JPH10239547A - Optical waveguide, optical component and method of manufacturing the same - Google Patents

Abstract

(57) [Problem] To provide an optical circuit and an optical component having no polarization dependency. An optical waveguide having a core portion for transmitting light on a planar substrate and a cladding layer having a lower refractive index than the core portion, wherein an ion implantation layer is provided in the cladding layer so as to be in contact with the core portion at the bottom. Is provided.

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical waveguide, a waveguide type optical component, and a method of manufacturing the same in the fields of optical communication, optical signal processing, and optical measurement. It is for providing circuits and optical components.

[0002]

2. Description of the Related Art A silica-based optical waveguide type circuit is excellent in stability of an operating wavelength with respect to a temperature change in an optical circuit utilizing an interference effect. Therefore, the quartz type optical waveguide type circuit is a passive optical component expected to be applied in the field of optical communication.
The silica-based optical waveguide combines the technology of forming a silica-based glass film with a thickness of several μm to several tens of μm and the technology of processing the formed core glass film into a pattern shape with a width of several μm using photolithography. Produced. Various optical circuits have been realized using such optical waveguides. Among these optical circuits, the array waveguide type diffraction grating having an optical multiplexing / demultiplexing function is a practical optical component constituting an optical communication system because of its excellent degree of freedom in circuit design and low insertion loss. As promising.

FIGS. 6A to 6D show a manufacturing process of an optical waveguide used in a conventional arrayed waveguide type diffraction grating. First, as shown in FIG. 6A, a lower clad glass layer 2 is formed on a silicon substrate 1 by using a flame deposition method. Next, as shown in FIG. 6B, a core layer 4 is formed by a flame deposition method, and as shown in FIG. 6C, a photo process and reactive ion etching are performed so that the core layer 4 has a waveguide pattern. Is used to process the rectangular core portion 5. Finally, FIG.
As shown in (d), a glass layer 6 serving as an upper clad is formed by a flame deposition method, and a buried quartz optical waveguide is manufactured.

[0004] This manufacturing method has a feature that an arbitrary circuit pattern can be faithfully manufactured on a photomask. Therefore, it is suitable for manufacturing an arrayed waveguide type diffraction grating having a complicated circuit configuration having at least an arrayed waveguide portion. In addition, the waveguide length difference of the array waveguide portion, the number of input / output waveguides, and the size of the slab waveguide can be manufactured as designed, and the number of channels is 8 to 32, and the wavelength separation interval for WDM is as wide as 16 nm. 0.4nm narrow FD from the circuit
The extinction ratio of 25 dB or more, up to the M circuit,
This is realized with an insertion loss of 3 dB or less. Further, since silicon having a high thermal conductivity is used as the substrate, it is possible to control the temperature of the quartz glass constituting the waveguide by controlling the temperature of the substrate. At present, the operating wavelength of an arrayed waveguide type diffraction grating composed of a silica-based optical waveguide changes with a temperature coefficient of 0.01 nm / ° C. However, stable operation is realized by controlling the substrate temperature using a Peltier device. ing.

[0005]

However, in the conventional array waveguide type diffraction grating, since the optical waveguide has birefringence, there is a problem that the operating wavelength in the TE polarization is different from the operating wavelength in the TM polarization. was there. The cause of the birefringence of the optical waveguide is a stress induced in the glass due to the difference in the thermal expansion coefficient between the quartz glass film and the silicon substrate that constitute the optical circuit. On the other hand, when an arrayed waveguide grating is used in an optical communication system, it has been desired that the operating wavelength does not depend on the polarization state.

As a method for eliminating the polarization dependence of the operating wavelength, there is a method of forming a groove in an array waveguide and inserting a wave plate (Y. Inoue et al, "Polarization mode concer").
terwith polyimide half waveplate in silica-based p
lanar lightwave circuits ", IEEE Photonics Technol.
Lett., Vol. 6, pp. 626-628, 1994). in this way,
By inserting a wave plate in the center of the array waveguide,
It has the characteristic that the polarization dependence can be eliminated for an arrayed waveguide type diffraction grating having an arbitrary wavelength separation wavelength and an arbitrary number of channels. Additional steps of board insertion and fixing are added,
There is a problem that the manufacturing process becomes complicated. Further, such a manufacturing process is not suitable for mass production.

The present invention has been made in view of these problems, and an object of the present invention is to provide an optical waveguide, an optical component, and a method of manufacturing the same, which have no polarization dependence.

[0008]

According to a first aspect of the present invention, there is provided an optical waveguide having a core portion for transmitting light on a flat substrate and a cladding layer having a lower refractive index than the core portion. An ion implantation layer is provided so as to be in contact with the core at the bottom.

According to a second aspect of the invention, there is provided a method of manufacturing an optical waveguide.
After the lower cladding layer is provided on the flat substrate, an ion implantation layer is formed on the lower cladding layer by using an ion implantation method, a core layer is formed on the ion implantation layer, and a core portion is formed by etching. An upper clad layer is formed on the injection layer and the core to bury the core.

