Patent Application
20150276985
1. Field
The present disclosure relates to optical materials and methods for producing the optical materials, optical elements, and hybrid optical elements.
2. Description of the Related Art
High-precision imaging devices such as digital still cameras adopt optical systems having a plurality of lens units, and various optical materials having different optical constants such as refractive indices, Abbe numbers, partial dispersion ratios are required. Therefore, optical glass materials and optical resin materials having various optical constants have been developed and used. In particular, optical glass materials having high refractive indices and high Abbe numbers have been frequently used in many imaging devices to improve optical performances thereof.
On the other hand, technological development has been actively conducted for synthesizing moldable nano-composite materials having optical constants which could not be achieved by conventional resin materials, by dispersing nano-fine particles having specific optical constants in resin materials. Such nano-composite materials having optical constants which could not be achieved even by optical glass are expected as substitutions for optical glass having specific optical constants such as a high refractive index and a high Abbe number, or optical glass having poor durability.
Among the nano-composite materials, a nano-composite material having a high refractive index has been actively developed. Japanese Laid-Open Patent Publication No. 2006-089706 discloses a material using yttrium oxide (Y2O3) as inorganic fine particles, and Japanese Laid-Open Patent Publication No. 2008-203821 discloses a material containing Al, Si, Ti, Zr, Ga, La, or the like.
The present disclosure provides: an optical material whose optical constants can be freely controlled in a wide range, and in particular, which has negative anomalous dispersion that cannot be achieved by optical glass, while maintaining high transmittance; a method for producing the optical material; and an optical element and a hybrid optical element each formed of the optical material.
The novel concepts disclosed herein were achieved in order to solve the foregoing problems in the related art, and herein is disclosed:
an optical material comprising a resin material and inorganic fine particles dispersed in the resin material, wherein
the inorganic fine particles are fine particles foamed of SiO2, and at least a part of a surface of each SiO2 fine particle is SiON obtained by substituting oxygen atoms at the surface with carbon atoms and then substituting the carbon atoms with nitrogen atoms.
The novel concepts disclosed herein were achieved in order to solve the foregoing problems in the related art, and herein is disclosed:
an optical element formed of an optical material composed of a resin material and inorganic fine particles dispersed in the resin material, wherein
the inorganic fine particles are fine particles formed of SiO2, and at least a part of a surface of each SiO2 fine particle is SiON obtained by substituting oxygen atoms at the surface with carbon atoms and then substituting the carbon atoms with nitrogen atoms.
The novel concepts disclosed herein were achieved in order to solve the foregoing problems in the related art, and herein is disclosed:
a hybrid optical element comprising a first optical element and a second optical element disposed on an optical surface of the first optical element, wherein
the second optical element is an optical element formed of an optical material composed of a resin material and inorganic fine particles dispersed in the resin material, wherein
the inorganic fine particles are fine particles formed of SiO2, and at least a part of a surface of each SiO2 fine particle is SiON obtained by substituting oxygen atoms at the surface with carbon atoms and then substituting the carbon atoms with nitrogen atoms.
The novel concepts disclosed herein were achieved in order to solve the foregoing problems in the related art, and herein is disclosed:
a method for producing an optical material composed of a resin material and inorganic fine particles dispersed in the resin material, wherein
the inorganic fine particles are fine particles formed of SiO2, and
the method comprises the steps of:
substituting oxygen atoms in at least a part of a surface of each SiO2 fine particle with carbon atoms; and
further substituting the carbon atoms with nitrogen atoms.
The optical material according to the present disclosure is a composite material in which SiO2 fine particles, each having a surface at least a part of which is SiON, are dispersed in a resin material. The composite material allows free control of its optical constants in a wide range, and in particular, has negative anomalous dispersion that cannot be achieved by optical glass, while maintaining high transmittance.
