WO2019189039A1 - Optical filter - Google Patents

Optical filter Download PDF

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Publication number
WO2019189039A1
WO2019189039A1 PCT/JP2019/012619 JP2019012619W WO2019189039A1 WO 2019189039 A1 WO2019189039 A1 WO 2019189039A1 JP 2019012619 W JP2019012619 W JP 2019012619W WO 2019189039 A1 WO2019189039 A1 WO 2019189039A1
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Prior art keywords
thin film
wavelength
film laminated
laminated structure
optical filter
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PCT/JP2019/012619
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French (fr)
Japanese (ja)
Inventor
満幸 舘村
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Agc株式会社
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Application filed by Agc株式会社 filed Critical Agc株式会社
Priority to CN201980023579.4A priority Critical patent/CN111954833B/en
Priority to JP2020510830A priority patent/JP7215476B2/en
Publication of WO2019189039A1 publication Critical patent/WO2019189039A1/en

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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B32LAYERED PRODUCTS
    • B32BLAYERED PRODUCTS, i.e. PRODUCTS BUILT-UP OF STRATA OF FLAT OR NON-FLAT, e.g. CELLULAR OR HONEYCOMB, FORM
    • B32B7/00Layered products characterised by the relation between layers; Layered products characterised by the relative orientation of features between layers, or by the relative values of a measurable parameter between layers, i.e. products comprising layers having different physical, chemical or physicochemical properties; Layered products characterised by the interconnection of layers
    • B32B7/02Physical, chemical or physicochemical properties
    • B32B7/023Optical properties
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/20Filters
    • G02B5/22Absorbing filters
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/20Filters
    • G02B5/26Reflecting filters
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/20Filters
    • G02B5/28Interference filters

Definitions

  • the present invention relates to an optical filter. Specifically, the present invention relates to an optical filter that restricts transmission of light having a wavelength in the near infrared region.
  • ambient light sensors have been used in devices such as smartphones, game machine bodies, and game machine controllers (see, for example, Patent Document 1).
  • the ambient light sensor is provided inside the device, detects ambient light around the device, which is taken in through the window of the housing of the device, and controls the brightness of the display based on the detection result.
  • the ambient light sensor measures the intensity of visible light in the detected ambient light. Therefore, the ambient light sensor uses an optical filter such as a near-infrared cut filter that cuts extra wavelength components such as light in the near-infrared region.
  • an optical filter such as a near-infrared cut filter that cuts extra wavelength components such as light in the near-infrared region.
  • Near-infrared cut filters are often used in solid-state imaging devices.
  • an optical multilayer film in which a high-refractive index film and a low-refractive index film are stacked with a predetermined film thickness and number of layers is formed on a substrate. Composed. The light incident on the near-infrared cut filter is cut at a wavelength in the near-infrared region by the optical multilayer film on the substrate, and only visible light is transmitted (see, for example, Patent Document 2).
  • the thickness of the device casing in which the ambient light sensor is provided has become very thin. For this reason, the distance from the window (opening) of the housing to the ambient light sensor is shortened, so that light is incident on the ambient light sensor from a wider angle (high incident angle).
  • the optical multilayer film described above has an incident angle dependency. Specifically, it is known that when the incident angle of light increases (the incident light angle increases with respect to the normal direction of the optical multilayer film surface), the light transmission characteristics shift to the short wavelength side. Yes. In addition, a phenomenon has been observed in which the transmittance in the visible light region of light having a high incident angle is partially reduced in the light transmitted through the optical multilayer film. In general, in a solid-state imaging device, it is only necessary to consider the incident angle of light from about 0 ° to about 35 °.
  • the ambient light sensor needs to have desired optical characteristics with respect to light with a high incident angle, and at a higher incident angle than a near-infrared cut filter used in a conventional solid-state imaging device.
  • an optical filter that can obtain desired optical characteristics, and improvement of optical characteristics is achieved by various methods (see, for example, Patent Documents 3 and 4).
  • An object of the present invention is to provide an optical filter having high visible light transmittance and low incidence angle dependency even for light incident at a wide angle.
  • the optical filter according to the present invention is an optical filter including a transparent substrate and three or more thin film laminated structures that limit transmission of light in a predetermined wavelength range in the near-infrared wavelength region, Each of the thin film stack structures is stacked on one surface of the transparent substrate, and at least two of the three or more thin film stack structures have a wavelength range that limits transmission.
  • the wavelength ranges in which transmission is limited by the three or more thin film multilayer structures are different, and the thin film multilayer structure disposed on the same surface side of at least one of the transparent substrates is transparent.
  • the limiting wavelength region is discontinuous.
  • the visible light transmittance is high even for light incident at a wide angle, and the incident angle dependency can be reduced. Therefore, it can be suitably used not only as an environmental sensor but also as an optical filter for a solid-state imaging device.
  • FIG. 1 is a cross-sectional view illustrating an optical filter according to the first embodiment.
  • FIG. 2 is a diagram illustrating optical characteristics of the optical filter according to the first embodiment.
  • FIG. 3 is a diagram illustrating optical characteristics (wavelengths 850 to 1050 nm) of the optical filter according to the first embodiment.
  • FIG. 4 is a diagram illustrating optical characteristics of the thin film laminated structure on one surface of the optical filter according to the first example.
  • FIG. 5 is a diagram illustrating optical characteristics of the thin film laminated structure on the other surface of the optical filter according to the first embodiment.
  • FIG. 6 is a diagram illustrating optical characteristics of the optical filter according to the second embodiment.
  • FIG. 1 is a cross-sectional view illustrating an optical filter according to the first embodiment.
  • FIG. 2 is a diagram illustrating optical characteristics of the optical filter according to the first embodiment.
  • FIG. 3 is a diagram illustrating optical characteristics (wavelengths 850 to 1050 nm) of the optical filter according to the first embodiment.
  • FIG. 7 is a diagram illustrating optical characteristics (wavelengths 850 to 1050 nm) of the optical filter according to the second embodiment.
  • FIG. 8 is a diagram illustrating optical characteristics of the thin film laminated structure on one surface of the optical filter according to the second embodiment.
  • FIG. 9 is a diagram illustrating optical characteristics of the thin film laminated structure on the other surface of the optical filter according to the second embodiment.
  • FIG. 10 is a diagram illustrating optical characteristics of the optical filter according to the third embodiment.
  • FIG. 11 is a diagram illustrating optical characteristics (wavelength 850 to 1050 nm) of the optical filter according to the third embodiment.
  • FIG. 12 is a diagram illustrating optical characteristics of the thin film laminated structure on one surface of the optical filter according to the third embodiment.
  • FIG. 13 is a diagram illustrating optical characteristics of the thin film laminated structure on the other surface of the optical filter according to the third embodiment.
  • FIG. 14 is a diagram illustrating the optical characteristics of the optical filter according to the first comparative example.
  • FIG. 15 is a diagram showing the optical characteristics (wavelength 850 to 1050 nm) of the optical filter according to Comparative Example 1.
  • FIG. 16 is a diagram showing optical characteristics of the thin film laminated structure on one surface of the optical filter according to Comparative Example 1.
  • FIG. 17 is a diagram showing optical characteristics of the thin film laminated structure on the other surface of the optical filter according to Comparative Example 1.
  • FIG. 18 is a diagram illustrating optical characteristics of the optical filter according to Comparative Example 2.
  • FIG. 19 is a diagram showing the optical characteristics (wavelength 850 to 1050 nm) of the optical filter according to Comparative Example 2.
  • FIG. 20 is a diagram illustrating optical characteristics of the thin film laminated structure on one surface of the optical filter according to Comparative Example 2.
  • the optical filter of the present invention includes a transparent substrate and three or more thin film laminated structures that restrict transmission of light in a predetermined wavelength range within the near infrared wavelength region, and each of the thin film laminated structures. Is laminated on one surface of the transparent substrate.
  • at least two of the three or more thin-film stacked structures have different wavelength ranges for limiting transmission, and the wavelengths for which transmission is limited by the three or more thin-film stacked structures. The range is continuous.
  • positioned at the same surface side of at least one of a transparent substrate is discontinuous.
  • transmission-limited wavelength range a phenomenon in which the transmittance partially decreases in a predetermined wavelength range (hereinafter referred to as “reflection ripple”) is likely to occur.
  • a general method for suppressing the reflection ripple is to use a thin film laminated structure having a narrow transmission limiting wavelength range. When this is applied, the transmittance is partially in a predetermined wavelength range in the near infrared wavelength region. May occur (hereinafter referred to as “transmission ripple”). Therefore, in an optical filter using a conventional technique, it is very difficult to achieve both suppression of reflection ripples in the visible wavelength band and suppression of transmission ripples in the near infrared wavelength region.
  • the cause of the decrease in the transmittance in the red region of the optical filter is mostly glass absorption or the shift of the near-infrared region in the near-infrared region to the short wavelength side due to the change in incident angle.
  • the amount of change is greatly influenced by the design of the optical system and can be expected.
  • the main reason for the decrease in transmittance in the blue and green regions is the generation of huge reflection ripples caused by a shift in the design balance of the short-pass filter that forms the stopband in the near-infrared wavelength region. It is difficult to predict the amount of change.
  • the green region is an important region that is frequently used in image processing, and the blue region is a region that requires a higher amount of light due to a problem such as low original susceptibility. Therefore, the optical filter in which the reflection ripples in the blue and green regions are suppressed (inhibition of the decrease in transmittance) can be suitably used as an image sensor such as a CCD or a CMOS or other optical sensor.
  • the optical filter of the present invention since transmission of light having a wavelength in the near-infrared region is restricted by three or more thin film laminated structures, even if a thin film laminated structure having a narrow transmission limited wavelength range is used. In addition, transmission ripples in the near-infrared wavelength region and reflection ripples in the visible wavelength region are unlikely to occur, and high transmission limiting performance can be maintained even when light is incident at a wide angle.
  • the optical filter 1 includes a transparent substrate 10 and three thin film stacked structures 11, 12, and 13.
  • the thin film laminated structures 11, 12, and 13 are each laminated on one surface of the transparent substrate 10.
  • a thin film laminated structure 12 is laminated on one surface 10a of a transparent substrate 10, and a thin film laminated structure 11 and a thin film laminated structure 13 are laminated on the other surface 10b.
  • the thin film laminated structure 12 may be provided on any surface of the transparent substrate 10, and in this case, the thin film laminated structure 11 and the thin film laminated structure 13 are the same as the thin film laminated structure 12 of the transparent substrate 10. It is provided on the surface opposite to the provided surface.
  • the thin film laminated structure 12 may be laminated on the surface 10b, and the thin film laminated structure 11 and the thin film laminated structure 13 may be laminated on the surface 10a.
  • the thin film laminated structures 11, 12, and 13 each limit the transmission of light in a predetermined wavelength range within the near-infrared wavelength region. Specifically, the thin film laminated structure 11 restricts transmission of light in the first wavelength range included in the near-infrared wavelength region, for example. Similarly, the thin film stack structure 12 transmits light in the second wavelength range included in the near infrared wavelength region, and the thin film stack structure 13 transmits light in the third wavelength range included in the near infrared wavelength region. Limit each. In addition, as for each thin film laminated structure used by this invention, it is preferable that the wavelength range in which transmission of the light within a near-infrared wavelength range is restrict
  • limited is continuous. In other words, each thin-film laminated structure preferably has one light transmission limited wavelength range in the near infrared wavelength region (the light transmission limited wavelength range is not divided into two or more).
  • the first wavelength range is a wavelength range including the range on the shortest wavelength side when the near-infrared wavelength region is divided into three ranges
  • the third wavelength range is the range on the longest wavelength side. It is a wavelength range including.
  • the second wavelength range is a wavelength range including an intermediate range between the first wavelength range and the third wavelength range.
  • the center wavelengths of the first wavelength range, the second wavelength range, and the third wavelength range are the center wavelength of the first wavelength range and the center of the second wavelength range from the short wavelength side to the long wavelength side.
  • the thin film laminated structures 11 and 13 are arranged in the order of the thin film laminated structure 11 and the thin film laminated structure 13 from the glass substrate side. They may be arranged in order. Moreover, the main part of the thin film laminated structure 12 needs to be arrange
  • transmission of the light of an ultraviolet wavelength range for example separately from said each thin film laminated structure.
  • the thin film laminated structure for restricting the transmission of light in the ultraviolet wavelength region is generated in a portion where the transmission restricted wavelength ranges overlap with each other because the transmission restricted wavelength ranges are not continuous with the thin film laminated structures 11, 12, and 13. It is because there is no influence of the transmission ripple which is easy to do.
  • “restrict light transmission” means that light having a predetermined wavelength has a light transmittance of less than 5% when incident at an incident angle of 0 degrees (normal incidence). Say something.
  • “transmission-limited wavelength range is discontinuous” means that the transmission-limited wavelength range is divided by the transmission ripple, and the degree of the transmission ripple is a state where the transmittance is 5% or more.
  • the wavelength range in which the transmission is limited by the thin film laminated structures 11, 12, and 13 is continuous. That is, the range obtained by superimposing the first wavelength range, the second wavelength range, and the third wavelength range includes all the predetermined regions of the near infrared wavelength region.
  • the thin film laminated structure 12 and the thin film laminated structure 13 are thin film laminated structures having a characteristic that reflection ripple of oblique incidence described later is small.
  • the thin film laminated structure 12 is more than the thin film laminated structure 13. It is preferable that all the thin films have a high average refractive index and a small amount of wavelength shift due to the oblique incidence dependence of incident light.
  • Thin-film multilayer structures with these characteristics often have narrower transmission-limited wavelength ranges than usual, but the number of layers of thin-film multilayer structures is increased due to the fundamentally small reflection ripple at oblique incidence. In this case, there is little problem of increase in reflection ripple due to oblique incidence, and it is easy to form a transmission limited wavelength range. Furthermore, since the thin film laminated structure 12 is disposed on a different surface from the others, the problem of transmission ripple caused by the overlapping of the thin film laminated structures is unlikely to occur.
  • the thin film laminated structure 12 can maintain the transmission limiting performance in a specific wavelength region stably at a wide angle by making the wavelength shift amount at the time of oblique incidence very small.
  • the wavelength shift amount at the oblique incidence of the thin film multilayer structure 13 is sufficiently larger than the wavelength shift amount at the oblique incidence of the thin film multilayer structure 12, if the incident angle is large, the transmission limited wavelength in the thin film multilayer structure 13 The range moves to the wavelength band that the thin film laminated structure 12 has been responsible for. Accordingly, the transmission limited wavelength ranges formed by the respective thin film laminated structures always overlap each other, which is preferable because it is easy to maintain the light blocking performance at wavelengths of 800 to 1000 nm.
  • permeability of the optical filter which this invention comprises is 0.05% or less in the wavelength with the lowest transmittance
  • the light transmittance can be measured using a spectrophotometer, for example, a spectrophotometer U4100 manufactured by Hitachi High-Tech Science. Unless otherwise specified, the light transmittance refers to the transmittance at an incident angle of 0 °.
  • the optical filter 1 which has the three thin film laminated structures 11, 12, and 13 was demonstrated above, the number of thin film laminated structures may be four or more.
  • a thin film laminated structure in which the center wavelength in the wavelength range for limiting transmission is longer than the center wavelength of the thin film laminated structures 11, 12, and 13 is additionally provided. be able to. That is, when there are four or more thin film laminated structures, the three thin film laminated structures 11, 12, and 13 described above are thin film laminated structures having a central wavelength in the wavelength range that restricts transmission on the shortest wavelength side, 2 The third is the thin film laminated structure on the short wavelength side, and the third is the thin film laminated structure on the short wavelength side.
  • the number of thin film laminated structures is preferably 3 or more and 7 or less, and particularly preferably 4 or more and 6 or less.
  • the thin film laminated structure is formed so that the transmission limiting wavelengths of the thin film laminated structures laminated on the same surface of the transparent substrate are not continuous. Be placed.
  • four thin-film stacked structures can be alternately stacked on both surfaces of the transparent substrate 10 in order from the shortest central wavelength in the transmission-limited wavelength range.
  • a thin film laminated structure having a second central wavelength in the wavelength range that restricts transmission of light in the near-infrared region is stacked on a different surface from the other thin film laminated structures. Good. By doing so, reflection ripples in the visible wavelength band can be suppressed.
  • the thin film laminated structures 11, 12, and 13 are configured to limit transmission in a desired wavelength range by using, for example, a dielectric multilayer film.
  • the dielectric multilayer film is selected from a low refractive index dielectric film (low refractive index film), a medium refractive index dielectric film (medium refractive index film) and a high refractive index dielectric film (high refractive index film). And a film having an optical function obtained by alternately laminating. By design, it is possible to develop a function of controlling the transmission of light in a specific wavelength region and the light transmission limitation using the interference of light.
  • the low refractive index, the high refractive index, and the medium refractive index mean that the refractive index has a high refractive index, a low refractive index, and an intermediate refractive index relative to the refractive index of the adjacent layer.
  • an optical multilayer film (near-infrared cut filter) having the following configuration can be suitably used as the thin film laminated structure that can reduce the reflection ripple of oblique incidence.
  • a band width of less than 5% is 100 to 280 nm
  • a QWOT (Quater-wave Optical Thickness) of the high refractive index film of the optical multilayer film is T H
  • the medium refractive index When QWOT of the film is T M and QWOT of the low refractive index film is T L , the refractive index of the medium refractive index film is intermediate between the refractive index of the high refractive index film and the refractive index of the low refractive index film.
