The present invention relates to a two-dimensional light deflector that two-dimensionally deflects a light beam.
Two-dimensional light deflectors that two-dimensionally deflect a light beam include a deflector in which two galvano deflectors each having a mirror are orthogonally disposed. In such a two-dimensional light deflector, when the light beam is actually two-dimensionally deflected, the locus of the light beam is distorted on an image plane.
U.S. Pat. No. 4,838,632 discloses a two-dimensional light deflector with such reduced distortion.
The two-dimensional light deflector 500 achieves a reduction in the distortion of the trajectory of the light beam on the image plane while being extremely compact with a simple configuration.
The present invention is directed to a two-dimensional light deflector that deflects a collimated light beam two-dimensionally. The two-dimensional light deflector includes a first deflector that deflects the collimated light beam in a plane, a second deflector that deflects the collimated light beam in another plane, and a fixing member directly fixing both the first deflector and the second deflector. The first deflector includes a light radiating portion that generates the collimated light beam from light guided by a light guide and radiates it. The light radiating portion is supported oscillatably around a first axis extending outside of the light radiating portion, and radiates the collimated light beam toward the first axis along a first plane perpendicular to the first axis, so that an oscillation of the light radiating portion causes deflection of the collimated light beam along the first plane. The second deflector includes an oscillatable reflecting face that reflects the collimated light beam radiated from the light radiating portion. The reflecting face is inclined by 45 degrees with respect to a plane including the first axis at a time of non-oscillation, and is also inclined by 45 degrees with respect to a plane including a second axis that coincides with a principal ray of the collimated light beam radiated from the light radiating portion at the time of non-oscillation, so that the reflecting face converts deflection of the collimated light beam in the first plane into deflection of the collimated light beam along a second plane perpendicular to the second axis. The reflecting face is also oscillatably supported around a third axis passing through an intersection of the first axis and the second axis, and perpendicular to both the first axis and the second axis, so that an oscillation of the reflecting face around the third axis causes deflection of the collimated light beam in a third plane perpendicular to the third axis.
Advantages of the invention will be set forth in the description that follows, and in part will be obvious from the description, or may be learned by practice of the invention. The advantages of the invention may be realized and obtained by means of the instrumentalities and combinations particularly pointed out hereinafter.
The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate embodiments of the invention, and together with the general description given above and the detailed description of the embodiments given below, serve to explain the principles of the invention.
The two-dimensional light deflector 100 is an optical device that deflects a collimated light beam two-dimensionally, and comprises a first deflector 110 that deflects the collimated light beam in a plane, for example, along a YZ-plane, a second deflector 150 that deflects the collimated light beam in another plane, for example, along an XY-plane, and a fixing member 180 directly fixing both the first deflector and the second deflector.
The fixing member 180 has two convex portions protruding upward from a base 182, a first deflector fixing stand 184 and a second deflector fixing stand 186. The first deflector fixing stand 184 has a first deflector fixing face 184a to which the first deflector 110 is fixed, the first deflector fixing face 184a being parallel to the ZX-plane. On the other hand, the second deflector fixing stand 186 has a second deflector fixing face 186a to which the second deflector 150 is fixed, the second deflector fixing face 186a being declined 45 degrees around the Z-axis with respect to the ZX-plane. Here, the expression 45 degrees includes a range in which a functional difference does not substantially occur.
The first deflector 110 comprises a light radiating portion 120 that generates and radiates a collimated light beam from light guided by an optical fiber 130, which is a light guide, and a cantilever 112 supporting the light radiating portion 120 oscillatably around the first axis A1 extending outside the light radiating portion 120. Although not shown, the first deflector 110 also includes a drive mechanism or a drive for oscillatably driving the cantilever 112. For driving the drive, any publicly-known drive such as an electromagnetic drive, an electrostatic drive, a piezoelectric drive, or the like may be adapted.
