Modern technology advances, such as big data, cloud computation, cloud storage, and Internet of Things (IoT), have driven exponential growth of various applications in processing and communications of data, e.g., high performance computers, data centers, and long-haul telecommunication. To address the emerging need of high data rate transmission, a modern semiconductor structure may include optical elements for providing optical data links to improve the data transmission rate of existing electrical data links. In the development of incorporating optical data links to the semiconductor device, the challenge of reducing device size of the optical data links has attracted a great deal of attention.
Aspects of the embodiments of the present disclosure are best understood from the following detailed description when read with the accompanying figures. It is noted that, in accordance with the standard practice in the industry, various structures are not drawn to scale. In fact, the dimensions of the various structures may be arbitrarily increased or reduced for clarity of discussion.
The following disclosure provides many different embodiments, or examples, for implementing different features of the provided subject matter. Specific examples of components and arrangements are described below to simplify the present disclosure. These are, of course, merely examples and are not intended to be limiting. For example, the formation of a first feature over or on a second feature in the description that follows may include embodiments in which the first and second features are formed in direct contact, and may also include embodiments in which additional features may be formed between the first and second features, such that the first and second features may not be in direct contact. In addition, the present disclosure may repeat reference numerals and/or letters in the various examples. This repetition is for the purpose of simplicity and clarity and does not in itself dictate a relationship between the various embodiments and/or configurations discussed.
Further, spatially relative terms, such as “beneath,” “below,” “lower,” “above,” “over,” “upper,” “on,” and the like, may be used herein for ease of description to describe one element or feature's relationship to another element(s) or feature(s) as illustrated in the figures. The spatially relative terms are intended to encompass different orientations of the device in use or operation in addition to the orientation depicted in the figures. The apparatus may be otherwise oriented (rotated 90 degrees or at other orientations) and the spatially relative descriptors used herein may likewise be interpreted accordingly.
As used herein, although the terms such as “first,” “second” and “third” describe various elements, components, regions, layers and/or sections, these elements, components, regions, layers and/or sections should not be limited by these terms. These terms may be only used to distinguish one element, component, region, layer or section from another. The terms such as “first,” “second” and “third” when used herein do not imply a sequence or order unless clearly indicated by the context.
Notwithstanding that the numerical ranges and parameters setting forth the broad scope of the disclosure are approximations, the numerical values set forth in the specific examples are reported as precisely as possible. Any numerical value, however, inherently contains certain errors necessarily resulting from the deviation normally found in the respective testing measurements. Also, as used herein, the terms “about,” “substantial” or “substantially” generally mean within 10%, 5%, 1% or 0.5% of a given value or range. Alternatively, the terms “about,” “substantial” or “substantially” mean within an acceptable standard error of the mean when considered by one of ordinary skill in the art. Other than in the operating/working examples, or unless otherwise expressly specified, all of the numerical ranges, amounts, values and percentages such as those for quantities of materials, durations of times, temperatures, operating conditions, ratios of amounts, and the likes thereof disclosed herein should be understood as modified in all instances by the terms “about,” “substantial” or “substantially.” Accordingly, unless indicated to the contrary, the numerical parameters set forth in the present disclosure and attached claims are approximations that can vary as desired. At the very least, each numerical parameter should at least be construed in light of the number of reported significant digits and by applying ordinary rounding techniques. Ranges can be expressed herein as being from one endpoint to another endpoint or between two endpoints. All ranges disclosed herein are inclusive of the endpoints, unless specified otherwise.
Embodiments of the present disclosure an optical edge coupler and a method of forming the optical edge coupler. Modern optical waveguides and optical edge couplers may be implemented with a silicon-based material due to its low transmission loss and compatibility with existing semiconductor fabrication processes. The edge coupler is useful in a photonic transmission/receiving system since it is used to convert the light beam from an optical fiber with a light field diameter of about 10 μm to a light beam traveling in a waveguide with the light field diameter less than that of the optical fiber, about 1 μm. Further, a typical edge coupler may have a coupling length up to hundreds of μm. As a result, the task of device size miniaturization becomes very challenging for incorporating the optical device into the semiconductor devices with smaller size. Further, polarization-dependent loss of the edge coupler due to mode mismatch is commonly observed due to design constraints. Therefore, the light coupling performance of the edge coupler may be compromised by the device size.