This and other objects and features of the present disclosure will become clear from the following description, taken in conjunction with the exemplary embodiments with reference to the accompanied drawings in which:
Hereinafter, embodiments will be described with reference to the drawings as appropriate. However, descriptions more detailed than necessary may be omitted. For example, detailed description of already well known matters or description of substantially identical configurations may be omitted. This is intended to avoid redundancy in the description below, and to facilitate understanding of those skilled in the art.
It should be noted that the applicants provide the attached drawings and the following description so that those skilled in the art can fully understand this disclosure. Therefore, the drawings and description are not intended to limit the subject defined by the claims.
Hereinafter, Embodiment 1 is described with reference to the drawings.
[1. Composite Material]
As shown in
[2. Inorganic Fine Particles]
The inorganic fine particles 20 are fine particles formed of SiO2. The surface of each SiO2 fine particle is SiON obtained by substituting oxygen atoms with nitrogen atoms. The entire surface of each SiO2 fine particle may be formed of SiON, or a part of the surface may be formed of SiON. Thus, the inorganic fine particles 20 according to the present disclosure each have a structure similar to a so-called core-shell structure having a core formed of SiO2, and a shell formed of SiON which covers at least a part of the surface of the SiO2 core. The structure of the inorganic fine particles 20 according to the present disclosure is also referred to as an SiO2—SiON structure.
The inorganic fine particles 20 may be either aggregated particles or non-aggregated particles. Generally, the inorganic fine particles 20 include primary particles 20a and secondary particles 20b which are aggregates of the primary particles 20a. The dispersion state of the inorganic fine particles 20 is not particularly limited because desired effects can be obtained as long as the inorganic fine particles 20 are present in the resin material 10 serving as a matrix material. However, it is beneficial that the inorganic fine particles 20 are uniformly dispersed in the resin material 10. As used herein, “the inorganic fine particles 20 uniformly dispersed in the resin material 10” means that the primary particles 20a and the secondary particles 20b of the inorganic fine particles 20 are substantially uniformly dispersed in the composite material 100 without being localized in any particular region in the composite material 100. It is beneficial that the particles have good dispersion property in order to prevent light transmittance of the optical material from being degraded. For this purpose, it is beneficial that the inorganic fine particles 20 consist of only the primary particles 20a.
The particle diameter of the inorganic fine particles 20 is an essential factor in ensuring the light transmittance of the composite material 100 in which the inorganic fine particles 20 having the SiO2—SiON structure are dispersed in the resin material 10. When the particle diameter of the inorganic fine particles 20 is sufficiently smaller than the wavelength of light, the composite material 100 in which the inorganic fine particles 20 are dispersed in the resin material 10 can be regarded as a homogeneous medium without variations in the refractive index. Therefore, it is beneficial that the particle diameter of the inorganic fine particles 20 is equal to or smaller than the wavelength of visible light. Since visible light has wavelengths ranging from 400 nm to 700 nm, it is beneficial that the maximum particle diameter of the inorganic fine particles 20 is 400 nm or less. It is noted that the maximum particle diameter of the inorganic fine particles 20 can be obtained by taking a scanning electron microscope photograph of the inorganic fine particles 20 and measuring the particle diameter of the largest inorganic fine particle 20 (the secondary particle diameter if the largest particle is a secondary particle).
When the particle diameter of the inorganic fine particles 20 is larger than one fourth of the wavelength of light, the light transmittance of the composite material 100 may be degraded by Rayleigh scattering. Therefore, it is beneficial that the effective particle diameter of the inorganic fine particles 20 is 100 nm or less in order to achieve high light transmittance in the visible light region. However, when the effective particle diameter of the inorganic fine particles 20 is less than 1 nm, fluorescence may occur if the inorganic fine particles 20 are made of a material that exhibits quantum effects. This fluorescence may affect the properties of an optical component formed of the composite material 100.