The ion species implanted into the ion implantation layer can be selected from the group consisting of charged particles of nitrogen, charged particles of oxygen, and charged particles of silicon.

According to a fourth aspect of the present invention, there is provided an array waveguide type diffraction grating manufactured using the optical waveguide of the first aspect.

[0012]

DESCRIPTION OF THE PREFERRED EMBODIMENTS An optical waveguide according to the present invention has a lower clad layer, an upper clad layer, a core portion, and an ion-implanted layer below the core portion on a flat substrate.

In the optical waveguide of the present invention, for example, after a lower cladding layer is provided on a flat substrate, an ion implantation layer is formed in the lower cladding layer by ion implantation, and a core layer is formed on the ion implantation layer. After the provision, the core portion is formed by etching, the upper clad layer is formed on the ion-implanted layer and the core portion, and the core portion is buried, thereby manufacturing the semiconductor device.

An arrayed waveguide type diffraction grating can be manufactured using the optical waveguide of the present invention. Further, in the present invention, by applying such an optical waveguide, other optical circuits and other optical components can be manufactured.

Hereinafter, the present invention will be described specifically with reference to examples.

Embodiment 1 FIGS. 1A to 1E show an optical waveguide manufacturing process of the present invention. First, on a silicon substrate 1, about 3
The lower clad glass layer 2 having a thickness of 0 μm is formed. next,
The surface of the lower clad glass layer 2 is ion-implanted with N
⁺ Injection layer 3 is formed. Note that the same result can be obtained by injecting charged particles of oxygen or charged particles of silicon into the ion implantation layer 3 instead of nitrogen ions. The implantation conditions are as follows: energy 300 keV, implantation amount 1 × 10 ¹⁷ /
cm ² . Under these conditions, N ⁺ ions are distributed in a Gaussian shape in the depth direction, and the concentration peak is estimated to be about 0.27 μm in depth, and the peak concentration is estimated to be 5 × 10 ²⁰ / cm ³ . Therefore, an ion implanted layer having a depth of about 0.5 μm is formed. Next, a core glass soot is deposited by a flame deposition method, and is placed in an electric furnace.
Hold at 200 ° C. for 2 hours, thickness 6 μm, refractive index difference 0.7
A core layer 4 of 5% is formed. Next, a rectangular core portion 5 having a core width of 6 μm is formed using reactive ion etching. Finally, the lower cladding layer 2 is formed using a flame deposition method.
The upper cladding layer 6 having a refractive index equal to
An optical waveguide is manufactured by a flame deposition method.

In Example 1, the flame deposition method was used for producing the glass layers 2, 6 and the glass film of the core glass soot, because this method is suitable for forming a relatively thick and high quality glass film. is there. In some cases, another method of synthesizing a glass film, for example, a CVD method or a sputtering method can be used for part or all.

Example 2 A polarization independent array waveguide type diffraction grating was fabricated using the optical waveguide of the present invention. FIG. 2 shows an outline of the circuit configuration. 7
Is an input waveguide, 8 is an input side slab waveguide, 9 is an array waveguide section, 10 is an output side slab waveguide, and 11 is an output waveguide. The optical waveguide was manufactured in the same manner as in Example 1.
In designing the optical multiplexing / demultiplexing operation, an array waveguide type diffraction grating is configured so that a wavelength interval of 0.4 nm (optical frequency interval of 50 GHz) can be obtained for 16 channels in a wavelength band of 1.55 μm used in optical communication. The optical path length difference between the channel waveguides was 126.4 μm. To operate this array waveguide type diffraction grating as an optical multiplexer / demultiplexer,
First, a transmission-side single-mode optical fiber is connected to the input waveguide, and frequency-multiplexed signal light (λ _{-j to} λ _j ) is incident. The signal light spread due to the diffraction effect in the input side slab waveguide propagates to a plurality of array waveguides constituting an arrayed waveguide type diffraction grating, reaches the output side waveguide slab, and is further condensed in the output waveguide. You. In this case, by changing the lengths of the individual array waveguides constituting the array waveguide type diffraction grating and providing the optical path length difference, the phase of the signal light after the propagation of the array waveguide is shifted, and this phase shift amount Accordingly, the wavefront of the focused light in the output side slab waveguide is inclined. The light condensing position is determined by the inclination angle. The amount of phase shift depends on the signal light frequency, and the focus position of the frequency multiplexed light is determined for each frequency. By arranging an output waveguide at the focus position, the signal light (λ _{j to} λ _{− j} ) can be taken out.

