JP2015043090A - Refractive index distribution type liquid crystal optical element and image display device - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a refractive index distribution type liquid crystal optical element and a display device capable easily driving with a simple structure at a low cost.SOLUTION: The refractive index distribution type liquid crystal optical element is a liquid crystal GRIN lens array, which has a constitution that a liquid crystal layer 4 is disposed between a first transparent substrate 11 formed over the front face of an image display section 5 and a second transparent substrate 12 facing to the first transparent substrate 11. The first substrate 11 includes a first transparent electrode 21; a second transparent electrode 22; a third transparent electrode 23; a fifth transparent electrode 25; and a transparent dielectric layer 3 formed on the plane at the liquid crystal layer. The first electrode 21, the second electrode 22, the third electrode 23 and fifth electrode 25 are formed extending in a second direction crossing a first direction 61.

Description

  Embodiments described herein relate generally to a gradient index liquid crystal optical element and an image display device.

  A display device capable of displaying a stereoscopic image (three-dimensional image) has been proposed. In addition, there is a demand for switching between the display of a two-dimensional image and the display of a three-dimensional image with the same display device, and a technique for meeting that demand has been proposed. For example, there is a technique for switching between two-dimensional image display and three-dimensional image display using a liquid crystal lens array element. This liquid crystal lens array element has rod-shaped electrodes periodically arranged on one substrate. Then, an electric field distribution is created between the electrodes formed on the other opposing substrate, and the orientation of the liquid crystal layer is changed by the electric field distribution to generate a refractive index distribution that acts as a lens. By controlling the voltage applied to the electrodes, the lens action can be turned on or off, so that the two-dimensional image display and the three-dimensional image display can be switched. Such a method of controlling the alignment direction of liquid crystal molecules by an electric field is called a liquid crystal gradient index lens method or a liquid crystal GRIN (gradient index) lens method.

  In addition, a technique has been proposed in which two different voltages are applied to rod-shaped electrodes periodically arranged on one substrate. By applying two different voltages, a refractive index distribution that is more preferable as a lens array is generated.

  Thus, attempts have been made to realize a liquid crystal GRIN lens. However, in order to realize good three-dimensional image display using the liquid crystal GRIN lens, it is necessary to set the focal length of the liquid crystal GRIN lens to the distance between the principal point of the liquid crystal GRIN lens and the pixel surface of the image display unit. There is. For this purpose, a certain amount of refractive power is required for the liquid crystal layer of the liquid crystal GRIN lens. However, since the refractive index anisotropy of liquid crystal molecules is usually as small as about 0.2, it is necessary to make the thickness of the liquid crystal layer considerably larger than that of a normal display panel. This not only increases the amount of liquid crystal used, leading to higher costs, but also increases the difficulty in manufacturing.

  Therefore, it has been proposed to convert the liquid crystal GRIN lens into a Fresnel lens. This is achieved by providing a large number of rod-shaped electrodes on one substrate and applying a large number of different voltages to realize a refractive index distribution as a Fresnel lens.

However, in the Fresnel lens type liquid crystal GRIN lens array, it is necessary to arrange a large number of rod-shaped electrodes for each lens, and a technique for finely processing the transparent electrode is required.
The microfabrication of the transparent electrode requires a high-precision stepper, a dry etching apparatus, and the like, which raises a problem of increasing costs. In addition, it is necessary to apply a large number of different voltages to a large number of rod-shaped electrodes, and there is a problem in that driving is complicated and cost increases.

JP 2000-102038 A JP 2010-224191 A US Patent Application Publication No. 2010/0026920

  SUMMARY OF THE INVENTION The problem to be solved by the present invention is to provide a low-cost gradient index liquid crystal optical element and display device that can be driven easily with a simple structure.

