WO2024247268A1 - Optical circuit - Google Patents
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- WO2024247268A1 WO2024247268A1 PCT/JP2023/020700 JP2023020700W WO2024247268A1 WO 2024247268 A1 WO2024247268 A1 WO 2024247268A1 JP 2023020700 W JP2023020700 W JP 2023020700W WO 2024247268 A1 WO2024247268 A1 WO 2024247268A1
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/03—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect
- G02F1/035—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on ceramics or electro-optical crystals, e.g. exhibiting Pockels effect or Kerr effect in an optical waveguide structure
Definitions
- the present invention relates to optical circuits, and more specifically to the structure of optical circuits that include ferroelectric thin films.
- the LN optical modulator is an optical modulator that utilizes the refractive index change caused by the Pockels effect of LiNbO 3 (hereinafter referred to as LN) crystal, and is one of the core devices for optical communication. It is used as an external modulator to modulate CW light from DFB lasers and the like, and is capable of high-speed modulation exceeding 100 GHz. It is also expected to be used as an optical modulator in optical modules such as the high-bandwidth coherent driver modulator (HB-CDM) proposed by OIF (The Optical Internetworking Forum). In order to achieve smaller size and lower cost, an optical modulator with a thin film LN attached onto a Si waveguide is expected due to its high efficiency and wide bandwidth.
- HB-CDM high-bandwidth coherent driver modulator
- FIG. 1 is a schematic diagram showing the configuration of an LN thin film SiPh hybrid optical modulator (Non-Patent Document 1).
- the optical modulator 700 has a hybrid configuration of an LN thin film and a SiPh circuit, in which an LN thin film 12 is attached to a silicon photonic (SiPh) circuit in which a SiO 2 layer and a core layer are formed on a Si substrate 10.
- SiPh silicon photonic
- a Mach-Zehnder interferometer (MZI) including two interference optical waveguides 21 is formed by the branched core layer.
- a high-frequency electrode 22 is further formed on the upper surface of the LN thin film 12 so as to sandwich each of the interference waveguides 21.
- MZI Mach-Zehnder interferometer
- the core, the surrounding SiO 2 cladding, and the LN thin film 12 adjacent to the core function together as an optical waveguide. Light is not only confined by the core, but also seeps into the LN and propagates, functioning as a composite optical waveguide in which the ferroelectric material LN and the Si core are integrated.
- the interference conditions of the MZI change and the combined optical output of the two interference optical waveguides is turned on and off.
- optical modules including optical modulators can be significantly miniaturized and made more efficient.
- the optical modulator with the LN thin film attached to the SiPh circuit shown in FIG. 1 has problems in manufacturability and assembly.
- the modulation electrode 22, to which an electric signal for refractive index modulation is applied, is formed on the LN thin film 12.
- the process of attaching the LN thin film to the SiPh circuit must be performed as an independent process after the photolithography for fabricating the SiPh circuit is completed.
- the photolithography process must be performed twice to form the high-frequency electrode 22.
- This manufacturing process of the optical modulator is complicated and expensive.
- the height of the PAD relative to the other electrodes fabricated in the SiPh circuit process differs from the height of the PAD relative to the modulation electrode 22.
- flip-chip mounting for miniaturization cannot be performed in the later process of assembling the fabricated optical modulator chip into an optical module, etc.
- the present invention was made in consideration of the above-mentioned problems, and provides an optical circuit configuration that combines a ferroelectric thin film and a SiPh circuit with improved manufacturability and mountability.
- One embodiment of the present invention is an optical circuit in which a silicon substrate, a cladding layer, and a ferroelectric thin film are arranged in that order, the optical circuit having a core formed within the cladding layer and one or more electrodes formed along the core for applying an electric field to the ferroelectric thin film.
- the present invention provides an optical circuit that combines a ferroelectric thin film and a SiPh circuit with improved manufacturability and mountability.
- FIG. 1 is a schematic diagram showing the configuration of an LN thin-SiPh hybrid optical modulator.
- FIG. 1 is a diagram illustrating a schematic configuration of a hybrid optical modulator according to a related art.
- 1A and 1B are diagrams illustrating the top and side cross-sectional configurations of an optical circuit according to a first embodiment.
- 11A and 11B are diagrams illustrating the top and side cross-sectional configurations of an optical circuit according to a second embodiment of the present invention.
- FIG. 1 shows the configuration of a mode converter between a SiN core and a Si core.
- 11A and 11B are diagrams illustrating the top and side cross-sectional configurations of an optical circuit according to a third embodiment.
- 11A and 11B are diagrams illustrating the top and side cross-sectional configurations of an optical circuit according to a fourth embodiment.
- 13A and 13B are diagrams illustrating the top and side cross-sectional configurations of an optical circuit according to a fifth embodiment.
- 13A and 13B are diagrams illustrating the top and side cross-sectional configurations of an optical circuit according to a sixth embodiment.
- the optical circuit disclosed herein provides a novel configuration that combines a ferroelectric thin film and a SiPh circuit, with improved manufacturability and mountability.
- a novel configuration suitable for an LN-Si hybrid optical modulator is presented. Electrodes to which an electrical signal that modulates the refractive index of the LN thin film is applied are formed in the SiPh circuit. All electrodes in the optical circuit are formed during the fabrication process of the SiPh circuit, so no additional photolithography is required after attaching the LN thin film. It becomes possible to fabricate high-frequency electrodes and other electrodes such as for bias at the same height, and the fabricated optical modulator chip can be flip-chip mounted in a later process. It improves the manufacturability and mountability of devices that utilize the electro-optical effect of LN, including optical modulators.
- a hybrid optical modulator refers to a Mach-Zehnder type modulator (MZM) that combines an LN thin film and a SiPh circuit.
- MZM Mach-Zehnder type modulator
- All drawings of the optical circuit structure described below are schematic diagrams, and the scales in each direction are not consistent.
- the substrate thickness direction (z direction) is shown significantly enlarged. Please also note that the relative relationships of the height, width, etc. of each element are not necessarily accurately expressed between different elements.
- the optical circuit of the present disclosure will be described as an example in which it is applied to a hybrid optical modulator.
- the configuration of the optical circuit of the present disclosure can also be applied to other optical circuits in which a ferroelectric thin film is attached to a SiPh circuit.
- Ferroelectric materials are not limited to lithium niobate (LN) and include lithium tantalate (LT) and barium titanate, as long as they are capable of changing the refractive index of the optical waveguide by the electro-optic effect.
- optical devices that utilize the refractive index modulation of the ferroelectric thin film near the core can include, in addition to optical modulators, polarization controllers and phase shifters that can be used to compensate for polarization mode dispersion.
- FIG. 2 is a diagram showing a schematic configuration of a hybrid optical modulator of the prior art.
- FIG. 2(a) is a top view of the Si substrate surface (x-y surface) of the SiPh circuit
- FIG. 2(b) is a side cross-sectional view (y-z surface) cut perpendicular to the substrate surface and the light traveling direction through line IIb-IIb
- FIG. 2(c) is a side cross-sectional view cut perpendicular to the substrate surface and the light traveling direction through line IIc-IIc.
- the SiPh circuit in the optical modulator 700 includes a SiO 2 layer 11 formed on a Si substrate 10 and a rectangular Si core 12.
- the SiPh circuit includes, for example, an electrode 23 formed inside SiO 2 functioning as a cladding layer.
- the electrode 23 may be a high-frequency electrode through which a modulation signal of the optical modulator is propagated, or may be an electrode for other circuits such as an electric circuit integrated with the optical modulator.
- the electrode 23 is a schematic diagram showing a configuration different from that of the modulation electrode 22, and the position on the upper surface of the optical circuit 700 does not matter. The position in the height direction on the cross-sectional view is also not limited to one shown in FIG. 2(c).
- This SiPh circuit can be fabricated by forming each layer on a Si substrate and patterning the core and electrodes by photolithography.
