROUND OF THE INVENTION
There exists a need in the art for a projection lens system and, in particular, a rear projection lens system, that has some and preferably all of the following properties:
(1) The system is fully color corrected.
(2) The system is a high speed system, e.g., it has an infinite conjugate f/# of 1.0.
(3) The system has a wide field of view in the direction of the screen, e.g., a half field of view in the direction of the screen of at least 25°.
(4) The system produces a high quality image, e.g., the system has an MTF above 0.5 at 10 cycles/millimeter.
(5) The quality of the image is insensitive to changes in temperature of the lens system, e.g., changes between room temperature and the system's operating temperature.
(6) The system produces an image which is bright in the corners, e.g., the pupil area in the corner is at least 50% of the pupil area on axis.
(7) The system is compact, i.e., its lens elements are spaced close together so that the overall system has a short barrel length.
(8) The system is suitable for use with small diameter cathode ray tubes (CRTs), e.g., it can be used with 3-inch CRTs which have a diagonal of about 65 millimeters.
(9) The system is economical to manufacture.
SUMMARY OF THE INVENTION
To satisfy this need in the art, it is an object of the invention to provide projection lens systems which have some and preferably all of the above nine features.
To achieve this object, the invention provides a projection lens system for use in combination with a cathode ray tube that comprises the following lens units in order from the image (i.e., screen or long conjugate) side:
(a) a negative first lens unit (U
1
) which comprises: (i) at least one aspheric surface and (ii) a negative lens element (E
1
) at the unit's image side, said negative lens element having an image side surface (S
1
) which is concave towards the image;
(b) a positive second lens unit (U
2
) which comprises the following lens subunits in order from the image side:
(i) a positive first lens subunit (U
S2
) which consists of a cemented color correcting doublet composed of glass and having spherical surfaces; and
(ii) a positive second lens subunit (U
S2
) which comprises at least one lens element of weak optical power having at least one aspheric surface; and
(c) a third lens unit (U
3
) which has a strong negative power, is associated with the CRT during use of the lens system, and contributes to the correction of the lens system's field curvature.
Compared to the typical CRT projection lens, the U
3
unit has reduced negative power, i.e., the ratio of the magnitude of the power of the U
3
unit to the overall power of the lens system is relatively small, e.g., less than 0.8 and preferably less than 0.7. This reduction is accomplished through the use of concave surface S
1
on lens element E
1
which helps correct the field curvature of the lens. As a result, the magnitude of the power of the negative third lens unit (U
3
) can be reduced. This reduction in power allows the lens to collect more light from the CRT, especially from the corners of the CRT.
The first and second lens units (U
1
and U
2
) have a retrofocus, i.e., a negative-positive, configuration. This configuration allows the combination of these units to have a short focal length and a back focal length which is sufficiently long to accommodate the third lens unit at the CRT faceplate.
In certain preferred embodiments of the invention, all of the lens elements of U
1
, U
S2
, and U
3
are composed of plastic. Thus, for these embodiments, the projection lens system is composed of a cemented glass doublet and plastic lens elements on either side of the doublet. This configuration provides a number of advantages to the lens system.
First, it makes the system inexpensive to manufacture. As illustrated in the examples presented below, the plastic elements of the lens have configurations which allow them to be readily molded in plastic. As also illustrated in the examples, the doublet has spherical surfaces and a relatively small clear aperture diameter (e.g., a clear aperture diameter of less than 65 millimeters and preferably less than 60 millimeters) which allows it to be readily made in glass. Accordingly, each of the components of the system can be readily manufactured at low cost.
Second, the most critical portion of the lens in terms of its optical performance is the second lens unit's first subunit (U
S1
), i.e., the cemented glass doublet. Because of its size and configuration, this doublet can be made with high precision, again at low cost. Accordingly, the use of this doublet provides an effective way to achieve a high level of optical performance in an inexpensive lens.
Third, the plastic-glass-plastic construction of the lenses of the invention, with the glass portion being of strong power, makes the lenses insensitive to changes in temperature. Again, this thermal stability is achieved for a lens that has both a high level of optical performance and a low cost.