  The gradient index liquid crystal optical element of the present embodiment includes a first substrate having a main surface, a second substrate, a liquid crystal layer provided between the main surface of the first substrate and the second substrate, A first electrode, a second electrode, a third electrode, and a fourth electrode provided side by side in a first direction parallel to the main surface between the main surface of the first substrate and the liquid crystal layer; A fifth electrode provided side by side in the first direction between the main surface of the first substrate and the liquid crystal layer, and at least partially overlapping the first electrode when projected onto the main surface; A sixth electrode that at least partially overlaps the second electrode when projected, a seventh electrode that at least partially overlaps the third electrode when projected onto the main surface, and the seventh electrode that projects onto the main surface when projected onto the main surface An eighth electrode at least partially overlapping the fourth electrode; and the main surface of the first substrate. A ninth electrode provided between the liquid crystal layer and positioned between the fifth electrode and the sixth electrode when projected onto the main surface; and the seventh electrode when projected onto the main surface. Between the first electrode and the eighth electrode, between the first electrode and the fifth electrode, between the second electrode and the sixth electrode, between the third electrode and the seventh electrode. And a dielectric layer provided between the fourth electrode and the eighth electrode, and an eleventh electrode provided between the second substrate and the liquid crystal layer, on the main surface The minimum distance between the projected fifth electrode and the ninth electrode is smaller than the minimum distance between the first electrode and the ninth electrode projected onto the main surface, and the first distance projected onto the main surface. The minimum distance between the six electrodes and the ninth electrode is smaller than the minimum distance between the second electrode and the ninth electrode projected onto the main surface. A minimum distance between the seventh electrode and the tenth electrode projected onto the main surface is smaller than a minimum distance between the third electrode and the tenth electrode projected onto the main surface; The minimum distance between the eighth electrode and the tenth electrode projected onto the main surface is smaller than the minimum distance between the fourth electrode and the tenth electrode projected onto the main surface, and the minimum distance projected onto the main surface The minimum distance between the sixth electrode and the third electrode is larger than the minimum distance between the second electrode and the third electrode projected onto the main surface, and the seventh electrode projected onto the main surface and the The minimum distance from the second electrode is larger than the minimum distance between the third electrode and the second electrode projected onto the main surface.

Sectional drawing which shows the image display apparatus by 1st Embodiment. The top view of the liquid-crystal GRIN lens array in 1st Embodiment. Sectional drawing which shows liquid-crystal director distribution at the time of the voltage application cut | disconnected by the cutting line AA of FIG. FIG. 4 is a graph showing a refractive index distribution calculated from the liquid crystal director distribution shown in FIG. 3 with the horizontal axis representing coordinates in the lens pitch direction and the vertical axis representing the optical path length. The block diagram which shows the image display apparatus of 1st Embodiment. Sectional drawing which shows the image display apparatus by the 1st modification of 1st Embodiment. Sectional drawing which shows the image display apparatus by the 2nd modification of 1st Embodiment. Sectional drawing which shows the image display apparatus by the 3rd modification of 1st Embodiment. Sectional drawing which shows the image display apparatus by the 4th modification of 1st Embodiment. Sectional drawing which shows the image display apparatus by 2nd Embodiment. Sectional drawing which shows the image display apparatus by 3rd Embodiment.

  Hereinafter, embodiments will be described in detail with reference to the drawings. Note that, in the following embodiments, the same reference numerals are assigned to the same operations, and duplicate descriptions are omitted as appropriate.

(First embodiment)
The image display apparatus according to the first embodiment will be described with reference to FIGS. An image display apparatus according to the first embodiment is shown in FIG. The image display device of this embodiment includes a gradient index liquid crystal optical element 1 and an image display unit 5. The image display unit 5 is a display panel having pixels arranged in a matrix on the display surface. For example, a liquid crystal panel, an organic EL panel, a plasma display panel, or the like can be suitably used. In the present embodiment, the image display unit 5 is configured to emit linearly polarized light in the first direction 61 indicated by the arrow.
In this embodiment, the gradient index liquid crystal optical element 1 is a liquid crystal GRIN lens array, and a top view of the liquid crystal GRIN lens array 1 is shown in FIG.

  The liquid crystal GRIN lens array 1 is provided on the front surface of the image display unit 5, and a liquid crystal layer 4 is disposed between a transparent first substrate 11 and a transparent second substrate 12 disposed to face the first substrate 11. It has a sandwiched configuration. On the surface of the first substrate 11 on the liquid crystal layer side, a transparent first electrode 21, a transparent second electrode 22, a transparent third electrode 23, a transparent fifth electrode 25, and a transparent dielectric layer 3 is provided. The first electrode 21, the second electrode 22, the third electrode 23, and the fifth electrode 25 are provided so as to extend in a second direction 62 that intersects the first direction 61, as shown in FIG. It is done. In FIG. 2, the second direction 62 is arranged so as to be orthogonal to the first direction 61, but may not be orthogonal. A transparent fourth electrode 24 is provided on the surface of the second substrate 12 on the liquid crystal layer side. The fourth electrode 24 is provided so as to face the first electrode 21, the second electrode 22, the third electrode 23, and the fifth electrode 25, and is substantially on the entire surface of the second substrate 12 on the liquid crystal layer side. Provided. The liquid crystal layer 4 includes liquid crystal molecules 41, and in the present embodiment, a material exhibiting uniaxial birefringence is used as the liquid crystal molecules 41. In the initial alignment of the liquid crystal molecules 41 when no voltage is applied to the first to fifth electrodes, the major axis direction is the first direction 61.

