Embodiments of a micro-mirror array device according to the present invention will be described below in detail by referring to the accompanying diagrams. However, the present invention is not restricted to these embodiments.
Further, if not otherwise specified, a structure of one end of a micro-mirror array device is explained. However, a structure of the other side of the micro-mirror array device is the same as the structure of one end side of the micro-mirror array device.
A first embodiment of the present invention will be described below. A micro-mirror array device 100 according to the first embodiment, as shown in
Moreover, in the first embodiment, as shown in
In the micro-mirror array device 100 according to the first embodiment, for example, it is possible to arrange 40 micro-mirrors in a direction of an arrangement. However, 40 mirrors is only an exemplification, and the number of mirrors is not restricted to 40.
In the micro-mirror array device 100 according to the first embodiment shown in
Because of the hinges 102 shown in
In the first embodiment, as shown in
As it has been described earlier by referring to
As shown in
According to the first embodiment which has these characteristics, the beams 103 are formed on both sides of each of the all mirrors 101. Therefore, even for the mirror 101 at the end, it is possible to make a structure in which the hinges 102 on both sides are supported by the thin beams 103. Therefore, it is possible to make a structure same as a structure of the other mirrors 101. Consequently, an amount of distortion of the thin beam becomes constant, and it is possible to suppress the characteristics unnecessary inclination in the mirrors 101 at the both ends. Therefore, it is possible to achieve a micro-mirror array having mirrors of a favorable optical quality.
Moreover, the present invention is capable of showing an effect which is special as compared to the conventional technology. According to this effect, it is possible to solve issues without causing a problem such as an increase in a device size, in a case when a method of providing mirrors which are not used on the outer sides is particularly used, is adopted, and while avoiding a reduction in number of channels by a method in which the mirrors at the both ends are not used.
Moreover, when stiffness (shape) of the beams on both sides of the micro-mirror is let to be almost the same, it is possible to make an amount of deformation due to a stress of the beam to be almost the same for both sides, and it is possible to let the status of all the micro-mirrors to be almost the same.
The beam on an outer side of the mirror at an end is formed by providing a slit in a supporting member which supports the beam. According to this structure, since it is possible to have substantially a same structure as of beams formed on the other portion, by providing a slit in a frame member, it is possible to achieve a desirable effect.
In the present invention, in other words, beams having substantially the same amount of deformation corresponding to an external force are connected to each of a plurality of elastic members disposed on the mirrors which are positioned at both ends of the micro-mirror array. According to the invention provided with this characteristic, it is possible to make same the amount of deformation of beams on both sides of the micro-mirrors at the both ends.
Therefore, it is possible to suppress an unnecessary inclination in the micro-mirrors at the both ends. As it has been described above, in the mirror array, particularly, since a small turning along right and left directions of the mirrors at the both ends has a substantial effect on optical characteristics, it is extremely important that all the mirrors have uniform characteristics.
Next, a second embodiment of the present invention will be described below. Same reference numerals are assigned to components which are same as in the first embodiment, and the description to be repeated is omitted. In the second embodiment, an example in which an electrostatically driven micro-mirror array device is structured will be described by referring to
A supporting layer 205 of a thickness of about 300 μm, which holds the entire mirror array, is formed. The supporting layer 205, as shown in
The active layer (micro-structure) 200 is formed by an SOI (Silicon On Insulator) substrate etc., and as shown in
At this time, similarly as described by referring to
Such micro-mirror array, as shown in
By connecting the micro-mirror 101 to a ground, and applying a voltage to the drive electrode 220, an electrostatic attraction is generated between the micro-mirror 101 and the drive electrode 220, and it is possible to deflect the micro-mirror 101.
When such an arrangement is made, it is possible to form only the supporting layer 205 which supports the entire micro-mirror array by a thick member. Therefore, it is possible to form a thin elastic member which enables deflection of the micro-mirror while avoiding distortion of the entire micro-mirror array.
Next, a third embodiment of the present invention will be described below by referring to
The third embodiment has a structure in which an interval of the micro-mirrors 101 becomes wide from left to right in
The interval of the micro-mirrors 101 is determined by characteristics of a spectroscope. For example, when a grating is used, a spread angle becomes large gradually toward a long wavelength side than toward a short wavelength side.
In order to deal with this, a structure is required to be such that the interval of the micro-mirrors 101 becomes wide gradually. In such case, including the beams provided outer sides of the micro-mirrors 101 at both ends, as shown in
By providing this characteristic, even in a case in which the interval of the micro-mirrors 101 in an optical design is changed gradually, and the shape of the beam is changed, when the shape of the beams on both sides of one micro-mirror 101 are almost the same, the stiffness also are almost the same. Therefore, it is possible to achieve a desired effect. In the WSS, according the characteristics of the spectroscope, there are times all intervals between the two mirrors are not constant, and by using the present invention it is possible to solve the issue.
Furthermore, in the present embodiment, it is possible to construct that the width of the micro-mirrors 101 becomes large in accordance with that the beam becomes thick. Meanwhile, it is possible to make all the micro-mirrors 101 to be the same size. The micro-mirrors 101 having the same size have the same driving characteristic. Accordingly, a control of each of the mirror is easier compared to a control of the micro-mirror array consisting of the micro-mirrors having different width, since a condition of the drive control becomes different in a case of the micro-mirror having different width.
A structure of a modified embodiment is shown in
A spot diameter of a spectral light beam spot which is converged to each of the micro-mirrors becomes large gradually toward a long wavelength side. Accordingly, when the size in the width direction of the micro-mirror become large toward the long wavelength side, the micro-mirror can catch the spectral beam spot certainly even in a case that a slight assemble error exist.
Moreover, as the mirror interval becomes wide, a beam diameter of light is also supposed to increase. Therefore, increasing the width of the micro-mirror 101 contributes also to improve further the optical quality.
When such an arrangement is made, by making same the stiffness (shape) of the beams 103 on both sides of the micro-mirror 101, the amount of deformation due to the stress of the beams 103 becomes almost the same on both sides, and in addition to becoming same the status of all the micro-mirrors 101, it is possible to secure the widest (largest) size of a reflecting surface of the micro-mirror 101. Therefore, it is possible to minimize an optical loss.
Finally, in a structure in which the beams are formed on outer sides of the micro-mirrors at both ends, mainly a structure in which the slits are provided has been described. However, even in a configuration in which the slit is in the form of a straight line, and in the other form, it is possible to select appropriately. Moreover, it is not restricted to a case of forming the slit by etching, and it is also possible to form the slit by a method such as a pattern cutting. Further, it is not restricted to form the micro-mirrors, the hinges, and the beams integrally from one substrate, and it is also possible to form the micro-mirror array device by combining a plurality of members, as described in the present embodiment.
For making the shape of all the beams and the surrounding thereof as uniform as possible, an idea of making the shape of the slits to be U-shaped as shown in
Moreover, it is desirable that for the beam on the outer side of the mirror at the end, an outer elastic member 120 substantially same shape as the elastic member, is formed between the beam and the frame member as shown in
In this manner, the present invention can take various modified embodiments which fairly fall within the basic teaching herein set forth.
As it has been described above, the micro-mirror array device according to the present invention is useful as a micro-mirror array device in which a high optical quality is sought, and is suitable as a micro-mirror array device used in the WSS.
According to the micro-mirror array device according to the present invention, an effect is shown that it is possible to improve the optical quality by suppressing unevenness in characteristics between the mirrors.
Number | Date | Country | Kind |
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JP 2006-227412 | Aug 2006 | JP | national |