In other preferred embodiments, the lens system has some or all of the following characteristics:
(1) to provide a high level of aberration correction, U
1
and U
S2
each have two aspheric surfaces;
(2) again to provide a high level of aberration correction, surface S
1
is an aspheric surface;
(3) to aid in the correction of field curvature, |Φ
E1
|/Φ
0
is at least 0.15, preferably at least 0.2, and most preferably at least 0.25, where |Φ
E1
| is the magnitude of the power of element E
1
and Φ
0
is the overall power of the lens system;
(4) to provide the foregoing power level without unduly increasing the curvature of the S
1
surface, E
1
is preferably biconcave;
(5) to provide a compact lens, D
12
/f
0
(or, equivalently, D
12
·Φ
0
) is less than or equal to 0.25, where D
12
is the distance between the object side surface of E
1
and the image side surface of U
S1
and f
0
is the effective focal length of the lens system (f
0
=1/Φ
0
); and
(6) to aid in thermal compensation, U
S1
is a strong lens unit and the image side lens element (E
2
) of U
S2
has a positive power.
When the above preferred embodiments of the invention are used in combination, each of the nine desired features for a CRT projection lens system, listed above, are achieved by the projection lens systems of the invention.
As used herein, the term “weak” is used to describe an element or unit whose focal length has a magnitude which is at least about 2.5 times the effective focal length of the entire lens system, and the term “strong” is used to describe an element or unit whose focal length has a magnitude which is less than about 2.5 times the effective focal length of the entire lens system. Also, the effective focal length and power of the entire lens system, as well as the effective focal length and power of the third lens unit (Φ
U3
), are determined for the lens system associated with the CRT.
BRIEF DESCRIPTION OF THE DRAWINGS
FIGS. 1-4
are schematic side views of lens systems constructed in accordance with the invention.
FIG. 5
is a schematic diagram of a projection TV employing a lens system constructed in accordance with the invention.
The foregoing drawings, which are incorporated in and constitute part of the specification, illustrate the preferred embodiments of the invention, and together with the description, serve to explain the principles of the invention. It is to be understood, of course, that both the drawings and the description are explanatory only and are not restrictive of the invention.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
FIGS. 1-4
illustrate various projection lenses constructed in accordance with the invention. Corresponding prescriptions appear in Tables 1-4. HOYA or SCHOTT designations are used for the glasses employed in the lens systems. Equivalent glasses made by other manufacturers can be used in the practice of the invention. Industry acceptable materials are used for the plastic elements.
The aspheric coefficients set forth in the tables are for use in the following equation:
where z is the surface sag at a distance y from the optical axis of the system, c is the curvature of the lens at the optical axis, and k is a conic constant, which is zero except where indicated in the prescriptions of Tables 1-4.
The abbreviations used in the tables are as follows:
|
EFL
effective focal length
|
FVD
front vertex distance
|
f/
f-number (finite conjugates)
|
ENP
entrance pupil as seen from the long conjugate
|
EXP
exit pupil as seen from the long conjugate
|
BRL
barrel length
|
OBJ HT
object height
|
MAG
magnification
|
STOP
location of aperture stop
|
IMD
image distance
|
OBD
object distance
|
OVL
overall length.
|
|
The designation “a” associated with various surfaces in the tables represents an aspheric surface, i.e., a surface for which at least one of D, E, F, G, H, or I in the above equation is not zero. The designation “c” represents a conic surface, i.e., a surface for which k in the above equation is not zero. The tables are constructed on the assumption that light travels from left to right in the figures. In actual practice, the viewing screen will be on the left and the CRT will be on the right, and light will travel from right to left. The designation “AS” is used in the figures to identify the lens system's aperture stop.
The CRT faceplate constitutes surfaces
15
-
16
in Tables 1 and 3, surfaces
13
-
14
in Table 2, and surfaces
17
-
18
in Table 4. A coupling fluid is located between surfaces
14
-
15
in Tables 1 and 3, surfaces
12
-
13
in Table 2, and surfaces
16
-
17
in Table 4. The material designation for the coupling fluid is set forth as a six digit number in the tables, where an Ne value for the material is obtained by adding 1,000 to the first three digits of the designation, and a Ve value is obtained from the last three digits by placing a decimal point before the last digit. All dimensions given in the prescription tables are in millimeters.