From the viewpoints described above, the effective particle diameter of the inorganic fine particles 20 is beneficially in the range from 1 nm to 100 nm, and more beneficially in the range from 1 nm to 50 nm. In particular, it is further beneficial that the effective particle diameter of the inorganic fine particles 20 is 20 nm or less because the negative effect of Rayleigh scattering is very small while the light transmittance of the composite material 100 is particularly high.
The effective particle diameter of the inorganic fine particles is described with reference to
As described above, the composite material 100 according to Embodiment 1 is obtained by dispersing the inorganic fine particles 20 having the SiO2—SiON structure in the resin material 10. The composite material 100 thus obtained allows easier control of optical properties in a wider range as compared to the case of using inorganic fine particles of SiO2 only, and in particular, allows significant reduction in the anomalous dispersion without degrading the transmittance.
νd=(nd−1)/(nF−nC) (1)
where
nd is the refractive index of the material to the d-line,
nF is the refractive index of the material to the F-line (wavelength of 486.1 nm), and
nC is the refractive index of the material to the C-line (wavelength of 656.3 nm)
PgF=(ng−nF)/(nF−nC) (2)
where
ng is the refractive index of the material to the g-line,
nF is the refractive index of the material to the F-line, and
nC is the refractive index of the material to the C-line.
The anomalous dispersion property ΔPgF is a deviation of the PgF of each material from a point on the reference line of normal partial dispersion glass corresponding to the νd of the material. In the present disclosure, the ΔPgF is calculated using a straight line (normal dispersion line in
As shown in
Further, in the SiO2—SiON structure, the optical properties can be controlled in a wider range and the negative anomalous dispersion can be enhanced, by increasing the ratio of SiON at the surface of SiO2 fine particle.
[3. Resin Material]
As the resin material 10, resins having high light transmittance, selected from resins such as thermoplastic resins, thermosetting resins, and energy ray-curable resins, can be used. For example, acrylic resins; methacrylic resins such as polymethyl methacrylate; epoxy resins; polyester resins such as polyethylene terephthalate, polybutylene terephthalate, and polycaprolactone; polystyrene resins such as polystyrene; olefin resins such as polypropylene; polyamide resins such as nylon; polyimide resins such as polyimide and polyether imide; polyvinyl alcohol; butyral resins; vinyl acetate resins; alicyclic polyolefin resins; silicone resins; and amorphous fluororesins may be used. Engineering plastics such as polycarbonate, liquid crystal polymers, polyphenylene ether, polysulfone, polyether sulfone, polyarylate, and amorphous polyolefin also may be used. Mixtures and copolymers of these resins also may be used. Resins obtained by modifying these resins also may be used.
Among these, acrylic resins, methacrylic resins, epoxy resins, polyimide resins, butyral resins, alicyclic polyolefin resins, and polycarbonate are beneficial because these resins have high transparency and good moldability. These resins can have refractive indices nd ranging from 1.4 to 1.7 by selecting a specific molecular skeleton.
The Abbe number νdm of the resin material 10 to the d-line is not particularly limited. Needless to say, the Abbe number νdCOM of the composite material 100 to the d-line, which is obtained by dispersing the inorganic fine particles 20, increases as the Abbe number νdm of the resin material 10 serving as a matrix material increases. In particular, it is beneficial to use a resin having an Abbe number νdm of 45 or more as the resin material 10 because the use of such a resin makes it possible to obtain a composite material having optical properties, such as an Abbe number νdCOM of 40 or more, enough for use in optical components such as lenses. Examples of the resin having an Abbe number νdm of 45 or more include: alicyclic polyolefin resins having an alicyclic hydrocarbon group in the skeleton; silicone resins having a siloxane structure; and amorphous fluororesins having a fluorine atom in the main chain. However, the resin having an Abbe number νdm of 45 or more is not limited to these resins.
