This U.S. non-provisional patent application claims priority under 35 U.S.C. §119 of Korean Patent Application Nos. 10-2009-0084581, filed on Sep. 8, 2009, and 10-2010-0066675, filed on Jul. 12, 2010, the entire contents of which are hereby incorporated by reference.
The present invention disclosed herein relates to a photonics device, and more particularly, to an electro-optic modulating device.
Silicon photonics technologies, which are alternative technologies for solving serious heat generation in computing devices and bottlenecks in data communication between semiconductor chips, are becoming an increasingly important issue. The silicon photonics technologies have been significantly developed for the past few years. Examples of the silicon photonics technologies include fast silicon optical modulators, Si—Ge photo-detectors, silicon Raman lasers, silicon optical amplifiers, silicon wavelength converters, and hybrid silicon lasers. Nevertheless, the last data transmission rate that has been realized by silicon modulators is about 10 Gb/s so far. Much faster modulation and data transmission characteristics need to be implemented to meet an increase of a bandwidth that is required for next-generation communication networks and future high-performance computing devices.
Most commercialized high-speed optical modulators are based on electro-optic materials such as lithium niobate and group III-V semiconductors, and are known to provide modulation characteristics of about 40 Gb/s (much faster than 10 Gb/s). In contrast, since single crystal silicon is a material without linear electro-optical characteristics (i.e., Pockels effect) and takes very weak Franz-Keldysh effect, it is difficult to implement fast modulation characteristics in silicon.
Although strained silicon was known to take the Pockels effect in recent years, its measured electro-optic coefficient is much smaller than that of LiNbO3. Also, even though strained Ge/SiGe quantum well structures was known to have relatively high electro-optic absorption characteristics because of the Quantum Confined Stark Effect, various technical limitations (e.g., strain engineering) must be solved in order to implement the strained Ge/SiGe quantum well structures.
As known so far, the high-speed modulation in silicon may be implemented only through the free carrier plasma dispersion effect. In silicon, a variation of the free carrier density incurs a variation of the refractive index of material, and thus the modulation rate of a silicon modulator based on the free carrier plasma dispersion effect is determined by how quickly the free carriers can be injected or removed. Device configuration proposed to implement phase modulation in silicon is roughly divided into three types of forward biased p-i-n diodes, MOS capacitors, and reverse biased PN-junctions.
The forward biased p-i-n diode manner disclosed in U.S. Pat. No. 5,908,305 has been proven to provide high modulation efficiency. However, because of slow charge generation process and slow recombination process, the forward biased p-i-n diode manner has a limitation in the modulation rate unless the lifespan of charges is dramatically reduced.
Both of the MOS capacitor and the reverse biased PN-junction are potentially based on the electric-field induced majority carrier dynamics that may realize about 10 Gb/s or more. However, these manners require a long phase-modulator due to low modulation efficiency. In addition, the reverse biased PN-junction manner disclosed in U.S. Pat. Pub. No. 2006/0008223 has a technical limitation in that optical waveguide loss is large because the entire region of an optical waveguide for phase-modulation is very heavily doped.
The present invention provides a high-performance electro-optic modulating device providing the characteristics such as high-speed, high modulation efficiency, miniaturization, low power consumption, and low optical waveguide loss.
Embodiments of the present invention provide electro-optic modulating devices including an optical waveguide where a vertical structure with at least two sidewalls is disposed, where the sidewalls are used to configure a junction.
In some embodiments, the thickness of the optical waveguide may be smaller than the sum of the lengths of the sidewalls of the vertical structure, projected on a plane vertical to a travelling direction of the optical waveguide.
In other embodiments, the optical waveguide may include a slab waveguide structure including a first slab portion, a second slab portion, and a rib portion disposed between the first slab portion and the second slab portion, and the vertical structure is disposed in the rib portion.
In still other embodiments, the optical waveguide may include: a first body region extended from the first slab portion to contact one sidewall of the vertical structure and a second body region extended from the second slab portion to contact the other sidewall of the vertical structure, where the first and second body regions are first conductive types, and the vertical structure includes at least one vertical doping region having a second conductive type different from the first conductive type.