  A plurality of third electrodes 23 are arranged in parallel in the first direction 61 on the surface of the first substrate 11 on the liquid crystal layer side, and the first electrodes 21 are arranged on both sides of each third electrode. ing. The fifth electrode 25 is arranged approximately at the center between the adjacent third electrodes. The first electrode 21, the third electrode 23, and the fifth electrode are covered with the dielectric layer 3. A second electrode 22 is provided on the dielectric layer 3 so as to correspond to each of the first electrodes 21. Therefore, the second electrode 22 is electrically insulated from the first electrode 21, the third electrode 23, the fifth electrode and the dielectric layer 3. In addition, each second electrode 22 is arranged such that a central axis extending in the second direction is located on the third electrode 23 side with respect to the central axis of the corresponding first electrode 21.

  In this specification, a set of the first electrode 21 disposed on the left side of the third electrode 23 in the drawing and the second electrode 22 corresponding to the first electrode 21 is referred to as an electrode pair 200A. A set of the first electrode 21 disposed on the right side of the second electrode 23 and the second electrode 22 corresponding to the first electrode 21 is referred to as an electrode pair 200B. Then, on the first substrate 11, the electrode pair 200A, the third electrode 23, the electrode pair 200B, the fifth electrode 25, the electrode pair 200A, the third electrode 23, and the electrode pair 200B are arranged in this order from the left in FIG. It has a configuration. That is, the electrode pair 200A and the electrode pair 200B are disposed between the adjacent third electrodes 23, and the fifth electrode is disposed between the electrode pair 200A and the electrode pair 200B. Further, the electrode pair 200 </ b> A and the electrode pair 200 </ b> B disposed on both sides of the third electrode 23 are disposed symmetrically with respect to the third electrode 23. That is, when viewed from the top view shown in FIG. 2, they are arranged symmetrically with respect to the central axis of the third electrode 23.

Next, the distance between the electrode pairs 200A and 200B will be described. When viewed from the second substrate side, the distance between the central axis of the third electrode 23 and the central axis of the electrode pair 200A disposed on the left side of the third electrode 23 is P1, and the central axis of the third electrode is The distance from the central axis of the electrode pair 200B disposed on the right side of the third electrode 23 is P2. At this time, when the distance between the central axes of the electrode pair 200A and the electrode pair 200B disposed between the adjacent third electrodes 23 is P3,
P3> P1 + P2
It is the structure arrange | positioned so that these conditions may be satisfy | filled (FIG. 2). The central axis of the electrode pair 200A disposed on the left side of the third electrode 23 is the middle between the farthest side surface and the nearest side surface parallel to the second direction 62 of the electrode pair 200A with respect to the third electrode 23. The center axis of the electrode pair 200B disposed on the right side of the third electrode 23 is parallel to the second direction 62 of the electrode pair 200B with respect to the third electrode 23, and the farthest side surface and the nearest side surface Located in the middle.

  Next, the operation of the liquid crystal GRIN lens array 1 in the display device of the first embodiment will be described. FIG. 3 shows the distribution of the liquid crystal directors in the plane cut along the cutting line AA shown in FIG. 2 when a voltage is applied to each electrode. The distribution of the liquid crystal director was obtained by simulation. FIG. 4 shows a refractive index distribution calculated from the liquid crystal director distribution shown in FIG. The horizontal axis shown in FIG. 4 is the coordinates in the lens pitch direction. The center axis of the fifth electrode 25 shown in FIG. 2 is the origin, the direction parallel to the first direction 61 is the x axis, and the distance from the origin. Is shown. The vertical axis in FIG. 4 indicates the optical path length.

  In the liquid crystal GRIN lens array 1 in the first embodiment, when the fourth electrode 24 is set to a reference voltage (for example, GND), the same voltage as the fourth electrode 24 is applied to the fifth electrode 25. In both the electrode pair 200 </ b> A and the electrode pair 200 </ b> B, a higher voltage is applied to the first electrode 21 than to the second electrode 22. Specifically, if the voltage of the first electrode 21 is V1, and the voltage of the second electrode 22 is V2, V1> V2.

  The voltage V2 of the second electrode 22 is set to be higher than the voltage of the fifth electrode 25. However, the voltage difference between the second electrode 22 and the fifth electrode 25 is set to be smaller than the threshold voltage Vth of the liquid crystal layer 4. That is, V2 <Vth. The voltage V3 of the third electrode 23 is the same voltage as the voltage V1 of the first electrode 21.

  The alignment state of the liquid crystal molecules 41 when the voltage is applied in this way will be described. First, since the voltage difference is zero between the fifth electrode 25 and the fourth electrode 24, the liquid crystal molecules 41 maintain the initial alignment state as shown in FIGS. That is, the apparent refractive index is large, and as a result, the optical path length is also large.

  Next, a predetermined voltage V1 is applied between the first electrode 21 and the fourth electrode 24, and the liquid crystal molecules 41 rise. As a result, the apparent refractive index is reduced, and as a result, the optical path length is also reduced. Note that the refractive index gradually changes between the fifth electrode 25 and the first electrode 21, and the optical path length gradually changes accordingly.