[4. Optical Properties of Composite Material]
The refractive index of the composite material 100 can be estimated from the refractive indices of the inorganic fine particles 20 and the resin material 10, for example, based on the Maxwell-Garnett theory represented by the following formula (3). It is also possible to estimate the refractive indices of the composite material 100 to the d-line, the F-line, and the C-line from the following formula (3), and further estimate the Abbe number νd of the composite material 100 from the above formula (1). Conversely, the weight ratio between the resin material 10 and the inorganic fine particles 20 may be determined from the estimation based on this theory.
nλ
COM
2
=[{nλ
p
2+2nλm2+2P(nλp2−nλm2)}/{nλp2+2nλm2−P(nλp2−nλm2)}]×nλm2 (3)
where
nλCOM is the average refractive index of the composite material 100 at a specific wavelength λ,
nλp is the refractive index of the inorganic fine particles 20 at the specific wavelength λ,
nλm is the refractive index of the resin material 10 at the specific wavelength λ, and
P is the volume ratio of the inorganic fine particles 20 to the composite material 100 as a whole.
In the case where the inorganic fine particles 20 absorb light or where the inorganic fine particles 20 contain metal, complex refractive indices are used as the refractive indices in the formula (3) for calculation. The formula (3) holds in the case of nλp≧nλm, and in the case of nλp<nλm, the refractive index of the composite material 100 is estimated by using the following formula (4):
nλ
COM
2
=[{nλ
m
2+2nλp2+2(1−P)(nλm2−nλp2)}/{nλm2+2nλp2−(1−P)(nλm2−nλp2)}]×nλp2 (4)
where nλCOM, nλp, nλm, and P are the same as those of the formula (3).
The actual refractive index of the composite material 100 can be evaluated by film-forming or molding the prepared composite material 100 into a shape suitable for a measurement method to be used, and actually measuring the formed or molded product by the method. The method is, for example, a spectroscopic measurement method such as an ellipsometric method, an Abeles method, an optical waveguide method or a spectral reflectance method, or a prism-coupler method.
A description is given of the optical properties of the composite material 100 estimated by using the above-mentioned Maxwell-Garnett theory, and the content of the inorganic fine particles 20 in the composite material 100. When the content of the inorganic fine particles 20 in the composite material 100 is too small, the effect of adjustment of the optical properties due to the inorganic fine particles 20, in particular, the effect of imparting negative anomalous dispersion, may not be sufficiently obtained. Therefore, the content of the inorganic fine particles 20 is beneficially 1% by weight or more, more beneficially 5% by weight or more, and further beneficially 10% by weight or more, with respect to the total weight of the composite material (optical material) 100. On the other hand, when the content of the inorganic fine particles 20 in the composite material 100 is too large, the fluidity of the composite material 100 decreases, which may make it difficult to mold the composite material 100 into optical elements, or even to add the inorganic fine particles 20 into the resin material 10. Thus, the content of the inorganic fine particles 20 is beneficially 80% by weight or less, more beneficially 60% by weight or less, and further beneficially 40% by weight or less, with respect to the total weight of the composite material 100.
[5. Production Method of Composite Material]
First, a method for forming the inorganic fine particles 20 is described. The inorganic fine particles 20 are formed by subjecting SiO2 fine particles to heat treatment under a predetermined gas atmosphere so that oxygen atoms at the surface of each SiO2 fine particle are substituted with nitrogen atoms, thereby to form SiON at the surface.
First, nitrogen gas is flowed at a flow rate of about 900 to 1100 ml/min to increase the temperature of the SiO2 fine particles to about 580 to 620° C. Thereafter, flow of the nitrogen gas is stopped, and ammonia gas is flowed at a flow rate of about 850 to 1100 ml/min, and simultaneously, hydrocarbon gas is flowed at a flow rate of about 5 to 15 ml/min to increase the temperature of the SiO2 fine particles to a predetermined temperature. At this temperature, heat treatment is carried out for about 0.5 to 3 hours to calcine the SiO2 fine particles with ammonia. After the calcined fine particles are slowly cooled to about 630 to 670° C., flow of the ammonia gas and flow of the hydrocarbon gas are stopped. Then, nitrogen gas is flowed at a flow rate of about 900 to 1100 ml/min, followed by slow cooling. Thus, the inorganic fine particles 20 having the desired SiO2—SiON structure are obtained.