In even other embodiments, the first and second body regions, and the vertical structure may form a pair of PN-junctions, the vertical structure having a vertical length larger than the thickness of the first slab portion and smaller than the half of the sum of the length of the PN junctions projected on a plane vertical to a travelling direction of the optical waveguide.
In yet other embodiments, the electro-optic modulating devices may further include: a first interconnection structure electrically connecting the vertical doping region and a first circuit; and a second interconnection structure electrically connecting the slab portion and a second circuit, where the first and the second circuits are configured to generate an electric potential difference for a reverse-bias operation of the PN junctions.
In further embodiments, the first slab portion may include a first doping region of a first conductive type, the second slab portion may include a second doping region of the first conductive type, the optical waveguide may include: a first body region extended from the first doping region to contact one sidewall of the vertical structure; and a second body region extended from the second doping region to contact the other sidewall of the vertical structure, the first and second body regions may be formed of intrinsic semiconductors, and the vertical structure may include at least one vertical doping region having a second conductive type different from the first conductive type.
In still further embodiments, the first doping region, the first body region and the vertical structure may form a PIN junction, and the second doping region, the second body region and the vertical structure may form a PIN junction.
In even further embodiments, the electro-optic modulating devices may further include: a first interconnection structure electrically connecting the vertical doping region and a first circuit: and a second interconnection structure electrically connecting the slab portion and a second circuit, where the first and second circuits are configured to generate an electric potential difference for a forward-bias operation of the PIN junctions.
In yet further embodiments, the first and second doping regions may have the substantially same thicknesses as the first and second slab portions, respectively.
In much further embodiments, the vertical structure may include: a plurality of vertical doping regions: and at least one internal region disposed between the vertical doing regions.
In still much further embodiments, the at least one internal region may include an internal doping region having a conductive type different from those of the vertical doping regions, to form a PN-junction along with the vertical doping regions.
In even much further embodiments, the at least one internal region may include a pair of intrinsic regions and an internal doping region disposed between the pair of intrinsic regions and having a conductive type different from those of the vertical doping regions, to form at least two PIN-junctions along with the vertical doping regions.
In yet much further embodiments, the optical waveguide may include a first slab portion, a second slab portion, and a rib portion disposed between the first and second slab portions, the first and second slab portions including first and second doping regions of a first conductive type, and the internal region and the first and second doping regions may be electrically connected to circuits generating different voltages.
In yet much further embodiments, the optical waveguide may include a first slab portion, a second slab portion, and a rib portion disposed between the first and second slab portions, the first and second slab portions including first and second doping regions of a first conductive type, and the internal region and the first and second doping regions may be electrically connected to each other to be in an equipotential state.
In yet much further embodiments, the first slab portion may include a first doping region of a first conductive type, and the second slab portion may include a second doping region of a second conductive type different from the first conductive type. The vertical structure may include: a first vertical doping region having the second conductive type and disposed adjacent to the first slab portion; and a second vertical doping region having the first conductive type and disposed adjacent to the second slab portion.
In yet much further embodiments, the electro-optic modulating devices may further include a buried insulating layer disposed under the optical waveguide, where the optical waveguide is formed to have a sidewall exposing an upper surface of the buried insulating layer.
The accompanying drawings are included to provide a further understanding of the present invention, and are incorporated in and constitute a part of this specification. The drawings illustrate exemplary embodiments of the present invention and, together with the description, serve to explain principles of the present invention. In the drawings:
Preferred embodiments of the present invention will be described below in more detail with reference to the accompanying drawings. The present invention may, however, be embodied in different forms and should not be constructed as limited to the embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete, and will fully convey the scope of the present invention to those skilled in the art.
