The present invention relates to an optical fiber array in which core end surfaces of a plurality of optical fibers are aligned and disposed with a predetermined core pitch.
Smaller and more advanced optical modules have been actively researched and developed to increase a communication capacity per device of optical communication devices. Examples of promising technologies for this purpose include silicon photonics (SiP) technology.
SiP technology is a technique for optical circuits using silicon (Si) as a core material and silica glass (SiO2) as a cladding material. Hereinafter, when referring to the optical waveguide of an optical circuit, it is referred to as a Si waveguide, and when referring to the entire optical circuit chip, it is referred to as a SiP circuit. Because the Si waveguide has a large refractive index contrast between a core and a cladding, a cross-sectional area of the waveguide and a minimum bending radius can be made significantly smaller than that of optical circuits formed of other materials, which enables high density integrated optical circuits.
In order to actually modularize and make the SiP circuit usable, it is necessary to bundle a plurality of optical fibers for input/output as an optical fiber array and to connect and fix it to an end surface of the optical waveguide of the SiP circuit.
In
A SiP circuit 107 is an optical circuit optically coupled and connected to the fiber array 101 and has a plurality of Si waveguides 108 near a surface of the SiP circuit as input/output waveguides for transmitting and receiving optical signals in correspondence with the optical fibers 104.
The SiP circuit 107 is bonded to the fiber array 101 with an optical adhesive or the like having a high transmittance for light in a communication wavelength band, and a core end surface of each of the Si waveguides 108 is disposed to be aligned with a core end surface of each of the optical fibers 104 of the fiber array 101 and is optically coupled thereto.
Accuracy required for optical axis alignment at a connection portion between the SiP circuit 107 and the fiber array 101 depends on a mode field diameter (MFD: an index representing the spread of optical power distribution in a cross section of a light beam) of the light at the connection portion. As the MFD becomes smaller, the deterioration of connection loss with respect to the same optical axis misalignment increases, and thus the accuracy requirement becomes more severe.
PTL 1: JP 2001-228345 A
However, the present inventors have found that even when the alignment between the core of the optical fiber and the Si waveguide can be performed with high accuracy, there are the following problems.
In
A two-dot dashed line 301 shows a position of the core in a Si waveguide 108 at a depth in the substrate cross section of the SiP circuit 107, and passes through the position of the core of the optical fiber 104 in a state in which there is no misalignment in
In the SiP circuit 107, because the Si waveguide 108 is located at a position very close to a substrate surface of the SiP circuit 107, which is at most within 10 μm, generally about 4 μm, from a substrate surface of the SiP circuit 107, the circuit surface does not reach an upper end of a cross section of a fiber.
Thus, when the fiber array 101 and the SiP circuit 107 are bonded by an optical adhesive 302, a region over which the optical adhesive 302 spreads is within a region 302 indicated by an alternated long and short dash line in
Here, in
In
Cited PTL 1 describes a structure in which a plate-covered glass for polishing reinforcement is adhered onto a silica planar lightwave circuit (PLC) which is an optical circuit containing silica glass as a main component. This is a commonly used structure for silica PLC today, and it is conceivable that this structure not only helps to reinforce during polishing, but also contributes to suppression of the optical axis misalignment because the entire surface of the fiber array including the pressing plate and the optical circuit are adhered to each other.
However, in the case of the SiP circuit 107, a circuit size is several millimeters square which is smaller than that of the silica PLC, and thus it is difficult to bond such a reinforcing glass plate to only a connection portion with the fiber array 101. In addition, in the SiP circuit 107, an electrode for driving a circuit element such as a modulator needs to be exposed on the surface thereof, and thus it is not possible to cover a chip surface with the reinforcing glass plate. In such circumstances, this structure is difficult to be applied to the SiP circuit 107.
In other words, because the SiP circuit 107 has a peculiar circumstance where only the V-groove substrate 102 is bonded and fixed in addition to the connection loss being sensitive to misalignment, the connection loss unfortunately increases and worsens due to the thermal expansion of the adhesive in the V-groove.
The present invention has been made in view of such problems, and an object thereof is to provide an optical fiber array which is optically coupled to a SiP circuit and is capable of suppressing a misalignment between a waveguide and a core of an optical fiber when a temperature varies and reducing temperature dependency of connection loss.
Examples of embodiments of the present invention include the following configurations to achieve the above object.