Table 5 summarizes the |Φ
E1
|/Φ
0
and D
12
/f
0
values of the projection lens systems of Tables 1-4. (D
12
×Φ
0
=D
12
/f
0
) As shown in this table, the lens systems of the examples satisfy the preferred values for these parameters set forth above. The infinite conjugate f/# for each of the projection lens systems of Tables 1-is 1.0 and the ratio of the magnitude of the power of the third lens unit (|Φ
U3
|)to Φ
0
is less than 0.8. Each of these lens systems is fully color corrected, thermally stable, has a half field of view in the direction of the screen of 27.5°, has an MTF above 0.5 at 10 cycles/millimeter, and produces an image whose pupil area in the corner is at least 50% of the pupil area on axis.
FIG. 5
is a schematic diagram of a CRT projection television
10
constructed in accordance with the invention. As shown in this figure, projection television
10
includes cabinet
12
having projection screen
14
along its front face and slanted mirror
18
along its back face. Module
13
schematically illustrates a lens system constructed in accordance with the invention and module
16
illustrates its associated CRT tube. In practice, three lens systems
13
and three CRT tubes
16
are used to project red, green, and blue images onto screen
14
.
Although specific embodiments of the invention have been described and illustrated, it is to be understood that a variety of modifications which do not depart from the scope and spirit of the invention will be evident to persons of ordinary skill in the art from the foregoing disclosure.
TABLE 1
|
|
Clear
|
Surf.
Aperture
|
No.
Type
Radius
Thickness
Glass
Diameter
|
|
1
ac
−108.1464
5.47000
ACRYLIC
51.54
|
2
286.6604
3.00000
47.00
|
3
a
−500.0000
6.41000
ACRYLIC
47.00
|
4
−183.8764
0.52000
49.89
|
5
71.5889
4.56000
FD10
55.12
|
6
38.0824
25.08000
SK18A
55.02
|
7
−55.0481
0.46000
55.67
|
8
Aperture stop
0.00000
50.41
|
9
a
32.3351
9.53000
ACRYLIC
48.18
|
10
61.7951
1.57000
46.15
|
11
a
500.0000
5.12000
ACRYLIC
45.11
|
12
a
490.0000
21.73000
42.28
|
13
a
−28.7710
2.70000
ACRYLIC
40.14
|
14
−24.6181
8.00000
402500
42.81
|
15
∞
2.00000
FDS9
63.00
|
16
∞
0.00222
66.00
|
|
Symbol Description
|
a - Polynomial asphere
|
c - Conic section
|
Even Polynomial Aspheres and Conic Constants
|
Surf.
|
No.
k
D
E
F
|
|
1
−4.3933E+00
−7.7139E−06
4.9036E−09
4.9665E−12
|
3
2.4262E−06
−8.3820E−09
−2.9667E−12
|
9
−1.8765E−06
1.5225E−09
−1.5045E−11
|
11
2.0474E−05
1.3320E−08
−2.9386E−11
|
12
2.4486E−05
1.9039E−09
3.7648E−11
|
13
−3.3649E−05
1.9291E−07
−1.1779E−09
|
|
Surf.
|
No.
G
H
I
|
|
1
−9.4186E−15
5.2747E−18
1.8607E−22
|
3
2.5026E−15
4.5121E−18
−1.0186E−20
|
9
2.3625E−14
1.5823E−17
−1.7883E−20
|
11
7.0801E−14
−9.3044E−17
−6.5831E−20
|
12
−9.6804E−14
4.6983E−16
−1.0605E−18
|
13
3.8267E−12
−6.4691E−15
3.8064E−18
|
|
System First Order Properties
|
OBJ. HT: −610.00 f/ 1.07 MAG: −0.0526
|
STOP: 0.00 after surface 8. DIA: 50.410
|
EFL: 44.9043
FVD: 96.1522
ENP: 28.2256
|
IMD: 0.221537E−02
BRL: 96.1500
EXP: −31.6619
|
OBD: −894.169
OVL: 990.321
|
|
First Order Properties of Elements
|
Element
Surface
|
Number
Numbers
Power
f′
|
|
1
1
2
−0.63171E−02
−158.30
|
2
3
4
0.17092E−02
585.07
|
3
5
6
−0.85049E−02
−117.58
|
4
6
7
0.25491E−01
39.229
|
5
9
10
0.80585E−02
124.09
|
6
11
12
−0.16743E−04
−59726.