In the specification, the dimensions of layers and regions are exaggerated for clarity of illustration. It will also be understood that when a layer (or film) is referred to as being ‘on’ another layer or substrate, it can be directly on the other layer or substrate, or intervening layers may also be present. Also, though terms like a first, a second, and a third are used to describe various regions and layers in various embodiments of the present invention, the regions and the layers are not limited to these terms. These terms are used only to tell one region or layer from another region or layer. Therefore, a layer referred to as a first layer in one embodiment can be referred to as a second layer in another embodiment. An embodiment described and exemplified herein includes a complementary embodiment thereof.
Hereinafter, it will be described about an exemplary embodiment of the present invention in conjunction with the accompanying drawings.
Referring to
According to an embodiment of the present invention, the semiconductor layer 30 may be formed of single crystal silicon. For example, the semiconductor layer 30 may form a SOI wafer along with the substrate 10. In this case, a buried insulating layer 20 may be disposed between the substrate and the semiconductor layer 30 as shown in
First and second doping regions D1 and D2 may be disposed in the first and second slab portions SP1 and SP2, respectively. A vertical doping region 50 may be disposed in the rib portion RP to form a vertical structure. According to the present embodiment, the first and second doping regions D1 and D2 are first conductive types, and the vertical doping region 50 may be a second conductive type different from the first conductive type. For example, when the first and second doping regions D1 and D2 are p-types, the vertical doping region 50 may be an n-type. Alternatively, when the first and second doping regions D1 and D2 are n-types, the vertical doping region 50 may be a p-type.
According to the present embodiment, a portion (hereinafter, a first body region B1) of the optical waveguide WG disposed between the first doping region D1 and the vertical doping region 50 may be the same conductive type as the first doping region D1. That is, the first body region B1 may be doped with a conductive type different from that of the vertical doping region 50. Thus, the first body region D1 and the vertical doping region 50 may form a PN-junction as shown in
Referring to
Referring to
In the meantime,
In addition, the first and second doping regions D1 and D2 have the same conductive type as the first and second body regions B1 and B2, and may be more heavily doped than the first and second body regions B1 and B2. Also, as shown in
According to the present embodiment, the vertical doping region 50 may be electrically connected to a first circuit C1 generating a first voltage V1 through a first interconnection structure 91, and the first and second doping regions D1 and D2 may be electrically connected to a second circuit C2 generating a second voltage V2 through second interconnection structures 92a and 92b.
According to an embodiment, the first voltage V1 and the second voltage V2 may be a modulation voltage and a ground voltage, respectively. Thus, a certain electric potential difference determined by the first voltage V1 may be generated between the vertical doping region 50 and the first and second body regions B1 and B2. As described above, since both sidewalls of the vertical doping region 50 are used to form PN-junctions, the electro-optic modulating device according to the embodiment described with reference to
Referring to
The internal doping region B3 may be the same conductive type as the first and second body regions B1 and B2, and the vertical doping regions 50 may be conductive types different from the first and second body regions B1 and B2. Thus, PN-junctions having a longer length than that of embodiment described with reference to
Meanwhile, as shown in
Upon operation, the first voltage V1 and the second voltage V2 may be a modulation voltage and a ground voltage, respectively. Thus, a certain electric potential difference determined by the first voltage V1 may be generated between the vertical doping regions 50 and the first and second body regions B1 and B2. According to an embodiment, the first voltage V1 and the second voltage V2 may be selected to allow the PN-junctions to operate in a PN reverse mode.
Referring to
The internal doping regions B31 and B32 may be the same conductive types as the first and second body regions B1 and B2, and the vertical doping regions 50 may be conductive types different from the first and second body regions B1 and B2. Thus, PN-junctions having a longer length than that of embodiment described with reference to
In the meantime, as shown in
Upon operation, the first voltage V1 and the second voltage V2 may be a modulation voltage and a ground voltage, respectively. Thus, a certain electric potential difference determined by the first voltage V1 may be generated between the vertical doping regions 50 and the first and second body regions B1 and B2. According to an embodiment, the first voltage V1 and the second voltage V2 may be selected to allow the PN-junctions to operate in a PN reverse mode.
