This application claims priority to Chinese Application No. 201310628447.9, filed on Nov. 29, 2013.
1. Field of the Invention
The present invention relates to an imaging lens and an electronic apparatus including the same.
2. Description of the Related Art
In recent years, as use of portable electronic devices (e.g., mobile phones and digital cameras) becomes ubiquitous, much effort has been put into reducing dimensions of portable electronic devices. Moreover, as dimensions of charged coupled device (CCD) and complementary metal-oxide semiconductor (CMOS) based optical sensors are reduced, dimensions of imaging lenses for use with the optical sensors must be correspondingly reduced without significantly compromising optical performance.
Each of U.S. Pat. Nos. 7,848,032, 8,284,502, 8,179,616, and TW patent publication no. 201109712 discloses a conventional imaging lens that includes four lens elements, and that has a system length of over 8mm. Particularly, the imaging lens disclosed in U.S. Pat. No. 8,179,616 has a system length of over 11 mm, which disfavors reducing thickness of portable electronic devices, such as mobile phones and digital cameras.
Reducing the system length of the imaging lens while maintaining satisfactory optical performance is always a goal in the industry.
Therefore, an object of the present invention is to provide an imaging lens having a shorter overall length while maintaining good optical performance.
According to one aspect of the present invention, an imaging lens comprises a first lens element, a second lens element, a third lens element and a fourth lens element arranged in order from an object side to an image side along an optical axis of the imaging lens. Each of the first lens element, the second lens element, the third lens element and the fourth lens element has a refractive power, an object-side surface facing toward the object side, and an image-side surface facing toward the image side.
The image-side surface of the first lens element has a convex portion in a vicinity of a periphery of the first lens element. The object-side surface of the second lens element has a concave portion in a vicinity of a periphery of the second lens element. The third lens element has a positive refractive power, and the image-side surface of the third lens element has a convex portion in a vicinity of a periphery of the third lens element. The fourth lens element is made of a plastic material, and the object-side surface of the fourth lens element has a concave portion in a vicinity of the optical axis, and a convex portion in a vicinity of a periphery of the fourth lens element.
The imaging lens does not include any lens element with refractive power other than the first lens element, the second lens element, the third lens element and the fourth lens element.
Another object of the present invention is to provide an electronic apparatus having an imaging lens with four lens elements.
According to another aspect of the present invention, an electronic apparatus includes a housing and an imaging module. The imaging module is disposed in the housing, and includes the imaging lens of the present invention, a barrel on which the imaging lens is disposed, a holder unit on which the barrel is disposed, and an image sensor disposed at the image side of the imaging lens.
Other features and advantages of the present invention will become apparent in the following detailed description of the preferred embodiments with reference to the accompanying drawings, of which:
a) to 5(d) show different optical characteristics of the imaging lens of the first preferred embodiment;
a) to 9(d) show different optical characteristics of the imaging lens of the second preferred embodiment;
a) to 13(d) show different optical characteristics of the imaging lens of the third preferred embodiment;
a) to 17(d) show different optical characteristics of the imaging lens of the fourth preferred embodiment;
a) to 21(d) show different optical characteristics of the imaging lens of the fifth preferred embodiment;
a) to 25(d) show different optical characteristics of the imaging lens of the sixth preferred embodiment;
a) to 29(d) show different optical characteristics of the imaging lens of the seventh preferred embodiment;
a) to 33(d) show different optical characteristics of the imaging lens of the eighth preferred embodiment;
Before the present invention is described in greater detail, it should be noted that like elements are denoted by the same reference numerals throughout the disclosure.
In the following description, “a lens element has a positive (or negative) refractive power” means the lens element has a positive (or negative) refractive power in a vicinity of an optical axis thereof. “An object-side surface (or image-side surface) has a convex (or concave) portion at a certain area” means that, compared to a radially exterior area adjacent to said certain area, said certain area is more convex (or concave) in a direction parallel to the optical axis. Referring to
Referring to
Each of the first, second, third, and fourth lens elements 3-6 and the optical filter 7 has an object-side surface 31, 41, 51, 61, 71 facing toward the object side, and an image-side surface 32, 42, 52, 62, 72 facing toward the image side. Light entering the imaging lens 10 travels through the aperture stop 2, the object-side and image-side surfaces 31, 32 of the first lens element 3, the object-side and image-side surfaces 41, 42 of the second lens element 4, the object-side and image-side surfaces 51, 52 of the third lens element 5, the object-side and image-side surfaces 61, 62 of the fourth lens element 6, and the object-side and image-side surfaces 71, 72 of the optical filter 7, in the given order, to form an image on the image plane 8. In this embodiment, each of the object-side surfaces 31, 41, 51, 61 and the image-side surfaces 32, 42, 52, 62 is aspherical and has a center point coinciding with the optical axis (I).