  • the optical multilayer film has 2T L / (T H + 2T M) where there is no portion where the transmittance is locally reduced by 5% or more in the wavelength range of 400 to 700 nm in the spectral characteristics under normal incidence conditions. ) Is set to 100% and the minimum value is set to 0%, 2T L / (T H + 2T M ) is in the range of 100% to 70%, and the refractive index of the medium refractive index film is high.
  • the optical multilayer film has a local transmittance within a wavelength range of 400 to 700 nm in terms of spectral characteristics under normal incidence conditions.
  • the optical multilayer film includes alternating medium refractive index films having a refractive index of 1.8 to 2.23 at a wavelength of 500 nm and low refractive index films having a refractive index of 1.45 to 1.49 at a wavelength of 500 nm.
  • a wavelength range in which the combination unit of the medium refractive index film and the low refractive index film has a number of 5 or more and 35 or less, and light incident on the optical multilayer film at 0 ° is limited in transmission Is a near-infrared cut filter having a width of 100 nm to 300 nm. This is described in detail in Japanese Patent Application No. 2017-253468 by the applicant.
  • the wavelength range in which the light incident on the optical multilayer film at 0 ° is limited in transmission is not limited to the range described therein.
  • the optical multilayer film is composed of a high refractive index film having a refractive index of 2.0 or more at a wavelength of 500 nm and a low refractive index film having a wavelength of 1.6 or less, and the optical multilayer film has a wavelength of the high refractive index film.
  • the constituent material of the high refractive index film is preferably a material having a refractive index of 2 or more, more preferably 2.2 to 2.7.
  • a constituent material include TiO 2 , Nb 2 O 5 (refractive index: 2.38), Ta 2 O 5 , and composite oxides thereof.
  • the constituent material of the medium refractive index film preferably has a refractive index of more than 1.6 and less than 2, and more preferably 1.62 to 1.92.
  • a constituent material for example, Al 2 O 3 , Y 2 O 3 (refractive index: 1.81), or a composite oxide thereof, a mixture film of Al 2 O 3 and ZrO 2 (refractive index: 1). .67) and the like.
  • the medium refractive index film may be replaced with an equivalent film in which a high refractive index film and a low refractive index film are combined.
  • the constituent material of the low refractive index film preferably has a refractive index of 1.3 to 1.6, for example.
  • Examples of such a constituent material include SiO 2 , SiO x N y , and MgF 2.
  • the number of layers depends on the optical characteristics of the dielectric multilayer film, 50 to 150 layers are preferred. If the total number of laminated layers is less than 50, the blocking performance at a wavelength of 800 nm to 1000 nm may not be sufficient. On the other hand, if the total number of laminated layers exceeds 150, the tact time during the production of the optical filter becomes long, and the warp of the optical filter due to the dielectric multilayer film occurs, which is not preferable.
  • the thinner one is preferable from the viewpoint of reducing the thickness of the optical filter 1 while satisfying the preferable number of laminated layers.
  • it is preferably 5 ⁇ m or more.
  • the thickness is preferably 15 ⁇ m or less.
  • the total film thicknesses of the thin film laminated structures arranged on both surfaces of the transparent substrate 10 are as close as possible to each other.
  • the transparent substrate 10 is also extremely thin. Therefore, when the physical film thickness of the thin film laminated structure on both surfaces of the transparent substrate 10 is greatly different, the optical filter 1 may have a convex warp on the side of the thin film laminated structure having a small physical film thickness.
  • the transmission limiting wavelength range is located on the second short wavelength side among the three thin film laminated structures, and is laminated alone on the surface of the transparent substrate 10. It is preferable that the physical film thickness of the thin film laminated structure 12 is larger than the other two thin film laminated structures 11 and 13. That is, the physical film thickness of the thin film laminated structure 12 having the center wavelength located at the second shortest wavelength among the central wavelengths in the transmission limited wavelength range of the three thin film laminated structures 11, 12, 13 is other than that It is preferably thicker than the physical film thickness of the two thin film laminated structures 11 and the thin film laminated structure 13. Thereby, the difference of the thickness of the whole thin film laminated structure in the both surfaces of the transparent substrate 10 when laminated
  • dielectric multilayer film thin film laminated structure
  • dry film formation processes such as IAD (Ion Assisted Deposition) deposition method, CVD method, sputtering method, vacuum deposition method, spray method, dipping method, etc.
  • a wet film formation process such as can be used.
  • the transparent substrate 10 is a material that transmits visible light.
  • glass glass ceramics, crystal such as crystal, sapphire, resin (polyester resin such as polyethylene terephthalate (PET), polybutylene terephthalate (PBT), polyolefin resin such as polyethylene, polypropylene, ethylene vinyl acetate copolymer, norbornene resin
  • PET polyethylene terephthalate
  • PBT polybutylene terephthalate
  • polyolefin resin such as polyethylene, polypropylene, ethylene vinyl acetate copolymer
  • norbornene resin Acrylic resins such as polyacrylate and polymethyl methacrylate, urethane resins, vinyl chloride resins, fluororesins, polycarbonate resins, polyvinyl butyral resins, polyvinyl alcohol resins, etc.
  • the transparent substrate 10 preferably has a property of absorbing light having a wavelength in the near infrared region.
  • the transparent substrate 10 has a property of absorbing light in the near-infrared wavelength region, so that the color is close to human visibility characteristics. Correction is possible. Since the thin-film multilayer structures 11, 12, and 13 can provide spectral characteristics with low incident angle dependency, the thin-film multilayer structure is provided on the transparent substrate 10 having the property of absorbing light having a wavelength in the near infrared region. Thus, an excellent spectral characteristic that restricts transmission of light having a wavelength in the near infrared region can be obtained. Therefore, it becomes possible to obtain the optical filter 1 having good characteristics as a near-infrared cut filter for a solid-state imaging device.
  • the transparent substrate 10 having the property of absorbing light having a wavelength in the near infrared region is a glass having the ability to transmit light in the visible light region and absorb light in the near infrared region, such as CuO-containing fluorophosphate glass.
  • it is preferably composed of a CuO-containing phosphate glass (hereinafter collectively referred to as “CuO-containing glass”).
  • the transparent substrate 10 is composed of CuO-containing glass, so that it has a high transmittance for visible light and a high transmission limiting property for light having a wavelength in the near infrared region.
  • the “phosphate glass” includes silicic acid phosphate glass in which a part of the glass skeleton is composed of SiO 2 .
  • the CuO-containing glass substrate has a feature that absorption of light having a wavelength of 400 to 450 nm is slight, and an absorptance ratio of light having a wavelength of 400 to 450 nm with respect to light having a wavelength of 775 to 900 nm is low. As a result, even if the CuO-containing glass substrate increases the absorption rate by increasing the CuO content so as to sufficiently limit the transmission of light having a wavelength of 775 to 900 nm by absorption, the visible light transmittance does not decrease significantly. Because it is useful.
  • the transparent resin As the transparent substrate 10 having the property of absorbing light having a wavelength in the near infrared region, as a material other than the CuO-containing glass, the transparent resin has a near resin that absorbs light having a wavelength in a specific range in the near infrared region.
  • a near-infrared absorbing substrate containing an infrared-absorbing dye is also included.
  • a near-infrared absorbing layer containing a near-infrared absorbing dye and a transparent resin on the surface of the transparent substrate 10 using the same material as the above-mentioned near-infrared absorbing substrate. May be formed.
  • the near-infrared absorbing layer is formed between the transparent substrate 10 and the thin film laminated structure 11 or the thin film laminated structure 12. Further, the near infrared absorption layer may be formed on at least one surface of the transparent substrate 10.
  • the near-infrared absorbing dye is not particularly limited as long as it is a near-infrared absorbing dye having the ability to transmit light in the visible light region and absorb light in the near infrared region.
  • the dye in the present invention may be a pigment, that is, a state in which molecules are aggregated.
  • cyanine compounds As near-infrared absorbing dyes, cyanine compounds, phthalocyanine compounds, naphthalocyanine compounds, dithiol metal complex compounds, diimonium compounds, polymethine compounds, phthalide compounds, naphthoquinone compounds, anthraquinone compounds, indophenol compounds, Examples include squarylium compounds.
  • squarylium compounds, cyanine compounds and phthalocyanine compounds are more preferred, and squarylium compounds are particularly preferred.
  • a near-infrared absorbing dye made of a squarylium compound is preferred because its absorption spectrum has little absorption of visible light and high storage stability and stability to light.
  • a near-infrared absorbing dye made of a cyanine compound is preferable because of its low absorption of visible light in its absorption spectrum and high light absorption on the long wavelength side in the near-infrared region.
  • cyanine compounds are low-cost, and long-term stability can be secured by salt formation.
  • Near-infrared absorbing dyes composed of phthalocyanine compounds are preferred because they are excellent in heat resistance and weather resistance.
  • the near-infrared absorbing dye one of the above compounds may be used alone, or two or more of them may be used in combination.
  • the transparent resin a transparent resin having a refractive index of 1.45 or more is preferable.
  • the refractive index is more preferably 1.5 or more, and particularly preferably 1.6 or more.
  • the upper limit of the refractive index of the transparent resin is not particularly limited, but is preferably about 1.72 in view of availability.
  • the refractive index means a refractive index at a wavelength of 500 nm unless otherwise specified.
  • Transparent resins include acrylic resin, epoxy resin, ene / thiol resin, polycarbonate resin, polyether resin, polyarylate resin, polysulfone resin, polyethersulfone resin, polyparaphenylene resin, polyarylene ether phosphine oxide resin, polyimide Examples include resins, polyamideimide resins, polyolefin resins, cyclic olefin resins, and polyester resins. As transparent resin, 1 type may be used individually from these resin, and 2 or more types may be mixed and used for it.
  • the transparent resin is at least one selected from acrylic resins, polyester resins, polycarbonate resins, ene / thiol resins, epoxy resins, and cyclic olefin resins. preferable. Further, the transparent resin is more preferably at least one selected from an acrylic resin, a polyester resin, a polycarbonate resin, and a cyclic olefin resin.
  • the polyester resin polyethylene terephthalate resin, polyethylene naphthalate resin and the like are preferable.
  • the near-infrared absorbing layer is, for example, a transparent coating liquid prepared by dissolving or dispersing a near-infrared absorbing dye and a transparent resin or a transparent resin raw material component, and optionally an ultraviolet absorber in a solvent or dispersion medium. It can be produced by coating on the substrate 10, drying, and further curing as necessary.
  • the near-infrared absorbing layer may contain other optional components as required, as long as the effects of the present invention are not impaired, in addition to the near-infrared absorbing dye, the transparent resin, and the optional ultraviolet absorber.
  • other optional components specifically, near infrared rays or infrared absorbers, color tone correction dyes, ultraviolet absorbers, leveling agents, antistatic agents, heat stabilizers, light stabilizers, antioxidants, dispersants, flame retardants , Lubricants, plasticizers and the like.
  • the component added to the coating liquid used when forming the near-infrared absorption layer mentioned later for example, the component derived from a silane coupling agent, a heat
  • the film thickness of the near-infrared absorbing layer is appropriately determined according to the arrangement space in the apparatus to be used and the required absorption characteristics.
  • the film thickness is preferably 0.1 to 100 ⁇ m. If the film thickness is less than 0.1 ⁇ m, the near-infrared absorbing ability may not be sufficiently exhibited. On the other hand, if the film thickness exceeds 100 ⁇ m, the flatness of the film is lowered, and there is a possibility that the absorption rate varies.
  • the film thickness is more preferably 0.5 to 50 ⁇ m. If it exists in this range, sufficient near-infrared absorptivity and flatness of a film thickness can be compatible.
  • the optical filter of the present invention described above, three or more thin film laminated structures having different transmission limiting wavelength ranges are laminated on the surface of the transparent substrate so that the transmission limiting wavelength ranges on the same surface are not continuous. As a result, it is possible to obtain spectral characteristics having high visible light transmittance and high blocking performance in the near infrared region even for light incident at a wide angle.
  • the optical filter of the present invention preferably has a transmittance of 1% or less for light in the near-infrared wavelength region, for example, a wavelength of 800 nm to 1000 nm. Further, it is preferable that the wavelength range in which the light transmittance is less than 0.05% at a wavelength of 800 nm to 1000 nm is 100 nm or more. Further, according to the optical filter of the present invention, it is possible to greatly reduce the decrease in transmittance due to the optical multilayer film in the wavelength range that transmits light having an incident angle of 0 to 50 °. This feature makes it suitable for use as an optical filter for imaging devices such as CCD and CMOS, and other optical sensor applications that can provide images with little flare and ghosting even in environments where near-infrared radiation is frequently used. can do.
  • the optical filter of the present invention can effectively suppress a decrease in transmittance in the visible light region, particularly in the blue and green regions having a wavelength of 430 nm to 560 nm, within a wide angle range where the incident angle of light is 0 to 50 °. . Therefore, the average transmittance in the wavelength range can be 85% or more in a wide range of light incident angles.
  • the transmission of light in the near-infrared wavelength range is surely limited by using a transparent substrate having near-infrared absorption or by providing a near-infrared absorption layer on the surface of the transparent substrate. Therefore, it is possible to obtain an optical filter having more excellent optical characteristics that enables color correction close to human visibility characteristics.
  • the optical filter (near-infrared cut filter) includes a transparent substrate (near-infrared absorbing glass, plate thickness: 0.3 mm, trade name: NF-50T, manufactured by AGC Techno Glass), and one surface of the transparent substrate. And a total of five thin film laminated structures provided on the other surface.
  • Each of the thin film laminated structures has a structure in which a high refractive index film and a low refractive index film are sequentially laminated from the transparent substrate surface side.
  • the four thin-film stacked structures are a repetition of a high refractive index film (titanium oxide (TiO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) having a total of four, 32 layers and a physical film thickness of 3796.98 nm.
  • This is a laminated structure (1-1 thin film laminated structure). That is, the transparent substrate has a first-first thin film laminated structure composed of four thin film laminated structures on one surface.
  • This thin film laminated structure is disposed on the other surface of the transparent substrate.
  • This thin film laminated structure is a repetitive laminated structure of a total of 52 layers of a high refractive index film (titanium oxide (TiO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) and a physical film thickness of 3093.23 nm. (1-2 thin film laminated structure).
  • Table 1 shows the configuration of the thin film laminated structure (1-1 thin film laminated structure) provided on one surface of the transparent substrate of the optical filter.
  • Table 2 shows the configuration of the thin film laminated structure (1-2 thin film laminated structure) provided on the other surface of the transparent substrate of the optical filter.
  • the number of film layers is the ordinal number of layers from the transparent substrate side, and the film thickness indicates the physical film thickness.
  • optical thin film simulation software manufactured by Spectra, Inc.
  • FIGS. 2 and 3 enlarged views in the wavelength region of 850 nm to 1050 nm.
  • the optical characteristics at 0 ° were verified using the optical thin film simulation software. The results are shown in FIG.
  • the wavelength is 970 nm, 1070 nm, and around 1190 nm at 0 ° incidence.
  • the optical filter (near-infrared cut filter) according to this example includes a transparent substrate similar to that used in Example 1, and a thin film laminated structure provided on one surface and the other surface of the transparent substrate. Prepare.
  • Each of the thin film laminated structures has a structure in which films having different refractive indexes are sequentially laminated from the transparent substrate surface side.
  • Two thin film laminated structures are disposed on one surface of the transparent substrate.
  • the two thin film laminated structures have a total of 50 layers and a physical film thickness of 5930.11 nm.
  • the two thin-film laminated structures have a total of 30 layers of a high refractive index film (zirconium oxide (ZrO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) provided on the transparent substrate side.
  • High refractive index film titanium oxide (TiO 2 )
  • medium refractive index provided on the laminated structure 2-1 thin film laminated structure
  • the 2-1 thin film laminated structure air side
  • It consists of a total of 20 layers of repeated lamination structure (second thin film laminated structure) with a film (aluminum oxide (Al 2 O 3 )).
  • This thin film laminated structure is disposed on the other surface of the transparent substrate.
  • This thin film laminated structure is a repetitive laminated structure having a total of 60 layers of a high refractive index film (titanium oxide (TiO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) and a physical film thickness of 3570.77 nm. (2-3 thin film laminated structure).
  • Table 3 shows the structures of the thin film laminated structures (2-1 thin film laminated structure and 2-2 thin film laminated structure) provided on one surface of the transparent substrate of the optical filter.
  • Table 4 shows the configuration of the thin film laminated structure (second-3 thin film laminated structure) provided on the other surface of the transparent substrate of the optical filter.
  • the number of film layers is the ordinal number of layers from the transparent substrate side, and the film thickness indicates the physical film thickness.
  • optical thin film simulation software manufactured by Spectra, Inc.
  • FIGS. 6 and 7 enlarged views in the wavelength region of 850 nm to 1050 nm.
  • the thin film laminated structure (the 2-1 thin film laminated structure and the 2-2 thin film laminated structure) provided on one surface of the transparent substrate (excluding the influence of light absorption by the transparent substrate) ) was verified using the optical thin film simulation software.
  • the optical characteristics at 0 ° were verified using the optical thin film simulation software.
  • the results are shown in FIG.
  • the optical filter (near-infrared cut filter) according to this example includes a transparent substrate similar to that used in Example 1, and a thin film laminated structure provided on one surface and the other surface of the transparent substrate. Prepare.