Referring to
First and second doping regions D1 and D2 may be disposed in the first and second slab portions SP1 and SP2. A vertical doping region 50 forming a vertical structure may be disposed in the rib portion RP. According to the present embodiment, the first and second doping regions D1 and D2 are first conductive types, and the vertical doping region 50 may be a second conductive type different from the first conductive type. For example, when the first and second doping regions D1 and D2 are p-types, the vertical doping region 50 may be an n-type.
According to the present embodiment, a portion (hereinafter, first body region B1) of the optical waveguide WG disposed between the first doping region D1 and the vertical doping region 50 may substantially have physical properties close to an intrinsic semiconductor. For example, the first body region B1 may be undoped silicon or silicon having a lower doping level by several orders than the first doping region D1. Thus, the first doping region D1, the first body region B1, and the vertical doping region 50 may form a PIN junction as shown in
In addition, the vertical doping region 50 may be formed to allow the undersurface of the vertical doping region 50 to contact the upper surface of the buried insulating layer 20. That is, the vertical doping region 50 may have the substantially same thickness as the rib portion RP. In this case, the first body region B1 and the second body region B2 may be separated from each other by the vertical doping region 50 as shown in
In the meantime,
According to the present embodiment, the first and second doping regions D1 and D2 may be formed to have the undersurface contacting the upper surface of the buried insulating layer 20. That is, the first and second doping regions D1 and D2 may have the substantially same thicknesses as the first and second slab portions SP1 and SP2. Also, although an abrupt junction structure is shown in FIG. 4B as an example, the concentration profiles of each portion of the PIN-junction may be variously modified from those shown in the drawing.
The vertical doping region 50 may be electrically connected to a first circuit C1 generating a first voltage V1 through a first interconnection structure 91, and the first and second doping regions D1 and D2 may be electrically connected to a second circuit C2 generating a second voltage V2 through second interconnection structures 92a and 92b.
According to an embodiment, the first voltage V1 and the second voltage V2 may be a modulation voltage and a ground voltage, respectively. Thus, a certain electric potential difference dependent on the first voltage V1 may be generated between the vertical doping region 50 and the first and second body regions B1 and B2. As described above, since both sidewalls of the vertical doping region 50 are used to form PIN-junctions, the electro-optic modulating device according to the embodiment described with reference to
Referring to
Similarly to the first and second body region B1 and B2 the intrinsic regions B33 and B34 may have physical properties close to an intrinsic semiconductor. However, the intrinsic regions B33 and B34 need not have the exact same physical properties as the first and second body regions B1 and B2.
The internal doping region B35 may have the same conductive type as the first and second doping regions D1 and D2. That is, the internal doping region B35 may have a conductive type different from the vertical doping regions 50, and therefore a pair of PIN-junctions may be formed in the vertical structure as shown in
In the meantime, as shown in
According to an embodiment, the first voltage V1 and the second voltage V2 may be a modulation voltage and a ground voltage, respectively. Thus, a certain electric potential difference dependent on the first voltage V1 may be generated between the vertical doping region 50 and the first and second body regions B1 and B2, In particular, when the first and second voltages V1 and V2 are generated such that the PIN-junctions operate in a PIN forward mode, the size of a current entering the optical waveguide may further increase compared to typical technologies or the embodiment described with reference to
Referring to
The internal doping region B35 may have the same conductive type as the first and second doping regions D1 and D2. That is, the internal doping region B35 may have a conductive type different from the vertical doping regions 50, and therefore a pair of PN-junctions may be formed in the vertical structure as shown in
According to an embodiment, as shown in
According to another embodiment, as shown in
Referring to
The internal doping regions B36 and B37 may have the same conductive type as the first and second doping regions D1 and D2. That is, the internal doping regions B36 and B37 may have a conductive type different from the vertical doping regions 50, and therefore four PN-junctions may be formed in the vertical structure as shown in
As shown in
Referring to
Specifically, according to an embodiment, a forward direct current voltage may be applied between the vertical doping regions 50 and the first and second doping regions D1 and D2, and therefore the PIN-junctions formed outside the vertical structure may operate in PIN forward mode. However, an electric potential difference applied between the vertical doping regions 50 and the internal doping regions B36 and B37 may be determined by the third voltage V3, the junctions in the vertical structure may operate under optimized conditions regardless of the operation of the PIN-junctions outside the vertical structure. As a result, the junctions inside and outside the vertical structure may operate independently of each other under optimized conditions. This independent optimization may be used to improve modulation characteristics in an electro-optic modulating device according to an embodiment.