In the first preferred embodiment, which is depicted in
The second lens element 4 has a negative refractive power. The object-side surface 41 of the second lens element 4 is a concave surface that has a concave portion 412 in a vicinity of the optical axis (I), and a concave portion 411 in a vicinity of a periphery of the second lens element 4. The image-side surface 42 of the second lens element 4 is a concave surface has a concave portion 423 in a vicinity of the optical axis (I), and a convex portion 422 in a vicinity of a periphery of the second lens element 4.
The third lens element 5 has a positive refractive power. The object-side surface 51 of the third lens element 5 is a concave surface has a concave portion 511 in a vicinity of the optical axis (I), and a concave portion 512 in a vicinity of a periphery of the third lens element 5. The image-side surface 52 of the third lens element 5 is a convex surface that has a convex portion 522 in a vicinity of the optical axis (I), and a convex portion 521 in a vicinity of a periphery of the third lens element 5.
The fourth lens element 6 has a negative refractive power. The object-side surface 61 of the fourth lens element 6 has a concave portion 611 in a vicinity of the optical axis (I), and a convex portion 612 in a vicinity of a periphery of the fourth lens element 6. The image-side surface 62 of the fourth lens element 6 has a concave portion 621 in a vicinity of the optical axis (I), and a convex portion 622 in a vicinity of the periphery of the fourth lens element 6.
In the first preferred embodiment, the imaging lens 10 does not include any lens element with refractive power other than the aforesaid lens elements 3-6.
Shown in
In this embodiment, each of the object-side surfaces 31-61 and the image-side surfaces 32-62 is aspherical, and satisfies the relationship of
where:
Y represents a perpendicular distance between an arbitrary point on an aspherical surface and the optical axis (I);
Z represents a depth of theaspherical surface, which is defined as a perpendicular distance between the arbitrary point on the aspherical surface that is spaced apart from the optical axis (I) by a distance Y, and a tangent plane at a vertex of the aspherical surface at the optical axis (I);
R represents a radius of curvature of the aspherical surface;
K represents a conic constant; and
α2i represents a 2ith aspherical coefficient.
Shown in
Relationships among some of the aforementioned lens parameters corresponding to the first preferred embodiment are shown in columns of
T1 represents a thickness of the first lens element 3 at the optical axis (I);
T2 represents a thickness of the second lens element 4 at the optical axis (I);
T3 represents a thickness of the third lens element 5 at the optical axis (I);
T4 represents a thickness of the fourth lens element 6 at the optical axis (I);
G12 represents an air gap length between the first lens element 3 and the second lens element 4 at the optical axis (I);
G23 represents an air gap length between the second lens element 4 and the third lens element 5 at the optical axis (I);
G34 represents an air gap length between the third lens element 5 and the fourth lens element 6 at the optical axis (I);
TTL represents a distance at the optical axis (I) between the object-side surface 31 of the first lens element 3 and the image plane 8 at the image side;
BFL represents a distance at the optical axis (I) between the image-side surface 62 of the fourth lens element 6 and the image plane 8 at the image side;
ALT represents a sum of the thicknesses of the first lens element 3, the second lens element 4, the third lens element 5 and the fourth lens element 6 at the optical axis (I);
AAG represents a sum of the air gap lengths among the first lens element 3, the second lens element 4, the third lens element 5, and the fourth lens element 6 at the optical axis (I); and
EFL represents a system focal length of the imaging lens 10.
a) to 5(d) respectively show simulation results corresponding to longitudinal spherical aberration, sagittal astigmatism aberration, tangential astigmatism aberration, and distortion aberration of the first preferred embodiment. In each of the simulation results, curves corresponding respectively to wavelengths of 470 nm, 555 nm, and 650 nm are shown.
It can be understood from
It can be understood from
Moreover, as shown in
In view of the above, even with the system length reduced down to 4.592 mm, the imaging lens 10 of the first preferred embodiment is still able to achieve a relatively good optical performance.