The cantilever 112 is fixed to the first deflector fixing face 184a of the first deflector fixing stand 184 of the fixing member 180 in a cantilever fashion. The first axis A1 extends through a fixed end 112a of the cantilever 112. The cantilever 112 has an extension 114 extending parallel to the first axis A1 near its free end 112b, and the light radiating portion 120 is provided at a distal end of the extension 114. The light radiating portion 120 radiates a collimated light beam towards the first axis A1 along the YZ-plane that is perpendicular to the first axis A1. Accordingly, the oscillation of the light radiating portion 120 around the first axis A1 causes deflection of the collimated light beam along the YZ-plane. Furthermore, the collimated light beam radiated from the light radiating portion 120 always passes through the first axis A1.
The second deflector 150 has an oscillatable reflecting face 152 that reflects the collimated light beam radiated from the light radiating portion 120. The reflecting face 152 is inclined by 45 degrees with respect to the ZX-plane including the first axis A1 at the time of non-oscillation. The reflecting face 152 is also inclined by 45 degrees with respect to the YZ-plane including a second axis A2 that coincides with a principal ray of the collimated light beam radiated from the light radiating portion 120 at the time of non-oscillation. Accordingly, the reflecting face 152 converts the deflection of the collimated light beam in the YZ-plane into a deflection of the collimated light beam along the XY-plane that is perpendicular to the second axis A2.
Furthermore, the reflecting face 152 is oscillatably supported around a third axis A3 passing through an intersection of the first axis A1 and the second axis A2, and perpendicular to both the first axis A1 and the second axis A2. Accordingly, the oscillation of the reflecting face 152 around the third axis A3 causes deflection of the collimated light beam along the XY-plane perpendicular to the third axis A3.
Therefore, the combination of the oscillation of the light radiating portion 120 around the first axis A1 and the oscillation of the reflecting face 152 around the third axis A3 deflects the collimated light beam two-dimensionally along the YZ-plane.
The second deflector 150 is configured by, for example, a MEMS deflector. The second deflector 150 configured by the MEMS deflector comprises a movable plate 154 provided with the reflecting face 152, a pair of hinges 156 supporting the movable plate 154 oscillatably around the third axis A3, and a pair of supports 158 supporting the hinges 156. The supports 158 are fixed to the second deflector fixing face 186a of the second deflector fixing stand 186 through a spacer 160. As a result, the movable plate 154 is oscillatably supported apart from the second deflector fixing face 186a. Although not shown, the second deflector 150 also comprises a drive mechanism or a drive for oscillatably driving the movable plate 154. For driving the drive, any publicly-known drive such as an electromagnetic drive, an electrostatic drive, a piezoelectric drive, or the like may be adapted. Since an actual MEMS deflector is provided with a drive, it is easily expected that the MEMS deflector is more complicated and larger than the illustrated configuration.
The second deflector 150 configured by the MEMS deflector is used as a high-speed scanning side in a raster scan. In high-speed scanning, adopting resonance driving, which can utilize a gain of a Q value, can further reduce power consumption. In addition, since a main material of the second deflector 150 is manufactured by MEMS technology, in many cases, a silicon substrate is used as the main material. However, for the hinges 156, a silicon compound such as silicon nitride, or an organic material such as polyimide may be adapted as well silicon. In addition, in the drawing, each hinge 156 has a straight shape, but may also be configured by a bending hinge or the like.
As shown in
As shown in
As shown in
The portion of the optical fiber 130 inserted into the cavity 116a of the cladding fixing portion 116 is a cladding 134 from which a jacket 138 and a coating portion 136 are stripped off of the optical fiber 130. Since the diameter of the coating portion 136 and the jacket 138 of the optical fiber 130 has a large tolerance, if the diameter of the cavity 116a is increased in accordance with the diameter of the coating portion 136 and the jacket 138, it would be difficult for the optical fiber 130 to be fixed while achieving good reproducibility of a light radiating direction from the optical fiber 130. On the other hand, since the tolerance of the diameter of the cladding 134 is smaller than that of the coating portion 136 and the jacket 138, the diameter of the cavity 116a can be appropriately designed; high reproducibility of the light radiating direction from the optical fiber 130 can be obtained.
