Optical Device
20220320831 ยท 2022-10-06
Inventors
- Takuma Tsurugaya (Tokyo, JP)
- Takuro Fujii (Tokyo, JP)
- Takaaki Kakitsuka (Tokyo, JP)
- Shinji Matsuo (Tokyo, JP)
Cpc classification
H01S5/0422
ELECTRICITY
H01S5/32
ELECTRICITY
International classification
Abstract
An active region formed on a substrate, and a p-type region and an n-type region formed so as to sandwich the active region are provided. The p-type region and the n-type region are formed so as to sandwich the active region. Both edges of a first side being a side of the p-type region and facing a first side surface of the active region are rounded in a direction separating from the active region. Also, both edges of a second side being a side of the n-type region and facing a second side surface of the active region are rounded in a direction separating from the active region.
Claims
1-6. (canceled)
7. An optical device, comprising: an active region on a substrate; and a p-type region and an n-type region on the substrate and sandwiching the active region, wherein edges of a first side of the p-type region are rounded in a direction separating from the active region in a planar view, the first side of the p-type region facing the active region, and wherein edges of a second side of the n-type region are rounded in a direction separating from the active region in the planar view, the second side of the n-type region facing the active region.
8. The optical device according to claim 7, wherein: the first side and a third side of the p-type region are connected by a curve in the planar view; the first side and a fourth side of the p-type region are connected by a curve in the planar view, the third side and the fourth side sandwiching the first side and facing each other; the second side and a fifth side of the n-type region are connected by a curve in the planar view; and the second side and a sixth side of the n-type region are connected by a curve in the planar view, the fifth side and the sixth side sandwiching the second side and facing each other.
9. The optical device according to claim 7, wherein: the first side of the p-type region is in contact with the active region; and the second side of the n-type region is in contact with the active region.
10. The optical device according to claim 7, further comprising a resonator.
11. An optical device, comprising: an active region on a substrate; and a p-type region and an n-type region on the substrate and sandwiching the active region, wherein edges of a first side surface of the active region are rounded in a direction separating from the p-type region in a planar view, the first side surface of the active region facing the p-type region, and wherein edges of a second side surface of the active region are rounded in a direction separating from the n-type region in the planar view, the second side surface of the active region facing the n-type region.
12. The optical device according to claim 1, wherein the active region is ovular in planar view.
13. The optical device according to claim 11, wherein: a surface of the p-type region facing the active region is in contact with the active region; and a surface of the n-type region facing the active region is in contact with the active region.
14. The optical device according to claim ii, further comprising a resonator.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0025]
[0026]
[0027]
[0028]
[0029]
[0030]
[0031]
[0032]
[0033]
[0034]
[0035]
[0036]
DETAILED DESCRIPTION OF ILLUSTRATIVE EMBODIMENTS
[0037] Hereinafter, optical devices according to embodiments of the present disclosure will be described.
First Embodiment
[0038] First, an optical device according to a first embodiment of the present disclosure will be described with reference to
[0039] The substrate 101 is, for example, a well-known photonic crystal, and is composed of, for example, a semiconductor such as InP. The active region 102 is embedded in a line defect waveguide of the photonic crystal, for example. Additionally, the p-type region 103 is a region in which impurities that become p-type are introduced into the photonic crystal by a thermal diffusion method, an ion implantation method, or the like. Furthermore, the n-type region 104 is a region in which impurities that become n-type are introduced into the photonic crystal by a thermal diffusion method, an ion implantation method, or the like.
[0040] Hereinafter, shapes in planar view of the active region 102, the p-type region 103, and the n-type region 104 of the optical device according to the first embodiment will be described in more detail. The active region 102 has a first side surface 105 and a second side surface 106 and is formed in a rectangular shape. In the first embodiment, the first side surface 105 and the second side surface 106 are formed along a waveguide direction. Additionally, the p-type region 103 and the n-type region 104 are formed so as to sandwich the active region 102 in directions of the first side surface 105 and the second side surface 106. Additionally, in this example, a surface, of the p-type region 103, facing the active region 102 (first side surface io5) is formed in contact with the active region 102 (first side surface 105). In addition, a surface, of the n-type region 104, facing the active region 102 (second side surface 106) is formed in contact with the active region 102 (second side surface 106).
[0041] Also, both edges of a first side 107 being a side of the p-type region 103 and facing the active region 102 are rounded in a direction separating from the active region 102. Also, both edges of a second side 108 being a side of the n-type region 104 and facing the active region 102 are rounded in a direction separating from the active region 102.