- the SiPh circuit can also be formed by processing an SOI (Silicon On Insulator) substrate on which a Si layer and a SiO 2 layer functioning as a core are formed in advance.
- SOI Silicon On Insulator
- the LN thin film 12 is attached on the SiPh circuit.
- the attachment of the LN thin film is performed by activating the surface layer of the LN thin film and the SiO2 layer, which are formed in advance to the size of the required area, with an argon beam, and then contacting them and applying pressure and heat. Since the LN thin film 12 is formed by bonding the LN thin film in this way, a physical attachment process other than the Si photolithography process is essential.
- gold electrodes 22a and 22b for modulation are formed on the LN thin film 12.
- PADs 24a and 24b for connection are formed.
- a second photolithography process is required after attaching the LN thin film 12, so the manufacturing process of the optical modulator 700 becomes complicated and the cost increases.
- the height of the modulation electrodes 22a, 22b is different from the height of the electrode 23 of the SiPh circuit.
- the electrode heights are different, high-density mounting technology using a ball grid array (BGA) cannot be used.
- BGA ball grid array
- the inability to use the powerful BGA technology is a major obstacle to miniaturization of optical modules and optical transmission devices.
- the optical circuit disclosed herein solves the problems of manufacturability and mountability shown in the above-mentioned optical modulator 700.
- FIG. 3 is a diagram showing the configuration of the top surface and the side cross section of the optical circuit of the first embodiment.
- the configuration of a hybrid optical modulator is shown.
- FIG. 3(a) is a top view of the SiPh circuit looking at the Si substrate surface (x-y surface)
- FIG. 3(b) is a side cross section (x-y surface) cut perpendicularly to the substrate surface and the light traveling direction along line IIIb-IIIb
- FIG. 3(c) is a side cross section (x-y surface) cut perpendicularly to line IIIc-IIIc to the substrate surface and the light traveling direction in the MZ type optical modulator.
- FIG. 3(a) is a top view of the SiPh circuit looking at the Si substrate surface (x-y surface)
- FIG. 3(b) is a side cross section (x-y surface) cut perpendicularly to the substrate surface and the light traveling direction along line IIIb-IIIb
- FIG. 3(c) is a side cross section (
- FIG. 3 shows a schematic diagram of a portion of one optical waveguide 31 of two interference optical waveguides in an MZ type optical modulator, which includes modulation electrodes 30a and 30b and functions as a refractive index modulation region.
- the configuration of the core 31 of the optical waveguide is the same as the core 21 of the optical circuit 700 of the conventional technology shown in FIG. 2. In the following, the differences from the optical circuit 700 of the conventional technology will be described.
- the optical circuit 100 differs from the conventional configuration in that the modulation electrodes 30a, 30b are formed in the SiO2 cladding area in a plane perpendicular to the substrate of the SiPh circuit, and are formed on the LN thin film outside the SiPh circuit.
- the PADs 34a, 34b connected to the modulation electrodes 30a, 30b do not contribute to the refractive index modulation of the LN thin film and are not included in the refractive index modulation area.
- the modulation electrodes 30a, 30b have PADs 34a, 34b at both ends through vias (VIA), and the PADs are connected to an electric circuit that supplies an electric signal, an electric signal source, etc. by some means.
- the modulation electrodes are high-frequency electrodes to which high-frequency electric signals are applied.
- PADs 34a and 34b are shown as being generally adjacent to the LN thin film 12.
- the modulation electrodes 30a and 30b may be extended, and the PADs may be formed at positions away from the region of the LN thin film 12. Please note that the positions of PADs 34a and 34b in FIG. 3 are just an example.
- the modulation electrodes 30a, 30b are formed in the SiO2 clad region in a plane perpendicular to the substrate of the SiPh circuit, the modulation electrodes are fabricated in the same photolithography process as all other electrodes of the SiPh circuit. No additional photolithography process is required after the attachment process of the LN thin film 12 as in the conventional technology. Furthermore, it is possible to form the PADs of all electrodes, including the modulation electrodes, to the same height. Therefore, flip chip mounting using BGA or bumps is possible.
- the optical circuit of the present invention can therefore be implemented as an optical circuit in which a silicon substrate 10, a cladding layer 11, and a ferroelectric thin film 12 are arranged in that order, with a core 31 formed within the cladding layer, and one or more electrodes 30a, 30b formed along the core for applying an electric field to the ferroelectric thin film.
- the modulating electrodes 30a, 30b are shown to have the same bottom height as the Si core 31 in the substrate thickness direction (z direction), but are not limited to this. As long as the modulating electrodes 30a, 30b are formed in the area of the SiO2 layer 11 in a plane perpendicular to the substrate of the SiPh circuit, the modulating electrodes are fabricated in the same photolithography process as all other electrodes of the SiPh circuit. Electrodes other than the modulating electrodes may be fabricated at different heights.
- FIG. 4 is a diagram showing the top and side cross-sectional configurations of the optical circuit of the second embodiment.
- the configuration of a hybrid optical modulator is shown.
- FIG. 4(a) is a top view of the Si substrate surface (xy plane) of the SiPh circuit
- FIG. 4(b) is a side cross-sectional view (xy plane) cut along line IVb-IVb
- FIG. 4(c) is a side cross-sectional view (xy plane) cut along line IVc-IVc perpendicular to the substrate surface and the light traveling direction.
- FIG. 4(a) is a top view of the Si substrate surface (xy plane) of the SiPh circuit
- FIG. 4(b) is a side cross-sectional view (xy plane) cut along line IVb-IVb
- FIG. 4(c) is a side cross-sectional view (xy plane) cut along line IVc-IVc perpendicular to the substrate surface and the light traveling direction.
- FIG. 4 shows a schematic diagram of a portion of one optical waveguide 32 of two interference optical waveguides in an MZ type optical modulator 200, which includes modulation electrodes 30a and 30b and functions as a refractive index modulation region.
- the differences from the optical circuit 100 of the first embodiment are as follows.
- the optical waveguide in which the refractive index is modulated is composed of the Si core 31, the surrounding SiO 2 clad, and the LN thin film 12 adjacent to the core in the refractive index modulation region, forming a composite waveguide.
- the Si core 31 also constitutes a continuous optical waveguide together with the surrounding SiO 2 clad through the inside and outside of the refractive index modulation region having a hybrid configuration with the LN thin film.
- the optical waveguide in which the refractive index is changed by an electric signal is composed of a silicon nitride (SiN) core 32 that is closer to the LN thin film 12 than the Si core.
- the optical waveguide is composed of the Si core 31, which is separate from the SiN core.
- the SiN core 32 can be formed at a higher position than the Si core 31 and closer to the LN thin film 12. Therefore, the refractive index modulation of the LN thin film 12 by an electric signal can be efficiently realized.
- the SiN core 32 and the Si core 31 having different heights can be optically connected by the mode converter 40 formed near the boundary of the LN thin film 12 in FIG.
- FIG. 5 is a diagram showing the configuration of a mode converter between a SiN core and a Si core.
- FIG. 5(a) is a top view of the Si substrate surface (xy surface) of the optical circuit 200, showing only two types of cores 32 and 31 near the mode converter 40.
- FIG. 5(b) is a side cross-sectional view (xz surface) of the mode converter 40, cut along the substrate surface and the light traveling direction through the center line (Vb-Vb line) of the core.
- the mode converter 40 has a first taper at the tip of the SiN core 32, in which the core width gradually narrows, and a second taper at the tip of the Si core 31, in which the core width gradually widens. Referring to FIG.
- the mode converter is not limited to the one shown in FIG. 5, and can be realized by other configurations as long as it is capable of converting the mode of light.
- the mode converter 40 is shown near the end of the LN thin film 12, but it may be located within the LN thin film 12 region or outside the LN region 12 region.
- the position of the mode converter 40 is not important as long as the SiN core 32 can produce a sufficient electro-optic effect (e.g., a change in refractive index) with the adjacent modulation electrodes 30a, 30b.