The present disclosure proposes a dual-member edge coupler to effectively enhancing the light coupling performance of the edge coupler. The proposed edge coupler incorporates two edge coupling members with different coupling design used for individually optimizing the coupling performance of the transverse electric (TE) and transverse magnetic (TM) modes of the light beam. Further, auxiliary edge couplers are also adopted to enhance the light coupling performance. As a result, the coupling performance of the edge coupler is improved while the coupling length of the edge coupler can be reduced by about one half.
The photonic system 10 may include an optical source 102, an optical fiber 104 and a photonic device 100. In some embodiments, the optical source 102 is configured to generate a light beam, e.g., with a wavelength centered at 850 nm, 1310 nm or 1550 nm. The optical source 102 may be a laser diode or a light-emitting diode. In some embodiments, the optical fiber 104 is configured to transmit the light beam to the photonic device 100. The optical fiber 104 may include a core component (not separately shown) and a cladding layer (not separately shown) wrapping around the core component, in which the light beam is allowed to propagate in the core component. The materials of the core component and the cladding layer may be determined to cause the light beam to travel in the optical fiber with minimal transmission loss. In some embodiments, the core component is made of a silica-based or plastic material, and the cladding layer is formed of, e.g., fluorinated polymer. In some embodiments, the optical fiber 104 includes an outer coating layer or a jacket layer (not separately shown) for providing additional cladding and/or protection functions. In some embodiments, the optical fiber 104 is classified into a single-mode optical fiber and a multimode optical fiber. In the depicted example, the optical fiber 104 is a single-mode optical fiber.
The photonic device 100 may include an input-stage edge coupler 106, a grating coupler 108, a splitter 110, an optical modulator 120, a grating coupler 130, and an output-stage edge coupler 114. In some embodiments, some of the abovementioned elements can be omitted, or additional optical elements can be added to the photonic device 100 where appropriate. The input-stage edge coupler 106 may be used to couple the incoming light beam from the optical fiber 104 to the photonic device 100, e.g., the grating coupler 108 of the photonic device 100. In some embodiments, the input-stage edge coupler 106 directs the light beam from a sidewall of the input-stage edge coupler 106 or a substrate of the photonic device 100 for facilitating processing of the light beam in the photonic device 100.
The grating coupler 108 is configured to couple the light beam from the optical fiber 104 or the input-stage edge coupler 106 to a waveguide of the splitter 110. In some embodiments, the grating coupler 108 includes an array of trenches or grooves on a surface of a waveguide of the grating coupler 108 to form a diffractive optical structure, which can help change the off-plane wave-vector direction of the light beam into an in-plane wave-vector direction of the waveguide of the splitter 110. The coupling efficiency of the grating coupler 108 may be related to the grating pitch, the grating depth, and the tilt angle and relative position of the input light beam, e.g., the tilt angle and the position of the incoming light beam are determined through tuning of the input-stage edge coupler 106.
In some embodiments, the grating coupler 108 is omitted, and the input-stage edge coupler 106 is coupled directly to the splitter 110 or subsequent optical devices.
In some embodiments, the splitter 110 is configured to spit the incoming light beam into two or more light beams. The split light beams may be processed with various functions to include different optical properties, and may be combined in a later stage.
In some embodiments, one of the split light beams is fed into the optical modulator 120. The optical modulator 120 may perform electro-optical phase modulation to change the delay or the phase of the incoming light beam. After the processing of the optical modulator 120, the modulated light beam may become an information-bearing light beam to carry data in optical form. Alternatively, the optical modulator 120 may serve the function of optical calibration to adjust the phase or delay of the split light beams before they are combined in a subsequent stage.