  • Each of the thin film laminated structures has a structure in which films having different refractive indexes are sequentially laminated from the transparent substrate surface side.
  • Two thin film laminated structures are disposed on one surface of the transparent substrate.
  • the two thin film laminated structures have a total of 44 layers and a physical film thickness of 5738.57 nm.
  • the two thin-film laminated structures have a total of 16 layers of a high refractive index film (zirconium oxide (ZrO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) provided on the transparent substrate side.
  • High refractive index film titanium oxide (TiO 2 )
  • medium refractive index film provided on the laminated structure (3-1 thin film laminated structure) and the 3-1 thin film laminated structure (air side) It consists of a total of 28 layers (3-2 thin film layered structure) with a film (silicon oxide (SiO 2 )).
  • This thin film laminated structure is disposed on the other surface of the transparent substrate.
  • This thin film laminated structure is a repetitive laminated structure having a total of 30 layers of a high refractive index film (zirconium oxide (ZrO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) and a physical film thickness of 3656.75 nm.
  • ZrO 2 zirconium oxide
  • SiO 2 silicon oxide
  • Table 5 shows the configuration of the thin film laminated structure (3-1 thin film laminated structure and 3-2 thin film laminated structure) provided on one surface of the transparent substrate of the optical filter.
  • Table 6 shows the configuration of the thin film stack structure (3-3 thin film stack structure) provided on the other surface of the transparent substrate of the optical filter.
  • the number of film layers is the ordinal number of layers from the transparent substrate side, and the film thickness indicates the physical film thickness.
  • optical thin film simulation software manufactured by Spectra, Inc.
  • FIGS. 10 and 11 enlarged views in the wavelength region of 850 nm to 1050 nm.
  • the optical filter (near infrared cut filter) according to this comparative example includes the same transparent substrate as that used in Example 1.
  • a plurality of thin film laminated structures are provided on only one surface of the transparent substrate.
  • This thin film laminated structure has a structure in which a high refractive index film and a low refractive index film are sequentially laminated from the transparent substrate surface side.
  • This thin film laminated structure is a repetitive laminated structure having a total of 40 layers of a high refractive index film (titanium oxide (TiO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) and a physical film thickness of 5151.58 nm. is there. That is, five thin film laminated structures having the same configuration are laminated on one surface of the transparent substrate.
  • the optical multilayer film provided on the other surface of the transparent substrate is an antireflection film.
  • Each of the optical multilayer films has a high-refractive index film of titanium oxide (TiO 2 ) and a low-refractive index film of silicon oxide (SiO 2 ). is there.
  • Table 3 shows the configuration of the thin film laminated structure provided on one surface of the transparent substrate of the optical filter.
  • Table 4 shows the configuration of the optical multilayer film provided on the other surface of the transparent substrate of the optical filter.
  • the number of film layers is the ordinal number of layers from the transparent substrate side, and the film thickness indicates the physical film thickness.
  • optical thin film simulation software (TFCalc, manufactured by Spectra, Inc.). The results are shown in FIGS. 14 and 15 (enlarged views in the wavelength region of 850 nm to 1050 nm). Further, the optical thin film simulation software described above shows the optical characteristics at the incident angles of 0 °, 40 ° and 50 ° of only the thin film laminated structure (excluding the influence of light absorption by the transparent substrate) provided on one surface of the transparent substrate. It verified using. The results are shown in FIG.
  • optical thin film simulation software described above shows the optical characteristics at the incident angles of 0 °, 40 ° and 50 ° of only the optical multilayer film provided on the other surface of the transparent substrate (excluding the influence of light absorption by the transparent substrate). Used to verify. The results are shown in FIG.
  • the optical filter (near-infrared cut filter) according to this comparative example includes a transparent substrate similar to that used in Example 1, and includes a thin film laminated structure only on one surface of the transparent substrate.
  • This thin film laminated structure has a structure in which a high refractive index film and a low refractive index film are sequentially laminated from the transparent substrate surface side.
  • Each of the five thin film laminated structures has a medium refractive index film (zirconium titanium (ZrO 2 )), a low refractive index film (silicon oxide (SiO 2 )), and a high refractive index film (titanium oxide (TiO 2 )).
  • a repetitive laminated structure having a total thickness of 56 and a physical film thickness of 7647.11 nm (third thin film laminated structure).
  • the first layer to the twentieth layer have a repeated laminated structure in which the medium refractive index film and the low refractive index film are alternately laminated from the transparent substrate side.
  • Up to the 56th layer is a repeated laminated structure in which high refractive index films and low refractive index films are alternately laminated. That is, this optical filter has five thin film laminated structures on one surface of a transparent substrate.
  • the optical multilayer film provided on the other surface of the transparent substrate is an antireflection film.
  • This optical multilayer film is the same optical multilayer film as used in Comparative Example 1. Therefore, description of the film configuration and spectral characteristics is omitted.
  • Table 9 shows the configuration of the thin film laminated structure (third thin film laminated structure) provided on one surface of the transparent substrate of the optical filter.
  • the number of film layers is the ordinal number of layers from the transparent substrate side, and the film thickness indicates the physical film thickness.
  • the optical characteristic in incident angles 0 degree, 40 degrees, and 50 degrees was verified using optical thin film simulation software (TFCalc, product made by Software Spectra). The results are shown in FIGS. 18 and 19 (enlarged views in the wavelength region of 850 nm to 1050 nm).
  • optical thin film simulation software described above shows the optical characteristics at the incident angles of 0 °, 40 ° and 50 ° of only the thin film laminated structure (excluding the influence of light absorption by the transparent substrate) provided on one surface of the transparent substrate. It verified using. The results are shown in FIG.
  • the optical filter of Example 1 has a transmittance of 850 nm to 990 nm in the near infrared region of 0.1% or less in the near infrared region even when the incident angle of light is 40 ° and 50 °, and the transmission ripple Is suppressed.
  • the transmittance in the visible region (450 nm to 550 nm) is 92% or more at the minimum even when the incident angle of light is 40 °, and the transmittance in the visible region is equal even when the incident angle of light is 50 °.
  • the minimum value is 81% or more, and the reflection ripple is suppressed.
  • it has a transmittance of 0.0001% or less at wavelengths of 898 nm to 955 nm, and has a high near infrared absorption ability.
  • the optical filter of Comparative Example 1 has a minimum transmittance of 80% or less in the visible region (450 nm to 550 nm) at a light incident angle of 50 °, and the reflection ripple cannot be suppressed.
  • the optical filter of Comparative Example 2 has a minimum transmittance of 80% or less in the visible region (450 nm to 550 nm) at a light incident angle of 50 °, and the reflection ripple cannot be suppressed. Further, even when the incident angle of light is 0 °, 40 °, and 50 °, the transmittance in the near infrared region (850 nm to 990 nm) is 0.1% or more, and the transmission ripple cannot be suppressed.

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Abstract

This invention pertains to an optical filter (1) comprising: a transparent substrate (10); and three or more thin-film laminated structures (11), (12) and (13) which respectively restrict the passage of light having predetermined wavelength ranges within the near-infrared wavelength region. Each of the thin-film laminated structures is laminated on one surface of the transparent substrate (10), and the wavelength ranges for which the passage of light is restricted are different to one another for at least two of the three or more thin-film laminated structures (11), (12) and (13). The wavelength ranges for which the passage of light is restricted by the three or more thin-film laminated structures (11), (12) and (13) are contiguous, and the wavelength regions for which the passage of light is restricted by the thin-film laminated structures (11) and (13) positioned on the same side of the transparent substrate (10) are not contiguous.

Description

光学フィルタOptical filter
 本発明は、光学フィルタに関する。詳しくは、近赤外領域の波長の光の透過を制限する光学フィルタに関する。 The present invention relates to an optical filter. Specifically, the present invention relates to an optical filter that restricts transmission of light having a wavelength in the near infrared region.
 近年、スマートフォン、ゲーム機本体やゲーム機のコントローラ等の機器に、環境光センサが用いられている(例えば、特許文献1参照。)。環境光センサは、機器内部に設けられ、上記機器の筐体の窓部を通して取り入れられた、機器周囲の環境光を検出し、その検出結果によりディスプレイの輝度を制御する。 In recent years, ambient light sensors have been used in devices such as smartphones, game machine bodies, and game machine controllers (see, for example, Patent Document 1). The ambient light sensor is provided inside the device, detects ambient light around the device, which is taken in through the window of the housing of the device, and controls the brightness of the display based on the detection result.
 環境光センサは、検出した環境光における可視光の強度を測定する。そのため、環境光センサには、近赤外領域の光など、余計な波長成分をカットする近赤外線カットフィルタ等の光学フィルタが用いられている。 The ambient light sensor measures the intensity of visible light in the detected ambient light. Therefore, the ambient light sensor uses an optical filter such as a near-infrared cut filter that cuts extra wavelength components such as light in the near-infrared region.
 近赤外線カットフィルタは、固体撮像装置で用いられることが多く、例えば、基板上に、高屈折率膜と低屈折率膜とを所定の膜厚及び層数で積層した光学多層膜を形成して構成される。近赤外線カットフィルタに入射した光は、基板上の光学多層膜によって近赤外領域の波長の光がカットされ、可視光のみが透過される(例えば、特許文献2参照。)。 Near-infrared cut filters are often used in solid-state imaging devices. For example, an optical multilayer film in which a high-refractive index film and a low-refractive index film are stacked with a predetermined film thickness and number of layers is formed on a substrate. Composed. The light incident on the near-infrared cut filter is cut at a wavelength in the near-infrared region by the optical multilayer film on the substrate, and only visible light is transmitted (see, for example, Patent Document 2).
 スマートフォンやゲーム機の薄型化の進展に伴い、環境光センサが設けられる機器筐体の厚さが非常に薄くなっている。そのため、筐体の窓部(開口部)から環境光センサまでの距離が短くなることで、環境光センサに対して、より広角度(高入射角)から光が入射されるようになった。 With the progress of thinning of smartphones and game machines, the thickness of the device casing in which the ambient light sensor is provided has become very thin. For this reason, the distance from the window (opening) of the housing to the ambient light sensor is shortened, so that light is incident on the ambient light sensor from a wider angle (high incident angle).
 前述の光学多層膜は、入射角依存性がある。具体的には、光の入射角度が大きくなる(光学多層膜表面の法線方向に対する、入射する光の角度が大きくなる)と、光の透過特性が短波長側にシフトすることが知られている。また、光学多層膜を透過した光では、高入射角の光の可視光領域の透過率が部分的に下がるという現象も観測されていた。通常、固体撮像装置では、光の入射角度は0°から35°程度までを配慮すればよい。しかしながら、前述のとおり環境光センサでは、高入射角の光に対して、所望の光学特性を備える必要があり、従来固体撮像装置で用いられる近赤外線カットフィルタと比較して、より高入射角においても所望の光学特性が得られる光学フィルタが求められており、種々の手法で光学特性の向上が図られている(例えば、特許文献3、4参照。)。 The optical multilayer film described above has an incident angle dependency. Specifically, it is known that when the incident angle of light increases (the incident light angle increases with respect to the normal direction of the optical multilayer film surface), the light transmission characteristics shift to the short wavelength side. Yes. In addition, a phenomenon has been observed in which the transmittance in the visible light region of light having a high incident angle is partially reduced in the light transmitted through the optical multilayer film. In general, in a solid-state imaging device, it is only necessary to consider the incident angle of light from about 0 ° to about 35 °. However, as described above, the ambient light sensor needs to have desired optical characteristics with respect to light with a high incident angle, and at a higher incident angle than a near-infrared cut filter used in a conventional solid-state imaging device. In addition, there is a demand for an optical filter that can obtain desired optical characteristics, and improvement of optical characteristics is achieved by various methods (see, for example, Patent Documents 3 and 4).
日本国特開2017-86922号公報Japanese Unexamined Patent Publication No. 2017-86922 日本国特開2006-60014号公報Japanese Unexamined Patent Publication No. 2006-60014 日本国特許第6119747号Japanese Patent No. 6119747 日本国特許第6206410号Japanese Patent No. 6206410
 本発明は、広角度で入射した光に対しても、可視光透過率が高く、入射角依存性の低い光学フィルタの提供を目的とする。 An object of the present invention is to provide an optical filter having high visible light transmittance and low incidence angle dependency even for light incident at a wide angle.
 本発明に係る光学フィルタは、透明基板と、それぞれ近赤外波長領域内の所定の波長範囲の光の透過を制限する、3つ以上の、薄膜積層構造体を備えた光学フィルタであって、各々の前記薄膜積層構造体は前記透明基板のいずれか一方の表面上に積層され、前記3つ以上の薄膜積層構造体のうち少なくとも2つの薄膜積層構造体は、透過を制限する波長範囲がそれぞれ異なっており、前記3つ以上の薄膜積層構造体によって透過が制限される波長範囲が連続しており、前記透明基板の少なくとも一方の同一の表面側に配置される前記薄膜積層構造体が透過を制限する波長領域が不連続である。 The optical filter according to the present invention is an optical filter including a transparent substrate and three or more thin film laminated structures that limit transmission of light in a predetermined wavelength range in the near-infrared wavelength region, Each of the thin film stack structures is stacked on one surface of the transparent substrate, and at least two of the three or more thin film stack structures have a wavelength range that limits transmission. The wavelength ranges in which transmission is limited by the three or more thin film multilayer structures are different, and the thin film multilayer structure disposed on the same surface side of at least one of the transparent substrates is transparent. The limiting wavelength region is discontinuous.
 本発明の光学フィルタによれば、広角度で入射した光に対しても、可視光透過率が高く、入射角依存性を低くすることができる。そのため、環境用センサだけでなく、固体撮像装置用の光学フィルタとしても好適に用いることができる。 According to the optical filter of the present invention, the visible light transmittance is high even for light incident at a wide angle, and the incident angle dependency can be reduced. Therefore, it can be suitably used not only as an environmental sensor but also as an optical filter for a solid-state imaging device.
図1は、第1の実施形態に係る光学フィルタを表す断面図である。FIG. 1 is a cross-sectional view illustrating an optical filter according to the first embodiment. 図2は、実施例1に係る光学フィルタの光学特性を示す図である。FIG. 2 is a diagram illustrating optical characteristics of the optical filter according to the first embodiment. 図3は、実施例1に係る光学フィルタの光学特性(波長850~1050nm)を示す図である。FIG. 3 is a diagram illustrating optical characteristics (wavelengths 850 to 1050 nm) of the optical filter according to the first embodiment. 図4は、実施例1に係る光学フィルタの一方の面の薄膜積層構造体による光学特性を示す図である。FIG. 4 is a diagram illustrating optical characteristics of the thin film laminated structure on one surface of the optical filter according to the first example. 図5は、実施例1に係る光学フィルタの他方の面の薄膜積層構造体による光学特性を示す図である。FIG. 5 is a diagram illustrating optical characteristics of the thin film laminated structure on the other surface of the optical filter according to the first embodiment. 図6は、実施例2に係る光学フィルタの光学特性を示す図である。FIG. 6 is a diagram illustrating optical characteristics of the optical filter according to the second embodiment. 図7は、実施例2に係る光学フィルタの光学特性(波長850~1050nm)を示す図である。FIG. 7 is a diagram illustrating optical characteristics (wavelengths 850 to 1050 nm) of the optical filter according to the second embodiment. 図8は、実施例2に係る光学フィルタの一方の面の薄膜積層構造体による光学特性を示す図である。FIG. 8 is a diagram illustrating optical characteristics of the thin film laminated structure on one surface of the optical filter according to the second embodiment. 図9は、実施例2に係る光学フィルタの他方の面の薄膜積層構造体による光学特性を示す図である。FIG. 9 is a diagram illustrating optical characteristics of the thin film laminated structure on the other surface of the optical filter according to the second embodiment. 図10は、実施例3に係る光学フィルタの光学特性を示す図である。FIG. 10 is a diagram illustrating optical characteristics of the optical filter according to the third embodiment. 図11は、実施例3に係る光学フィルタの光学特性(波長850~1050nm)を示す図である。FIG. 11 is a diagram illustrating optical characteristics (wavelength 850 to 1050 nm) of the optical filter according to the third embodiment. 図12は、実施例3に係る光学フィルタの一方の面の薄膜積層構造体による光学特性を示す図である。FIG. 12 is a diagram illustrating optical characteristics of the thin film laminated structure on one surface of the optical filter according to the third embodiment. 図13は、実施例3に係る光学フィルタの他方の面の薄膜積層構造体による光学特性を示す図である。FIG. 13 is a diagram illustrating optical characteristics of the thin film laminated structure on the other surface of the optical filter according to the third embodiment. 図14は、比較例1に係る光学フィルタの光学特性を示す図である。FIG. 14 is a diagram illustrating the optical characteristics of the optical filter according to the first comparative example. 図15は、比較例1に係る光学フィルタの光学特性(波長850~1050nm)を示す図である。FIG. 15 is a diagram showing the optical characteristics (wavelength 850 to 1050 nm) of the optical filter according to Comparative Example 1. 図16は、比較例1に係る光学フィルタの一方の面の薄膜積層構造体による光学特性を示す図である。FIG. 16 is a diagram showing optical characteristics of the thin film laminated structure on one surface of the optical filter according to Comparative Example 1. 図17は、比較例1に係る光学フィルタの他方の面の薄膜積層構造体による光学特性を示す図である。FIG. 17 is a diagram showing optical characteristics of the thin film laminated structure on the other surface of the optical filter according to Comparative Example 1. 図18は、比較例2に係る光学フィルタの光学特性を示す図である。FIG. 18 is a diagram illustrating optical characteristics of the optical filter according to Comparative Example 2. 図19は、比較例2に係る光学フィルタの光学特性(波長850~1050nm)を示す図である。FIG. 19 is a diagram showing the optical characteristics (wavelength 850 to 1050 nm) of the optical filter according to Comparative Example 2. 図20は、比較例2に係る光学フィルタの一方の面の薄膜積層構造体による光学特性を示す図である。FIG. 20 is a diagram illustrating optical characteristics of the thin film laminated structure on one surface of the optical filter according to Comparative Example 2.