- the optical circuit of the present invention can therefore be implemented as a core that includes a first core 32 of silicon nitride formed on the side of the ferroelectric thin film 12 in the thickness direction (z direction) of the substrate in the region where the ferroelectric thin film 12 is formed on the substrate surface (x-y plane), and a second core 31 of silicon formed on the side of the substrate closer to the first core in the thickness direction, and the first core and second core are optically coupled.
- an additional photolithography process is not required after the process of attaching the LN thin film 12, and it is possible to form the PADs of all electrodes, including the modulation electrodes, to the same height.
- the SiN core in the refractive index modulation region where the LN thin film is attached can also be formed within the series of manufacturing processes for the SiPh circuit. Since the SiN core 32 and the LN thin film 12 can be placed close to each other, applying the configuration of the optical circuit 200 to an optical modulator can efficiently generate refractive index modulation.
- the modulating electrodes 30a, 30b are shown as being located between the SiN core 32 and the Si core 31 in the substrate thickness direction (z direction), but are not limited thereto. As long as the modulating electrodes 30a, 30b are formed in the region of the SiO2 layer 11 in a plane perpendicular to the substrate of the SiPh circuit, the modulating electrodes are fabricated in the same photolithography process as all other electrodes of the SiPh circuit. Electrodes other than the modulating electrodes may be fabricated at different heights.
- FIG. 6 is a diagram showing the configuration of the top and side cross sections of the optical circuit of the third embodiment.
- the configuration of a hybrid optical modulator is shown.
- FIG. 6(a) is a top view of the SiPh circuit looking at the Si substrate surface (xy plane)
- FIG. 6(b) is a side cross section (xy plane) cut perpendicularly to the substrate surface and the light traveling direction along the line VIb-VIb
- FIG. 6(c) is a side cross section (xy plane) cut perpendicularly to the substrate surface and the light traveling direction along the line VIc-VIc in the MZ type optical modulator 300.
- FIG. 6 shows a schematic diagram of a portion of one optical waveguide 31 of two interference optical waveguides, which includes modulation electrodes 30a and 30b and functions as a refractive index modulation region.
- the differences from the optical circuit 100 of the first embodiment are as follows.
- the LN thin film 12 is configured only in the refractive index modulation region where the MZI including the two interference optical waveguides 21 is configured.
- the ends of the modulation electrodes 30a, 30b to which an electrical signal is applied are provided with PADs to which bonding wires or the like from an electrical signal source are connected, so it is essential to align the LN thin film so that it does not cover the PADs.
- PADs to which bonding wires or the like from an electrical signal source are connected
- the optical circuit 300 of this embodiment differs from the first and second embodiments in that the PADs 35a, 35b of the modulating electrodes 30a, 30b are configured on the back surface of the Si substrate opposite the LN thin film 12.
- the PADs 35a, 35b are formed on the side of the Si substrate 10 opposite the side on which the LN thin film 12 is attached.
- the modulating electrodes 30a, 30b and the PADs 35a, 35b are connected by through-silicon vias (TSVs) 36a, 36b, respectively.
- TSVs through-silicon vias
- the external electric signal source and the PADs 35a and 35b can be connected to the surface of the Si substrate opposite to the LN thin film 12, there is no need to limit the position of the LN thin film 12, and the accuracy of the attachment position may be low.
- one LN thin film can be attached to the entire surface of the SiO2 layer 11.
- the modulating electrodes 30a and 30b are shown as having the same bottom height as the Si core 31 in the substrate thickness direction (z direction), but are not limited to this configuration. If the modulating electrodes 30a and 30b are configured in the region of the SiO2 layer 11 in a plane perpendicular to the substrate of the SiPh circuit, the modulating electrodes can be fabricated in the same photolithography process as all other electrodes of the SiPh circuit. Electrodes other than the modulating electrodes may be fabricated at different heights.
- FIG. 7 is a diagram showing the configuration of the top surface and the side cross section of the optical circuit of the fourth embodiment.
- the configuration of a hybrid optical modulator is shown.
- FIG. 7(a) is a top view of the SiPh circuit looking at the Si substrate surface (xy surface)
- FIG. 7(b) is a side cross section (xy surface) cut along the line VIIb-VIIb
- FIG. 7(c) is a side cross section (xy surface) cut along the line VIIc-VIIc perpendicular to the substrate surface and the light traveling direction.
- FIG. 7(a) is a top view of the SiPh circuit looking at the Si substrate surface (xy surface)
- FIG. 7(b) is a side cross section (xy surface) cut along the line VIIb-VIIb
- FIG. 7(c) is a side cross section (xy surface) cut along the line VIIc-VIIc perpendicular to the substrate surface and the light traveling direction.
- FIG. 7(a)
- FIG. 6 shows a schematic diagram of a portion of one of two interference optical waveguides in an MZ type optical modulator 400, which includes modulation electrodes 30a and 30b and functions as a refractive index modulation region.
- the differences between the optical circuits 100, 200, and 300 of the above-mentioned embodiments and the optical circuit 400 are as follows.
- the core is composed of a SiN 32 core in the refractive index modulation region and a Si core 31 outside the refractive index modulation region, similar to the optical modulator 200 of embodiment 2. It also has a mode converter 40 between the SiN core and the Si core shown in FIG. 5.
- the modulation electrodes 33a, 33b differ from the electrodes of the other embodiments described above in that they extend in the x direction along the core and have a wall-like shape standing in the z direction.
- the TSV can be considered to be continuously formed in the x direction.
- the high-frequency electrodes as modulation electrodes are wall-like electrodes 33a, 33b that are continuously formed and penetrate from the height of the core 32 to the surface opposite the cladding layer 11 of the substrate in the thickness direction of the substrate 10.
- FIG. 7 is a schematic diagram, and the scales in each direction are not the same.
- the substrate thickness direction (z direction) is shown significantly enlarged, and the cross sections (y-z planes) of the modulation electrodes 30a and 30b in the first to third embodiments are actually rectangular with a horizontal length in the y direction.
- the cross sections (y-z planes) of the modulation electrodes 33a and 33b in the fourth embodiment shown in FIG. 7(b) can be rectangular with a vertical length in the z direction as well as a horizontal length in the y direction, allowing the electrode shape to be changed significantly.
- the characteristic impedance as a transmission path for high-frequency electrical signals can also be calculated with different parameter values.
- the same characteristic impedance can be obtained with electrodes 33a and 33b that are narrower in the y direction parallel to the substrate surface than the modulation electrodes in the first to third embodiments. Therefore, by narrowing the width of the electrodes, the wall-shaped modulation electrodes 33a and 33b in the fourth embodiment shown in FIG. 7(b) are more suitable for high-density integration.
- FIG. 8 is a diagram showing the configuration of the top surface and the side cross section of the optical circuit of the fifth embodiment.
- the configuration of a hybrid optical modulator is shown.
- FIG. 8(a) is a top view of the SiPh circuit looking at the Si substrate surface (xy surface)
- FIG. 8(b) is a side cross section (xy surface) cut perpendicularly to the substrate surface and the light traveling direction along the line VIIIb-VIIIb
- FIG. 8(c) is a side cross section (xy surface) cut perpendicularly to the line VIIIc-VIIIc.
- FIG. 8 shows a schematic diagram of a portion of one optical waveguide 31 of two MZ type interference optical waveguides in an MZ type optical modulator, which includes modulation electrodes 37a and 37b and functions as a refractive index modulation region.
- the configuration of the optical circuit 500 of this embodiment is the same as that of the optical circuit 300 of embodiment 3 shown in FIG. 6 in terms of the configuration of the optical waveguide and the modulation electrodes.
- the modulation electrodes 37a and 37b are made of Si with impurities added by ion implantation, rather than metals such as aluminum, copper, or gold.
- the high-frequency electrodes can be formed in the same layer as the Si core 31.
- the modulation electrodes 37a and 37b can be formed directly next to the Si core 31 at the same height, so that the electric field tends to concentrate inside the LN thin film 12. If the configuration of the optical circuit 500 is applied to an optical modulator, efficient refractive index modulation becomes possible.
