The present invention relates to an optical film structure, and more particularly to an optical film structure with high angle and high spectral shift.
In the existing optical filters using dielectric films, most of them have spectral shift due to the difference in the incident angle of light. Therefore, the coating-based optical application is limited and cannot be effectively utilized.
In the case of an optical film structure 1 applied to the Bragg reflector and having a film configuration as shown in
Take an optical film structure 2, applied to an optical filter and having the film configuration shown in
The transmittance test results are shown in
Therefore, how to make the optical film with a spectral shift caused by the difference of incident angles of light still be used effectively is an issue to be solved.
One objective of the present invention is to provide an optical film structure that can increase the spectral shift caused by the difference in the incident angle of light.
Another objective of the present invention is to provide an optical film structure which can be used effectively even in the presence of spectral shift caused by the difference of the incident angles of light.
Yet another objective of the present invention is to provide an optical film structure which can be applied to various devices or components that require their filtering properties to change with the different incident angles of light, such as, but not limited to, devices or components that have the anti-spy function (or anti-peeping function), color changing with the different incident angles of light, or wavelength filtering changing with the different incident angles of light.
To achieve the above objectives, an optical film structure in accordance with an embodiment of the present invention comprises a plurality of film sets stacked along an axis, and each film set of the plurality of film sets including a first film and a second film which are stacked, wherein for each film set of the plurality of film sets, a refractive index of the first film is greater than a refractive index of the second film, and a thickness ratio of the first film to the second film is greater than 0 and less than or equal to 0.28.
In some embodiments, in one film set of the plurality of film sets, the thickness ratio of the first film to the second film is 0.01˜0.27.
In some embodiments, in one film set of the plurality of film sets, a thickness of the first film is 0.08-0.50 times of a quarter of a wavelength of incident light, and a thickness of the second film is 1.80-6.20 times of a quarter of the wavelength of the incident light.
In some embodiments, in one film set of the plurality of film sets, a thickness of the first film is less than or equal to 0.5 times of one quarter of a wavelength of the incident light, and a thickness of the second film is greater than or equal to 1.80 times of one quarter of the wavelength of the incident light. Or, in each film set of the plurality of film sets, the thickness of the first film is less than or equal to 0.5 times of one quarter of the wavelength of the incident light, and the thickness of the second film is greater than or equal to 1.80 times of one quarter of the wavelength of the incident light.
In some embodiments, in one of the film sets, a thickness of the first film is 0.2 times of a quarter of a wavelength of an incident light, and a thickness of the second film is 2 times of a quarter of the wavelength of the incident light.
In some embodiments, in one of the film sets, a material of the first film is titanium dioxide, tantalum pentoxide, niobium pentoxide, silicon oxide, silicon nitride, tin dioxide or zinc sulfide.
In some embodiments, a material of the second film is silicon dioxide, magnesium fluoride, barium fluoride, aluminum fluoride or strontium fluoride.
In some embodiments, the first film of each of the film sets contacts the second film of another adjacent film set, and the first film of each of the film sets is closer to the light incidence end than the second film.
In some embodiments, the thickness ratio of the first film to the second film of each of the film sets is the same. Or, the thickness ratio of the first film to the second film of one of the film sets is different from the thickness ratio of the first film to the second film of another of the film sets.
After studying the detailed description in conjunction with the following drawings, other aspects and advantages of the present invention will be discovered:
In the following detailed description, many specific details are set forth in order to provide a thorough understanding of the invention. However, those skilled in the art will understand that the invention can be practiced without these specific details. In other cases, well-known methods, processes, and/or elements are not described in detail so as not to obscure the invention.
Referring to
The first film 31 is a high refractive film, and the second film 32 is a low refractive film, so the refractive index of the first film 31 is greater than that of the second film 32. The materials of the first film 31 include, for example, but are not limited to, titanium dioxide, tantalum pentoxide, niobium pentoxide, silicon oxide, silicon nitride, tin dioxide, zinc sulfide or other existing optical coating materials. The materials of the second film 32 include, for example, but are not limited to, silicon dioxide, magnesium fluoride, barium fluoride, aluminum fluoride, strontium fluoride or other existing optical coating materials.
The thickness ratio of the first film 31 to the second film 32 of at least one of the film sets 30 is about greater than 0 and less than or equal to 0.28 (that is, the thickness of the first film 31 is at least less than or equal to about 0.28 times the thickness of the second film 32), preferably 0.01˜0.27.
