The present application is based upon and claims the benefit of priority from the prior Japanese Patent Application No. 2011-024223 filed on Feb. 7, 2011; the entire contents of which are incorporated herein by reference.
1. Field of the Invention
The present invention relates to an optical element having anti-reflection film.
2. Description of the Related Art
In an optical element such as a lens or a prism used in a camera, a microscope, an endoscope, and binoculars, for suppressing surface reflection and improving a transmittance of light of the optical element, an anti-reflection film is formed on a surface of the optical element.
A number of basic structures have been known for the anti-reflection film. For instance, on page 127 of ‘Optical thin film’ written by H. A. Maclaod, translated by Ogura Shigetaro et al., published by ‘NIKKAN KOGYO SHINBUN LTD. (BUSINESS & TECHNOLOGY DAILY NEWS)’, the following film structure has been described. A film structure of a glass substrate (refractive index n=1.52), a first layer (refractive index n=1.90, optical film thickness 1.00), a second layer (refractive index n=2.00, optical film thickness 1.00), a third layer (refractive index n=1.38, optical film thickness 1.00), and air, when an optical film thickness λ0/4 at a reference wavelength λ0 (unit: nm) is let to be λ0/4=1.00, has been described.
The authors have indicated a result when a reflectance characteristic was calculated letting the reference wavelength λ0=530 nm as the anti-reflection film of a visible range from this film structure. A curve of the reflectance characteristic has a W-shaped waveform when a horizontal axis is let to be wavelength (unit: nm) and a vertical axis is let to be reflectance (unit: %). Therefore, it is called as a W-coat. Moreover, in Japanese Patent Application Laid-open Publication No. Sho 52-76942, from a point of view of productivity, a W-coat having a five-layered structure or a seven-layered structure in which a film material having refractive indices of two types namely high refractive index and low refractive index are used.
In an optical element such as a lens and a prism, it is desirable that a ghost image and a flare are reduced as much as possible. This is because when there is a ghost image or a flare on a screen or in a field of view, an image quality is degraded or an observation of an object is hindered. A ghost image and a flare occur due to light being reflected for a plurality of times (for example, internal reflection) between a front lens surface and a rear lens surface, or between lenses.
Even when an anti-reflection film is formed on a specific optical surface, due to the abovementioned W-shaped characteristic curve, it is difficult to reduce the reflectance characteristic uniformly in all ranges of a desired wavelength range. Accordingly, at the optical surface on which the anti-reflection film is formed, light of a wavelength for which an intensity of light cannot be reduced fully, is reflected at a certain optical surface (first reflecting surface), and is incident on another optical surface (second reflecting surface). Furthermore, by light which has been reflected from the second reflecting surface, forming an image on an image forming surface, or being incident on an image pickup element, there is a ghost image or a flare.
An optical element having anti-reflection film according to the present invention is an optical element which is used in an optical system for guiding light generated from a light source, to an image pickup element or an image forming surface, includes
an anti-reflection film having a reflectance characteristic expressed by a function Fm(x) (where, x denotes a wavelength), which is formed on an mth optical surface when counted from a side of the light source, and
an anti-reflection film having a reflectance characteristic expressed by a function Fn(x) (where, x denotes a wavelength), which is formed on an nth optical surface when counted from the side of the light source, and
at least one of the function Fm(x) and the function Fn(x) has the maximum value of reflectance in a predetermined wavelength, and has a characteristic curve of W-shape, and
the other of the function Fm(x) and the function Fn(x) has a wavelength that negates at least one maximum value of one of the function Fm(x) and the function Fn(x), and
the anti-reflection film having reflectance characteristic expressed by the function Fm(x) is formed on an optical surface on a side nearer to the light source, than the anti-reflection film having reflectance characteristic expressed by the function Fn(x),
where, m and n are positive integers, and m<n.
Examples of an optical element having anti-reflection film according to the present invention will be described below in detail by referring to the accompanying diagrams. However, the present invention is not restricted to the examples described below.
In these examples, cases in which, lenses of glass materials having three types of refractive indices, and anti-reflection films corresponding to the refractive indices of the glass material are combined will be described. However, the present invention is not restricted to the following examples. Moreover, refractive indices are not restricted to the refractive indices of the glass materials described in these examples.
A method of forming an anti-reflection film on a lens or a prism may be any of a vacuum vapor deposition method, a sputtering method, an ion assist film-forming method, a chemical vapor deposition method, a spin coat method, and a dipping method.
Moreover, an optical film thickness of a film structure of these examples is a value when λ0/4 at a reference wavelength (unit: nm) is let to be λ0/4=1.00.
The optical element having anti-reflection film according to an embodiment will be described below.
The optical system 10 is used for guiding light from the light source 11 to the image pickup element 12. The lens La and the lens Lb are optical elements in the optical system 10.
An anti-reflection film Lm having reflectance characteristic expressed by a function Fn(x) (where, x denotes a wavelength), is formed on an mth optical surface, when counted from the side of the light source 11.
Moreover, an anti-reflection film Ln having reflectance characteristic expressed by a function Fn(x) (where, x denotes the wavelength), is formed on an nth optical surface, when counted from the side of the light source 11.