  On the other hand, the voltage difference between the second electrode 22 and the fourth electrode 24 is set to V2 which is smaller than the threshold voltage Vth of the liquid crystal layer 4. For this reason, the rise of the liquid crystal molecules 41 is hardly seen. As a result, the apparent refractive index is increased and the optical path length is also increased. In addition, since the first electrode 21 and the second electrode 22 are formed by being laminated, the change in the refractive index in this portion is steep.

  Since the same voltage as the voltage V1 of the first electrode 21 is applied between the third electrode 23 and the fourth electrode 24 as described above, the apparent refractive index is reduced, and as a result, the optical path length is also reduced. It is getting smaller.

  In this way, a refractive index distribution (optical path length distribution) as a Fresnel lens is realized.

  As shown in FIG. 5, the liquid crystal GRIN lens array 1 is driven by the drive circuit 81, and voltages satisfying the above-described conditions are applied to the electrodes 21 to 25 of the liquid crystal GRIN lens array 1. Further, the image display unit 5 is driven by the drive circuit 85. At this time, the drive circuit 81 synchronizes with the drive circuit 85, and when the image display unit 5 displays a three-dimensional image, a voltage that satisfies the above-described condition is applied by the drive circuit 81 to the electrodes 21 to 21 of the liquid crystal GRIN lens array 1. 25. At this time, the distance between adjacent third electrodes 23 shown in FIG. 1 is one unit of the lens, that is, the lens pitch, and corresponds to one of the exit pupils when displaying a three-dimensional image. When the image display unit 5 displays a two-dimensional image, a reference voltage (GND) is applied to each electrode 21 to 25 of the liquid crystal GRIN lens array 1 by the drive circuit 81.

  Next, effects of the first embodiment will be described.

  In the present embodiment, as described above, the central axis of the second electrode 22 in the electrode pair 200A is disposed closer to the third electrode 23 than the central axis of the first electrode 21, and the second electrode 22 of the electrode pair 200B The center is arranged closer to the third electrode 23 than the center of the first electrode 21. As a result, a Fresnel lens array can be realized with a smaller number of electrodes than in the prior art. For this reason, it becomes possible to process using a normal semiconductor manufacturing technique without using a dedicated technique for finely processing the transparent electrode, and a liquid crystal GRIN lens array can be produced at a low cost. Further, since the number of electrodes is small, the types of voltages required for control can be reduced, and driving can be simplified and the cost can be reduced.

  In addition, by forming the first electrode 21 and the second electrode 22 corresponding to the first electrode 21 as in the present embodiment, a steep refractive index distribution suitable for a Fresnel lens can be created. High performance can be achieved. In order to generate such a steep refractive index profile, the gap between the first electrode 21 and the second electrode 22, that is, the minimum distance between the first electrode 21 and the second electrode 22 is reduced. It was proved by the present inventors that this is preferable. Here, the minimum distance between the first electrode 21 and the second electrode 22 means the minimum value among the distances between an arbitrary point on the first electrode 21 and an arbitrary point on the second electrode 22. In the present embodiment, since the first electrode 21 and the second electrode 22 overlap when viewed from the fourth electrode 24, the gap between the two electrodes is equal to the thickness of the dielectric layer 3 and the first electrode. The thickness of the electrode 21 is different. As a result, as shown in FIG. 3, the overlapping portion of the electric field lines is confined between the electrodes, and a steep refractive index distribution is generated by the electric field leaking from the non-overlapping portion. However, the distance between the first electrode 21 and the second electrode 22 in the first direction 61, that is, the maximum distance in the first direction 61 of the non-overlapping portion when viewed from the fourth electrode 24 is at least the dielectric layer 3. It is preferable that it becomes below this thickness. This is because when the maximum distance is larger than the thickness of the dielectric layer 3, the leakage electric field between both electrodes is increased, and an electric field component parallel to the first direction 61 is generated, thereby generating a steep refractive index distribution. This is because it becomes difficult. Here, the maximum distance between the first electrode 21 and the second electrode 22 means the maximum value among the distances between an arbitrary point on the first electrode 21 and an arbitrary point on the second electrode 22.

As described above, the arrangement of the electrodes in the first direction 61 is
P3> P1 + P2
The thickness of the liquid crystal layer 4 can be further reduced. Referring to the refractive index distribution shown in FIG. 4, rather than providing a Fresnel step near the optical axis of the lens, that is, the central axis of the fifth electrode 25, the end of the lens, that is, the center of the third electrode 23. It is obvious that the thickness near the axis can reduce the thickness of the liquid crystal layer 4. Note that the thickness of the liquid crystal layer 4 can be minimized when the value on the optical axis and the value on the step portion of the Fresnel match in the refractive index distribution shown in FIG. In order to realize such a refractive index distribution, it is preferable to arrange each electrode in advance and adjust the applied voltage.