Shown in
Shown in
Relationships among some of the aforementioned lens parameters corresponding to the second preferred embodiment are shown in columns of
a) to 9(d) respectively show simulation results corresponding to longitudinal spherical aberration, sagittal astigmatism aberration, tangential astigmatism aberration, and distortion aberration of the second preferred embodiment. It can be understood from
Shown in
Shown in
Relationships among some of the aforementioned lens parameters corresponding to the third preferred embodiment are shown in columns of
a) to 13(d) respectively show simulation results corresponding to longitudinal spherical aberration, sagittal astigmatism aberration, tangential astigmatism aberration, and distortion aberration of the third preferred embodiment. It can be understood from
Shown in
Shown in
Relationships among some of the aforementioned lens parameters corresponding to the fourth preferred embodiment are shown in columns of
a) to 17(d) respectively show simulation results corresponding to longitudinal spherical aberration, sagittal astigmatism aberration, tangential astigmatism aberration, and distortion aberration of the fourth preferred embodiment. It can be understood from
Shown in
Shown in
Relationships among some of the aforementioned lens parameters corresponding to the fifth preferred embodiment are shown in columns of
a) to 21(d) respectively show simulation results corresponding to longitudinal spherical aberration, sagittal astigmatism aberration, tangential astigmatism aberration, and distortion aberration of the fifth preferred embodiment. It can be understood from
Shown in
Shown in
Relationships among some of the aforementioned lens parameters corresponding to the sixth preferred embodiment are shown in columns of
a) to 25(d) respectively show simulation results corresponding to longitudinal spherical aberration, sagittal astigmatism aberration, tangential astigmatism aberration, and distortion aberration of the sixth preferred embodiment. It can be understood from
Shown in
Shown in
Relationships among some of the aforementioned lens parameters corresponding to the seventh preferred embodiment are shown in columns of
a) to 29(d) respectively show simulation results corresponding to longitudinal spherical aberration, sagittal astigmatism aberration, tangential astigmatism aberration, and distortion aberration of the seventh preferred embodiment. It can be understood from
Referring to
Shown in
Shown in
Relationships among some of the aforementioned lens parameters corresponding to the eighth preferred embodiment are shown in columns of
a) to 33(d) respectively show simulation results corresponding to longitudinal spherical aberration, sagittal astigmatism aberration, tangential astigmatism aberration, and distortion aberration of the eighth preferred embodiment. It can be understood from
Shown in
(1) EFL/T4≦8.5: Since reduction in EFL favors reduction in the system length, and the fourth lens element 6 having a relatively large effective optical diameter should have a sufficient thickness for ease of manufacture thereof, the system length of the imaging lens 10 may be effectively reduced when EFL/T4 is designed to be small. Preferably, 5≦EFL/T4≦8.5.
(2) T3/G23≦1.9: Since the third lens element 5 has a relatively small effective optical diameter, the design of T3 may tend to be small. Since the third lens element 5 has a positive refractive power, G23 should be designed to be within a proper range to allow light entering the third lens element 5 at an appropriate height for convergence. Therefore, good optical performance may be maintained with the reduced system length when this relationship is satisfied. Preferably, 0.9≦T3/G23≦1.9.
(3) 1.5≦T4/(G12+G34): The fourth lens element 6 has a relatively large effective optical diameter, and a relatively large T4 which facilitates ease of manufacture thereof is required. By virtue of configurations of the convex portion 321 of the first lens element 3 and the concave portion 411 of the second lens element 4, G12 may be made smaller without causing edge interference between the first and second lens elements 3 and 4. By virtue of configurations of the convex portion 521 of the third lens element 5 and a large difference in the effective optical diameters between the third and fourth lens elements 5, 6, G34 may be made smaller without causing edge interference between the third and fourth lens elements 5 and 6. Therefore, design of T4/(G12+G34) should tend to be small. Preferably, 1.5≦T4/(G12+G34)≦4.8.
(4) 1.9≦T4/G34: As mentioned above, it is relatively difficult to reduce T4, whereas the reducible ratio of G34 is relatively large. Therefore, design of T4/G34 should tend to be large. Preferably, 1.9≦T4/G34≦8.5.