Here, m and n are positive integers, and m<n.
Here, an angle of incidence is an angle z (unit: degree) between a normal N of an incidence surface and a light of incidence as shown in
In
A curve which indicates the reflectance characteristic is let to be a function Fn(x). The function Fn(x), as it is clear from
Structures of seven types of examples from the anti-reflection film H1 to the anti-reflection film H7 are indicated below in tables from table 2 to table 8 respectively.
Next, a result of calculating an average value of reflectance characteristic of the anti-reflection film Ln (two types W1 and W2) and the anti-reflection film Lm (seven types H1 to H7) at the angle of incidence 0° is shown.
G1—00=(H1—00+W1—00)/2
G2—00=(H2—00+W2—00)/2
G3—00=(H3—00+W1—00)/2
G4—00=(H4—00+W2—00)/2
G5—00=(H5—00+W1—00)/2
G6—00=(H6—00+W2—00)/2
G7—00=(H7—00+W2—00)/2
Conventional examples in which, the average value of reflectance characteristic is calculated for comparison and reference are shown below.
In
As a first example for comparison
W1—00=(W1—00+W1—00)/2
As a second example for comparison
W2—00=(W2—00+W2—00)/2
As a third example for comparison
Wa
—00=(W1—00+W2—00)/2
In
As a first example for comparison
W1—30=(W1—30+W1—30)/2
As a second example for comparison
W2—30=(W2—30+W2—30)/2
As a third example for comparison
Wa
—30=(W1—30+W2—30)/2
G1—30=(H1—30+W1—30)/2
G2—30=(H2—30+W2—30)/2
G3—30=(H3—30+W1—30)/2
G4—30=(H4—30+W2—30)/2
G5—30=(H5—30+W1—30)/2
G6—30=(H6—30+W2—30)/2
G7—30=(H7—30+W2—30)/2
A difference between the maximum value and the minimum value of reflectance in a range of wavelength 450 nm ˜650 nm in diagrams from
As shown in table 9, when in a range 0°≦z≦30° of the angle of incidence z of a light ray with respect to the anti-reflection film, G(x) is let to be
G(x)=(Fm(x)+Fn(x))/2,
In the range of wavelength x=450 nm˜650 nm at the predetermined angle of incidence within the range, a reflectance difference f % between the maximum value and the minimum value of the function Fn(x) and a reflectance difference g % between the maximum value and the minimum value of the function G(x) at the predetermined angle of incidence, satisfy the following expression.
g≦f
Accordingly, the ghost image and flare are reduced.
In these examples, two types W1 and W2 are mentioned as the anti-reflection film Ln. Reflectance characteristic of W1 is as shown in
Next, an anti-reflection band of the anti-reflection film Lm (seven types from H1 to H7) and the anti-reflection film. Ln (two types W1 and W2) at the angle of incidence 0° and 30° is shown in table 10. The ‘anti-reflection band’ means a value which is obtained by reading a width of the wavelength range in which the reflectance is 1% or less, and by rounding off the units. For instance, when the wavelength of an end of a short-wavelength side for which the reflectance is 1% is 400 nm and the wavelength of an end of a long-wavelength side is 700 nm, the anti-reflection band of the anti-reflection film is calculated to be ‘700 nm-400 nm’, which is 300 nm.
As shown in table 10, when the anti-reflection band of the anti-reflection film Lm (seven types H1 to H7) for which the reflectance characteristic is Fm(X) is let to be Uz (unit: nm), and the anti-reflection band of the anti-reflection film Ln (two types W1 and W2) for which the reflectance characteristic is Fn(X) is let to be Vz (unit: nm), the anti-reflection band in the range 0°≦z≦30° of the angle of incidence z is Vz≦Uz.
Accordingly, in the wavelength range, the reflection of light is prevented, and the ghost image and flare are reduced.
A diagrammatic example in which, the anti-reflection band Uz when the angle of incidence is 0° is shown as the function Fm (X) of the reflectance characteristic in the diagram is shown in
Diagrams of the other examples are also similar to
As it is shown in
Accordingly, in a wide range of the angle of incidence, the reflection of light is prevented, and the ghost image and flare are reduced.
Let a curve expressing the reflectance characteristic of the anti-reflection film formed on the mth optical surface be the function Fm(x). The function Fm(x), as it is evident from
Moreover, the anti-reflection film Lm having reflectance characteristic shown by the function Fm(x) is formed on the optical surface on a side nearer to the light source 11, than the anti-reflection film Ln having reflectance characteristic shown by the function Fn(x).
Accordingly, it is possible to reduce light reflected from the nth optical surface, at the mth optical surface. Therefore, it is possible to reduce the ghost image and flare.
As it has been described above, the present invention is useful for an optical system having a lens and a prism for reducing the flare and ghost image.
The present invention shows an effect that it is possible to provide an optical element having an anti-reflection film with a favorable reflectance, which reduces the ghost image and flare.
Number | Date | Country | Kind |
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2011-024223 | Feb 2011 | JP | national |