[0042] Here, in the p-type region 103, two sides being a third side 131 and a fourth side 133, sandwiching the first side 107, and facing each other are inclined in directions in which a width between the two sides increases as the two sides separate farther from the first side 107. In other words, each of an angle formed by the first side 107 and the third side 131, and an angle formed by the first side 107 and the fourth side 133 is an obtuse angle. The first side 107 and the third side 131 of the p-type region 103 configured in this manner are connected by a curve 132, and the first side 107 and the fourth side 133 of the p-type region 103 configured in this manner are connected by a curve 134. In other words, the p-type region 103 has a substantially trapezoidal shape in which an upper base having a shorter length serves as the first side 107, and the third side 131 and the fourth side 133 serve as legs.
[0043] In addition, in the n-type region 104, two sides being a fifth side 141 and a sixth side 143, facing each other, and sandwiching the second side 108 are inclined in directions in which a width between the two sides increases as the two sides separate farther from the second side 108. In other words, each of an angle formed by the second side 108 and the fifth side 141, and an angle formed by the second side 108 and the sixth side 143 is an obtuse angle. The second side 108 and the fifth side 141 of the n-type region 104 configured in this manner are connected by a curve 142, and the second side 108 and the sixth side 143 of the n-type region 104 configured in this manner are connected by a curve 144. In other words, the n-type region 104 has a substantially trapezoidal shape in which an upper base having a shorter length serves as the second side 108, and the fifth side 141 and the sixth side 143 serve as legs.
[0044] Incidentally, in the description described above, the shape of the p-type region 103 and the shape of the n-type region 104 are symmetrical with respect to each other, but these are not necessarily symmetrical. For example, as illustrated in
[0045] Here, in the p-type region 103a, two sides being a third side 131a and a fourth side 133a, sandwiching the first side 1o7a, and facing each other are inclined in directions in which a width between the two sides increases as the two sides separate farther from the first side 107a. In other words, each of an angle formed by the first side 107a and the third side 131a, and an angle formed by the first side 107a and the fourth side 133a is an obtuse angle. The first side 107a and the third side 131a of the p-type region io3a configured in this manner are connected by a curve 132a, and the first side 107a and the fourth side 133a of the p-type region 103a configured in this manner are connected by a curve 134a. In other words, the p-type region 103a has a substantially trapezoidal shape in which an upper base having a shorter length serves as the first side 107a, and the third side 131a and the fourth side 133a serve as legs.
[0046] For example, as is well known, a resist pattern having an opening at a position to be formed with the p-type region 103 is formed on the substrate 101 by a well-known lithographic technique, and ion implantation can be selectively performed by using this resist pattern as a mask to form the p-type region 103. In addition, a p-type layer containing a high concentration of p-type impurities can be formed at the position to be formed with the p-type region 103 on the substrate 101 by a well-known lithographic technique, and thus, the p-type region 103 can be formed by thermal diffusion. The same applies to the n-type region.
[0047] In the design stage of the mask to be used in the lithographic technique described above, each of the p-type region 103 and the n-type region 104 having the shape described above can be formed, in consideration of the effect of dopant diffusion by thermal diffusion or ion implantation, by reducing the opening of the resist pattern inward from the final shape by the amount of the diffusion.
[0048] Next, in the optical device according to the first embodiment, a simulation result of an electron current distribution when a bias voltage of 1.2 V was applied to the p-type region 103 and the n-type region 104 is illustrated in
[0049] As illustrated in
[0050] Incidentally, concerning a well-known photonic crystal laser, wavelength-scale light confinement is possible, so a length in a waveguide direction of an active region can be shortened to several hundreds nm that is substantially the same degree as a width of the active region. For example, in NPLs 2 and 3, a structure in which an active region is embedded in a line defect waveguide of a two-dimensional photonic crystal is used. In this structure, it is conceivable that in order to achieve reduction of a resistance value in a p-type region and an n-type region, each of the p-type region and the n-type region is formed in a waveguide direction of a line defect waveguide region that does not have holes, that is, the active region, rather than a region having holes of the photonic crystal. In a case of such a configuration, when the configuration according to the first embodiment is applied, a similar effect to that described above can be achieved.
Second Embodiment
[0051] Next, an optical device according to a second embodiment of the present disclosure will be described with reference to
[0052] The substrate 201 is, for example, a well-known photonic crystal, and is composed of, for example, a semiconductor such as InP. The active region 202 is embedded in a line defect waveguide of the photonic crystal, for example. Additionally, the p-type region 203 is a region in which impurities that become p-type are introduced into the photonic crystal by a thermal diffusion method, an ion implantation method, or the like. Furthermore, the n-type region 204 is a region in which impurities that become n-type are introduced into the photonic crystal by a thermal diffusion method, an ion implantation method, or the like.
[0053] Hereinafter, shapes in planar view of the active region 202, the p-type region 203, and the n-type region 204 of the optical device according to the second embodiment will be described in more detail.