(5) 1.6≦G23/(G12+G34): As mentioned above, since G23 should be designed to be within a proper range and the reducible ratios of G12 and G34 are relatively large, design of G23/(G12+G34) should tend to be large. When the imaging lens 10 further satisfies condition of 1.6≦G23/(G12+G34)≦3, G34 is allowed to be larger, thus resulting in a relatively simple assembling process. Preferably, 1.6≦G23/(G12+G34)≦4.2.
(6) AAG/T4≦3: As mentioned above, T4 should be made thicker for ease of manufacture of the fourth lens element 6, and reduction in AAG favors reduction of the system length of the imaging lens 10. Thus, design of AAG/T4 should tend to be small. Preferably, 0.7≦AAG/T4≦3.
(7) T1/G23≦1.55: Since the surface profile of the first lens element 3 around the optical axis (I) is not limited, and the effective optical diameter of the first lens element 3 is relatively small, the first lens element 3 may be manufactured to have a relatively small thickness. As mentioned above, G23 should be sufficiently large to maintain good optical performance. Thus, design of T1/G23 should tend to be small. Preferably, 0.65≦T1/G23≦1.55.
(8) 3.9≦BFL/T2: Since the surface profile of the second lens element 4 around the optical axis (I) is not limited, and the effective optical diameter of the second lens element 4 is relatively small, the second lens element 4 may be manufactured to have a relatively small thickness. Design of BFL should be sufficient for accommodating the optical filter 7 and other elements. Thus, design of BFL/T2 should tend to be large. Preferably, 3.9≦BFL/T2≦6.5.
(9) TTL/T4≦9.35: As mentioned above, T4 should be sufficiently large for ease of manufacture of the fourth lens element 6 while TTL is reduced. Thus, the design of TTL/T4 should tend to be small. Preferably, 6≦TTL/T4≦9.35.
(10) T2/G23≦0.8: As mentioned above, G23 should be designed to be within a proper range, and the reducible ratio of T2 is relatively large. Thus, design of T2/G23 should tend to be small. Preferably, 0.2≦T2/G23≦0.8.
(11) 3.8≦BFL/(G12+G34): As mentioned above, BFL should be sufficiently large, and the reducible ratios of G12 and G34 are relatively large. Thus, design of BFL/(G12+G34) should tend to be large. Preferably, 3.8≦BFL/(G12+G34)≦9.
(12) ALT/G23≦5.5: Since reduction in ALT favors reduction of the system length of the imaging lens 10, and G23 should be designed to be within a proper range, design of ALT/G23 should tend to be small. Preferably, 2.8≦ALT/G23≦5.5.
(13) 2.0≦BFL/T1: Since reducible ratio of T1 is relatively large and BFL should be sufficiently large, design of BFL/T1 should tend to be large. Preferably, 2≦BFL/T1≦2.7.
(14) T3/T4≦2.15: As mentioned above, T4 is relatively large and T3 is relatively small. Thus, design of T3/T4 should tend to be small. Preferably, 1≦T3/T4≦2.15
(15) T2/T4≦0.7: As mentioned above, T4 is relatively large and T2 is relatively small. Thus, design of T2/T4 should tend to be small. Preferably, 0.2≦T2/T4≦0.7.
To sum up, effects and advantages of the imaging lens 10 according to the present invention are described hereinafter.
1. By virtue of the third lens element 5 with the positive refractive power that provides a portion of the positive refractive power required by the imaging lens 10, the convex portion 321, the concave portion 411, the convex portion 521, the concave portion 611 and the convex portion 612, image aberration of the imaging lens 10 may be corrected. Since the fourth lens element 6 is made of a plastic material, weight and cost of the imaging lens 10 may be reduced.
2. Through design of the relevant optical parameters, such as EFL/T4, T3/G23, T4/(G12+G34), T4/G34, G23/(G12+G34), AAG/T4, T1/G23, BFL/T2, TTL/T4, T2/G23, BFL/(G12+G34), ALT/G23, BFL/T1, T3/T4 and T2/T4, optical aberrations, such as spherical aberration, may be reduced or even eliminated. Further, through surface design and arrangement of the lens elements 3-6, even with reduced system length, optical aberrations may still be reduced or even eliminated, resulting in relatively good optical performance.
3. Through the aforesaid eight preferred embodiments, it is known that the system length (TTL) of this invention may be reduced down to below 5 mm. As compared to the conventional imaging lens, the present invention provides a relatively compact imaging lens so as to facilitate developing relevant products and to meet market requirements while maintaining good optical performance.