As shown in
The collimating lens 122 is fixed directly to the optical fiber 130 as shown in, for example,
In
The cantilever 112 oscillates around the first axis A1 that is parallel to the X-axis and passes through the first deflector fixing face 184a. Since the first deflector fixing face 184a is at the same height as the oscillation axis of the reflecting face 152 of the second deflector 150, although a traveling direction of the collimated light beam reflected by the prism 124 changes in response to the oscillation of the cantilever 112, the collimated light beam reflected by the prism 124 always travels toward an intersection of the first axis A1 and the third axis A3. Subsequently, the collimated light beam is reflected frontward, that is, in the +X direction by the reflecting face 152 that is disposed at the intersection of the first axis A1 and the third axis A3. The collimated light beam reflected by the reflecting face 152 is deflected in the second plane by the oscillation of the light radiating portion 120, and is deflected in the third plane by the oscillation of the reflecting face 152.
Hereinafter, a deflection operation of the collimated light beam in the two-dimensional light deflector 100 will be explained in detail with reference to
The light radiating portion 120 is disposed on the first plane P1 in an oscillatable manner around the first axis A1. When oscillating, the light radiating portion 120 reciprocates in a predetermined angular range on a circumference having a constant radius from the first axis A1. Since the light radiating portion 120 radiates the collimated light beam toward the first axis A1 on the first plane P1, the collimated light beam radiated from the light radiating portion 120 always reaches an intersection of the first axis A1 and the first plane P1. The reflecting face 152 is disposed on the intersection of the first axis A1 and the first plane P1. The reflecting face 152 is disposed in an oscillatable manner around the third axis A3. The third axis A3 passes through the intersection of the first axis A1 and the first plane P1 and extends perpendicularly to both the first axis A1 and the second axis A2. The reflecting face 152 is inclined by 45 degrees with respect to the first plane P1 around the third axis A3 at the time of non-oscillation.
The collimated light beam radiated from the light radiating portion 120 at the time of non-oscillation travels along the second axis A2, falls on the reflecting face 152, and is reflected along the first axis A1 by the reflecting face 152 at the time of non-oscillation.
As shown in
Furthermore, as shown in
Accordingly, combining the oscillation of the light radiating portion 120 around the first axis A1 and the oscillation of the reflecting face 152 around the third axis A3 allows the collimated light beam reflected by the reflecting face 152 to be two-dimensionally scanned, as shown in
Now, a case in which a raster scan is performed using the two-dimensional light deflector 100 will be explained. Here, the first deflector 110 is adapted for a low-speed scan and the second deflector 150 is adapted for a high-speed scan. The collimated light beam radiated from the light radiating portion 120 and reflected by the reflecting face 152 is scanned in a low-speed scan SL direction shown in
Here, the third axis A3, which is the oscillation axis of the reflecting face 152 of the second deflector 150, is not exactly on the reflecting face 152 of the second deflector 150, but is located at the center of a cross-section of the hinges 156, so that there is an offset d between the third axis A3 and the reflecting face 152, as shown in
Although the two-dimensional light deflector 100 of the present embodiment is not configured in a manner that a deflector is mounted on another deflector as in the two-dimensional light deflector 500 of the conventional example disclosed in U.S. Pat. No. 4,838,632, a raster scan can be achieved with a substantially rectangular scanning surface in the same manner as the two-dimensional light deflector 500 of the conventional example. On the other hand, since the elements mounted on the cantilever 112 are only the optical fiber 130, the collimating lens 122, and the prism 124, which are compact and lightweight, the moment of inertia of the cantilever 112 is greatly reduced as compared to the two-dimensional light deflector 500 of the conventional example. Therefore, even when securing the same responsiveness as the two-dimensional light deflector 500 of the conventional example, the driving force required thereby is greatly reduced, so that the power consumption required for oscillation is greatly reduced. In addition, as the driving force is reduced, the volume required for driving is also reduced, which enables to achieve significant downsizing from the two-dimensional light deflector 500 of the conventional example.