Referring to
First and second doping regions D1 and D2 may be disposed in the first and second slab portions SP1 and SP2, and a vertical structure may be disposed in the rib portion RP. According to an embodiment, the first doping region D1 and the second doping region D2 may have different conductive types from each other. For example, the first doping region D1 is a p-type, and the second doping region D2 may be an n-type. Thus, the first and second slab portions SP1 and SP2 may be asymmetric at the side of a doping profile around the rib portion RP.
The vertical structure may include a first vertical doping region 51 and a second vertical doping region 52 that are spaced from each other, and an internal region B3 disposed therebetween. The first vertical doping region 51 and the second vertical doping region 52 may have different conductive types from each other, and the internal region B3 may be an intrinsic semiconductor. Thus, the first vertical doping region 51 and the second vertical doping region 52, and the internal region B3, which are disposed in the vertical structure, may form a PIN-junction.
In addition, the first vertical doping region 51 may have a different conductive type from the first doping region D1, and may be disposed adjacent to the first doping region D1. The second vertical doping region 52 may have a different conductive type from the second doping region D2, and may be disposed adjacent to the second doping region D2. A first body region B1 disposed between the first vertical doping region 51 and the first doping region. D1, and a second body region B2 disposed between the second vertical doping region 52 and the second doping region D2 may be intrinsic semiconductors. In this case, the first vertical doping region 51, the first body region B1, and the first doping region D1 may form a PIN-junction, and the second vertical doping region 52, the second body region B2, and the second doping region D2 may form another PIN-junction.
The first and second vertical doping regions 51 and 52 may be extended to a depth less than the thickness of the rib portion RP as shown in
The first vertical doping region 51 and the second doping region D2 may be electrically connected to a first circuit C1 generating a first voltage V1 through a first interconnection structure 91, and the second vertical doping region 52 and the first doping region D1 may be electrically connected to a second circuit C2 generating a second voltage V2 through a second interconnection structure 92. According to an embodiment, the first voltage V1 and the second voltage V2 may be a modulation voltage and a ground voltage, respectively. Also, the first and second circuits C1 and C2 may generate the first and second voltages V1 and V2 such that the PIN-junctions may operate in PIN forward mode.
Referring to
A vertical structure having at least one pair of vertical doping regions 50 may be disposed in the optical waveguide WG. The vertical structure may further include an internal doping region B35 disposed between the vertical doping regions 50 and at least two internal regions B36 and B37 disposed between the internal doping region B35 and the vertical doping regions 50. The internal doping region B35 may have a different type from the vertical doping regions 50. The internal regions B36 and B37 may be doped with certain impurities as shown in
When the internal region B36 and B37 are doped, as shown in
When the internal regions B36 and B37 are intrinsic semiconductors, as shown in
The vertical doping regions 50 may be electrically connected to a first circuit C1 generating a first voltage V1 through a first interconnection structure 91, and the internal doping region B35 may be electrically connected to a second circuit C2 generating a second voltage V2 through a second interconnection structure 92. The first voltage V1 and the second voltage V2 may be a modulation voltage and a ground voltage, respectively. In the embodiment described with reference to
Referring to
Referring to
In operation, the optical beam 1010 may be separated from the first cascaded Y-branch coupler after being incident to the input of the MZI. As a result, a first portion of the optical beam 1010 may travel to one of the arms of the MZI, and a second portion of the optical beam 1010 may travel to the other arm of the MZI.