After modulated or calibrated by the optical modulator 120, the light beam is transmitted to the grating coupler 130. The grating coupler 130 is configured to couple the light beam from a waveguide of the optical modulator 120 to the output-stage edge coupler 114. In some embodiments, the grating coupler 130 includes an array of trenches or grooves on a surface of a waveguide of the grating coupler 130 to form a diffractive optical structure, which can help change the an in-plane wave vector direction in the waveguide of the optical modulator 120 to an off-plane wave-vector direction for the output-stage edge coupler 114. The coupling efficiency of the grating coupler 130 may be related to the grating pitch, the grating depth, and the tilt angle and relative position of the output light beam, e.g., the tilt angle and the position of the outgoing light beam are determined through arrangement of the output-stage edge coupler 114. In some embodiments, the parameters of the grating coupler 130 is similar to or different from those of the grating coupler 108.
In some embodiments, the grating coupler 130 is omitted, and the output-stage edge coupler 114 directly couples the optical modulator 120 to an output device.
The output-stage edge coupler 114 may be used to couple the incoming light beam from the photonic device 100, e.g., the grating coupler 130, to an output device, e.g., another optical fiber. In some embodiments, the output-stage edge coupler 114 directs the light beam the light beam from the grating coupler 130 to a sidewall of the output-stage edge coupler 114 or a sidewall of a substrate in the photonic device 100 for facilitating processing of the light beam external to the photonic device 100.
Referring to
In some embodiments, the edge coupler 106 is arranged in a substrate (not shown in
In some embodiments, the edge coupler 106 extends in a direction, e.g., along the X-axis, different from, e.g., perpendicular to, the direction of the sidewall 106S, e.g., along the Y-axis. The edge coupler 106 may have a varying width W measured in a direction along the Y-axis and a uniform length Lt measured in a direction along the X-axis.
In some embodiments, the edge coupler 106 includes two edge coupling members 202 and 204 stacked over one another in the vertical direction, e.g., along the Z-axis. In some embodiments, each of the edge coupling members 202, 204 alone can be regarded as an edge coupler. The edge coupling members 202 and 204 may be formed of the same or different materials. The edge coupling members 202 and 204 each function as an independent edge couplers but with different coupling properties. In some embodiments, the edge coupling members 202 and 204 are configured to couple the input light beam from the optical fiber 104 to the waveguide 112 through the transverse electric (TE) mode and the transverse magnetic (TM) mode, respectively, of the light beam, or alternatively, through the TM mode and the TE mode, respectively.
As shown in
In some embodiments, the sides 202S1, 202S2, 204S1, 204S2 are at least partially non-linear from a top-view perspective. In some embodiments, each of the sides 202S1, 202S2, 204S1, 204S2 is overall curved or non-linear from a top-view perspective. On the one hand, the single-tip edge coupler 106 is used to convert the optical mode of the light beam from the larger-sized optical fiber 104 to the smaller-sized waveguide 112, and therefore the width W1 or W2 of the edge coupling members 202, 204 should be made progressively increased or equal (or monotonically non-decreasing) along the longitudinal direction of the edge coupling member 202 or 204. On the other hand, the energy of the light beam is concentrated in one or more dominant optical components corresponding to one or more critical coupling width Wc. Therefore, the coupling efficiency of the edge coupling members 202, 204 would be determined based on whether the range of the width W1 or W2 of the respective edge coupling member 202 or 204 includes the critical widths Wc. The greater percentage the critical widths Wc is included, the better optical coupling performance the edge coupling member 202 or 204 will achieve. Based on the foregoing, since the coupling performance of the edge coupling members 202, 204 is determined by the critical width Wc, the coupling performance of the edge coupling members 202, 204 would be determined by the distribution of the width W1 or W2, i.e., the shapes of the lateral sides 202S1, 202S2, 204S1, 204S2.
In some embodiments, as discussed previously, the width W1 or W2 progressively increases from the first end 106A to the second end 106B. In some embodiments, the width W1 or W2 has a minimal value Wt at the sidewall 106S or the first end 106A. In some embodiments, the width W1 or W2 has a maximal value Ww at the second end 106B or the sidewall of the waveguide 112. In some embodiments, the width Ww is substantially equal to the width of the waveguide 112.
In Equation (1) above, the argument z represents the horizontal location along the X-axis, the output W represents the width W1 or W2 obtained through Equation (1) given different ranges of the exponent a. The lateral sides can be obtained through the width W directly. In Equation (1), the constant Wt represents the initial width at the first end 106A, and the constant Ww represents the final width at the second end 106B. The exponent a determines the type and level of curvature of the lateral side expressed by Equation (1).