 本発明の光学フィルタは、透明基板と、それぞれ近赤外波長領域内の所定の波長範囲の光の透過を制限する、3つ以上の、薄膜積層構造体を備え、各々の前記薄膜積層構造体は透明基板のいずれか一方の表面上に積層される。そして、3つ以上の薄膜積層構造体のうちの少なくとも2つの薄膜積層構造体は透過を制限する波長範囲がそれぞれ異なっており、かつ、3つ以上の薄膜積層構造体によって透過が制限される波長範囲が連続している。そして、透明基板の少なくとも一方の同一の表面側に配置される薄膜積層構造体による透過制限波長範囲が不連続である。 The optical filter of the present invention includes a transparent substrate and three or more thin film laminated structures that restrict transmission of light in a predetermined wavelength range within the near infrared wavelength region, and each of the thin film laminated structures. Is laminated on one surface of the transparent substrate. In addition, at least two of the three or more thin-film stacked structures have different wavelength ranges for limiting transmission, and the wavelengths for which transmission is limited by the three or more thin-film stacked structures. The range is continuous. And the transmission limiting wavelength range by the thin film laminated structure arrange | positioned at the same surface side of at least one of a transparent substrate is discontinuous.
 従来一般的な、透過を制限する光の波長範囲(以下「透過制限波長範囲」ともいう。)の広い薄膜積層構造体のみを使用した光学フィルタでは光の入射角が大きくなると、可視波長領域の所定の波長範囲において透過率が部分的に低下する現象(以下「反射リップル」という。)が起こり易くなる。他方、反射リップルを抑える一般的な手法は、透過制限波長範囲の狭い薄膜積層構造体を使用することであるが、これを適用すると近赤外波長領域の所定の波長範囲において透過率が部分的に上昇する現象(以下「透過リップル」という。)が発生するおそれがある。そのため、従来技術を用いた光学フィルタにおいては、可視波長帯域における反射リップルの抑制と近赤外波長領域の透過リップルの抑制とを両立させることは非常に難しい。 In a conventional optical filter using only a thin film laminated structure having a wide wavelength range of light for limiting transmission (hereinafter also referred to as “transmission-limited wavelength range”), when the incident angle of light increases, A phenomenon in which the transmittance partially decreases in a predetermined wavelength range (hereinafter referred to as “reflection ripple”) is likely to occur. On the other hand, a general method for suppressing the reflection ripple is to use a thin film laminated structure having a narrow transmission limiting wavelength range. When this is applied, the transmittance is partially in a predetermined wavelength range in the near infrared wavelength region. May occur (hereinafter referred to as “transmission ripple”). Therefore, in an optical filter using a conventional technique, it is very difficult to achieve both suppression of reflection ripples in the visible wavelength band and suppression of transmission ripples in the near infrared wavelength region.
 通常、光学フィルタの赤色領域の透過率の低下の原因としては、ガラスの吸収もしくは、入射角度変化による近赤外領域の透過制限波長範囲の短波長側へのシフトがほとんどである。その変化量は光学系のデザインに大きく影響されるため、予期しうる。これに対し、青色、緑色領域の透過率低下の原因は、近赤外波長領域の阻止帯を形成するショートパスフィルタの設計バランスのずれから生じる巨大な反射リップル発生が主原因であり、透過率変化量の予期が難しい。そして、緑色領域は画像処理上で多用される重要な領域であり、青色領域は元々の感受率が低い等の問題から、より高い光量が必要な領域である。そのため、青色、緑色領域のおける反射リップルの抑制(透過率の低下の抑制)された光学フィルタは、CCDやCMOS等の撮像素子、その他光センサ用途の光学フィルタとして好適に利用することができる。 Usually, the cause of the decrease in the transmittance in the red region of the optical filter is mostly glass absorption or the shift of the near-infrared region in the near-infrared region to the short wavelength side due to the change in incident angle. The amount of change is greatly influenced by the design of the optical system and can be expected. On the other hand, the main reason for the decrease in transmittance in the blue and green regions is the generation of huge reflection ripples caused by a shift in the design balance of the short-pass filter that forms the stopband in the near-infrared wavelength region. It is difficult to predict the amount of change. The green region is an important region that is frequently used in image processing, and the blue region is a region that requires a higher amount of light due to a problem such as low original susceptibility. Therefore, the optical filter in which the reflection ripples in the blue and green regions are suppressed (inhibition of the decrease in transmittance) can be suitably used as an image sensor such as a CCD or a CMOS or other optical sensor.
 本発明の光学フィルタにおいては、近赤外領域の波長の光の透過を、3つ以上の薄膜積層構造体によって制限するため、各々の透過制限波長範囲が狭い薄膜積層構造体を用いたとしても、近赤外波長領域の透過リップル及び可視波長領域の反射リップルが生じにくく、広角度の光の入射に対しても高い透過制限性能を維持することができる。 In the optical filter of the present invention, since transmission of light having a wavelength in the near-infrared region is restricted by three or more thin film laminated structures, even if a thin film laminated structure having a narrow transmission limited wavelength range is used. In addition, transmission ripples in the near-infrared wavelength region and reflection ripples in the visible wavelength region are unlikely to occur, and high transmission limiting performance can be maintained even when light is incident at a wide angle.
 以下、図面を参照して、本発明の実施形態を詳細に説明する。図1に示すように、第1の実施形態に係る光学フィルタ1は、透明基板10と、3つの薄膜積層構造体11、12、13を備えている。薄膜積層構造体11、12、13は、各々、透明基板10のいずれか一方の表面上に積層される。図1においては、透明基板10の一方の表面10a上に薄膜積層構造体12が、他方の表面10b上に、薄膜積層構造体11及び薄膜積層構造体13が積層されている。なお、薄膜積層構造体12は、透明基板10のいずれの表面上に設けられてもよく、この場合、薄膜積層構造体11及び薄膜積層構造体13は、透明基板10の薄膜積層構造体12の設けられた面と反対側の面に設けられる。例えば、薄膜積層構造体12が表面10b上に、薄膜積層構造体11及び薄膜積層構造体13が表面10a上に積層されてもよい。 Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings. As shown in FIG. 1, the optical filter 1 according to the first embodiment includes a transparent substrate 10 and three thin film stacked structures 11, 12, and 13. The thin film laminated structures 11, 12, and 13 are each laminated on one surface of the transparent substrate 10. In FIG. 1, a thin film laminated structure 12 is laminated on one surface 10a of a transparent substrate 10, and a thin film laminated structure 11 and a thin film laminated structure 13 are laminated on the other surface 10b. In addition, the thin film laminated structure 12 may be provided on any surface of the transparent substrate 10, and in this case, the thin film laminated structure 11 and the thin film laminated structure 13 are the same as the thin film laminated structure 12 of the transparent substrate 10. It is provided on the surface opposite to the provided surface. For example, the thin film laminated structure 12 may be laminated on the surface 10b, and the thin film laminated structure 11 and the thin film laminated structure 13 may be laminated on the surface 10a.
 この薄膜積層構造体11、12、13は、それぞれ、近赤外波長領域内の所定の波長範囲の光の透過を制限する。具体的には、薄膜積層構造体11は、例えば、近赤外波長領域に含まれる第1の波長範囲の光の透過を制限する。同様に、薄膜積層構造体12は、近赤外波長領域に含まれる第2の波長範囲を、薄膜積層構造体13は、近赤外波長領域に含まれる第3の波長範囲の光の透過を、それぞれ制限する。なお、本発明で用いられる各薄膜積層構造体は、近赤外波長領域内の光の透過が制限される波長範囲が連続していることが好ましい。言い換えると、各薄膜積層構造体は、近赤外波長領域内において、一つの光透過制限波長範囲を有する(光透過制限波長範囲が二つ以上に分かれていない)ことが好ましい。 The thin film laminated structures 11, 12, and 13 each limit the transmission of light in a predetermined wavelength range within the near-infrared wavelength region. Specifically, the thin film laminated structure 11 restricts transmission of light in the first wavelength range included in the near-infrared wavelength region, for example. Similarly, the thin film stack structure 12 transmits light in the second wavelength range included in the near infrared wavelength region, and the thin film stack structure 13 transmits light in the third wavelength range included in the near infrared wavelength region. Limit each. In addition, as for each thin film laminated structure used by this invention, it is preferable that the wavelength range in which transmission of the light within a near-infrared wavelength range is restrict | limited is continuous. In other words, each thin-film laminated structure preferably has one light transmission limited wavelength range in the near infrared wavelength region (the light transmission limited wavelength range is not divided into two or more).
 薄膜積層構造体11、12、13が透過を制限する波長範囲は互いに異なっている。例えば、第1の波長範囲は、近赤外線波長領域を3つの範囲に分けたときの、最も短波長側の範囲を含む波長範囲であり、第3の波長範囲は、最も長波長側の範囲を含む波長範囲である。第2の波長範囲は、第1の波長範囲と、第3の波長範囲の中間の範囲を含む波長範囲である。この場合、第1の波長範囲、第2の波長範囲、第3の波長範囲の中心波長は、短波長側から長波長側に、第1の波長範囲の中心波長、第2の波長範囲の中心波長、第3の波長範囲の中心波長の順、もしくは、長波長側から短波長側に、第1の波長範囲の中心波長、第2の波長範囲の中心波長、第3の波長範囲の中心波長の順に位置することが好ましい。 The wavelength ranges in which the thin film laminated structures 11, 12, and 13 restrict transmission are different from each other. For example, the first wavelength range is a wavelength range including the range on the shortest wavelength side when the near-infrared wavelength region is divided into three ranges, and the third wavelength range is the range on the longest wavelength side. It is a wavelength range including. The second wavelength range is a wavelength range including an intermediate range between the first wavelength range and the third wavelength range. In this case, the center wavelengths of the first wavelength range, the second wavelength range, and the third wavelength range are the center wavelength of the first wavelength range and the center of the second wavelength range from the short wavelength side to the long wavelength side. Wavelength, in order of the center wavelength of the third wavelength range, or from the long wavelength side to the short wavelength side, the center wavelength of the first wavelength range, the center wavelength of the second wavelength range, and the center wavelength of the third wavelength range It is preferable to position in order.
 また、図1において、薄膜積層構造体11、13は、ガラス基板側から薄膜積層構造体11、薄膜積層構造体13の順で配置されるが、薄膜積層構造体13、薄膜積層構造体11の順で配置されてもよい。また、薄膜積層構造体12の主要部分は薄膜積層構造体11、薄膜積層構造体13が配置される面とは異なる面に配置されることが必要である。つまり、光学フィルタ1が透過を制限する光の阻止量のほとんどは薄膜積層構造体11、薄膜積層構造体13が配置される面とは反対側の薄膜積層構造体12が作り出すことが好ましい。なお、上記各薄膜積層構造体とは別に、例えば紫外波長領域の光の透過を制限する薄膜積層構造体を設けてもよい。紫外波長領域の光の透過を制限るための薄膜積層構造体は、薄膜積層構造体11、12、13と透過制限波長範囲が連続していないため、透過制限波長範囲同士が重なりあう部分に発生しやすい透過リップルの影響がないからである。 In FIG. 1, the thin film laminated structures 11 and 13 are arranged in the order of the thin film laminated structure 11 and the thin film laminated structure 13 from the glass substrate side. They may be arranged in order. Moreover, the main part of the thin film laminated structure 12 needs to be arrange | positioned on the surface different from the surface where the thin film laminated structure 11 and the thin film laminated structure 13 are arrange | positioned. That is, most of the light blocking amount that the optical filter 1 restricts transmission is preferably created by the thin film laminated structure 12 on the side opposite to the surface on which the thin film laminated structure 11 and the thin film laminated structure 13 are arranged. In addition, you may provide the thin film laminated structure which restrict | limits permeation | transmission of the light of an ultraviolet wavelength range, for example separately from said each thin film laminated structure. The thin film laminated structure for restricting the transmission of light in the ultraviolet wavelength region is generated in a portion where the transmission restricted wavelength ranges overlap with each other because the transmission restricted wavelength ranges are not continuous with the thin film laminated structures 11, 12, and 13. It is because there is no influence of the transmission ripple which is easy to do.
 なお、本実施形態の光学フィルタにおいて、「光の透過を制限する」とは、所定の波長の光に関し、入射角0度(垂直入射)で入射した場合の光の透過率が5%未満であることをいう。また、「透過制限波長範囲が不連続」とは、透過リップルによって透過制限波長範囲が分断されることを言い、この透過リップルの程度が透過率5%以上の大きさとなった状態をいう。 In the optical filter according to the present embodiment, “restrict light transmission” means that light having a predetermined wavelength has a light transmittance of less than 5% when incident at an incident angle of 0 degrees (normal incidence). Say something. Further, “transmission-limited wavelength range is discontinuous” means that the transmission-limited wavelength range is divided by the transmission ripple, and the degree of the transmission ripple is a state where the transmittance is 5% or more.
 薄膜積層構造体11、12、13によって透過を制限する波長範囲は、連続している。すなわち、第1の波長範囲、第2の波長範囲、第3の波長範囲を重ね合わせた範囲は、近赤外線波長領域の所定領域のすべてを含む。 The wavelength range in which the transmission is limited by the thin film laminated structures 11, 12, and 13 is continuous. That is, the range obtained by superimposing the first wavelength range, the second wavelength range, and the third wavelength range includes all the predetermined regions of the near infrared wavelength region.
 薄膜積層構造体12と、薄膜積層構造体13は、後述する斜入射の反射リップルが小さい特徴を持つ薄膜積層構造体とすることが好ましく、特に薄膜積層構造体12は薄膜積層構造体13よりも全ての薄膜の平均屈折率が高く、入射光の斜入射依存による波長シフト量が小さいものであることが好ましい。 It is preferable that the thin film laminated structure 12 and the thin film laminated structure 13 are thin film laminated structures having a characteristic that reflection ripple of oblique incidence described later is small. In particular, the thin film laminated structure 12 is more than the thin film laminated structure 13. It is preferable that all the thin films have a high average refractive index and a small amount of wavelength shift due to the oblique incidence dependence of incident light.
 これらの特徴を持つ薄膜積層構造体は、透過制限波長範囲の幅が通常のものより狭いことが多いが、斜入射の反射リップルが根本的に小さいことにより、薄膜積層構造体の層数を増やした場合の斜入射の反射リップル増大の問題が少なく、透過制限波長範囲を形成しやすい。さらに、薄膜積層構造体12がその他とは別の面に配置されるため、薄膜積層構造体同士の重ね合わせによって発生する透過リップルの問題が起きにくい。 Thin-film multilayer structures with these characteristics often have narrower transmission-limited wavelength ranges than usual, but the number of layers of thin-film multilayer structures is increased due to the fundamentally small reflection ripple at oblique incidence. In this case, there is little problem of increase in reflection ripple due to oblique incidence, and it is easy to form a transmission limited wavelength range. Furthermore, since the thin film laminated structure 12 is disposed on a different surface from the others, the problem of transmission ripple caused by the overlapping of the thin film laminated structures is unlikely to occur.
 また、薄膜積層構造体12は、斜入射時の波長シフト量が非常に小さいものとすることで、広角において安定して特定波長域における透過制限性能を維持できる。そして、薄膜積層構造体13の斜入射時の波長シフト量が薄膜積層構造体12の斜入射時の波長シフト量よりも十分に大きい場合、入射角度が大きいと薄膜積層構造体13における透過制限波長範囲が、薄膜積層構造体12が受け持っていた波長帯に移動してくる。それによりそれぞれの薄膜積層構造体が形成する透過制限波長範囲が常に重複することとなり、波長800~1000nmにおける光の阻止性能を維持しやすく好ましい。また、薄膜積層構造体12が受け持つ入射角度0度の波長範囲内のもっとも透過率が低い波長において、本発明が構成する光学フィルタの透過率が0.05%以下であることが好ましい。 Moreover, the thin film laminated structure 12 can maintain the transmission limiting performance in a specific wavelength region stably at a wide angle by making the wavelength shift amount at the time of oblique incidence very small. When the wavelength shift amount at the oblique incidence of the thin film multilayer structure 13 is sufficiently larger than the wavelength shift amount at the oblique incidence of the thin film multilayer structure 12, if the incident angle is large, the transmission limited wavelength in the thin film multilayer structure 13 The range moves to the wavelength band that the thin film laminated structure 12 has been responsible for. Accordingly, the transmission limited wavelength ranges formed by the respective thin film laminated structures always overlap each other, which is preferable because it is easy to maintain the light blocking performance at wavelengths of 800 to 1000 nm. Moreover, it is preferable that the transmittance | permeability of the optical filter which this invention comprises is 0.05% or less in the wavelength with the lowest transmittance | permeability within the wavelength range of the incident angle of 0 degree which the thin film laminated structure 12 has.