For example, the thickness ratio of the first film 31 to the second film 32 is about 0.02, 0.03, 0.06, 0.08, 0.09 or 0.10. Specifically, in at least one of the film sets 30, the thickness of the first film 31 is, for example, but not limited to, equal to or less than about 0.08˜0.50 times of ¼λ, preferably 0.09˜0.48 times of ¼λ, such as, but not limited to, 0.10, 0.11, 0.18, 0.19, 0.20, 0.23 or 0.24 times of ¼λ; and the thickness of the second film 32 is, for example, but not limited to equal to or greater than about 1.80˜6.20 times of ¼λ, preferably 1.82˜6.18 times of ¼λ, such as, but not limited to, 1.85, 2.0, 2.17, 2.18, 2.2, 3.8, 3.81, 3.82, 3.90, 3.94 or 6.18 times of ¼λ. λ is the wavelength of the incident light.
In the invention, by arranging a thinner first film 31 and a thicker second film 32 in the same film set 30, the spectral shift of the optical film structure 3 at the light incident angle of 0 degree to 30 degrees can be greater than or equal to 30 nm, so as to achieve the purpose of high angle (i.e., the incident angle is greater than or equal to 30 degrees) and high spectral shift.
In this way, the optical film structure 3 can be applied to various devices or components that require their filtering properties to change with the different incident angles of light, such as, but not limited to, devices or components that have the function of anti-spy, color changing with the different incident angles of light, or wavelength filtering changing with the different incident angles of light.
The following examples of the optical film structure 3 with different film configurations are presented for a transmittance test to illustrate the spectral shift of the optical film structure 3 of the invention. For the convenience of explanation and test, the optical film structure 3 of these examples adopts the film configuration containing only four film sets 30, namely, the film set 30_1 to the film set 30_4, and N=4.
In the four film sets 30 of the optical film structure 3 of the first example, these four film sets 30 have the same thickness, and the thickness ratio of the first film 31 to the second film 32 of each film set 30 is the same. The thickness of the first film 31 of each film set 30 is about 0.2 times of ¼λ, and the thickness of the second film 32 is about 2 times ¼λ.
The transmittance test is to set the optical film structure 3 of the first example in the test environment as shown in
In the four film sets 30 of the optical film structure 3 of the second example, the thicknesses of these four film sets 30 are the same, and the thickness ratio of the first film 31 to the second film 32 of each film set 30 is the same. The thickness of the first film 31 of each film set 30 is about 0.5 times of ¼λ, and the thickness of the second film 32 is about 1.85 times of ¼λ.
The transmittance test is to set the optical film structure 3 of the second example in the test environment as shown in
In the four film sets 30 of the optical film structure 3 of the third example, the thickness of at least two film sets 30 can be different, for example, and the thickness ratio of the first film 31 to the second film 32 of each film set 30 is different. For the film set 30_1, the thickness of the first film 31 is about 0.1089 times of ¼λ, and the thickness of the second film 32 is about 3.9434 times of ¼λ. For the film set 30_2, the thickness of the first film 31 is about 0.0895 times of ¼λ, and the thickness of the second film 32 is about 6.182 times of ¼λ. For the film set 30_3, the thickness of the first film 31 is about 0.1861 times of ¼λ, and the thickness of the second film 32 is about 2.1758 times of ¼λ. For the film set 30_4, the thickness of the first film 31 is about 0.2396 times of ¼λ, and the thickness of the second film 32 is about 3.8189 times of ¼λ.
The transmittance test is to set the optical film structure 3 of the third example in the test environment as shown in
It can be seen from the above tests that the greater the thickness difference between the first film 31 and the second film 32 of each film set 30, the more obvious the spectral shift may become. The smaller the thickness ratio of the first film 31 to the second film 32 of each film set 30, the more obvious the spectral shift may become. Stacking at least two film sets 30 with different thickness ratios of the first film 31 to the second film 32 may also make the spectral shift more obvious.
Although the invention is disclosed as above with the aforementioned embodiments, these embodiments are not intended to limit the invention. Without departing from the spirit and scope of the invention, the combination of changes, retouching and various embodiments belongs to the scope of claims of the invention. For the scope of protection defined by the invention, please refer to the attached claims.
Number | Date | Country | Kind |
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111117757 | May 2022 | TW | national |