In some embodiments, each of the edge coupling members 202, 204 has a width W measured in the direction of Y-axis monotonically non-decreasing in the direction of X-axis. In some embodiments, one of the edge coupling members 202, 204 includes at least a portion in a concave shape, and the other of the edge coupling members 202, 204 includes at least a portion in a convex shape. In some embodiments, the edge coupling member 204 is fully overlapped with the edge coupling member 202.
In some embodiments, as illustrated in
In some embodiments, since the polarization-dependent loss observed during the optical coupling of the edge coupler 106 may cause noticeable coupling loss, and the edge coupler 106 with a single edge coupling member 202 or 204 can only be optimized for only either the TE mode or the TM mode, the coupling performance would not be enhanced significantly. As such, the dual-member design of the edge coupler 106 uses the edge coupling members 202 and 204 to receive and guide the light beam components in the TE mode and TM mode separately. Since the critical widths Wc's for the TE mode and the TM mode of the same light beam may be different, the edge coupling members 202 and 204 can include different shapes for allocating a majority of the widths W1 or W2 to be around the critical widths Wc of the TE mode and TM mode, respectively. The optical coupling performance can thus be improved, and the polarization-dependent loss can be mitigated.
In some embodiments, the critical width Wc of the edge coupling member 202 or 204 is determined based on factors such as the selection of the TE/TM mode, the refractive index of the edge coupling members 202, 204, the refractive index of the cladding layer 206, the fiber mode diameter of the light beam, the thickness or height of the edge coupler 106, and the like. In some embodiments, the critical width We of the edge coupling member 202 or 204 corresponding to the dominant optical components of the light beam of interest is included in the range of Wt<=W<=Ww. In some embodiments, if the critical width We is closer to the width Wt than to the width Ww, the optimal shapes of the edge coupling member 202 or 204 would tend to be formed like the edge coupling member 302 with a concave shape, e.g., formed with the condition of α>1, since a majority of the width distribution for the edge coupling member 202 or 204 tends to be closer to the width Wt. In some other embodiments, if the critical width We is closer to the width Ww than to the width Wt, the optimal shapes of the edge coupling member 202 or 204 would tend to be formed like the edge coupling member 306 with a convex shape, e.g., formed with the condition of α<1, since a majority of the width distribution of the edge coupling member 202 or 204 tends to be closer to the width Ww. The edge coupling member 304 can be seen as a boundary case of both the edge coupling members 302 and 306 since the width W of the edge coupling member 304 is uniformly distributed between the initial width Wt and the final width Ww, and is closer to neither the initial width Wt nor the final width Ww. In the depicted example, the edge coupling member 202 is in a convex shape with the exponent of about α=0.5 optimized for the TE mode, and the edge coupling member 204 is in a concave shape with the exponent of about α=3 optimized for the TM mode.
In equation (2), the first exponent is determined as α1>1, representing the section 312A with a concave shape, while the second exponent is determined as α2>1, representing the section 312C with a concave shape. The section 312B has a uniform width WK, corresponding to the dominant optical components We of the light beam in one of the TE mode and the TM mode. In some embodiments, the lateral sides from different sections of the edge coupling member 312 meeting at the boundary of the location of w=LK1 and w=LK2 may include corners of transition, which may cause transmission loss. In some embodiments, the exponents α1, α2, and the lengths LK1 and LK2 are determined so that the corners of transition of lateral sides at the boundary between the sections 312A and 312B, and between the sections 312B and 312C, are minimized to reduce transmission loss.
In some embodiments, the edge coupling member 322 is similar to the edge coupling member 312 as expressed by Equation (2) and is formed of sections 322A, 312B and 312C. The width W of the section 322A is expressed by the same formula as the section 312A except that the exponent is determined as α1<1, representing that the section 322A has a convex shape. One of the edge coupling member 312 or 322 may be preferred over the other according to which one will exhibit less transition loss or a smaller corner at the boundary of the sections 312A (322A) and 312B.