 本発明において、光の透過率は、分光光度計、例えば、日立ハイテクサイエンス製分光光度計U4100を用いて測定できる。また、特に指定しない場合、光の透過率とは、入射角が0°における透過率をいうものである。 In the present invention, the light transmittance can be measured using a spectrophotometer, for example, a spectrophotometer U4100 manufactured by Hitachi High-Tech Science. Unless otherwise specified, the light transmittance refers to the transmittance at an incident angle of 0 °.
 なお、上記では、3つの薄膜積層構造体11、12、13を有する光学フィルタ1について説明したが、薄膜積層構造体の数は4つ以上であってもよい。薄膜積層構造体が4つ以上の場合、透過を制限する波長範囲の中心波長が、薄膜積層構造体11、12、13の中心波長よりも長波長側にある薄膜積層構造体を付加的に設けることができる。すなわち、薄膜積層構造体が4つ以上の場合、前述の3つの薄膜積層構造体11、12、13は、透過を制限する波長範囲の中心波長が最も短波長側にある薄膜積層構造体、2番目に短波長側にある薄膜積層構造、及び3番目に短波長側にある薄膜積層構造体である。薄膜積層構造体の数は3つ以上7つ以下が好ましく、4つ以上6つ以下であることが特に好ましい。実施形態の光学フィルタが4つ以上の薄膜積層構造体を有する場合にも、透明基板の同一の表面上に積層される薄膜積層構造体の透過制限波長は連続しないように、薄膜積層構造体が配置される。例えば、透過制限波長範囲の中心波長が短いものから順に4つの薄膜積層構造体について、透明基板10の両表面に交互に積層することができる。或いは、近赤外領域の波長の光の透過を制限する波長範囲の中心波長が2番目に短波長側にある薄膜積層構造体がそれ以外の薄膜積層構造体とは異なる表面に積層されてもよい。このようにすることで、可視波長帯域の反射リップルを抑制することができる。 In addition, although the optical filter 1 which has the three thin film laminated structures 11, 12, and 13 was demonstrated above, the number of thin film laminated structures may be four or more. When there are four or more thin film laminated structures, a thin film laminated structure in which the center wavelength in the wavelength range for limiting transmission is longer than the center wavelength of the thin film laminated structures 11, 12, and 13 is additionally provided. be able to. That is, when there are four or more thin film laminated structures, the three thin film laminated structures 11, 12, and 13 described above are thin film laminated structures having a central wavelength in the wavelength range that restricts transmission on the shortest wavelength side, 2 The third is the thin film laminated structure on the short wavelength side, and the third is the thin film laminated structure on the short wavelength side. The number of thin film laminated structures is preferably 3 or more and 7 or less, and particularly preferably 4 or more and 6 or less. In the case where the optical filter of the embodiment has four or more thin film laminated structures, the thin film laminated structure is formed so that the transmission limiting wavelengths of the thin film laminated structures laminated on the same surface of the transparent substrate are not continuous. Be placed. For example, four thin-film stacked structures can be alternately stacked on both surfaces of the transparent substrate 10 in order from the shortest central wavelength in the transmission-limited wavelength range. Alternatively, even if a thin film laminated structure having a second central wavelength in the wavelength range that restricts transmission of light in the near-infrared region is stacked on a different surface from the other thin film laminated structures. Good. By doing so, reflection ripples in the visible wavelength band can be suppressed.
 次に、本実施形態の光学フィルタ1が有する各構成について説明する。 Next, each configuration of the optical filter 1 of the present embodiment will be described.
 薄膜積層構造体11、12、13は、例えば、誘電体多層膜によって、所望の波長範囲の透過を制限するように構成される。誘電体多層膜は、低屈折率の誘電体膜(低屈折率膜)、中屈折率の誘電体膜(中屈折率膜)及び高屈折率の誘電体膜(高屈折率膜)から選択して交互に積層することで得られる光学的機能を有する膜である。設計により、光の干渉を利用して特定の波長領域の光の透過や、光の透過制限を制御する機能を発現させることができる。なお、低屈折率、高屈折率、中屈折率とは、隣接する層の屈折率に対して高い屈折率と低い屈折率、またその中間の屈折率を有することを意味する。 The thin film laminated structures 11, 12, and 13 are configured to limit transmission in a desired wavelength range by using, for example, a dielectric multilayer film. The dielectric multilayer film is selected from a low refractive index dielectric film (low refractive index film), a medium refractive index dielectric film (medium refractive index film) and a high refractive index dielectric film (high refractive index film). And a film having an optical function obtained by alternately laminating. By design, it is possible to develop a function of controlling the transmission of light in a specific wavelength region and the light transmission limitation using the interference of light. The low refractive index, the high refractive index, and the medium refractive index mean that the refractive index has a high refractive index, a low refractive index, and an intermediate refractive index relative to the refractive index of the adjacent layer.
 本発明の光学フィルタにおいて、斜入射の反射リップルを低減できる薄膜積層構造体としては、以下の構成の光学多層膜(近赤外線カットフィルタ)を好適に用いることができる。 In the optical filter of the present invention, an optical multilayer film (near-infrared cut filter) having the following configuration can be suitably used as the thin film laminated structure that can reduce the reflection ripple of oblique incidence.
 波長500nmにおける屈折率が2.0以上である高屈折率膜と、波長500nmにおける屈折率が1.6以上で前記高屈折率膜の屈折率未満である中屈折率膜と、波長500nmにおける屈折率が1.6未満である低屈折率膜とを備え、前記高屈折率膜をH、前記中屈折率膜をM、前記低屈折率膜をLとしたとき、(LMHML)^n(nは1以上の自然数)の繰り返しで表される繰り返し積層構造を有し、400~700nmの波長範囲に平均透過率が85%以上となる透過帯と、750~1100nmの波長範囲において平均透過率が5%未満の領域の幅が100~280nmである阻止帯とを有し、前記光学多層膜の前記高屈折率膜のQWOT(Quater-wave Optical Thickness)をT、前記中屈折率膜のQWOTをT、前記低屈折率膜のQWOTをTとした場合、前記中屈折率膜の屈折率が前記高屈折率膜の屈折率と前記低屈折率膜の屈折率との中間値以上の場合、前記光学多層膜は、垂直入射条件での分光特性で400~700nmの波長範囲内に透過率が局所的に5%以上低下する箇所が存在しない2T/(T+2T)の最大値を100%、最小値を0%と設定した場合、2T/(T+2T)が100%~70%の範囲内であり、前記中屈折率膜の屈折率が前記高屈折率膜の屈折率と前記低屈折率膜の屈折率との中間値未満の場合、前記光学多層膜は、垂直入射条件での分光特性で400~700nmの波長範囲内に透過率が局所的に5%以上低下する箇所が存在しない(2T+2T)/Tの最大値を100%、最小値を0%と設定した場合、(2T+2T)/Tが100%~70%の範囲内となるように、前記高屈折率膜、前記中屈折率膜及び前記低屈折率膜を積層した近赤外線カットフィルタである。これについては、特許文献3に詳細に記載されている。 A high refractive index film having a refractive index of 2.0 or more at a wavelength of 500 nm, a medium refractive index film having a refractive index of 1.6 or more at a wavelength of 500 nm and less than the refractive index of the high refractive index film, and a refraction at a wavelength of 500 nm. A low refractive index film having a refractive index of less than 1.6, where the high refractive index film is H, the medium refractive index film is M, and the low refractive index film is L, (LMMHML) ^ n (n Is a repetitive laminated structure represented by repetition of a natural number of 1 or more, a transmission band having an average transmittance of 85% or more in a wavelength range of 400 to 700 nm, and an average transmittance in a wavelength range of 750 to 1100 nm. A band width of less than 5% is 100 to 280 nm, and a QWOT (Quater-wave Optical Thickness) of the high refractive index film of the optical multilayer film is T H , and the medium refractive index When QWOT of the film is T M and QWOT of the low refractive index film is T L , the refractive index of the medium refractive index film is intermediate between the refractive index of the high refractive index film and the refractive index of the low refractive index film. When the value is greater than or equal to the value, the optical multilayer film has 2T L / (T H + 2T M) where there is no portion where the transmittance is locally reduced by 5% or more in the wavelength range of 400 to 700 nm in the spectral characteristics under normal incidence conditions. ) Is set to 100% and the minimum value is set to 0%, 2T L / (T H + 2T M ) is in the range of 100% to 70%, and the refractive index of the medium refractive index film is high. When the refractive index is less than the intermediate value between the refractive index of the refractive index film and the refractive index of the low refractive index film, the optical multilayer film has a local transmittance within a wavelength range of 400 to 700 nm in terms of spectral characteristics under normal incidence conditions. most of the no portion to lower than 5% (2T L + 2T M ) / T H 100% value, if the minimum value was set to 0%, (2T L + 2T M) / T H so is in the range of from 100% to 70%, the high-refractive-index film, the intermediate refractive index layer and It is a near infrared cut filter in which the low refractive index film is laminated. This is described in detail in Patent Document 3.
 また、光学多層膜は、波長500nmにおける屈折率が1.8以上2.23以下の中屈折率膜と、波長500nmにおける屈折率が1.45以上1.49以下の低屈折率膜とが交互に積層されてなり、前記中屈折率膜と前記低屈折率膜の組み合わせ単位を5以上35以下の数で有し、前記光学多層膜に0°で入射した光が透過の制限される波長範囲の幅を100nm以上300nm以下とした近赤外線カットフィルタである。これについては、本出願人が特願2017-253468号に詳細に記載した。ただし、光学多層膜に0°で入射した光が透過の制限される波長範囲は、これに記載された範囲に限らない。 The optical multilayer film includes alternating medium refractive index films having a refractive index of 1.8 to 2.23 at a wavelength of 500 nm and low refractive index films having a refractive index of 1.45 to 1.49 at a wavelength of 500 nm. A wavelength range in which the combination unit of the medium refractive index film and the low refractive index film has a number of 5 or more and 35 or less, and light incident on the optical multilayer film at 0 ° is limited in transmission Is a near-infrared cut filter having a width of 100 nm to 300 nm. This is described in detail in Japanese Patent Application No. 2017-253468 by the applicant. However, the wavelength range in which the light incident on the optical multilayer film at 0 ° is limited in transmission is not limited to the range described therein.
 また、光学多層膜は、波長500nmにおける屈折率が2.0以上の高屈折率膜と、1.6以下の低屈折率膜とから構成され、前記光学多層膜は、高屈折率膜の波長500nmにおけるQWOTをQ、低屈折率膜の波長500nmにおけるQWOTをQとしたときに、(a、b、c、d)の基本単位がn個積層された繰り返し構造(ここで、a、b、c、dは、各基本単位における膜の物理膜厚がQWOTの何倍であるかを示す係数であり、またnは1以上の自然数を表す。)を有する近赤外線カットフィルタである。これについて、特許文献4に詳細に記載されている。ただし、紫外線カットの特性は必須構成ではないので、前記係数は限定されない。 The optical multilayer film is composed of a high refractive index film having a refractive index of 2.0 or more at a wavelength of 500 nm and a low refractive index film having a wavelength of 1.6 or less, and the optical multilayer film has a wavelength of the high refractive index film. the QWOT at 500nm Q H, when a QWOT at a wavelength 500nm for the low refractive index film was Q L, (a n Q H , b n Q L, c n Q H, d n Q L) basic units n of in pieces stacked repeating structure (where, a n, b n, c n, d n is the physical thickness of the membrane in each basic unit is a coefficient indicating how many times the QWOT, and n is 1 This is a near-infrared cut filter having the above natural number). This is described in detail in Patent Document 4. However, since the characteristic of ultraviolet cut is not an essential component, the coefficient is not limited.
 また、他の態様として、高屈折率膜の構成材料は、屈折率が2以上である材料が好ましく、2.2~2.7がより好ましい。このような構成材料としては、例えば、TiO、Nb(屈折率:2.38)、Ta、又はこれらの複合酸化物等が挙げられる。 As another aspect, the constituent material of the high refractive index film is preferably a material having a refractive index of 2 or more, more preferably 2.2 to 2.7. Examples of such a constituent material include TiO 2 , Nb 2 O 5 (refractive index: 2.38), Ta 2 O 5 , and composite oxides thereof.
 このとき、中屈折率膜の構成材料は、例えば屈折率が1.6を超え、2未満であることが好ましく、1.62~1.92がより好ましい。このような構成材料としては、例えば、Al、Y(屈折率:1.81)、又はこれらの複合酸化物、AlとZrOの混合物膜(屈折率:1.67)等が挙げられる。また、中屈折率膜は、高屈折率膜と低屈折率膜とを組み合わせた等価膜で代用してもよい。 At this time, the constituent material of the medium refractive index film preferably has a refractive index of more than 1.6 and less than 2, and more preferably 1.62 to 1.92. As such a constituent material, for example, Al 2 O 3 , Y 2 O 3 (refractive index: 1.81), or a composite oxide thereof, a mixture film of Al 2 O 3 and ZrO 2 (refractive index: 1). .67) and the like. The medium refractive index film may be replaced with an equivalent film in which a high refractive index film and a low refractive index film are combined.
 低屈折率膜の構成材料は、例えば屈折率が1.3以上1.6以下であることが好ましい。このような構成材料としては、例えば、SiO、SiO、MgFなどが挙げられる The constituent material of the low refractive index film preferably has a refractive index of 1.3 to 1.6, for example. Examples of such a constituent material include SiO 2 , SiO x N y , and MgF 2.
 誘電体多層膜(薄膜積層構造体)は、異なる屈折率の薄膜を交互に積層して構成される場合、その層数は、誘電体多層膜の有する光学特性によるが、薄膜の合計積層数として50~150層が好ましい。合計積層数が50層未満であると、波長800nm~1000nmの阻止性能が十分とならないおそれがある。また、合計積層数が150層を超えると、光学フィルタの製作時のタクトタイムが長くなり、誘電体多層膜に起因する光学フィルタの反りなどが発生するため好ましくない。 When the dielectric multilayer film (thin film laminated structure) is configured by alternately laminating thin films having different refractive indexes, the number of layers depends on the optical characteristics of the dielectric multilayer film, 50 to 150 layers are preferred. If the total number of laminated layers is less than 50, the blocking performance at a wavelength of 800 nm to 1000 nm may not be sufficient. On the other hand, if the total number of laminated layers exceeds 150, the tact time during the production of the optical filter becomes long, and the warp of the optical filter due to the dielectric multilayer film occurs, which is not preferable.
 誘電体多層膜(薄膜積層構造体)の膜厚としては、上記好ましい積層数を満たした上で、光学フィルタ1の薄型化の観点からは、薄い方が好ましい。しかしながら、所望の光学特性を得るには、5μm以上であることが好ましい。また、誘電体多層膜に起因する光学フィルタの反りなどを考慮し、15μm以下であることが好ましい。 As the film thickness of the dielectric multilayer film (thin film laminated structure), the thinner one is preferable from the viewpoint of reducing the thickness of the optical filter 1 while satisfying the preferable number of laminated layers. However, in order to obtain desired optical characteristics, it is preferably 5 μm or more. In consideration of the warp of the optical filter caused by the dielectric multilayer film, the thickness is preferably 15 μm or less.
 また、3つの薄膜積層構造体を備える光学フィルタ1においては、透明基板10の両表面に配置される薄膜積層構造体の合計膜厚が互いにできるだけ近いほうが好ましい。環境光センサに用いられる光学フィルタ1では、光学フィルタ1が極めて薄く形成されるため、透明基板10も極めて薄い。そのため、透明基板10の両表面の薄膜積層構造体の物理膜厚が大きく異なると、光学フィルタ1において、物理膜厚の小さい薄膜積層構造側に凸状の反りが生じることがあるためである。 Further, in the optical filter 1 including three thin film laminated structures, it is preferable that the total film thicknesses of the thin film laminated structures arranged on both surfaces of the transparent substrate 10 are as close as possible to each other. In the optical filter 1 used for the ambient light sensor, since the optical filter 1 is formed extremely thin, the transparent substrate 10 is also extremely thin. Therefore, when the physical film thickness of the thin film laminated structure on both surfaces of the transparent substrate 10 is greatly different, the optical filter 1 may have a convex warp on the side of the thin film laminated structure having a small physical film thickness.
 したがって、3つの薄膜積層構造体を備える光学フィルタ1においては、3つの薄膜積層構造体のうち、透過制限波長範囲が2番目に短波長側に位置し、透明基板10の表面に単独で積層される薄膜積層構造体12の物理膜厚を、その他の2つの薄膜積層構造体11、13よりも大きくすることが好ましい。すなわち、3つの薄膜積層構造体11、12、13の透過制限波長範囲の中心波長のうち2番目に短波長側に位置する中心波長を有する薄膜積層構造体12の物理膜厚が、それ以外の2つの薄膜積層構造体11及び薄膜積層構造体13の物理膜厚よりも厚いことが好ましい。これにより、透明基板10に積層された際の、透明基板10の両表面での薄膜積層構造体全体の厚さの差を小さくして、光学フィルタ1の反りを抑制することができる。 Therefore, in the optical filter 1 including three thin film laminated structures, the transmission limiting wavelength range is located on the second short wavelength side among the three thin film laminated structures, and is laminated alone on the surface of the transparent substrate 10. It is preferable that the physical film thickness of the thin film laminated structure 12 is larger than the other two thin film laminated structures 11 and 13. That is, the physical film thickness of the thin film laminated structure 12 having the center wavelength located at the second shortest wavelength among the central wavelengths in the transmission limited wavelength range of the three thin film laminated structures 11, 12, 13 is other than that It is preferably thicker than the physical film thickness of the two thin film laminated structures 11 and the thin film laminated structure 13. Thereby, the difference of the thickness of the whole thin film laminated structure in the both surfaces of the transparent substrate 10 when laminated | stacked on the transparent substrate 10 can be made small, and the curvature of the optical filter 1 can be suppressed.