  Further, regarding the voltage applied to the liquid crystal GRIN lens array 1 of the first embodiment, the voltage difference between the second electrode 22 and the fourth electrode 24 is smaller than the threshold voltage Vth of the liquid crystal layer 4. Is set. Thereby, it is possible to suppress the rise of the liquid crystal molecules 41 between the second electrode 22 and the fourth electrode 24, and it is possible to realize a steep refractive index distribution suitable as a Fresnel lens. Furthermore, since the voltage applied to the second electrode 22 can be increased, the voltage difference with the first electrode 21 can be reduced, and the leakage electric field between the first electrode 21 and the second electrode is suppressed. it can. As a result, a component parallel to the first direction 61 of the leakage electric field can be reduced, and a steeper refractive index characteristic can be realized.

  In the first embodiment, each of the first electrode 21 and the second electrode 22 corresponding to the first electrode is opposite to the third electrode 23 side, that is, each end (side surface) on the fifth electrode 25 side. As shown in FIG. 1, the position of the end of the second electrode 22 is closer to the third electrode 23 than the position of the end of the first electrode 21. However, the end portion of the second electrode 22 may protrude from the end portion of the first electrode 21 toward the fifth electrode 25. However, if the thickness of the dielectric layer 3 is t, the amount of the end of the second electrode 22 protruding from the end of the first electrode 21 to the fifth electrode 25 side may be t or less. preferable. If the amount of protrusion is larger than t, the electric lines of force due to the second electrode 22 are not sufficiently shielded by the first electrode 21, and the refractive index distribution as a lens is disturbed, resulting in performance. It is because it falls. That is, by configuring as described above, an appropriate refractive index distribution as a Fresnel lens can be realized, and performance can be improved.

  In the first embodiment, the positions of the respective end portions on the third electrode 23 side with respect to the first electrode 21 and the second electrode 22 corresponding to the first electrode 21 are the second positions as shown in FIG. The position of the end of the electrode 22 protrudes from the position of the end of the first electrode 21. This amount of protrusion is preferably t or more, where t is the thickness of the dielectric layer 3. This is because if the amount of protrusion is smaller than t, the electric lines of force due to the second electrode 22 are shielded by the first electrode 21 and the performance as a Fresnel lens is deteriorated. That is, the lens performance can be improved by configuring as described above, which is preferable.

  Furthermore, when comparing the width of the first electrode 21 and the second electrode corresponding to the first electrode 21, the width of the portion of the second electrode 22 that does not overlap the first electrode 21 when viewed from the fourth electrode 24 is A width larger than the width of the first electrode 21 is preferable. By configuring in this way, it is possible to suitably realize a refractive index distribution unique to the Fresnel lens. In other words, it is preferable that the electrode width of the second electrode 22 that should realize a gentle refractive index distribution be larger than the electrode width of the first electrode 21 that should realize a steeper refractive index distribution.

  In the first embodiment, the electrode pair 200 </ b> A and the electrode pair 200 </ b> B have been described as being symmetrically disposed with respect to the third electrode 23. However, the present invention is not limited to this. It is not always necessary to arrange them symmetrically. However, it is preferable to arrange them symmetrically because the refractive index distribution as a lens can be made more desirable.

  In the first embodiment, since the second electrode 22 is disposed on the dielectric layer 3, the second electrode 22 is located closer to the liquid crystal layer 4 than the first electrode 21. It becomes possible to suppress the disturbance of the electric field in the portion (near the electrode 22) where a more gentle refractive index distribution should be realized, and the lens performance can be improved.

  In the first embodiment, since the fifth electrode 25 is provided between the adjacent third electrodes 23, it is possible to make the refractive index distribution as a lens more ideal and improve the lens performance. be able to.

  As described above, according to the first embodiment, it is possible to provide a low-cost gradient index liquid crystal optical element and a display device that can be driven easily with a simple structure.

(First modification)
Next, an image display apparatus according to a first modification of the first embodiment is shown in FIG. FIG. 6 is a cross-sectional view showing an image display device of a first modification. The image display apparatus according to the first modification has a configuration in which the liquid crystal GRIN lens array 1 is replaced with a liquid crystal GRIN lens array 1A in the image display apparatus according to the first embodiment shown in FIG. In this liquid crystal GRIN lens array 1A, in the liquid crystal GRIN lens array 1 shown in FIG. It has a configuration.

