Silicon nitride broadband optical switch
Technical Field
The invention relates to the technical field of integrated optoelectronic devices, in particular to a silicon nitride broadband optical switch.
Background
The optical switch is used as a basic unit of optical communication and widely applied to the fields of optical delay lines, laser radars, optical neural networks and the like. Mach-zehnder interferometer (MZI) optical switches are widely used in integrated photonic systems due to their large process tolerance and compact structure. However, the coupling effect of the optical power coupler in the existing MZI optical switch is affected by the wavelength change, and it is difficult to maintain the 3dB optical splitting effect in a wider operating bandwidth, so that it is important to research a broadband optical switch for an integrated photonic system with a larger optical bandwidth requirement.
Multimode interference couplers (MMI) and Directional Couplers (DC) are commonly used 3dB couplers in MZIs, but they cause unexpected reflection to the light source, and the directional couplers have strong wavelength dependence due to the dispersion of the waveguide, which ultimately leads to the non-ideal use of MZIs. In the silicon waveguide, an integrated Variable Optical Attenuator (VOA) can be adopted to make up the extinction ratio and suppress crosstalk, but due to the particularity of the silicon nitride waveguide, the VOA cannot be integrated, so that the extinction ratio in the working bandwidth of the silicon nitride optical switch directly determines whether the silicon nitride optical switch can be applied to a silicon nitride optical subsystem or not.
The loss of the silicon nitride waveguide has obvious advantages compared with the silicon waveguide, so that the silicon nitride broadband optical switch is more and more important when the silicon nitride broadband optical switch is applied to more and more extensive silicon nitride delay lines and silicon nitride phased array radar systems. Compared with the silicon nitride, the silicon nitride can bear higher optical power without obvious nonlinear effect, and the waveguide loss is lower, but the silicon nitride is suitable for passive devices, and the silicon nitride optical switch cannot be integrated with a variable optical attenuator to make up the extinction ratio.
Disclosure of Invention
The invention provides a silicon nitride broadband optical switch, which solves the problem that silicon nitride materials cannot integrate an adjustable optical attenuator to make up the extinction ratio.
The technical scheme adopted by the invention for solving the technical problems is as follows: the silicon nitride broadband optical switch comprises a first 3dB asymmetric adiabatic coupler, a second 3dB asymmetric adiabatic coupler, an interference arm waveguide, a reference arm waveguide and a thermal phase shifter; the first 3dB asymmetric adiabatic coupler and the second 3dB asymmetric adiabatic coupler have the same structure and respectively comprise a first waveguide part, a coupling region part and a second waveguide part which are sequentially connected, wherein the first waveguide part is of an asymmetric structure; a first end of the second waveguide section of the first 3dB adiabatic asymmetric coupler is connected to a second end of the second waveguide section of the second 3dB adiabatic asymmetric coupler by the interference arm waveguide, and a second end of the second waveguide section of the first 3dB adiabatic asymmetric coupler is connected to a first end of the second waveguide section of the second 3dB adiabatic asymmetric coupler by the reference arm waveguide; the interference arm waveguide and the reference arm waveguide are silicon nitride waveguides with equal length, and the thermal phase shifter is arranged on the interference arm waveguide.
The thickness of the interference arm waveguide, the reference arm waveguide and the second waveguide part is 0.8um, and the width is 1 um.
The waveguide width at the first end of the first waveguide section is not equal to the waveguide width at the second end.
The ratio of the waveguide width at the first end to the waveguide width at the second end of the first waveguide section is 1: 2.
The waveguide width of the first end of the first waveguide portion is 0.5um, and the waveguide width of the second end is 1 um.
The length of the interference arm waveguide and the reference arm waveguide is 750 um.
The thermal phase shifter adopts the aluminium electrode to heat, the width of aluminium electrode is 1.4um, and thickness is 0.4 um.
The thermal phase shifter is located 1.7um above the interference arm waveguide, and the total length of the thermal phase shifter is 750 um.
Advantageous effects
Due to the adoption of the technical scheme, compared with the prior art, the invention has the following advantages and positive effects: the silicon nitride waveguide is adopted, and compared with the silicon waveguide, the silicon nitride waveguide has lower loss and has greater advantages in a delay line and a laser radar. The invention adopts the 3dB asymmetric adiabatic coupler to ensure that the wavelength sensitivity is low, the silicon nitride waveguide can not be electrically adjusted, so that an adjustable optical attenuator can not be integrated to make up the extinction ratio, and the working bandwidth of the silicon nitride optical switch is limited. The invention adopts an asymmetric structure to reduce the length of the coupling part of the adiabatic coupler, and can reduce the volume of the whole optical device.
Drawings
FIG. 1 is a schematic structural diagram of an embodiment of the present invention;
FIG. 2 is a schematic diagram of a 3dB asymmetric adiabatic coupler according to an embodiment of the present invention;
FIG. 3 is a field strength transmission diagram for a 3dB asymmetric adiabatic coupler in an embodiment of the present invention;
FIG. 4 is a wavelength scan of a 3dB asymmetric adiabatic coupler in an embodiment of the present invention;
FIG. 5 is a schematic cross-sectional view of a thermal phase shifter according to an embodiment of the present invention;
FIG. 6 is a graph of field strength distribution when a thermal phase shifter is heated to Pi phase shift in an embodiment of the present invention;
FIG. 7 is a graph of the optical field intensity propagation for an embodiment of the present invention with a phase shift of 0;
FIG. 8 is a graph of extinction ratio versus wavelength for an embodiment of the present invention.
