1. Field of the Invention
The present invention relates to an optical lens assembly, and more particularly, to an optical lens assembly having an optical refractive index matching layer.
2. Description of the Prior Art
The unexpected light in an optical lens assembly may cause flare, ghost or a decrease in the overall image contrast and adversely affect the image quality. In addition to the multiple reflections between the lenses, the unexpected light may be the result of reflections from other discontinuous interfaces in the lens assembly, such as the reflection from the interface between the outer edge of the lens and air, or the reflection from the inner edge of the lens barrel. To eliminate the multiple reflections, the lenses in a modern lens assembly are usually coated with multiple anti-reflection layers to increase the transmittance thereof and reduce the unexpected reflections therebetween. To eliminate the reflection from the inner edge of the lens barrel, the interior of the lens barrel is usually made of a dark-colored material, and the inner surface of the lens barrel may also be provided with a coating to increase the light absorption rate of the lens barrel.
The reflection from the interface between the outer edge of the lens and air is another problem to be solved in lens design. In an optical lens assembly, the lenses are fixed inside the lens barrel. As described above, although the anti-reflection processing is usually performed on the inner edge of the lens barrel, there is a gap between the outer edge of the lens and the inner edge of the lens barrel, and thus the outer edge of the lens is actually in direct contact mainly with air. Optical glasses or optical plastic materials are common materials used to fabricate lenses. Such materials are significantly different in refractive index from air. For a lens made of any of such materials, the interface between the outer edge thereof and air causes the occurrence of full reflection easily and results in the formation of unexpected light in the lens assembly. In the past, a dark light-absorbing material, such as the carbon black disclosed in U.S. Pat. No. 4,332,706 or the anti-reflection black material disclosed in the US Publication No. 2005/0226608, is often disposed between the outer edge of the lens and the lens barrel to increase the light absorption rate and thereby to reduce the reflection.
In view of the aforementioned prior art, the present invention proposes an improved method that prevents the occurrence of full reflection from the aforementioned lens edge by adding an optically transmissive optical refractive index matching layer between the outer edge of the lens and the lens barrel.
The present invention provides an optical lens assembly, comprising: a lens barrel made of plastic material and having a lens insertion opening and a lens barrel central axis, the lens barrel accommodating a first lens element with refractive power, a second lens element with refractive power made of plastic material, a third lens element with refractive power, and an optical refractive index matching layer disposed in a gap between the lens barrel and the second lens element and respectively connecting the lens barrel and the second lens element; wherein the first lens element is disposed farther from the lens insertion opening than the second lens element, and the second lens element is disposed farther from the lens insertion opening than the third lens element; and wherein there is an air space between the first lens element and the second lens element on the lens barrel central axis, and there is another air space between the second lens element and the third lens element on the lens barrel central axis.
In the optical lens assembly of the present invention, it is preferable that the second lens element has a second lens element fitting surface abutting against an adjacent lens and forming an angle A together with the lens barrel central axis. The angle A satisfies the following relation: |A|<45 degrees.
In the optical lens assembly of the present invention, it is preferable that the second lens element fitting surface is arranged at the side of the second lens element farther away from the lens insertion opening.
In the optical lens assembly of the present invention, it is preferable that the first lens element has a first lens element fitting surface lap joining the second lens element fitting surface and arranged farther away from the lens barrel central axis than the second lens element fitting surface.
In the optical lens assembly of the present invention, it is preferable that the second lens element comprises a front side surface facing away from the lens insertion opening and a back side surface facing the lens insertion opening, and that each of the front side surface and the back side surface comprises a second lens element fitting surface.
In the optical lens assembly of the present invention, it is preferable that at least one of the first lens element and the second lens element has at least one aspheric surface.
In the optical lens assembly of the present invention, it is preferable that a visible light absorption rate of the lens barrel is Ab which satisfies the following relation: Ab>80%.
Preferably, the optical lens assembly of the present invention comprises a ring-shaped optical component disposed at one side of the second lens element.
In the optical lens assembly of the present invention, it is preferable that the ring-shaped optical component has an outer diameter Ds and the second lens element has an outer diameter D2, and they satisfy the following relation: Ds/D2<1.
In the optical lens assembly of the present invention, it is preferable that a refractive index of the optical refractive index matching layer is nc and a refractive index of the second lens element is n2, and they satisfy the following relation: 0.75<nc/n2<1.50.
In the optical lens assembly of the present invention, it is preferable that the refractive index of the optical refractive index matching layer is nc and the refractive index of the second lens element is n2, and they further satisfy the following relation: 0.8<nc/n2<1.2.
In the optical lens assembly of the present invention, it is preferable that the optical refractive index matching layer is made of a polymer material.
In the optical lens assembly of the present invention, it is preferable that a visible light transmittance of the optical refractive index matching layer is Tc which satisfies the following relation: Tc>80%.