An optical fiber array including:
a V-groove substrate in which a V-groove for optical fiber alignment is formed;
The optical fiber array of Configuration 1, wherein a half angle θ of an opening angle of the V-groove satisfies
θ>sin −1(r/(r+20))
The optical fiber array of Configuration 1, wherein
The optical fiber array of Configuration 1, wherein
A method for forming a V-groove in a V-groove substrate of an optical fiber array, the method including:
According to the optical fiber array of the present invention described above, it is possible to provide an optical fiber array which is optically coupled to a SiP circuit and is capable of suppressing a misalignment between a waveguide and a core of an optical fiber when a temperature varies and reducing temperature dependency of connection loss.
Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.
First, because a misalignment of an optical axis between a Si waveguide and an optical fiber is caused by expansion of an adhesive between the optical fiber and a V-groove, it is necessary to reduce a thickness of the adhesive at the corresponding portion.
In the following Embodiment 1 to 3, as shown in
It is assumed that an operating temperature range to be considered is from −5° C. to 85° C. In addition, because a linear expansion coefficient of the adhesive used when the optical fiber array is assembled is at most 10−4 [K−1], it is preferable that d be less than 20 μm.
In this way, the expansion of the adhesive, that is, a displacement in which the fiber is pushed up is suppressed to less than 0.18 μm at the most, and a variation in the connection loss is less than 0.04 dB from
As shown in
d=r(1/ sin θ−1)
From a condition of d<20 μm,
θ>sin −1(r/(r+20)) Expression (1)
is obtained. This gives a condition of the opening angle of the V-groove 403.
In the case of a fiber with r=62.5 μm, it is required that θ>49.25°, that is, the opening angle is greater than 98.5°.
In this way, the distance d of a portion of the adhesive 106 which is located between the optical fiber 104 and the V-groove 403 on the lower side of the optical fiber 104 can be less than 20 μm, and a fiber array with a sufficiently small temperature variation in the connection loss with respect to the SiP circuit can be obtained.
In Embodiment 2 of
Similarly, let θ be a half of the opening angle of the V-groove 503, and let r1 [μm] be the radius of the optical fiber. When the radius of curvature of the tip end of the V-groove is r2 [μm], d is expressed by the following equation.
d=(r1−r2)(1/sin θ−1) Expression (2)
From 0 μm<d<20 μm,
r1−20 sin θ/(1−sin θ)<r2≤r1 Expression (3)
is obtained for a condition of r2.
In the case of r1=62.5 μm and θ=30°, the relationship 42.5 μm<r2≤62.5 μm is derived. When a V-groove shape satisfies this condition, a fiber array in which the temperature variation of the connection loss with respect to the SiP circuit is sufficiently small can be obtained.
In particular, when a radius of curvature of the tip end of the V-groove is equal to a radius of the optical fiber 104 (r2=r1), a thickness d of the adhesive 106 which causes the optical fiber 104 to rise due to expansion can be minimized.
In Embodiment 3 of
At this time, the following equation is derived.
d=r(1/sin θ−1)−w/2 tan θ Expression (4)
From d<20 μm,
w>2 tan θ{r(1/sin θ−1)−20} Expression (5)
is obtained for a condition of w.
When r=62.5 μm and 0=30°, the relationship w>49.1 μm is obtained.
When a cross-sectional shape of the V-groove satisfies this condition, a fiber array in which the temperature variation of the connection loss with respect to the SiP circuit is sufficiently small can be obtained.
A shape of the V-groove 603 of Embodiment 3 is suitable for producing a V-groove substrate by pressing instead of directly grinding the substrate with a blade to form a V-groove.
In other words, as shown in the steps of forming the V-groove of Embodiment 3 of
Then, molding is performed using the mold 700. Molding is performed by forming a release film on the mold in advance and then applying pressure, by the mold 700, to glass preform 702 which is heated. After molding, cooling is performed while a pressing force is reduced, and a completed V-groove substrate on which the V-groove 703 is formed is taken out from the mold.
As described above, according to the optical fiber array of the present invention, it is possible to provide an optical fiber array which can suppress a misalignment between a waveguide and a core of an optical fiber when a temperature varies in a SiP circuit, and can reduce temperature dependency of connection loss.
Filing Document | Filing Date | Country | Kind |
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PCT/JP2019/046637 | 11/28/2019 | WO |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2021/106163 | 6/3/2021 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
5737138 | Someno | Apr 1998 | A |
20050129380 | Takeuchi | Jun 2005 | A1 |
Number | Date | Country |
---|---|---|
H09-54222 | Feb 1997 | JP |
H11-305058 | Nov 1999 | JP |
2001-228345 | Aug 2001 | JP |
2003-337245 | Nov 2003 | JP |
2004-245853 | Sep 2004 | JP |
Number | Date | Country | |
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20220413223 A1 | Dec 2022 | US |