Although the SiO2—SiON structure is formed by calcining the SiO2 fine particles with ammonia, flow of the hydrocarbon gas is performed simultaneously with flow of the ammonia gas as described above. The reason is as follows. Since activation energy for directly substituting oxygen atoms of SiO2 with nitrogen atoms is excessively high, oxygen atoms of SiO2 are first substituted with carbon atoms and then the carbon atoms are substituted with nitrogen atoms. Therefore, as the hydrocarbon gas, for example, ethylene gas, propane gas, butane gas, or the like may be used. Alternatively, solid carbon may be used.
The temperature for calcining the SiO2 fine particles with ammonia is beneficially 1100 to 1400° C. When the calcining temperature is lower than 1100° C., oxygen atoms of SiO2 are hardly substituted with nitrogen atoms, and no SiO2−SiON structure may be formed, which may cause the SiO2 fine particles to remain. On the other hand, when the calcining temperature exceeds 1400° C., not only oxygen atoms at the surface of each SiO2 fine particle but also oxygen atoms inside the particle are substituted with nitrogen atoms, and no SiO2—SiON structure may be formed, which may results in Si3N4 fine particles. A composite material obtained by dispersing such Si3N4 fine particles in a resin material has reduced transmittance due to black color of Si3N4, and therefore, is not suitable as an optical material.
Next, a method for preparing the composite material 100 is described. There is no particular limitation on the method for preparing the composite material 100 by dispersing the inorganic fine particles 20 formed by the above-described method in the resin material 10 serving as a matrix material. The composite material 100 may be prepared by a physical method or by a chemical method. For example, the composite material 100 can be prepared by any of the following Methods (1) to (4).
Method (1): A resin or a solution in which a resin is dissolved is mechanically and/or physically mixed with inorganic fine particles.
Method (2): A monomer, an oligomer, or the like as a raw material of a resin is mechanically and/or physically mixed with inorganic fine particles to obtain a mixture, and then the monomer, the oligomer, or the like as a raw material of a resin is polymerized.
Method (3): A resin or a solution in which a resin is dissolved is mixed with a raw material of inorganic fine particles, and then the raw material of the inorganic fine particles is reacted so as to form the inorganic fine particles in the resin.
Method (4): After a monomer, an oligomer, or the like as a raw material of a resin is mixed with a raw material of inorganic fine particles, a step of reacting the raw material of inorganic fine particles so as to form the inorganic fine particles and a step of polymerizing the monomer, the oligomer, or the like as a raw material of a resin so as to synthesize the resin are performed.
The above methods (1) and (2) are advantageous in that various pre-formed inorganic fine particles can be used and that composite materials can be prepared by a general-purpose dispersing machine On the other hand, the above methods (3) and (4) require chemical reactions, and therefore, usable materials are limited to some extent. However, since the raw materials are mixed at the molecular level in the methods (3) and (4), these methods are advantageous in that the dispersion property of the inorganic fine particles can be enhanced.
In the above methods, there is no particular limitation on the order of mixing the inorganic fine particles or the raw material of the inorganic fine particles with a resin, or a monomer, an oligomer, or the like as the raw material of the resin. A desirable order can be selected as appropriate. For example, the resin or the raw material of the resin or a solution in which the resin or the raw material of the resin is dissolved may be added to a solution in which inorganic fine particles having a primary particle diameter substantially in the range from 1 nm to 100 nm are dispersed to mix them mechanically and/or physically. The production method of the composite material 100 is not particularly limited as long as the effect of the present disclosure can be achieved.
The composite material 100 may contain components other than the inorganic fine particles 20 and the resin material 10 serving as a matrix material, as long as the effect of the present disclosure can be achieved. For example, a dispersant or a surfactant that improves the dispersion property of the inorganic fine particles 20 in the resin material 10, or a dye or a pigment that absorbs electromagnetic waves within a specific range of wavelengths may coexist in the composite material 100, although not shown in the drawings.
