JP2017021324A - Varifocal lens - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a varifocal lens capable of changing a focal length at high speed without depending on polarization of incident light.SOLUTION: A varifocal lens comprises: an electro-optical material made of a single crystal having inversion symmetry; and a plurality of electrode pairs which are formed at positions severally facing a first face of the electro-optical material and a second face opposing to the first face, in which a cylindrical varifocal lens which varies a focal point of light passing through the electro-optical material by changing an applied voltage between the electrode pairs is used as a basic unit element, a polarization beam splitter, a Faraday rotation element, the basic unit element and a reflector are arrayed in order while sharing an optical axis, light of a given polarization direction which is made incident to the polarization beam splitter passes through the basic unit element after passing through the Faraday rotation element, is reflected on the reflector, passes through the basic unit element again, and passes through the Faraday rotation element to be emitted from the polarization beam splitter.SELECTED DRAWING: Figure 4

Description

  The present invention relates to a variable focus lens, and more particularly to a variable focus lens that can change a focal length using an optical material having an electro-optic effect.

  Conventionally, optical components such as optical lenses and prisms are optical devices such as cameras, microscopes, and telescopes, electrophotographic recording devices such as printers and copiers, optical recording devices such as DVDs, optical devices for communication, industrial use, etc. It is used for. A normal optical lens has a fixed focal length. However, a lens that can adjust the focal length according to the situation, a so-called variable focus lens may be used in the above-described devices and apparatuses. The conventional variable focus lens mechanically adjusts the focal length by combining a plurality of lenses. However, such a mechanical variable focus lens has a limit in extending the application range from the viewpoint of response speed, manufacturing cost, miniaturization, power consumption, and the like.

  Therefore, a variable focus lens in which a material capable of changing the refractive index is applied to the transparent medium constituting the optical lens, a variable focus lens that mechanically deforms the shape of the optical lens, instead of moving the position of the optical lens, etc. It was issued. As the former variable focus lens, a variable focus lens using liquid crystal as an optical lens has been proposed. This variable focus lens encloses the liquid crystal in a container made of a transparent material by sandwiching the liquid crystal between two glass plates. When the inside of the container is processed into a spherical surface and the liquid crystal is molded into a lens shape, a variable focus lens can be configured. A transparent electrode is provided inside the container, and the refractive index is controlled by applying an electric field to the liquid crystal, and the focal length is variably controlled (for example, see Non-Patent Document 1).

  As the latter variable focus lens, liquid is often used as the material of the deformable lens. For example, the variable focus lens described in Non-Patent Document 1 has a structure in which a liquid such as silicon oil is sealed in a space sandwiched between glass plates. The glass plate is thinly processed. By applying pressure to the glass plate with a lead zirconate titanate (PZT) piezo actuator from the outside, the lens composed of the oil and the entire glass plate is deformed, and the focal position is Control.

Bin Wang, Mao Ye, and Susumu Sato, “Lens of electrically controllable focal length made by a glass lens and liquid-crystal layers”, Applied Optics 43, 3420 (2004) Takashi Kaneko et al., "Long focal depth visual mechanism using variable focus lens", Denso Technical Review, Vol.3, No.1, p.52-58, 1998

  However, the conventional variable focus lens includes any one of a variable focus lens that mechanically adjusts the focal length, a variable focus lens that controls the refractive index by applying an electric field to liquid crystal, and a variable focus lens that deforms the lens by a PZT piezo actuator. However, the response speed required to change the focal length is limited, and there is a problem that it cannot be applied to a high-speed response of 1 ms or less.

  An object of the present invention is to provide a variable focus lens that can change the focal length at high speed without depending on the polarization of incident light.

  In order to achieve the above object, according to an embodiment of the present invention, an embodiment of the present invention includes an electro-optic material made of a single crystal having inversion symmetry, a first surface of the electro-optic material, and the first surface. A plurality of electrode pairs formed at positions facing the second surface opposite to the second surface, and changing a voltage applied between the electrode pairs, thereby focusing the light transmitted through the electro-optic material. A variable cylindrical variable focus lens is used as a basic unit element, and a polarization beam splitter, a Faraday rotation element, the basic unit element, and a reflecting mirror are sequentially arranged sharing an optical axis, and are given to the polarization beam splitter. Light having a polarization direction passes through the basic unit element after passing through the Faraday rotator, is reflected by the reflecting mirror, passes through the basic unit again, and passes through the Faraday rotator. Characterized in that it is emitted from the polarization beam splitter and.

  As described above, according to the present invention, an electro-optic material composed of a single crystal having inversion symmetry and a plurality of electrode pairs formed on the surface of the electro-optic material, the applied voltage between the electrode pairs is set. Since the focal point of the emitted light is controlled by changing the focal length, the focal length can be changed at high speed.

  In addition, since the light is transmitted twice through the basic unit element made of an electro-optic material, the lens effect is doubled, and light in a given polarization direction is incident on the polarization beam splitter, thereby minimizing the reduction in optical power. To the limit.

It is a figure which shows the structure of the basic unit element of the variable focus lens concerning one Embodiment of this invention. It is a figure for demonstrating the principle of the basic unit element of a variable focus lens. It is a figure which shows the structure of the variable focus lens which can condense biaxially using two basic unit elements. It is a figure which shows the structure of the variable focus lens concerning the 1st Embodiment of this invention. It is a figure which shows the structure of the variable focus lens concerning the 2nd Embodiment of this invention. It is a figure which shows the structure of the variable focus lens concerning the 3rd Embodiment of this invention. It is a figure which shows the structure of the variable focus lens concerning the 3rd Embodiment of this invention. It is a figure which shows the structure of the variable focus lens concerning the 4th Embodiment of this invention. It is a figure which shows the structure of the variable focus lens concerning the 4th Embodiment of this invention. It is a figure which shows the structure of the variable focus lens concerning the 4th Embodiment of this invention. It is a figure which shows the structure of the basic unit element of the variable focus lens concerning the 5th Embodiment of this invention.

  Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings. The variable focus lens of this embodiment is composed of an electro-optic material and an electrode attached thereto. By utilizing the electro-optic effect, a much faster response speed can be obtained as compared with a conventional variable focus lens. First, a basic variable focus lens will be described.

(Configuration of cylindrical variable focus lens)
FIG. 1 shows a configuration of a basic unit element of a variable focus lens according to an embodiment of the present invention. Two electrode pairs are formed on the upper surface (first surface) and the lower surface (second surface) of the substrate 1 obtained by processing the electro-optic material into a plate shape at positions facing each other. An anode 2 (first anode) is disposed as an upper electrode on the light incident side, and a cathode 3 (first cathode) is disposed as a lower electrode across the substrate 1. Further, another pair of electrodes is disposed on the light emission side, with a distance from these electrode pairs, the upper electrode being the cathode 4 (second cathode), and the lower electrode being the anode 5 (second anode). It is. The four strip-shaped electrodes have a shape in which all the sides in the longitudinal direction are parallel.

  Incident light 6 is incident from a surface (third surface) orthogonal to the surface on which the electrodes are arranged, travels in the x-axis direction inside the substrate 1, and between these anodes 2 and 3, It penetrates in a direction perpendicular to the longitudinal direction. Next, after passing between the cathode 4 and the anode 5, the outgoing light 7 is emitted from the surface (fourth surface) opposite to the incident surface into the air.

  In such a configuration, a voltage is applied between the anode and the cathode. The direction of applying a voltage (z-axis direction) is opposite between the light incident side electrode pair and the light emission side electrode pair. The potentials of the anode 2 and the anode 5 may be different, and the potentials of the cathode 3 and the cathode 4 are the same. The lower potential of the anodes 2 and 5 is set to be higher than the higher potential of the cathodes 3 and 4.

  At this time, an electric field distribution is generated between these electrodes, and the refractive index is modulated by the electro-optic effect of the substrate 1. When light is transmitted through the refractive index modulated portion, the light is bent by this refractive index distribution, and as a result, the light is condensed or diverged. When condensed, according to the structure of FIG. 1, it functions as a cylindrical convex lens, and when diverged, it functions as a cylindrical concave lens. In this way, the light is condensed or diverged in the uniaxial direction, and thus is called uniaxial modulation. Further, since the degree of bending of light changes depending on the applied voltage, the focal length can be controlled by the voltage.

  The electro-optic effect responds in a time of 1 μs or less even if it is late estimated from the application of the voltage. Therefore, it is possible to realize a variable focus lens that responds significantly faster than the conventional variable focus lens. As described above, the element shown in FIG. 1 is a cylindrical variable focus lens and is a basic unit constituting various lenses. In order to realize a normal spherical lens, two cylindrical variable focus lenses and a half-wave plate inserted between them are combined as basic unit elements, and the two basic unit elements are 90.degree. Arrange them at an angle of degrees. In this way, the light is condensed or diverged in the biaxial direction, which is called biaxial modulation. In the present embodiment, the material of the substrate 1 is characterized by using a material made of a crystal having inversion symmetry, among materials having an electro-optic effect, and the reason will be described later.

  Hereinafter, the state of refractive index modulation and the function as a lens will be described in detail with reference to FIG. FIG. 2 shows a side view of the variable focus lens shown in FIG. 1 as viewed from the y-axis direction. The substrate 1 has a uniform refractive index when no voltage is applied to the four electrodes, so that light passes through without being modulated. Therefore, there is no lens function. However, when a plane wave is incident, the wavefront of the light emitted from the substrate 1 remains a plane, and it can be regarded as a lens with an infinite focal length considering that the radius of curvature is infinite.

  When voltages are applied to the four electrodes, electric lines of force 11 as shown in FIG. 2 are generated between these electrodes. The lines of electric force 11 are generated not only between the anode 2 and the cathode 3 and between the cathode 4 and the anode 5 but also widely spread outside these electrodes. The generation of electric lines of force means that an electric field is generated. At this time, since the substrate 1 has an electro-optic effect, the refractive index is modulated at a portion where an electric field is generated inside the substrate 1. Inside the substrate 1, in the vicinity of the four electrodes, that is, in the vicinity of the surface of the substrate 1, the electric field is large and the refractive index change is large. On the other hand, in the central part of the substrate 1 (near the center in all axial directions), the electric field is relatively small and the refractive index change is small.

  The right side of FIG. 2 schematically shows a refractive index modulation curve 12 representing a distribution of refractive index change. The vertical axis of the refractive index modulation curve 12 is the z-axis coordinate, and the horizontal axis is the refractive index change Δn from when no voltage is applied. FIG. 2 shows that the refractive index changes in the negative direction as a whole, but the modulation is large near the surface of the substrate 1, and therefore the refractive index change Δn is large in the negative direction. Become. On the other hand, the modulation is small in the vicinity of the central portion, and therefore the refractive index change Δn is not as large in the negative direction as in the vicinity of the surface. When light passes through such a refractive index distribution, it functions as a convex lens because the speed of light near the surface is higher than the speed of light at the center of the substrate 1. That is, the focal point moves from an infinite focal length when no voltage is applied to a finite focal length. The focal length varies depending on the applied voltage. When an electro-optic material having inversion symmetry described later is used as the substrate, the focal length is inversely proportional to the square of the applied voltage.