 誘電体多層膜(薄膜積層構造体)は、その形成にあたっては、例えば、IAD(Ion Assisted Deposition)蒸着法、CVD法、スパッタ法、真空蒸着法等の乾式成膜プロセスや、スプレー法、ディップ法等の湿式成膜プロセス等を使用できる。 In forming the dielectric multilayer film (thin film laminated structure), for example, dry film formation processes such as IAD (Ion Assisted Deposition) deposition method, CVD method, sputtering method, vacuum deposition method, spray method, dipping method, etc. A wet film formation process such as can be used.
 透明基板10は、可視光を透過する材料である。例えば、ガラス、ガラスセラミックス、水晶、サファイア等の結晶、樹脂(ポリエチレンテレフタレート(PET)、ポリブチレンテレフタレート(PBT)等のポリエステル樹脂、ポリエチレン、ポリプロピレン、エチレン酢酸ビニル共重合体等のポリオレフィン樹脂、ノルボルネン樹脂、ポリアクリレート、ポリメチルメタクリレート等のアクリル樹脂、ウレタン樹脂、塩化ビニル樹脂、フッ素樹脂、ポリカーボネート樹脂、ポリビニルブチラール樹脂、ポリビニルアルコール樹脂等)等が挙げられる。 The transparent substrate 10 is a material that transmits visible light. For example, glass, glass ceramics, crystal such as crystal, sapphire, resin (polyester resin such as polyethylene terephthalate (PET), polybutylene terephthalate (PBT), polyolefin resin such as polyethylene, polypropylene, ethylene vinyl acetate copolymer, norbornene resin Acrylic resins such as polyacrylate and polymethyl methacrylate, urethane resins, vinyl chloride resins, fluororesins, polycarbonate resins, polyvinyl butyral resins, polyvinyl alcohol resins, etc.).
 透明基板10は、近赤外領域の波長の光を吸収する性質を有することが好ましい。例えば、本発明の光学フィルタ1を固体撮像装置用の近赤外線カットフィルタとして用いる場合、透明基板10が近赤外波長域の光を吸収する性質を有することで、人の視感度特性に近い色補正が可能となる。薄膜積層構造体11、12、13により、入射角依存性の低い分光特性が得られるため、近赤外領域の波長の光を吸収する性質を有する透明基板10に上記薄膜積層構造体を設けることで、近赤外領域の波長の光の透過を制限する優れた分光特性が得られる。そのため、固体撮像装置用の近赤外線カットフィルタとして良好な特性を有する光学フィルタ1を得ることが可能となる。 The transparent substrate 10 preferably has a property of absorbing light having a wavelength in the near infrared region. For example, when the optical filter 1 of the present invention is used as a near-infrared cut filter for a solid-state imaging device, the transparent substrate 10 has a property of absorbing light in the near-infrared wavelength region, so that the color is close to human visibility characteristics. Correction is possible. Since the thin- film multilayer structures 11, 12, and 13 can provide spectral characteristics with low incident angle dependency, the thin-film multilayer structure is provided on the transparent substrate 10 having the property of absorbing light having a wavelength in the near infrared region. Thus, an excellent spectral characteristic that restricts transmission of light having a wavelength in the near infrared region can be obtained. Therefore, it becomes possible to obtain the optical filter 1 having good characteristics as a near-infrared cut filter for a solid-state imaging device.
 近赤外領域の波長の光を吸収する性質を有する透明基板10は、可視光領域の光を透過し、近赤外領域の光を吸収する能力を有するガラス、例えば、CuO含有フツリン酸塩ガラス又はCuO含有リン酸塩ガラス(以下、これらをまとめて「CuO含有ガラス」ともいう。)で構成されることが好ましい。 The transparent substrate 10 having the property of absorbing light having a wavelength in the near infrared region is a glass having the ability to transmit light in the visible light region and absorb light in the near infrared region, such as CuO-containing fluorophosphate glass. Alternatively, it is preferably composed of a CuO-containing phosphate glass (hereinafter collectively referred to as “CuO-containing glass”).
 透明基板10は、CuO含有ガラスで構成されることで、可視光に対し高い透過率を有するとともに、近赤外領域の波長の光に対して高い透過制限性を有する。なお、「リン酸塩ガラス」には、ガラスの骨格の一部がSiOで構成されるケイリン酸塩ガラスも含まれる。 The transparent substrate 10 is composed of CuO-containing glass, so that it has a high transmittance for visible light and a high transmission limiting property for light having a wavelength in the near infrared region. The “phosphate glass” includes silicic acid phosphate glass in which a part of the glass skeleton is composed of SiO 2 .
 CuO含有ガラス基板は、波長400~450nmの光の吸収は僅かで、波長775~900nmの光に対する波長400~450nmの光の吸収率比が低い特徴がある。その結果、CuO含有ガラス基板は、波長775~900nmの光の透過を、吸収により十分制限するようにCuO含有量を増やして吸収率を高くしても、可視光の顕著な透過率低下とならないため有用である。 The CuO-containing glass substrate has a feature that absorption of light having a wavelength of 400 to 450 nm is slight, and an absorptance ratio of light having a wavelength of 400 to 450 nm with respect to light having a wavelength of 775 to 900 nm is low. As a result, even if the CuO-containing glass substrate increases the absorption rate by increasing the CuO content so as to sufficiently limit the transmission of light having a wavelength of 775 to 900 nm by absorption, the visible light transmittance does not decrease significantly. Because it is useful.
 近赤外領域の波長の光を吸収する性質を有する透明基板10としては、CuO含有ガラス以外の材料として、透明樹脂中に、近赤外領域のうち特定の範囲の波長の光を吸収する近赤外線吸収色素を含有した近赤外線吸収基板も挙げられる。 As the transparent substrate 10 having the property of absorbing light having a wavelength in the near infrared region, as a material other than the CuO-containing glass, the transparent resin has a near resin that absorbs light having a wavelength in a specific range in the near infrared region. A near-infrared absorbing substrate containing an infrared-absorbing dye is also included.
 また、光学フィルタの近赤外光の吸収性能を高めるために、透明基板10の表面に、上記近赤外線吸収基板と同様の材料を用いて、近赤外線吸収色素及び透明樹脂を含む近赤外線吸収層を形成してもよい。この場合、近赤外線吸収層は、透明基板10と、薄膜積層構造体11又は薄膜積層構造体12の間に形成される。また、近赤外線吸収層は透明基板10の少なくとも一方の表面に形成されればよい。 Moreover, in order to improve the near-infrared light absorption performance of the optical filter, a near-infrared absorbing layer containing a near-infrared absorbing dye and a transparent resin on the surface of the transparent substrate 10 using the same material as the above-mentioned near-infrared absorbing substrate. May be formed. In this case, the near-infrared absorbing layer is formed between the transparent substrate 10 and the thin film laminated structure 11 or the thin film laminated structure 12. Further, the near infrared absorption layer may be formed on at least one surface of the transparent substrate 10.
 近赤外線吸収色素としては、可視光領域の光を透過し、近赤外領域の光を吸収する能力を有する近赤外線吸収色素であれば特に制限されない。なお、本発明における色素は顔料、すなわち分子が凝集した状態でもよい。 The near-infrared absorbing dye is not particularly limited as long as it is a near-infrared absorbing dye having the ability to transmit light in the visible light region and absorb light in the near infrared region. The dye in the present invention may be a pigment, that is, a state in which molecules are aggregated.
 近赤外線吸収色素としては、シアニン系化合物、フタロシアニン系化合物、ナフタロシアニン系化合物、ジチオール金属錯体系化合物、ジイモニウム系化合物、ポリメチン系化合物、フタリド化合物、ナフトキノン系化合物、アントラキノン系化合物、インドフェノール系化合物、スクアリリウム系化合物等が挙げられる。 As near-infrared absorbing dyes, cyanine compounds, phthalocyanine compounds, naphthalocyanine compounds, dithiol metal complex compounds, diimonium compounds, polymethine compounds, phthalide compounds, naphthoquinone compounds, anthraquinone compounds, indophenol compounds, Examples include squarylium compounds.
 これらの中ではスクアリリウム系化合物、シアニン系化合物及びフタロシアニン系化合物がより好ましく、スクアリリウム系化合物が特に好ましい。スクアリリウム系化合物からなる近赤外線吸収色素は、その吸収スペクトルにおいて、可視光の吸収が少なく、保存安定性及び光に対する安定性が高いため好ましい。シアニン系化合物からなる近赤外線吸収色素は、その吸収スペクトルにおいて、可視光の吸収が少なく、近赤外線領域のうち、長波長側で光の吸収率が高いため好ましい。また、シアニン系化合物は低コストであって、塩形成することにより長期の安定性も確保できることが知られている。フタロシアニン系化合物からなる近赤外線吸収色素は、耐熱性や耐候性に優れるため好ましい。 Of these, squarylium compounds, cyanine compounds and phthalocyanine compounds are more preferred, and squarylium compounds are particularly preferred. A near-infrared absorbing dye made of a squarylium compound is preferred because its absorption spectrum has little absorption of visible light and high storage stability and stability to light. A near-infrared absorbing dye made of a cyanine compound is preferable because of its low absorption of visible light in its absorption spectrum and high light absorption on the long wavelength side in the near-infrared region. In addition, it is known that cyanine compounds are low-cost, and long-term stability can be secured by salt formation. Near-infrared absorbing dyes composed of phthalocyanine compounds are preferred because they are excellent in heat resistance and weather resistance.
 近赤外線吸収色素としては、上記した化合物のうち1種を単独で用いてもよく2種以上を併用してもよい。 As the near-infrared absorbing dye, one of the above compounds may be used alone, or two or more of them may be used in combination.
 透明樹脂としては、屈折率が、1.45以上の透明樹脂が好ましい。屈折率は1.5以上がより好ましく、1.6以上が特に好ましい。透明樹脂の屈折率の上限は特にないが、入手のしやすさ等から1.72程度が好ましい。なお、本明細書において屈折率とは、特に断りのない限り、波長500nmでの屈折率をいう。 As the transparent resin, a transparent resin having a refractive index of 1.45 or more is preferable. The refractive index is more preferably 1.5 or more, and particularly preferably 1.6 or more. The upper limit of the refractive index of the transparent resin is not particularly limited, but is preferably about 1.72 in view of availability. In the present specification, the refractive index means a refractive index at a wavelength of 500 nm unless otherwise specified.
 透明樹脂としては、アクリル樹脂、エポキシ樹脂、エン・チオール樹脂、ポリカーボネート樹脂、ポリエーテル樹脂、ポリアリレート樹脂、ポリサルホン樹脂、ポリエーテルサルホン樹脂、ポリパラフェニレン樹脂、ポリアリーレンエーテルフォスフィンオキシド樹脂、ポリイミド樹脂、ポリアミドイミド樹脂、ポリオレフィン樹脂、環状オレフィン樹脂、及びポリエステル樹脂が挙げられる。透明樹脂としては、これらの樹脂から1種を単独で使用してもよく、2種以上を混合して使用してもよい。 Transparent resins include acrylic resin, epoxy resin, ene / thiol resin, polycarbonate resin, polyether resin, polyarylate resin, polysulfone resin, polyethersulfone resin, polyparaphenylene resin, polyarylene ether phosphine oxide resin, polyimide Examples include resins, polyamideimide resins, polyolefin resins, cyclic olefin resins, and polyester resins. As transparent resin, 1 type may be used individually from these resin, and 2 or more types may be mixed and used for it.
 上記の中でも、近赤外線吸収色素の透明樹脂に対する溶解性の観点から、透明樹脂は、アクリル樹脂、ポリエステル樹脂、ポリカーボネート樹脂、エン・チオール樹脂、エポキシ樹脂、及び環状オレフィン樹脂から選ばれる1種以上が好ましい。さらに、透明樹脂は、アクリル樹脂、ポリエステル樹脂、ポリカーボネート樹脂、及び環状オレフィン樹脂から選ばれる1種以上がより好ましい。ポリエステル樹脂としては、ポリエチレンテレフタレート樹脂、ポリエチレンナフタレート樹脂等が好ましい。 Among the above, from the viewpoint of solubility of the near-infrared absorbing dye in the transparent resin, the transparent resin is at least one selected from acrylic resins, polyester resins, polycarbonate resins, ene / thiol resins, epoxy resins, and cyclic olefin resins. preferable. Further, the transparent resin is more preferably at least one selected from an acrylic resin, a polyester resin, a polycarbonate resin, and a cyclic olefin resin. As the polyester resin, polyethylene terephthalate resin, polyethylene naphthalate resin and the like are preferable.
 近赤外線吸収層は、例えば、近赤外線吸収色素及び、透明樹脂又は透明樹脂の原料成分、さらに任意に紫外線吸収体を溶媒又は分散媒に、溶解させ又は分散させて調製した塗工液を、透明基板10上に塗工し、乾燥させ、さらに必要に応じて硬化させて製造できる。 The near-infrared absorbing layer is, for example, a transparent coating liquid prepared by dissolving or dispersing a near-infrared absorbing dye and a transparent resin or a transparent resin raw material component, and optionally an ultraviolet absorber in a solvent or dispersion medium. It can be produced by coating on the substrate 10, drying, and further curing as necessary.
 近赤外線吸収層は、近赤外線吸収色素及び透明樹脂、任意成分の紫外線吸収体以外に、本発明の効果を阻害しない範囲で、必要に応じてその他の任意成分を含有してもよい。その他の任意成分として、具体的には、近赤外線ないし赤外線吸収剤、色調補正色素、紫外線吸収剤、レベリング剤、帯電防止剤、熱安定剤、光安定剤、酸化防止剤、分散剤、難燃剤、滑剤、可塑剤等が挙げられる。また、後述する近赤外線吸収層を形成する際に用いる塗工液に添加する成分、例えば、シランカップリング剤、熱もしくは光重合開始剤、重合触媒に由来する成分等が挙げられる。 The near-infrared absorbing layer may contain other optional components as required, as long as the effects of the present invention are not impaired, in addition to the near-infrared absorbing dye, the transparent resin, and the optional ultraviolet absorber. As other optional components, specifically, near infrared rays or infrared absorbers, color tone correction dyes, ultraviolet absorbers, leveling agents, antistatic agents, heat stabilizers, light stabilizers, antioxidants, dispersants, flame retardants , Lubricants, plasticizers and the like. Moreover, the component added to the coating liquid used when forming the near-infrared absorption layer mentioned later, for example, the component derived from a silane coupling agent, a heat | fever or photoinitiator, a polymerization catalyst, etc. are mentioned.
 近赤外線吸収層の膜厚は、使用する装置内の配置スペースや要求される吸収特性等に応じて適宜定められる。上記膜厚は、0.1~100μmが好ましい。膜厚が0.1μm未満では、近赤外線吸収能を十分に発現できないおそれがある。また、膜厚が100μm超では膜の平坦性が低下し、吸収率のバラツキが生じるおそれがある。膜厚は、0.5~50μmがより好ましい。この範囲にあれば、十分な近赤外線吸収能と膜厚の平坦性を両立できる。 The film thickness of the near-infrared absorbing layer is appropriately determined according to the arrangement space in the apparatus to be used and the required absorption characteristics. The film thickness is preferably 0.1 to 100 μm. If the film thickness is less than 0.1 μm, the near-infrared absorbing ability may not be sufficiently exhibited. On the other hand, if the film thickness exceeds 100 μm, the flatness of the film is lowered, and there is a possibility that the absorption rate varies. The film thickness is more preferably 0.5 to 50 μm. If it exists in this range, sufficient near-infrared absorptivity and flatness of a film thickness can be compatible.
 以上説明した本発明の光学フィルタによれば、透明基板の表面に、透過制限波長範囲の異なる3つ以上の薄膜積層構造体が、同一の表面上における透過制限波長範囲が連続しないように積層されることで、広角度で入射した光に対しても、可視光透過率が高く、近赤外域の阻止性能も高い分光特性を得ることができる。 According to the optical filter of the present invention described above, three or more thin film laminated structures having different transmission limiting wavelength ranges are laminated on the surface of the transparent substrate so that the transmission limiting wavelength ranges on the same surface are not continuous. As a result, it is possible to obtain spectral characteristics having high visible light transmittance and high blocking performance in the near infrared region even for light incident at a wide angle.