In the first embodiment, the mechanism that oscillates the light radiating portion 120 is configured using the cantilever; however, in the present embodiment, the mechanism is configured using a movable plate.
A two-dimensional light deflector 200 comprises a first deflector 210 that deflects a collimated light beam in a plane, for example, along the YZ-plane, the second deflector 150 that deflects the collimated light beam in another plane, for example, along the XY-plane, and a fixing member 280 directly fixing both the first deflector and the second deflector.
The fixing member 280 includes two convex portions protruding upward from a base 282, a support 284 and a second deflector fixing stand 286. The second deflector fixing stand 286 has the same configuration as the second deflector fixing stand 186 of the first embodiment. In other words, a second deflector fixing face of the second deflector fixing stand 286 is inclined by 45 degrees with respect to the YZ-plane around a Z-axis. The second deflector 150 is as explained in the first embodiment.
The first deflector 210 comprises two torsion hinges 214 extending from the fixing member 280 along the first axis A1, an oscillation member 212 supported by the torsion hinges 214, and the light radiating portion 120 attached to the oscillation member 212. The configuration of the light radiating portion 120 is as explained in the first embodiment. Although not shown, the first deflector 210 also comprises a drive mechanism or a drive for oscillatably driving the oscillation member 212. For driving the drive, any publicly-known drive such as an electromagnetic drive, an electrostatic drive, a piezoelectric drive, or the like may be adapted.
One torsion hinge 214 extends from the support 284 of the fixing member 280 along the first axis A1, while the other torsion hinge 214 extends from the second deflector fixing stand 286 along the first axis A1. The two torsion hinges 214 are disposed coaxially so that their center axes are aligned with each other. The two torsion hinges 214 oscillatably support the oscillation member 212 around the first axis A1 with respect to the fixing member 280.
The oscillation member 212 has an extension 216 extending frontward, that is, in a +X direction parallel to the first axis A1, at the end on the upper side, that is, on a +Y direction side, and the light radiating portion 120 is provided at the distal end of the extension 216. As in the first embodiment, the extension 216 has a cladding fixing portion fixing a cladding of an optical fiber 130, which is a light guide. Although not shown, the cladding fixing portion provided in the extension 216 has the same structure as the cladding fixing portion 116 explained in the first embodiment.
The oscillation member 212 further has an adjusting extension 218 extending parallel to the first axis A1 in the backward direction, that is, in a −X direction, and parallel to the first axis A1 in a direction opposite to the extension 216, at the end on the lower side, that is, on the side in a −Y direction. The adjusting extension 218 has the same mechanical characteristics as the extension 216. The extension 216 and the adjusting extension 218 are symmetrically disposed with respect to a point on the first axis A1. That is, the extension 216 and the adjusting extension 218 are positioned on opposite sides with reference to the first axis A1, and extend in mutually opposite directions.
Since the adjusting extension 218 is also formed at the end of the oscillation member 212 on the side opposite to the side on which the light radiating portion 120 is provided in the above manner, the oscillation member 212 is configured to have the same moment of inertia on both sides thereof, with the center at the center axis of the torsion hinge 214.
In the two-dimensional light deflector 200 of the present embodiment, the oscillation axis of the first deflector 210 extends on the first axis A1, the oscillation axis of the reflecting face 152 of the second deflector 150 is located on the third axis A3, and the third axis A3 crosses through a point on the first axis A1 and extends perpendicular to the first axis A1.
Similar to the two-dimensional light deflector 100 of the first embodiment, in the two-dimensional light deflector 200 of the present embodiment, such configuration allows the collimated light beam radiated from the light radiating portion 120 to always fall on the reflecting face 152 of the second deflector 150 on its oscillation axis. The collimated light beam reflected by the reflecting face 152 of the second deflector 150 is deflected along the YZ-plane by the oscillation member 212 of the first deflector 210 oscillating around the first axis A1, and is deflected along the XY-plane by the reflecting face 152 of the second deflector 150 oscillating around the third axis A3.