  FIG. 2 shows a state in which the side surface of the substrate 1 is viewed from the y-axis direction, and the electric lines of force are drawn in a plane parallel to the xz plane. For this reason, the electric field component in the y-axis direction does not appear in this figure, but is actually very small to a negligible level. This is because the crystal material having the electro-optic effect constituting the substrate 1 has a very high dielectric constant, and the reason will be described in detail below.

  Electromagnetism explains that the lines of electric force are refracted at the interface between the dielectric and air. A crystal having reversal symmetry, which will be described later, generally has a huge relative dielectric constant exceeding 10,000. At such an interface between the dielectric and air, the electric lines of force are very refracted, and the electric lines of force inside the dielectric are almost parallel to the surface regardless of the direction of the electric lines of force on the air side. Become. Therefore, among the six surfaces of the substrate 1, the electric lines of force are substantially on the surface even in the plane parallel to the xz plane, that is, in the vicinity of the front side surface 8 a and the opposite side surface 8 b in the substrate 1 of FIG. 1. Parallel. Therefore, the electric field component in the y-axis direction is very small from the side surface 8a to the side surface 8b, and the magnitude thereof is as small as the magnitude of the electric field component in the x-axis direction and the z-axis direction divided by the relative dielectric constant.

  Here, it is assumed that another variable focus lens having the same structure as that of the variable focus lens of FIG. 1 (hereinafter referred to as lens 1) is placed in front of the side surface 8a and in close contact with the side surface 8a. If the surface on which the electrodes are installed, the light incident surface and the light exit surface are aligned and regarded as one lens (hereinafter referred to as lens 2), it can be considered that the width of the variable focus lens is doubled when viewed from the light incident surface. The lens placed in front is a mirror image of the side surface 8a with respect to the original lens.

  The internal lines of electric force of the lens 2 and the lens 1 are compared. Although it can be considered that the side surface 8a of the lens 1 is located at the center of the lens 2 along the optical axis, the lens 2 is symmetric with respect to the side surface 8a, and therefore there is no y-axis direction component of the electric field in the vicinity of the side surface 8a. . On the other hand, if there is a y-axis direction component of the electric field in the vicinity of the side surface 8a in the lens 1, the electric field distribution of the lens 1 is not equal to the electric field distribution of the lens 2. However, as described above, the lens 1 can also ignore the y-axis direction component of the electric field. From this, it can be said that the electric field distributions of the lens 1 and the lens 2 are not contradictory, in other words, the same.

  When this concept is repeated and the number of variable focus lenses in FIG. 1 is increased to three and four, an infinitely wide lens (hereinafter referred to as lens 3) can be formed. This lens 3 should also have the same electric field distribution as the lens 1 and the lens 2. The lens 3 has translational symmetry that it overlaps the original lens 3 even if it moves a certain distance in the y-axis direction. For this reason, the electric field distribution is the same regardless of the y coordinate, and at the same time, no y-axis component of the electric field exists anywhere inside the lens 3. In other words, the lens effect remains the same regardless of the position on the y-axis where light enters. This is the same for the lens 1, and the lens effect is the same regardless of the y coordinate. This means that the variable focus lens of FIG. 1 realizes an ideal cylindrical lens that is uniform in the y-axis direction.

  Note that the variable focus lens of FIG. 1 has different lens effects depending on the polarization because of the anisotropy of the electro-optic effect. There are linearly polarized light with an electric field parallel to the y axis and linearly polarized light with an electric field parallel to the z axis, but it works as a good convex lens for polarized light parallel to the z axis, but for polarized light parallel to the y axis. It is known that the lens effect is small.

(Configuration of variable-focus lens for biaxial focusing)
FIG. 3 shows a configuration of a variable focus lens that can focus on two axes using two basic unit elements. The basic unit element shown in FIG. 1 is a variable focus lens that generates an ideal refractive index profile as a cylindrical lens. Since it is a cylindrical lens, unlike a more general spherical lens, condensing is only in the direction of one axis. The variable focus lens (lens 1) of FIG. 1 is a basic unit element, and a basic unit element 21, a half-wave plate 22, and another basic unit element 23 are arranged in series with the optical axis (x-axis) aligned. To do. The basic unit element 21 and the basic unit element 23 are arranged so that the surfaces on which the electrodes are installed form 90 °.

  With such a configuration, it is possible to collect light in two axes similar to a general spherical lens. At this time, the basic unit element has anisotropy as described above, and the lens effect changes depending on the direction of linearly polarized light with respect to the basic unit element. Since the basic unit element 21 and the basic unit element 23 are different in 90 ° direction, a wavelength plate or the like is placed between the two basic unit elements to rotate the polarized light by 90 ° in order to exhibit the same lens effect.

(Arrangement of Faraday rotator and polarizing beam splitter)
The principle of the basic unit element of the variable focus lens has been described above. However, there is a limit to the magnitude of the refractive index change of the electro-optic effect, and thus there is a limit to the magnitude of the lens effect that can be controlled by voltage. Therefore, in order to increase the lens effect, the basic unit element shown in FIG. 1 is configured by adding a Faraday rotation element and a polarization beam splitter as components.