The present invention provides another optical lens assembly, comprising: a lens barrel made of plastic material and having a lens insertion opening and a lens barrel central axis, the lens barrel accommodating a first lens element with refractive power, a second lens element with refractive power made of plastic material, a ring-shaped optical component made of a light absorbable material and disposed between the first lens element and the second lens element, and an optical refractive index matching layer disposed at one surface of the ring-shaped optical component; wherein the first lens element is disposed farther from the lens insertion opening than the second lens element; and wherein there is an air space between the first lens element and the second lens element on the lens barrel central axis.
Preferably, the optical lens assembly of the present invention comprises another optical refractive index matching layer disposed in a gap between the second lens element and the lens barrel and respectively connecting the second lens element and the lens barrel. A visible light absorption rate of the lens barrel is Ab which satisfies the following relation: Ab>90%.
In the optical lens assembly of the present invention, it is preferable that a visible light absorption rate of the ring-shaped optical component is As which satisfies the following relation: As>80%.
In the optical lens assembly of the present invention, it is preferable that the ring-shaped optical component is a light shielding element.
In
n
g SIN θi=nc SIN θt
According to the above equation, nc and ng satisfy the following relation:
SIN θi>/ng
Regarding the occurrence of full reflection, as the refractive index nc of the optical refractive index matching layer 230 is greater than the refractive index (approximately 1) of air, full reflection is less likely to occur with the arrangement of the optical refractive index matching layer 230 between the lens 210 and the lens barrel 200. Full reflection can be completely prevented even under the circumstance that nc is greater than ng.
The total amount of reflection of the light 250 incident to the interface between the lens 210 and the optical refractive index matching layer 230 will be estimated below. According to the polarization of the light 250, the reflection coefficients of the energy between the lens 210 and the optical refractive index matching layer 230 are Rs and Rp. Rs which respectively satisfy the following relations:
R
s=[(ng COS θi−nc COS θt)/(ng COS θi+nc COS θt)]2
R
p=[(ng COS θt−nc COS θi)/(ng COS θt+nc COS θi)]2
Under normal circumstances, the light 250 is not polarized and thus not characterized by polarization. Therefore, the ratio R of the energy of the reflected light 260a to the energy of the incident light 250 satisfies the following relation: R=(Rs+Rp)/2
The ratio T of the energy of the refracted light 270a to the energy of the incident light 250 satisfies the following relation:
T=1−R
Under the circumstance that the deduction is not affected, suppose the optical refractive index matching layer 230 does not absorb any light, the majority of the refracted light 270a will be absorbed by the lens barrel. As shown in
In the first example of the embodiment, the incident angle θi of the incident light 250 is 36°, the visible light absorption rate Ab of the lens barrel is 90%, and the refractive index of the lens 210 is 1.5168 (d-line). Table 1 below lists the first reflection coefficient R, the multi-reflection coefficient Rm, and the total reflection coefficient RT of various optical refractive index matching layer materials (the refractive index ranges from 1 to 2.5) estimated according to the above method.
Referring to data in Table 1, the circumstance that the refractive index of the material is 1 can be regarded as the circumstance that no optical refractive index matching layer is added (air has a refractive index of approximately 1) and is compared with the data of other optical coating materials listed in Table 1. As can be seen from the data in Table 1, the total reflection is mainly contributed from the accumulated multiple reflections portion when the incident angle θi is 36°, with the exception of Nc=1 (no optical refractive index matching layer is provided). In this example, if the lens barrel has a higher visible light absorption rate, the multi-reflection coefficient Rm will decrease. The multi-reflection coefficient Rm is more related to the visible light absorption rate of the lens barrel than the optical refractive index matching layer. On the other hand, the closer the refractive index of the optical refractive index matching layer is to the refractive index of the lens, the lower the first reflection coefficient R is, and the total reflection coefficient RT also decreases correspondingly. In this example, the total reflection amount is not large, but the arrangement of the optical refractive index matching layer still reduces the total reflection amount. While the lens barrel in each example of the embodiment has a visible light absorption rate Ab of 90%, Ab can be above 95% in real practice. If a lens barrel has a visible light absorption rate of approximately 10%, multiple reflections will not occur; meanwhile, the total reflection amount can be reduced to below 1% if the optical refractive index matching layer and the refractive index of the lens match well, thereby completely controlling the internal reflection.
In the second example of the embodiment, the incident angle θi of the incident light 250 is 38°, the visible light absorption rate Ab of the lens barrel is 90%, and the refractive index of the lens 210 is 1.5168 (d-line). Table 2 below lists the first reflection coefficient R, the multi-reflection coefficient Rm, and the total reflection coefficient RT of various optical refractive index matching layer materials (the refractive index ranges from 1 to 2.5) estimated according to the above method.
According to the data in Table 2, the first reflection coefficient R and the total reflection coefficient RT both increase with the increasing incident angle but the result is similar to that of the first example. The total reflection is mainly contributed from the accumulated multiple reflections portion, with the exception of Nc=1 (no optical refractive index matching layer is provided). The closer the refractive index of the optical refractive index matching layer is to the refractive index of the lens, the lower the total reflection coefficient RT is because of the decrease of the first reflection coefficient R.