In the same manner as in the two-dimensional light deflector 100 of the first embodiment, the two-dimensional light deflector 200 of the present embodiment can achieve a raster scan with a substantially rectangular scanning surface, in the same manner as in the two-dimensional light deflector 500 of the conventional example, in which a deflector is mounted on another deflector, disclosed in U.S. Pat. No. 4,838,632. On the other hand, since the elements mounted on the oscillation member 212 are only the optical fiber 130, the collimating lens 122, and the prism 124, which are compact and lightweight, the moment of inertia of the oscillating member 212 is greatly reduced as compared to the two-dimensional light deflector 500 of the conventional example. Therefore, even when securing the same responsiveness as the two-dimensional light deflector 500 of the conventional example, the driving force required thereby is greatly reduced, so that the power consumption required for oscillation is greatly reduced. In addition, as the driving force is reduced, the volume required for driving is also reduced, which enables to achieve significant downsizing from the two-dimensional light deflector 500 of the conventional example.
Furthermore, the two-dimensional light deflector 200 of the present embodiment has a configuration that is more robust against external forces than the two-dimensional light deflector 100 of the first embodiment. In the case where the first deflector 110 includes the cantilever 112 as in the first embodiment, strong vibration from the outside may cause unexpected oscillation of the collimated light beam from the optical fiber 130. On the contrary, in the present embodiment, since the oscillation member 212 is balanced with the same moment of inertia on both sides, with the torsion hinge 214 at the center, it is difficult for unexpected oscillation to occur due to external vibration. Therefore, the two-dimensional light deflector 200 according to the present embodiment, in which the first deflector 210 includes the oscillation member 212, has a configuration with higher robustness against external forces as compared to the two-dimensional light deflector 100 of the first embodiment, in which the first deflector 110 includes the cantilever 112.
A two-dimensional light deflector 300 of the present embodiment comprises a galvano deflector 312 in the same manner as the two-dimensional light deflector 500 of the conventional example disclosed in U.S. Pat. No. 4,838,632. However, the second deflector 150 is not mounted on the galvano deflector 312.
The two-dimensional light deflector 300 comprises a first deflector 310 that deflects a collimated light beam in a plane, for example, along the YZ-plane, the second deflector 150 that deflects the collimated light beam in another plane, for example, along the XY-plane, and a fixing member 380 directly fixing both the first deflector and the second deflector.
The fixing member 380 includes two convex portions protruding upward from a base 382, a first deflector fixing stand 384 and a second deflector fixing stand 386. The second deflector fixing stand 386 has the same configuration as the second deflector fixing stand 186 of the first embodiment. That is, a second deflector fixing face of the second deflector fixing stand 386 is inclined by 45 degrees with respect to the YZ-plane around the Z-axis. The second deflector 150 is as explained in the first embodiment.
The first deflector 310 comprises the galvano deflector 312 fixed to the first deflector fixing stand 384. The galvano deflector 312 has a rotating shaft 312a that is oscillatable around the first axis A1. The first deflector 310 further comprises an optical fiber fixing jig 314 fixing an optical fiber, which is a light guide attached to the rotating shaft 312a of the galvano deflector 312, and the light radiating portion 120 provided on the optical fiber fixing jig 314.
The optical fiber fixing jig 314 has an extension 316 extending parallel to the first axis A1. The light radiating portion 120 is provided at a distal end of the extension 316. The light radiating portion 120 includes the optical fiber 130 inserted and fixed in a through hole formed at the distal end of the extension 316, and the collimating lens 122 provided at a distal end of the optical fiber 130.