 本発明の光学フィルタは、近赤外波長領域、例えば、波長800nm~1000nmの光に対する透過率が1%以下であることが好ましい。また、波長800nm~1000nmにおいて光の透過率が0.05%未満である波長範囲を100nm以上とする阻止性能を持つことが好ましい。また、本発明の光学フィルタによれば、入射角が0~50°の光を透過する波長範囲の光学多層膜に起因する透過率の低下を大幅に低減することができる。この特徴により、近赤外線照射光が多用されるような環境下においてもフレアやゴーストなどが少ない画像を提供可能な、CCDやCMOS等の撮像素子、その他の光センサ用途の光学フィルタとして好適に利用することができる。 The optical filter of the present invention preferably has a transmittance of 1% or less for light in the near-infrared wavelength region, for example, a wavelength of 800 nm to 1000 nm. Further, it is preferable that the wavelength range in which the light transmittance is less than 0.05% at a wavelength of 800 nm to 1000 nm is 100 nm or more. Further, according to the optical filter of the present invention, it is possible to greatly reduce the decrease in transmittance due to the optical multilayer film in the wavelength range that transmits light having an incident angle of 0 to 50 °. This feature makes it suitable for use as an optical filter for imaging devices such as CCD and CMOS, and other optical sensor applications that can provide images with little flare and ghosting even in environments where near-infrared radiation is frequently used. can do.
 本発明の光学フィルタは、可視光領域内、特に波長430nm~560nmの青色、緑色の領域における透過率の低下を、光の入射角が0~50°の広角の範囲内で効果的に抑制できる。そのため、光の入射角の広い範囲で、前記波長範囲における平均透過率を85%以上とすることができる。 The optical filter of the present invention can effectively suppress a decrease in transmittance in the visible light region, particularly in the blue and green regions having a wavelength of 430 nm to 560 nm, within a wide angle range where the incident angle of light is 0 to 50 °. . Therefore, the average transmittance in the wavelength range can be 85% or more in a wide range of light incident angles.
 また、本発明の光学フィルタにおいて、近赤外線吸収性を有する透明基板を用いるか、透明基板の表面に近赤外線吸収層を設けることで、近赤外波長範囲の光の透過を確実に制限することができ、人の視感度特性に近い色補正が可能となる、より優れた光学特性を有する光学フィルタを得ることができる。 Moreover, in the optical filter of the present invention, the transmission of light in the near-infrared wavelength range is surely limited by using a transparent substrate having near-infrared absorption or by providing a near-infrared absorption layer on the surface of the transparent substrate. Therefore, it is possible to obtain an optical filter having more excellent optical characteristics that enables color correction close to human visibility characteristics.
(実施例1)
 本実施例に係る光学フィルタ(近赤外線カットフィルタ)は、透明基板(近赤外線吸収ガラス、板厚0.3mm、商品名:NF-50T、AGCテクノグラス社製)と、透明基板の一方の面及び他方の面に設けられた合計5つの薄膜積層構造体とを備える。この薄膜積層構造体は、それぞれ、上記透明基板表面側から、高屈折率膜と低屈折率膜とを順に積層した構造である。
Example 1
The optical filter (near-infrared cut filter) according to this example includes a transparent substrate (near-infrared absorbing glass, plate thickness: 0.3 mm, trade name: NF-50T, manufactured by AGC Techno Glass), and one surface of the transparent substrate. And a total of five thin film laminated structures provided on the other surface. Each of the thin film laminated structures has a structure in which a high refractive index film and a low refractive index film are sequentially laminated from the transparent substrate surface side.
 透明基板の一方の面には4つの薄膜積層構造体が配置される。4つの薄膜積層構造体は、4つの合計で32層、物理膜厚3796.98nmの、高屈折率膜(酸化チタン(TiO))と低屈折率膜(酸化珪素(SiO))の繰り返し積層構造(第1-1の薄膜積層構造体)である。すなわち、透明基板の一方の面には4つの薄膜積層構造体からなる第1-1の薄膜積層構造体を有している。 Four thin film laminated structures are disposed on one surface of the transparent substrate. The four thin-film stacked structures are a repetition of a high refractive index film (titanium oxide (TiO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) having a total of four, 32 layers and a physical film thickness of 3796.98 nm. This is a laminated structure (1-1 thin film laminated structure). That is, the transparent substrate has a first-first thin film laminated structure composed of four thin film laminated structures on one surface.
 透明基板の他方の面には、1つの薄膜積層構造体が配置される。この薄膜積層構造体は、高屈折率膜(酸化チタン(TiO))と、低屈折率膜(酸化珪素(SiO))の合計52層、物理膜厚3093.23nmの繰り返し積層構造である(第1-2の薄膜積層構造体)。 One thin film laminated structure is disposed on the other surface of the transparent substrate. This thin film laminated structure is a repetitive laminated structure of a total of 52 layers of a high refractive index film (titanium oxide (TiO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) and a physical film thickness of 3093.23 nm. (1-2 thin film laminated structure).
 上記の光学フィルタの透明基板の一方の面に設けられた薄膜積層構造体(第1-1の薄膜積層構造体)の構成を表1に示す。また、光学フィルタの透明基板の他方の面に設けられた薄膜積層構造体(第1-2の薄膜積層構造体)の構成を表2に示す。表1及び表2において、膜層数は透明基板側からの層の序数であり、膜厚は物理膜厚を示す。 Table 1 shows the configuration of the thin film laminated structure (1-1 thin film laminated structure) provided on one surface of the transparent substrate of the optical filter. Table 2 shows the configuration of the thin film laminated structure (1-2 thin film laminated structure) provided on the other surface of the transparent substrate of the optical filter. In Tables 1 and 2, the number of film layers is the ordinal number of layers from the transparent substrate side, and the film thickness indicates the physical film thickness.
 この光学フィルタについて、入射角0°、40°及び50°における光学特性を、光学薄膜シミュレーションソフト(TFCalc、Software Spectra社製)を用いて検証した。結果を図2、図3(波長850nm~1050nmの領域における拡大図)に示す。 The optical characteristics of the optical filter at incident angles of 0 °, 40 °, and 50 ° were verified using optical thin film simulation software (TFCalc, manufactured by Spectra, Inc.). The results are shown in FIGS. 2 and 3 (enlarged views in the wavelength region of 850 nm to 1050 nm).
 また、透明基板の一方の面に設けられた薄膜積層構造体(第1-1の薄膜積層構造体)のみ(透明基板による光の吸収の影響を除く)の入射角0°、40°及び50°における光学特性を、上記光学薄膜シミュレーションソフトを用いて検証した。結果を図4に示す。また、透明基板の他方の面に設けられた薄膜積層構造体(第1-2の薄膜積層構造体)のみ(透明基板による光の吸収の影響を除く)の入射角0°、40°及び50°における光学特性を、上記光学薄膜シミュレーションソフトを用いて検証した。結果を図5に示す。 Also, incident angles of 0 °, 40 ° and 50 ° only on the thin film laminated structure (1-1 thin film laminated structure) provided on one surface of the transparent substrate (excluding the influence of light absorption by the transparent substrate). The optical characteristics at 0 ° were verified using the optical thin film simulation software. The results are shown in FIG. Also, incident angles of 0 °, 40 ° and 50 ° only for the thin film laminated structure (1-2 thin film laminated structure) provided on the other surface of the transparent substrate (excluding the influence of light absorption by the transparent substrate). The optical characteristics at 0 ° were verified using the optical thin film simulation software. The results are shown in FIG.
 図4に示されるように、本発明の実施例1の光学フィルタでは、透明基板の同一の表面側に配置される薄膜積層構造体の光学特性において、0°入射において波長970nm、1070nm、1190nm付近に透過率が5%以上の部分を有しており、当該薄膜積層構造体が透過を制限する波長領域が不連続である。そして、特定の近赤外領域の透過を制限する薄膜積層構造体のみを他方の面に形成しているため、当該他方の面の薄膜積層構造体の透過制限波長範囲の幅は狭いものの、光の入射角が大きくなったとしても可視領域に反射リップルが発生しがたい薄膜積層構造体を設けることができる。 As shown in FIG. 4, in the optical filter of Example 1 of the present invention, in the optical characteristics of the thin film laminated structure disposed on the same surface side of the transparent substrate, the wavelength is 970 nm, 1070 nm, and around 1190 nm at 0 ° incidence. Have a portion with a transmittance of 5% or more, and the wavelength region in which the thin film laminated structure restricts transmission is discontinuous. Since only the thin film laminated structure that restricts transmission in a specific near-infrared region is formed on the other surface, the width of the transmission restricted wavelength range of the thin film laminated structure on the other surface is narrow. Even when the incident angle of the thin film is increased, it is possible to provide a thin film laminated structure in which reflection ripples hardly occur in the visible region.
Figure JPOXMLDOC01-appb-T000001
Figure JPOXMLDOC01-appb-T000001
Figure JPOXMLDOC01-appb-T000002
Figure JPOXMLDOC01-appb-T000002
(実施例2)
 本実施例に係る光学フィルタ(近赤外線カットフィルタ)は、実施例1にて用いたものと同様の透明基板と、透明基板の一方の面及び他方の面に設けられた薄膜積層構造体とを備える。この薄膜積層構造体は、それぞれ、上記透明基板表面側から、異なる屈折率の膜を順に積層した構造である。
(Example 2)
The optical filter (near-infrared cut filter) according to this example includes a transparent substrate similar to that used in Example 1, and a thin film laminated structure provided on one surface and the other surface of the transparent substrate. Prepare. Each of the thin film laminated structures has a structure in which films having different refractive indexes are sequentially laminated from the transparent substrate surface side.
 透明基板の一方の面には2つの薄膜積層構造体が配置される。2つの薄膜積層構造体は、合計50層、物理膜厚5930.11nmである。2つの薄膜積層構造体は、透明基板側の上に設けられた、高屈折率膜(酸化ジルコニウム(ZrO))と低屈折率膜(酸化珪素(SiO))との合計30層の繰り返し積層構造(第2-1の薄膜積層構造体)及び第2-1の薄膜積層構造体の上(空気側)に設けられた、高屈折率膜(酸化チタン(TiO))と中屈折率膜(酸化アルミニウム(Al))との合計20層の繰り返し積層構造(第2-2の薄膜積層構造体)とからなる。 Two thin film laminated structures are disposed on one surface of the transparent substrate. The two thin film laminated structures have a total of 50 layers and a physical film thickness of 5930.11 nm. The two thin-film laminated structures have a total of 30 layers of a high refractive index film (zirconium oxide (ZrO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) provided on the transparent substrate side. High refractive index film (titanium oxide (TiO 2 )) and medium refractive index provided on the laminated structure (2-1 thin film laminated structure) and the 2-1 thin film laminated structure (air side) It consists of a total of 20 layers of repeated lamination structure (second thin film laminated structure) with a film (aluminum oxide (Al 2 O 3 )).
 透明基板の他方の面には、1つの薄膜積層構造体が配置される。この薄膜積層構造体は、高屈折率膜(酸化チタン(TiO))と、低屈折率膜(酸化珪素(SiO))の合計60層、物理膜厚3570.77nmの繰り返し積層構造である(第2-3の薄膜積層構造体)。 One thin film laminated structure is disposed on the other surface of the transparent substrate. This thin film laminated structure is a repetitive laminated structure having a total of 60 layers of a high refractive index film (titanium oxide (TiO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) and a physical film thickness of 3570.77 nm. (2-3 thin film laminated structure).
 上記の光学フィルタの透明基板の一方の面に設けられた薄膜積層構造体(第2-1の薄膜積層構造体及び第2-2の薄膜積層構造体)の構成を表3に示す。また、光学フィルタの透明基板の他方の面に設けられた薄膜積層構造体(第2-3の薄膜積層構造体)の構成を表4に示す。表3及び表4において、膜層数は透明基板側からの層の序数であり、膜厚は物理膜厚を示す。 Table 3 shows the structures of the thin film laminated structures (2-1 thin film laminated structure and 2-2 thin film laminated structure) provided on one surface of the transparent substrate of the optical filter. Table 4 shows the configuration of the thin film laminated structure (second-3 thin film laminated structure) provided on the other surface of the transparent substrate of the optical filter. In Tables 3 and 4, the number of film layers is the ordinal number of layers from the transparent substrate side, and the film thickness indicates the physical film thickness.
 この光学フィルタについて、入射角0°、40°及び50°における光学特性を、光学薄膜シミュレーションソフト(TFCalc、Software Spectra社製)を用いて検証した。結果を図6、図7(波長850nm~1050nmの領域における拡大図)に示す。 The optical characteristics of the optical filter at incident angles of 0 °, 40 °, and 50 ° were verified using optical thin film simulation software (TFCalc, manufactured by Spectra, Inc.). The results are shown in FIGS. 6 and 7 (enlarged views in the wavelength region of 850 nm to 1050 nm).
 また、透明基板の一方の面に設けられた薄膜積層構造体(第2-1の薄膜積層構造体及び第2-2の薄膜積層構造体))のみ(透明基板による光の吸収の影響を除く)の入射角0°、40°及び50°における光学特性を、上記光学薄膜シミュレーションソフトを用いて検証した。結果を図8に示す。また、透明基板の他方の面に設けられた薄膜積層構造体(第2-3の薄膜積層構造体)のみ(透明基板による光の吸収の影響を除く)の入射角0°、40°及び50°における光学特性を、上記光学薄膜シミュレーションソフトを用いて検証した。結果を図9に示す。 Further, only the thin film laminated structure (the 2-1 thin film laminated structure and the 2-2 thin film laminated structure) provided on one surface of the transparent substrate (excluding the influence of light absorption by the transparent substrate) ) Was verified using the optical thin film simulation software. The results are shown in FIG. In addition, incident angles of 0 °, 40 °, and 50 ° only for the thin film laminated structure (the second and third thin film laminated structures) provided on the other surface of the transparent substrate (excluding the influence of light absorption by the transparent substrate). The optical characteristics at 0 ° were verified using the optical thin film simulation software. The results are shown in FIG.
Figure JPOXMLDOC01-appb-T000003
Figure JPOXMLDOC01-appb-T000003
Figure JPOXMLDOC01-appb-T000004
Figure JPOXMLDOC01-appb-T000004
(実施例3)
 本実施例に係る光学フィルタ(近赤外線カットフィルタ)は、実施例1にて用いたものと同様の透明基板と、透明基板の一方の面及び他方の面に設けられた薄膜積層構造体とを備える。この薄膜積層構造体は、それぞれ、上記透明基板表面側から、異なる屈折率の膜を順に積層した構造である。
Example 3
The optical filter (near-infrared cut filter) according to this example includes a transparent substrate similar to that used in Example 1, and a thin film laminated structure provided on one surface and the other surface of the transparent substrate. Prepare. Each of the thin film laminated structures has a structure in which films having different refractive indexes are sequentially laminated from the transparent substrate surface side.
 透明基板の一方の面には2つの薄膜積層構造体が配置される。2つの薄膜積層構造体は、合計44層、物理膜厚5738.57nmである。2つの薄膜積層構造体は、透明基板側の上に設けられた、高屈折率膜(酸化ジルコニウム(ZrO))と低屈折率膜(酸化珪素(SiO))との合計16層の繰り返し積層構造(第3-1の薄膜積層構造体)及び第3-1の薄膜積層構造体の上(空気側)に設けられた、高屈折率膜(酸化チタン(TiO))と中屈折率膜(酸化珪素(SiO))との合計28層の繰り返し積層構造(第3-2の薄膜積層構造体)とからなる。 Two thin film laminated structures are disposed on one surface of the transparent substrate. The two thin film laminated structures have a total of 44 layers and a physical film thickness of 5738.57 nm. The two thin-film laminated structures have a total of 16 layers of a high refractive index film (zirconium oxide (ZrO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) provided on the transparent substrate side. High refractive index film (titanium oxide (TiO 2 )) and medium refractive index provided on the laminated structure (3-1 thin film laminated structure) and the 3-1 thin film laminated structure (air side) It consists of a total of 28 layers (3-2 thin film layered structure) with a film (silicon oxide (SiO 2 )).
 透明基板の他方の面には、1つの薄膜積層構造体が配置される。この薄膜積層構造体は、高屈折率膜(酸化ジルコニウム(ZrO))と、低屈折率膜(酸化珪素(SiO))の合計30層、物理膜厚3656.75nmの繰り返し積層構造である(第3-3の薄膜積層構造体)。 One thin film laminated structure is disposed on the other surface of the transparent substrate. This thin film laminated structure is a repetitive laminated structure having a total of 30 layers of a high refractive index film (zirconium oxide (ZrO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) and a physical film thickness of 3656.75 nm. (3-3 Thin Film Laminated Structure)
 上記の光学フィルタの透明基板の一方の面に設けられた薄膜積層構造体(第3-1の薄膜積層構造体及び第3-2の薄膜積層構造体)の構成を表5に示す。また、光学フィルタの透明基板の他方の面に設けられた薄膜積層構造体(第3-3の薄膜積層構造体)の構成を表6に示す。表5及び表6において、膜層数は透明基板側からの層の序数であり、膜厚は物理膜厚を示す。 Table 5 shows the configuration of the thin film laminated structure (3-1 thin film laminated structure and 3-2 thin film laminated structure) provided on one surface of the transparent substrate of the optical filter. Table 6 shows the configuration of the thin film stack structure (3-3 thin film stack structure) provided on the other surface of the transparent substrate of the optical filter. In Tables 5 and 6, the number of film layers is the ordinal number of layers from the transparent substrate side, and the film thickness indicates the physical film thickness.
 この光学フィルタについて、入射角0°、40°及び50°における光学特性を、光学薄膜シミュレーションソフト(TFCalc、Software Spectra社製)を用いて検証した。結果を図10、図11(波長850nm~1050nmの領域における拡大図)に示す。 The optical characteristics of the optical filter at incident angles of 0 °, 40 °, and 50 ° were verified using optical thin film simulation software (TFCalc, manufactured by Spectra, Inc.). The results are shown in FIGS. 10 and 11 (enlarged views in the wavelength region of 850 nm to 1050 nm).