In the third example of the embodiment, the incident angle θi of the incident light 250 is 40°, the visible light absorption rate Ab of the lens barrel is 90%, and the refractive index of the lens 210 is 1.5168 (d-line). Table 3 below lists the first reflection coefficient R, the multi-reflection coefficient Rm, and the total reflection coefficient RT of various optical refractive index matching layer materials (the refractive index ranges from 1 to 2.5) estimated according to the above method.
In the third example of the embodiment, the incident angle θi is 40°, which is only 2° greater than the incident angle of the previous example. However, the first reflection coefficient R has increased significantly under the circumstance that no optical refractive index matching layer is disposed, and this is a typical phenomenon that normally occurs when the incident angle is close to the total reflection critical angle (in this embodiment, the critical angle is slightly greater than 41°). This is when the optical refractive index matching layer has a great effect. Although the closer the refractive index of the optical refractive index matching layer is to the refractive index of the lens, the lower the total reflection coefficient RT is, it can be seen from the data in Table 3 that even if the optical refractive index matching layer is significantly different in refractive index from the lens (for example, Nc=1.1 or Nc=2.5), the first reflection coefficient R and the total reflection coefficient RT still decrease significantly compared with the circumstance that no optical refractive index matching layer is disposed. Therefore, there is a great deal of flexibility in the selection of material for the coating.
In the fourth example of the embodiment, the incident angle θi of the incident light 250 is 42°, the visible light absorption rate Ab of the lens barrel is 90%, and the refractive index of the lens 210 is 1.5168 (d-line). Table 4 below lists the first reflection coefficient R, the multi-reflection coefficient Rm, and the total reflection coefficient RT of various optical refractive index matching layer materials (the refractive index ranges from 1 to 2.5) estimated according to the above method.
As described above, in this example, the incident angle exceeds the critical angle, full reflection occurs, and the total reflection coefficient RT is 1 without the optical refractive index matching layer. This is when the optical refractive index matching layer has a great effect. Even if the refractive index of the optical refractive index matching layer is as low as 1.2 or as high as 2.4, the total reflection coefficient RT is controlled within 15%. Generally speaking, the optical refractive index matching layers have great effects as long as the relation of 0.75<nc/ng<1.50 is satisfied. To further control the total reflection coefficient RT within 11%, it merely requires the satisfaction of the relation of 0.85<nc/ng<1.25. Regarding the elimination of reflection, it is close to the optimal effect under the framework of the present invention. According to the data in Table 4, the total reflection coefficient RT remains to be approximately 10% even if the refractive index of the optical refractive index matching layer is extremely close to the refractive index of the lens.
The above deduction shows that the relation between the refractive index of the lens and the refractive index of the optical refractive index matching layer does not limit the type of material used to make the lens. Therefore, the lens can be made of glass, plastic material or any other material that satisfies optical requirements under the framework of the present invention. Regarding various materials, selection of material for the optical refractive index matching layer can be made according to the limitation on the refractive index of the optical refractive index matching layer as described above. As the range of the refractive index of the optical refractive index matching layer is wide, selection of material can be made to meet other requirements in system design. For example, the optical refractive index matching layer is viscous and is advantageous in fixing the lens to reinforce the rigidity of the lens assembly. Specifically, the optical refractive index matching layer can be UV glue having the aforementioned features. Moreover, the refractive indexes of UV glues available on the market generally range from 1.47 to 1.54 that match well with the refractive indexes of materials commonly used to make lenses.
The optical refractive index matching layer described in the first embodiment of the present invention is applicable to the interface between any lens and the lens barrel in the optical lens assembly.
In this embodiment, the first lens element 410 has a bulging first lens element fitting surface 480 (which consists of a first abutment section 481 and a second abutment section 482 of the first lens element 410, as shown in
As described above, the arrangement of the optical refractive index matching layer will not pose any limitation on the materials used to make lenses of the optical lens assembly. Therefore, in this embodiment, the first lens element 410 and the second lens element 420 can be made of glass or plastic material. Most plastic lenses are fabricated by molding, thus aspheric surfaces can be made easily. Furthermore, the size of the optical lens assembly can be reduced or the optical quality can be increased. Most of the lenses in the optical lens assembly are provided with coating layers on the surfaces thereof to reduce the reflection between. The arrangement of the coating layer will not affect the arrangement of the optical refractive index matching layer in the present invention.
As demonstrated by various examples of the first embodiment, even if the refractive index of the optical refractive index matching layer matches well with the refractive index of the lens, a portion of the reflected light will still be reflected back to the interior of the lens assembly from the outer edge of the lens due to the limitation of the absorption rate of the lens barrel. Therefore, when the visible light absorption rate Ab of the lens barrel cannot be increased under certain circumstance (for example, the manufacturing cost is taken into consideration), additional means is required to deal with the residual reflected light generated thereby. In the second embodiment of the present invention shown in
Different data of the different embodiments are used to explain the implementation methods and to prove the effect of the present invention. Therefore, any optical lens assembly of the same structure is considered to be within the scope of the present invention even if it uses different data. The embodiments depicted above and the appended drawings are exemplary and are not intended to limit the scope of the present invention.
Number | Date | Country | Kind |
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103202367 | Feb 2014 | TW | national |