- the PADs 35a, 35b are formed on the back side of the Si substrate, and the modulation electrodes 37a, 37b made of Si doped with impurities are combined.
- the present invention can also be applied to the case in which the PADs 34a, 34b are formed on the top surface of the SiO2 layer 11 as in the first and second embodiments shown above. In this case, however, the LN thin film needs to be attached only to the top side of the modulation electrodes.
- FIG. 9 is a diagram showing the top and side cross-sectional configurations of the optical circuit of the sixth embodiment.
- the diagram shows the configuration of a hybrid optical modulator 600.
- FIG. 9(a) is a top view of the SiPh circuit looking at the Si substrate surface (xy plane)
- FIG. 9(b) is a side cross-sectional view (xy plane) cut perpendicularly to the substrate surface and the light traveling direction along line IXb-IXb
- FIG. 9(c) is a side cross-sectional view (xy plane) cut perpendicularly to line IXc-IXc and line IXc in the MZ type optical modulator 600.
- FIG. 9 shows a schematic diagram of a portion of one optical waveguide of two interference optical waveguides in the MZ type optical modulator 600, which includes a modulation electrode and functions as a refractive index modulation region.
- the optical circuit 600 like the optical circuit 200 of the second embodiment, has an optical waveguide structure in which the SiN core 32 and the Si core 31 are coupled by the mode conversion section 40.
- the SiN core 32 and the LN thin film 12 can be brought into close proximity, so that, like the optical circuit 200, refractive index modulation can be efficiently generated.
- the optical circuit 600 of this embodiment differs from the optical circuit of embodiment 2 in that the positions of the modulation electrodes 30a, 30b in the substrate thickness direction (z direction) are at the same height as the SiN core 32.
- PADs 35a, 35b to which bonding wires from an electrical signal source are connected for applying an electrical signal to the modulation electrodes are formed on the back surface of the Si substrate 10 on the side opposite the LN thin film 12, as in embodiments 3 to 5.
- the modulation electrodes 30a, 30b and the PADs 35a, 35b are connected by TSVs 36a, 36b, respectively.
- the modulating electrodes 30a, 30b are formed at the same height directly beside the SiN core, which makes it easier for the electric field to concentrate inside the LN thin film 12. If the configuration of the optical circuit 600 is applied to an optical modulator, efficient refractive index modulation becomes possible. Since the external electric signal source and the PADs 35a and 35b can be connected on the opposite side of the LN thin film 12, there is no need to limit the position of the LN thin film 12, and the accuracy of the attachment position may be low. For multiple optical modulator chips, one LN thin film can be attached to the entire surface of the SiO2 layer 11.
- the optical circuit 600 of Fig. 9 an example is shown in which PADs 35a, 35b are formed on the back side of the Si substrate, and the positions of the modulating electrodes 30a, 30b in the substrate thickness direction are at the same height as the SiN core 32.
- the present invention can also be applied to the case in which the PADs 34a, 34b are formed on the upper surface of the SiO2 layer 11 in the above-mentioned embodiment 2. In this case, however, the LN thin film needs to be attached only to the upper side of the modulating electrode.
- the optical circuit 600 of this embodiment can be combined with the modulating electrode 3 made of Si to which impurities are added by ion implantation or the like in embodiment 5.
- a hybrid optical modulator combining an LN thin film and a SiPh circuit has been described as an example, but instead of the LN thin film, a ferroelectric such as lithium tantalate (LT) or barium titanate can be used.
- optical devices that utilize the electro-optical effect of a ferroelectric thin film are not limited to optical modulators.
- a polarization controller that arbitrarily controls the polarization state of light, or a phase shifter that arbitrarily changes the phase state of light can be realized.
- a low-frequency control signal, a constant-value DC signal, or the like can be applied to the electrodes that apply an electric field to the above-mentioned ferroelectric thin film, rather than a modulation signal.
- the polarization controller is operated as a polarization scrambler, the signal may be on the order of several GHz.
- the optical circuit of the present invention can improve the manufacturability and mountability of optical circuits that combine ferroelectric thin films and SiPh circuits.
- This invention can be used in optical communications.
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Abstract
Description
本発明は光回路に関し、より詳細には、強誘電体薄膜を含む光回路の構造に関する。 The present invention relates to optical circuits, and more specifically to the structure of optical circuits that include ferroelectric thin films.
IoTや5G(第5世代移動通信システム)サービスの普及などに伴い、これらを支える光通信ネットワークに対して、より一層の高速化が求められている。キーデバイスの1つである光変調器においても、高性能化と小型・低消費電力化を実現するための研究開発が続けられている。 As IoT and 5G (fifth generation mobile communications system) services become more widespread, there is a demand for even faster optical communications networks that support these services. Research and development is also ongoing for optical modulators, one of the key devices, to achieve higher performance, smaller size, and lower power consumption.
LN光変調器は、LiNbO3(以下LN)結晶のポッケルス効果による屈折率変化を利用した光変調器で光通信の基幹デバイスの1つである。DFBレーザなどのCW光を変調する外部変調器として使用されており、100GHzを越える高速変調が可能である。OIF(The Optical Internetworking Forum)による高帯域幅コヒーレントドライバ変調器(HB-CDM)などの光モジュール内の光変調器としても期待されている。より小型および低コスト化を実現するために、薄膜LNをSi導波路上に貼り付けた光変調器がその効率の高さと帯域の広さから期待されている。 The LN optical modulator is an optical modulator that utilizes the refractive index change caused by the Pockels effect of LiNbO 3 (hereinafter referred to as LN) crystal, and is one of the core devices for optical communication. It is used as an external modulator to modulate CW light from DFB lasers and the like, and is capable of high-speed modulation exceeding 100 GHz. It is also expected to be used as an optical modulator in optical modules such as the high-bandwidth coherent driver modulator (HB-CDM) proposed by OIF (The Optical Internetworking Forum). In order to achieve smaller size and lower cost, an optical modulator with a thin film LN attached onto a Si waveguide is expected due to its high efficiency and wide bandwidth.
図1は、LN薄膜SiPhハイブリッド光変調器の構成を示す概要図である(非特許文献1)。光変調器700は、Si基板10上にSiO2層およびコア層が形成されたシリコンフォトニック(SiPh:Silicon Photonic)回路に、LN薄膜12を貼り付けたLN薄膜とSiPh回路のハイブリッド構成を持っている。分岐したコア層によって、2本の干渉光導波路21を含むマッハツエンダー型干渉計(MZI)が構成されている。LN薄膜12の上面には、干渉導波路21の各々を挟み込むように高周波電極22がさらに形成されていている。コア、周囲のSiO2クラッド、およびコアに近接しているLN薄膜12が一体となって、光導波路として機能する。光は、コアによって閉じ込められるだけでなく、LNにも染み出して伝搬し、強誘電体材料のLNおよびSiコアが一体となった複合光導波路として機能する。
FIG. 1 is a schematic diagram showing the configuration of an LN thin film SiPh hybrid optical modulator (Non-Patent Document 1). The
変調用電極22に印可した高周波電気信号で、貼り付けられた薄膜LNの屈折率を変調することで、MZIの干渉条件が変化し2本の干渉光導波路の合波光出力がON/OFFされる。薄膜LNとSiPh回路を組み合わせることで、光変調器を含む光モジュールの大幅な小型化と高効率化が期待されている。
By modulating the refractive index of the attached thin-film LN with a high-frequency electrical signal applied to the
しかしながら、図1に示したSiPh回路上にLN薄膜を貼り付けた構成の光変調器には、その製造性および実装性に問題があった。屈折率変調のための電気信号が印可される変調用電極22は、LN薄膜12の上に形成されている。通常、SiPh回路上にLN薄膜を貼り付ける工程は、SiPh回路の作製のためのフォトリソグラフィを一旦終了して、独立した工程として実施されなければならない。結果として、高周波電極22の形成のために、フォトリソグラフィ工程を2回に分けて実施せざるを得ない。光変調器のこのような製造工程は複雑であり、高コストとなる。さらに、SiPh回路の工程で作製される他の電極に対するPADと、変調用電極22に対するPADの高さが異なることになる。作製された光変調器チップを光モジュール等に組み立てる後工程で、小型化のためのフリップチップ実装ができない制限もあった。
However, the optical modulator with the LN thin film attached to the SiPh circuit shown in FIG. 1 has problems in manufacturability and assembly. The
本発明は上述のような問題を鑑みてなされたもので、製造性および実装性を改善した強誘電体薄膜とSiPh回路を組み合わせた光回路の構成を提供する。 The present invention was made in consideration of the above-mentioned problems, and provides an optical circuit configuration that combines a ferroelectric thin film and a SiPh circuit with improved manufacturability and mountability.