  FIG. 4 shows the configuration of the variable focus lens according to the first embodiment of the present invention. In the variable focus lens, a polarization beam splitter 31, a Faraday rotation element 32, a basic unit element 33, and a mirror (reflecting mirror) 34 are arranged in order in common with an optical axis.

  As shown in FIG. 4A, when polarized incident light whose electric field oscillates in the vertical direction in the figure enters the polarizing beam splitter 31, it passes through the polarizing beam splitter 31 as it is. The transmitted light enters the Faraday rotation element 32, and the polarization direction of the transmitted light is rotated by 45 °. Light having a polarization direction of 45 ° is incident on the basic unit element 33, and a desired lens effect is given. The light subjected to the lens effect is reflected by the mirror 34.

  As shown in FIG. 4B, the reflected light is transmitted again through the basic unit element 33, and the lens effect is given again. The light that has undergone the lens effect again enters the Faraday rotator 32 again, and the polarization direction is again rotated by 45 °. As a result, the oscillating electric field of the transmitted light is in a direction perpendicular to the paper surface. When the light having a polarization direction of 90 ° is incident on the polarization beam splitter 31, it is reflected inside and emitted as outgoing light from a direction different from the incident light.

  For ease of illustration, the display of the coordinate axes is omitted in FIGS. 4A and 4B, and the angles at which the respective components are installed around the optical axis are not shown. Light having a polarization direction rotated by 45 ° with respect to incident light is incident on the basic unit element 33. As described above, the lens effect of the basic unit element 33 is parallel to the z axis shown in FIG. Since it is the maximum with respect to the polarized light, the basic unit element 33 is arranged so that the direction in which the polarization direction is rotated by 45 ° is parallel to the z axis. In other words, the z-axis of the basic unit element 33 is inclined by 45 ° with respect to the polarization direction of the incident light, or the polarization direction of incident light is inclined by 45 ° with respect to the z-axis of the basic unit element 33.

  In the variable focus lens having this configuration, the light is transmitted twice through the basic unit element 33, so that the lens effect is doubled. The reciprocal of the focal length is called “lens power”, and the larger the value, the stronger the lens effect. The variable focus lens of the first embodiment has twice the lens power as compared with the basic unit element of the variable focus lens shown in FIG. Further, by the polarization operation by the Faraday rotation element 32, the direction of polarization in the basic unit element 33 is constant, the same lens effect can be exhibited, and the decrease in optical power can be minimized.

  The variable focus lens described above is a cylindrical lens. However, as shown in FIG. 3, by combining two basic unit elements, a lens capable of biaxial focusing similar to a spherical lens can be manufactured. A biaxial condensing lens in which the lens power is doubled by inserting the variable focus lens shown in FIG. 3 between the Faraday rotation element 32 and the mirror 34 instead of the basic unit element 33 in FIG. Can be realized.

(Increase the number of transmission repetitions)
As described above, by utilizing the Faraday rotator element, the light return path and the outbound path can be separated even if light is transmitted back and forth through the basic unit element of the variable focus lens. Further, the direction of polarization in the basic unit element is constant, and the reduction in optical power can be minimized. Further, the number of transmissions of the basic unit element can be increased, and the lens power can be dramatically increased. Hereinafter, the principle will be described.

  FIG. 5 shows a configuration of a variable focus lens according to the second embodiment of the present invention. A structure in which light is transmitted four times through the basic unit element 43 by adding one polarization beam splitter 46, one Faraday rotation element 47, and one half-wave plate 48 to the variable focus lens of the first embodiment. It has become. As shown in FIG. 5A, when polarized incident light whose electric field oscillates in the vertical direction in the figure enters the polarizing beam splitter 41, it passes through the polarizing beam splitter 41 as it is. The transmitted light enters the Faraday rotation element 42, and the polarization direction of the transmitted light is rotated by 45 °. Light having a polarization direction of 45 ° is incident on the basic unit element 43 via the mirrors 45a and 45b, and a desired lens effect is given. The light subjected to the lens effect is reflected by the mirror 44b.

  As shown in FIG. 5B, the reflected light passes through the basic unit element 43 again, and a second lens effect is given. The light that has received the lens effect is incident again on the Faraday rotation element 42 via the mirrors 45b and 45a, and the polarization direction is again rotated by 45 °. As a result, the oscillating electric field of the transmitted light is in a direction perpendicular to the paper surface. When light having a polarization direction of 90 ° is incident on the polarization beam splitter 41, the light is reflected inside and emitted to the polarization beam splitter 46.

  Since the oscillating electric field of light is perpendicular to the paper surface, it is reflected inside the polarizing beam splitter 46, passes through the half-wave plate 48, and the polarized light rotates 90 degrees. Further, the polarization direction of the light incident on and transmitted through the Faraday rotation element 47 is rotated by 45 °. Light having a polarization direction of 45 ° is incident on the basic unit element 43 via the mirrors 45d and 45c, and is given a third lens effect. The light subjected to the lens effect is reflected by the mirror 44a.

  As shown in FIG. 5C, the reflected light passes through the basic unit element 43 again, and is given a fourth lens effect. The light that has received the lens effect is incident again on the Faraday rotation element 47 via the mirrors 45b and 45a, and the polarization direction is again rotated by 45 °. As a result, the oscillating electric field of the transmitted light is in a direction perpendicular to the paper surface. When the light passes through the half-wave plate 48 again and the polarized light rotates 90 degrees and enters the polarization beam splitter 46, the light passes through the inside and is emitted as outgoing light.