|
7
13
14
0.35173E−02
284.31
|
8
14
15
−0.16329E−01
−61.239
|
|
First-Order Properties of Doublets
|
Element
Surface
|
Numbers
Numbers
Power
f′
|
|
3
4
5
7
0.17813E−01
56.139
|
|
TABLE 2
|
|
Clear
|
Surf.
Aperture
|
No.
Type
Radius
Thickness
Glass
Diameter
|
|
1
ac
−188.4224
5.47069
ACRYLIC
48.84
|
2
a
573.1565
5.11766
47.94
|
3
72.3919
4.5589
FD11
54.09
|
4
48.9493
22.41794
SK18A
54.40
|
5
−49.9518
0.45589
55.39
|
6
Aperture stop
0.00000
49.49
|
7
a
37.5739
8.57922
ACRYLIC
45.74
|
8
82.9018
1.57044
43.00
|
9
a
603.4897
6.37276
ACRYLIC
43.22
|
10
a
799.6455
19.55170
39.97
|
11
a
−24.7210
2.70000
ACRYLIC
38.94
|
12
∞
−24.6181
8.00000
402500
42.06
|
13
∞
2.00000
FDS9
62.00
|
14
0.00531
66.00
|
Symbol Description
|
a - Polynomial asphere
|
c - Conic section
|
Even Polynomial Aspheres and Conic Constants
|
Surf.
|
No.
k
D
E
F
|
|
1
−4.3933E+00
−1.0207E−05
5.5020E−09
1.2768E−11
|
2
−4.1831E−06
1.1504E−08
1.0166E−11
|
7
−4.4696E−07
6.7055E−09
−1.7111E−11
|
9
1.1408E−05
9.3445E−09
−1.4071E−11
|
10
1.6041E−05
−6.7617E−09
3.8184E−11
|
11
−2.3158E−05
1.3009E−07
−1.0145E−09
|
|
Surf.
|
No.
G
H
I
|
|
1
−1.2666E−14
−1.6314E−17
1.6179E−20
|
2
1.2060E−15
−3.7885E−17
2.7498E−20
|
7
8.4366E−15
2.3469E−17
2.3603E−21
|
9
5.9708E−14
−4.9726E−17
−1.3740E−19
|
10
9.6888E−15
3.0196E−16
−1.1045E−18
|
11
3.9497E−12
−7.0758E−15
3.9721E−18
|
|
System First Order Properties
|
OBJ. HT: −610.00 f/ 1.07 MAG: −0.0526
|
STOP: 0.00 after surface 6. DIA: 49.488
|
EFL: 44.9038
FVD: 86.8005
ENP: 25.8876
|
IMD: 0.531171E−02
BRL: 86.7952
EXP: −29.4690
|
OBD: −901.821
OVL: 988.621
|
First Order Properties of Elements
|
Element
Surface
|
Number
Numbers
Power
f′
|
|
1
1
2
−0.34904E−02
−286.50
|
2
3
4
−0.47887E−02
−208.82
|
3
4
5
0.23642E−01
42.298
|
4
7
8
0.76349E−02
130.98
|
5
9
10
0.20286E−03
4929.4
|
6
11
12
0.80760E−03
1238.2
|
7
12
13
−0.16329E−01
−61.239
|
|
First-Order Properties of Doublets
|
Element
Surface
|
Numbers
Numbers
Power
f′
|
|
2
3
3
5
0.19035E−01
52.536
|
|
TABLE 3
|
|
Clear
|
Surf.
Aperture
|
No.