As shown in the drawing, the optical phase shifter 1110 may be formed in one of the arms of the MZI, and may control a relative phase difference between the first and second portions of the optical beam 1010 in response to external signals V1 and V2. The first and second portions of the optical beam 1010 may be joined together at the output of the MZI. As a result of constructive interference and destructive interference between the first and second portions of the optical beam 1010 by the relative phase difference, the optical beam 1010 emitted from the output of the MZI may have modulated characteristics. According to an embodiment, the optical beam 1010 incident to the input of the MZI may be a continuous wave, and the optical beam 1010 emitted from the output of the MZI may have a saw-tooth waveform as a result of the modulation. According to a modified embodiment of the present invention, both of the two arms of the MZI may be configured to have the electro-optic modulating devices disclosed in the present invention.
In the meantime, the optical device 1004 may be implemented with various methods other than MZI. For example, the optical device 1004 may also be implemented through a ring-resonator structure including a structure identical or similar to one of the electro-optic modulating devices described with reference to
According to an embodiment of the present invention, the optical waveguides described with reference to
The above-disclosed subject matter is to be considered illustrative, and not restrictive, and the appended claims are intended to cover all such modifications, enhancements, and other embodiments, which fall within the true spirit and scope of the present invention. Thus, to the maximum extent allowed by law, the scope of the present invention is to be determined by the broadest permissible interpretation of the following claims and their equivalents, and shall not be restricted or limited by the foregoing detailed description.
Number | Date | Country | Kind |
---|---|---|---|
10-2009-0084581 | Sep 2009 | KR | national |
10-2010-0066675 | Jul 2010 | KR | national |
Number | Name | Date | Kind |
---|---|---|---|
3866143 | Jacobs et al. | Feb 1975 | A |
4675518 | Oimura et al. | Jun 1987 | A |
4904039 | Soref | Feb 1990 | A |
4997246 | May et al. | Mar 1991 | A |
5359679 | Tanaka et al. | Oct 1994 | A |
5757986 | Crampton et al. | May 1998 | A |
5908305 | Crampton et al. | Jun 1999 | A |
6298177 | House | Oct 2001 | B1 |
6584239 | Dawnay et al. | Jun 2003 | B1 |
7251408 | Gunn, III et al. | Jul 2007 | B1 |
7280712 | Liu | Oct 2007 | B2 |
7474811 | Quitoriano et al. | Jan 2009 | B1 |
7657146 | Laval et al. | Feb 2010 | B2 |
7764850 | Bratkovski et al. | Jul 2010 | B2 |
7826688 | Sadagopan et al. | Nov 2010 | B1 |
8149493 | Chen | Apr 2012 | B2 |
8362494 | Lo et al. | Jan 2013 | B2 |
20060008223 | Gunn, III et al. | Jan 2006 | A1 |
20080212913 | Gill et al. | Sep 2008 | A1 |
20090190875 | Bratkovski et al. | Jul 2009 | A1 |
20090214151 | Keeling | Aug 2009 | A1 |
20090263078 | Hosomi et al. | Oct 2009 | A1 |
20100080504 | Shetrit et al. | Apr 2010 | A1 |
20100099242 | Fedeli | Apr 2010 | A1 |
20100158426 | Manipatruni et al. | Jun 2010 | A1 |
20100316325 | Okamoto et al. | Dec 2010 | A1 |
20110176762 | Fujikata et al. | Jul 2011 | A1 |
20120043527 | Ding et al. | Feb 2012 | A1 |
Number | Date | Country |
---|---|---|
102004007251 | Sep 2005 | DE |
100772538 | Oct 2007 | KR |
Entry |
---|
D. Marris-Morini et al. Low loss and high speed silicon optical modulator based on a lateral carrier depletion structure. Optics Express, 16:1:334-339, Jan. 2008. |
Ansheng Liu et al., “High-speed optical modulation based on carrier depletion in a silicon waveguide”, Optics Express, Jan. 22, 2007, pp. 660-668, vol. 15, No. 2, Optical Society of America. |
Number | Date | Country | |
---|---|---|---|
20110058764 A1 | Mar 2011 | US |