本発明の1つの実施態様は、シリコンによる基板、クラッド層、および、強誘電体薄膜が、順に配置された光回路であって、前記クラッド層の内に形成されたコアと、前記コアに沿って形成された、前記強誘電体薄膜に電界を印可する1つ以上の電極とを備えた光回路である。 One embodiment of the present invention is an optical circuit in which a silicon substrate, a cladding layer, and a ferroelectric thin film are arranged in that order, the optical circuit having a core formed within the cladding layer and one or more electrodes formed along the core for applying an electric field to the ferroelectric thin film.
本発明により、製造性および実装性を改善した強誘電体薄膜とSiPh回路を組み合わせた光回路を提供する。 The present invention provides an optical circuit that combines a ferroelectric thin film and a SiPh circuit with improved manufacturability and mountability.
本開示の光回路は、製造性および実装性を改善した、強誘電体薄膜とSiPh回路を組み合わせた新規な構成を提供する。一例として、LN-Siのハイブリッド光変調器に好適な新規な構成を提示する。LN薄膜の屈折率を変調する電気信号が印可される電極が、SiPh回路内に形成されている。光回路におけるすべての電極が、SiPh回路の作製工程中に形成されるため、LN薄膜の貼り付け後に追加のフォトリソグラフィが不要となる。高周波電極とバイアス用などの他の電極を同じ高さで作製することが可能となり、作製された光変調器のチップを、後工程においてフリップチップ実装することが可能となる。光変調器を始めとして、LNの電気光学効果を利用するデバイスの製造性および実装性を改善する。 The optical circuit disclosed herein provides a novel configuration that combines a ferroelectric thin film and a SiPh circuit, with improved manufacturability and mountability. As an example, a novel configuration suitable for an LN-Si hybrid optical modulator is presented. Electrodes to which an electrical signal that modulates the refractive index of the LN thin film is applied are formed in the SiPh circuit. All electrodes in the optical circuit are formed during the fabrication process of the SiPh circuit, so no additional photolithography is required after attaching the LN thin film. It becomes possible to fabricate high-frequency electrodes and other electrodes such as for bias at the same height, and the fabricated optical modulator chip can be flip-chip mounted in a later process. It improves the manufacturability and mountability of devices that utilize the electro-optical effect of LN, including optical modulators.
以下では、光変調器を一例として、まず従来技術の光回路の構成とその問題を明らかにする。次いで、本開示の光回路の基本構成および変形例ならびに製造工程について詳細に説明する。以下の説明で、ハイブリッド光変調器は、LN薄膜とSiPh回路を組み合わせたマッハツエンダー型変調器(MZM)を言うものとする。以下で説明される光回路の構造のすべての図面は模式図であり、各方向の縮尺は一致していない。基板厚さ方向(z方向)の著しく拡大して示されている。また各要素の高さ・幅などの相対関係も、異なる要素間で必ずしも正確に表現されていない点に留意されたい。 Below, we will first clarify the configuration of the optical circuit of the prior art and its problems, using an optical modulator as an example. Next, we will explain in detail the basic configuration and modified examples of the optical circuit of the present disclosure, as well as the manufacturing process. In the following explanation, a hybrid optical modulator refers to a Mach-Zehnder type modulator (MZM) that combines an LN thin film and a SiPh circuit. All drawings of the optical circuit structure described below are schematic diagrams, and the scales in each direction are not consistent. The substrate thickness direction (z direction) is shown significantly enlarged. Please also note that the relative relationships of the height, width, etc. of each element are not necessarily accurately expressed between different elements.
以下の説明では、本開示の光回路をハイブリッド光変調器に適用した場合を例として説明する。しかしながら本開示の光回路の構成は、SiPh回路上に強誘電体薄膜を貼り付けた構成の他の光回路にも適用可能なものである。強誘電体材料は、電気光学効果によって光導波路の屈折率を変化させることが可能なものであれば、ニオブ酸リチウム(LN)だけに限られず、タンタル酸リチウム(LT)、 チタン酸バリウムなども含む。また、コアの近傍の強誘電体薄膜の屈折率変調を利用する光デバイスには、光変調器の他に、偏波モード分散の補償などに利用できる偏波制御器、移相器なども含み得る。 In the following explanation, the optical circuit of the present disclosure will be described as an example in which it is applied to a hybrid optical modulator. However, the configuration of the optical circuit of the present disclosure can also be applied to other optical circuits in which a ferroelectric thin film is attached to a SiPh circuit. Ferroelectric materials are not limited to lithium niobate (LN) and include lithium tantalate (LT) and barium titanate, as long as they are capable of changing the refractive index of the optical waveguide by the electro-optic effect. Furthermore, optical devices that utilize the refractive index modulation of the ferroelectric thin film near the core can include, in addition to optical modulators, polarization controllers and phase shifters that can be used to compensate for polarization mode dispersion.