Shown in
The holder unit 120 includes a first holder portion 121 in which the barrel 21 is disposed, and a second holder portion 122 having a portion interposed between the first holder portion 121 and the image sensor 130. The barrel 21 and the first holder portion 121 of the holder unit 120 extend along an axis (II), which coincides with the optical axis (I) of the imaging lens 10. It should be noted that the image sensor 130 in this embodiment is packaged using chip on board (COB) techniques. Compared to the conventional CSP (chip scale package), a cover glass is not required for the COB technique. Hence, the imaging lens of the present invention does not include the cover glass, but the present invention should not be limited in this respect.
Shown in
The inner section 123 and the barrel 21, together with the imaging lens 10 therein, are movable with respect to the image sensor 130 along an axis (III), which coincides with the optical axis (I) of the imaging lens 10. The optical filter 7 of the imaging lens 10 is disposed at the second holder portion 122, which is disposed to abut against the outer section 124. Configuration and arrangement of other components of the electronic apparatus 1 in the second exemplary application are identical to those in the first exemplary application, and hence will not be described hereinafter for the sake of brevity.
By virtue of the imaging lens 10 of the present invention, the electronic apparatus 1 in each of the exemplary applications may be configured to have a relatively reduced overall thickness with good optical and imaging performance, so as to reduce cost of materials, and satisfy requirements of product miniaturization.
While the present invention has been described in connection with what are considered the most practical and preferred embodiments, it is understood that this invention is not limited to the disclosed embodiments but is intended to cover various arrangements included within the spirit and scope of the broadest interpretation so as to encompass all such modifications and equivalent arrangements.
Number | Date | Country | Kind |
---|---|---|---|
2013 1 0628447 | Nov 2013 | CN | national |
Number | Name | Date | Kind |
---|---|---|---|
7660049 | Tang | Feb 2010 | B2 |
7848032 | Chen et al. | Dec 2010 | B1 |
7911715 | Shinohara | Mar 2011 | B2 |
8014080 | Chen et al. | Sep 2011 | B1 |
8179616 | Hsu et al. | May 2012 | B1 |
8189272 | Huang et al. | May 2012 | B1 |
8274593 | Chen et al. | Sep 2012 | B2 |
8284502 | Hsu et al. | Oct 2012 | B2 |
8405919 | Tsai et al. | Mar 2013 | B2 |
8411377 | Tsai et al. | Apr 2013 | B2 |
8422146 | Tsai et al. | Apr 2013 | B1 |
8988794 | Ota | Mar 2015 | B2 |
9001436 | Tsai | Apr 2015 | B2 |
20110069401 | Jo | Mar 2011 | A1 |
20110261470 | Chen et al. | Oct 2011 | A1 |
20110261471 | Taniyama | Oct 2011 | A1 |
20120044403 | Tang et al. | Feb 2012 | A1 |
20120140339 | Huang et al. | Jun 2012 | A1 |
20130044379 | Hsieh et al. | Feb 2013 | A1 |
20130063827 | Hsu et al. | Mar 2013 | A1 |
20130107378 | Kubota et al. | May 2013 | A1 |
20150077622 | Ueno | Mar 2015 | A1 |
20150153543 | Chen | Jun 2015 | A1 |
Number | Date | Country |
---|---|---|
201300828 | Jan 2013 | AD |
103185958 | Jul 2013 | CN |
2009003443 | Jan 2009 | JP |
2009069196 | Apr 2009 | JP |
2011227131 | Nov 2011 | JP |
2011232449 | Nov 2011 | JP |
1020110085465 | Jul 2011 | KR |
1020120106021 | Sep 2012 | KR |
M354079 | Apr 2009 | TW |
I309727 | May 2009 | TW |
M356127 | May 2009 | TW |
M360369 | Jul 2009 | TW |
201109712 | Mar 2011 | TW |
201137429 | Nov 2011 | TW |
201217853 | May 2012 | TW |
201229612 | Jul 2012 | TW |
201237497 | Sep 2012 | TW |
201300829 | Jan 2013 | TW |
201303352 | Jan 2013 | TW |
201312151 | Mar 2013 | TW |
201326885 | Jul 2013 | TW |
201331616 | Aug 2013 | TW |
2010140515 | Dec 2010 | WO |
2013111612 | Aug 2013 | WO |
Number | Date | Country | |
---|---|---|---|
20150153545 A1 | Jun 2015 | US |