  Similarly to the first embodiment, the first modified example configured as described above can provide a low-cost gradient index liquid crystal optical element and a display device that can be easily driven with a simple structure. In the first modification, the first electrode 21 and the third electrode 23 are arranged on the liquid crystal layer 4 side of the dielectric layer 3. Thereby, in the 1st electrode 21 and the 3rd electrode 23, the voltage drop by the dielectric material layer 3 can be suppressed. Since the first electrode 21 and the third electrode 23 apply a relatively higher voltage than the second electrode 22 and the fifth electrode 25, the effect of reducing the driving voltage is great. That is, since the maximum output voltage of the drive circuit can be reduced, not only the drive circuit can be simplified, but also power consumption can be reduced.

(Second modification)
Next, an image display apparatus according to a second modification of the first embodiment is shown in FIG. FIG. 7 is a cross-sectional view illustrating an image display apparatus according to a second modification. The image display device of the second modification has a configuration in which the liquid crystal GRIN lens array 1 is replaced with a liquid crystal GRIN lens array 1B in the image display device of the first embodiment shown in FIG. The liquid crystal GRIN lens array 1B has a configuration in which the third electrode 23 is disposed on the dielectric layer 3 in the liquid crystal GRIN lens array 1 shown in FIG.

  Similarly to the first embodiment, the second modification configured as described above can also provide a low-cost gradient index liquid crystal optical element and a display device that have a simple structure and can be driven easily.

  Further, as in the second modification, the second electrode 22 is provided on the liquid crystal layer 4 side as compared with the first electrode 21, thereby realizing a more gentle refractive index distribution than in the first modification. It is possible to suppress disturbance of the electric field in the portion to be (the vicinity of the electrode 22), and to improve the lens performance.

(Third Modification)
Next, an image display apparatus according to a third modification of the first embodiment is shown in FIG. FIG. 8 is a cross-sectional view illustrating an image display device according to a third modification. The image display device of the third modification has a configuration in which the liquid crystal GRIN lens array 1A is replaced with a liquid crystal GRIN lens array 1C in the image display device of the first modification shown in FIG. This liquid crystal GRIN lens array 1C has a configuration in which the fifth electrode 25 is omitted from the liquid crystal GRIN lens array 1A shown in FIG.

  Similarly to the first modified example, the third modified example configured as described above can provide a low-cost gradient index liquid crystal optical element and a display device that can be driven easily with a simple structure.

(Fourth modification)
Next, an image display apparatus according to a fourth modification of the first embodiment is shown in FIG. FIG. 9 is a cross-sectional view showing an image display device according to a fourth modification. The image display device of the fourth modification has a configuration in which the liquid crystal GRIN lens array 1 is replaced with a liquid crystal GRIN lens array 1D in the image display device of the first embodiment shown in FIG. The liquid crystal GRIN lens array 1D has a configuration in which the first electrode 21 is disposed on the dielectric layer 3 and the second electrode 22 is disposed on the first substrate 11 in the liquid crystal GRIN lens array 1 shown in FIG. Yes. That is, the second electrode 22, the third electrode 23 and the fifth electrode 25 are arranged on the first substrate 11.

  In general, an alignment error may occur between the electrode formed on the first substrate 11 and the electrode formed on the dielectric layer 3 when formed. In order to reduce the influence of this alignment error, it is effective in the present modification to form the third electrode 23, the fifth electrode 25, and the second electrode 22 on the same layer, that is, the first substrate 11. Thereby, since the positional relationship between the lens end and the lens center can be created by the same exposure process, it is possible to suppress the deviation of the main part such as the center of the lens, and the lens performance can be improved. In addition, it is more preferable to form both the lens end and the lens center electrode on the first substrate 11 than on the dielectric layer 3. This is because the former can eliminate the influence of the dielectric layer 3. Further, in the fourth modification, the third electrode 23, the fifth electrode 25, and the second electrode 22 are formed on the first substrate 11, and the first electrode is formed on the dielectric layer 3. It may be formed. That is, the third electrode 23, the fifth electrode 25, and the second electrode 22 may be formed on the dielectric layer 3, and the first electrode may be formed on the first substrate 11.

  Similarly to the first embodiment, the fourth modified example configured as described above can provide a low-cost gradient index liquid crystal optical element and a display device that can be driven with a simple structure.

  In the first embodiment and the first to fourth modified examples, the initial alignment of the liquid crystal has been described as the horizontal alignment in the horizontal direction, but the initial alignment of the liquid crystal is not limited to this. Other liquid crystal alignment modes are also applicable.

  In the first embodiment and the first to fourth modified examples, the gradient index liquid crystal optical element is described as a liquid crystal lens array element. However, the present invention is not limited to this. The optical element should just have the performance for implement | achieving the display of a three-dimensional image. For example, the refractive index distribution as a complete lens may not be realized, or may function as a prism array element.

  Further, in the first embodiment and the first to fourth modified examples, the refractive index distribution type liquid crystal optical element is used as the refractive index distribution type optical element for controlling the light beam from the image display unit 5. The material to be used is not limited to liquid crystal. Any material having the same electro-optic effect can be applied as the gradient index optical element.