There is no particular limitation on the method for producing an optical element such as a lens from the composite material 100, and known techniques may be adopted. For example, the composite material 100 may be filled in a mold having a shape corresponding to an optical element such as a lens, and cured with an energy ray such as an ultraviolet ray being applied thereto, thereby to form an optical element such as a lens.
Hereinafter, Embodiment 2 is described with reference to the drawings.
The first lens 31 is a first optical element, and an example of a glass lens. The first lens 31 is formed of a glass material, and is a bi-convex lens.
The second lens 32 is a second optical element, and an example of a resin lens. The second lens 32 is formed of a composite material, and the composite material 100 according to Embodiment 1 is used as the composite material.
The both surfaces of the hybrid lens 30 shown in
There is no particular limitation on the method for producing the hybrid lens 30, and known techniques may be adopted. For example, the hybrid lens 30 may be produced as follows. After the first lens 31 as an example of a glass lens is molded by lens polishing, injection molding, press molding, or the like, the composite material 100 is filled in a mold having a shape corresponding to the second lens 32, and the first lens 31 is placed onto the composite material 100 so that the composite material 100 is pressed and extended to a predetermined thickness. Then, for example, an energy ray such as an ultraviolet ray is applied toward the top of the first lens 31 to cure the composite material 100, thereby obtaining the hybrid lens 30 as an example of a hybrid optical element in which the second lens 32 is disposed on the optical surface of the first lens 31.
As described above, Embodiments 1 to 2 have been described as examples of art disclosed in the present application. However, the art in the present disclosure is not limited to these embodiments. It is understood that various modifications, replacements, additions, omissions, and the like have been performed in these embodiments to give optional embodiments, and the art in the present disclosure can be applied to the optional embodiments.
Hereinafter, examples according to the embodiments of the present disclosure, and comparative examples are described. However, the present disclosure is not limited to these examples.
First, nitrogen gas was flowed at a flow rate of 1000 ml/min, and SiO2 fine particles (AEROSIL (registered trademark) 380, hydrophilic fumed silica, specific surface area: 380 m2/g, manufactured by NIPPON AEROSIL CO., LTD.) in a calcining container made of alumina were heated up to 600° C. Next, flow of the nitrogen gas was stopped, and ammonia gas was flowed at a flow rate of 990 ml/min, and simultaneously, ethylene gas was flowed at a flow rate of 10 ml/min, and the SiO2 fine particles were heated up to 1400° C. At this temperature, heat treatment was carried out for one hour to calcine the SiO2 fine particles with ammonia.
After the calcined fine particles were slowly cooled down to 650° C., flow of the ammonia gas and flow of the ethylene gas were stopped. Then, nitrogen gas was flowed at a flow rate of 1000 ml/min, followed by slow cooling, thereby to obtain inorganic fine particles having the SiO2—SiON structure.
Thus obtained inorganic fine particles having the SiO2—SiON structure were subjected to surface element analysis by using an X-ray photoelectron spectroscopic apparatus (Quantera SXM, manufactured by ULVAC-PHI, Inc.) to obtain the composition ratio of C, N, O and Si. Further, the SiO2 fine particles as a raw material, and Si3N4 (SII08PB manufactured by Kojundo Chemical Laboratory Co., Ltd.) formed by substitution of all oxygen atoms of SiO2 with nitrogen atoms were also subjected to similar surface element analysis to obtain the composition ratio of C, N, O and Si. Table 1 shows the results.
As shown in Table 1, it is found, from the percentages of N and O, that the inorganic fine particles having the SiO2—SiON structure have a surface composition corresponding to an intermediate between SiO2 and Si3N4.