[0054] The active region 202 has a first side surface 205 and a second side surface 206, and is formed in a rectangular shape. In the second embodiment, the first side surface 205 and the second side surface 206 are formed along a waveguide direction. Additionally, the p-type region 203 and the n-type region 204 are formed so as to sandwich the active region 202 in directions of the first side surface 205 and the second side surface 206. Additionally, in this example, a surface, of the p-type region 203, facing the active region 202 (first side surface 205) is formed in contact with the active region 202, and a surface, of the n-type region 204, facing the active region 202 (second side surface 206) is formed in contact with the active region 202.
[0055] In addition, in the optical device according to the second embodiment, both edges of the first side surface 205 and the second side surface 206 being side surfaces of the active region 202 and respectively facing the p-type region 203 and the n-type region 204 are rounded respectively in directions separating from the p-type region 203 and the n-type region 204. For example, the active region 202 is oval in planar view. The active region 202 having such a shape can be implemented by making a mask shape of a photomask that is used in lithography for forming the active region 202 similar to the shape to be fabricated.
[0056] Note that in this example, a surface, of the p-type region 203, facing the active region 202 (first side surface 205) is formed in contact with the active region 202, and a surface, of the n-type region 204, facing the active region 202 (second side surface 206) is formed in contact with the active region 202. In addition, in the second embodiment, the p-type region 203 has a substantially trapezoidal shape in which a side facing the active region 202 serves as an upper base having a shorter length, and two sides connected to the side serve as legs. The same applies to the n-type region 204.
[0057] Typically, a rectangular active region in planar view is used, but in the second embodiment, shapes of edge portions in a waveguide direction are curves rather than straight lines, and these curves are smoothly connected with straight lines of the side surfaces along the waveguide direction. A specific shape of the curve may be an arc in planar view, and it is only required that the shape is a smooth curve so as not to generate an indifferentiable portion (that is, a corner) in an outline of the active region 202. Note that the p-type region 203 and the n-type region 204 can have a shape in which the edge portions at the active region 202 side have corners.
[0058] In addition, as illustrated in
[0059] According to the second embodiment, there are no corners in the shape of the active region 202 in planar view, so the edge effect is suppressed. In addition, the current concentration on the entire sides, at the active region 202 side, of the p-type region 203 and the n-type region 204 can be achieved to more effectively inject a current.
[0060] Incidentally, concerning a well-known photonic crystal laser, wavelength-scale light confinement is possible, so a length in the waveguide direction of an active region can be shortened to several hundreds nm that is substantially the same degree as a width of the active region. For example, in NPLs 2 and 3, a structure in which an active region is embedded in a line defect waveguide of a two-dimensional photonic crystal is used. In this structure, it is conceivable that in order to achieve reduction of a resistance value in a p-type region and an n-type region, each of the p-type region and the n-type region is formed in a waveguide direction of a line defect waveguide region that does not have holes, that is, the active region, rather than a region having holes of the photonic crystal. In a case of such a configuration, when the configuration according to the second embodiment is applied, a similar effect to that described above can be achieved.
[0061] As described above, in the present disclosure, both edges of the first side being a side of the p-type region and facing the active region are rounded in the direction separating from the active region, and both edges of the second side being a side of the n-type region and facing the active region are rounded in the direction separating from the active region. Additionally, in the present disclosure, both edges of the first side surface and the second side surface being side surfaces of the active region and respectively facing the p-type region and the n-type region are rounded respectively in the directions separating from the p-type region and the n-type region. As a result, according to the present disclosure, the edge effect that is generated at the edge portions of the active region can be suppressed.
[0062] The present disclosure focuses on the mechanism of laser performance degradation to which attention has not been paid, and that is referred to as the edge effect derived from the shape of the active region. The present disclosure achieves elimination of the non-uniformity of a current density distribution and reduction in leakage current in the periphery of the active region by appropriately controlling the shape of the p-type region and the shape of the n-type region near the active region, and the shape of the active region in order to resolve the laser performance degradation.
[0063] The present disclosure is not limited to the embodiments described above, and it is obvious that many modifications and combinations can be implemented by a person having ordinary knowledge in the field within the technical spirit of the present disclosure.
REFERENCE SIGNS LIST
[0064] 101 Substrate
[0065] 102 Active region
[0066] 103 p-type region
[0067] 104 n-type region
[0068] 105 First side surface
[0069] 106 Second side surface
[0070] 107 First side
[0071] 108 Second side
[0072] 131 Third side
[0073] 132 Curve
[0074] 133 Fourth side
[0075] 134 Curve
[0076] 141 Fifth side
[0077] 142 Curve
[0078] 143 Sixth side
[0079] 144 Curve.