Detailed Description
The invention will be further illustrated with reference to the following specific examples. It should be understood that these examples are for illustrative purposes only and are not intended to limit the scope of the present invention. Further, it should be understood that various changes or modifications of the present invention may be made by those skilled in the art after reading the teaching of the present invention, and such equivalents may fall within the scope of the present invention as defined in the appended claims.
Embodiments of the present invention relate to a silicon nitride broadband optical switch, as shown in fig. 1, comprising a first 3dB asymmetric adiabatic coupler 1, a second 3dB asymmetric adiabatic coupler 2, an interference arm waveguide 3, a reference arm waveguide 4, and a thermal phase shifter 5.
As shown in fig. 2, the first 3dB asymmetric adiabatic coupler 1 and the second 3dB asymmetric adiabatic coupler 2 have the same structure, and each includes a first waveguide portion a, a coupling region portion B, and a second waveguide portion C, which are connected in sequence, where the first waveguide portion a has an asymmetric structure. In this embodiment, the ratio of the waveguide width W1 at the first end of the first waveguide portion a to the waveguide width W2 at the second end is 1:2, for example, the waveguide width W1 at the first end of the first waveguide portion a is 0.5um, and the waveguide width W2 at the second end is 1um, in this embodiment, the widths at the two ends of the first waveguide portion a are designed to be different, so that mode mismatch is generated, and the wavelength sensitivity is reduced, fig. 3 is a field intensity transmission diagram of a 3dB asymmetric adiabatic coupler in the embodiment of the present invention, and fig. 4 is a wavelength scanning diagram of a 3dB asymmetric adiabatic coupler in the embodiment of the present invention. As can be seen from fig. 4, the sensitivity to wavelength is significantly reduced and the operating bandwidth is significantly increased due to the mode mismatch generated by the asymmetric design.
The first end C1 of the second waveguide section C of the first 3dB asymmetric adiabatic coupler 1 is connected to the second end C2 of the second waveguide section C of the second 3dB asymmetric adiabatic coupler 2 through the interference arm waveguide 3, and the second end C2 of the second waveguide section C of the first 3dB asymmetric adiabatic coupler 1 is connected to the first end C1 of the second waveguide section C of the second 3dB asymmetric adiabatic coupler 2 through the reference arm waveguide 4; the interference arm waveguide 3 and the reference arm waveguide 4 are silicon nitride waveguides with equal length, and the thermal phase shifter 5 is arranged on the interference arm waveguide 3. It can be found that the silicon nitride broadband optical switch of the present embodiment has asymmetric adiabatic couplers on the left and right sides, the phase modulation is performed in the middle by a thermal phase shifter, the adiabatic couplers on both sides can cancel out the phase difference caused by asymmetry by antisymmetric connection, and the coupling part length of the adiabatic coupler is reduced by adopting an asymmetric structure.
In the present embodiment, the thickness of the interference arm waveguide 3, the reference arm waveguide 4, the second waveguide portion C is 0.8um, the width is 1um, and the length of the interference arm waveguide 3 and the reference arm waveguide 4 is 750 um.
As shown in fig. 5, the thermal phase shifter 5 in the present embodiment is heated using an aluminum electrode having a width of 1.4um and a thickness of 0.4 um. The aluminium electrode is located 1.7um department above the arm waveguide of interfering (being carborundum waveguide), the total length that hot phase shifter 5 was the same with interfering arm waveguide 3, is 750 um. FIG. 6 is a diagram showing the distribution of the field strength when the thermal phase shifter is heated to Pi phase shift, and the phase difference between the two arms is realized by heating to generate the optical path switching, in this embodiment, the Pi phase shift power is 0.135W.
Fig. 7 is a diagram of the propagation of the optical field intensity at a phase shift of 0 according to an embodiment of the present invention. FIG. 8 is a graph of extinction ratio versus wavelength for an embodiment of the present invention. It can be seen that the extinction ratio of the silicon nitride broadband optical switch of the present embodiment is greater than 20dB in a large bandwidth range of 130nm or more in the c-band, and the extinction ratio of the silicon nitride broadband optical switch of the present embodiment exceeds 40dB in the vicinity of 1550nm, by the design of the present embodiment.
As can be easily found, the silicon nitride waveguide adopted by the invention has lower loss compared with the silicon waveguide and has greater advantages in delay lines and laser radars. The invention adopts the 3dB asymmetric adiabatic coupler to ensure that the wavelength sensitivity is low, the silicon nitride waveguide can not be electrically adjusted, so that an adjustable optical attenuator can not be integrated to make up the extinction ratio, and the working bandwidth of the silicon nitride optical switch is limited. The invention adopts an asymmetric structure to reduce the length of the coupling part of the adiabatic coupler, and can reduce the volume of the whole optical device.