Type
Radius
Thickness
Glass
Diameter
|
|
1
ac
−127.7240
5.40000
ACRYLIC
54.64
|
2
a
276.8658
2.34190
53.05
|
3
136.8248
4.20000
FD6
53.91
|
4
61.3922
21.06709
SK18A
55.29
|
5
−50.0802
0.10000
57.17
|
6
ac
47.1027
19.31498
ACRYLIC
53.89
|
7
−78.1228
0.09209
50.53
|
8
Aperture stop
0.00000
44.30
|
9
ac
353.7641
5.00000
ACRYLIC
43.01
|
10
72.7600
2.00984
40.84
|
11
196.7119
4.00000
ACRYLIC
40.82
|
12
a
634.0427
16.98669
40.23
|
13
a
−24.4615
2.50000
ACRYLIC
39.07
|
14
−24.5000
8.00000
402500
41.88
|
15
∞
2.00000
FDS9
62.00
|
16
∞
0.00130
65.00
|
|
Symbol Description
|
a - Polynomial asphere
|
c - Conic section
|
Even Polynomial Aspheres and Conic Constants
|
Surf.
|
No.
k
D
E
F
|
|
1
−4.3933E+00
−9.9052E−06
8.7010E−09
2.1612E−12
|
2
−2.4028E−06
1.4253E−08
−6.1304E−12
|
6
8.9690E−02
0.0000E+00
0.0000E+00
0.0000E+00
|
9
1.0500E+00
3.6426E−06
1.1748E−08
−3.4344E−11
|
12
4.5912E−06
4.4017E−09
1.3033E−11
|
13
−2.1233E−05
1.4959E−07
−1.1822E−09
|
|
Surf.
|
No.
G
H
I
|
|
1
−1.8320E−14
1.7435E−17
−5.2334E−21
|
2
9.4739E−16
−8.0192E−18
6.1041E−21
|
6
0.0000E+00
0.0000E+00
0.00CCE+00
|
9
4.3912E−14
2.3317E−17
−8.4011E−20
|
12
−1.5225E−13
6.3015E−16
−1.0588E−18
|
13
4.6558E−12
−8.7622E−15
5.7104E−18
|
|
System First Order Properties
|
OBJ. HT: −610.00 f/ 1.05 MAG: −0.0526
|
STOP: 0.00 after surface 8. DIA: 44.267
|
EFL: 44.9290
FVD: 93.0139
ENP: 35.9852
|
IMD: 0.130180E−02
BRL: 93.0126
EXP: −26.4020
|
OBD: −901.499
OVL: 994.512
|
First Order Properties of Elements
|
Element
Surface
|
Number
Numbers
Power
f′
|
|
1
1
2
−0.56743E−02
−176.23
|
2
3
4
−0.71154E−02
−140.54
|
3
4
5
0.21534E−01
46.438
|
4
6
7
0.15947E−01
62.709
|
5
9
10
−0.53589E−02
−186.61
|
6
11
12
0.17366E−02
575.83
|
7
13
14
0.64911E−03
1540.6
|
8
14
15
−0.16408E−01
−60.945
|
|
First-Order Properties of Doublets
|
Element
Surface
|
Numbers
Numbers
Power
f′
|
|
2
3
3
5
0.15292E−01
65.395
|
|
TABLE 4
|
|
Clear
|
Surf.
Aperture
|
No.
Type
Radius
Thickness
Glass
Diameter
|
|
1
ac
−100.1109
5.40000
ACRYLIC
54.09
|
2
a
797.3015
3.67790
53.44
|
3
339.4130
4.20000
FD6
54.49
|
4
97.1412
19.80000
SK18A
56.23
|
5
−46.8441
0.20000
58.38
|
6
ac
102.1081
9.80000
ACRYLIC
55.76
|
7
−125.2404
0.05000
55.01
|
8
Aperture stop
0.05000
53.36
|
9
ac
102.1081
9.80090
ACRYLIC
55.76
|
10
−125.2404
0.20000
55.01
|
11
ac
419.5975
6.50000
ACRYLIC
46.91
|
12
a
78.0417
2.45081
44.76
|
13
739.7583
4.00000
ACRYLIC
44.53
|
14
a
634.0427
18.59644
41.37
|
15
a
−30.6568
2.50000
ACRYLIC
40.19
|
16
−25.5000
8.00000
402500
44.00
|
17
∞
2.00000
FDS9
66.00
|
18
∞
−0.00096
66.00
|
|
Symbol Description
|
a - Polynomial asphere
|
c - Conic section
|
Even Polynomial Aspheres and Conic Constants
|
Surf.