図2は、従来技術のハイブリッド光変調器の構成を模式的に示した図である。図2の(a)は、SiPh回路のSi基板面(x-y面)を見た上面図であり、図2の(b)はIIb-IIb線を通り基板面および光進行方向に垂直に切った側断面図(y-z面)である。図2の(c)は(b)はIIc-IIc線を基板面および光進行方向に垂直に切った側断面図である。図1に示した従来技術のMZ型のハイブリッド光変調器700において、2本の干渉光導波路の内の1本の光導波路21について、変調用電極22a、22bを含み、屈折率変調領域として機能する部分を模式的に示している。図2の(b)、(c)の2つの側断面図を参照すれば、光変調器700の内のSiPh回路は、Si基板10の上に形成されたSiO2層11と、矩形状のSiコア12を含む。
FIG. 2 is a diagram showing a schematic configuration of a hybrid optical modulator of the prior art. FIG. 2(a) is a top view of the Si substrate surface (x-y surface) of the SiPh circuit, and FIG. 2(b) is a side cross-sectional view (y-z surface) cut perpendicular to the substrate surface and the light traveling direction through line IIb-IIb. FIG. 2(c) is a side cross-sectional view cut perpendicular to the substrate surface and the light traveling direction through line IIc-IIc. In the prior art MZ type hybrid
SiPh回路は、例えば、クラッド層として機能するSiO2の内部に形成された電極23を含む。電極23は、光変調器の変調信号が伝搬される高周波電極であり得るし、光変調器とともに集積化される電気回路等の他の回路のための電極でもあり得る。電極23は、変調用電極22とは異なる構成を模式的に示したものであって、光回路700の上面における位置は問わない。また、断面図上の高さ方向の位置も、図2の(c)の一に限定されない。このSiPh回路は、Si基板の上に各層を形成し、フォトリソグラフによってコアや電極をパターン形成することで作製可能である。また、予めコアと機能するSi層とSiO2層が形成されたSOI(Silicon On Insulator)基板を加工してSiPh回路を形成することもできる。
The SiPh circuit includes, for example, an
上述のSiPh回路の上には、LN薄膜12が貼り付けられている。LN薄膜の貼り付けは、予め必要な領域のサイズに形成されたLN薄膜およびSiO2層の表層をアルゴンビームにより活性化させ、両者を接触させたのちに加圧、加熱をすることで実施される。このようにLN薄膜12は、LN薄膜をボンディングすることで形成されるため、Siフォトリソグラフの工程とは別の物理的な貼り付け工程が必須となる。Siコア12から染み出す光の光導波路の一部としてのLN薄膜12に屈折率変化を生じさせるために、LN薄膜12の上に、変調用の例えば金電極22a、22bが形成される。電極の端部には、接続用のPAD24a、24bが形成されている。この変調用電極22a、22bの形成のためには、LN薄膜12を貼り付け後の2回目のフォトリソグラフ工程が必要なため、光変調器700の製造工程は煩雑となりコストも増加する。
The LN
また図2の(b)および(c)を参照すれば、変調用電極22a、22bの高さとSiPh回路の電極23の高さは異なる。光回路の回路構成面で、電極高さが異なっていれば、ボールグリッドアレイ(BGA)を用いた高密度の実装技術を利用することができない。小型化および高密度実装が要求される光変調器などにおいて、有力なBGA技術が利用できないのは、光モジュール、光伝送装置の小型化にも大きな障害となる。本開示の光回路は、上述の光変調器700において示された製造性および実装性などの問題を解決するものである。
Also, referring to (b) and (c) of FIG. 2, the height of the
[実施形態1]
図3は、実施形態1の光回路の上面および側断面の構成を模式的に示した図である。本実施形態の光回路100の一例として、ハイブリッド光変調器の構成を模式的に示した図である。図2と同様に、図3の(a)はSiPh回路のSi基板面(x-y面)を見た上面図であり、(b)はIIIb-IIIb線を、(c)はIIIc-IIIc線を基板面および光進行方向に垂直に切った側断面図(x-y面)である。図3は、MZ型の光変調器において、2本の干渉光導波路の内の1本の光導波路31について、変調用電極30a、30bを含み、屈折率変調領域として機能する部分を模式的に示している。光導波路のコア31の構成は、図2に示した従来技術の光回路700のコア21と同様である。以下では、従来技術の光回路700との相違点について絞って説明する。
[Embodiment 1]
FIG. 3 is a diagram showing the configuration of the top surface and the side cross section of the optical circuit of the first embodiment. As an example of the
光回路100は、変調用電極30a、30bが、SiPh回路の基板に垂直な面内において、SiO2クラッドの領域内に形成されている点で、SiPh回路の外部のLN薄膜上に形成されていた従来技術の構成と相違する。ここで、変調用電極30a、30bに接続されるPAD34a、34bは、LN薄膜の屈折率変調に寄与せず、屈折率変調領域に含まれないものとする。変調用電極30a、30bは、それぞれの両端にビア(VIA)を介してPAD34a、34bを有しており、PADには電気信号を供給する電気回路、電気信号源などと何らかの手段で接続される。ワイヤボンディングされても良いし、BGAによって他の電気素子、ドライバ回路に接続されても良い。また、PADを備えずに、光変調器と同一のSi基板上に集積化された電気回路から直接接続されていても良い。変調用電極は、光変調器では、高周波電気信号が印可される高周波電極となる。
The
図3では変調信号の入力点を示す目的で、PAD34a、34bはLN薄膜12に概ね隣接して在るものとして示している。変調用電極30a、30bが延長され、LN薄膜12の領域から離れた位置にPADが形成されていても良い。図3におけるPAD34a、34bの位置は一例であることに留意されたい。
In FIG. 3, for the purpose of showing the input point of the modulation signal,
変調用電極30a、30bが、SiPh回路の基板に垂直な面内において、SiO2クラッドの領域内に形成されているため、変調用電極は他の全ての電極と同様に、SiPh回路の一連のフォトリソグラフィ工程の中で、作製される。従来技術のようにLN薄膜12の貼り付け工程の後の、追加のフォトリソグラフィ工程が不要である。さらに、変調用電極を含めたすべての電極のPADを、同一の高さに形成することが可能となる。したがって、BGAやバンプを使ったフリップチップ実装が可能となる。
Since the
したがって本発明の光回路は、シリコンによる基板10、クラッド層11、および、強誘電体薄膜12が、順に配置された光回路であって、前記クラッド層の内に形成されたコア31と、前記コアに沿って形成された前記強誘電体薄膜に電界を印可する1つ以上の電極30a、30bとを備えたものとして実施できる。
The optical circuit of the present invention can therefore be implemented as an optical circuit in which a
図3の(b)、(c)によれば、変調用電極30a、30bは、基板厚さ方向(z方向)で、Siコア31と同じ底面高さを持つものとして示されているが、これに限定されない。変調用電極30a、30bが、SiPh回路の基板に垂直な面内において、SiO2層11の領域内に形成されていれば、変調用電極は他の全ての電極と同様に、SiPh回路の一連のフォトリソグラフィ工程の中で作製される。変調用電極とは他の異なる電極が、異なる高さに作製されていても良い。
3(b) and 3(c), the modulating
[実施形態2]
図4は、実施形態2の光回路の上面および側断面の構成を模式的に示した図である。本実施形態の光回路200の一例として、ハイブリッド光変調器の構成を模式的に示している。図4の(a)はSiPh回路のSi基板面(x-y面)を見た上面図であり、(b)はIVb-IVb線を、図4の(c)はIVc-IVc線を基板面および光進行方向に垂直に切った側断面図(x-y面)である。図4は、MZ型の光変調器200において、2本の干渉光導波路の内の1本の光導波路32について、変調用電極30a、30bを含み、屈折率変調領域として機能する部分を模式的に示している。実施形態1の光回路100との相違点は、以下の通りである。
[Embodiment 2]
FIG. 4 is a diagram showing the top and side cross-sectional configurations of the optical circuit of the second embodiment. As an example of the
前述の実施形態1の光回路100では、屈折率が変調される光導波路は、屈折率変調領域では、Siコア31、周囲のSiO2クラッドおよびコアに隣接するLN薄膜12からなり、複合導波路を形成していた。またSiコア31は、LN薄膜とのハイブリッド構成を有する屈折率変調領域の内外を通じて、周囲のSiO2クラッドとともに連続した光導波路を構成していた。一方、本実施形態の光回路200では、電気信号によって屈折率を変化させる光導波路が、Siコアと比べてLN薄膜12にさらに近接した窒化シリコン(SiN)コア32によって構成されている。LN薄膜とのハイブリッド構成を有する屈折率変調領域の外では、SiNコアとは別の、Siコア31によって光導波路が構成されている。基板の厚さ方向(z方向)において、SiNコア32はSiコア31よりも高い位置に、LN薄膜12より近接して形成することができる。このため、電気信号によるLN薄膜12の屈折率変調を効率良く実現できる。高さの異なるSiNコア32およびSiコア31は、図4の(a)でLN薄膜12の境界付近に作成されたモード変換器40によって光学的に接続することができる。
In the