The inorganic fine particles obtained in Production Example 1 were blended into a diethylacrylamide resin A, and the particles and the resin A were mixed by stirring to obtain composite materials of Examples 1 to 3. The contents of the inorganic fine particles in the composite materials were 10% by weight (Example 1), 15% by weight (Example 2), and 20% by weight (Example 3), respectively.
Only the diethylacrylamide resin A was used as a composite material without blending the inorganic fine particles obtained in Production Example 1.
The inorganic fine particles obtained in Production Example 1 were blended into a diethylacrylamide resin B, and the particles and the resin B were mixed by stirring to obtain composite materials of Examples 4 to 6. The contents of the inorganic fine particles in the composite materials were 10% by weight (Example 4), 15% by weight (Example 5), and 20% by weight (Example 6), respectively.
Only the diethylacrylamide resin B was used as a composite material without blending the inorganic fine particles obtained in Production Example 1.
The inorganic fine particles obtained in Production Example 1 were blended into a diethylacrylamide resin C, and the particles and the resin C were mixed by stirring to obtain composite materials of Examples 7 to 9. The contents of the inorganic fine particles in the composite materials were 10% by weight (Example 7), 15% by weight (Example 8), and 20% by weight (Example 9), respectively.
Only the diethylacrylamide resin C was used as a composite material without blending the inorganic fine particles obtained in Production Example 1.
The materials of Examples 1 to 9 and the materials of Comparative Examples 1 to 3 were subjected to measurement of refractive indices to the g-line, the F-line, the d-line, and the C-line by using a precision refractometer (KPR-200, manufactured by Shimadzu Device Corporation), and the Abbe numbers νd and the partial dispersion ratios PgF were calculated from the above formulae (1) and (2). Further, the anomalous dispersion properties ΔPgF were calculated from the following formula (5). Table 2 shows the results.
ΔPgF=PgF−(−0.001802397685×νd+0.648327036) (5)
As shown in Table 2, the composite materials (optical materials) of Examples 1 to 9 each have the negative anomalous dispersion which cannot be achieved by optical glass, due to the effect of the optical property of SiON at the surface of each inorganic fine particle having the SiO2−SiON structure. As compared to the materials of Comparative Examples 1 to 3 in which the inorganic fine particles having the SiO2—SiON structure are not used, the composite materials of Examples 1 to 3, Examples 4 to 6, and Examples 7 to 9 each have reduced anomalous dispersion. In particular, the composite materials of Examples 3, 6 and 9 each have the anomalous dispersion reduced by 0.06 as compared to the materials of Comparative Examples 1 to 3. That is, the inorganic fine particles having the SiO2—SiON structure can significantly reduce the anomalous dispersion. Thus, it is found that the composite materials of Examples 1 to 9 each allow free control of its optical constants in a wide range, and consequently, a property of negative anomalous dispersion is imparted.
The present disclosure can be suitably used for optical elements such as a lens, a prism, an optical filter, and a diffractive optical element.
As described above, embodiments have been described as examples of art in the present disclosure. Thus, the attached drawings and detailed description have been provided.
Therefore, in order to illustrate the art, not only essential elements for solving the problems but also elements that are not necessary for solving the problems may be included in elements appearing in the attached drawings or in the detailed description. Therefore, such unnecessary elements should not be immediately determined as necessary elements because of their presence in the attached drawings or in the detailed description.
Further, since the embodiments described above are merely examples of the art in the present disclosure, it is understood that various modifications, replacements, additions, omissions, and the like can be performed in the scope of the claims or in an equivalent scope thereof.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2014-060155 | Mar 2014 | JP | national |
This application is a Continuation of International Application No. PCT/JP2014/005412, filed on Oct. 27, 2014, which in turn claims the benefit of Japanese Application No. 2014-060155, filed on Mar. 24, 2014, the disclosures of which Applications are incorporated by reference herein.
| Number | Date | Country | |
|---|---|---|---|
| Parent | PCT/JP2014/005412 | Oct 2014 | US |
| Child | 14738015 | US |