|
No.
k
D
E
F
|
|
1
−4.3933E+00
−9.4878E−06
8.1734E−09
1.3834E−12
|
2
−1.1705E−06
1.3723E−08
−8.8623E−12
|
6
−5.4476E+00
−1.6425E−06
−9.2148E−10
1.0047E−12
|
9
−5.4476E+00
−1.6425E−06
−9.2148E−10
1.0047E−12
|
11
1.0500E+00
9.5442E−06
1.7043E−08
−3.8171E−11
|
12
−7.9579E−06
−6.1592E−10
1.7222E−11
|
14
1.4245E−05
2.2940E−10
7.5152E−11
|
15
−3.3104E−05
2.0008E−07
−1.3812E−09
|
|
Surf.
0
|
No.
G
H
I
|
|
1
−2.0367E−14
2.2941E−17
−8.0011E−21
|
2
2.9148E−15
−5.6145E−18
3.8426E−21
|
6
1.8933E−15
−7.6685E−19
−2.9776E−22
|
9
1.8933E−15
−7.6685E−19
−2.9776E−22
|
11
6.7103E−14
−9.9260E−18
−2.8456E−20
|
12
3.1644E−14
5.8619E−18
−1.1468E−19
|
14
−4.3106E−13
9.1134E−16
−7.5696E−19
|
15
4.8327E−12
−8.3519E−15
5.0919E−18
|
|
System First Order Properties
|
0BJ. HT: −610.00 f/ 1.05 MAG: −0.0526
|
STOP: 0.00 after surface 8. DIA: 53.357
|
EFL: 44.9354
FVD: 97.2242
ENP: 25.7703
|
IMD: −.960536E−03
BRL: 97.2252
EXP: −32.7637
|
OBD: −894.792
OVL: 992.016
|
First Order Properties of Elements
|
Element
Surface
|
Number
Numbers
Power
f′
|
|
1
1
2
−0.55626E−02
−179.77
|
2
3
4
−0.59249E−02
−168.78
|
3
4
5
0.19201E−01
52.080
|
4
6
7
0.86534E−02
115.56
−
|
5
9
10
−0.86534E−02
115.56
|
6
11
12
−0.51179E−02
−195.39
|
7
13
14
−0.10990E−03
−9099.2
|
8
15
16
0. 37792E−02
264.61
|
9
16
17
−0.15765E−01
−63.433
|
|
First-Order Properties of Doublets
|
Element
Surface
|
Numbers
Numbers
Power
f′
|
|
2
3
3 5
0.14148E−01
70.681
|
|
TABLE 5
|
|
Exam-
Φ
0
Φ
E1
|
ple
(mm
−1
)
(mm
−1
)
D
12
|Φ
E1
|/Φ
0
D
12
· Φ
0
|Φ
U3
|/Φ
0
|
|
1
0.0223
−0.0063
9.93
0.283
0.221
0.60
|
2
0.0223
−0.0035
5.12
0.157
0.114
0.72
|
3
0.0223
−0.0057
2.34
0.256
0.082
0.73
|
4
0.0223
−0.0056
3.68
0.251
0.082
0.56
|
|
Φ
0
is the optical power of the whole lens
|
Φ
E1
is the optical power of the first element
|
D
12
is the axial distance from the last surface of the first element to the first surface of the glass doublet
|
Φ
U3
is the optical power of the third lens unit
|
Claims
- 1. A projection lens system for use in combination with a cathode ray tube, said system producing an image, having a power Φ0, and comprising in order from its image side:(a) a negative first lens unit which comprises: (i) at least one aspheric surface and (ii) a negative lens element at the unit's image side, said negative lens element having a power ΦE1 and an image side surface which is concave towards the image; (b) a positive second lens unit which comprises in order from its image side: (i) a positive first lens subunit which consists of a cemented color correcting doublet composed of glass and having spherical surfaces; and (ii) a positive second lens subunit which comprises at least one lens element of weak optical power having at least one aspheric surface; and (c) a third lens unit which is associated with the CRT during use of the lens system, has a strong negative power ΦU3, and contributes to the correction of the lens system's field curvature.