Although not shown in detail in
The optical fiber fixing jig 314 further has an adjusting extension 318 on a portion opposite to the extension 316 with reference to the first axis A1. The adjusting extension 318 has the same mechanical characteristics as the extension 316, for example, the weight, and is designed so that the moment of inertia is balanced with the center at an oscillation axis. The adjusting extension 318 may be of course adjusted in the moment of inertia by changing the thickness.
The second deflector 150 is disposed so that the oscillation axis of the reflecting face 152 crosses through a point on the first axis A1. Therefore, the collimated light beam radiated from the optical fiber 130 is configured to falls on an intersection point of the oscillation axis of the galvano deflector 312 and the oscillation axis of the second deflector 150. Although a direction in which the collimated light beam falls on the reflecting face 152 of the second deflector 150 varies depending on the oscillation of the galvano deflector 312, a position on the reflecting face 152 of the second deflector 150 on which the collimated light beam falls does not change. The collimated light beam reflected by the reflecting face 152 of the second deflector 150 is deflected along the ZX-plane by the first deflector 310, that is, by an oscillation of the optical fiber fixing jig 314, and is deflected along an XY-plane by the second deflector 150, that is, by an oscillation of the reflecting face 152. Therefore, combining these oscillations allows the collimated light beam reflected by the reflecting face 152 of the second deflector 150 to be two-dimensionally scanned. Here, the galvano deflector 312 is adapted for a low-speed scan and the second deflector 150 is adapted for a high-speed scan, which achieves a favorable raster scan.
With the above configuration, in the same manner as the first and second embodiments, a raster scan with a substantially rectangular scanning surface can be achieved in the same manner as the two-dimensional light deflector 500 of the conventional example, in which a deflector is mounted on another deflector, disclosed in U.S. Pat. No. 4,838,632. On the other hand, since the elements mounted on the galvano deflector 312 are only the optical fiber fixing jig 314, the optical fiber 130, and the collimating lens 122, which are small and lightweight, the moment of inertia applied to the rotating shaft 312a of the galvano deflector 312 is greatly reduced as compared to the two-dimensional light deflector 500 of the conventional example. Therefore, even when securing the same responsiveness as the two-dimensional light deflector 500 of the conventional example, the driving force required thereby is greatly reduced, so that the power consumption required for oscillation is greatly reduced.
The configuration of the two-dimensional light deflector 300 according to the present embodiment is close to the configuration of the conventional two-dimensional light deflector 500 of the conventional example, in which a second deflector is disposed on a galvano deflector. Furthermore, the galvano deflector 312 is generally commercially available, and it is easy to switch from the configuration in which the second deflector is disposed on the galvano deflector.
A two-dimensional light deflector 300A of the present modified example is provided with a first deflector 310A instead of the first deflector 310 shown in
In the two-dimensional light deflector 300A of the present modified example, the optical fiber fixing jig 314A has an extension 316A extending parallel to the first axis A1. A light radiating portion 120 is provided at a distal end of the extension 316A.
Although not shown in detail in
The light radiating portion 120 comprises the collimating lens 122 that shapes light radiated from the optical fiber 130 into a collimated light beam, and the prism 124 that deflects the collimated light beam radiated from the collimating lens 122 along the first axis A1 toward a reflecting face along the second axis A2. The light radiating portion 120 is configured in the same manner as in the first embodiment.
In the two-dimensional light deflector 300A of the present modified example, the cavity 316a for installing the optical fiber 130 is longer than that of the two-dimensional light deflector 300 shown in
Additional advantages and modifications will readily occur to those skilled in the art. Therefore, the invention in its broader aspects is not limited to the specific details and representative embodiments shown and described herein. Accordingly, various modifications may be made without departing from the spirit or scope of the general inventive concept as defined by the appended claims and their equivalents.
This application is a Continuation Application of PCT Application No. PCT/JP2016/063665, filed May 6, 2016, the entire contents of which are incorporated herein by reference.
Number | Date | Country | |
---|---|---|---|
Parent | PCT/JP2016/063665 | May 2016 | US |
Child | 16179243 | US |