 また、透明基板の一方の面に設けられた薄膜積層構造体(第3-1の薄膜積層構造体及び第3-2の薄膜積層構造体)のみ(透明基板による光の吸収の影響を除く)の入射角0°、40°及び50°における光学特性を、光学薄膜シミュレーションソフトを用いて検証した。結果を図12に示す。また、透明基板の他方の面に設けられた薄膜積層構造体(第3-3の薄膜積層構造体)のみ(透明基板による光の吸収の影響を除く)の入射角0°、40°及び50°における光学特性を、光学薄膜シミュレーションソフトを用いて検証した。結果を図13に示す。 Also, only the thin film laminated structure (3-1 thin film laminated structure and 3-2 thin film laminated structure) provided on one surface of the transparent substrate (excluding the influence of light absorption by the transparent substrate) The optical characteristics at 0 °, 40 ° and 50 ° of the incident angle were verified using optical thin film simulation software. The results are shown in FIG. Also, incident angles of 0 °, 40 ° and 50 ° only on the thin film laminated structure (3-3 thin film laminated structure) provided on the other surface of the transparent substrate (excluding the influence of light absorption by the transparent substrate). The optical characteristics at ° were verified using optical thin film simulation software. The results are shown in FIG.
Figure JPOXMLDOC01-appb-T000005
Figure JPOXMLDOC01-appb-T000005
Figure JPOXMLDOC01-appb-T000006
Figure JPOXMLDOC01-appb-T000006
(比較例1)
 本比較例に係る光学フィルタ(近赤外線カットフィルタ)は、実施例1にて用いたものと同様の透明基板を備える。透明基板の一方の面のみに複数の薄膜積層構造体と備える。この薄膜積層構造体は、上記透明基板表面側から、高屈折率膜と低屈折率膜とを順に積層した構造である。
(Comparative Example 1)
The optical filter (near infrared cut filter) according to this comparative example includes the same transparent substrate as that used in Example 1. A plurality of thin film laminated structures are provided on only one surface of the transparent substrate. This thin film laminated structure has a structure in which a high refractive index film and a low refractive index film are sequentially laminated from the transparent substrate surface side.
 透明基板の一方の面には、5つの薄膜積層構造体が配置される。この薄膜積層構造体は、いずれも高屈折率膜(酸化チタン(TiO))と低屈折率膜(酸化珪素(SiO))の合計40層、物理膜厚5151.58nmの繰り返し積層構造である。すなわち、透明基板の一方の面には同様の構成の5つの薄膜積層構造体が積層されている。 Five thin film laminated structures are disposed on one surface of the transparent substrate. This thin film laminated structure is a repetitive laminated structure having a total of 40 layers of a high refractive index film (titanium oxide (TiO 2 )) and a low refractive index film (silicon oxide (SiO 2 )) and a physical film thickness of 5151.58 nm. is there. That is, five thin film laminated structures having the same configuration are laminated on one surface of the transparent substrate.
 透明基板の他方の面に設けられた光学多層膜は反射防止膜である。この光学多層膜は、それぞれ高屈折率膜が酸化チタン(TiO)、低屈折率膜が酸化珪素(SiO)であり、それらの合計6層、物理膜厚237.58nmの繰り返し積層構造である。 The optical multilayer film provided on the other surface of the transparent substrate is an antireflection film. Each of the optical multilayer films has a high-refractive index film of titanium oxide (TiO 2 ) and a low-refractive index film of silicon oxide (SiO 2 ). is there.
 上記の光学フィルタの透明基板の一方の面に設けられた薄膜積層構造体の構成を表3に示す。また、光学フィルタの透明基板の他方の面に設けられた光学多層膜の構成を表4に示す。表7及び表8において、膜層数は透明基板側からの層の序数であり、膜厚は物理膜厚を示す。 Table 3 shows the configuration of the thin film laminated structure provided on one surface of the transparent substrate of the optical filter. Table 4 shows the configuration of the optical multilayer film provided on the other surface of the transparent substrate of the optical filter. In Tables 7 and 8, the number of film layers is the ordinal number of layers from the transparent substrate side, and the film thickness indicates the physical film thickness.
 この光学フィルタについて、入射角0°、40°及び50°における光学特性を、光学薄膜シミュレーションソフト(TFCalc、Software Spectra社製)を用いて検証した。結果を図14、図15(波長850nm~1050nmの領域における拡大図)に示す。また、透明基板の一方の面に設けられた薄膜積層構造体のみ(透明基板による光の吸収の影響を除く)の入射角0°、40°及び50°における光学特性を、上記光学薄膜シミュレーションソフトを用いて検証した。結果を図16に示す。また、透明基板の他方の面に設けられた光学多層膜のみ(透明基板による光の吸収の影響を除く)の入射角0°、40°及び50°における光学特性を、上記光学薄膜シミュレーションソフトを用いて検証した。結果を図17に示す。 The optical characteristics of the optical filter at incident angles of 0 °, 40 °, and 50 ° were verified using optical thin film simulation software (TFCalc, manufactured by Spectra, Inc.). The results are shown in FIGS. 14 and 15 (enlarged views in the wavelength region of 850 nm to 1050 nm). Further, the optical thin film simulation software described above shows the optical characteristics at the incident angles of 0 °, 40 ° and 50 ° of only the thin film laminated structure (excluding the influence of light absorption by the transparent substrate) provided on one surface of the transparent substrate. It verified using. The results are shown in FIG. In addition, the optical thin film simulation software described above shows the optical characteristics at the incident angles of 0 °, 40 ° and 50 ° of only the optical multilayer film provided on the other surface of the transparent substrate (excluding the influence of light absorption by the transparent substrate). Used to verify. The results are shown in FIG.
Figure JPOXMLDOC01-appb-T000007
Figure JPOXMLDOC01-appb-T000007
Figure JPOXMLDOC01-appb-T000008
Figure JPOXMLDOC01-appb-T000008
(比較例2)
 本比較例に係る光学フィルタ(近赤外線カットフィルタ)は、実施例1にて用いたものと同様の透明基板を備え、透明基板の一方の面のみに薄膜積層構造体を備える。この薄膜積層構造体は、上記透明基板表面側から、高屈折率膜と低屈折率膜とを順に積層した構造である。
(Comparative Example 2)
The optical filter (near-infrared cut filter) according to this comparative example includes a transparent substrate similar to that used in Example 1, and includes a thin film laminated structure only on one surface of the transparent substrate. This thin film laminated structure has a structure in which a high refractive index film and a low refractive index film are sequentially laminated from the transparent substrate surface side.
 透明基板の一方の面には、5つの薄膜積層構造体が配置される。5つの薄膜積層構造体は、いずれも、中屈折率膜(酸化ジルコニウムチタン(ZrO))、低屈折率膜(酸化珪素(SiO))及び高屈折率膜(酸化チタン(TiO))で構成される合計56層、物理膜厚7647.11nmの繰り返し積層構造である(第3の薄膜積層構造体)。そしてこの第3の薄膜積層構造体において、第1層から第20層までは、透明基板側から上記中屈折率膜と低屈折率膜を交互に積層した繰り返し積層構造であり、第21層から第56層までは、高屈折率膜と低屈折率膜を交互に積層した繰り返し積層構造である。すなわちこの光学フィルタは、透明基板の一方の面に、5つの薄膜積層構造体を有する。 Five thin film laminated structures are disposed on one surface of the transparent substrate. Each of the five thin film laminated structures has a medium refractive index film (zirconium titanium (ZrO 2 )), a low refractive index film (silicon oxide (SiO 2 )), and a high refractive index film (titanium oxide (TiO 2 )). A repetitive laminated structure having a total thickness of 56 and a physical film thickness of 7647.11 nm (third thin film laminated structure). In the third thin film laminated structure, the first layer to the twentieth layer have a repeated laminated structure in which the medium refractive index film and the low refractive index film are alternately laminated from the transparent substrate side. Up to the 56th layer is a repeated laminated structure in which high refractive index films and low refractive index films are alternately laminated. That is, this optical filter has five thin film laminated structures on one surface of a transparent substrate.
 透明基板の他方の面に設けられた光学多層膜は反射防止膜である。この光学多層膜は、比較例1にて用いたものと同様の光学多層膜である。そのため、膜構成、分光特性の説明は省略する。 The optical multilayer film provided on the other surface of the transparent substrate is an antireflection film. This optical multilayer film is the same optical multilayer film as used in Comparative Example 1. Therefore, description of the film configuration and spectral characteristics is omitted.
 上記の光学フィルタの透明基板の一方の面に設けられた薄膜積層構造体(第3の薄膜積層構造体)の構成を表9に示す。表9において、膜層数は透明基板側からの層の序数であり、膜厚は物理膜厚を示す。この光学フィルタについて、入射角0°、40°及び50°における光学特性を、光学薄膜シミュレーションソフト(TFCalc、Software Spectra社製)を用いて検証した。結果を図18、図19(波長850nm~1050nmの領域における拡大図)に示す。また、透明基板の一方の面に設けられた薄膜積層構造体のみ(透明基板による光の吸収の影響を除く)の入射角0°、40°及び50°における光学特性を、上記光学薄膜シミュレーションソフトを用いて検証した。結果を図20に示す。 Table 9 shows the configuration of the thin film laminated structure (third thin film laminated structure) provided on one surface of the transparent substrate of the optical filter. In Table 9, the number of film layers is the ordinal number of layers from the transparent substrate side, and the film thickness indicates the physical film thickness. About this optical filter, the optical characteristic in incident angles 0 degree, 40 degrees, and 50 degrees was verified using optical thin film simulation software (TFCalc, product made by Software Spectra). The results are shown in FIGS. 18 and 19 (enlarged views in the wavelength region of 850 nm to 1050 nm). Further, the optical thin film simulation software described above shows the optical characteristics at the incident angles of 0 °, 40 ° and 50 ° of only the thin film laminated structure (excluding the influence of light absorption by the transparent substrate) provided on one surface of the transparent substrate. It verified using. The results are shown in FIG.
Figure JPOXMLDOC01-appb-T000009
Figure JPOXMLDOC01-appb-T000009
 以上より、例えば、実施例1の光学フィルタは、光の入射角が40°、50°であっても近赤外領域のうち850nm~990nmの透過率が0.1%以下であり、透過リップルが抑制されている。また、同様に光の入射角が40°であっても可視領域(450nm~550nm)の透過率が最小値で92%以上、光の入射角が50°であっても可視領域の透過率の最小値が81%以上であり、反射リップルが抑制されている。また、波長898nm~955nmにおいて透過率が0.0001%以下であり、高い近赤外線の吸収能を備える。 From the above, for example, the optical filter of Example 1 has a transmittance of 850 nm to 990 nm in the near infrared region of 0.1% or less in the near infrared region even when the incident angle of light is 40 ° and 50 °, and the transmission ripple Is suppressed. Similarly, the transmittance in the visible region (450 nm to 550 nm) is 92% or more at the minimum even when the incident angle of light is 40 °, and the transmittance in the visible region is equal even when the incident angle of light is 50 °. The minimum value is 81% or more, and the reflection ripple is suppressed. Further, it has a transmittance of 0.0001% or less at wavelengths of 898 nm to 955 nm, and has a high near infrared absorption ability.
 これに対し、比較例1の光学フィルタは、光の入射角が50°において可視領域(450nm~550nm)の透過率の最小値が80%以下であり、反射リップルが抑制できていない。また、比較例2の光学フィルタは、光の入射角が50°において可視領域(450nm~550nm)の透過率の最小値が80%以下であり、反射リップルが抑制できていない。さらに、光の入射角が0°、40°、50°であっても近赤外領域(850nm~990nm)の透過率が0.1%以上であり、透過リップルが抑制できていない。 On the other hand, the optical filter of Comparative Example 1 has a minimum transmittance of 80% or less in the visible region (450 nm to 550 nm) at a light incident angle of 50 °, and the reflection ripple cannot be suppressed. The optical filter of Comparative Example 2 has a minimum transmittance of 80% or less in the visible region (450 nm to 550 nm) at a light incident angle of 50 °, and the reflection ripple cannot be suppressed. Further, even when the incident angle of light is 0 °, 40 °, and 50 °, the transmittance in the near infrared region (850 nm to 990 nm) is 0.1% or more, and the transmission ripple cannot be suppressed.
 比較例1、2の光の入射角が50°において可視領域の反射リップルが抑制できていないのは、近赤外領域の透過を制限する薄膜積層構造体が、一方の面のみに形成されていることに起因するものと考えられる。 The reason why the reflection ripple in the visible region is not suppressed when the incident angle of light in Comparative Examples 1 and 2 is 50 ° is that the thin film laminated structure that restricts the transmission in the near infrared region is formed only on one surface. This is thought to be due to the fact that
 本発明を詳細に、また特定の実施態様を参照して説明したが、本発明の精神と範囲を逸脱することなく、様々な変更や修正を加えることができることは、当業者にとって明らかである。
 本出願は、2018年3月30日出願の日本特許出願2018-067598に基づくものであり、その内容はここに参照として取り込まれる。
Although the present invention has been described in detail and with reference to specific embodiments, it will be apparent to those skilled in the art that various changes and modifications can be made without departing from the spirit and scope of the invention.
This application is based on Japanese Patent Application No. 2018-067598 filed on Mar. 30, 2018, the contents of which are incorporated herein by reference.
 1…光学フィルタ、2…透明基板、11,12,13…薄膜積層構造体、10a,10b…表面。 DESCRIPTION OF SYMBOLS 1 ... Optical filter, 2 ... Transparent substrate, 11, 12, 13 ... Thin-film laminated structure, 10a, 10b ... Surface.

Claims (6)

  1.  透明基板と、それぞれ近赤外波長領域内の所定の波長範囲の光の透過を制限する、3つ以上の、薄膜積層構造体を備えた光学フィルタであって、
     各々の前記薄膜積層構造体は前記透明基板のいずれか一方の表面上に積層され、
     前記3つ以上の薄膜積層構造体のうち少なくとも2つの薄膜積層構造体は、透過を制限する波長範囲がそれぞれ異なっており、
     前記3つ以上の薄膜積層構造体によって透過が制限される波長範囲が連続しており、
     前記透明基板の少なくとも一方の同一の表面側に配置される前記薄膜積層構造体が透過を制限する波長領域が不連続である、光学フィルタ。
    An optical filter comprising a transparent substrate and three or more thin film laminate structures that limit transmission of light in a predetermined wavelength range in the near-infrared wavelength region,
    Each of the thin film laminated structures is laminated on one surface of the transparent substrate,
    Of the three or more thin film laminated structures, at least two thin film laminated structures have different wavelength ranges for limiting transmission, respectively.
    The wavelength range in which transmission is limited by the three or more thin film laminated structures is continuous,
    An optical filter in which a wavelength region in which transmission of the thin film laminated structure disposed on the same surface side of at least one of the transparent substrates restricts transmission is discontinuous.
  2.  前記3つ以上の薄膜積層構造体のうち、近赤外領域の波長の光の透過を制限する波長範囲の中心波長が2番目に短波長側にある薄膜積層構造体がそれ以外の薄膜積層構造体とは異なる表面に積層され、且つ、物理膜厚が、それ以外の前記薄膜積層構造体のそれぞれの物理膜厚よりも厚いことを特徴とする請求項1に記載の光学フィルタ。 Among the three or more thin film laminated structures, the thin film laminated structure in which the center wavelength in the wavelength range that restricts the transmission of light having a wavelength in the near infrared region is the second shortest wavelength side is the other thin film laminated structure. 2. The optical filter according to claim 1, wherein the optical filter is laminated on a surface different from the body and has a physical film thickness that is larger than each of the other physical film thicknesses of the thin film laminated structure.
  3.  近赤外領域の波長の光の透過を制限する波長範囲の中心波長が2番目に短波長側にある前記薄膜積層構造体の透過制限波長範囲では、前記波長範囲内の最も透過率が低い波長において、透過率が0.05%以下である、請求項2に記載の光学フィルタ。 In the transmission limiting wavelength range of the thin film laminated structure, the wavelength having the center wavelength of the wavelength range that limits the transmission of light in the near-infrared region wavelength is the second shortest wavelength, the wavelength having the lowest transmittance within the wavelength range The optical filter according to claim 2, wherein the transmittance is 0.05% or less.
  4.  前記透明基板は、ガラス、ガラスセラミックス、水晶、樹脂及びサファイアから選ばれるいずれか1つ以上からなる、請求項1~3のいずれか1項に記載の光学フィルタ。 The optical filter according to any one of claims 1 to 3, wherein the transparent substrate is made of at least one selected from glass, glass ceramics, crystal, resin, and sapphire.
  5.  前記透明基板は、近赤外領域の波長の光を吸収する性質を有する、請求項1~4のいずれか1項に記載の光学フィルタ。 The optical filter according to claim 1, wherein the transparent substrate has a property of absorbing light having a wavelength in a near infrared region.
  6.  前記透明基板の少なくとも一方の表面上に、近赤外領域の波長の光を吸収する成分を含む近赤外線吸収層を有する、請求項1~5のいずれか1項に記載の光学フィルタ。 6. The optical filter according to claim 1, further comprising a near-infrared absorbing layer including a component that absorbs light having a wavelength in the near-infrared region on at least one surface of the transparent substrate.
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