In some embodiments, the edge coupling member 314, formed of sections 314A, 314B and 314C, is similar to the edge coupling member 312 or 322 and can be expressed by Equation (3) as follows:
In equation (3), the third exponent is determined as α3<1, representing the section 314A with a convex shape, while the fourth exponent is determined as α4<1, representing the section 314C with a concave shape. The section 314B has a uniform width WH, corresponding to the dominant optical components of the light beam in the other one of the TE mode and the TM mode with respect to the edge coupling members 312, 322. In some embodiments, the lateral sides from different sections of the edge coupling member 314 meeting at the boundary of the location of w=LH1 and w=LH2 may include corners of transition, which may cause transmission loss. In some embodiments, the exponents α3, α4, and the lengths LH1 and LH2 are determined so that the corners of transition of lateral sides at the boundary between the sections 314A and 314B, and between the sections 314B and 314C are minimized to reduce transmission loss.
In some embodiments, the edge coupling member 324 is similar to the edge coupling member 314 as expressed by Equation (3) and is formed of sections 314A, 314B and 324C. The width W of the section 324C is expressed by the same formula as the section 314C except that the exponent is given as α4>1, representing that the section 324C has a convex shape. One of the edge coupling member 314 or 324 may be preferred over the other according to which one will exhibit less transition loss or a smaller corner at the boundary of the sections 314B and 314C (324C).
In some embodiments, the edge coupling member 312 or 322 is referred to herein as a partial concave shape, meaning that the edge coupling member 312 or 322 includes portions of a concave shape and portions with a uniform width while keeping the entire width monotonically non-decreasing. In some embodiments, the edge coupling member 314 or 324 is referred to herein as a partial convex shape, meaning that the edge coupling member 314 or 324 includes portions of a convex shape and portions with a uniform width while keeping and the entire width monotonically non-decreasing.
Although
In some embodiments, the auxiliary edge couplers 402, e.g., the auxiliary edge couplers 402A, 402B, 402C, and 402D, are another type of single-tip edge coupler different from the single-tip edge coupler 106. In some embodiments, the auxiliary edge couplers 402 are arranged around the single-tip edge coupler 106 to aid in optical coupling and guide the light beam from the optical fiber 104 to the edge coupler 106 and the waveguide 112. The mode mismatch between the optical fiber 104 and the waveguide 112 at the interface of the sidewall 106S can be further reduced. In some embodiments, as shown in
In some embodiments, the auxiliary edge couplers 402 are formed of a material similar to the edge coupler 106. Referring to
In some embodiments, the auxiliary edge couplers 402 have substantially equal widths measured in direction of the Y-axis. In some embodiments, the auxiliary edge couplers 402 have substantially equal heights or thicknesses measured in direction of the Z-axis. In some embodiments, the auxiliary edge couplers 402 have a width Wt measured in the Y-axis from a top-view perspective at the sidewall 106S, which is substantially equal to the initial width of the single-tip edge coupler 106. In some embodiments, the width W of the auxiliary edge couplers 402 is progressively decreased from the location corresponding to the first end 106A to the end of the auxiliary edge couplers 402. In some embodiments, the auxiliary edge couplers 402 tapers from a location corresponding to the sidewall 106S. In some embodiments, the lateral sides of the auxiliary edge coupler 402 is curved from a top-view perspective, e.g., in a shape similar to the sides of the edge coupling member 302 or 306 shown in
In some embodiments, the edge coupler 106 and the auxiliary edge couplers 402 and 502 form a rectangular array, in which any vertical spacing between the adjacent edge couplers 106, 402 or 502 in the rectangular array is substantially equal, or any horizontal spacing between the adjacent edge couplers 106, 402 or 502 in the rectangular array is substantially equal. In some embodiments, the spaces between the edge coupler 106 and the auxiliary edge couplers 402 and 502 and spaces in intermediate layers L2, L4 between the layers L1, L3 and L5 are filled with the material of the cladding layer 206. The introduction of the additional edge couplers 502 may improve the optical coupling efficiency between the optical fiber 104 and the waveguide 112 as compared to the multi-tip edge coupler 400. Further, the arrangement of the auxiliary edge couplers 502 in the same layer as the auxiliary edge couplers 402 would simplify the process and cost of the manufacturing of the multi-tip edge coupler 500.