- 2. The projection lens system of claim 1 wherein:0.4≦|ΦU3|/Φ0≦0.8.
- 3. The projection lens system of claim 1 wherein all of the lens elements of the first lens unit, the second lens subunit of the second lens unit, and the third lens unit are composed of plastic.
- 4. The projection lens system of claim 1 wherein the clear aperture diameter of the first lens subunit of the second lens unit is less than 65millimeters.
- 5. The projection lens system of claim 1 wherein the first lens unit comprises two aspheric surfaces and the second lens subunit of the second lens unit comprises two aspheric surfaces.
- 6. The projection lens system of claim 1 wherein the concave image side surface of the negative lens element of the first lens unit is aspheric.
- 7. The projection lens system of claim 1 wherein:|ΦE1|/Φ0≧0.15.
- 8. The projection lens system of claim 1 wherein the negative lens element of the first lens unit is biconcave.
- 9. The projection lens system of claim 1 wherein:D12·Φ0≦0.25 where D12 is the distance between the object side surface of the negative lens element of the first lens unit and the image side surface of the cemented color correcting doublet of the first lens subunit of the second lens unit.
- 10. The projection lens system of claim 1 wherein the second lens subunit of the second lens unit comprises a positive image side lens element.
- 11. The projection lens system of claim 1 wherein the lens system has a half angle field of view in the direction of the image of at least 25 degrees.
- 12. The projection lens system of claim 1 wherein the f-number of the lens system for an infinite conjugate is 1.0.
- 13. The projection lens system of claim 1 wherein the system has an MTF above 0.5 at 10 cycles/millimeter.
- 14. The projection lens system of claim 1 wherein the system produces an image which has a pupil area in its corner that is at least 50 percent of the pupil area on axis.
- 15. The projection lens system of claim 1 wherein (i) the first, second, and third lens units are the only lens units in the system, (ii) the first lens unit consists of two lens elements, and (iii) the second lens subunit of the second lens unit consists of two lens elements.
- 16. A projection television set comprising a cathode ray tube, a screen, and a projection lens system for projecting light from the cathode ray tube onto the screen to form an image, said projection lens system comprising the projection lens system of claim 1.
- 17. The projection television set of claim 16 wherein the cathode ray tube is a three inch cathode ray tube.
- 18. A projection television set comprising three cathode ray tubes, a screen, and three projection lens systems, one projection lens system being associated with each of the cathode ray tubes for projecting light from that tube onto the screen to form an image, each projection lens system comprising the projection lens system of claim 1.
- 19. The projection television set of claim 18 wherein each of the cathode ray tubes is a three inch cathode ray tube.
- 20. A projection lens system for use in combination with a cathode ray tube, said system producing an image, having a power Φ0, and consisting in order from its image side of:(a) a negative first lens unit which comprises: (i) at least one aspheric surface and (ii) a negative lens element at the unit's image side, said negative lens element having a power ΦE1 and an image side surface which is concave towards the image; (b) a positive second lens unit which consists in order from its image side of: (i) a positive first lens subunit which consists of a cemented color correcting doublet composed of glass and having spherical surfaces; and (ii) a positive second lens subunit which comprises at least one lens element of weak optical power having at least one aspheric surface; and a third lens unit which is associated with the CRT during use of the lens system, has a strong negative power ΦU3, and contributes to the correction of the lens system's field curvature.
US Referenced Citations (16)
Foreign Referenced Citations (4)
Number |
Date |
Country |
833 179 A1 |
Apr 1998 |
EP |
WO9741477 |
Nov 1997 |
WO |
WO9903006 |
Jan 1999 |
WO |
WO9967662 |
Dec 1999 |
WO |