図5は、SiNコアおよびSiコアの間のモード変換器の構成を示した図である。図5の(a)は、光回路200のSi基板面(x-y面)を見た上面図であり、モード変換器40の近くの2種類のコア32、31のみを示している。図5(b)はコアの中心線(Vb-Vb線)を通り、基板面および光進行方向に沿って切った、モード変換器40の側断面図(x-z面)である。図5の(a)を参照すれば、モード変換器40は、SiNコア32の先端に、コア幅が徐々に狭くなる第1のテーパを有し、Siコア31の先端が、コア幅が徐々に広くなる第2のテーパを有する。図5の(b)を参照すれば、SiO2クラッド層11のモード変換器40の領域内で、上下に2つのテーパ部がオーバラップしており、高さの異なる光導波路間を効率良く光結合する。モード変換器は、図5だけのものに限られず、光のモード変換ができるものであれば、他の構成によっても実現できる。
FIG. 5 is a diagram showing the configuration of a mode converter between a SiN core and a Si core. FIG. 5(a) is a top view of the Si substrate surface (xy surface) of the
図4において、モード変換器40は、LN薄膜12の端近傍にあるものとして示しているが、LN薄膜12の領域内にあっても良いし、LN領域12の領域外にあっても良い。SiNコア32が隣接する変調用電極30a、30bと十分な電気光学効果の作用(例えば屈折率の変化)を生じさせられる限り、モード変換器40の位置は問わない。
In FIG. 4, the
したがって本発明の光回路は、コアが、基板面(x-y面)内の強誘電体薄膜12が形成された領域内で、前記基板の厚さ方向(z方向)における前記強誘電体薄膜の側に形成された窒化シリコンの第1のコア32、および、前記厚さ方向における前記第1のコアよりも前記基板の側に形成されたシリコンの第2のコア31を含み、前記第1のコアと前記第2のコアが光結合されているものとして実施できる。
The optical circuit of the present invention can therefore be implemented as a core that includes a
実施形態2の光回路200によれば、LN薄膜12の貼り付け工程後の、追加のフォトリソグラフィ工程が不要であり、変調用電極を含めたすべての電極のPADを、同一の高さに形成することが可能となる。LN薄膜が貼り付けられた屈折率変調領域におけるSiNコアも、SiPh回路の一連の作製工程の中で形成することが可能である。SiNコア32とLN薄膜12を近接することができるため、光回路200の構成を光変調器に適用すれば、屈折率変調を効率的に生じさせることができる。
According to the
図4の(b)、(c)によれば、変調用電極30a、30bは、基板厚さ方向(z方向)で、SiNコア32およびSiコア31の中間に位置するものとして示されているが、これに限定されない。変調用電極30a、30bが、SiPh回路の基板に垂直な面内において、SiO2層11の領域内に形成されていれば、変調用電極は他の全ての電極と同様に、SiPh回路の一連のフォトリソグラフィ工程の中で作製される。変調用電極とは他の異なる電極が、異なる高さに作製されていても良い。
4(b) and (c), the modulating
[実施形態3]
図6は、実施形態3の光回路の上面および側断面の構成を模式的に示した図である。本実施形態の光回路300の一例として、ハイブリッド光変調器の構成を模式的に示した図である。図6の(a)はSiPh回路のSi基板面(x-y面)を見た上面図であり、(b)はVIb-VIb線を、(c)はVIc-VIc線を基板面および光進行方向に垂直に切った側断面図(x-y面)である。図6は、MZ型の光変調器300において、2本の干渉光導波路の内の1本の光導波路31について、変調用電極30a、30bを含み、屈折率変調領域として機能する部分を模式的に示している。実施形態1の光回路100との相違点は、以下の通りである。
[Embodiment 3]
FIG. 6 is a diagram showing the configuration of the top and side cross sections of the optical circuit of the third embodiment. As an example of the
前述の実施形態1の光回路100では、LN薄膜12は、2本の干渉光導波路21を含むMZIが構成されている屈折率変調領域のみに限定的に構成されている。電気信号が印可される変調用電極30a、30bの端部には、電気信号源からのボンディングワイヤ等が接続されるPADを備えるため、PAD上にLN薄膜が被らないように、LN薄膜の位置合わせが必須となる。さらに、複数の光変調器の1つのウェファ上に作製する場合には、複数のLN薄膜の位置合わせを行って、それぞれを貼り付ける工程が必要となる。
In the
本実施形態の光回路300は、変調用電極30a、30bのPAD35a、35bが、LN薄膜12とは逆のSi基板の裏面上に構成されている点で、実施形態1および実施形態2と異なっている。PAD35a、35bは、Si基板10のLN薄膜12が貼り付けられた面とは逆の面側に、形成される。変調用電極30a、30bとPAD35a、35bの間は、シリコン貫通ビア(TSV:Through-Silicon Via)36a、36bによってそれぞれ接続される。
The
外部の電気信号源とPAD35a、35bを、Si基板のLN薄膜12とは反対側の面で接続することができるので、LN薄膜12の位置を限定する必要が無く、貼り付け位置の精度は低くて良い。複数の光変調器のチップに対して、1枚のLN薄膜をSiO2層11の全面に貼り付けることもできる。
Since the external electric signal source and the
図6の(b)、(c)では、変調用電極30a、30bは、基板厚さ方向(z方向)でSiコア31と同じ底面高さを持つものとして示されているが、この構成に限定はされない。変調用電極30a、30bが、SiPh回路の基板に垂直な面内において、SiO2層11の領域内に構成されていれば、変調用電極は他の全ての電極と同様に、SiPh回路の一連のフォトリソグラフィ工程の中で作製できる。変調用電極とは他の異なる電極が、異なる高さに作製されていても良い。
6(b) and 6(c), the modulating
[実施形態4]
図7は、実施形態4の光回路の上面および側断面の構成を模式的に示した図である。本実施形態の光回路400の一例として、ハイブリッド光変調器の構成を模式的に示している。図7の(a)はSiPh回路のSi基板面(x-y面)を見た上面図であり、(b)はVIIb-VIIb線を、(c)はVIIc-VIIc線を基板面および光進行方向に垂直に切った側断面図(x-y面)である。図6は、MZ型の光変調器400において、2本の干渉光導波路の内の1本の光導波路について、変調用電極30a、30bを含み、屈折率変調領域として機能する部分を模式的に示している。上述の各実施形態の光回路100、200、300と光回路400との相違点は、以下の通りである。
[Embodiment 4]
FIG. 7 is a diagram showing the configuration of the top surface and the side cross section of the optical circuit of the fourth embodiment. As an example of the
本実施形態の光回路400による光変調器では、コアは、実施形態2の光変調器200と同様、屈折率変調領域のSiN32コア、および、屈折率変調領域よりも外のSiコア31から成っている。図5に示したSiNコアおよびSiコアの間のモード変換器40も備えている。変調用電極33a、33bは、コアに沿ってx方向に延び、z方向に立った壁状の形状を有する点で、上述の他の実施形態の電極と相違している。TSVがx方向に連続的に形成されているものと見なすことができる。すなわち、変調用電極としての高周波電極は、基板10の厚さ方向において、コア32の高さから基板のクラッド層11とは反対面まで貫通し、連続的に形成された壁状電極33a、33bである。
In the optical modulator using the
前述のように図7は模式図であり、各方向の縮尺は一致していない。基板厚さ方向(z方向)が著しく拡大して示されており、実施形態1~3における変調用電極30a、30bの断面(y―z面)は、実際にはy方向に横長の矩形である。一方、図7の(b)に示した実施形態4の変調用電極33a、33bの断面(y―z面)は、y方向に横長だけでなく、z方向に縦長の矩形とすることも可能であって、電極形状を大きく変えることができる。高周波電気信号の伝送路としての特性インピーダンスも異なるパラメータ値で計算され得ることに留意されたい。実施形態1~3の変調用電極と比べて、基板面に平行なy方向でより幅の狭い電極33a、33bで、同一の特性インピーダンスを得ることもできる。したがって、電極の幅をより狭くすることで、図7の(b)に示した実施形態4の壁状の変調用電極33a、33bは、高密度集積化により適している。
As mentioned above, FIG. 7 is a schematic diagram, and the scales in each direction are not the same. The substrate thickness direction (z direction) is shown significantly enlarged, and the cross sections (y-z planes) of the
LN薄膜12を貼り付ける際の位置精度が低くても構わないし、複数の光変調器のチップに対して、1枚のLN薄膜をSiO2層11の全面に貼り付けることもできる。
It does not matter if the positional accuracy in attaching the LN
[実施形態5]
図8は、実施形態5の光回路の上面および側断面の構成を模式的に示した図である。本実施形態の光回路500の一例として、ハイブリッド光変調器の構成を模式的に示している。図8の(a)はSiPh回路のSi基板面(x-y面)を見た上面図であり、(b)はVIIIb-VIIIb線を、(c)はVIIIc-VIIIc線を基板面および光進行方向に垂直に切った側断面図(x-y面)である。図8は、MZ型の光変調器において、MZ型の2本の干渉光導波路の内の1本の光導波路31について、変調用電極37a、37bを含み、屈折率変調領域として機能する部分を模式的に示している。
[Embodiment 5]
FIG. 8 is a diagram showing the configuration of the top surface and the side cross section of the optical circuit of the fifth embodiment. As an example of the