  The mirrors 45a-45b are used to incline the first round trip path and the second round trip path by a slight angle to form different optical paths. In the second embodiment, since light passes through the basic unit element four times, the lens power can be increased almost four times as compared with the basic unit element of the variable focus lens shown in FIG. it can.

6 and 7 show a configuration of a variable focus lens according to the third embodiment of the present invention. The structure which increased the frequency | count of permeation | transmission of a basic unit element to 6 times is shown. The order of light transmission is summarized.
6A: Polarizing beam splitter 51-Faraday rotator 52-half wave plate 56- [basic unit element 53] -mirror 54a
6B: mirror 54a- [basic unit element 53] -half wavelength plate 56-Faraday rotation element 52-polarization beam splitter 51-polarization beam splitter 57-Faraday rotation element 58-half wavelength plate 59-mirror 55d, 55c- [basic unit element 53] -mirror 54b
7 (a): mirror 54b- [basic unit element 53] -mirrors 55c, 55d-half wavelength plate 59-Faraday rotation element 58-polarization beam splitter 57-mirrors 60a, 60b-polarization beam splitter 61-Faraday rotation element 62-half wave plate 63-mirrors 55a, 55b- [basic unit element 53] -mirror 54c
7B: mirror 54c- [basic unit element 53] -mirrors 55b and 55a-half-wave plate 63-Faraday rotation element 62-polarizing beam splitter 61.

8 to 10 show the configuration of a variable focus lens according to the fourth embodiment of the present invention. The structure which increased the frequency | count of permeation | transmission of a basic unit element to 10 times is shown. The order of light transmission is summarized.
FIG. 8A: Polarizing beam splitter 71-Faraday rotation element 72-half wave plate 76- [basic unit element 73] -mirror 74a
8B: mirror 74a- [basic unit element 73] -half wavelength plate 76-Faraday rotation element 72-polarization beam splitter 71-polarization beam splitter 77-Faraday rotation element 78-half wavelength plate 79-mirror 75d, 75c- [basic unit element 73] -mirror 74b
9 (a): mirror 74b- [basic unit element 73] -mirrors 75c, 75d-half wave plate 79-Faraday rotation element 78-polarization beam splitter 77-mirrors 80a, 80b-polarization beam splitter 81-Faraday rotation element 82-half wave plate 83-mirrors 75a, 75b- [basic unit element 73] -mirror 74c
9B: mirror 74c- [basic unit element 73] -mirrors 75b and 75a-half wave plate 83-Faraday rotation element 82-polarization beam splitter 81-polarization beam splitter 84-Faraday rotation element 85-half wavelength plate 86-mirror 87a, 87b- [basic unit element 73] -mirror 74d
FIG. 10A: mirror 74d- [basic unit element 73] -mirrors 87b, 87a-half-wave plate 86-Faraday rotation element 85-polarization beam splitter 84-mirrors 88a, 88b-polarization beam splitter 89-Faraday rotation element 90-half wave plate 91-mirrors 87d, 87c- [basic unit element 73] -mirror 74e
-Fig. 10 (b): mirror 74e-[basic unit element 73]-mirrors 87c and 87d-half-wave plate 91-Faraday rotator 90-polarizing beam splitter 89.

  To summarize the first to fourth embodiments, a plurality of optical systems including a polarizing beam splitter, a Faraday rotator, and a half-wave plate if necessary are prepared, and the optical path of each optical system passes through the basic unit element. In this manner, the reflecting mirror is arranged. It is configured such that light of a given polarization direction incident from one polarization beam splitter of a plurality of optical systems passes through the basic unit element a plurality of times and is emitted from one polarization beam splitter of the plurality of optical systems. .

  In the description of the first to fourth embodiments, since the basic unit element of the variable focus lens is used, these embodiments are cylindrical lenses. If the basic unit elements 33, 43, 53, 73 are replaced with the biaxial condensing variable focus lens shown in FIG. 3, the lens power can be increased in the biaxial condensing lens function.

(Electro-optic material)
The electro-optic effect includes several different-order electro-optic effects, but generally, a first-order electro-optic effect (hereinafter referred to as Pockels effect) is used. In the Pockels effect, the refractive index change is proportional to the electric field. In the configuration shown in FIGS. 1 and 2, the direction of the electric field is reversed and the refractive index distribution is also reversed between the anode 2 and the cathode 3 and between the cathode 4 and the anode 5. Therefore, when the Pockels effect is used, when light passes between these two electrode pairs, the deflection of the light due to the refractive index distribution is canceled out between positive and negative, and the function as a lens is not achieved.

  On the other hand, when the secondary electro-optic effect (hereinafter referred to as the Kerr effect) is used, the refractive index change is proportional to the square of the electric field. Therefore, even if the direction of the electric field is reversed between the anode 2 and the cathode 3 and between the cathode 4 and the anode 5, the refractive index distribution is the same, so that the light deflection is canceled out. We will strengthen each other.

  Many electro-optic materials do not have inversion symmetry and develop a Pockels effect. On the other hand, some electro-optic materials have inversion symmetry, do not exhibit the Pockels effect, and the Kerr effect is dominant. Therefore, it is important to use a material having inversion symmetry as the electro-optic material constituting the substrate 1 of the present embodiment.

  In general, when an electric field is applied from the outside to a dielectric, polarization proportional to the electric field is generated, but when the electric field is removed, the polarization returns to zero. However, there are substances that retain finite polarization even when the electric field is removed. Polarization that exists even without an external electric field is called spontaneous polarization. There exists a substance capable of reversing the direction of this spontaneous polarization by an external electric field, which is called a ferroelectric.