FIG. 3 shows the result of measurement of the transmission spectrum of this optical multiplexer / demultiplexer near a wavelength of 1.5 μm. This proved that the transmission wavelength did not depend on the polarization state of TE or TM. Further, the insertion loss at the peak wavelength is 3.
0 dB, crosstalk between channels is 25 dB,
It has been found that the transmission characteristics are equivalent to those of an arrayed waveguide grating manufactured by a conventional manufacturing method.

As described above, it was possible to realize an arrayed waveguide type diffraction grating using the optical waveguide of the present invention and having a low loss and a high extinction ratio without polarization dependence.

In order to clarify the temperature stability of the polarization independent array waveguide type diffraction grating of the present invention, TE polarization and T
FIG. 4 shows the temperature dependence of the transmission wavelength in the M polarization. FIG. 4 shows the results when the arrayed waveguide type diffraction grating was held at a predetermined temperature in an electric furnace for 1 hour and then measured at room temperature. From this, it was found that the polarization independent operation of the arrayed waveguide type diffraction grating was guaranteed at 1200 ° C. or less, and that long-term reliability was high. This is a step of forming a core glass on the ion-implanted layer by a flame deposition method.
This is because the sintering process has been performed at ℃ and the ion-implanted layer is embedded in the clad glass.

In the second embodiment, an arrayed waveguide type diffraction grating was manufactured. In addition, the present invention can be applied to an optical circuit using optical interference, for example, a Mach-Zehnder type multiplexer / demultiplexer, a photo-induced grating, etc. It is also effective to apply the present invention to a directional coupler, a Y-branch, or the like using optical branching coupling.

Comparative Example 1 An optical circuit was manufactured by a conventional method without ion implantation, and an optical demultiplexer designed in the same manner as in Example 1 was manufactured using the optical circuit. When the transmission spectrum of this was measured, the result of FIG. 5 was obtained. From this result, two polarizations (T
E, TM) has a transmission spectrum of about 0.
It was found that there was a 2 nm shift polarization dependence. Comparative Example 1
By comparing with the result of Example 1, the effect of ion implantation shown in Example 1 could be confirmed.

[0024]

As described above, according to the optical waveguide of the present invention, by providing the ion implantation layer on the bottom surface of the core by using the ion implantation method, the stress field near the core glass can be changed or the ion field can be reduced. A change in the refractive index of the injection layer is induced, and the polarization dependence of the multiplexing / demultiplexing characteristics of the arbitrarily designed arrayed waveguide type diffraction grating can be eliminated. Further, the ion-implanted layer is formed by being buried in the glass, and the non-polarization operation is maintained semipermanently. Further, since the ion-implanted layer formed by the ion-implantation method is optically homogeneous glass, the ion-implanted layer does not cause loss of the optical waveguide and deterioration of the extinction ratio. In addition, the manufacturing of the optical circuit according to the present invention merely adds an ion implantation step to the manufacturing process of the conventional waveguide type optical circuit, and the complexity of the manufacturing process can be minimized. Note that the ion implantation method is widely used in the LSI process and is a technique suitable for mass production. Therefore,
The optical waveguide of the present invention can be mass-produced, which is advantageous in cost.

[Brief description of the drawings]

FIG. 1 is a sectional view of an optical waveguide showing an optical waveguide manufacturing process of the present invention.

FIG. 2 is a diagram showing a circuit configuration of an arrayed waveguide type diffraction grating of the present invention.

FIG. 3 is a graph showing transmission characteristics of the arrayed waveguide grating of the present invention.

FIG. 4 is a graph showing the polarization dependence of the array waveguide type diffraction grating of the present invention with respect to temperature change.

FIG. 5 is a graph showing transmission characteristics of an arrayed waveguide grating for comparison.

FIG. 6 is a cross-sectional view of an optical waveguide showing a conventional optical waveguide manufacturing process.

[Explanation of symbols]

 DESCRIPTION OF SYMBOLS 1 Silicon substrate 2 Lower cladding layer 3 Ion implantation layer 4 Core layer 5 Core part 6 Upper cladding layer 7 Input waveguide 8 Input side slab waveguide 9 Array waveguide part 10 Output side slab waveguide 11 Output waveguide

Claims (4)

[Claims] An optical waveguide having a core portion for transmitting light on a planar substrate and a cladding layer having a lower refractive index than the core portion, wherein the optical waveguide is in contact with the core portion at a bottom portion in the cladding layer. An optical waveguide comprising an ion implantation layer. 2. After a lower cladding layer is provided on a planar substrate, an ion implantation layer is formed in the lower cladding layer by ion implantation, and a core layer is provided on the ion implantation layer, and then a core is formed by etching. Forming a portion, forming an upper cladding layer on the ion-implanted layer and the core portion, and burying the core portion. 3. The optical waveguide according to claim 2, wherein the ion species implanted into the ion implantation layer is selected from the group consisting of charged particles of nitrogen, charged particles of oxygen, and charged particles of silicon. Manufacturing method. 4. An array waveguide type diffraction grating manufactured using the optical waveguide according to claim 1.