本実施形態の光回路500の構成は、図6に示した実施形態3の光回路300と、光導波路および変調用電極の構成の点では同一である。実施形態3の構成との相違点は、変調用電極37a、37bがアルミや銅や金などの金属ではなくて、イオン注入などにより不純物を添加したSiによって構成されていることである。高周波用電極の材料をイオン注入したSiとすることで、Siコア31と同じ層として高周波用電極を形成することができる。本実施形態の光回路500の構成によれば、変調用電極37a、37bをSiコア31の真横に、同一の高さに形成できるため、LN薄膜12の内部に電界が集中しやすくなる。光回路500の構成を光変調器に適用すれば、効率的な屈折率変調が可能となる。
The configuration of the
図8の光回路500では、Si基板の裏面側にPAD35a、35bを形成した構成に不純物を添加したSiによる変調用電極37a、37bを組み合わせた例を示した。しかしながら先に示した実施形態1、実施形態2のようにPAD34a、34bが、SiO2層11の上面に作製されている場合にも、当然適用できる。ただしこの場合は、LN薄膜は、変調用電極の上側のみに限定的に張りつける必要がある。
In the
[実施形態6]
図9は、実施形態6の光回路の上面および側断面の構成を模式的に示した図である。一例として、ハイブリッド光変調器600の構成を模式的に示した図である。図9の(a)はSiPh回路のSi基板面(x-y面)を見た上面図であり、(b)はIXb-IXb線を、(c)はIXc-IXc線を基板面および光進行方向に垂直に切った側断面図(x-y面)である。図9は、MZ型の光変調器600において、2本の干渉光導波路の内の1本の光導波路について、変調用電極を含み、屈折率変調領域として機能する部分を模式的に示している。
[Embodiment 6]
9 is a diagram showing the top and side cross-sectional configurations of the optical circuit of the sixth embodiment. As an example, the diagram shows the configuration of a hybrid
光回路600は、実施形態2の光回路200と同様に、SiNコア32およびSiコア31をモード変換部40で結合した光導波路構造を有する。SiNコア32とLN薄膜12を近接することができるため、光回路200同様に、屈折率変調を効率的に生じさせることができる。
The
本実施形態の光回路600では、変調用電極30a、30bの基板厚さ方向(z方向)の位置が、SiNコア32と同一の高さにある点で、実施形態2の光回路と相違する。また、変調用電極に電気信号を印可するための、電気信号源からのボンディングワイヤ等が接続されるPAD35a、35bは、実施形態3~5と同様にLN薄膜12とは反対側のSi基板10の裏面上に形成されている。変調用電極30a、30bとPAD35a、35bの間は、TSV36a、36bによってそれぞれ接続される。
The
本実施形態の光回路600の構成によれば、変調用電極30a、30bをSiNコアの真横に、同一の高さに形成することで、LN薄膜12の内部に電界が集中しやすくなる。光回路600の構成を光変調器に適用すれば、効率的な屈折率変調が可能となる。
外部の電気信号源とPAD35a、35bは、LN薄膜12とは反対側で接続することができるので、LN薄膜12の位置を限定する必要が無く、貼り付け位置の精度は低くて良い。複数の光変調器のチップに対して、1枚のLN薄膜をSiO2層11の全面に貼り付けることもできる。
According to the configuration of the
Since the external electric signal source and the
図9の光回路600では、Si基板の裏面側にPAD35a、35bを形成した構成で、変調用電極30a、30bの基板厚さ方向の位置が、SiNコア32と同一の高さにある例を示した。しかしながら先に示した実施形態2においてPAD34a、34bが、SiO2層11の上面に作製されている場合にも、当然適用できる。ただしこの場合は、LN薄膜は、変調用電極の上側のみに限定的に張りつける必要がある。また、本実施形態の光回路600に、実施形態5のイオン注入などにより不純物を添加したSiによる変調用電極3を組み合わせることもできる。
In the
上述の各実施形態は、LN薄膜とSiPh回路を組み合わせたハイブリッド光変調器を例に説明をしたが、LN薄膜の代わりに、タンタル酸リチウム(LT)、チタン酸バリウムなどの強誘電体を利用することもできる。さらに強誘電体薄膜の電気光学効果を利用する光デバイスであれば、光変調器だけに限られない。例えば、光の偏波状態を任意に制御する偏波制御器、光の位相状態を任意に変化させる移相器などを実現可能である。偏波制御器や移相器として利用される場合、上述の強誘電体薄膜に電界を印可する電極には、変調信号ではなく、低い周波数の制御信号、一定値のDC信号などが印可され得ることに留意されたい。また偏波制御器を偏波スクランブラとして動作させる際には数GHz程度の信号となる場合もある。 In the above-mentioned embodiments, a hybrid optical modulator combining an LN thin film and a SiPh circuit has been described as an example, but instead of the LN thin film, a ferroelectric such as lithium tantalate (LT) or barium titanate can be used. Furthermore, optical devices that utilize the electro-optical effect of a ferroelectric thin film are not limited to optical modulators. For example, a polarization controller that arbitrarily controls the polarization state of light, or a phase shifter that arbitrarily changes the phase state of light can be realized. When used as a polarization controller or phase shifter, it should be noted that a low-frequency control signal, a constant-value DC signal, or the like can be applied to the electrodes that apply an electric field to the above-mentioned ferroelectric thin film, rather than a modulation signal. In addition, when the polarization controller is operated as a polarization scrambler, the signal may be on the order of several GHz.
以上、様々な実施形態で説明したように、本発明の光回路によって、強誘電体薄膜とSiPh回路を組み合わせた光回路の製造性および実装性を改善することができる。 As described above in various embodiments, the optical circuit of the present invention can improve the manufacturability and mountability of optical circuits that combine ferroelectric thin films and SiPh circuits.
本発明は、光通信に利用することができる。 This invention can be used in optical communications.
Claims (8)
前記クラッド層の内に形成されたコアと、
前記コアに沿って形成された、前記強誘電体薄膜に電界を印可する1つ以上の電極と
を備えた光回路。 An optical circuit comprising a silicon substrate, a cladding layer, and a ferroelectric thin film, arranged in that order,
a core formed within the cladding layer;
and one or more electrodes formed along the core for applying an electric field to the ferroelectric thin film.
基板面内の前記強誘電体薄膜が形成された領域内で、前記基板の厚さ方向における前記強誘電体薄膜の側に形成された窒化シリコンの第1のコア、および、
前記厚さ方向における前記第1のコアよりも前記基板の側に形成されたシリコンの第2のコアを含み、
前記第1のコアと前記第2のコアが光結合されている請求項1に記載の光回路。 The core is
a first core of silicon nitride formed on the side of the ferroelectric thin film in a thickness direction of the substrate in a region in a substrate surface where the ferroelectric thin film is formed; and
a second core of silicon formed on a side of the substrate relative to the first core in the thickness direction;
The optical circuit according to claim 1 , wherein the first core and the second core are optically coupled.
前記強誘電体薄膜は、ニオブ酸リチウム(LN)、タンタル酸リチウム(LT)、チタン酸バリウムのいずれかであり、
前記1つ以上の電極は、前記強誘電体薄膜に電気光学効果を生じさせる電気信号が与えられる請求項1乃至3いずれかに記載の光回路。 The cladding layer is made of SiO2 ,
the ferroelectric thin film is any one of lithium niobate (LN), lithium tantalate (LT), and barium titanate;
4. The optical circuit according to claim 1, wherein the one or more electrodes are supplied with an electric signal that causes an electro-optic effect in the ferroelectric thin film.
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