  A single crystal having inversion symmetry refers to a crystal that has the same arrangement as the original arrangement of atoms when the arrangement of atoms is inverted in the x, y, z coordinate system around a certain origin. When a crystal having spontaneous polarization is inverted on the coordinate axis, the direction of spontaneous polarization is inverted, so that such a crystal cannot be said to have inversion symmetry. Therefore, since the ferroelectric has spontaneous polarization, it does not have inversion symmetry.

  On the other hand, there are substances that have spontaneous polarization but cannot be inverted by an external electric field. Such a material does not have inversion symmetry, but is not a ferroelectric material. Therefore, not all materials that do not have inversion symmetry are ferroelectric materials. Further, it cannot be a ferroelectric and has inversion symmetry.

As an electro-optic material having inversion symmetry, there is a single crystal material having a perovskite crystal structure. The perovskite single crystal material becomes a cubic phase having inversion symmetry in the use state if the use temperature is appropriately selected. In the cubic phase, the Pockels effect is not expressed and the Kerr effect is dominant. For example, even the most well-known barium titanate (BaTiO ₃ , hereinafter referred to as BT) may exceed the temperature at which the phase transition from the tetragonal phase to the cubic phase (hereinafter referred to as the phase transition temperature) occurs at around 120 ° C. For example, it becomes a cubic phase and exhibits the Kerr effect.

A single crystal material mainly composed of potassium tantalate niobate (KTN: KTa _1-x Nb _x O ₃ , 0 ≦ x ≦ 1) has more preferable characteristics. BT has a predetermined phase transition temperature, whereas KTN can select a phase transition temperature depending on the composition ratio of tantalum and niobium. Thereby, the phase transition temperature can be set near room temperature. KTN has a cubic phase at a temperature higher than the phase transition temperature, has inversion symmetry, and has a large Kerr effect. Even in the same cubic phase, the Kerr effect becomes overwhelmingly closer to the phase transition temperature. For this reason, setting the phase transition temperature around room temperature is very important for easily realizing a large Kerr effect.

Further, as a single crystal material related to KTN, the main component of the crystal is composed of periodic group Ia group and Va group, group Ia is potassium, and group Va includes at least one of niobium and tantalum. Materials can be used. Moreover, 1 or multiple types of periodic table group Ia except potassium as an additional impurity, for example, lithium, or IIa group can also be included. For example, a cubic phase KLTN (K _1-y Li _y Ta _1-x Nb _x O ₃ , 0 ≦ x ≦ 1, 0 <y <1) crystal may be used.

(Place electrode)
In the variable focus lens shown in FIG. 1, an anode 2 and a cathode 4 are arranged on the upper surface of the substrate 1 as a basic unit element, and a cathode 3 and an anode 5 are arranged on the lower surface. However, the basic unit element may have a configuration in which both the electrodes on the upper surface are anodes and the electrodes on the lower surface are both cathodes. The lens effect is small compared to the variable focus lens shown in FIG. 1, but the function is the same.

(Electrode material)
When a high voltage is applied to the electro-optic material, charges are injected from the electrodes, and space charges can be generated in the crystal. This space charge causes a gradient in the magnitude of the electric field in the direction in which the voltage is applied. Therefore, in order to obtain a desired refractive index distribution for causing the electro-optic material to function as a lens, or to prevent light transmitted through the electro-optic material from being deflected, when a voltage is applied to the substrate 1, It is better that no space charge is formed inside the substrate 1.

  Since the amount of space charge depends on the carrier injection efficiency, the carrier injection efficiency injected from the electrode should be small. Therefore, the electrode is preferably a material that forms a Schottky junction with the electro-optic material. Specifically, when the carrier contributing to electrical conduction in the electro-optic crystal is an electron, the work function of the electrode material is preferably 5.0 eV or more. For example, a metal such as Au (5.1), Ir (5.27), or Pt (5.65) can be used as an electrode material having a work function of 5.0 eV or more. The parentheses indicate work functions, and the unit is eV.

  When a high voltage is applied to the electro-optic material, charges are injected from the electrodes, and space charges are generated in the crystal. This space charge disturbs the refractive index distribution and adversely affects the lens function. By generating a Schottky barrier between the electrode and the substrate, charge injection can be suppressed. For this purpose, the work function of the electrode material is preferably 5.0 eV or more, and noble metals such as Au, Ir, and Pt are suitable.

(Other configuration of cylindrical variable focus lens)
FIG. 11 shows a configuration of a basic unit element of a variable focus lens according to the fifth embodiment of the present invention. The arrangement of the electrodes 102-105 with respect to the substrate 101 is the same as that of the basic unit element of FIG. 1 is different from the basic unit element in FIG. 1 in the incident direction of incident light 106 and the outgoing direction of outgoing light 107. As shown in FIG. 8, incident light 106 is incident from between the anode 102 and the cathode 104 on the upper surface of the substrate 101, travels in the z-axis direction inside the substrate 101, and The light is emitted as emitted light 107 from between the air. Also, in the basic unit elements of the first to fourth embodiments, both of the upper surface electrodes may be anodes and the lower surface electrodes may be both cathodes. Conversely, the upper surface is a cathode and the lower surface is an anode. But it ’s okay.