  In the first embodiment and the first to fourth modifications, the lens array is described as being arranged along the first direction 61. However, the present invention is not limited to this. For example, a fly-eye lens can be realized by two-dimensional arrangement.

(Second Embodiment)
Next, an image display apparatus according to a second embodiment will be described with reference to FIG. FIG. 10 is a cross-sectional view showing an image display apparatus according to the second embodiment.

  The image display device according to the second embodiment has a configuration in which the liquid crystal GRIN lens array 1A is replaced with a liquid crystal GRIN lens array 1E in the image display device according to the first modification of the first embodiment shown in FIG. The liquid crystal GRIN lens array 1E includes an electrode pair 200B including a first electrode 21 and a second electrode 22 on the left side of the fifth electrode 25 and between the third electrode 23 in the liquid crystal GRIN lens array 1A shown in FIG. And at least one pair of electrode pairs including the first electrode 21 and the second electrode 22 between the right side of the fifth electrode 25 and the third electrode 23. ing. In addition, in FIG. 10, the electrode pairs 200A and 200B further provided are each a set. That is, in the first embodiment and the first to fourth modifications, the liquid crystal GRIN lens array is a two-stage Fresnel lens. On the other hand, the second embodiment is different in that a multi-stage Fresnel lens is realized.

  The operation in the second embodiment is the same as that described in the first embodiment.

  In the second embodiment, the thickness of the liquid crystal layer 4 can be further reduced and the cost can be reduced by increasing the number of Fresnel lenses.

  Also, the second embodiment can provide a low-cost refractive index distribution type liquid crystal optical element and a display device that have a simple structure and can be easily driven, as in the first embodiment.

  Note that the multi-stage Fresnel lens as in the second embodiment can also be applied to the first embodiment or modifications thereof.

(Third embodiment)
Next, an image display apparatus according to a third embodiment will be described with reference to FIG. FIG. 11 is a cross-sectional view showing an image display apparatus according to the third embodiment.

  In the first and second embodiments, the liquid crystal GRIN lens array has the dielectric layer 3, and the first electrode 21 and the second electrode 22 are formed in different layers with the dielectric layer 3 interposed therebetween. In contrast, the third embodiment is different in that the dielectric layer 3 is not provided and the first electrode 21 and the second electrode 22 are formed on the first substrate 11. The operation in the third embodiment is the same as that described in the first embodiment.

  In the third embodiment, the Fresnelization of the liquid crystal GRIN lens can be realized with the electrodes configured by the same layer (single layer). A single-layer electrode can reduce the number of processes compared to the production of an electrode having a laminated structure as in the first to second embodiments, so that the cost can be reduced.

  Also, the third embodiment can provide a low-cost refractive index distribution type liquid crystal optical element and a display device that are simple in structure and easy to drive, as in the first embodiment.

  Although several embodiments of the present invention have been described, these embodiments are presented by way of example and are not intended to limit the scope of the invention. These embodiments can be implemented in various other forms, and various omissions, replacements, and changes can be made without departing from the scope of the invention. These embodiments and modifications thereof are included in the invention described in the claims and equivalents thereof as well as included in the scope and gist of the invention.

1 liquid crystal GRIN lens array 1A liquid crystal GRIN lens array 1B liquid crystal GRIN lens array 1C liquid crystal GRIN lens array 1D liquid crystal GRIN lens array 1E liquid crystal GRIN lens array 1F liquid crystal GRIN lens array 11 first substrate 12 second substrate 21 first electrode 22 second electrode Electrode 23 3rd electrode 24 4th electrode 25 5th electrode 3 Dielectric layer 4 Liquid crystal layer 41 Liquid crystal molecule 5 Image display part 61 1st direction 62 2nd direction 200A Electrode pair 200B Electrode pair

Claims (7)