In some embodiments, the auxiliary edge couplers 604 may form an edge coupler array together with the edge coupler 106 and the auxiliary edge couplers 602, in which the auxiliary edge couplers 604A, 604C and 106 are arranged in a layer L3 of the edge coupler 601. The edge couplers 604A and 604B may be arranged in the layer L1 where the auxiliary edge couplers 602B resides. Likewise, the edge couplers 604C and 604D may be arranged in the layer L5 where the auxiliary edge couplers 602D resides.
In some embodiments, the auxiliary edge couplers 612 may form an edge coupler array together with the edge coupler 106 and the auxiliary edge couplers 612, in which the auxiliary edge couplers 612A through 612D are formed on the circumference S1 where the edge couplers 602 resides.
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The waveguide (or at least portions thereof) 716 is formed in the trench T1, as shown in
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At step 902, a substrate, e.g., substrate 702, is received or provided. At step 904, a first cladding layer, e.g., the cladding layer 706 is deposited over the substrate.
At step 906, one or more first auxiliary edge couplers, e.g., auxiliary edge couplers 402B, 502A, 502B, 512A, 512B, 602B, 604A, 604B, 612A and 612B, are formed in a first layer, e.g., layer L1 or L6, over the first cladding layer. In some embodiments, step 906 is omitted. At step 908, an edge coupler, e.g., the edge coupler 106, is formed in a second layer, e.g., layer L3, over the first layer.
At step 910, one or more second auxiliary edge couplers, e.g., auxiliary edge couplers 402A, 402C, 602A and 602C, are formed in the second layer adjacent to the edge coupler. At step 912, one or more third auxiliary edge couplers e.g., auxiliary edge couplers 402D, 502C, 502D, 512C, 512D, 602D and 604C, 604D, 612C and 612D, are formed in a third layer, e.g., L5 or L7, over the second layer.
At step 914, a second cladding layer, e.g., the cladding layer 706 shown in
In accordance with some embodiments of the present disclosure, a method is provided. The method includes: receiving a substrate; and forming an edge coupler on the substrate, the edge coupler configured to receive light. The forming includes: depositing a first edge coupling member extending in a first direction in a first layer over the substrate; and depositing a second edge coupling member extending in the first direction in a second layer over the first layer. Each of the first and second edge coupling members has a width measured in a second direction monotonically non-decreasing in the first direction. One of the first and second edge coupling members includes a portion in a concave shape and the other includes a portion in a convex shape.
In accordance with some embodiments of the present disclosure, a method is provided. The method includes: receiving a substrate; and forming a multi-tip edge coupler on the substrate. The forming includes: depositing an single-tip edge coupler on an edge of the substrate in a first layer, the single-tip edge coupler having a first width monotonically non-decreasing in a first direction; depositing a first auxiliary edge coupler on the edge of the substrate in a second layer over the first layer, the first auxiliary edge coupler having a second width monotonically non-increasing in the first direction; and depositing a second auxiliary edge coupler on the edge of the substrate in a third layer below the first layer, the second auxiliary edge coupler having a third side monotonically non-increasing in the first direction.
In accordance with some embodiments of the present disclosure, a photonic device includes: a first edge coupler, including: a first edge coupling member on a side of a substrate in a first layer, the first edge coupling member having a first width monotonically non-increasing in a first direction; and a second edge coupling member on the side of the substrate in a second layer over the first layer, the second edge coupling member having a second with non-monotonically increasing in the first direction. One of the first and second widths at least includes a portion with a concave shape and the other at least includes a portion with a convex shape. The second edge coupling member is fully overlapped with the first edge coupling member.
The foregoing outlines structures of several embodiments so that those skilled in the art may better understand the aspects of the present disclosure. Those skilled in the art should appreciate that they may readily use the present disclosure as a basis for designing or modifying other processes and structures for carrying out the same purposes and/or achieving the same advantages of the embodiments introduced herein. Those skilled in the art should also realize that such equivalent constructions do not depart from the spirit and scope of the present disclosure, and that they may make various changes, substitutions, and alterations herein without departing from the spirit and scope of the present disclosure.