  As shown in FIG. 1, an anode 2, a cathode 3, a cathode 4, and an anode 5 are formed on the upper and lower surfaces of a substrate 1 obtained by processing an electro-optic material into a plate shape. The substrate 1 is cut out from a KTN single crystal and formed into a shape of 7 mm × 7 mm × (thickness T =) 4 mm. All six surfaces of the substrate 1 are parallel to the (100) plane of the crystal and optical polishing is performed. Since this KTN single crystal had a phase transition temperature of 35 ° C., it is used at 40 ° C., which is slightly higher than this. The relative dielectric constant at this temperature is 20,000. The four electrodes have a strip shape of 0.8 mm × 7 mm, and the distance between the electrodes on the same plane is 4 mm. The two electrode pairs are formed by depositing platinum (Pt) on the 7 mm × 7 mm surface of the substrate 1. Each side of the electrode is parallel to the side of the substrate 1.

Collimated laser light is incident on the cylindrical variable focus lens while the temperature is controlled at 40 ° C. The polarization of light is a straight line, and the direction of the oscillating electric field is the z-axis direction. When a voltage of 1000 V is applied between the upper and lower electrodes, the light emitted from the substrate 1 is condensed in the z-axis direction and functions as a cylindrical convex lens. The focal length is 59 cm. The lens power is 1.7 m ^-1 which is the reciprocal of this lens power.

Using this cylindrical variable focus lens as a basic unit element, a polarization beam splitter and a Faraday rotation element are combined to produce the variable focus lens of the first embodiment shown in FIG. The direction of the oscillating electric field with respect to the basic unit element is as described above. When a voltage of 1000 V is applied between the upper and lower electrodes, the light emitted from the polarizing beam splitter is condensed in a direction that forms 45 ° with the paper surface of FIG. 4 and functions as a cylindrical convex lens. The lens power is 3.4 m ⁻¹ , twice that of the basic unit element alone. The focal length is 29.5 cm, which is half of the basic unit element alone.

In the basic unit element produced in Example 1, both the upper electrode is used as an anode and the lower electrode is used as both a cathode. Collimated laser light is incident on the cylindrical variable focus lens while the temperature is controlled at 40 ° C. The polarization of light is a straight line, and the direction of the oscillating electric field is the z-axis direction. When a voltage of 1000 V is applied between the upper and lower electrodes, the light emitted from the substrate 1 is condensed in the z-axis direction and functions as a cylindrical convex lens. The focal length is 115 cm. The lens power is 0.87 m ^-1 which is the reciprocal of this lens power.

Using this cylindrical variable focus lens as a basic unit element, a polarization beam splitter and a Faraday rotation element are combined to produce the variable focus lens of the first embodiment shown in FIG. The direction of the oscillating electric field with respect to the basic unit element is as described above. When a voltage of 1000 V is applied between the upper and lower electrodes, the light emitted from the polarization beam splitter is condensed in a direction that forms 45 ° with the paper surface of FIG. 4 and functions as a cylindrical convex lens. The lens power is 1.74 m ⁻¹ , twice that of the basic unit element alone. The focal length is 58 cm, which is half of the basic unit element alone.

The basic unit element produced in Example 1 is used as the basic unit element of the cylindrical variable focus lens of the fifth embodiment shown in FIG. Collimated laser light is incident on the cylindrical variable focus lens while the temperature is controlled at 40 ° C. The polarization of light is a straight line, and the direction of the oscillating electric field is the x-axis direction. When a voltage of 1000 V is applied between the upper and lower electrodes, the light emitted from the substrate 41 is condensed in the x-axis direction and functions as a cylindrical convex lens. The focal length is 104 cm. The lens power is 0.96 m ^-1 which is the reciprocal of this lens power.

Using this cylindrical variable focus lens as a basic unit element, a polarization beam splitter and a Faraday rotation element are combined to produce the variable focus lens of the first embodiment shown in FIG. The direction of the oscillating electric field with respect to the basic unit element is as described above. When a voltage of 1000 V is applied between the upper and lower electrodes, the light emitted from the polarization beam splitter is condensed in a direction that forms 45 ° with the paper surface of FIG. 4 and functions as a cylindrical convex lens. The lens power is 1.92 m ⁻¹ , twice that of the basic unit element alone. The focal length is 52 cm, which is half of the basic unit element alone.

In the basic unit element produced in Example 3, both the upper surface electrodes are used as anodes and the lower surface electrodes are both used as cathodes. Under the same conditions as in Example 3, the focal length was 114 cm. The lens power is 0.88 m ^-1 which is the reciprocal of this lens power.

Using this cylindrical variable focus lens as a basic unit element, a polarization beam splitter and a Faraday rotation element are combined to produce the variable focus lens of the first embodiment shown in FIG. The direction of the oscillating electric field with respect to the basic unit element is as described above. When a voltage of 1000 V is applied between the upper and lower electrodes, the light emitted from the polarization beam splitter is condensed in a direction that forms 45 ° with the paper surface of FIG. 4 and functions as a cylindrical convex lens. The lens power is 1.75 m ⁻¹ , twice that of the basic unit element alone. The focal length is 57 cm, which is half of the basic unit element alone.

The cylindrical variable focus lens used in Example 1 is used as a basic unit element, and two polarization beam splitters, two Faraday rotation elements, and one half-wave plate are combined, and the variable focus of the second embodiment shown in FIG. Make a lens. The direction of the oscillating electric field with respect to the basic unit element is as described above. When a voltage of 1000 V is applied between the upper and lower electrodes, the light emitted from the polarization beam splitter is condensed and functions as a cylindrical convex lens. The lens power is 6.8 m ⁻¹ , four times that of the basic unit element alone. The focal length is 15 cm, which is a quarter of the basic unit element alone.