A first substrate having a main surface;
A second substrate;
A liquid crystal layer provided between the main surface of the first substrate and the second substrate;
A first electrode, a second electrode, a third electrode, and a fourth electrode arranged in a first direction parallel to the main surface between the main surface of the first substrate and the liquid crystal layer;
A fifth electrode provided side by side in the first direction between the main surface of the first substrate and the liquid crystal layer, and at least partially overlapping the first electrode when projected onto the main surface; A sixth electrode that at least partially overlaps with the second electrode when projected onto the seventh electrode, a seventh electrode that at least partially overlaps with the third electrode when projected onto the major surface, and when projected onto the major surface An eighth electrode at least partially overlapping the fourth electrode;
A ninth electrode provided between the main surface of the first substrate and the liquid crystal layer and positioned between the fifth electrode and the sixth electrode when projected onto the main surface; and the main surface A tenth electrode positioned between the seventh electrode and the eighth electrode when projected onto
Provided between the first electrode and the fifth electrode, between the second electrode and the sixth electrode, between the third electrode and the seventh electrode, and between the fourth electrode and the eighth electrode. A dielectric layer formed;
An eleventh electrode provided between the second substrate and the liquid crystal layer;
With
The minimum distance between the fifth electrode and the ninth electrode projected onto the main surface is smaller than the minimum distance between the first electrode and the ninth electrode projected onto the main surface, and is projected onto the main surface. The minimum distance between the sixth electrode and the ninth electrode is smaller than the minimum distance between the second electrode and the ninth electrode projected onto the main surface, and the seventh distance projected onto the main surface. A minimum distance between the electrode and the tenth electrode is smaller than a minimum distance between the third electrode and the tenth electrode projected onto the main surface, and the eighth electrode and the tenth electrode projected onto the main surface. The minimum distance from the electrode is smaller than the minimum distance between the fourth electrode and the tenth electrode projected on the main surface,
The minimum distance between the sixth electrode and the third electrode projected onto the main surface is larger than the minimum distance between the second electrode and the third electrode projected onto the main surface, and is projected onto the main surface. A gradient index liquid crystal optical element, wherein a minimum distance between the seventh electrode and the second electrode is larger than a minimum distance between the third electrode and the second electrode projected onto the main surface. The difference between the minimum distance between the sixth electrode and the third electrode projected onto the main surface and the minimum distance between the second electrode and the third electrode projected onto the main surface is the first distance Less than or equal to the thickness of the dielectric layer provided between two electrodes and the sixth electrode;
The difference between the minimum distance between the seventh electrode and the second electrode projected onto the main surface and the minimum distance between the third electrode and the second electrode projected onto the main surface is the first distance The gradient index liquid crystal optical element according to claim 1, wherein the gradient index liquid crystal optical element is equal to or less than a thickness of the dielectric layer provided between three electrodes and the seventh electrode. The difference between the minimum distance between the sixth electrode and the ninth electrode projected onto the main surface and the minimum distance between the second electrode and the ninth electrode projected onto the main surface is More than the thickness of the dielectric layer provided between the two electrodes and the sixth electrode,
The difference between the minimum distance between the seventh electrode and the tenth electrode projected onto the main surface and the minimum distance between the third electrode and the tenth electrode projected onto the main surface is the first distance 3. The gradient index liquid crystal optical element according to claim 1, wherein the refractive index distribution type liquid crystal optical element is equal to or greater than a thickness of the dielectric layer provided between three electrodes and the seventh electrode. The difference between the minimum distance between the fifth electrode and the ninth electrode projected onto the main surface and the minimum distance between the first electrode and the ninth electrode projected onto the main surface is the first distance. More than the thickness of the dielectric layer provided between the electrode and the fifth electrode,
The difference between the minimum distance between the eighth electrode and the tenth electrode projected onto the main surface and the minimum distance between the fourth electrode and the tenth electrode projected onto the main surface is the fourth distance. 4. The gradient index liquid crystal optical element according to claim 1, wherein the gradient index liquid crystal optical element is equal to or greater than a thickness of the dielectric layer provided between the electrode and the eighth electrode. 5.   The length along the first direction of the portion of the fifth electrode projected on the main surface that does not overlap the first electrode is longer than the length along the first direction of the first electrode, The length along the first direction of the portion of the sixth electrode projected on the main surface that does not overlap the second electrode is longer than the length along the first direction of the second electrode. The length along the first direction of the portion of the seventh electrode projected on the surface that does not overlap the third electrode is longer than the length along the first direction of the third electrode, and the main surface The length along the first direction of the portion of the eighth electrode projected on the fourth electrode that does not overlap the fourth electrode is longer than the length of the fourth electrode along the first direction. 5. The gradient index liquid crystal optical element according to any one of 4 above.   The twelfth electrode is further provided between the main surface of the first substrate and the liquid crystal layer, and is positioned between the second electrode and the third electrode when projected onto the main surface. 6. A gradient index liquid crystal optical element according to any one of 1 to 5. Between the first electrode and the eleventh electrode, between the second electrode and the eleventh electrode, between the third electrode and the eleventh electrode, and between the fourth electrode and the eleventh electrode, A first voltage is applied between
Between the fifth electrode and the eleventh electrode, between the sixth electrode and the eleventh electrode, between the seventh electrode and the eleventh electrode, and between the eighth electrode and the eleventh electrode, A second voltage lower than the first voltage is applied during
The drive part which applies the 3rd voltage larger than the said 2nd voltage between the said 9th electrode and the said 11th electrode, and between the said 10th electrode and the said 11th electrode is further provided. The gradient index liquid crystal optical element according to any one of the above.