DESCRIPTION OF SYMBOLS 1,101 Board | substrate 2,5,102,105 Anode 3,4,103,104 Cathode 6,106 Incident light 7,107 Output light 11 Electric field line 12 Refractive index modulation curve 21,23,33,43,53,73 Basic unit elements 22, 48, 56, 59, 63, 76, 79, 83, 86, 91 Half-wave plates 31, 41, 46, 51, 57, 61, 71, 77, 81, 84, 89 Polarizing beam splitter 32 , 42, 47, 52, 58, 62, 72, 78, 82, 85, 90 Faraday rotator 34, 44, 45, 54, 55, 60, 74, 75, 80, 87, 88 Mirror

Claims (11)

An electro-optic material made of a single crystal having inversion symmetry;
A plurality of electrode pairs formed at positions facing the first surface of the electro-optic material and the second surface facing the first surface,
A cylindrical variable focus lens that changes the focus of light transmitted through the electro-optic material by changing an applied voltage between the electrode pair is a basic unit element.
A polarizing beam splitter, a Faraday rotator, the basic unit element and a reflecting mirror are sequentially arranged sharing an optical axis,
Light of a given polarization direction incident on the polarization beam splitter is transmitted through the Faraday rotator, then transmitted through the basic unit element, reflected by the reflecting mirror, and again transmitted through the basic unit element. A varifocal lens which is transmitted through the Faraday rotation element and emitted from the polarization beam splitter. An electro-optic material made of a single crystal having inversion symmetry;
A plurality of electrode pairs formed at positions facing the first surface of the electro-optic material and the second surface facing the first surface,
A cylindrical variable focus lens that changes the focus of light transmitted through the electro-optic material by changing an applied voltage between the electrode pair is a basic unit element.
A plurality of optical systems in which a polarizing beam splitter and a Faraday rotator are arranged sharing the optical axis,
Reflecting mirrors are arranged so that the optical axis of each optical system passes through the basic unit element, and light of a given polarization direction incident from one polarization beam splitter of the plurality of optical systems is A varifocal lens, which passes through the basic unit element a plurality of times and is emitted from one polarization beam splitter of the plurality of optical systems. The basic unit element is:
A first anode formed on the first surface of the electro-optic material and a second surface formed on a second surface opposite to the first surface and facing the first anode. A first electrode pair composed of one cathode, a second cathode formed on the first surface and spaced from the first anode, and on the second surface A second electrode pair formed with a second anode formed at a position facing the second cathode and spaced apart from the first cathode;
When light is incident from a third surface orthogonal to the first surface, the light passes through the first electrode pair and then passes through the second electrode pair, so that the third Light is emitted from the fourth surface opposite to the surface of
3. The focus of light emitted from the fourth surface of the electro-optic material is varied by changing an applied voltage between the first and second electrode pairs. The variable focus lens described. The basic unit element is:
A first anode formed on a first surface of the electro-optic material;
A first cathode formed on a second surface opposite to the first surface and formed at a position facing the first anode;
A second cathode formed on the first surface and spaced from the first anode;
A second anode formed on the second surface, facing the second cathode, and spaced apart from the first cathode;
When light is incident on the first surface between the first anode and the second cathode and passes through the electro-optic material, the first cathode and the second anode Light is emitted from the second surface between
3. The focus of light emitted from the second surface of the electro-optic material is varied by changing an applied voltage between the two anodes and the two cathodes. The variable focus lens described in 1. The basic unit element is:
A first anode formed on the first surface of the electro-optic material and a second surface formed on a second surface opposite to the first surface and facing the first anode. A first electrode pair comprising a first cathode; a second anode formed on the first surface and spaced apart from the first anode; and on the second surface A second electrode pair formed with a second cathode formed at a position facing the second anode and spaced apart from the first cathode;
When light is incident from a third surface orthogonal to the first surface, the light passes through the first electrode pair and then passes through the second electrode pair, so that the third Light is emitted from the fourth surface opposite to the surface of
3. The focus of light emitted from the fourth surface of the electro-optic material is varied by changing an applied voltage between the first and second electrode pairs. The variable focus lens described. The basic unit element is:
A first anode formed on a first surface of the electro-optic material;
A first cathode formed on a second surface opposite to the first surface and formed at a position facing the first anode;
A second anode formed on the first surface and spaced from the first anode;
A second cathode formed on the second surface and facing the second anode, and spaced apart from the first cathode;
When light is incident on the first surface between the first anode and the second anode and passes through the electro-optic material, the first cathode and the second cathode Light is emitted from the second surface between
3. The focus of light emitted from the second surface of the electro-optic material is varied by changing an applied voltage between the two anodes and the two cathodes. The variable focus lens described in 1.   7. The variable focus lens according to claim 1, wherein the electro-optic material is a single crystal material having a perovskite crystal structure. The electro-optic material is KTa _1-x Nb _x O ₃ (0 ≦ x ≦ 1, KTN) crystal, or K _1-y Li _y Ta _1-x Nb _x O ₃ (0 ≦ x ≦ 1, 0 <y The varifocal lens according to claim 7, wherein the varifocal lens is <1, KLTN) crystal.   The electro-optic material is characterized in that the main component of the crystal is composed of groups Ia and Va in the periodic table, group Ia is potassium, and group Va includes at least one of niobium and tantalum. The variable focus lens according to claim 7.   8. The variable focus lens according to claim 7, wherein the electro-optical material further includes one or more members of Group Ia or Group IIa of the periodic table excluding potassium as an additive impurity.   7. The first and second anodes and the first and second cathodes are made of a material that forms a Schottky junction with the electro-optic material. Variable focus lens.

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